Recent interesting articles

The electrical conductivity of solid-state matter is a fundamental physical property and can be precisely derived from the resistance measured via the four-point probe technique excluding contributions from parasitic contact resistances. Over time, this method has become an interdisciplinary characterization tool in materials science, semiconductor industries, geology, physics, etc, and is employed for both fundamental and application-driven research. However, the correct derivation of the conductivity is a demanding task which faces several difficulties, e.g. the homogeneity of the sample or the isotropy of the phases. In addition, these sample-specific characteristics are intimately related to technical constraints such as the probe geometry and size of the sample. In particular, the latter is of importance for nanostructures which can now be probed technically on very small length scales. On the occasion of the 100th anniversary of the four-point probe technique, introduced by Frank Wenner, in this review we revisit and discuss various correction factors which are mandatory for an accurate derivation of the resistivity from the measured resistance. Among others, sample thickness, dimensionality, anisotropy, and the relative size and geometry of the sample with respect to the contact assembly are considered. We are also able to derive the correction factors for 2D anisotropic systems on circular finite areas with variable probe spacings. All these aspects are illustrated by state-of-the-art experiments carried out using a four-tip STM/SEM system. We are aware that this review article can only cover some of the most important topics. Regarding further aspects, e.g. technical realizations, the influence of inhomogeneities or different transport regimes, etc, we refer to other review articles in this field.

http://iopscience.iop.org/article/10.1088/0953-8984/27/22/223201/pdf

November 3.

Boros Csanád Örs

Margination of micro- and nano-particles in blood flow and its effect on drug delivery

Kathrin Müller, Dmitry A. Fedosov & Gerhard Gompper

Drug delivery by micro- and nano-carriers enables controlled transport of pharmaceuticals to targeted sites. Even though carrier fabrication has made much progress recently, the delivery including controlled particle distribution and adhesion within the body remains a great challenge. The adhesion of carriers is strongly affected by their margination properties (migration toward walls) in the microvasculature. To investigate margination characteristics of carriers of different shapes and sizes and to elucidate the relevant physical mechanisms, we employ mesoscopic hydrodynamic simulations of blood flow. Particle margination is studied for a wide range of hematocrit values, vessel sizes, and flow rates, using two- and three-dimensional models. The simulations show that the margination properties of particles improve with increasing carrier size. Spherical particles yield slightly better margination than ellipsoidal carriers; however, ellipsoidal particles exhibit a slower rotational dynamics near a wall favoring their adhesion. In conclusion, micron-sized ellipsoidal particles are favorable for drug delivery in comparison with sub-micron spherical particles.

http://www.nature.com/articles/srep04871

Szeptember 8-15.

Scherübl Zoltán

Guiding of Electrons in a Few Mode Ballistic Graphene Channel

Peter Rickhaus, Ming-Hao Liu, Péter Makk, Romain Maurand, Samuel Hess, Simon Zihlmann, Markus Weiss, Klaus Richter, Christian Schönenberger

http://arxiv.org/abs/1509.02653

Hexagonal boron nitride as an atomically thin oxidation barrier for ferromagnetic nano structures

Simon Zihlmann, Péter Makk, C. A. F. Vaz, Christian Schönenberger

http://arxiv.org/abs/1509.03087

Giga-Hertz quantized charge pumping in bottom gate defined InAs nanowire quantum dots

S. d'Hollosy, M. Jung, A. Baumgartner, V.A. Guzenko, M.H. Madsen, J. Nygård, C. Schönenberger

http://arxiv.org/abs/1509.01574

Coherent coupling of a single spin to microwave cavity photons

J. J. Viennot, M. C. Dartiailh, A. Cottet, T. Kontos

http://arxiv.org/abs/1509.03839

Negative local resistance due to viscous electron backflow in graphene

D. A. Bandurin, I. Torre, R. Krishna Kumar, M. Ben Shalom, A. Tomadin, A. Principi, G. H. Auton, E. Khestanova, K. S. Novoselov, I. V. Grigorieva, L. A. Ponomarenko, A. K. Geim, M. Polini

http://arxiv.org/abs/1509.04165

Point contacts in encapsulated graphene

Clevin Handschin, Balint Fülöp, Péter Makk, Sofya Blanter, Markus Weiss, K. Watanabe, T. Taniguchi, Szabolcs Csonka, Christian Schönenberger

http://arxiv.org/abs/1509.04137

Coherent manipulation of Andreev states in superconducting atomic contacts

C. Janvier (1), L. Tosi (1), L. Bretheau (1), Ç. Ö. Girit (1), M. Stern (1), P. Bertet (1), P. Joyez (1), D. Vion (1), D. Esteve (1), M.F. Goffman (1), H. Pothier (1), C. Urbina (1) ((1) QUANTRONICS)

http://arxiv.org/abs/1509.03961

Realization of Microwave Quantum Circuits Using Hybrid Superconducting-Semiconducting Nanowire Josephson Elements

G. de Lange, B. van Heck, A. Bruno, D. J. van Woerkom, A. Geresdi, S. R. Plissard, E. P. A. M. Bakkers, A. R. Akhmerov, and L. DiCarlo

http://journals.aps.org/prl/abstract/10.1103/PhysRevLett.115.127002

Semiconductor-Nanowire-Based Superconducting Qubit

T. W. Larsen, K. D. Petersson, F. Kuemmeth, T. S. Jespersen, P. Krogstrup, J. Nygård, and C. M. Marcus

http://journals.aps.org/prl/abstract/10.1103/PhysRevLett.115.127001

Charge Number Dependence of the Dephasing Rates of a Graphene Double Quantum Dot in a Circuit QED Architecture

Guang-Wei Deng, Da Wei, J. R. Johansson, Miao-Lei Zhang, Shu-Xiao Li, Hai-Ou Li, Gang Cao, Ming Xiao, Tao Tu, Guang-Can Guo, Hong-Wen Jiang, Franco Nori, and Guo-Ping Guo

http://journals.aps.org/prl/abstract/10.1103/PhysRevLett.115.126804

Spin pairs in a weakly coupled many-electron quantum dot

S. Hellmüller, D. Bischoff, T. Müller, M. Beck, K. Ensslin, and T. Ihn

http://journals.aps.org/prb/abstract/10.1103/PhysRevB.92.115401

Observation of negative refraction of Dirac fermions in graphene

Gil-Ho Lee, Geon-Hyoung Park, Hu-Jong Lee

http://www.nature.com/nphys/journal/vaop/ncurrent/full/nphys3460.html

Parity lifetime of bound states in a proximitized semiconductor nanowire

A. P. Higginbotham, S. M. Albrecht, G. Kiršanskas, W. Chang, F. Kuemmeth, P. Krogstrup, T. S. Jespersen, J. Nygård, K. Flensberg, C. M. Marcus

http://www.nature.com/nphys/journal/vaop/ncurrent/full/nphys3461.html

Reliable Exfoliation of Large-Area High-Quality Flakes of Graphene and Other Two-Dimensional Materials

Yuan Huang, Eli Sutter, Norman N. Shi, Jiabao Zheng, Tianzhong Yang, Dirk Englund, Hong-Jun Gao, and Peter Sutter

http://pubs.acs.org/doi/abs/10.1021/acsnano.5b04258

Aug. 25. - szept. 7.

Coupling Two Distant Double Quantum Dots with a Microwave Resonator

Guang-Wei Deng, Da Wei, Shu-Xiao Li, J. R. Johansson, Wei-Cheng Kong, Hai-Ou Li, Gang Cao, Ming Xiao, Guang-Can Guo, Franco Nori, Hong-Wen Jiang, and Guo-Ping Guo

We fabricated a hybrid device with two distant graphene double quantum dots (DQDs) and a microwave resonator. A nonlinear response is observed in the resonator reflection amplitude when the two DQDs are jointly tuned to the vicinity of the degeneracy points. This observation can be well fitted by the Tavis–Cummings (T–C) model which describes two two-level systems coupling with one photonic field. Furthermore, the correlation between the DC currents in the two DQDs is studied. A nonzero cross-current correlation is observed which has been theoretically predicted to be an important sign of nonlocal coupling between two distant systems. Our results explore T–C physics in electronic transport and also contribute to the study of nonlocal transport and future implementations of remote electronic entanglement.

http://pubs.acs.org/doi/abs/10.1021/acs.nanolett.5b02400

Reliable Exfoliation of Large-Area High-Quality Flakes of Graphene and Other Two-Dimensional Materials

Yuan Huang, Eli Sutter, Norman N. Shi, Jiabao Zheng, Tianzhong Yang, Dirk Englund, Hong-Jun Gao, and Peter Sutter

Mechanical exfoliation has been a key enabler of the exploration of the properties of two-dimensional materials, such as graphene, by providing routine access to high-quality material. The original exfoliation method, which remained largely unchanged during the past decade, provides relatively small flakes with moderate yield. Here, we report a modified approach for exfoliating thin monolayer and few-layer flakes from layered crystals. Our method introduces two process steps that enhance and homogenize the adhesion force between the outermost sheet in contact with a substrate: Prior to exfoliation, ambient adsorbates are effectively removed from the substrate by oxygen plasma cleaning, and an additional heat treatment maximizes the uniform contact area at the interface between the source crystal and the substrate. For graphene exfoliation, these simple process steps increased the yield and the area of the transferred flakes by more than 50 times compared to the established exfoliation methods. Raman and AFM characterization shows that the graphene flakes are of similar high quality as those obtained in previous reports. Graphene field-effect devices were fabricated and measured with back-gating and solution top-gating, yielding mobilities of ∼4000 and 12 000 cm2/(V s), respectively, and thus demonstrating excellent electrical properties. Experiments with other layered crystals, e.g., a bismuth strontium calcium copper oxide (BSCCO) superconductor, show enhancements in exfoliation yield and flake area similar to those for graphene, suggesting that our modified exfoliation method provides an effective way for producing large area, high-quality flakes of a wide range of 2D materials.

http://pubs.acs.org/doi/abs/10.1021/acsnano.5b04258

Influence of Impurity Spin Dynamics on Quantum Transport in Epitaxial Graphene

Samuel Lara-Avila, Sergey Kubatkin, Oleksiy Kashuba, Joshua A. Folk, Silvia Lüscher, Rositza Yakimova, T. J. B. M. Janssen, Alexander Tzalenchuk, and Vladimir Fal’ko

Experimental evidence from both spin-valve and quantum transport measurements points towards unexpectedly fast spin relaxation in graphene. We report magnetotransport studies of epitaxial graphene on SiC in a vector magnetic field showing that spin relaxation, detected using weak-localization analysis, is suppressed by an in-plane magnetic field B∥, and thereby proving that it is caused at least in part by spinful scatterers. A nonmonotonic dependence of the effective decoherence rate on B∥ reveals the intricate role of the scatterers’ spin dynamics in forming the interference correction to the conductivity, an effect that has gone unnoticed in earlier weak localization studies.

http://journals.aps.org/prl/pdf/10.1103/PhysRevLett.115.106602

Highly thermally conductive and mechanically strong graphene fibers

Guoqing Xin, Tiankai Yao, Hongtao Sun, Spencer Michael Scott, Dali Shao, Gongkai Wang, Jie Lian

Graphene, a single layer of carbon atoms bonded in a hexagonal lattice, is the thinnest, strongest, and stiffest known material and an excellent conductor of heat and electricity. However, these superior properties have yet to be realized for graphene-derived macroscopic structures such as graphene fibers. We report the fabrication of graphene fibers with high thermal and electrical conductivity and enhanced mechanical strength. The inner fiber structure consists of large-sized graphene sheets forming a highly ordered arrangement intercalated with small-sized graphene sheets filling the space and microvoids. The graphene fibers exhibit a submicrometer crystallite domain size through high-temperature treatment, achieving an enhanced thermal conductivity up to 1290 watts per meter per kelvin. The tensile strength of the graphene fiber reaches 1080 megapascals.

https://www.sciencemag.org/content/349/6252/1083.abstract

A quantum circuit rule for interference effects in single-molecule electrical junctions

David Zsolt Manrique, Cancan Huang, Masoud Baghernejad, Xiaotao Zhao, Oday A. Al-Owaedi, Hatef Sadeghi, Veerabhadrarao Kaliginedi, Wenjing Hong, Murat Gulcur, Thomas Wandlowski, Martin R. Bryce, Colin J. Lambert

A quantum circuit rule for combining quantum interference (QI) effects in the conductive properties of oligo(phenyleneethynylene) (OPE)-type molecules possessing three aromatic rings was investigated both experimentally and theoretically. Molecules were of the type X-Y-X, where X represents pyridyl anchors with para (p), meta (m) or ortho (o) connectivities and Y represents a phenyl ring with p and m connectivities. The conductances GXmX (GXpX) of molecules of the form X-m-X (X-p-X), with meta (para) connections in the central ring were predominantly lower (higher), irrespective of the meta, para, or ortho nature of the anchor groups X, demonstrating that conductance is dominated by the nature of QI in the central ring Y. The single-molecule conductances were found to satisfy the quantum circuit rule Gppp/Gpmp = Gmpm/Gmmm. This demonstrates that the contribution to the conductance from the central ring is independent of the para versus meta nature of the anchor groups.

http://xxx.lanl.gov/abs/1509.00990

Spawning rings of exceptional points out of Dirac cones

Bo Zhen, Chia Wei Hsu, Yuichi Igarashi, Ling Lu, Ido Kaminer, Adi Pick, Song-Liang Chua, John D. Joannopoulos & Marin Soljacˇic

The Dirac cone underlies many unique electronic properties of graphene1 and topological insulators, and its band structure— two conical bands touching at a single point—has also been realized for photons in waveguide arrays2 , atoms in optical lattices3 , and through accidental degeneracy4,5. Deformation of the Dirac cone often reveals intriguing properties; an example is the quantum Hall effect, where a constant magnetic field breaks the Dirac cone into isolated Landau levels. A seemingly unrelated phenomenon is the exceptional point6,7, also known as the parity–time symmetry breaking point8–11, where two resonances coincide in both their positions and widths. Exceptional points lead to counter-intuitive phenomena such as loss-induced transparency12, unidirectional transmission or reflection11,13,14, and lasers with reversed pump dependence15 or single-mode operation16,17. Dirac cones and exceptional points are connected: it was theoretically suggested that certain non-Hermitian perturbations can deform a Dirac cone and spawn a ring of exceptional points18–20. Here we experimentally demonstrate such an ‘exceptional ring’ in a photonic crystal slab. Angle-resolved reflection measurements of the photonic crystal slab reveal that the peaks of reflectivity follow the conical band structure of a Dirac cone resulting from accidental degeneracy, whereas the complex eigenvalues of the system are deformed into a two-dimensional flat band enclosed by an exceptional ring. This deformation arises from the dissimilar radiation rates of dipole and quadrupole resonances, which play a role analogous to the loss and gain in parity–time symmetric systems. Our results indicate that the radiation existing in any open system can fundamentally alter its physical properties in ways previously expected only in the presence of material loss and gain.

http://www.nature.com/nature/journal/vaop/ncurrent/pdf/nature14889.pdf

A Short Course on Topological Insulators: Band-structure topology and edge states in one and two dimensions

János K. Asbóth, László Oroszlány, András Pályi

This course-based primer provides newcomers to the field with a concise introduction to some of the core topics in the emerging field of topological band insulators in one and two dimensions. The aim is to provide a basic understanding of edge states, bulk topological invariants, and of the bulk--boundary correspondence with as simple mathematical tools as possible. We use noninteracting lattice models of topological insulators, building gradually on these to arrive from the simplest one-dimensional case (the Su-Schrieffer-Heeger model for polyacetylene) to two-dimensional time-reversal invariant topological insulators (the Bernevig-Hughes-Zhang model for HgTe). In each case the model is introduced first and then its properties are discussed and subsequently generalized. The only prerequisite for the reader is a working knowledge in quantum mechanics, the relevant solid state physics background is provided as part of this self-contained text, which is complemented by end-of-chapter problems.

http://xxx.lanl.gov/abs/1509.02295

Március 24-31.

Fülöp Gergő

Graphene-templated directional growth of an inorganic nanowire

Won Chul Lee, Kwanpyo Kim, Jungwon Park, Jahyun Koo, Hu Young Jeong, Hoonkyung Lee, David A. Weitz, Alex Zettl & Shoji Takeuchi

http://www.nature.com/nnano/journal/vaop/ncurrent/full/nnano.2015.36.html

Coaxial lithography

Tuncay Ozel, Gilles R. Bourret & Chad A. Mirkin

http://www.nature.com/nnano/journal/vaop/ncurrent/full/nnano.2015.33.html

Coupling between electrons and optical phonons in suspended bilayer graphene

Antti Laitinen, Manohar Kumar, Mika Oksanen, Bernard Plaçais, Pauli Virtanen, and Pertti Hakonen

http://journals.aps.org/prb/abstract/10.1103/PhysRevB.91.121414

Nonlocal electromagnetic response of graphene nanostructures

Arya Fallahi, Tony Low, Michele Tamagnone, and Julien Perruisseau-Carrier

http://journals.aps.org/prb/abstract/10.1103/PhysRevB.91.121405

Nonequilibrium spin transport in Zeeman-split superconductors

Tatiana Krishtop, Manuel Houzet, and Julia S. Meyer

http://journals.aps.org/prb/abstract/10.1103/PhysRevB.91.121407

Finite-frequency noise in a quantum dot with normal and superconducting leads

Stephanie Droste, Janine Splettstoesser, and Michele Governale

http://journals.aps.org/prb/abstract/10.1103/PhysRevB.91.125401

Március 24.

Boros Csanád Örs

Spin and charge transport in graphene-based spin transport devices with Co/MgO spin injection and spin detection electrodes

'F. Volmer, M. Drögeler, G. Güntherodt, C. Stampfer, B. Beschoten'

In this review we discuss spin and charge transport properties in graphene-based single-layer and few-layer spin-valve devices. We give an overview of challenges and recent advances in the field of device fabrication and discuss two of our fabrication methods in more detail which result in distinctly different device performances. In the first class of devices, Co/MgO electrodes are directly deposited onto graphene which results in rough MgO-to-Co interfaces and favor the formation of conducting pinholes throughout the MgO layer. We show that the contact resistance area product (RcA) is a benchmark for spin transport properties as it scales with the measured spin lifetime in these devices indicating that contact-induced spin dephasing is the bottleneck for spin transport even in devices with large RcA values. In a second class of devices, Co/MgO electrodes are first patterned onto a silicon substrate. Subsequently, a graphene-hBN heterostructure is directly transferred onto these prepatterned electrodes which provides improved interface properties. This is seen by a strong enhancement of both charge and spin transport properties yielding charge carrier mobilities exceeding 20000 cm2/(Vs) and spin lifetimes up to 3.7 ns at room temperature. We discuss several shortcomings in the determination of both quantities which complicates the analysis of both extrinsic and intrinsic spin scattering mechanisms. Furthermore, we show that contacts can be the origin of a second charge neutrality point in gate dependent resistance measurements which is influenced by the quantum capacitance of the underlying graphene layer.

http://arxiv.org/abs/1503.01735v1

Nov. 1-21.

Scherübl Zoltán

Unusual resistance-voltage dependence of nanojunctions during electromigration in ultra-high vacuum

D. Stöffler, M. Marz, B. Kießig, T. Tomanic, R. Schäfer, H. v. Löhneysen, R. Hoffmann-Vogel

The electrical resistance R of metallic nanocontacts subjected to controlled cyclic electromigration in ultra-high vacuum has been investigated in-situ as a function of applied voltage V. For sufficiently small contacts, i.e., large resistance, a decrease of R(V) while increasing V is observed. This effect is tentatively attributed to the presence of contacts separated by thin vacuum barriers in parallel to ohmic nanocontacts. Simple model calculations indicate that both thermal activation or tunneling can lead to this unusual behavior. We describe our data by a tunneling model whose key parameter, i.e., the tunneling distance, changes because of thermal expansion due to Joule heating and/or electrostatic strain arising from the applied voltage. Oxygen exposure during electromigration prevents the formation of negative R(V) slopes, and at the same time enhances the probability of uncontrolled melting, while other gases show little effects. In addition, indication for field emission has been observed in some samples

http://arxiv.org/abs/1411.0105

Pb/InAs nanowire Josephson junction with high critical current and magnetic flux focusing

J. Paajaste, M. Amado, S. Roddaro, F. S. Bergeret, D. Ercolani, L. Sorba, F. Giazotto

We have studied mesoscopic Josephson junctions formed by highly n-doped InAs nanowires and superconducting Ti/Pb source and drain leads. The current-voltage properties of the system are investigated by varying temperature and external out-of-plane magnetic field. Superconductivity in the Pb electrodes persists up to ∼7 K and with magnetic field values up to 0.4 T. Josephson coupling at zero backgate voltage is observed up to 4.5 K and the critical current is measured to be as high as 615 nA. The supercurrent suppression as a function of the magnetic field reveals a diffraction pattern that is explained by a strong magnetic flux focusing provided by the superconducting electrodes forming the junction.

http://xxx.lanl.gov/abs/1411.0990

Room temperature magnetic order on zigzag edges of narrow graphene nanoribbons

Gabor Zsolt Magda, Xiaozhan Jin, Imre Hagymasi, Peter Vancso, Zoltan Osvath, Peter Nemes-Incze, Chanyong Hwang, Laszlo P. Biro, Levente Tapaszto

Magnetic order emerging in otherwise non-magnetic materials as carbon is a paradigmatic example of a novel type of s-p electron magnetism predicted to be of exceptional high-temperature stability. It has been demonstrated that atomic scale structural defects of graphene can host unpaired spins. However, it is still unclear under which conditions long-range magnetic order can emerge from such defect-bound magnetic moments. Here we propose that in contrast to random defect distributions, atomic scale engineering of graphene edges with specific crystallographic orientation, comprising edge atoms only from one sub-lattice of the bipartite graphene lattice, can give rise to a robust magnetic order. We employ a nanofabrication technique based on Scanning Tunneling Microscopy to define graphene nanoribbons with nanometer precision and well-defined crystallographic edge orientations. While armchair ribbons display quantum confinement gap, zigzag ribbons narrower than 7 nm reveal a bandgap of about 0.2 - 0.3 eV, which can be identified as a signature of interaction induced spin ordering along their edges. Moreover, a semiconductor to metal transition is revealed upon increasing the ribbon width, indicating the switching of the magnetic coupling between opposite ribbon edges from antiferromagnetic to ferromagnetic configuration. We found that the magnetic order on graphene edges of controlled zigzag orientation can be stable even at room temperature, raising hope for graphene-based spintronic devices operating under ambient conditions.

http://xxx.lanl.gov/abs/1411.1196

Using polymer electrolyte gates to set-and-freeze threshold voltage and local potential in nanowire-based devices and thermoelectrics

Sofia Fahlvik Svensson, Adam M. Burke, Damon J. Carrad, Martin Leijnse, Heiner Linke, Adam P. Micolich

We use the strongly temperature-dependent ionic mobility in polymer electrolytes to 'freeze in' specific ionic charge environments around a nanowire using a local wrap-gate geometry. This enables us to set both the threshold voltage for a conventional doped substrate gate and the local disorder potential at temperatures below 200 Kelvin, which we characterize in detail by combining conductance and thermovoltage measurements with modeling. Our results demonstrate that local polymer electrolyte gates are compatible with nanowire thermoelectrics, where they offer the advantage of a very low thermal conductivity, and hold great potential towards setting the optimal operating point for solid-state cooling applications.

http://xxx.lanl.gov/abs/1411.2727

Revisiting the measurement of the spin relaxation time in graphene-based devices

H. Idzuchi, A. Fert, Y. Otani

A long spin relaxation time (tausf) is the key for the applications of graphene to spintronics but the experimental values of tausf have been generally much shorter than expected. We show that the usual determination by the Hanle method underestimates tausf if proper account of the spin absorption by contacts is lacking. By revisiting series of experimental results, we find that the corrected tausf are longer and less dispersed, which leads to a more unified picture of tausf derived from experiments. We also discuss how the correction depends on the parameters of the graphene and contacts.

http://xxx.lanl.gov/abs/1411.2949

Detecting nonlocal Cooper pair entanglement by optical Bell inequality violation

Simon E. Nigg, Rakesh P. Tiwari, Stefan Walter, Thomas L. Schmidt

Based on the Bardeen Cooper Schrieffer (BCS) theory of superconductivity, the coherent splitting of Cooper pairs from a superconductor to two spatially separated quantum dots has been predicted to generate nonlocal pairs of entangled electrons. In order to test this hypothesis, we propose a scheme to transfer the spin state of a split Cooper pair onto the polarization state of a pair of optical photons. We show that the produced photon pairs can be used to violate a Bell inequality, unambiguously demonstrating the entanglement of the split Cooper pairs.

http://arxiv.org/abs/1411.3945

Current noise cross correlation mediated by Majorana bound states

Hai-Feng Lu, Hai-Zhou Lu, Shun-Qing Shen

We study the transport properties of a quantum dot-Majorana hybrid system, in which each of paired Majorana bound states is connected to one quantum dot. With the help of non-equilibrium Green's function method, we obtain an exact solution of the Green's functions and calculate the currents through the quantum dots and nonlocal noise cross correlation between the currents. As a function of dot energy levels ϵ1 and ϵ2, we find that for the symmetric level configuration ϵ1=ϵ2, the noise cross correlation is negative in the low lead voltage regime, while it becomes positive with the increase of the lead voltages. Due to the particle-hole symmetry, the cross correlation is always positive in the anti-symmetric case ϵ1=−ϵ2. In contrast, the cross correlation of non-Majorana setups is always positive. For comparison, we also perform the diagonalized master equation calculation to check its applicability. It is found that the diagonalized master equations work well in most regimes of system parameters. Nevertheless, it shows an obvious deviation from the exact solution by the non-equilibrium Green's function method when all eigenenergies of the dot-Majorana hybrid system and simultaneously the energy intervals are comparable to the dot-lead coupling strength.

http://arxiv.org/abs/1411.4260

Detecting bit-flip errors in a logical qubit using stabilizer measurements

D. Ristè, S. Poletto, M.-Z. Huang, A. Bruno, V. Vesterinen, O.-P. Saira, L. DiCarlo

Quantum data is susceptible to decoherence induced by the environment and to errors in the hardware processing it. A future fault-tolerant quantum computer will use quantum error correction (QEC) to actively protect against both. In the smallest QEC codes, the information in one logical qubit is encoded in a two-dimensional subspace of a larger Hilbert space of multiple physical qubits. For each code, a set of non-demolition multi-qubit measurements, termed stabilizers, can discretize and signal physical qubit errors without collapsing the encoded information. Experimental demonstrations of QEC to date, using nuclear magnetic resonance, trapped ions, photons, superconducting qubits, and NV centers in diamond, have circumvented stabilizers at the cost of decoding at the end of a QEC cycle. This decoding leaves the quantum information vulnerable to physical qubit errors until re-encoding, violating a basic requirement for fault tolerance. Using a five-qubit superconducting processor, we realize the two parity measurements comprising the stabilizers of the three-qubit repetition code protecting one logical qubit from physical bit-flip errors. We construct these stabilizers as parallelized indirect measurements using ancillary qubits, and evidence their non-demolition character by generating three-qubit entanglement from superposition states. We demonstrate stabilizer-based quantum error detection (QED) by subjecting a logical qubit to coherent and incoherent bit-flip errors on its constituent physical qubits. While increased physical qubit coherence times and shorter QED blocks are required to actively safeguard quantum information, this demonstration is a critical step toward larger codes based on multiple parity measurements.

http://arxiv.org/abs/1411.5542

In-situ Raman Spectroscopy of the Graphene / Water Interface of a Solution-Gated Field Effect Transistor: Electron-Phonon Coupling and Spectroelectrochemistry

J. Binder, J. M. Urban, R. Stepniewski, W. Strupinski, A. Wysmolek

We present a novel measurement approach which combines aqueous solution-gated field effect transistors based on epitaxial bilayer graphene on 4H-SiC (0001) with simultaneous Raman spectroscopy. Since SiC is transparent in the visible wavelength range, we took advantage of the fact that one can measure graphene through the substrate. By sweeping the gate voltage, we observed Raman signatures related to the resonant electron-phonon coupling. The positions of these features allowed the extraction of the geometrical capacitance of the system and thus facilitated the accurate calculation of the Fermi levels for bilayer graphene. An intentional application of higher gate voltages allowed us to trigger electrochemical reactions, which we followed in-situ with Raman spectroscopy. The reactions showed a partially reversible character, which was monitored by an emergence / disappearance of peaks assigned to C-H and Si-H vibration modes as well as an increase / decrease of the defect-related Raman D band intensity. Our setup provides chemically specific information and electrical control by using a graphene solution-gated field-effect transistor and constitutes a highly interesting platform for future spectroelectrochemical research on electrically induced sorption processes of graphene in the micrometer scale.

http://arxiv.org/abs/1411.4837

Study of dynamical spin injection at ferromagnet-graphene interfaces

S. Singh, A. Ahmadi, C.T. Cherian, E. R. Mucciolo, E. del Barco, B. Özyilmaz

We present a study of dynamical spin injection from a three-dimensional ferromagnet into two-dimensional single-layer graphene. Comparative ferromagnetic resonance (FMR) studies of ferromagnet/graphene strips buried underneath the central line of a coplanar waveguide show that the FMR linewidth broadening is the largest when the graphene layer protrudes laterally away from the ferromagnetic strip, indicating that the spin current is injected into the graphene areas away from the area directly underneath the ferromagnet being excited. Our results confirm that the observed damping is indeed a signature of dynamical spin injection, wherein a pure spin current is pumped into the single-layer graphene from the precessing magnetization of the ferromagnet. The observed spin pumping efficiency is difficult to reconcile with the expected backflow of spins according to the standard spin pumping theory and the characteristics of graphene, and constitutes an enigma for spin pumping in two-dimensional structures.

http://arxiv.org/abs/1411.5339

Inverted singlet-triplet qubit coded on a two-electron double quantum dot

Sebastian Mehl and David P. DiVincenzo

The sz=0 spin configuration of two electrons confined at a double quantum dot (DQD) encodes the singlet-triplet qubit (STQ). We introduce the inverted STQ (ISTQ) that emerges from the setup of two quantum dots (QDs) differing significantly in size and out-of-plane magnetic fields. The strongly confined QD has a two-electron singlet ground state, but the weakly confined QD has a two-electron triplet ground state in the sz=0 subspace. Spin-orbit interactions act nontrivially on the sz=0 subspace and provide universal control of the ISTQ together with electrostatic manipulations of the charge configuration. GaAs and InAs DQDs can be operated as ISTQs under realistic noise conditions.

http://journals.aps.org/prb/abstract/10.1103/PhysRevB.90.195424

Majorana fermions in Ge/Si hole nanowires

Franziska Maier, Jelena Klinovaja, and Daniel Loss

We consider Ge/Si core/shell nanowires with hole states coupled to an s-wave superconductor in the presence of electric and magnetic fields. We employ a microscopic model that takes into account material-specific details of the band structure such as strong and electrically tunable Rashba-type spin-orbit interaction and g factor anisotropy for the holes. In addition, the proximity-induced superconductivity Hamiltonian is derived starting from a microscopic model. In the topological phase, the nanowires host Majorana fermions with localization lengths that depend strongly on both the magnetic and electric fields. We identify the optimal regime in terms of the directions and magnitudes of the fields in which the Majorana fermions are the most localized at the nanowire ends. In short nanowires, the Majorana fermions hybridize and form a subgap fermion whose energy is split away from zero and oscillates as a function of the applied fields. The period of these oscillations could be used to measure the dependence of the spin-orbit interaction on the applied electric field and the g factor anisotropy.

http://journals.aps.org/prb/abstract/10.1103/PhysRevB.90.195421

Revealing Topological Superconductivity in Extended Quantum Spin Hall Josephson Junctions

Shu-Ping Lee, Karen Michaeli, Jason Alicea, and Amir Yacoby

Quantum spin Hall–superconductor hybrids are promising sources of topological superconductivity and Majorana modes, particularly given recent progress on HgTe and InAs/GaSb. We propose a new method of revealing topological superconductivity in extended quantum spin Hall Josephson junctions supporting “fractional Josephson currents.” Specifically, we show that as one threads magnetic flux between the superconductors, the critical current traces an interference pattern featuring sharp fingerprints of topological superconductivity—even when noise spoils parity conservation.

http://journals.aps.org/prl/abstract/10.1103/PhysRevLett.113.197001

Axially Tunable Carbon Nanotube Resonators Using Co-integrated Microactuators

Stuart Truax , Shih-Wei Lee , Matthias Muoth , and Christofer Hierold *

Tuning of the mechanical resonance frequency of single-walled carbon nanotubes (SWCNTs) is achieved by application of uniaxial strain by purely mechanical means, utilizing both directly grown and dry-transferred SWCNTs. The induction of a beam-to-string transition is achieved, resulting in an axial tension sensitivity of 9.4 × 1010 Hz/ε in the vibrating string regime. Increases in the resonant Q-factor, removal of residual slack, and resonance frequency changes from 10 to 60 MHz are affected.

http://pubs.acs.org/doi/abs/10.1021/nl501853w

Giant Magnetoconductance Oscillations in Hybrid Superconductor−Semiconductor Core/Shell Nanowire Devices

Ö. Gül †, H. Y. Günel *†‡, H. Lüth †, T. Rieger †, T. Wenz †, F. Haas †, M. Lepsa †, G. Panaitov §, D. Grützmacher †, and Th. Schäpers *†

The magnetotransport of GaAs/InAs core/shell nanowires contacted by two superconducting Nb electrodes is investigated, where the InAs shell forms a tube-like conductive channel around the highly resistive GaAs core. By applying a magnetic field along the nanowire axis, regular magnetoconductance oscillations with an amplitude in the order of e2/h are observed. The oscillation amplitude is found to be larger by 2 orders of magnitude compared to the measurements of a reference sample with normal metal contacts. For the Nb-contacted core/shell nanowire the oscillation period corresponds to half a flux quantum Φ0/2 = h/2e in contrast to the period of Φ0 of the reference sample. The strongly enhanced magnetoconductance oscillations are explained by phase-coherent resonant Andreev reflections at the Nb-core/shell nanowire interface.

http://pubs.acs.org/doi/abs/10.1021/nl502598s

Quantum Noise and Asymmetric Scattering of Electrons and Holes in Graphene

Atikur Rahman , Janice Wynn Guikema , and Nina Marković *

We present measurements of quantum interference noise in double-gated single layer graphene devices at low temperatures. The noise characteristics show a nonmonotonic dependence on carrier density, which is related to the interplay between charge inhomogeneity and different scattering mechanisms. Linearly increasing 1/f noise at low carrier densities coincides with the observation of weak localization, suggesting the importance of short-range disorder in this regime. Using perpendicular and parallel p–n junctions, we find that the observed asymmetry of the noise with respect to the Dirac point can be related to asymmetric scattering of electrons and holes on the disorder potential.

http://pubs.acs.org/doi/abs/10.1021/nl503276s

Multimode Silicon Nanowire Transistors

Sebastian Glassner †, Clemens Zeiner †, Priyanka Periwal ‡§, Thierry Baron ‡§, Emmerich Bertagnolli †, and Alois Lugstein *†

The combined capabilities of both a nonplanar design and nonconventional carrier injection mechanisms are subject to recent scientific investigations to overcome the limitations of silicon metal oxide semiconductor field effect transistors. In this Letter, we present a multimode field effect transistors device using silicon nanowires that feature an axial n-type/intrinsic doping junction. A heterostructural device design is achieved by employing a self-aligned nickel-silicide source contact. The polymorph operation of the dual-gate device enabling the configuration of one p- and two n-type transistor modes is demonstrated. Not only the type but also the carrier injection mode can be altered by appropriate biasing of the two gate terminals or by inverting the drain bias. With a combined band-to-band and Schottky tunneling mechanism, in p-type mode a subthreshold swing as low as 143 mV/dec and an ON/OFF ratio of up to 104 is found. As the device operates in forward bias, a nonconventional tunneling transistor is realized, enabling an effective suppression of ambipolarity. Depending on the drain bias, two different n-type modes are distinguishable. The carrier injection is dominated by thermionic emission in forward bias with a maximum ON/OFF ratio of up to 107 whereas in reverse bias a Schottky tunneling mechanism dominates the carrier transport.

http://pubs.acs.org/doi/abs/10.1021/nl503476t

Realization of the Meminductor

Jiahao Han , Cheng Song *, Shuang Gao , Yuyan Wang , Chao Chen , and Feng Pan

The meminductor was proposed to be a fundamental circuit memdevice parallel with the memristor, linking magnetic flux and current. However, a clear material model or experimental realization of a meminductor has been challenging. Here we demonstrate pinched hysteretic magnetic flux–current signals at room temperature based on the spin Hall magnetoresistance effect in several-nanometer-thick thin films, exhibiting the nonvolatile memorizing property and magnetic energy storage ability of the meminductor. Similar to the parameters of the capacitor, resistor, and inductor, meminductance, LM, is introduced to characterize the capability of the prepared meminductor. Our findings present an indispensable element of memdevices and open an avenue for nanoscale meminductor design and manufacture, which might contribute to low-power electronic circuits, information storage, and artificial intelligence.

http://pubs.acs.org/doi/abs/10.1021/nn502655u

Szept.19-30.

Márton Attila

Előadás: SNS junctions in nanowires with spin-orbit coupling: role of confinement and helicity on the sub-gap spectrum (http://arxiv.org/abs/1410.6074) pptx (pptx)

Photons made to dance together

Physicists have made two beams of light interact at the level of individual photons.

Getting photons to interact is important for all-optical computation and for producing new quantum states of light. Kristin Beck at the Massachusetts Institute of Technology in Cambridge and her colleagues crossed two beams of light inside a cavity filled with trapped and cooled caesium atoms. When photons from each beam tried to pass through the system at the same time, the trapped atoms changed their internal state, allowing only one photon to be transmitted, while the other one was reflected or scattered.

The interaction creates two entangled beams of light, which the authors say could eventually be used to improve the accuracy of measurements, such as of a gyroscope's rotation, that would otherwise be limited by the laws of quantum mechanics.

http://www.nature.com/nature/journal/v513/n7519/full/513463a.html

Quantum bits get their first compression

Without algorithms that compress data to encode information into fewer bits, hard drives would clog up and Internet traffic would slow to a snail's pace. Now, a group of physicists in Canada has shown for the first time that it is possible to compress the kind of data that might be used in the computers of tomorrow — known as quantum bits, or qubits.

http://www.nature.com/news/quantum-bits-get-their-first-compression-1.15961

Transmission Phase in the Kondo Regime Revealed in a Two-Path Interferometer

S. Takada, C. Bäuerle, M. Yamamoto, K. Watanabe, S. Hermelin, T. Meunier, A. Alex, A. Weichselbaum, J. von Delft, A. Ludwig, A. D. Wieck, and S. Tarucha

We report on the direct observation of the transmission phase shift through a Kondo correlated quantum dot by employing a new type of two-path interferometer. We observed a clear π/2-phase shift, which persists up to the Kondo temperature TK. Above this temperature, the phase shifts by more than π/2 at each Coulomb peak, approaching the behavior observed for the standard Coulomb blockade regime. These observations are in remarkable agreement with two-level numerical renormalization group calculations. The unique combination of experimental and theoretical results presented here fully elucidates the phase evolution in the Kondo regime.

http://journals.aps.org/prl/abstract/10.1103/PhysRevLett.113.126601

Entanglement Entropy in Fermi Gases and Anderson’s Orthogonality Catastrophe

A. Ossipov

We study the ground-state entanglement entropy of a finite subsystem of size L of an infinite system of noninteracting fermions scattered by a potential of finite range a. We derive a general relation between the scattering matrix and the overlap matrix and use it to prove that for a one-dimensional symmetric potential the von Neumann entropy, the Rényi entropies, and the full counting statistics are robust against potential scattering, provided that L/a≫1. The results of numerical calculations support the validity of this conclusion for a generic potential.

http://journals.aps.org/prl/abstract/10.1103/PhysRevLett.113.130402

Experimental realization of a Coulomb blockade refrigerator

A. V. Feshchenko, J. V. Koski, J. P. Pekola

We present an experimental realization of a Coulomb blockade refrigerator (CBR) based on a single - electron transistor (SET). In the present structure, the SET island is interrupted by a superconducting inclusion to permit charge transport while preventing heat flow. At certain values of the bias and gate voltages, the current through the SET cools one of the junctions. The measurements follow theoretical model down to about 80 mK, which was the base temperature of the current measurements. The observed cooling increases rapidly with decreasing temperature in agreement with the theory, reaching about 15 mK drop at the base temperature. CBR appears as a promising electronic cooler at temperatures well below 100 mK.

http://xxx.lanl.gov/abs/1409.5637

Klein-tunneling transistor with ballistic graphene

Quentin Wilmart, Salim Berada, David Torrin, V. Hung Nguyen, Gwendal Fève, Jean-Marc Berroir, Philippe Dollfus, Bernard Plaçais

Today the availability of high mobility graphene up to room temperature makes ballistic transport in nanodevices achievable. In particular, p-n-p transistor in the ballistic regime gives access to the Klein tunneling physics and allows the realization of devices exploiting the optics-like behavior of Dirac Fermions (DF) as in the Vesalego lens or the Fabry P\'erot cavity. Here we propose a Klein tunneling transistor based on geometrical optics of DF. We consider the case of a prismatic active region delimited by a triangular gate, where total internal reflection may occur, which leads to the tunable suppression of the transistor transmission. We calculate the transmission and the current by means of scattering theory and the finite bias properties using Non Equilibrium Green's Function(NEGF) simulation.

http://xxx.lanl.gov/abs/1409.6170

Directly accessible entangling gates for capacitively coupled singlet-triplet qubits

Fernando A. Calderon-Vargas, Jason P. Kestner

The recent experimental advances in capacitively coupled singlet-triplet qubits, particularly the demonstration of entanglement, opens the question of what type of entangling gates the system's Hamiltonian can produce directly via a single square pulse. We address this question by considering the system's Hamiltonian from first principles and using the representation of its nonlocal properties in terms of local invariants. In the analysis we include the three different ways in which the system can be biased and their effect on the generation of entangling gates. We find that, in one of the possible biasing modes, the Hamiltonian has an especially simple form, which can directly generate a wide range of different entangling gates including the iSWAP gate. Moreover, using the complete form of the Hamiltonian we find that, for any biasing mode, a CNOT gate can be generated directly.

http://xxx.lanl.gov/abs/1409.6292

Zeeman splitting spin filter in a single quantum dot electron transport with Coulomb blockade effect

Wenxi Lai

Electron spin filter induced by Zeeman splitting in a few-electron quantum dot coupled to two normal electrodes is studied considering Coulomb blockade effect. Based on the Anderson model and Liouville-von Neumann equation, equation of motion of the system is derived and analytical solutions are achieved. Transport windows for perfectly polarized current, partially polarized current and non-polarized current induced by the Zeeman splitting energy and Coulomb blockade potential are exploited. We will give the relations of voltage, magnetic field and temperature for high quality spin filtering.

http://xxx.lanl.gov/abs/1409.6389

Majorana bound states without topological superconductivity

Pablo San-Jose, Jorge Cayao, Elsa Prada, Ramón Aguado

Recent experimental efforts towards the detection of Majorana bound states have focused on creating the conditions for topological superconductivity. Here we demonstrate an alternative route, which achieves fully localised zero-energy Majorana bound states when a topologically trivial superconductor is opened to a normal region. The emergence of Majorana states is a consequence of non-hermitian degeneracies of the resulting open quantum system, while arbitrarily large Majorana lifetimes follow from high junction transparency and helicity of the normal side. At these degeneracies, also known as `exceptional points', both the eigenvalues and the eigenstates coalesce, and acquire Majorana properties (zero-energy, self-conjugation, 4π-periodic braiding...) despite the trivial band topology. Exceptional Majoranas are thus the open-system counterparts of conventional Majorana bound states, to which they are continuously connected, and exhibit all their phenomenology while not requiring topological superconductivity.

http://xxx.lanl.gov/abs/1409.7306

Majorana Fermions in Ge/Si Hole Nanowires

Franziska Maier, Jelena Klinovaja, Daniel Loss

We consider Ge/Si core/shell nanowires with hole states coupled to an s-wave superconductor in the presence of electric and magnetic fields. We employ a microscopic model that takes into account material-specific details of the band structure such as strong and electrically tunable Rashba-type spin-orbit interaction and g factor anisotropy for the holes. In addition, the proximity-induced superconductivity Hamiltonian is derived starting from a microscopic model. In the topological phase, the nanowires host Majorana fermions with localization lengths that depend strongly on both the magnetic and electric fields. We identify the optimal regime in terms of the directions and magnitudes of the fields in which the Majorana fermions are the most localized at the nanowire ends. In short nanowires, the Majorana fermions hybridize and form a subgap fermion whose energy is split away from zero and oscillates as a function of the applied fields. The period of these oscillations could be used to measure the dependence of the spin-orbit interaction on the applied electric field and the g factor anisotropy.

http://xxx.lanl.gov/abs/1409.8645

Szept.13-19.

Tóvári Endre

Crossover from Josephson Effect to Single Interface Andreev Reflection in Asymmetric Superconductor/Nanowire Junctions

'H. Y. Günel, N. Borgwardt, I. E. Batov, H. Hardtdegen, K. Sladek, G. Panaitov, D. Grützmacher, and Th. Schäpers'

We report on the fabrication and characterization of symmetric nanowire-based Josephson junctions, that is, Al- and Nb-based junctions, and asymmetric junctions employing superconducting Al and Nb. In the symmetric junctions, a clear and pronounced Josephson supercurrent is observed. These samples also show clear signatures of subharmonic gap structures. At zero magnetic field, a Josephson coupling is found for the asymmetric Al/InAs-nanowire/Nb junctions as well. By applying a magnetic field above the critical field of Al or by raising the temperature above the critical temperature of Al the junction can be switched to an effective single-interface superconductor/nanowire structure. In this regime, a pronounced zero-bias conductance peak due to reflectionless tunneling has been observed.

http://pubs.acs.org/doi/abs/10.1021/nl501350v

Robust Electron Pairing in the Integer Quantum Hall Effect Regime

'Hyungkook Choi, Itamar Sivan, Amir Rosenblatt, Moty Heiblum, Vladimir Umansky, Diana Mahalu'

Electron pairing is a rare phenomenon appearing only in a few unique physical systems; e.g., superconductors and Kondo-correlated quantum dots. Here, we report on an unexpected, but robust, electron "pairing" in the integer quantum Hall effect (IQHE) regime. The pairing takes place within an interfering edge channel circulating in an electronic Fabry-Perot interferometer at a wide range of bulk filling factors, 2<νB<5. The main observations are: (a) High visibility Aharonov-Bohm conductance oscillations with magnetic flux periodicity Δϕ=φ0/2=h/2e (instead of the ubiquitous h/e), with e the electron charge and h the Planck constant; (b) An interfering quasiparticle charge e∗∼2e - revealed by quantum shot noise measurements; and (c) Full dephasing of the h/2e periodicity by induced dephasing of the adjacent edge channel (while keeping the interfering edge channel intact) : a clear realization of inter-channel entanglement. While this pairing phenomenon clearly results from inter-channel interaction, the exact mechanism that leads to e-e attraction within a single edge channel is not clear.

http://xxx.lanl.gov/abs/1409.4427

Robust 2D Topological Insulators in van der Waals Heterostructures

'Liangzhi Kou, Shu-Chun Wu, Claudia Felser, Thomas Frauenheim, Changfeng Chen, and Binghai Yan'

We predict a family of robust two-dimensional (2D) topological insulators in van der Waals heterostructures comprising graphene and chalcogenides BiTeX (X = Cl, Br, and I). The layered structures of both constituent materials produce a naturally smooth interface that is conducive to proximity-induced topological states. First-principles calculations reveal intrinsic topologically nontrivial bulk energy gaps as large as 70–80 meV, which can be further enhanced up to 120 meV by compression. The strong spin–orbit coupling in BiTeX has a significant influence on the graphene Dirac states, resulting in the topologically nontrivial band structure, which is confirmed by calculated nontrivial Z2 index and an explicit demonstration of metallic edge states. Such heterostructures offer a unique Dirac transport system that combines the 2D Dirac states from graphene and 1D Dirac edge states from the topological insulator, and it offers ideas for innovative device designs.

http://pubs.acs.org/doi/abs/10.1021/nn503789v

Pseudospin-driven spin relaxation mechanism in graphene

'Dinh Van Tuan, Frank Ortmann, David Soriano, Sergio O. Valenzuela & Stephan Roche'

The prospect of transporting spin information over long distances in graphene, possible because of its small intrinsic spin–orbit coupling (SOC) and vanishing hyperfine interaction, has stimulated intense research exploring spintronics applications. However, measured spin relaxation times are orders of magnitude smaller than initially predicted, while the main physical process for spin dephasing and its charge-density and disorder dependences remain unconvincingly described by conventional mechanisms. Here, we unravel a spin relaxation mechanism for non-magnetic samples that follows from an entanglement between spin and pseudospin driven by random SOC, unique to graphene. The mixing between spin and pseudospin-related Berry’s phases results in fast spin dephasing even when approaching the ballistic limit, with increasing relaxation times away from the Dirac point, as observed experimentally. The SOC can be caused by adatoms, ripples or even the substrate, suggesting novel spin manipulation strategies based on the pseudospin degree of freedom.

http://www.nature.com/nphys/journal/vaop/ncurrent/full/nphys3083.html

Observation of topological surface state quantum Hall effect in an intrinsic three-dimensional topological insulator

'Yang Xu, Ireneusz Miotkowski, Chang Liu, Jifa Tian, Hyoungdo Nam, Nasser Alidoust, Jiuning Hu, Chih-Kang Shih, M. Zahid Hasan, Yong P. Chen'

A three-dimensional (3D) topological insulator (TI) is a quantum state of matter with a gapped insulating bulk yet a conducting surface hosting topologically-protected gapless surface states. One of the most distinct electronic transport signatures predicted for such topological surface states (TSS) is a well-defined half-integer quantum Hall effect (QHE) in a magnetic field, where the surface Hall conductivities become quantized in units of (1/2)e2/h (e being the electron charge, h the Planck constant) concomitant with vanishing resistance. Here, we observe well-developed QHE arising from TSS in an intrinsic TI of BiSbTeSe2. Our samples exhibit surface dominated conduction even close to room temperature, while the bulk conduction is negligible. At low temperatures and high magnetic fields perpendicular to the top and bottom surfaces, we observe well-developed integer quantized Hall plateaus, where the two parallel surfaces each contributing a half integer e2/h quantized Hall (QH) conductance, accompanied by vanishing longitudinal resistance. When the bottom surface is gated to match the top surface in carrier density, only odd integer QH plateaus are observed, representing a half-integer QHE of two degenerate Dirac gases. This system provides an excellent platform to pursue a plethora of exotic physics and novel device applications predicted for TIs, ranging from magnetic monopoles and Majorana particles to dissipationless electronics and fault-tolerant quantum computers.

http://xxx.lanl.gov/abs/1409.3778

MoS2: a Choice Substrate for Accessing and Tuning the Electronic Properties of Graphene

'Chih-Pin Lu, Guohong Li, K. Watanabe, T. Taniguchi, Eva Y. Andrei'

One of the enduring challenges in graphene research and applications is the extreme sensitivity of its charge carriers to external perturbations, especially those introduced by the substrate. The best available substrates to date, graphite and hBN, still pose limitations: graphite being metallic does not allow gating, while both hBN and graphite having lattice structures closely matched to that of graphene, may cause significant band structure reconstruction. Here we show that the atomically smooth surface of exfoliated MoS2 provides access to the intrinsic electronic structure of graphene without these drawbacks. Using scanning tunneling microscopy and Landau-level spectroscopy in a device configuration which allows tuning the carrier concentration, we find that graphene on MoS2 is ultra-flat producing long mean free paths, while avoiding band structure reconstruction. Importantly, the screening of the MoS2 substrate can be tuned by changing the position of the Fermi energy with relatively low gate voltages. We show that shifting the Fermi energy from the gap to the edge of the conduction band gives rise to enhanced screening and to a substantial increase in the mean-free-path and quasiparticle lifetime. MoS2 substrates thus provide unique opportunities to access the intrinsic electronic properties of graphene and to study in situ the effects of screening on electron-electron interactions and transport.

http://xxx.lanl.gov/abs/1409.5179

Aharonov-Bohm Oscillations in a Quasi-Ballistic 3D Topological Insulator Nanowire

'S. Cho, B. Dellabetta, R. D. Zhong, J. Schneeloch, T. S. Liu, G. Gu, Matthew J. Gilbert, Nadya Mason'

In three-dimensional topological insulators (3D TI) nanowires, transport occurs via gapless surface states where the spin is fixed perpendicular to the momentum[1-6]. Carriers encircling the surface thus acquire a \pi Berry phase, which is predicted to open up a gap in the lowest-energy 1D surface subband. Inserting a magnetic flux ({\Phi}) of h/2e through the nanowire should cancel the Berry phase and restore the gapless 1D mode[7-8]. However, this signature has been missing in transport experiments reported to date[9-11]. Here, we report measurements of mechanically-exfoliated 3D TI nanowires which exhibit Aharonov-Bohm oscillations consistent with topological surface transport. The use of low-doped, quasi-ballistic devices allows us to observe a minimum conductance at {\Phi} = 0 and a maximum conductance reaching e^2/h at {\Phi} = h/2e near the lowest subband (i.e. the Dirac point), as well as the carrier density dependence of the transport.

http://xxx.lanl.gov/abs/1409.5095

Experimental Realization of a Three-Dimensional Dirac Semimetal

'Sergey Borisenko, Quinn Gibson, Danil Evtushinsky, Volodymyr Zabolotnyy, Bernd Büchner, and Robert J. Cava'

We report the direct observation of the three-dimensional (3D) Dirac semimetal phase in cadmium arsenide (Cd3As2) by means of angle-resolved photoemission spectroscopy. We identify two momentum regions where electronic states that strongly disperse in all directions form narrow conelike structures, and thus prove the existence of the long sought 3D Dirac points. This electronic structure naturally explains why Cd3As2 has one of the highest known bulk electron mobilities. This realization of a 3D Dirac semimetal in Cd3As2 not only opens a direct path to a wide spectrum of applications, but also offers a robust platform for engineering topologically nontrivial phases including Weyl semimetals and quantum spin Hall systems.

http://journals.aps.org/prl/abstract/10.1103/PhysRevLett.113.027603

Terahertz Generation by Dynamical Photon Drag Effect in Graphene Excited by Femtosecond Optical Pulses

'J. Maysonnave, S. Huppert, F. Wang, S. Maero, C. Berger, W. de Heer, T. B. Norris, L. A. De Vaulchier, S. Dhillon, J. Tignon, R. Ferreira, and J. Mangeney'

Graphene has been proposed as a particularly attractive material for the achievement of strong optical nonlinearities, in particular generation of terahertz radiation. However, owing to the particular symmetries of the C-lattice, second-order nonlinear effects such as difference-frequency or rectification processes are predicted to vanish in a graphene layer for optical excitations (ℏω ≫ 2EF) involving the two relativistic dispersion bands. Here we experimentally demonstrate that graphene excited by femtosecond optical pulses generate a coherent THz radiation ranging from 0.1 to 4 THz via a second-order nonlinear effect. We fully interpret its characteristics with a model describing the electron and hole states beyond the usual massless relativistic scheme. This second-order nonlinear effect is dynamical photon drag, which relies on the transfer of light momentum to the carriers by the ponderomotive electric and magnetic forces. The model highlights the key roles of next-C-neighbor couplings and of unequal electron and hole lifetimes in the observed second-order response. Finally, our results indicate that dynamical photon drag effect in graphene can provide emission up to 60 THz, opening new routes for the generation of ultrabroadband terahertz pulses.

http://pubs.acs.org/doi/abs/10.1021/nl502684j

Exceptional Charge Transport Properties of Graphene on Germanium

'Francesca Cavallo, Richard Rojas Delgado, Michelle M. Kelly, José R. Sánchez Pérez, Daniel P. Schroeder, Huili Grace Xing, Mark A. Eriksson, and Max G. Lagally'

The excellent charge transport properties of graphene suggest a wide range of application in analog electronics. While most practical devices will require that graphene be bonded to a substrate, such bonding generally degrades these transport properties. In contrast, when graphene is transferred to Ge(001) its conductivity is extremely high and the charge carrier mobility derived from the relevant transport measurements is, under some circumstances, higher than that of freestanding, edge-supported graphene. We measure a mobility of ∼5 × 105 cm2 V–1 s–1 at 20 K, and ∼103 cm2 V–1 s–1 at 300 K. These values are close to the theoretical limit for doped graphene. Carrier densities in the graphene are as high as 1014 cm–2 at 300 K.

http://pubs.acs.org/doi/abs/10.1021/nn503381m

Direct Laser Writing of Graphene Electronics

http://pubs.acs.org/doi/abs/10.1021/nn504946k

Room-temperature coupling between electrical current and nuclear spins in OLEDs

'H. Malissa, M. Kavand, D. P. Waters, K. J. van Schooten, P. L. Burn, Z. V. Vardeny, B. Saam, J. M. Lupton, C. Boehme'

The effects of external magnetic fields on the electrical conductivity of organic semiconductors have been attributed to hyperfine coupling of the spins of the charge carriers and hydrogen nuclei. We studied this coupling directly by implementation of pulsed electrically detected nuclear magnetic resonance spectroscopy in organic light-emitting diodes (OLEDs). The data revealed a fingerprint of the isotope (protium or deuterium) involved in the coherent spin precession observed in spin-echo envelope modulation. Furthermore, resonant control of the electric current by nuclear spin orientation was achieved with radiofrequency pulses in a double-resonance scheme, implying current control on energy scales one-millionth the magnitude of the thermal energy.

http://www.sciencemag.org/content/345/6203/1487

Large, non-saturating magnetoresistance in WTe2

'Mazhar N. Ali, Jun Xiong, Steven Flynn, Jing Tao, Quinn D. Gibson, Leslie M. Schoop, Tian Liang, Neel Haldolaarachchige, Max Hirschberger, N. P. Ong & R. J. Cava'

Magnetoresistance is the change in a material’s electrical resistance in response to an applied magnetic field. Materials with large magnetoresistance have found use as magnetic sensors1, in magnetic memory2, and in hard drives3 at room temperature, and their rarity has motivated many fundamental studies in materials physics at low temperatures4. Here we report the observation of an extremely large positive magnetoresistance at low temperatures in the non-magnetic layered transition-metal dichalcogenide WTe2: 452,700 per cent at 4.5 kelvins in a magnetic field of 14.7 teslas, and 13 million per cent at 0.53 kelvins in a magnetic field of 60 teslas. In contrast with other materials, there is no saturation of the magnetoresistance value even at very high applied fields. Determination of the origin and consequences of this effect, and the fabrication of thin films, nanostructures and devices based on the extremely large positive magnetoresistance of WTe2, will represent a significant new direction in the study of magnetoresistivity.

http://www.nature.com/nature/journal/vaop/ncurrent/full/nature13763.html

Fast non-thermal switching between macroscopic charge-ordered quantum states induced by charge injection

'I. Vaskivskyi, I. A. Mihailovic, S. Brazovskii, J. Gospodaric, T. Mertelj, D. Svetin, P. Sutar, D. Mihailovic'

The functionality of logic and memory elements in current electronics is based on multi-stability, driven either by manipulating local concentrations of electrons in transistors, or by switching between equivalent states of a material with a degener- ate ground state in magnetic or ferroelectric materials. Another possibility is offered by phase transitions with switching between metallic and insulating phases, but classical phase transitions are limited in speed by slow nucleation, proliferation of domains and hysteresis. We can in principle avoid these problems by using quantum states for switching, but microscopic systems suffer from decoherence which prohibits their use in everyday devices. Macroscopic quantum states, such as the superconducting ground state have the advantage that on a fundamental level they do not suffer from decoherence plaguing microscopic systems. Here we demonstrate for the first time ultrafast non-thermal switching between different metastable electronically ordered states by pulsed electrical charge injection. The macroscopic nature of the many-body quantum states(1-4) - which are not part of the equilibrium phase diagram - gives rise to unprecedented stability and remarka- bly sharp switching thresholds. Fast sub-50 ps switching, large associated re- sistance changes, 2-terminal operation and demonstrable high fidelity of bi-stability control suggest new opportunities for the use of macroscopic quantum states in electronics, particularly for an ultrafast non-volatile quantum charge-order resistive random access memory (QCOR-RAM).

http://xxx.lanl.gov/abs/1409.3794

Imaging the two-component nature of Dirac–Landau levels in the topological surface state of Bi2Se3

'Ying-Shuang Fu, M. Kawamura, K. Igarashi, H. Takagi, T. Hanaguri & T. Sasagawa'

Massless Dirac electrons in condensed matter1, 2, 3, 4, 5, 6 are, unlike conventional electrons, described by two-component wavefunctions associated with the spin degrees of freedom in the surface state of topological insulators5, 6. Hence, the ability to observe the two-component wavefunction is useful for exploring novel spin phenomena. Here we show that the two-component nature is manifest in Landau levels, the degeneracy of which is lifted by a Coulomb potential. Using spectroscopic-imaging scanning tunnelling microscopy, we visualize energy and spatial structures of Landau levels in Bi2Se3, a prototypical topological insulator. The observed Landau-level splitting and internal structures of Landau orbits are distinct from those in a conventional electron system7 and are well reproduced by a two-component model Dirac Hamiltonian. Our model further predicts energy-dependent spin-magnetization textures in a potential variation and provides a way for manipulating spins in the topological surface state.

http://www.nature.com/nphys/journal/vaop/ncurrent/full/nphys3084.html

Ultrafast non-local control of spontaneous emission

http://www.nature.com/nnano/journal/vaop/ncurrent/full/nnano.2014.190.html

http://www.sciencedirect.com/science/article/pii/S0008622314007465

http://journals.aps.org/prb/abstract/10.1103/PhysRevB.90.125428

For fun:

Spraying Quantum Dot Conjugates in the Colon of Live Animals Enabled Rapid and Multiplex Cancer Diagnosis Using Endoscopy

http://pubs.acs.org/doi/abs/10.1021/nn5009269

Szept.2-12.

Tóvári Endre

Fabry-Pérot Interference in Gapped Bilayer Graphene with Broken Anti-Klein Tunneling

'Anastasia Varlet, Ming-Hao Liu (劉明豪), Viktor Krueckl, Dominik Bischoff, Pauline Simonet, Kenji Watanabe, Takashi Taniguchi, Klaus Richter, Klaus Ensslin, and Thomas Ihn'

We report the experimental observation of Fabry-Pérot interference in the conductance of a gate-defined cavity in a dual-gated bilayer graphene device. The high quality of the bilayer graphene flake, combined with the device’s electrical robustness provided by the encapsulation between two hexagonal boron nitride layers, allows us to observe ballistic phase-coherent transport through a 1−μm-long cavity. We confirm the origin of the observed interference pattern by comparing to tight-binding calculations accounting for the gate-tunable band gap. The good agreement between experiment and theory, free of tuning parameters, further verifies that a gap opens in our device. The gap is shown to destroy the perfect reflection for electrons traversing the barrier with normal incidence (anti-Klein tunneling). The broken anti-Klein tunneling implies that the Berry phase, which is found to vary with the gate voltages, is always involved in the Fabry-Pérot oscillations regardless of the magnetic field, in sharp contrast with single-layer graphene.

http://journals.aps.org/prl/abstract/10.1103/PhysRevLett.113.116601

Anomalous Sequence of Quantum Hall Liquids Revealing a Tunable Lifshitz Transition in Bilayer Graphene

'Anastasia Varlet, Dominik Bischoff, Pauline Simonet, Kenji Watanabe, Takashi Taniguchi, Thomas Ihn, Klaus Ensslin, Marcin Mucha-Kruczyński, and Vladimir I. Fal’ko'

Bilayer graphene is a unique system where both the Fermi energy and the low-energy electron dispersion can be tuned. This is brought about by an interplay between trigonal warping and the band gap opened by a transverse electric field. Here, we drive the Lifshitz transition in bilayer graphene to experimentally controllable carrier densities by applying a large transverse electric field to a h-BN-encapsulated bilayer graphene structure. We perform magnetotransport measurements and investigate the different degeneracies in the Landau level spectrum. At low magnetic fields, the observation of filling factors −3 and −6 quantum Hall states reflects the existence of three maxima at the top of the valence-band dispersion. At high magnetic fields, all integer quantum Hall states are observed, indicating that deeper in the valence band the constant energy contours are singly connected. The fact that we observe ferromagnetic quantum Hall states at odd-integer filling factors testifies to the high quality of our sample. This enables us to identify several phase transitions between correlated quantum Hall states at intermediate magnetic fields, in agreement with the calculated evolution of the Landau level spectrum. The observed evolution of the degeneracies, therefore, reveals the presence of a Lifshitz transition in our system.

http://journals.aps.org/prl/abstract/10.1103/PhysRevLett.113.116602

Characterizing wave functions in graphene nanodevices: Electronic transport through ultrashort graphene constrictions on a boron nitride substrate

'D. Bischoff, F. Libisch, J. Burgdörfer, T. Ihn, and K. Ensslin'

We present electronic transport measurements through short and narrow (30×30nm) single-layer graphene constrictions on a hexagonal boron nitride substrate. While the general observation of Coulomb blockade is compatible with earlier work, the details are not: We show that the area on which charge is localized can be significantly larger than the area of the constriction, suggesting that the localized states responsible for the Coulomb blockade leak out into the graphene bulk. The high bulk mobility of graphene on hexagonal boron nitride, however, seems to be inconsistent with the short bulk localization length required to see Coulomb blockade. To explain these findings, charge must instead be primarily localized along the imperfect edges of the devices and extend along the edge outside of the constriction. In order to better understand the mechanisms, we compare the experimental findings with tight-binding simulations of such constrictions with disordered edges. Finally, we discuss previous experiments in the light of our findings.

http://journals.aps.org/prb/abstract/10.1103/PhysRevB.90.115405

Twist-controlled resonant tunnelling in graphene/boron nitride/graphene heterostructures

'A. Mishchenko, J. S. Tu, Y. Cao, R. V. Gorbachev, J. R. Wallbank, M. T. Greenaway, V. E. Morozov, S. V. Morozov, M. J. Zhu, S. L. Wong, F. Withers, C. R. Woods, Y-J. Kim, K. Watanabe, T. Taniguchi, E. E. Vdovin, O. Makarovsky, T. M. Fromhold, V. I. Fal'ko, A. K. Geim, L. Eaves & K. S. Novoselov'

Recent developments in the technology of van der Waals heterostructures1, 2 made from two-dimensional atomic crystals3, 4 have already led to the observation of new physical phenomena, such as the metal–insulator transition5 and Coulomb drag6, and to the realization of functional devices, such as tunnel diodes7, 8, tunnel transistors9, 10 and photovoltaic sensors11. An unprecedented degree of control of the electronic properties is available not only by means of the selection of materials in the stack12, but also through the additional fine-tuning achievable by adjusting the built-in strain and relative orientation of the component layers13, 14, 15, 16, 17. Here we demonstrate how careful alignment of the crystallographic orientation of two graphene electrodes separated by a layer of hexagonal boron nitride in a transistor device can achieve resonant tunnelling with conservation of electron energy, momentum and, potentially, chirality. We show how the resonance peak and negative differential conductance in the device characteristics induce a tunable radiofrequency oscillatory current that has potential for future high-frequency technology.

http://www.nature.com/nnano/journal/vaop/ncurrent/full/nnano.2014.187.html

Resistance-voltage dependence of nanojunctions during electromigration in ultrahigh vacuum

'D. Stöffler, M. Marz, B. Kießig, T. Tomanic, R. Schäfer, H. v. Löhneysen, and R. Hoffmann-Vogel'

The electrical resistance R of metallic nanocontacts subjected to controlled cyclic electromigration in ultrahigh vacuum has been investigated in situ as a function of applied voltage V. For sufficiently small contacts, i.e., large resistance, a decrease of R(V) while increasing V is observed. This effect is tentatively attributed to the presence of contacts separated by thin vacuum barriers in parallel to ohmic nanocontacts. Simple model calculations indicate that both thermal activation or tunneling can lead to this unusual behavior. We describe our data by a tunneling model whose key parameter, i.e., the tunneling distance, changes because of thermal expansion due to Joule heating and/or electrostatic strain arising from the applied voltage. Oxygen exposure during electromigration prevents the formation of negative R(V) slopes, and at the same time enhances the probability of uncontrolled melting, while other gases show little effects. In addition, indication for field emission has been observed in some samples.

http://journals.aps.org/prb/abstract/10.1103/PhysRevB.90.115406

Quantum interference in off-resonant transport through single molecules

'Kim G. L. Pedersen, Mikkel Strange, Martin Leijnse, Per Hedegård, Gemma C. Solomon, and Jens Paaske'

We provide a simple set of rules for predicting interference effects in off-resonant transport through single molecule junctions. These effects fall into two classes, showing, respectively, an odd or an even number of nodes in the linear conductance within a given molecular charge state, and we demonstrate how to decide the interference class directly from the contacting geometry. For neutral alternant hydrocarbons, we employ the Coulson-Rushbrooke-McLachlan pairing theorem to show that the interference class is decided simply by tunneling on and off the molecule from same or different sublattices. More generally, we investigate a range of smaller molecules by means of exact diagonalization combined with a perturbative treatment of the molecule-lead tunnel coupling. While these results generally agree well with GW calculations, they are shown to be at odds with simpler mean-field treatments. For molecules with spin-degenerate ground states, we show that for most junctions interference causes no transmission nodes, but we argue that it may lead to a nonstandard gate dependence of the zero-bias Kondo resonance.

http://journals.aps.org/prb/abstract/10.1103/PhysRevB.90.125413

All-optical control of ferromagnetic thin films and nanostructures

'C-H. Lambert, S. Mangin, B. S. D. Ch. S. Varaprasad, Y. K. Takahashi, M. Hehn, M. Cinchetti, G. Malinowski, K. Hono, Y. Fainman, M. Aeschlimann, E. E. Fullerton'

The interplay of light and magnetism allowed light to be used as a probe of magnetic materials. Now the focus has shifted to use polarized light to alter or manipulate magnetism. Here, we demonstrate optical control of ferromagnetic materials ranging from magnetic thin films to multilayers and even granular films being explored for ultra-high-density magnetic recording. Our finding shows that optical control of magnetic materials is a much more general phenomenon than previously assumed and may have a major impact on data memory and storage industries through the integration of optical control of ferromagnetic bits.

http://www.sciencemag.org/content/345/6202/1337

Ultrafast optical control of orbital and spin dynamics in a solid-state defect

'Lee C. Bassett, F. Joseph Heremans, David J. Christle, Christopher G. Yale, Guido Burkard, Bob B. Buckley, David D. Awschalom'

Atom-scale defects in semiconductors are promising building blocks for quantum devices, but our understanding of their material-dependent electronic structure, optical interactions, and dissipation mechanisms is lacking. Using picosecond resonant pulses of light, we study the coherent orbital and spin dynamics of a single nitrogen-vacancy center in diamond over time scales spanning six orders of magnitude. We develop a time-domain quantum tomography technique to precisely map the defect’s excited-state Hamiltonian and exploit the excited-state dynamics to control its ground-state spin with optical pulses alone. These techniques generalize to other optically addressable nanoscale spin systems and serve as powerful tools to characterize and control spin qubits for future applications in quantum technology.

http://www.sciencemag.org/content/345/6202/1333

Environment-assisted quantum control of a solid-state spin via coherent dark states

'Jack Hansom, Carsten H. H. Schulte, Claire Le Gall, Clemens Matthiesen, Edmund Clarke, Maxime Hugues, Jacob M. Taylor & Mete Atatüre'

Understanding the interplay between a quantum system and its environment lies at the heart of quantum science and its applications. So far most efforts have focused on circumventing decoherence induced by the environment by either protecting the system from the associated noise1, 2, 3, 4, 5 or by manipulating the environment directly6, 7, 8, 9. Recently, parallel efforts using the environment as a resource have emerged, which could enable dissipation-driven quantum computation and coupling of distant quantum bits10, 11, 12, 13, 14. Here, we realize the optical control of a semiconductor quantum-dot spin by relying on its interaction with an adiabatically evolving spin environment. The emergence of hyperfine-induced, quasi-static optical selection rules enables the optical generation of coherent spin dark states without an external magnetic field. We show that the phase and amplitude of the lasers implement multi-axis manipulation of the basis spanned by the dark and bright states, enabling control via projection into a spin-superposition state. Our approach can be extended, within the scope of quantum control and feedback15, 16, to other systems interacting with an adiabatically evolving environment.

http://www.nature.com/nphys/journal/vaop/ncurrent/full/nphys3077.html

Graphene nanoribbon heterojunctions

http://www.nature.com/nnano/journal/vaop/ncurrent/full/nnano.2014.184.html

Generation and electric control of spin–valley-coupled circular photogalvanic current in WSe2

http://www.nature.com/nnano/journal/vaop/ncurrent/full/nnano.2014.183.html

Sensitive room-temperature terahertz detection via the photothermoelectric effect in graphene

'Xinghan Cai, Andrei B. Sushkov, Ryan J. Suess, Mohammad M. Jadidi, Gregory S. Jenkins, Luke O. Nyakiti, Rachael L. Myers-Ward, Shanshan Li, Jun Yan, D. Kurt Gaskill, Thomas E. Murphy, H. Dennis Drew & Michael S. Fuhrer'

Terahertz radiation has uses in applications ranging from security to medicine1. However, sensitive room-temperature detection of terahertz radiation is notoriously difficult2. The hot-electron photothermoelectric effect in graphene is a promising detection mechanism; photoexcited carriers rapidly thermalize due to strong electron–electron interactions3, 4, but lose energy to the lattice more slowly3, 5. The electron temperature gradient drives electron diffusion, and asymmetry due to local gating6, 7 or dissimilar contact metals8 produces a net current via the thermoelectric effect. Here, we demonstrate a graphene thermoelectric terahertz photodetector with sensitivity exceeding 10 V W–1 (700 V W–1) at room temperature and noise-equivalent power less than 1,100 pW Hz–1/2 (20 pW Hz–1/2), referenced to the incident (absorbed) power. This implies a performance that is competitive with the best room-temperature terahertz detectors9 for an optimally coupled device, and time-resolved measurements indicate that our graphene detector is eight to nine orders of magnitude faster than those7, 10. A simple model of the response, including contact asymmetries (resistance, work function and Fermi-energy pinning) reproduces the qualitative features of the data, and indicates that orders-of-magnitude sensitivity improvements are possible.

http://www.nature.com/nnano/journal/vaop/ncurrent/full/nnano.2014.182.html

Polycrystalline Graphene with Single Crystalline Electronic Structure

http://pubs.acs.org/doi/abs/10.1021/nl502445j

Angle-dependent van Hove singularities and their breakdown in twisted graphene bilayers

'Wei Yan, Lan Meng, Mengxi Liu, Jia-Bin Qiao, Zhao-Dong Chu, Rui-Fen Dou, Zhongfan Liu, Jia-Cai Nie, Donald G. Naugle, and Lin He'

The creation of van der Waals heterostructures based on a graphene monolayer and other two-dimensional crystals has attracted great interest because the atomic registry of the two-dimensional crystals can modify the electronic spectra and properties of graphene. A twisted graphene bilayer can be viewed as a special van der Waals structure composed of two mutually misoriented graphene layers, where the sublayer graphene not only plays the role of a substrate, but also acts in an equivalent role as the top graphene layer in the structure. Here we report the electronic spectra of slightly twisted graphene bilayers studied by scanning tunneling microscopy and spectroscopy. Our experiment demonstrates that twist-induced van Hove singularities are ubiquitously present for rotation angles θ of less than about 3.5°, corresponding to moiré-pattern periods D longer than 4 nm. However, they totally vanish for θ>5.5° (D<2.5nm). Such a behavior indicates that the continuum models, which capture moiré-pattern periodicity more accurately at small rotation angles, are no longer applicable at large rotation angles.

http://journals.aps.org/prb/abstract/10.1103/PhysRevB.90.115402

Excitation of complex spin dynamics patterns in a quantum-dot electron spin ensemble

http://journals.aps.org/prb/abstract/10.1103/PhysRevB.90.121301

Tunable Floquet Majorana fermions in driven coupled quantum dots

'Yantao Li, Arijit Kundu, Fan Zhong, and Babak Seradjeh'

We propose a system of coupled quantum dots in proximity to a superconductor and driven by separate ac potentials to realize and detect Floquet Majorana fermions. We show that the appearance of Floquet Majorana fermions can be finely controlled in the expanded parameter space of the drive frequency, amplitude, and phase difference across the two dots. While these Majorana fermions are not topologically protected, the highly tunable setup provides a realistic system for observing the exotic physics associated with Majorana fermions as well as their dynamical generation and manipulation.

http://journals.aps.org/prb/abstract/10.1103/PhysRevB.90.121401

Unrelated:

Inventing a Modern Periscope

http://www.tested.com/science/464266-inventing-modern-periscope/

Recent interesting articles

From NanoWiki

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December 8.

November 3.

Szeptember 8-15.

Aug. 25. - szept. 7.

Március 24-31.

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Szept.19-30.

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Szept.2-12.

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@@ Line 1: / Line 1: @@
-[http://www.sciencemag.org/current.dtl#twis Science this week issue]
+[https://www.science.org/toc/science/current Science this week issue]
-[http://www.nature.com/search/executeSearch?sp-advanced=true&include-collections=journals_nature%2Ccrawled_content&exclude-collections=journals_palgrave%2Clab_animal&sp-m=0&sp-q=&sp-p=all&sp-q-9%5BNATURE%5D=1&sp-q-2=&sp-p-2=all&sp-q-3=&sp-p-3=all&sp-q-4=&sp-q-5=&sp-q-6=&pub-date-mode=range&sp-date-range=7&sp-q-8=&sp-s=date_descending&sp-c=25 Nature last week]
+[https://www.nature.com/nature/current-issue Nature last week]
-[http://www.nature.com/search/executeSearch?sp-advanced=true&include-collections=journals_nature%2Ccrawled_content&exclude-collections=journals_palgrave%2Clab_animal&sp-m=0&sp-q=&sp-p=all&sp-q-9%5BNPHYS%5D=1&sp-q-2=&sp-p-2=all&sp-q-3=&sp-p-3=all&sp-q-4=&sp-q-5=&sp-q-6=&pub-date-mode=range&sp-date-range=7&sp-q-8=&sp-s=date_descending&sp-c=25 Nature Physics last week]
+[https://www.nature.com/nphys/current-issue Nature Physics last week]
-[http://www.nature.com/search/executeSearch?sp-advanced=true&include-collections=journals_nature%2Ccrawled_content&exclude-collections=journals_palgrave%2Clab_animal&sp-m=0&sp-q=&sp-p=all&sp-q-9%5BNNANO%5D=1&sp-q-2=&sp-p-2=all&sp-q-3=&sp-p-3=all&sp-q-4=&sp-q-5=&sp-q-6=&pub-date-mode=range&sp-date-range=7&sp-q-8=&sp-s=date_descending&sp-c=25 Nature Nanotechnology last week]
+[https://www.nature.com/nnano/current-issue Nature Nanotechnology last week]
 [http://pubs.acs.org/toc/nalefd/0/0 Nano Letters ASAP]
@@ Line 11: / Line 11: @@
 [http://pubs.acs.org/toc/ancac3/0/0 ACS Nano ASAP]
-[http://xxx.lanl.gov/list/cond-mat.mes-hall/recent Cond-mat Mesoscale and Nanoscale Physics - recent papers]
+[http://xxx.lanl.gov/list/cond-mat.mes-hall/recent Cond-mat Mesoscale and Nanoscale Physics - recent papers] ''Note: all the papers in a certain month can be listed as e.g. http://xxx.lanl.gov/list/cond-mat.mes-hall/1104 , where 11 stands for 2011 and 04 for April.''
 [http://prl.aps.org/browse Physical Review Letters]
@@ Line 17: / Line 17: @@
 [http://prb.aps.org/browse Physical Review B]
-== Feb 9. - Feb. 16. (2011) ==
+[http://magnetooptics.phy.bme.hu]
-''Válogatta: Makk Péter ''
+[[Recent interesting articles - archive 2013 - | Link to the archive of this series before 2014]]
-----
-'''Scanning tunnelling microscopy and spectroscopy of ultra-flat graphene on hexagonal boron nitride'''
-Jiamin Xue, Javier Sanchez-Yamagishi,Danny Bulmash, Philippe Jacquod, Aparna Deshpande, K. Watanabe,  T. Taniguchi, Pablo Jarillo-Herrero & Brian J. LeRoy
-Graphene has demonstrated great promise for future electronics technology as well as fundamental physics applications because of its linear energy–momentum dispersion relations which cross at the Dirac point1, 2. However, accessing the physics of the low-density region at the Dirac point has been difficult because of disorder that leaves the graphene with local microscopic electron and hole puddles3, 4, 5. Efforts have been made to reduce the disorder by suspending graphene, leading to fabrication challenges and delicate devices which make local spectroscopic measurements difficult6, 7. Recently, it has been shown that placing graphene on hexagonal boron nitride (hBN) yields improved device performance8. Here we use scanning tunnelling microscopy to show that graphene conforms to hBN, as evidenced by the presence of Moiré patterns. However, contrary to predictions9, 10, this conformation does not lead to a sizeable band gap because of the misalignment of the lattices. Moreover, local spectroscopy measurements demonstrate that the electron–hole charge fluctuations are reduced by two orders of magnitude as compared with those on silicon oxide. This leads to charge fluctuations that are as small as in suspended graphene6, opening up Dirac point physics to more diverse experiments.
-http://www.nature.com/nmat/journal/vaop/ncurrent/full/nmat2968.html
 ----
-'''Gate-controlled guiding of electrons in graphene'''
-J. R. Williams, Tony Low, M. S. Lundstrom & C. M. Marcus
-Ballistic semiconductor structures have allowed the realization of optics-like phenomena in electronic systems, including the magnetic focusing1 and electrostatic lensing2 of electrons. An extension that appears unique to graphene is to use both n and p carrier types to create electronic analogues of optical devices with both positive and negative indices of refraction3. Here, we use the gate-controlled density of both p and n carrier types in graphene to demonstrate the electronic analogue of fibre-optic guiding4, 5, 6, 7, 8. Two basic effects are investigated: bipolar p–n junction guiding, based on the principle of angle-selective transmission through the interface between the graphene and the p–n junction; and unipolar fibre-optic guiding, using total internal reflection controlled by carrier density. We also demonstrate modulation of the guiding efficiency through gating, and comparison of these data with numerical simulations indicates that guiding performance is limited by the roughness of the interface. The development of p–n and fibre-optic guiding in graphene may lead to electrically reconfigurable wiring in high-mobility devices.
-http://www.nature.com/nnano/journal/vaop/ncurrent/full/nnano.2011.3.html
 ----
-'''Programmable nanowire circuits for nanoprocessors'''
-Hao Yan, Hwan Sung Choe, SungWoo Nam,Yongjie Hu, Shamik Das, James F. Klemic, James C. Ellenbogen & Charles M. Lieber
+'''Mindig a legfrissebb bejegyzés van legfelül.'''
-A nanoprocessor constructed from intrinsically nanometre-scale building blocks is an essential component for controlling memory, nanosensors and other functions proposed for nanosystems assembled from the bottom up1, 2, 3. Important steps towards this goal over the past fifteen years include the realization of simple logic gates with individually assembled semiconductor nanowires and carbon nanotubes1, 4, 5, 6, 7, 8, but with only 16 devices or fewer and a single function for each circuit. Recently, logic circuits also have been demonstrated that use two or three elements of a one-dimensional memristor array9, although such passive devices without gain are difficult to cascade. These circuits fall short of the requirements for a scalable, multifunctional nanoprocessor10, 11 owing to challenges in materials, assembly and architecture on the nanoscale. Here we describe the design, fabrication and use of programmable and scalable logic tiles for nanoprocessors that surmount these hurdles. The tiles were built from programmable, non-volatile nanowire transistor arrays. Ge/Si core/shell nanowires12 coupled to designed dielectric shells yielded single-nanowire, non-volatile field-effect transistors (FETs) with uniform, programmable threshold voltages and the capability to drive cascaded elements. We developed an architecture to integrate the programmable nanowire FETs and define a logic tile consisting of two interconnected arrays with 496 functional configurable FET nodes in an area of ~960 μm2. The logic tile was programmed and operated first as a full adder with a maximal voltage gain of ten and input–output voltage matching. Then we showed that the same logic tile can be reprogrammed and used to demonstrate full-subtractor, multiplexer, demultiplexer and clocked D-latch functions. These results represent a significant advance in the complexity and functionality of nanoelectronic circuits built from the bottom up with a tiled architecture that could be cascaded to realize fully integrated nanoprocessors with computing, memory and addressing capabilities.
+== December 8. ==
+''Boros Csanád Örs''
-http://www.nature.com/nature/journal/v470/n7333/full/nature09749.html
+'''The 100th anniversary of the four-point probe technique: the role of probe geometries in isotropic and anisotropic systems'''
-----
-== Jan. 26. - Feb. 8. (2011) ==
+The electrical conductivity of solid-state matter is a fundamental physical property and can be
+precisely derived from the resistance measured via the four-point probe technique excluding
+contributions from parasitic contact resistances. Over time, this method has become an
+interdisciplinary characterization tool in materials science, semiconductor industries, geology,
+physics, etc, and is employed for both fundamental and application-driven research. However, the
+correct derivation of the conductivity is a demanding task which faces several difficulties, e.g. the
+homogeneity of the sample or the isotropy of the phases. In addition, these sample-specific
+characteristics are intimately related to technical constraints such as the probe geometry and size of
+the sample. In particular, the latter is of importance for nanostructures which can now be probed
+technically on very small length scales. On the occasion of the 100th anniversary of the four-point
+probe technique, introduced by Frank Wenner, in this review we revisit and discuss various
+correction factors which are mandatory for an accurate derivation of the resistivity from the
+measured resistance. Among others, sample thickness, dimensionality, anisotropy, and the relative
+size and geometry of the sample with respect to the contact assembly are considered. We are also
+able to derive the correction factors for 2D anisotropic systems on circular finite areas with variable
+probe spacings. All these aspects are illustrated by state-of-the-art experiments carried out using a
+four-tip STM/SEM system. We are aware that this review article can only cover some of the most
+important topics. Regarding further aspects, e.g. technical realizations, the influence of
+inhomogeneities or different transport regimes, etc, we refer to other review articles in this field.
-''Válogatta: Makk Péter és Geresdi Attila''
+http://iopscience.iop.org/article/10.1088/0953-8984/27/22/223201/pdf
-----
-'''Transport through Andreev bound states in a graphene quantum dot'''
-Travis Dirks, Taylor L. Hughes, Siddhartha Lal, Bruno Uchoa, Yung-Fu Chen, Cesar Chialvo, Paul M. Goldbart and Nadya Mason
+== November 3. ==
+''Boros Csanád Örs''
-When a low-energy electron is incident on an interface between a metal and superconductor, it causes the injection of a Cooper pair into the superconductor and the generation of a hole that reflects back into the metal—a process known as Andreev reflection. In confined geometries, this process can give rise to discrete Andreev bound states (ABS), which can enable transport of supercurrents through non-superconducting materials and have recently been proposed as a means of realizing solid-state qubits1, 2, 3. Here, we report transport measurements of sharp, gate-tunable ABS formed in a superconductor–quantum dot (QD)–normal system realized on an exfoliated graphene sheet. The QD is formed in graphene beneath a superconducting contact as a result of a work-function mismatch4, 5. Individual ABS form when the discrete QD levels are proximity-coupled to the superconducting contact. Owing to the low density of states of graphene and the sensitivity of the QD levels to an applied gate voltage, the ABS spectra are narrow and can be continuously tuned down to zero energy by the gate voltage.
+'''Margination of micro- and nano-particles in blood flow and its effect on drug delivery'''
-http://dx.doi.org/10.1038/nphys1911
+Kathrin Müller, Dmitry A. Fedosov & Gerhard Gompper
-----
+Drug delivery by micro- and nano-carriers enables controlled transport of pharmaceuticals to targeted sites.
+Even though carrier fabrication has made much progress recently, the delivery including controlled particle
+distribution and adhesion within the body remains a great challenge. The adhesion of carriers is strongly
+affected by their margination properties (migration toward walls) in the microvasculature. To investigate
+margination characteristics of carriers of different shapes and sizes and to elucidate the relevant physical
+mechanisms, we employ mesoscopic hydrodynamic simulations of blood flow. Particle margination is
+studied for a wide range of hematocrit values, vessel sizes, and flow rates, using two- and three-dimensional
+models. The simulations show that the margination properties of particles improve with increasing carrier
+size. Spherical particles yield slightly better margination than ellipsoidal carriers; however, ellipsoidal
+particles exhibit a slower rotational dynamics near a wall favoring their adhesion. In conclusion,
+micron-sized ellipsoidal particles are favorable for drug delivery in comparison with sub-micron spherical
+particles.
-'''Single-layer MoS_2 transistors'''
+http://www.nature.com/articles/srep04871
-B. Radisavljevic,A. Radenovic, J. Brivio, V. Giacometti and A. Kis
+== Szeptember 8-15. ==
+''Scherübl Zoltán''
-Two-dimensional materials are attractive for use in next-generation nanoelectronic devices because, compared to one-dimensional materials, it is relatively easy to fabricate complex structures from them. The most widely studied two-dimensional material is graphene1, 2, both because of its rich physics3, 4, 5 and its high mobility6. However, pristine graphene does not have a bandgap, a property that is essential for many applications, including transistors7. Engineering a graphene bandgap increases fabrication complexity and either reduces mobilities to the level of strained silicon films8, 9, 10, 11, 12, 13 or requires high voltages14, 15. Although single layers of MoS2  have a large intrinsic bandgap of 1.8 eV (ref. 16), previously reported mobilities in the 0.5–3 cm2 V−1 s−1 range17  are too low for practical devices. Here, we use a halfnium oxide gate dielectric to demonstrate a room-temperature single-layer MoS2  mobility of at least 200 cm2 V−1 s−1, similar to that of graphene nanoribbons, and demonstrate transistors with room-temperature current on/off ratios of 1 × 108 and ultralow standby power dissipation. Because monolayer MoS2 has a direct bandgap16, 18, it can be used to construct interband tunnel FETs19, which offer lower power consumption than classical transistors. Monolayer MoS2 could also complement graphene in applications that require thin transparent semiconductors, such as optoelectronics and energy harvesting.
+'''Guiding of Electrons in a Few Mode Ballistic Graphene Channel'''
-http://dx.doi.org/10.1038/nnano.2010.279
+Peter Rickhaus, Ming-Hao Liu, Péter Makk, Romain Maurand, Samuel Hess, Simon Zihlmann, Markus Weiss, Klaus Richter, Christian Schönenberger
-----
+http://arxiv.org/abs/1509.02653
-'''The origins and limits of metal–graphene junction resistance'''
+'''Hexagonal boron nitride as an atomically thin oxidation barrier for ferromagnetic nano structures'''
-Fengnian Xia, Vasili Perebeinos, Yu-ming Lin, Yanqing Wu and Phaedon Avouris
+Simon Zihlmann, Péter Makk, C. A. F. Vaz, Christian Schönenberger
-A high-quality junction between graphene and metallic contacts is crucial in the creation of high-performance graphene transistors. In an ideal metal–graphene junction, the contact resistance is determined solely by the number of conduction modes in graphene. However, as yet, measurements of contact resistance have been inconsistent, and the factors that determine the contact resistance remain unclear. Here, we report that the contact resistance in a palladium–graphene junction exhibits an anomalous temperature dependence, dropping significantly as temperature decreases to a value of just 110 ± 20 Ω µm at 6 K, which is two to three times the minimum achievable resistance. Using a combination of experiment and theory we show that this behaviour results from carrier transport in graphene under the palladium contact. At low temperature, the carrier mean free path exceeds the palladium–graphene coupling length, leading to nearly ballistic transport with a transfer efficiency of ~75%. As the temperature increases, this carrier transport becomes less ballistic, resulting in a considerable reduction in efficiency.
+http://arxiv.org/abs/1509.03087
-http://dx.doi.org/10.1038/nnano.2011.6
+'''Giga-Hertz quantized charge pumping in bottom gate defined InAs nanowire quantum dots'''
-----
+S. d'Hollosy, M. Jung, A. Baumgartner, V.A. Guzenko, M.H. Madsen, J. Nygård, C. Schönenberger
-'''Does a ferromagnet with spin-dependent masses produce a spin-filtering effect in a ferromagnetic/insulator/superconductor junction?'''
+http://arxiv.org/abs/1509.01574
-Gaetano Annunziata, Mario Cuoco, Paola Gentile, Alfonso Romano, Canio Noce
+'''Coherent coupling of a single spin to microwave cavity photons'''
-We analyze charge transport through a ballistic ferromagnet/insulator/superconductor junction by means of the Bogoliubov-de Gennes equations. We take into account the possibility that ferromagnetism in the first electrode may be driven by a mass renormalization of oppositely polarized carriers, i.e. by a spin bandwidth asymmetry, rather than by a rigid splitting of up-and down-spin electron bands as in a standard Stoner ferromagnet. By evaluating the averaged charge conductance for both an s- and a $d_{x^2-y^2}$-wave order parameter for the S side, we show that the mass mismatch in the ferromagnetic electrode may mimic a spin active barrier. Indeed, in the $s$-wave case we show that under suitable conditions the spin dependent conductance of minority carriers below the energy gap $\Delta_0$ can be larger than for majority carriers, and lower above $\Delta_0$. On the other hand, for a d_{x^2-y^2}-wave superconductor similar spin-dependent effects give rise to an asymmetric peak splitting in the conductance. These results suggest that the junction may work as a spin-filtering device.
+J. J. Viennot, M. C. Dartiailh, A. Cottet, T. Kontos
-http://arxiv.org/abs/1101.4780v1
+http://arxiv.org/abs/1509.03839
-----
+'''Negative local resistance due to viscous electron backflow in graphene'''
-'''Novel E-beam lithography technique for in-situ junction fabrication: the controlled undercut'''
+D. A. Bandurin, I. Torre, R. Krishna Kumar, M. Ben Shalom, A. Tomadin, A. Principi, G. H. Auton, E. Khestanova, K. S. Novoselov, I. V. Grigorieva, L. A. Ponomarenko, A. K. Geim, M. Polini
-Florent Lecocq (NEEL), Cécile Naud (NEEL), Ioan M. Pop (NEEL), Zhi-Hui Peng (NEEL), Iulian Matei (NEEL), Thierry Crozes (NEEL), Thierry Fournier (NEEL), Wiebke Guichard (NEEL), Olivier Buisson (NEEL)
+http://arxiv.org/abs/1509.04165
-We present a novel shadow evaporation technique for the realization of junctions and capacitors. The design by E-beam lithography of strongly asymmetric undercuts on a bilayer resist enables in-situ fabrication of junctions and capacitors without the use of the well-known suspended bridge[1]. The absence of bridges increases the mechanical robustness of the resist mask as well as the accessible range of the junction size, from 0.01 to more than 10000 micron square. We have fabricated Al/AlOx/Al Josephson junctions, phase qubit and capacitors using a 100kV E- beam writer. Although this high voltage enables a precise control of the undercut, implementation using a conventional 20kV E-beam is also discussed. The phase qubit coherence times, extracted from spectroscopy resonance width, Rabi and Ramsey oscillations decay and energy relaxation measurements, are longer than the ones obtained in our previous samples realized by standard techniques. These results demonstrate the high quality of the junction obtained by this controlled undercut technique.
+'''Point contacts in encapsulated graphene'''
-http://arxiv.org/abs/1101.4576v2
+Clevin Handschin, Balint Fülöp, Péter Makk, Sofya Blanter, Markus Weiss, K. Watanabe, T. Taniguchi, Szabolcs Csonka, Christian Schönenberger
-----
+http://arxiv.org/abs/1509.04137
-'''Tuning of the spin-orbit interaction in a quantum dot by an in-plane magnetic field'''
+'''Coherent manipulation of Andreev states in superconducting atomic contacts'''
-M.P. Nowak, B. Szafran, F.M. Peeters, B. Partoens, W. Pasek
+C. Janvier (1), L. Tosi (1), L. Bretheau (1), Ç. Ö. Girit (1), M. Stern (1), P. Bertet (1), P. Joyez (1), D. Vion (1), D. Esteve (1), M.F. Goffman (1), H. Pothier (1), C. Urbina (1) ((1) QUANTRONICS)
-Using an exact diagonalization approach we show that one- and two-electron InAs quantum dots exhibit avoided crossing in the energy spectra that are induced by the spin-orbit coupling in the presence of an in-plane external magnetic field. The width of the avoided crossings depends strongly on the orientation of the magnetic field which reveals the intrinsic anisotropy of the spin-orbit coupling interactions. We find that for specific orientations of the magnetic field avoided crossings vanish. Value of this orientation can be used to extract the ratio of the strength of Rashba and Dresselhaus interactions. The spin-orbit anisotropy effects for various geometries and orientations of the confinement potential are discussed. Our analysis explains the physics behind the recent measurements performed on a gated self-assembled quantum dot [S. Takahashi et al. Phys. Rev. Lett. 104, 246801 (2010)].
+http://arxiv.org/abs/1509.03961
-http://arxiv.org/abs/1102.1002v1
+'''Realization of Microwave Quantum Circuits Using Hybrid Superconducting-Semiconducting Nanowire Josephson Elements'''
-----
+G. de Lange, B. van Heck, A. Bruno, D. J. van Woerkom, A. Geresdi, S. R. Plissard, E. P. A. M. Bakkers, A. R. Akhmerov, and L. DiCarlo
-'''Self heating and nonlinear current-voltage characteristics in bilayer graphene'''
+http://journals.aps.org/prl/abstract/10.1103/PhysRevLett.115.127002
-J. K. Viljas, A. Fay, M. Wiesner, P. J. Hakonen
+'''Semiconductor-Nanowire-Based Superconducting Qubit'''
-We demonstrate by experiments and numerical simulations that the low-temperature current-voltage characteristics in diffusive bilayer graphene (BLG) exhibit a strong superlinearity at finite bias voltages. The superlinearity is weakly dependent on doping and on the length of the graphene sample. This effect can be understood as a result of Joule heating. It is stronger in BLG than in monolayer graphene (MLG), since the conductivity of BLG is more sensitive to temperature due to the higher density of electronic states at the Dirac point.
+T. W. Larsen, K. D. Petersson, F. Kuemmeth, T. S. Jespersen, P. Krogstrup, J. Nygård, and C. M. Marcus
-http://arxiv.org/abs/1102.0658v1
+http://journals.aps.org/prl/abstract/10.1103/PhysRevLett.115.127001
-----
+'''Charge Number Dependence of the Dephasing Rates of a Graphene Double Quantum Dot in a Circuit QED Architecture'''
-'''Vibrational Instabilities in Resonant Electron Transport through Single-Molecule Junctions'''
+Guang-Wei Deng, Da Wei, J. R. Johansson, Miao-Lei Zhang, Shu-Xiao Li, Hai-Ou Li, Gang Cao, Ming Xiao, Tao Tu, Guang-Can Guo, Hong-Wen Jiang, Franco Nori, and Guo-Ping Guo
-R. Härtle, M. Thoss
+http://journals.aps.org/prl/abstract/10.1103/PhysRevLett.115.126804
-We analyze various limits of vibrationally coupled resonant electron transport in single-molecule junctions. Based on a master equation approach, we discuss analytic and numerical results for junctions under a high bias voltage or weak electronic-vibrational coupling. It is shown that in these limits the vibrational excitation of the molecular bridge increases indefinitely, i.e. the junction exhibits a vibrational instability. Moreover, our analysis provides analytic results for the vibrational distribution function and reveals that these vibrational instabilities are related to electron-hole pair creation processes.
+'''Spin pairs in a weakly coupled many-electron quantum dot'''
-http://arxiv.org/abs/1102.0840v1
+S. Hellmüller, D. Bischoff, T. Müller, M. Beck, K. Ensslin, and T. Ihn
-----
+http://journals.aps.org/prb/abstract/10.1103/PhysRevB.92.115401
-'''Graphene quantum dots formed by a spatial modulation of the Dirac gap'''
+'''Observation of negative refraction of Dirac fermions in graphene'''
-G. Giavaras, Franco Nori
+Gil-Ho Lee, Geon-Hyoung Park, Hu-Jong Lee
-An electrostatic quantum dot cannot be formed in monolayer graphene, because of the Klein tunnelling. However, a dot can be formed with the help of a uniform magnetic field. As shown here, a spatial modulation of the Dirac gap leads to confined states with discrete energy levels, thus defining a dot, without applying external electric and magnetic fields. Gap-induced dot states can coexist and couple with states introduced by an electrostatic potential. This property allows the region in which the resulting states are localized to be tuned with the potential.
+http://www.nature.com/nphys/journal/vaop/ncurrent/full/nphys3460.html
-http://arxiv.org/abs/1102.1042v1
+'''Parity lifetime of bound states in a proximitized semiconductor nanowire'''
-----
+A. P. Higginbotham, S. M. Albrecht, G. Kiršanskas, W. Chang, F. Kuemmeth, P. Krogstrup, T. S. Jespersen, J. Nygård, K. Flensberg, C. M. Marcus
-'''Realtime magnetic field sensing and imaging using a single spin in diamond'''
+http://www.nature.com/nphys/journal/vaop/ncurrent/full/nphys3461.html
-Rolf Simon Schoenfeld, Wolfgang Harneit
+'''Reliable Exfoliation of Large-Area High-Quality Flakes of Graphene and Other Two-Dimensional Materials'''
-The Zeeman splitting of a localized single spin can be used to construct a magnetometer allowing high precision measurements of magnetic fields with almost atomic spatial resolution. While sub-{\mu}T sensitivity can in principle be obtained using pulsed techniques and long measurement times, a fast and easy-to-use method without laborious data post-processing is desirable for a scanning-probe approach with high spatial resolution. In order to measure the resonance frequency in realtime, we applied a field-frequency lock to the continuous wave ODMR signal of a single electron spin in a nanodiamond. In our experiment, we achieved a sampling rate of up to 100 readings per second with a sensitivity of 6 {\mu}T/$\sqrt{Hz}$. Using this method we have imaged the microscopic field distribution around a magnetic wire. Images with \sim 30 {\mu}T resolution and 4096 sub-micron sized pixels were acquired in 10 minutes. By measuring the field response of multiple spins on the same object we were able to partly reconstruct the orientation of the field.
+Yuan Huang, Eli Sutter, Norman N. Shi, Jiabao Zheng, Tianzhong Yang, Dirk Englund, Hong-Jun Gao, and Peter Sutter
-http://arxiv.org/abs/1009.4138v2
+http://pubs.acs.org/doi/abs/10.1021/acsnano.5b04258
-'''Mechanical Deformation of Nanoscale Metal Rods: When Size and Shape Matter'''
+== Aug. 25. - szept. 7. ==
-M. J. Lagos, F. Sato, D. S. Galvão, and D. Ugarte
+'''Coupling Two Distant Double Quantum Dots with a Microwave Resonator'''
-Face centered cubic metals deform mainly by propagating partial dislocations generating planar fault ribbons. How do metals deform if the size is smaller than the fault ribbons? We studied the elongation of Au and Pt nanorods by in situ electron microscopy and ab initio  calculations. Planar fault activation barriers are so low that, for each temperature, a minimal rod size is required to become active for releasing elastic energy. Surface effects dominate deformation energetics; system size and shape determine the preferred fault gliding directions which induce different tensile and compressive behavior.
+Guang-Wei Deng, Da Wei, Shu-Xiao Li, J. R. Johansson, Wei-Cheng Kong, Hai-Ou Li, Gang Cao, Ming Xiao, Guang-Can Guo, Franco Nori, Hong-Wen Jiang, and Guo-Ping Guo
-http://link.aps.org/doi/10.1103/PhysRevLett.106.055501
+We fabricated a hybrid device with two distant graphene double quantum dots (DQDs) and a microwave resonator. A nonlinear response is observed in the resonator reflection amplitude when the two DQDs are jointly tuned to the vicinity of the degeneracy points. This observation can be well fitted by the Tavis–Cummings (T–C) model which describes two two-level systems coupling with one photonic field. Furthermore, the correlation between the DC currents in the two DQDs is studied. A nonzero cross-current correlation is observed which has been theoretically predicted to be an important sign of nonlocal coupling between two distant systems. Our results explore T–C physics in electronic transport and also contribute to the study of nonlocal transport and future implementations of remote electronic entanglement.
-----
-'''Breakdown of Atomic-Sized Metallic Contacts Measured on Nanosecond Scale'''
+http://pubs.acs.org/doi/abs/10.1021/acs.nanolett.5b02400
-Shaoyin Guo, Joshua Hihath, and Nongjian Tao
+'''Reliable Exfoliation of Large-Area High-Quality Flakes of Graphene and Other Two-Dimensional Materials'''
-We report on a study of atomic-sized metallic contacts on a time scale of nanoseconds using a combined DC and AC circuit. The approach leads to a time resolution 3−4 orders of magnitude faster than the measurements carried out to date, making it possible to observe fast transient conductance-switching events associated with the breakdown, re-formation, and atomic scale structural rearrangements of the contact. The study bridges the wide gap in the time scales between the molecular dynamic simulations and real world experiments, and the method may be applied to study nano- and subnanosecond processes in other nanoscale devices, such as molecular junctions.
+Yuan Huang, Eli Sutter, Norman N. Shi, Jiabao Zheng, Tianzhong Yang, Dirk Englund, Hong-Jun Gao, and Peter Sutter
-http://pubs.acs.org/doi/abs/10.1021/nl1026748
+Mechanical exfoliation has been a key enabler of the exploration of the properties of two-dimensional materials, such as graphene, by providing routine access to high-quality material. The original exfoliation method, which remained largely unchanged during the past decade, provides relatively small flakes with moderate yield. Here, we report a modified approach for exfoliating thin monolayer and few-layer flakes from layered crystals. Our method introduces two process steps that enhance and homogenize the adhesion force between the outermost sheet in contact with a substrate: Prior to exfoliation, ambient adsorbates are effectively removed from the substrate by oxygen plasma cleaning, and an additional heat treatment maximizes the uniform contact area at the interface between the source crystal and the substrate. For graphene exfoliation, these simple process steps increased the yield and the area of the transferred flakes by more than 50 times compared to the established exfoliation methods. Raman and AFM characterization shows that the graphene flakes are of similar high quality as those obtained in previous reports. Graphene field-effect devices were fabricated and measured with back-gating and solution top-gating, yielding mobilities of ∼4000 and 12 000 cm2/(V s), respectively, and thus demonstrating excellent electrical properties. Experiments with other layered crystals, e.g., a bismuth strontium calcium copper oxide (BSCCO) superconductor, show enhancements in exfoliation yield and flake area similar to those for graphene, suggesting that our modified exfoliation method provides an effective way for producing large area, high-quality flakes of a wide range of 2D materials.
------
-'''Grain Boundary Mapping in Polycrystalline Graphene'''
+http://pubs.acs.org/doi/abs/10.1021/acsnano.5b04258
-Kwanpyo Kim†‡, Zonghoon Lee§, William Regan†‡, C. Kisielowski§, M. F. Crommie†‡, and A. Zettl†‡*
+'''Influence of Impurity Spin Dynamics on Quantum Transport in Epitaxial Graphene'''
-We report direct mapping of the grains and grain boundaries (GBs) of large-area monolayer polycrystalline graphene sheets, at large (several micrometer) and single-atom length scales. Global grain and GB mapping is performed using electron diffraction in scanning transmission electron microscopy (STEM) or using dark-field imaging in conventional TEM. Additionally, we employ aberration-corrected TEM to extract direct images of the local atomic arrangements of graphene GBs, which reveal the alternating pentagon−heptagon structure along high-angle GBs. Our findings provide a readily adaptable tool for graphene GB studies.
+Samuel Lara-Avila, Sergey Kubatkin, Oleksiy Kashuba, Joshua A. Folk, Silvia Lüscher, Rositza Yakimova, T. J. B. M. Janssen, Alexander Tzalenchuk, and Vladimir Fal’ko
-http://pubs.acs.org/doi/abs/10.1021/nn1033423
+Experimental evidence from both spin-valve and quantum transport measurements points towards unexpectedly fast spin relaxation in graphene. We report magnetotransport studies of epitaxial graphene on SiC in a vector magnetic field showing that spin relaxation, detected using weak-localization analysis, is suppressed by an in-plane magnetic field B∥, and thereby proving that it is caused at least in part by spinful scatterers. A nonmonotonic dependence of the effective decoherence rate on B∥ reveals the intricate role of the scatterers’ spin dynamics in forming the interference correction to the conductivity, an effect that has gone unnoticed in earlier weak localization studies.
-----
-'''Universal Segregation Growth Approach to Wafer-Size Graphene from Non-Noble Metals'''
+http://journals.aps.org/prl/pdf/10.1103/PhysRevLett.115.106602
-Nan Liu†, Lei Fu†, Boya Dai, Kai Yan, Xun Liu, Ruiqi Zhao, Yanfeng Zhang, and Zhongfan Liu*
+'''Highly thermally conductive and mechanically strong graphene fibers'''
-Graphene has been attracting wide interests owing to its excellent electronic, thermal, and mechanical performances. Despite the availability of several production techniques, it is still a great challenge to achieve wafer-size graphene with acceptable uniformity and low cost, which would determine the future of graphene electronics. Here we report a universal segregation growth technique for batch production of high-quality wafer-scale graphene from non-noble metal films. Without any extraneous carbon sources, 4 in. graphene wafers have been obtained from Ni, Co, Cu−Ni alloy, and so forth via thermal annealing with over 82% being 1−3 layers and excellent reproducibility. We demonstrate the first example of monolayer and bilayer graphene wafers using Cu−Ni alloy by combining the distinct segregation behaviors of Cu and Ni. Together with the easy detachment from growth substrates, we believe this facile segregation technique will offer a great driving force for graphene research.
+Guoqing Xin, Tiankai Yao, Hongtao Sun, Spencer Michael Scott, Dali Shao, Gongkai Wang, Jie Lian
-http://pubs.acs.org/doi/abs/10.1021/nl103962a#cor1
+Graphene, a single layer of carbon atoms bonded in a hexagonal lattice, is the thinnest, strongest, and stiffest known material and an excellent conductor of heat and electricity. However, these superior properties have yet to be realized for graphene-derived macroscopic structures such as graphene fibers. We report the fabrication of graphene fibers with high thermal and electrical conductivity and enhanced mechanical strength. The inner fiber structure consists of large-sized graphene sheets forming a highly ordered arrangement intercalated with small-sized graphene sheets filling the space and microvoids. The graphene fibers exhibit a submicrometer crystallite domain size through high-temperature treatment, achieving an enhanced thermal conductivity up to 1290 watts per meter per kelvin. The tensile strength of the graphene fiber reaches 1080 megapascals.
-----
-'''Graphene Spintronics: The Role of Ferromagnetic Electrodes'''
+https://www.sciencemag.org/content/349/6252/1083.abstract
-Jesse Maassen*†, Wei Ji*†‡, and Hong Guo†
+'''A quantum circuit rule for interference effects in single-molecule electrical junctions'''
-We report a first principles study of spin transport under finite bias through a graphene−ferromagnet (FM) interface, where FM = Co(111), Ni(111). The use of Co and Ni electrodes achieves spin efficiencies reaching 80% and 60%, respectively. This large spin filtering results from the materials specific interaction between graphene and the FM which destroys the linear dispersion relation of the graphene bands and leads to an opening of spin-dependent energy gaps of ≈0.4−0.5 eV at the K points. The minority spin band gap resides higher in energy than the majority spin band gap located near EF, a feature that results in large minority spin dominated currents.
+David Zsolt Manrique, Cancan Huang, Masoud Baghernejad, Xiaotao Zhao, Oday A. Al-Owaedi, Hatef Sadeghi, Veerabhadrarao Kaliginedi, Wenjing Hong, Murat Gulcur, Thomas Wandlowski, Martin R. Bryce, Colin J. Lambert
-http://pubs.acs.org/doi/abs/10.1021/nl1031919
+A quantum circuit rule for combining quantum interference (QI) effects in the conductive properties of oligo(phenyleneethynylene) (OPE)-type molecules possessing three aromatic rings was investigated both experimentally and theoretically. Molecules were of the type X-Y-X, where X represents pyridyl anchors with para (p), meta (m) or ortho (o) connectivities and Y represents a phenyl ring with p and m connectivities. The conductances GXmX (GXpX) of molecules of the form X-m-X (X-p-X), with meta (para) connections in the central ring were predominantly lower (higher), irrespective of the meta, para, or ortho nature of the anchor groups X, demonstrating that conductance is dominated by the nature of QI in the central ring Y. The single-molecule conductances were found to satisfy the quantum circuit rule Gppp/Gpmp = Gmpm/Gmmm. This demonstrates that the contribution to the conductance from the central ring is independent of the para versus meta nature of the anchor groups.
-----
-'''Thermal Dynamics of Graphene Edges Investigated by Polarized Raman Spectroscopy'''
-Ya Nan Xu†‡, Da Zhan†, Lei Liu†, Hui Suo‡, Zhen Hua Ni§*, Thuong Thuong Nguyen, Chun Zhao‡, and Ze Xiang Shen†*
+http://xxx.lanl.gov/abs/1509.00990
-In this report, we present Raman spectroscopy investigation of the thermal stability and dynamics of graphene edges. It is found that graphene edges (both armchair and zigzag) are not stable and undergo modifications even at temperature as low as 200 °C. On the basis of polarized Raman results, we provide possible structural models on how graphene edges change during annealing. The zigzag edges rearrange and form armchair segments that are ±30° relative to the edge direction, while armchair edges are dominated by armchair segments even at annealing temperature as high as 500 °C. The modifications of edge structures by thermal annealing (zigzag segments rearrange in form of armchair segments) provide a flexible way to control the electronic properties of graphene and graphene nanostructures.
+'''Spawning rings of exceptional points out of Dirac cones'''
-http://pubs.acs.org/doi/abs/10.1021/nn101920c
+Bo Zhen, Chia Wei Hsu, Yuichi Igarashi, Ling Lu, Ido Kaminer, Adi Pick, Song-Liang Chua, John D. Joannopoulos & Marin Soljacˇic
-----
-'''Fully Electrical Read-Write Device Out of a Ferromagnetic Semiconductor'''
+The Dirac cone underlies many unique electronic properties of
+graphene1 and topological insulators, and its band structure—
+two conical bands touching at a single point—has also been realized
+for photons in waveguide arrays2
+, atoms in optical lattices3
+,
+and through accidental degeneracy4,5. Deformation of the Dirac cone often reveals intriguing properties; an example is the quantum Hall effect, where a constant magnetic field breaks the
+Dirac cone into isolated Landau levels. A seemingly unrelated phenomenon is the exceptional point6,7, also known as the parity–time symmetry breaking point8–11, where two resonances coincide in both their positions and widths. Exceptional points lead to counter-intuitive phenomena such as loss-induced transparency12, unidirectional transmission or reflection11,13,14, and lasers with reversed pump dependence15 or single-mode operation16,17. Dirac cones and exceptional points are connected: it was theoretically suggested that certain non-Hermitian perturbations can deform a Dirac cone and spawn a ring of exceptional points18–20. Here we experimentally demonstrate such an ‘exceptional ring’ in a photonic crystal slab. Angle-resolved reflection measurements of the photonic crystal slab reveal that the peaks of reflectivity follow the conical band structure of a Dirac cone resulting from accidental degeneracy, whereas the complex eigenvalues of the system are deformed into a two-dimensional flat band enclosed by an exceptional ring. This deformation arises from the dissimilar radiation rates of dipole and quadrupole resonances, which play a role analogous to the loss and gain in parity–time symmetric systems. Our results indicate that the radiation existing in any open system can
+fundamentally alter its physical properties in ways previously expected only in the presence of material loss and gain.
-S. Mark, P. Dürrenfeld, K. Pappert, L. Ebel, K. Brunner, C. Gould, and L. W. Molenkamp
+http://www.nature.com/nature/journal/vaop/ncurrent/pdf/nature14889.pdf
-We report the realization of a read-write device out of the ferromagnetic semiconductor (Ga,Mn)As as the first step to a fundamentally new information processing paradigm. Writing the magnetic state is achieved by current-induced switching and readout of the state is done by the means of the tunneling anisotropic magnetoresistance effect. This 1 bit demonstrator device can be used to design an electrically programmable memory and logic device.
+'''A Short Course on Topological Insulators: Band-structure topology and edge states in one and two dimensions'''
-http://prl.aps.org/abstract/PRL/v106/i5/e057204
+János K. Asbóth, László Oroszlány, András Pályi
-----
-'''Deterministic Entanglement of Photons in Two Superconducting Microwave Resonators'''
+This course-based primer provides newcomers to the field with a concise introduction to some of the core topics in the emerging field of topological band insulators in one and two dimensions. The aim is to provide a basic understanding of edge states, bulk topological invariants, and of the bulk--boundary correspondence with as simple mathematical tools as possible. We use noninteracting lattice models of topological insulators, building gradually on these to arrive from the simplest one-dimensional case (the Su-Schrieffer-Heeger model for polyacetylene) to two-dimensional time-reversal invariant topological insulators (the Bernevig-Hughes-Zhang model for HgTe). In each case the model is introduced first and then its properties are discussed and subsequently generalized. The only prerequisite for the reader is a working knowledge in quantum mechanics, the relevant solid state physics background is provided as part of this self-contained text, which is complemented by end-of-chapter problems.
-H. Wang1,2, Matteo Mariantoni1, Radoslaw C. Bialczak1, M. Lenander1, Erik Lucero1, M. Neeley1, A. D. O’Connell1, D. Sank1, M. Weides1, J. Wenner1, T. Yamamoto1,3, Y. Yin1, J. Zhao1, John M. Martinis1, and A. N. Cleland1,*
+http://xxx.lanl.gov/abs/1509.02295
-Quantum entanglement, one of the defining features of quantum mechanics, has been demonstrated in a variety of nonlinear spinlike systems. Quantum entanglement in linear systems has proven significantly more challenging, as the intrinsic energy level degeneracy associated with linearity makes quantum control more difficult. Here we demonstrate the quantum entanglement of photon states in two independent linear microwave resonators, creating N-photon NOON states (entangled states |N0⟩+|0N⟩) as a benchmark demonstration. We use a superconducting quantum circuit that includes Josephson qubits to control and measure the two resonators, and we completely characterize the entangled states with bipartite Wigner tomography. These results demonstrate a significant advance in the quantum control of linear resonators in superconducting circuits.
+== Március 24-31. ==
+''Fülöp Gergő''
-http://prl.aps.org/abstract/PRL/v106/i6/e060401
+'''Graphene-templated directional growth of an inorganic nanowire'''
------
-== Jan. 09. - Jan. 26. (2011) ==
+''Won Chul Lee,	Kwanpyo Kim,	Jungwon Park,	Jahyun Koo,	Hu Young Jeong,	Hoonkyung Lee,	David A. Weitz,	Alex Zettl	& Shoji Takeuchi''
-''Válogatta: Makk Péter''
+http://www.nature.com/nnano/journal/vaop/ncurrent/full/nnano.2015.36.html
-----
-'''Local charge of the ν = 5/2 fractional quantum Hall state'''
-Vivek Venkatachalam, Amir Yacoby, loren Pfeiffer & Ken West
+'''Coaxial lithography'''
-Electrons moving in two dimensions under the influence of strong magnetic fields effectively lose their kinetic energy and display exotic behaviour dominated by Coulomb forces. When the ratio of electrons to magnetic flux quanta in the system (ν) is near 5/2, the electrons are predicted to condense into a correlated phase with fractionally charged quasiparticles and a ground-state degeneracy that grows exponentially as these quasiparticles are introduced1. The only way for electrons to transform between the many ground states would be to braid the fractional excitations around each other. This property has been proposed as the basis of a fault-tolerant quantum computer2. Here we present observations of localized quasiparticles at ν = 5/2, confined to puddles by disorder. Using a local electrometer to compare how quasiparticles at ν = 5/2 and ν = 7/3 charge these puddles, we were able to extract the ratio of local charges for these states. Averaged over several disorder configurations and samples, we found the ratio to be 4/3, suggesting that the local charges are = e/3 and = e/4, where e is the charge of an electron. This is in agreement with theoretical predictions for a paired state at ν = 5/2. Confirming the existence of localized e/4 quasiparticles shows that proposed interferometry experiments to test statistics and computational ability of the state at ν = 5/2 would be possible.
+''Tuncay Ozel,	Gilles R. Bourret	& Chad A. Mirkin''
-http://www.nature.com/nature/journal/v469/n7329/full/nature09680.html
+http://www.nature.com/nnano/journal/vaop/ncurrent/full/nnano.2015.33.html
-----
+'''Coupling between electrons and optical phonons in suspended bilayer graphene'''
-'''Novel E-beam lithography technique for in-situ junction fabrication: the controlled undercut'''
-Florent Lecocq (NEEL), Cécile Naud (NEEL), Ioan M. Pop (NEEL), Zhi-Hui Peng (NEEL), Iulian Matei (NEEL), Thierry Crozes (NEEL), Thierry Fournier (NEEL), Wiebke Guichard (NEEL), Olivier Buisson (NEEL)
+''Antti Laitinen, Manohar Kumar, Mika Oksanen, Bernard Plaçais, Pauli Virtanen, and Pertti Hakonen''
-We present a novel shadow evaporation technique for the realization of junctions and capacitors. The design by E-beam lithography of strongly asymmetric undercuts on a bilayer resist enables in-situ fabrication of junctions and capacitors without the use of the well-known suspended bridge[1]. The absence of bridges increases the mechanical robustness of the resist mask as well as the accessible range of the junction size, from 0.01 to more than 10000 micron square. We have fabricated Al/AlOx/Al Josephson junctions, phase qubit and capacitors using a 100kV E- beam writer. Although this high voltage enables a precise control of the undercut, implementation using a conventional 20kV E-beam is also discussed. The phase qubit coherence times, extracted from spectroscopy resonance width, Rabi and Ramsey oscillations decay and energy relaxation measurements, are longer than the ones obtained in our previous samples realized by standard techniques. These results demonstrate the high quality of the junction obtained by this controlled undercut technique.
+http://journals.aps.org/prb/abstract/10.1103/PhysRevB.91.121414
-http://arxiv.org/abs/1101.4576
+'''Nonlocal electromagnetic response of graphene nanostructures'''
-----
+''Arya Fallahi, Tony Low, Michele Tamagnone, and Julien Perruisseau-Carrier''
-'''Quasi one-dimensional transport in single GaAs/AlGaAs core-shell nanowires'''
-Damien Lucot, Fauzia Jabeen, Jean-Christophe Harmand, Gilles Patriarche, Romain Giraud, Giancarlo Faini, Dominique Mailly
+http://journals.aps.org/prb/abstract/10.1103/PhysRevB.91.121405
-We present an original approach to fabricate single GaAs/AlGaAs core-shell nanowire with robust and reproducible transport properties. The core-shell structure is buried in an insulating GaAs overlayer and connected as grown in a two probe set-up using the highly doped growth substrate and a top diffused contact. The measured conductance shows a non-ohmic behavior with temperature and voltage-bias dependences following power laws, as expected for a quasi-1D system.
+'''Nonequilibrium spin transport in Zeeman-split superconductors'''
-http://arxiv.org/abs/1101.0421
+''Tatiana Krishtop, Manuel Houzet, and Julia S. Meyer''
-----
-'''Transition Voltage Spectroscopy and the Nature of Vacuum Tunneling'''
-M.L. Trouwborst, C.A. Martin, R.H.M. Smit, C.M. Guedon, T.A. Baart, S.J. van der Molen, J.M. van Ruitenbeek
+http://journals.aps.org/prb/abstract/10.1103/PhysRevB.91.121407
-Transition Voltage Spectroscopy (TVS) has been proposed as a tool to analyze charge transport through molecular junctions. We extend TVS to Au-vacuum-Au junctions and study the distance dependence of the transition voltage V_t(d) for clean electrodes in cryogenic vacuum. On the one hand, this allows us to provide an important reference for V_t(d)-measurements on molecular junctions. On the other hand, we show that TVS forms a simple and powerful test for vacuum tunneling models.
+'''Finite-frequency noise in a quantum dot with normal and superconducting leads'''
-http://arxiv.org/abs/1101.1779
+''Stephanie Droste, Janine Splettstoesser, and Michele Governale''
-http://pubs.acs.org/doi/abs/10.1021/nl103699t
------
-'''A spin-filter device based on armchair graphene nanoribbons'''
-A. Saffarzadeh, R. Farghadan
+http://journals.aps.org/prb/abstract/10.1103/PhysRevB.91.125401
-The coherent spin-polarized electron transport through a zigzag-edge graphene flake (ZGF), sandwiched between two semi-infinite armchair graphene nanoribbons, is investigated by means of Landauer-Buttiker formalism. To study the edge magnetism of the ZGF, we use the half-filled Hubbard model within the Hartree-Fock approximation. The results show that the junction acts as a spin filter with high degree of spin polarization in the absence of magnetic electrodes and external fields. By applying a gate voltage the spin-filtering efficiency of this device can be effectively controlled and the spin polarization can reach values as high as 90%.
+== Március 24. ==
+''Boros Csanád Örs''
-http://arxiv.org/abs/1101.2948
+'''Spin and charge transport in graphene-based spin transport devices with Co/MgO spin injection and spin detection electrodes'''
-----
+'F. Volmer, M. Drögeler, G. Güntherodt, C. Stampfer, B. Beschoten'
-'''Surprising lack of magnetism in the conductance channels of Pt atomic chains'''
-Manohar Kumar, Oren Tal, Roel H.M. Smit, Jan M. van Ruitenbeek
+In this review we discuss spin and charge transport properties in graphene-based single-layer and few-layer spin-valve devices. We give an overview of challenges and recent advances in the field of device fabrication and discuss two of our fabrication methods in more detail which result in distinctly different device performances. In the first class of devices, Co/MgO electrodes are directly deposited onto graphene which results in rough MgO-to-Co interfaces and favor the formation of conducting pinholes throughout the MgO layer. We show that the contact resistance area product (RcA) is a benchmark for spin transport properties as it scales with the measured spin lifetime in these devices indicating that contact-induced spin dephasing is the bottleneck for spin transport even in devices with large RcA values. In a second class of devices, Co/MgO electrodes are first patterned onto a silicon substrate. Subsequently, a graphene-hBN heterostructure is directly transferred onto these prepatterned electrodes which provides improved interface properties. This is seen by a strong enhancement of both charge and spin transport properties yielding charge carrier mobilities exceeding 20000 cm2/(Vs) and spin lifetimes up to 3.7 ns at room temperature. We discuss several shortcomings in the determination of both quantities which complicates the analysis of both extrinsic and intrinsic spin scattering mechanisms. Furthermore, we show that contacts can be the origin of a second charge neutrality point in gate dependent resistance measurements which is influenced by the quantum capacitance of the underlying graphene layer.
-Pt is known to show spontaneous formation of chains of metal atoms upon breaking a metallic contact. From model calculations these have been predicted to be spin polarized, which is reasonable in view of the Stoner enhanced susceptibility of bulk Pt and the increased density of states due to the reduced dimensionality. Here, we demonstrate that shot noise reveals information on the magnetic state of Pt atomic chains. Against all predictions, we find clear evidence for a non-magnetic ground state for the conductance channels of Pt atomic chains.
+http://arxiv.org/abs/1503.01735v1
-http://arxiv.org/abs/1101.3939
+== Nov. 1-21. ==
+''Scherübl Zoltán
-----
+'''Unusual resistance-voltage dependence of nanojunctions during electromigration in ultra-high vacuum'''
-'''Cotunneling through a magnetic single-molecule transistor based on N\atC60'''
-Nicolas Roch, Romain Vincent, Florian Elste, Wolfgang Harneit, Wolfgang Wernsdorfer, Carsten Timm, Franck Balestro
+''D. Stöffler, M. Marz, B. Kießig, T. Tomanic, R. Schäfer, H. v. Löhneysen, R. Hoffmann-Vogel''
-We present an experimental and theoretical study of a magnetic single-molecule transistor based on N@C60 connected to gold electrodes. Particular attention is paid to the regime of intermediate molecule-lead coupling, where cotunneling effects manifest themselves in the Coulomb-blockade regime. The experimental results for the differential conductance as a function of bias, gate voltage, and external magnetic field are in agreement with our analysis of the tunneling rates and provide evidence of magnetic signatures in single-N@C60 devices arising from an antiferromagnetic exchange interaction between the C60 spin and the nitrogen spin.
+The electrical resistance R of metallic nanocontacts subjected to controlled cyclic electromigration in ultra-high vacuum has been investigated in-situ as a function of applied voltage V. For sufficiently small contacts, i.e., large resistance, a decrease of R(V) while increasing V is observed. This effect is tentatively attributed to the presence of contacts separated by thin vacuum barriers in parallel to ohmic nanocontacts. Simple model calculations indicate that both thermal activation or tunneling can lead to this unusual behavior. We describe our data by a tunneling model whose key parameter, i.e., the tunneling distance, changes because of thermal expansion due to Joule heating and/or electrostatic strain arising from the applied voltage. Oxygen exposure during electromigration prevents the formation of negative R(V) slopes, and at the same time enhances the probability of uncontrolled melting, while other gases show little effects. In addition, indication for field emission has been observed in some samples
-http://arxiv.org/abs/1101.4198
+http://arxiv.org/abs/1411.0105
 ----
-'''Negative differential resistance in scanning tunneling microscopy: simulations on C$_{60}$-based molecular overlayers'''
-Frederico D. Novaes, Manuel Cobian, Alberto Garcia, Pablo Ordejon, Hiromu Ueba, Nicolas Lorente
+'''Pb/InAs nanowire Josephson junction with high critical current and magnetic flux focusing'''
-We determine the conditions in which negative differential resistance (NDR) appears in the C$_{60}$-based molecular device of [Phys. Rev. Lett. {\bf 100}, 036807 (2008)] by means of ab-initio electron-transport simulations. Our calculations grant access to bias-dependent intrinsic properties of the molecular device, such as electronic levels and their partial widths. We show that these quantities depend on the molecule-molecule and molecule-electrode interactions of the device. Hence, NDR can be tuned by modifying the bias behavior of levels and widths using both types of interactions.
+''J. Paajaste, M. Amado, S. Roddaro, F. S. Bergeret, D. Ercolani, L. Sorba, F. Giazotto''
-http://arxiv.org/abs/1101.3714
+We have studied mesoscopic Josephson junctions formed by highly n-doped InAs nanowires and superconducting Ti/Pb source and drain leads. The current-voltage properties of the system are investigated by varying temperature and external out-of-plane magnetic field. Superconductivity in the Pb electrodes persists up to ∼7 K and with magnetic field values up to 0.4 T. Josephson coupling at zero backgate voltage is observed up to 4.5 K and the critical current is measured to be as high as 615 nA. The supercurrent suppression as a function of the magnetic field reveals a diffraction pattern that is explained by a strong magnetic flux focusing provided by the superconducting electrodes forming the junction.
-----
+http://xxx.lanl.gov/abs/1411.0990
-'''Electrical Detection of Surface Plasmon Polaritons by 1G0 Gold Quantum Point Contacts'''
-Naomi Ittah and Yoram Selzer*
-Electrical detection of surface plasmons polaritons (SPPs) is essential for realization of integrated fast nanoscale plasmonic circuits. We demonstrate electrical detection of SPPs by measuring their remote gating effect on 1G0 metal quantum point contacts (MQPC) made of gold. Gating is argued to take place by a photoassisted transport mechanism with nonmonotonic behavior of its magnitude as a function of distance between the MQPCs and the position of SPPs creation.
-http://pubs.acs.org/doi/abs/10.1021/nl103398z
 ----
-'''Observation of Hole Accumulation in Ge/Si Core/Shell Nanowires Using off-Axis Electron Holography'''
-Luying Li*†, David J. Smith†, Eric Dailey‡, Prashanth Madras‡, Jeff Drucker†, and Martha R. McCartney†
+'''Room temperature magnetic order on zigzag edges of narrow graphene nanoribbons'''
-Hole accumulation in Ge/Si core/shell nanowires (NWs) has been observed and quantified using off-axis electron holography and other electron microscopy techniques. The epitaxial 110-oriented Ge/Si core/shell NWs were grown on Si (111) substrates by chemical vapor deposition through the vapor−liquid−solid growth mechanism. High-angle annular-dark-field scanning transmission electron microscopy images and off-axis electron holograms were obtained from specific NWs. The excess phase shifts measured by electron holography across the NWs indicated the presence of holes inside the Ge cores. Calculations based on a simplified coaxial cylindrical model gave hole densities of (0.4 ± 0.2) /nm3 in the core regions.
-http://pubs.acs.org/doi/abs/10.1021/nl1033107
+''Gabor Zsolt Magda, Xiaozhan Jin, Imre Hagymasi, Peter Vancso, Zoltan Osvath, Peter Nemes-Incze, Chanyong Hwang, Laszlo P. Biro, Levente Tapaszto''
------
-'''Toward Intrinsic Graphene Surfaces: A Systematic Study on Thermal Annealing and Wet-Chemical Treatment of SiO2-Supported Graphene Devices'''
-Zengguang Cheng, Qiaoyu Zhou, Chenxuan Wang, Qiang Li, Chen Wang*, and Ying Fang*
+Magnetic order emerging in otherwise non-magnetic materials as carbon is a paradigmatic example of a novel type of s-p electron magnetism predicted to be of exceptional high-temperature stability. It has been demonstrated that atomic scale structural defects of graphene can host unpaired spins. However, it is still unclear under which conditions long-range magnetic order can emerge from such defect-bound magnetic moments. Here we propose that in contrast to random defect distributions, atomic scale engineering of graphene edges with specific crystallographic orientation, comprising edge atoms only from one sub-lattice of the bipartite graphene lattice, can give rise to a robust magnetic order. We employ a nanofabrication technique based on Scanning Tunneling Microscopy to define graphene nanoribbons with nanometer precision and well-defined crystallographic edge orientations. While armchair ribbons display quantum confinement gap, zigzag ribbons narrower than 7 nm reveal a bandgap of about 0.2 - 0.3 eV, which can be identified as a signature of interaction induced spin ordering along their edges. Moreover, a semiconductor to metal transition is revealed upon increasing the ribbon width, indicating the switching of the magnetic coupling between opposite ribbon edges from antiferromagnetic to ferromagnetic configuration. We found that the magnetic order on graphene edges of controlled zigzag orientation can be stable even at room temperature, raising hope for graphene-based spintronic devices operating under ambient conditions.
-By combining atomic force microscopy and trans-port measurements, we systematically investigated effects of thermal annealing on surface morphologies and electrical properties of single-layer graphene devices fabricated by electron beam lithography on silicon oxide (SiO2) substrates. Thermal treatment above 300 °C in vacuum was required to effectively remove resist residues on graphene surfaces. However, annealing at high temperature was found to concomitantly bring graphene in close contact with SiO2 substrates and induce increased coupling between them, which leads to heavy hole doping and severe degradation of mobilities in graphene devices. To address this problem, a wet-chemical approach employing chloroform was developed in our study, which was shown to enable both intrinsic surfaces and enhanced electrical properties of graphene devices. Upon the recovery of intrinsic surfaces of graphene, the adsorption and assisted fibrillation of amyloid β-peptide (Aβ1-42) on graphene were electrically measured in real time.
+http://xxx.lanl.gov/abs/1411.1196
-http://pubs.acs.org/doi/abs/10.1021/nl103977d
 ----
-'''Scanning tunnelling microscopy: Closing in on molecular junctions'''
+'''Using polymer electrolyte gates to set-and-freeze threshold voltage and local potential in nanowire-based devices and thermoelectrics'''
-Andreas Heinrich
+''Sofia Fahlvik Svensson, Adam M. Burke, Damon J. Carrad, Martin Leijnse, Heiner Linke, Adam P. Micolich''
-Contacts between a single molecule and a metal electrode can be good or bad depending on the number of metal atoms that are in direct contact with the molecule.
+We use the strongly temperature-dependent ionic mobility in polymer electrolytes to 'freeze in' specific ionic charge environments around a nanowire using a local wrap-gate geometry. This enables us to set both the threshold voltage for a conventional doped substrate gate and the local disorder potential at temperatures below 200 Kelvin, which we characterize in detail by combining conductance and thermovoltage measurements with modeling. Our results demonstrate that local polymer electrolyte gates are compatible with nanowire thermoelectrics, where they offer the advantage of a very low thermal conductivity, and hold great potential towards setting the optimal operating point for solid-state cooling applications.
-http://www.nature.com/nnano/journal/v6/n1/full/nnano.2011.266.html
+http://xxx.lanl.gov/abs/1411.2727
 ----
-'''Vibrational and electronic heating in nanoscale junction'''
-Daniel R. Ward, David A. Corley, James M. Tour & Douglas Natelson
+'''Revisiting the measurement of the spin relaxation time in graphene-based devices'''
-Understanding and controlling the flow of heat is a major challenge in nanoelectronics. When a junction is driven out of equilibrium by light or the flow of electric charge, the vibrational and electronic degrees of freedom are, in general, no longer described by a single temperature1, 2, 3, 4, 5, 6. Moreover, characterizing the steady-state vibrational and electronic distributions in situ is extremely challenging. Here, we show that surface-enhanced Raman emission may be used to determine the effective temperatures for both the vibrational modes and the electrons in the current in a biased metallic nanoscale junction decorated with molecules7. Molecular vibrations show mode-specific pumping by both optical excitation8 and d.c. current9, with effective temperatures exceeding several hundred kelvin. Anti-Stokes electronic Raman emission10, 11 indicates that the effective electronic temperature at bias voltages of a few hundred millivolts can reach values up to three times the values measured when there is no current. The precise effective temperatures are model-dependent, but the trends as a function of bias conditions are robust, and allow direct comparisons with theories of nanoscale heating.
+''H. Idzuchi, A. Fert, Y. Otani''
-http://www.nature.com/nnano/journal/v6/n1/full/nnano.2010.240.html
+A long spin relaxation time (tausf) is the key for the applications of graphene to spintronics but the experimental values of tausf have been generally much shorter than expected. We show that the usual determination by the Hanle method underestimates tausf if proper account of the spin absorption by contacts is lacking. By revisiting series of experimental results, we find that the corrected tausf are longer and less dispersed, which leads to a more unified picture of tausf derived from experiments. We also discuss how the correction depends on the parameters of the graphene and contacts.
-----
+http://xxx.lanl.gov/abs/1411.2949
-'''Gate-dependent spin–orbit coupling in multielectron carbon nanotubes'''
-T. S. Jespersen, K. Grove-Rasmussen, J. Paaske, K. Muraki, T. Fujisawa, J. Nygård & K. Flensberg
-Understanding how the orbital motion of electrons is coupled to the spin degree of freedom in nanoscale systems is central for applications in spin-based electronics and quantum computation. Here we demonstrate such spin–orbit coupling in a carbon-nanotube quantum dot in the general multielectron regime and in the presence of finite disorder. Also, we find a systematic dependence of the spin–orbit coupling on the electron occupation of the quantum dot. Such a dependence has not been seen in any other system and follows from the curvature-induced spin–orbit-split Dirac spectrum of the underlying graphene lattice. Our findings suggest that the spin–orbit coupling is a general property of carbon-nanotube quantum dots, which should provide a unique platform for the study of spin–orbit effects and their applications.
-http://www.nature.com/nphys/journal/vaop/ncurrent/full/nphys1880.html
 ----
-'''Long-range Kondo signature of a single magnetic impurity'''
-Henning Prüser, Martin Wenderoth, Piet E. Dargel, Alexander Weismann, Robert Peters, Thomas Pruschke & Rainer G. Ulbrich
+'''Detecting nonlocal Cooper pair entanglement by optical Bell inequality violation'''
-The Kondo effect, one of the first recognized correlation phenomena in condensed-matter physics1, has regained attention because of scanning tunnelling spectroscopy (STS) experiments carried out on single magnetic impurities2, 3. Despite the subnanometre resolution capability of local probe techniques, one of the fundamental aspects of Kondo physics, its spatial extension, is still subject to discussion. Until now all STS studies on single adsorbed atoms have shown that observable Kondo features vanish rapidly with increasing distance from the impurity4, 5, 6, 7, 8, 9. Here we report on a hitherto unobserved long-range Kondo signature for single magnetic atoms of Fe and Co buried under a Cu(100) surface. We present a theoretical interpretation of the measured signatures using a combined approach of band-structure and many-body numerical renormalization group calculations. These are in excellent agreement with the rich spatially and spectroscopically resolved experimental data.
+''Simon E. Nigg, Rakesh P. Tiwari, Stefan Walter, Thomas L. Schmidt''
-http://www.nature.com/nphys/journal/vaop/ncurrent/full/nphys1876.html
+Based on the Bardeen Cooper Schrieffer (BCS) theory of superconductivity, the coherent splitting of Cooper pairs from a superconductor to two spatially separated quantum dots has been predicted to generate nonlocal pairs of entangled electrons. In order to test this hypothesis, we propose a scheme to transfer the spin state of a split Cooper pair onto the polarization state of a pair of optical photons. We show that the produced photon pairs can be used to violate a Bell inequality, unambiguously demonstrating the entanglement of the split Cooper pairs.
-----
+http://arxiv.org/abs/1411.3945
-'''Atomic-scale engineering of electrodes for single-molecule contacts'''
-Guillaume Schull,  Thomas Frederiksen, Andrés Arnau, Daniel Sánchez-Portal & Richard Berndt
-The transport of charge through a conducting material depends on the intrinsic ability of the material to conduct current and on the charge injection efficiency at the contacts between the conductor and the electrodes carrying current to and from the material1, 2, 3. According to theoretical considerations4, this concept remains valid down to the limit of single-molecule junctions5. Exploring this limit in experiments requires atomic-scale control of the junction geometry. Here we present a method for probing the current through a single C60 molecule while changing, one by one, the number of atoms in the electrode that are in contact with the molecule. We show quantitatively that the contact geometry has a strong influence on the conductance. We also find a crossover from a regime in which the conductance is limited by charge injection at the contact to a regime in which the conductance is limited by scattering at the molecule. Thus, the concepts of ‘good’ and ‘bad’ contacts, commonly used in macro- and mesoscopic physics, can also be applied at the molecular scale.
-http://www.nature.com/nnano/journal/v6/n1/abs/nnano.2010.215.html
 ----
-'''Spin-Torque Ferromagnetic Resonance Induced by the Spin Hall Effect'''
-Luqiao Liu, Takahiro Moriyama, D. C. Ralph, and R. A. Buhrman
+'''Current noise cross correlation mediated by Majorana bound states'''
-We demonstrate that the spin Hall effect in a thin film with strong spin-orbit scattering can excite magnetic precession in an adjacent ferromagnetic film. The flow of alternating current through a Pt/NiFe bilayer generates an oscillating transverse spin current in the Pt, and the resultant transfer of spin angular momentum to the NiFe induces ferromagnetic resonance dynamics. The Oersted field from the current also generates a ferromagnetic resonance signal but with a different symmetry. The ratio of these two signals allows a quantitative determination of the spin current and the spin Hall angle.
+''Hai-Feng Lu, Hai-Zhou Lu, Shun-Qing Shen''
-http://prl.aps.org/abstract/PRL/v106/i3/e036601
+We study the transport properties of a quantum dot-Majorana hybrid system, in which each of paired Majorana bound states is connected to one quantum dot. With the help of non-equilibrium Green's function method, we obtain an exact solution of the Green's functions and calculate the currents through the quantum dots and nonlocal noise cross correlation between the currents. As a function of dot energy levels ϵ1 and ϵ2, we find that for the symmetric level configuration ϵ1=ϵ2, the noise cross correlation is negative in the low lead voltage regime, while it becomes positive with the increase of the lead voltages. Due to the particle-hole symmetry, the cross correlation is always positive in the anti-symmetric case ϵ1=−ϵ2. In contrast, the cross correlation of non-Majorana setups is always positive. For comparison, we also perform the diagonalized master equation calculation to check its applicability. It is found that the diagonalized master equations work well in most regimes of system parameters. Nevertheless, it shows an obvious deviation from the exact solution by the non-equilibrium Green's function method when all eigenenergies of the dot-Majorana hybrid system and simultaneously the energy intervals are comparable to the dot-lead coupling strength.
-----
-'''Interference and Switching of Josephson Current Carried by Nonlocal Spin-Entangled Electrons in a SQUID-Like System with Quantum Dots'''
-Zhi Wang and Xiao Hu
-The Josephson current of spin-entangled electrons through the two branches of a SQUID-like structure with two quantum dots exhibits a magnetic-flux response different from the conventional Josephson current. Because of their interference, the period of maximum Josephson current changes from h/2e to h/e, which can be used for detecting the Cooper-pair splitting efficiency. The nonlocal spin entanglement provides a quantum mechanical functionale for switching on and off this novel Josephson current, and explicitly a switch is formulated by including a pilot junction. It is shown that the device can be used to measure the magnitude of split-tunneling Josephson current.
+http://arxiv.org/abs/1411.4260
-http://prl.aps.org/abstract/PRL/v106/i3/e037002
 ----
-== Dec. 16. - Jan. 09. (2011) ==
+'''Detecting bit-flip errors in a logical qubit using stabilizer measurements'''
-''Válogatta: Csontos Miklós''
+''D. Ristè, S. Poletto, M.-Z. Huang, A. Bruno, V. Vesterinen, O.-P. Saira, L. DiCarlo''
-----
-'''Signatures of Wigner localization in epitaxially grown nanowires'''
-L. H. Kristinsdóttir, J. C. Cremon, H. A. Nilsson, H. Q. Xu, L. Samuelson, H. Linke, A. Wacker, and S. M. Reimann
+Quantum data is susceptible to decoherence induced by the environment and to errors in the hardware processing it. A future fault-tolerant quantum computer will use quantum error correction (QEC) to actively protect against both. In the smallest QEC codes, the information in one logical qubit is encoded in a two-dimensional subspace of a larger Hilbert space of multiple physical qubits. For each code, a set of non-demolition multi-qubit measurements, termed stabilizers, can discretize and signal physical qubit errors without collapsing the encoded information. Experimental demonstrations of QEC to date, using nuclear magnetic resonance, trapped ions, photons, superconducting qubits, and NV centers in diamond, have circumvented stabilizers at the cost of decoding at the end of a QEC cycle. This decoding leaves the quantum information vulnerable to physical qubit errors until re-encoding, violating a basic requirement for fault tolerance. Using a five-qubit superconducting processor, we realize the two parity measurements comprising the stabilizers of the three-qubit repetition code protecting one logical qubit from physical bit-flip errors. We construct these stabilizers as parallelized indirect measurements using ancillary qubits, and evidence their non-demolition character by generating three-qubit entanglement from superposition states. We demonstrate stabilizer-based quantum error detection (QED) by subjecting a logical qubit to coherent and incoherent bit-flip errors on its constituent physical qubits. While increased physical qubit coherence times and shorter QED blocks are required to actively safeguard quantum information, this demonstration is a critical step toward larger codes based on multiple parity measurements.
-It was predicted by Wigner in 1934 that an electron gas will undergo a transition to a crystallized state when its density is very low. Whereas significant progress has been made toward the detection of electronic Wigner states, their clear and direct experimental verification still remains a challenge. Here we address signatures of Wigner molecule formation in the transport properties of InSb nanowire quantum-dot systems, where a few electrons may form localized states depending on the size of the dot (i.e., the electron density). Using a configuration interaction approach combined with an appropriate transport formalism, we are able to predict the transport properties of these systems, in excellent agreement with experimental data. We identify specific signatures of Wigner state formation, such as the strong suppression of the antiferromagnetic coupling, and are able to detect the onset of Wigner localization, both experimentally and theoretically, by studying different dot sizes.
+http://arxiv.org/abs/1411.5542
-http://prb.aps.org/abstract/PRB/v83/i4/e041101
 ----
-'''Kondo Quantum Criticality of Magnetic Adatoms in Graphene'''
-Bruno Uchoa, T. G. Rappoport, and A. H. Castro Neto
+'''In-situ Raman Spectroscopy of the Graphene / Water Interface of a Solution-Gated Field Effect Transistor: Electron-Phonon Coupling and Spectroelectrochemistry'''
-We examine the exchange Hamiltonian for magnetic adatoms in graphene with localized inner shell states. On symmetry grounds, we predict the existence of a class of orbitals that lead to a distinct class of quantum critical points in graphene, where the Kondo temperature scales as TK∝|J-Jc|1/3 near the critical coupling Jc, and the local spin is effectively screened by a super-Ohmic bath. For this class, the RKKY interaction decays spatially with a fast power law ∼1/R7. Away from half filling, we show that the exchange coupling in graphene can be controlled across the quantum critical region by gating. We propose that the vicinity of the Kondo quantum critical point can be directly accessed with scanning tunneling probes and gating.
+''J. Binder, J. M. Urban, R. Stepniewski, W. Strupinski, A. Wysmolek''
-http://prl.aps.org/abstract/PRL/v106/i1/e016801
+We present a novel measurement approach which combines aqueous solution-gated field effect transistors based on epitaxial bilayer graphene on 4H-SiC (0001) with simultaneous Raman spectroscopy. Since SiC is transparent in the visible wavelength range, we took advantage of the fact that one can measure graphene through the substrate. By sweeping the gate voltage, we observed Raman signatures related to the resonant electron-phonon coupling. The positions of these features allowed the extraction of the geometrical capacitance of the system and thus facilitated the accurate calculation of the Fermi levels for bilayer graphene. An intentional application of higher gate voltages allowed us to trigger electrochemical reactions, which we followed in-situ with Raman spectroscopy. The reactions showed a partially reversible character, which was monitored by an emergence / disappearance of peaks assigned to C-H and Si-H vibration modes as well as an increase / decrease of the defect-related Raman D band intensity. Our setup provides chemically specific information and electrical control by using a graphene solution-gated field-effect transistor and constitutes a highly interesting platform for future spectroelectrochemical research on electrically induced sorption processes of graphene in the micrometer scale.
-----
-'''Coexistence of Coulomb Blockade and Zero Bias Anomaly in a Strongly Coupled Nanodot'''
-L. Bitton, D. B. Gutman, R. Berkovits, and A. Frydman
+http://arxiv.org/abs/1411.4837
-The current-voltage characteristics through a metallic nanoparticle which is well coupled to a metallic lead are measured. It is shown that the I–V curves are composed of two contributions. One is a suppression of the tunneling conductivity at the Fermi level, and the second is an oscillating feature which shifts with gate voltage. The results indicate that zero-bias anomaly and Coulomb blockade phenomena coexist in an asymmetric strongly coupled zero-dimensional system.
-http://prl.aps.org/abstract/PRL/v106/i1/e016803
-----
-''Válogatta: Makk Péter''
 ----
-'''Sublattice asymmetry and spin-orbit interaction induced out-of-plane spin polarization of photoelectrons'''
-Peter Rakyta, Andor Kormanyos, Jozsef Cserti
+'''Study of dynamical spin injection at ferromagnet-graphene interfaces'''
-We study theoretically the effect of spin-orbit coupling and sublattice asymmetry in graphene on the spin polarization of photoelectrons. We show that sublattice asymmetry in graphene not only opens a gap in the band structure but in case of finite spin-orbit interaction it also gives rise to an out-of-plane spin polarization of electrons close to the Dirac point of the Brillouin zone. This can be detected by measuring the spin polarization of photoelectrons and therefore spin resolved photoemission spectroscopy can reveal the presence of a band gap even if it is too small to be observed directly by angle resolved photoemission spectroscopy because of the finite resolution of measurements or because the sample is $p$-doped. We present analytical and numerical calculations on the energy and linewidth dependence of photoelectron intensity distribution and spin polarization.
+''S. Singh, A. Ahmadi, C.T. Cherian, E. R. Mucciolo, E. del Barco, B. Özyilmaz''
-http://arxiv.org/abs/1101.0624
+We present a study of dynamical spin injection from a three-dimensional ferromagnet into two-dimensional single-layer graphene. Comparative ferromagnetic resonance (FMR) studies of ferromagnet/graphene strips buried underneath the central line of a coplanar waveguide show that the FMR linewidth broadening is the largest when the graphene layer protrudes laterally away from the ferromagnetic strip, indicating that the spin current is injected into the graphene areas away from the area directly underneath the ferromagnet being excited. Our results confirm that the observed damping is indeed a signature of dynamical spin injection, wherein a pure spin current is pumped into the single-layer graphene from the precessing magnetization of the ferromagnet. The observed spin pumping efficiency is difficult to reconcile with the expected backflow of spins according to the standard spin pumping theory and the characteristics of graphene, and constitutes an enigma for spin pumping in two-dimensional structures.
-----
-'''Quasi one-dimensional transport in single GaAs/AlGaAs core-shell nanowires'''
-Damien Lucot, Fauzia Jabeen, Jean-Christophe Harmand, Gilles Patriarche, Romain Giraud, Giancarlo Faini, Dominique Mailly
+http://arxiv.org/abs/1411.5339
-We present an original approach to fabricate single GaAs/AlGaAs core-shell nanowire with robust and reproducible transport properties. The core-shell structure is buried in an insulating GaAs overlayer and connected as grown in a two probe set-up using the highly doped growth substrate and a top diffused contact. The measured conductance shows a non-ohmic behavior with temperature and voltage-bias dependences following power laws, as expected for a quasi-1D system.
-http://arxiv.org/abs/1101.0421
 ----
-'''Real-time observation of discrete Andreev tunneling events'''
-V. F. Maisi, O.-P. Saira, Yu. A. Pashkin, J. S. Tsai, D. V. Averin, J. P. Pekola
+'''Inverted singlet-triplet qubit coded on a two-electron double quantum dot'''
-Electronic transport across a boundary between conductors with dissimilar carriers is a non-trivial process. Of particular interest in this respect is the transport through a superconductor - normal metal interface that at low energies is dominated by the so-called Andreev reflection. In this process, a Cooper pair in a superconductor is converted into two electrons (quasiparticles) in the normal metal, or, oppositely, two electrons combine into a pair in a reverse event. We have performed a real-time detection of these events and directly distinguished them from one-electron processes providing a direct proof of the existence of the two-electron Andreev transitions and allowing us to measure their rate. Since the rate depends on coherence properties of the wavefunctions of two electrons, it gives a fingerprint of the junction. The tunneling rates we observe indicate that the standard barriers are quite far from being atomically flat insulator layers.
+''Sebastian Mehl and David P. DiVincenzo''
-http://arxiv.org/abs/1012.5750
+The sz=0 spin configuration of two electrons confined at a double quantum dot (DQD) encodes the singlet-triplet qubit (STQ). We introduce the inverted STQ (ISTQ) that emerges from the setup of two quantum dots (QDs) differing significantly in size and out-of-plane magnetic fields. The strongly confined QD has a two-electron singlet ground state, but the weakly confined QD has a two-electron triplet ground state in the sz=0 subspace. Spin-orbit interactions act nontrivially on the sz=0 subspace and provide universal control of the ISTQ together with electrostatic manipulations of the charge configuration. GaAs and InAs DQDs can be operated as ISTQs under realistic noise conditions.
-----
-== Dec. 9. - Dec. 15. (2010) ==
+http://journals.aps.org/prb/abstract/10.1103/PhysRevB.90.195424
-''Válogatta: Makk Péter''
 ----
-'''Spin reconstruction in quantum wires subject to a perpendicular magnetic field'''
-Gilad Barak, Loren N. Pfeiffer, Ken W. West, Bertrand I. Halperin, Amir Yacoby
+'''Majorana fermions in Ge/Si hole nanowires'''
-We study the effects of a perpendicular magnetic field on the spin and charge distribution across a quantum wire. Using momentum resolved tunneling between two parallel wires we measure the dispersion relation for different perpendicular magnetic fields. We find that as the magnetic field increases, a strip of spin polarized electrons separates in the cross section of the wire. We provide a quantitative description of the emerging structure within a Hartree-Fock approximation, showing that it results from exchange interaction between electrons in the wire. We discuss the relation of these results to the structure of Quantum Hall edge states.
+''Franziska Maier, Jelena Klinovaja, and Daniel Loss''
-http://arxiv.org/abs/1012.1845
+We consider Ge/Si core/shell nanowires with hole states coupled to an s-wave superconductor in the presence of electric and magnetic fields. We employ a microscopic model that takes into account material-specific details of the band structure such as strong and electrically tunable Rashba-type spin-orbit interaction and g factor anisotropy for the holes. In addition, the proximity-induced superconductivity Hamiltonian is derived starting from a microscopic model. In the topological phase, the nanowires host Majorana fermions with localization lengths that depend strongly on both the magnetic and electric fields. We identify the optimal regime in terms of the directions and magnitudes of the fields in which the Majorana fermions are the most localized at the nanowire ends. In short nanowires, the Majorana fermions hybridize and form a subgap fermion whose energy is split away from zero and oscillates as a function of the applied fields. The period of these oscillations could be used to measure the dependence of the spin-orbit interaction on the applied electric field and the g factor anisotropy.
-----
-'''Nonequilibrium transport in molecular junctions with strong electron-phonon interactions '''
+http://journals.aps.org/prb/abstract/10.1103/PhysRevB.90.195421
-R. C. Monreal, F. Flores, A. Martin-Rodero
-We present a combined theoretical approach to study the nonequilibrium transport properties of nanoscale systems coupled to metallic electrodes and exhibiting strong electron-phonon interactions. We use the Keldysh Green function formalism to generalize beyond linear theory in the applied voltage an equation of motion method and an interpolative self-energy approximation previously developed in equilibrium. We analyze the specific characteristics of inelastic transport appearing in the intensity versus voltage curves and in the conductance, providing qualitative criteria for the sign of the step-like features in the conductance. Excellent overall agreement between both approaches is found for a wide range of parameters.
-http://arxiv.org/abs/1012.2015
 ----
-'''Probing Charge Transfer at Surfaces Using Graphene Transistors'''
-Pierre L. Levesque*†‡, Shadi S. Sabri†§, Carla M. Aguirre†, Jonathan Guillemette†§, Mohamed Siaj†, Patrick Desjardins†, Thomas Szkopek*†§, and Richard Martel*†‡
+'''Revealing Topological Superconductivity in Extended Quantum Spin Hall Josephson Junctions'''
-Graphene field effect transistors (FETs) are extremely sensitive to gas exposure. Charge transfer doping of graphene FETs by atmospheric gas is ubiquitous but not yet understood. We have used graphene FETs to probe minute changes in electrochemical potential during high-purity gas exposure experiments. Our study shows quantitatively that electrochemistry involving adsorbed water, graphene, and the substrate is responsible for doping. We not only identify the water/oxygen redox couple as the underlying mechanism but also capture the kinetics of this reaction. The graphene FET is highlighted here as an extremely sensitive potentiometer for probing electrochemical reactions at interfaces, arising from the unique density of states of graphene. This work establishes a fundamental basis on which new electrochemical nanoprobes and gas sensors can be developed with graphene.
+''Shu-Ping Lee, Karen Michaeli, Jason Alicea, and Amir Yacoby''
-http://pubs.acs.org/doi/abs/10.1021/nl103015w
+Quantum spin Hall–superconductor hybrids are promising sources of topological superconductivity and Majorana modes, particularly given recent progress on HgTe and InAs/GaSb. We propose a new method of revealing topological superconductivity in extended quantum spin Hall Josephson junctions supporting “fractional Josephson currents.” Specifically, we show that as one threads magnetic flux between the superconductors, the critical current traces an interference pattern featuring sharp fingerprints of topological superconductivity—even when noise spoils parity conservation.
-----
-'''Nonvolatile Memory Functionality of ZnO Nanowire Transistors Controlled by Mobile Protons'''
-Jongwon Yoon†§, Woong-Ki Hong†§, Minseok Jo†, Gunho Jo†, Minhyeok Choe†, Woojin Park†, Jung Inn Sohn‡, Stanko Nedic‡, Hyungsang Hwang†, Mark E. Welland‡, and Takhee Lee†*
+http://journals.aps.org/prl/abstract/10.1103/PhysRevLett.113.197001
-We demonstrated the nonvolatile memory functionality of ZnO nanowire field effect transistors (FETs) using mobile protons that are generated by high-pressure hydrogen annealing (HPHA) at relatively low temperature (400 °C). These ZnO nanowire devices exhibited reproducible hysteresis, reversible switching, and nonvolatile memory behaviors in comparison with those of the conventional FET devices. We show that the memory characteristics are attributed to the movement of protons between the Si/SiO2 interface and the SiO2/ZnO nanowire interface by the applied gate electric field. The memory mechanism is explained in terms of the tuning of interface properties, such as effective electric field, surface charge density, and surface barrier potential due to the movement of protons in the SiO2 layer, consistent with the UV photoresponse characteristics of nanowire memory devices. Our study will further provide a useful route of creating memory functionality and incorporating proton-based storage elements onto a modified CMOS platform for FET memory devices using nanomaterials.
-http://pubs.acs.org/doi/abs/10.1021/nn102633z
 ----
-'''Dephasing time of GaAs electron-spin qubits coupled to a nuclear bath exceeding 200 μs'''
-Hendrik Bluhm, Sandra Foletti, Izhar Neder, Mark Rudner, Diana Mahalu, Vladimir Umansky & Amir Yacoby
+'''Axially Tunable Carbon Nanotube Resonators Using Co-integrated Microactuators'''
-Qubits, the quantum mechanical bits required for quantum computing, must retain their quantum states for times long enough to allow the information contained in them to be processed. In many types of electron-spin qubits, the primary source of information loss is decoherence due to the interaction with nuclear spins of the host lattice. For electrons in gate-defined GaAs quantum dots, spin-echo measurements have revealed coherence times of about 1 μs at magnetic fields below 100 mT (refs 1, 2). Here, we show that coherence in such devices can survive much longer, and provide a detailed understanding of the measured nuclear-spin-induced decoherence. At fields above a few hundred millitesla, the coherence time measured using a single-pulse spin echo is 30 μs. At lower fields, the echo first collapses, but then revives at times determined by the relative Larmor precession of different nuclear species. This behaviour was recently predicted3, 4, and can, as we show, be quantitatively accounted for by a semiclassical model for the dynamics of electron and nuclear spins. Using a multiple-pulse Carr–Purcell–Meiboom–Gillecho sequence, the decoherence time can be extended to more than 200 μs, an improvement by two orders of magnitude compared with previous measurements1, 2, 5.
+''Stuart Truax , Shih-Wei Lee , Matthias Muoth , and Christofer Hierold *''
-http://www.nature.com/nphys/journal/vaop/ncurrent/full/nphys1856.html
+Tuning of the mechanical resonance frequency of single-walled carbon nanotubes (SWCNTs) is achieved by application of uniaxial strain by purely mechanical means, utilizing both directly grown and dry-transferred SWCNTs. The induction of a beam-to-string transition is achieved, resulting in an axial tension sensitivity of 9.4 × 1010 Hz/ε in the vibrating string regime. Increases in the resonant Q-factor, removal of residual slack, and resonance frequency changes from 10 to 60 MHz are affected.
-----
+http://pubs.acs.org/doi/abs/10.1021/nl501853w
-'''Andreev bound states in supercurrent-carrying carbon nanotubes revealed'''
-J-D. Pillet, C. H. L. Quay, P. Morfin, C. Bena, A. Levy Yeyati & P. Joyez
-Carbon nanotubes (CNTs) are not intrinsically superconducting but they can carry a supercurrent when connected to superconducting electrodes1, 2, 3, 4. This supercurrent is mainly transmitted by discrete entangled electron–hole states confined to the nanotube, called Andreev bound states (ABS). These states are a key concept in mesoscopic superconductivity as they provide a universal description of Josephson-like effects in quantum-coherent nanostructures (for example molecules, nanowires, magnetic or normal metallic layers) connected to superconducting leads5. We report here the first tunnelling spectroscopy of individually resolved ABS, in a nanotube–superconductor device. Analysing the evolution of the ABS spectrum with a gate voltage, we show that the ABS arise from the discrete electronic levels of the molecule and that they reveal detailed information about the energies of these levels, their relative spin orientation and the coupling to the leads. Such measurements hence constitute a powerful new spectroscopic technique capable of elucidating the electronic structure of CNT-based devices, including those with well-coupled leads. This is relevant for conventional applications (for example, superconducting or normal transistors, superconducting quantum interference devices3 (SQUIDs)) and quantum information processing (for example, entangled electron pair generation6, 7, ABS-based qubits8). Finally, our device is a new type of d.c.-measurable SQUID.
-http://www.nature.com/nphys/journal/v6/n12/full/nphys1811.html
 ----
-'''Coherent electron–nuclear coupling in oligothiophene molecular wires'''
+'''Giant Magnetoconductance Oscillations in Hybrid Superconductor−Semiconductor Core/Shell Nanowire Devices'''
-Jascha Repp, Peter Liljeroth & Gerhard Meyer
+''Ö. Gül †, H. Y. Günel *†‡, H. Lüth †, T. Rieger †, T. Wenz †, F. Haas †, M. Lepsa †, G. Panaitov §, D. Grützmacher †, and Th. Schäpers *†''
-In molecular electronics individual molecules serve as electronic devices. In these systems, electron–vibron (e–ν) coupling can be expected to lead to new physical phenomena and potential device functions1, 2, 3. In previous studies of molecular wires, the e–ν coupling occurred as a result of the well-known Franck–Condon principle, for which the Born–Oppenheimer approximation holds. This means that after a vibronic excitation, the electrons and the vibrations evolve independently from each other. Here we show that this simple picture changes markedly when two electronic levels in a molecule are coupled by a molecular vibration4, 5. In molecular wires we observe a non-Born–Oppenheimer regime, for which a coherent coupling of electronic and nuclear motion emerges6. This phenomenon should occur in all systems with strong electron–vibration coupling and an electronic level spacing of the order of vibrational energies. The coherent coupling of electronic and nuclear motion could be used to implement mechanical control of electron transport in molecular electronics.
-http://www.nature.com/nphys/journal/v6/n12/full/nphys1802.html
-----
-'''Vibrational and electronic heating in nanoscale junctions'''
-Daniel R. Ward, David A. Corley, James M. Tour & Douglas Natelson
+The magnetotransport of GaAs/InAs core/shell nanowires contacted by two superconducting Nb electrodes is investigated, where the InAs shell forms a tube-like conductive channel around the highly resistive GaAs core. By applying a magnetic field along the nanowire axis, regular magnetoconductance oscillations with an amplitude in the order of e2/h are observed. The oscillation amplitude is found to be larger by 2 orders of magnitude compared to the measurements of a reference sample with normal metal contacts. For the Nb-contacted core/shell nanowire the oscillation period corresponds to half a flux quantum Φ0/2 = h/2e in contrast to the period of Φ0 of the reference sample. The strongly enhanced magnetoconductance oscillations are explained by phase-coherent resonant Andreev reflections at the Nb-core/shell nanowire interface.
-Understanding and controlling the flow of heat is a major challenge in nanoelectronics. When a junction is driven out of equilibrium by light or the flow of electric charge, the vibrational and electronic degrees of freedom are, in general, no longer described by a single temperature1, 2, 3, 4, 5, 6. Moreover, characterizing the steady-state vibrational and electronic distributions in situ is extremely challenging. Here, we show that surface-enhanced Raman emission may be used to determine the effective temperatures for both the vibrational modes and the electrons in the current in a biased metallic nanoscale junction decorated with molecules7. Molecular vibrations show mode-specific pumping by both optical excitation8 and d.c. current9, with effective temperatures exceeding several hundred kelvin. Anti-Stokes electronic Raman emission10, 11 indicates that the effective electronic temperature at bias voltages of a few hundred millivolts can reach values up to three times the values measured when there is no current. The precise effective temperatures are model-dependent, but the trends as a function of bias conditions are robust, and allow direct comparisons with theories of nanoscale heating.
+http://pubs.acs.org/doi/abs/10.1021/nl502598s
-http://www.nature.com/nnano/journal/vaop/ncurrent/full/nnano.2010.240.html
 ----
-'''Scanning probe microscopy: STM hits the fast lane'''
+'''Quantum Noise and Asymmetric Scattering of Electrons and Holes in Graphene'''
-Alexander Ako Khajetoorians & André Kubetzka
+''Atikur Rahman , Janice Wynn Guikema , and Nina Marković *''
-A pump–probe approach allows the relaxation times of single spins to be measured.
+We present measurements of quantum interference noise in double-gated single layer graphene devices at low temperatures. The noise characteristics show a nonmonotonic dependence on carrier density, which is related to the interplay between charge inhomogeneity and different scattering mechanisms. Linearly increasing 1/f noise at low carrier densities coincides with the observation of weak localization, suggesting the importance of short-range disorder in this regime. Using perpendicular and parallel p–n junctions, we find that the observed asymmetry of the noise with respect to the Dirac point can be related to asymmetric scattering of electrons and holes on the disorder potential.
-http://www.nature.com/nnano/journal/v5/n12/full/nnano.2010.243.html
+http://pubs.acs.org/doi/abs/10.1021/nl503276s
-----
-'''Electroluminescence from a single nanotube–molecule–nanotube junction'''
-Christoph W. Marquardt, Sergio Grunder, Alfred Bl strokeaszczyk, Simone Dehm, Frank Hennrich, Hilbert v. Löhneysen, Marcel Mayor & Ralph Krupke
-The positioning of single molecules between nanoscale electrodes1, 2, 3, 4, 5, 6, 7, 8 has allowed their use as functional units in electronic devices. Although the electrical transport in such devices has been widely explored, optical measurements have been restricted to the observation of electroluminescence from nanocrystals and nanoclusters9, 10 and from molecules in a scanning tunnelling microscope setup11, 12. In this Letter, we report the observation of electroluminescence from the core of a rod-like molecule between two metallic single-walled carbon nanotube electrodes forming a rigid solid-state device. We also develop a simple model to explain the onset voltage for electroluminescence. These results suggest new characterization and functional possibilities, and demonstrate the potential of carbon nanotubes for use in molecular electronics.
-http://www.nature.com/nnano/journal/v5/n12/full/nnano.2010.230.html
 ----
-'''Kondo effect of a Co atom on Cu(111) in contact with an iron tip'''
-N. Néel, J. Kröger*, and R. Berndt
+'''Multimode Silicon Nanowire Transistors'''
-Single Co atoms, which exhibit a Kondo effect on Cu(111), are contacted with Cu and Fe tips in a low-temperature scanning tunneling microscope. With Fe tips, the Kondo effect persists with the Abrikosov-Suhl resonance significantly broadened. In contrast, for Cu-covered W tips, the resonance width remains almost constant throughout the tunneling and contact ranges. The distinct changes in the line width are interpreted in terms of modifications of the Co d state occupation owing to hybridization with the tip apex atoms.
+''Sebastian Glassner †, Clemens Zeiner †, Priyanka Periwal ‡§, Thierry Baron ‡§, Emmerich Bertagnolli †, and Alois Lugstein *†''
-http://prb.aps.org/abstract/PRB/v82/i23/e235303
+The combined capabilities of both a nonplanar design and nonconventional carrier injection mechanisms are subject to recent scientific investigations to overcome the limitations of silicon metal oxide semiconductor field effect transistors. In this Letter, we present a multimode field effect transistors device using silicon nanowires that feature an axial n-type/intrinsic doping junction. A heterostructural device design is achieved by employing a self-aligned nickel-silicide source contact. The polymorph operation of the dual-gate device enabling the configuration of one p- and two n-type transistor modes is demonstrated. Not only the type but also the carrier injection mode can be altered by appropriate biasing of the two gate terminals or by inverting the drain bias. With a combined band-to-band and Schottky tunneling mechanism, in p-type mode a subthreshold swing as low as 143 mV/dec and an ON/OFF ratio of up to 104 is found. As the device operates in forward bias, a nonconventional tunneling transistor is realized, enabling an effective suppression of ambipolarity. Depending on the drain bias, two different n-type modes are distinguishable. The carrier injection is dominated by thermionic emission in forward bias with a maximum ON/OFF ratio of up to 107 whereas in reverse bias a Schottky tunneling mechanism dominates the carrier transport.
-----
-'''Controlling Electron-Phonon Interactions in Graphene at Ultrahigh Carrier Densities'''
-Dmitri K. Efetov and Philip Kim
-We report on the temperature dependent electron transport in graphene at different carrier densities n. Employing an electrolytic gate, we demonstrate that n can be adjusted up to 4×1014  cm-2 for both electrons and holes. The measured sample resistivity ρ increases linearly with temperature T in the high temperature limit, indicating that a quasiclassical phonon distribution is responsible for the electron scattering. As T decreases, the resistivity decreases more rapidly following ρ(T)∼T4. This low temperature behavior can be described by a Bloch-Grüneisen model taking into account the quantum distribution of the two-dimensional acoustic phonons in graphene. We map out the density dependence of the characteristic temperature ΘBG defining the crossover between the two distinct regimes, and show that, for all n, ρ(T) scales as a universal function of the normalized temperature T/ΘBG.
+http://pubs.acs.org/doi/abs/10.1021/nl503476t
-http://prl.aps.org/abstract/PRL/v105/i25/e256805
 ----
-== Dec. 2. - Dec. 8. (2010) ==
+'''Realization of the Meminductor'''
-''Válogatta: Balogh Zoltán''
+''Jiahao Han , Cheng Song *, Shuang Gao , Yuyan Wang , Chao Chen , and Feng Pan''
-----
-'''Low Energy Coherent Transport in Metallic Carbon Nanotube Junctions'''
-Authors: A.A. Maarouf, E.J. Mele
+The meminductor was proposed to be a fundamental circuit memdevice parallel with the memristor, linking magnetic flux and current. However, a clear material model or experimental realization of a meminductor has been challenging. Here we demonstrate pinched hysteretic magnetic flux–current signals at room temperature based on the spin Hall magnetoresistance effect in several-nanometer-thick thin films, exhibiting the nonvolatile memorizing property and magnetic energy storage ability of the meminductor. Similar to the parameters of the capacitor, resistor, and inductor, meminductance, LM, is introduced to characterize the capability of the prepared meminductor. Our findings present an indispensable element of memdevices and open an avenue for nanoscale meminductor design and manufacture, which might contribute to low-power electronic circuits, information storage, and artificial intelligence.
-We study the low-energy electronic properties of a junction made of two crossed metallic carbon nanotubes of general chiralities. We derive a tight binding tunneling matrix element that couples low-energy states on the two tubes, which allows us to calculate the contact conductance of the junction. We find that the intrinsic asymmetries of the junction cause the forward and backward hopping probabilities from one tube to another to be different. This defines a zero-field Hall conductance for the junction, which we find to scale inversely with the junction contact conductance. Through a systematic study of the dependence of the junction conductance on different junction parameters, we find that the crossing angle is the dominant factor which determines the magnitude of the conductance.
+http://pubs.acs.org/doi/abs/10.1021/nn502655u
-http://arxiv.org/abs/1012.0355
 ----
-'''Imaging charge density fluctuations in graphene using Coulomb blockade spectroscopy'''
-Authors: A. Deshpande, W. Bao, H. Zhang, Z. Zhao, C.N. Lau, B.J. LeRoy
+== Szept.19-30.==
+''Márton Attila''
-Using scanning tunneling microscopy, we have imaged local charge density fluctuations in monolayer graphene. By placing a small gold nanoparticle on the end of the STM tip, a charge sensor is created. By raster scanning the tip over the surface and using Coulomb blockade spectroscopy, we map the local charge on the graphene. We observe a series of electron and hole doped puddles with a characteristic length scale of about 20 nm. Theoretical calculations for the correlation length of the puddles based on the number of impurities are in agreement with our measurements.
+Előadás: SNS junctions in nanowires with spin-orbit coupling: role of confinement and helicity on the sub-gap spectrum (http://arxiv.org/abs/1410.6074) [[:file:Jc_141028_MA.pptx |pptx (pptx)]]'''
-http://arxiv.org/abs/1012.0374
+'''Photons made to dance together
-----
-'''Anomalous Josephson current via Majorana bound states in topological insulators'''
-Authors: P. A. Ioselevich, M. V. Feigel'man
+Physicists have made two beams of light interact at the level of individual photons.
-We propose a setup involving Majorana bound states (MBS) hosted by a vortex on a superconducting surface of a 3D Topological Insulator (TI). We consider a narrow channel drilled across a TI slab with both sides covered by s-wave superconductor. In the presence of a vortex pinned to such a channel, it acts as a ballistic nanowire connecting the superconducting surfaces, with a pair of MBS localized in it. The energies of the MBS possess a 4\pi-periodic dependence on the superconductive phase difference \phi between the surfaces. It results in the appearence of an anomalous term in the current-phase relation, I_a(\phi) for the supercurrent flowing along the channel between the superconductive surfaces. We have calculated the shape of the 4\pi-periodic function I_a(\phi), as well as the dependence of its amplitude on temperature and system parameters.
+Getting photons to interact is important for all-optical computation and for producing new quantum states of light. Kristin Beck at the Massachusetts Institute of Technology in Cambridge and her colleagues crossed two beams of light inside a cavity filled with trapped and cooled caesium atoms. When photons from each beam tried to pass through the system at the same time, the trapped atoms changed their internal state, allowing only one photon to be transmitted, while the other one was reflected or scattered.
-http://arxiv.org/abs/1012.0407
+The interaction creates two entangled beams of light, which the authors say could eventually be used to improve the accuracy of measurements, such as of a gyroscope's rotation, that would otherwise be limited by the laws of quantum mechanics.
-----
-'''Symmetry breaking in commensurate graphene rotational stacking; a comparison of theory and experiment''''
-J. Hicks, M. Sprinkle, K. Shepperd, F. Wang, A. Tejeda, A. Taleb-Ibrahimi, F. Bertran, P. Le Fèvre, W.A. de Heer, C. Berger, E.H. Conrad
+http://www.nature.com/nature/journal/v513/n7519/full/513463a.html
-Graphene stacked in a Bernal configuration (60 degrees relative rotations between sheets) differs electronically from isolated graphene due to the broken symmetry introduced by interlayer bonds forming between only one of the two graphene unit cell atoms. A variety of experiments have shown that non-Bernal rotations restore this broken symmetry; consequently, these stacking varieties have been the subject of intensive theoretical interest. Most theories predict substantial changes in the band structure ranging from the development of a Van Hove singularity and an angle dependent electron localization that causes the Fermi velocity to go to zero as the relative rotation angle between sheets goes to zero. In this work we show by direct measurement that non-Bernal rotations preserve the graphene symmetry with only a small perturbation due to weak effective interlayer coupling. We detect neither a Van Hove singularity nor any significant change in the Fermi velocity. These results suggest significant problems in our current theoretical understanding of the origins of the band structure of this material.
+-----
-http://arxiv.org/abs/1012.0460
+'''Quantum bits get their first compression
-----
-'''Controlling non-Abelian statistics of Majorana fermions in quasi-one-dimensional wire networks'''
-Authors: Jay D. Sau, D. J. Clarke, S. Tewari
+Without algorithms that compress data to encode information into fewer bits, hard drives would clog up and Internet traffic would slow to a snail's pace. Now, a group of physicists in Canada has shown for the first time that it is possible to compress the kind of data that might be used in the computers of tomorrow — known as quantum bits, or qubits.
-Under appropriate external conditions a spin-orbit coupled semiconductor in proximity to a s-wave superconductor can be in a topological superconducting (TS) phase. In the topological phase, various defects of the order parameter trap zero energy excitations called Majorana bound states. For a semiconductor nanowire, the relevant defects are the two ends of the wire, and each traps a localized zero energy excitation. A network of such nanowires with 1D TS segments separated by non-topological superconducting (NTS) regions has been proposed recently as a platform for topological quantum computation (TQC). For TQC, a primary requirement is that the spatial positions of the Majorana excitations can be pairwise exchanged, and that they follow non-Abelian statistics under such an exchange. Alicea et al. have shown how non-Abelian statistics arises on the wire network by approximately mapping the system to a 1D lattice model of fermions. Here we present an alternative approach to realizing the non-Abelian statistics on a wire-network based on gate-controlled tunneling between Majorana fermions. The non-Abelian phases realized by this scheme are found to be uniquely determined by the microscopic tunneling parameters of a given wire network and can be computed using the Heisenberg equations of motion.
-http://arxiv.org/abs/1012.0561
+http://www.nature.com/news/quantum-bits-get-their-first-compression-1.15961
-----
-'''Energy-efficient mixed mode switching of a multiferroic nanomagnet for logic and memory'''
-Authors: Kuntal Roy, Supriyo Bandyopadhyay, Jayasimha Atulasimha
+-----
-In magnetic memory and logic devices, a magnet's magnetization is usually flipped with a spin polarized current delivering a spin transfer torque (STT). This mode of switching consumes too much energy and considerable energy saving can accrue from using a multiferroic nanomagnet switched with a combination of STT and mechanical stress generated with a voltage (VGS). The VGS mode consumes less energy than STT, but cannot rotate magnetization by more than 90?, so that a combination of the two modes is needed for energy-efficient switching.
+'''Transmission Phase in the Kondo Regime Revealed in a Two-Path Interferometer
-http://arxiv.org/abs/1012.0819
+''S. Takada, C. Bäuerle, M. Yamamoto, K. Watanabe, S. Hermelin, T. Meunier, A. Alex, A. Weichselbaum, J. von Delft, A. Ludwig, A. D. Wieck, and S. Tarucha
-----
-'''Switching energy-delay of all-spin logic devices'''
-Authors: Behtash Behin-Aein, Angik Sarkar, Srikant Srinivasan, Supriyo Datta
+We report on the direct observation of the transmission phase shift through a Kondo correlated quantum dot by employing a new type of two-path interferometer. We observed a clear π/2-phase shift, which persists up to the Kondo temperature TK. Above this temperature, the phase shifts by more than π/2 at each Coulomb peak, approaching the behavior observed for the standard Coulomb blockade regime. These observations are in remarkable agreement with two-level numerical renormalization group calculations. The unique combination of experimental and theoretical results presented here fully elucidates the phase evolution in the Kondo regime.
-The need to find low power alternatives to digital electronic circuits has led to increasing interest in alternative switching schemes like the magnetic quantum cellular automata(MQCA) that store information in nanomagnets which communicate through their magnetic fields. A recent proposal called all spin logic (ASL) proposes to communicate between nanomagnets using spin currents which are spatially localized and can be conveniently routed. The objective of this paper is to present a model for ASL devices that is based on established physics and is benchmarked against available experimental data and to use it to investigate switching energy-delay of ASL devices.
+http://journals.aps.org/prl/abstract/10.1103/PhysRevLett.113.126601
-http://arxiv.org/abs/1012.0861
+-----
-----
-'''Quantum noise of an electromagnetically controlled two level system'''
-Authors: Ching-Kit Chan, L. J. Sham
+'''Entanglement Entropy in Fermi Gases and Anderson’s Orthogonality Catastrophe
-Coherent control of a spin is limited by both the decoherence due to coupling with the environment and noise coming from the quantized control. The quantum noise study of this system is particularly important in fault tolerant quantum computation where a very high fidelity is demanded. Here, we present a time evolution study of a two level system (TLS) interacting with a laser pulse and the electromagnetic vacuum based on the multimode Jaynes-Cummings model. We develop a diagrammatic formalism in which one can easily identify the coherent Rabi oscillation of the TLS and its relaxation from corresponding diagrams. In the small time limit ($t\ll T_1$), where the noise level is small but still an issue to fault tolerant quantum computing, this method gives a quantitative evaluation of the quantum noise of the TLS under an optical control with an arbitrary pulse shape. Furthermore, this approach can be naturally extended from the Markovian to the non-Markovian regime, resulting in dynamics different from that obtained in the optical Bloch analysis. All these calculations are done without any stochastic assumption.
+''A. Ossipov
-http://arxiv.org/abs/1012.1051
+We study the ground-state entanglement entropy of a finite subsystem of size L of an infinite system of noninteracting fermions scattered by a potential of finite range a. We derive a general relation between the scattering matrix and the overlap matrix and use it to prove that for a one-dimensional symmetric potential the von Neumann entropy, the Rényi entropies, and the full counting statistics are robust against potential scattering, provided that L/a≫1. The results of numerical calculations support the validity of this conclusion for a generic potential.
-----
-'''Ballistic transport at room temperature in micrometer size multigraphene'''
-Authors: S. Dusari, J. Barzola-Quiquia, P. Esquinazi, N. García
+http://journals.aps.org/prl/abstract/10.1103/PhysRevLett.113.130402
-The intrinsic values of the carriers mobility and density of the graphene layers inside graphite, the well known structure built on these layers in the Bernal stacking configuration, are not well known mainly because most of the research was done in rather bulk samples where lattice defects hide their intrinsic values. By measuring the electrical resistance through microfabricated constrictions in micrometer small graphite flakes of a few tens of nanometers thickness we studied the ballistic behavior of the carriers. We found that the carriers' mean free path is micrometer large with a mobility $\mu \simeq 6 \times 10^6 $cm$^2$/Vs and a carrier density $n \simeq 7 \times 10^8 $cm$^{-2}$ per graphene layer at room temperature. These distinctive transport and ballistic properties have important implications for understanding the values obtained in single graphene and in graphite as well as for implementing this last in nanoelectronic devices.
+-----
-http://arxiv.org/abs/1012.1100
+'''Experimental realization of a Coulomb blockade refrigerator
-----
-'''Enhanced DNA sequencing performance through edge-hydrogenation of graphene electrodes'''
-Authors: Yuhui He, Ralph H. Scheicher, Anton Grigoriev, Rajeev Ahuja, Shibing Long, ZongLiang Huo, Ming Liu
+''A. V. Feshchenko, J. V. Koski, J. P. Pekola
-We propose using graphene electrodes with hydrogenated edges for solid-state nanopore-based DNA sequencing, and perform molecular dynamics simulations in conjunction with electronic transport calculations to explore the potential merits of this idea. The results of our investigation show that, compared to the unhydrogenated system, edge-hydrogenated graphene electrodes facilitate the temporary formation of H-bonds with suitable atomic sites in the translocating DNA molecule. As a consequence, the average conductivity is drastically raised by about 3 orders of magnitude while exhibiting significantly reduced statistical variance. We have furthermore investigated how these results are affected when the distance between opposing electrodes is varied and have identified two regimes: for narrow electrode separation, the mere hindrance due to the presence of protruding hydrogen atoms in the nanopore is deemed more important, while for wider electrode separation, the formation of H-bonds becomes the dominant effect. Based on these findings, we conclude that hydrogenation of graphene electrode edges represents a promising approach to reduce the translocation speed of DNA through the nanopore and substantially improve the accuracy of the measurement process for whole-genome sequencing.
+We present an experimental realization of a Coulomb blockade refrigerator (CBR) based on a single - electron transistor (SET). In the present structure, the SET island is interrupted by a superconducting inclusion to permit charge transport while preventing heat flow. At certain values of the bias and gate voltages, the current through the SET cools one of the junctions. The measurements follow theoretical model down to about 80 mK, which was the base temperature of the current measurements. The observed cooling increases rapidly with decreasing temperature in agreement with the theory, reaching about 15 mK drop at the base temperature. CBR appears as a promising electronic cooler at temperatures well below 100 mK.
-http://arxiv.org/abs/1012.0031
+http://xxx.lanl.gov/abs/1409.5637
-----
-'''Weak magnetism in insulating and superconducting cuprates'''
-G. M. De Luca,*, G. Ghiringhelli, M. Moretti Sala, S. Di Matteo, M. W. Haverkort, H. Berger, V. Bisogni, J. C. Cezar, N. B. Brookes, and M. Salluzzo
+-----
-X-ray magnetic circular dichroism provides evidence of an out-of-plane spin moment in undoped and doped cuprates. In La2CuO4 this moment is related to the canting of the antiferromagnetically ordered Cu2+ spins caused by the Dzyaloshinskii-Moriya interaction within the CuO2 planes. This canting gives rise to the well-known weak ferromagnetism in high magnetic fields. We find a similar behavior in doped compounds, both in the normal and in the superconducting state, but with a different temperature dependence typical of paramagnetic systems. This result suggests that, together with short-range in-plane antiferromagnetic correlations, the Dzyaloshinskii-Moriya interaction survives up to optimal doping and in the superconducting state.
+'''Klein-tunneling transistor with ballistic graphene
-http://prb.aps.org/abstract/PRB/v82/i21/e214504
+''Quentin Wilmart, Salim Berada, David Torrin, V. Hung Nguyen, Gwendal Fève, Jean-Marc Berroir, Philippe Dollfus, Bernard Plaçais
-----
-'''Spin-triplet supercurrent through inhomogeneous ferromagnetic trilayers'''
-Mohammad Alidoust and Jacob Linder
+Today the availability of high mobility graphene up to room temperature makes ballistic transport in nanodevices achievable. In particular, p-n-p transistor in the ballistic regime gives access to the Klein tunneling physics and allows the realization of devices exploiting the optics-like behavior of Dirac Fermions (DF) as in the Vesalego lens or the Fabry P\'erot cavity. Here we propose a Klein tunneling transistor based on geometrical optics of DF. We consider the case of a prismatic active region delimited by a triangular gate, where total internal reflection may occur, which leads to the tunable suppression of the transistor transmission. We calculate the transmission and the current by means of scattering theory and the finite bias properties using Non Equilibrium Green's Function(NEGF) simulation.
-Motivated by a recent experiment [J. W. A. Robinson, J. D. S. Witt, and M. G. Blamire, Science 329, 5987 (2010)], we report here the possibility of establishing a long-range spin-triplet supercurrent through an inhomogeneous ferromagnetic region consisting of a Ho∣Co∣Ho trilayer sandwiched between conventional s-wave superconducting leads. We utilize a full numerical solution in the diffusive regime of transport and study the behavior of the supercurrent for various experimentally realistic configurations of the ferromagnetic trilayer. We obtain qualitatively very good agreement with experimental data regarding the behavior of the supercurrent as a function of the width of the Co layer, LCo. Moreover, we find a synthesis of 0-π oscillations with superimposed rapid oscillations when varying the width of the Ho layers symmetrically, which pertain specifically to the spiral magnetization texture in Ho. Although we are not able to reproduce the anomalous sharp peaks in the supercurrent vs Ho-layer thickness observed experimentally in this regime, the results obtained are quite sensitive to the exact magnetization profile in the Ho layers. This might be the reason for the discrepancy between our results and the experimental reported data for this particular aspect. We also investigate the supercurrent in a system where the intrinsically inhomogeneous Ho ferromagnets are replaced with domain-wall ferromagnets and find similar behavior as in the Ho∣Co∣Ho case. Furthermore, we propose magnetic Josephson junctions including only a domain-wall ferromagnet and a homogeneous ferromagnetic layer. The hybrid structure not only is simple regarding the magnetization profile but also offers a tunable long-range spin-triplet supercurrent. Finally, we discuss some experimental aspects of our findings.
+http://xxx.lanl.gov/abs/1409.6170
-http://prb.aps.org/abstract/PRB/v82/i22/e224504
+-----
-----
-'''Imaging the electron density in solids by using multi-Brillouin-zone angle resolved photoelectron spectroscopy'''
-W. S. Jung, C. S. Leem, Chul Kim, S. R. Park, S. Y. Park, B. J. Kim, E. Rotenberg, and C. Kim
+'''Directly accessible entangling gates for capacitively coupled singlet-triplet qubits
-We propose a method to measure the electron density in the real space by using angle resolved photoelectron spectroscopy (ARPES). By expanding the wave function in terms of Wannier functions, multi-Brillouin-zone ARPES data contains information on the coefficients of the Wannier function. It is shown, in the case of noninteracting electrons, that ARPES spectral functions in different Brillouin zones are related to the absolute value of the Fourier components of the initial states. In addition, the phases, which are a pseudospin in the graphene, of these components are shown to be real numbers in the function of ARPES intensity. We simulate ARPES data from tight-binding model to obtain phase information. This information combined with a proper consideration of the electronic potential can be used to construct the real-space wave function.
+''Fernando A. Calderon-Vargas, Jason P. Kestner
-http://prb.aps.org/abstract/PRB/v82/i23/e235105
+The recent experimental advances in capacitively coupled singlet-triplet qubits, particularly the demonstration of entanglement, opens the question of what type of entangling gates the system's Hamiltonian can produce directly via a single square pulse. We address this question by considering the system's Hamiltonian from first principles and using the representation of its nonlocal properties in terms of local invariants. In the analysis we include the three different ways in which the system can be biased and their effect on the generation of entangling gates. We find that, in one of the possible biasing modes, the Hamiltonian has an especially simple form, which can directly generate a wide range of different entangling gates including the iSWAP gate. Moreover, using the complete form of the Hamiltonian we find that, for any biasing mode, a CNOT gate can be generated directly.
-----
-'''Spin-orbit coupling and phase coherence in InAs nanowires'''
-S. Estévez Hernández, M. Akabori, K. Sladek, Ch. Volk, S. Alagha, H. Hardtdegen, M. G. Pala, N. Demarina, D. Grützmacher, and Th. Schäpers
+http://xxx.lanl.gov/abs/1409.6292
-We investigated the magnetotransport of InAs nanowires grown by selective-area metal-organic vapor phase epitaxy. In the temperature range between 0.5 and 30 K reproducible fluctuations in the conductance upon variation in the magnetic field or the backgate voltage are observed, which are attributed to electron interference effects in small disordered conductors. From the correlation field of the magnetoconductance fluctuations the phase-coherence length lϕ is determined. At the lowest temperatures lϕ is found to be at least 300 nm while for temperatures exceeding 2 K a monotonous decrease in lϕ with temperature is observed. A direct observation of the weak antilocalization effect indicating the presence of spin-orbit coupling is masked by the strong magnetoconductance fluctuations. However, by averaging the magnetoconductance over a range of gate voltages a clear peak in the magnetoconductance due to the weak antilocalization effect was resolved. By comparison of the experimental data to simulations based on a recursive two-dimensional Green’s-function approach a spin-orbit scattering length of approximately 70 nm was extracted, indicating the presence of strong spin-orbit coupling.
+-----
-http://prb.aps.org/abstract/PRB/v82/i23/e235303
+'''Zeeman splitting spin filter in a single quantum dot electron transport with Coulomb blockade effect
-----
-'''Nanomechanical effects in an Andreev quantum dot'''
-I. A. Sadovskyy, G. B. Lesovik, T. Jonckheere, and T. Martin
+''Wenxi Lai
-We consider a quantum dot with mechanical degrees of freedom which is coupled to superconducting electrodes. A Josephson current is generated by applying a phase difference. In the absence of coupling to vibrations, this setup was previously proposed as a detector of magnetic flux and we wish here to address the effect of the phonon coupling to this detection scheme. We compute the charge on the quantum dot and determine its dependence on the phase difference in the presence of phonon coupling and Coulomb interaction. This allows to identify regions in parameter space with the highest charge to phase sensitivity, which are relevant for flux detection. Further insight about the interplay of such couplings and subsequent entanglement properties between electron and phonon degrees of freedom are gained by computing the von Neumann entropy.
+Electron spin filter induced by Zeeman splitting in a few-electron quantum dot coupled to two normal electrodes is studied considering Coulomb blockade effect. Based on the Anderson model and Liouville-von Neumann equation, equation of motion of the system is derived and analytical solutions are achieved. Transport windows for perfectly polarized current, partially polarized current and non-polarized current induced by the Zeeman splitting energy and Coulomb blockade potential are exploited. We will give the relations of voltage, magnetic field and temperature for high quality spin filtering.
-http://prb.aps.org/abstract/PRB/v82/i23/e235310
+http://xxx.lanl.gov/abs/1409.6389
-----
-'''Disentangling Cooper-pair formation above the transition temperature from the pseudogap state in the cuprates'''
-Takeshi Kondo, Yoichiro Hamaya, Ari D. Palczewski, Tsunehiro Takeuchi, J. S. Wen, Z. J. Xu, Genda Gu, Jörg Schmalian & Adam Kaminski
+-----
-The discovery of the pseudogap in the cuprates1, 2, 3 created significant excitement as it was believed to be a signature of pairing4, in some cases above room temperature. Indeed, a number of experiments detected phase-fluctuating superconductivity above the transition temperature Tc (refs 5, 6, 7 8, 9). However, several recent experiments reported that the pseudogap and superconducting state are characterized by different energy scales10, 11, 12, 13, 14, and probably compete with each other15, 16, leaving open the question of whether the pseudogap is caused by pair formation. Here we report the discovery of a spectroscopic signature of pair formation and demonstrate that in a region commonly referred to as the pseudogap, two distinct states coexist: one that is due to pair formation and persists to an intermediate temperature Tpair<T* and a second—the ‘proper’ pseudogap—characterized by the loss of spectral weight and anomalies in transport properties that extends up to T*. Tpair has a value around 120–150 K even for materials with very different Tc values and it probably sets a limit on the highest attainable Tc in the cuprates.
+'''Majorana bound states without topological superconductivity
-http://www.nature.com/nphys/journal/vaop/ncurrent/full/nphys1851.html
+''Pablo San-Jose, Jorge Cayao, Elsa Prada, Ramón Aguado
-----
-'''Direct observation of single-charge-detection capability of nanowire field-effect transistors'''
-J. Salfi, I. G. Savelyev, M. Blumin, S. V. Nair & H. E. Ruda
+Recent experimental efforts towards the detection of Majorana bound states have focused on creating the conditions for topological superconductivity. Here we demonstrate an alternative route, which achieves fully localised zero-energy Majorana bound states when a topologically trivial superconductor is opened to a normal region. The emergence of Majorana states is a consequence of non-hermitian degeneracies of the resulting open quantum system, while arbitrarily large Majorana lifetimes follow from high junction transparency and helicity of the normal side. At these degeneracies, also known as `exceptional points', both the eigenvalues and the eigenstates coalesce, and acquire Majorana properties (zero-energy, self-conjugation, 4π-periodic braiding...) despite the trivial band topology. Exceptional Majoranas are thus the open-system counterparts of conventional Majorana bound states, to which they are continuously connected, and exhibit all their phenomenology while not requiring topological superconductivity.
-A single localized charge can quench the luminescence of a semiconductor nanowire1, but relatively little is known about the effect of single charges on the conductance of the nanowire. In one-dimensional nanostructures embedded in a material with a low dielectric permittivity, the Coulomb interaction and excitonic binding energy are much larger than the corresponding values when embedded in a material with the same dielectric permittivity2, 3. The stronger Coulomb interaction is also predicted to limit the carrier mobility in nanowires4. Here, we experimentally isolate and study the effect of individual localized electrons on carrier transport in InAs nanowire field-effect transistors, and extract the equivalent charge sensitivity. In the low carrier density regime, the electrostatic potential produced by one electron can create an insulating weak link in an otherwise conducting nanowire field-effect transistor, modulating its conductance by as much as 4,200% at 31 K. The equivalent charge sensitivity, 4 × 10−5 e Hz−1/2 at 25 K and 6 × 10−5 e Hz−1/2 at 198 K, is orders of magnitude better than conventional field-effect transistors5 and nanoelectromechanical systems6, 7, and is just a factor of 20–30 away from the record sensitivity for state-of-the-art single-electron transistors operating below 4 K (ref. 8). This work demonstrates the feasibility of nanowire-based single-electron memories9 and illustrates a physical process of potential relevance for high performance chemical sensors10, 11. The charge-state-detection capability we demonstrate also makes the nanowire field-effect transistor a promising host system for impurities (which may be introduced intentionally or unintentionally) with potentially long spin lifetimes12, 13, because such transistors offer more sensitive spin-to-charge conversion readout than schemes based on conventional field-effect transistors13.
+http://xxx.lanl.gov/abs/1409.7306
-http://www.nature.com/nnano/journal/v5/n10/full/nnano.2010.180.html
+-----
-----
-'''Low-Voltage p- and n-Type Organic Self-Assembled Monolayer Field Effect Transistors'''
-Michael Novak, Alexander Ebel, Timo Meyer-Friedrichsen, Abdesselam Jedaa, Benito F. Vieweg, Guang Yang, Kislon Voitchovsky, Francesco Stellacci, Erdmann Spiecker, Andreas Hirsch, and Marcus Halik
+'''Majorana Fermions in Ge/Si Hole Nanowires
-We report on p- and n-type organic self-assembled monolayer field effect transistors. On the base of quaterthiophene and fullerene units, multifunctional molecules were synthesized, which have the ability to self-assemble and provide multifunctional monolayers. The self-assembly approach, based on phosphonic acids, is very robust and allows the fabrication of functional devices even on larger areas. The p- and n-type transistor devices with only one molecular active layer were demonstrated for transistor channel lengths up to 10 μm. The monolayer composition is proven by electrical experiments and by high-resolution transmission electron microscopy, electron energy loss spectroscopy, XPS, and AFM experiments. Because of the molecular design and the contribution of isolating alkyl chains to the hybrid dielectric, our devices operate at low supply voltages (−4 V to +4 V), which is a key requirement for practical use and simplifies the integration in standard applications. The monolayer devices operate in ambient air and show hole and electron mobilities of 10−5 cm2/(V s) and 10−4 cm2/(V s) respectively. In particular the n-type operation of self-assembled monolayer transistors has not been reported before. Hereby, structure−property relations of the SAMs have been studied. Furthermore an approach to protect the sensitive C60 from immediate degradation within the molecular design is provided.
+''Franziska Maier, Jelena Klinovaja, Daniel Loss
-http://pubs.acs.org/doi/abs/10.1021/nl103200r
+We consider Ge/Si core/shell nanowires with hole states coupled to an s-wave superconductor in the presence of electric and magnetic fields. We employ a microscopic model that takes into account material-specific details of the band structure such as strong and electrically tunable Rashba-type spin-orbit interaction and g factor anisotropy for the holes. In addition, the proximity-induced superconductivity Hamiltonian is derived starting from a microscopic model. In the topological phase, the nanowires host Majorana fermions with localization lengths that depend strongly on both the magnetic and electric fields. We identify the optimal regime in terms of the directions and magnitudes of the fields in which the Majorana fermions are the most localized at the nanowire ends. In short nanowires, the Majorana fermions hybridize and form a subgap fermion whose energy is split away from zero and oscillates as a function of the applied fields. The period of these oscillations could be used to measure the dependence of the spin-orbit interaction on the applied electric field and the g factor anisotropy.
-----
-'''Single-Molecule Mapping of Long-range Electron Transport for a Cytochrome b562 Variant'''
-Eduardo Antonio Della Pia, Qijin Chi, D. Dafydd Jones, J. Emyr Macdonald, Jens Ulstrup, and Martin Elliott
+http://xxx.lanl.gov/abs/1409.8645
-Cytochrome b562 was engineered to introduce a cysteine residue at a surface-exposed position to facilitate direct self-assembly on a Au(111) surface. The confined protein exhibited reversible and fast electron exchange with a gold substrate over a distance of 20 Å between the heme redox center and the gold surface, a clear indication that a long-range electron-transfer pathway is established. Electrochemical scanning tunneling microscopy was used to map electron transport features of the protein at the single-molecule level. Tunneling resonance was directly imaged and apparent molecular conductance was measured, which both show strong redox-gated effects. This study has addressed the first case of heme proteins and offered new perspectives in single-molecule bioelectronics.
+== Szept.13-19.==
+''Tóvári Endre''
-http://pubs.acs.org/doi/abs/10.1021/nl103334q
+'''Crossover from Josephson Effect to Single Interface Andreev Reflection in Asymmetric Superconductor/Nanowire Junctions'''
-----
-'''Graphene Edge from Armchair to Zigzag: The Origins of Nanotube Chirality?'''
-Yuanyue Liu, Alex Dobrinsky, and Boris I. Yakobson
+'H. Y. Günel, N. Borgwardt, I. E. Batov, H. Hardtdegen, K. Sladek, G. Panaitov, D. Grützmacher, and Th. Schäpers'
-The energy of an arbitrary graphene edge, from armchair (A) to zigzag (Z) orientation, is derived in analytical form. It contains a “chemical phase shift” determined by the chemical conditions at the edge. Direct atomistic computations support the universal nature of the relationship, definitive for graphene formation, and shapes of the voids or ribbons. It has further profound implications for nanotube chirality selection and possibly control by chemical means, at the nucleation stage.
+We report on the fabrication and characterization of symmetric nanowire-based Josephson junctions, that is, Al- and Nb-based junctions, and asymmetric junctions employing superconducting Al and Nb. In the symmetric junctions, a clear and pronounced Josephson supercurrent is observed. These samples also show clear signatures of subharmonic gap structures. At zero magnetic field, a Josephson coupling is found for the asymmetric Al/InAs-nanowire/Nb junctions as well. By applying a magnetic field above the critical field of Al or by raising the temperature above the critical temperature of Al the junction can be switched to an effective single-interface superconductor/nanowire structure. In this regime, a pronounced zero-bias conductance peak due to reflectionless tunneling has been observed.
-http://prl.aps.org/abstract/PRL/v105/i23/e235502
-----
-== Nov. 26. - Dec. 1. (2010) ==
+http://pubs.acs.org/doi/abs/10.1021/nl501350v
-''Válogatta: Scherübl Zoltán''
 ----
-'''Functionalized Graphene for High Performance Two-dimensional Spintronics Devices'''
-Authors: Linze Li, Rui Qin, Hong Li, Qihang Liu, Guangfu Luo, Jing Lu, Zhengxiang Gao
+'''Robust Electron Pairing in the Integer Quantum Hall Effect Regime'''
-Using first-principles calculations, we explore the possibility of functionalized graphene as high performance two-dimensional spintronics device. Graphene functionalized with O on one side and H on the other side in the chair conformation is found to be a ferromagnetic metal with a spin-filter efficiency up to 85% at finite bias. The ground state of graphene semi-functionalized with F in the chair conformation is an antiferromagnetic semiconductor, and we construct a magnetoresistive device from it by introducing a magnetic field to stabilize its ferromagnetic metallic state. The resulting room-temperature magnetoresistance is up to 5400%, which is one order of magnitude larger than the available experimental values.
+'Hyungkook Choi, Itamar Sivan, Amir Rosenblatt, Moty Heiblum, Vladimir Umansky, Diana Mahalu'
-arXiv:1011.6014v1
+Electron pairing is a rare phenomenon appearing only in a few unique physical systems; e.g., superconductors and Kondo-correlated quantum dots. Here, we report on an unexpected, but robust, electron "pairing" in the integer quantum Hall effect (IQHE) regime. The pairing takes place within an interfering edge channel circulating in an electronic Fabry-Perot interferometer at a wide range of bulk filling factors, 2<νB<5. The main observations are: (a) High visibility Aharonov-Bohm conductance oscillations with magnetic flux periodicity Δϕ=φ0/2=h/2e (instead of the ubiquitous h/e), with e the electron charge and h the Planck constant; (b) An interfering quasiparticle charge e∗∼2e - revealed by quantum shot noise measurements; and (c) Full dephasing of the h/2e periodicity by induced dephasing of the adjacent edge channel (while keeping the interfering edge channel intact) : a clear realization of inter-channel entanglement. While this pairing phenomenon clearly results from inter-channel interaction, the exact mechanism that leads to e-e attraction within a single edge channel is not clear.
-----
-'''The competition between superconductivity and ferromagnetism in small metallic grains: thermodynamic properties''''
-Authors: K. Van Houcke, Y. Alhassid, S. Schmidt, S. M. A. Rombouts
+http://xxx.lanl.gov/abs/1409.4427
-We study the thermodynamic properties of a small superconducting metallic grain using a quantum Monte Carlo method. The grain is described by the universal Hamiltonian, containing pairing and ferromagnetic exchange correlations. In particular, we study how the thermodynamic signatures of pairing correlations are affected by the spin exchange interaction. We find the exchange interaction effects to be qualitatively different in the BCS and fluctuation-dominated regimes of pairing correlations.
-arXiv:1011.5421v1
 ----
-'''Molecule States in a Gate Tunable Graphene Double Quantum Dot'''
-Authors: L. J. Wang, H. O. Li, Z. Su, T. Tu, G. Cao, C. Zhou, X. J. Hao, G. C. Guo, G. P. Guo
+'''Robust 2D Topological Insulators in van der Waals Heterostructures'''
-We have measured a graphene double quantum dot device with multiple electrostatic gates that are used to enhance control to investigate it. At low temperatures the transport measurements reveal honeycomb charge stability diagrams which can be tuned from weak to strong interdot tunnel coupling regimes. We precisely extract a large interdot tunnel coupling strength for this system allowing for the observation of tunnel-coupled molecular states extending over the whole double dot. This clean, highly controllable system serves as an essential building block for quantum devices in a nuclear-spin-free world.
+'Liangzhi Kou, Shu-Chun Wu, Claudia Felser, Thomas Frauenheim, Changfeng Chen, and Binghai Yan'
-arXiv:1011.5347v1
+We predict a family of robust two-dimensional (2D) topological insulators in van der Waals heterostructures comprising graphene and chalcogenides BiTeX (X = Cl, Br, and I). The layered structures of both constituent materials produce a naturally smooth interface that is conducive to proximity-induced topological states. First-principles calculations reveal intrinsic topologically nontrivial bulk energy gaps as large as 70–80 meV, which can be further enhanced up to 120 meV by compression. The strong spin–orbit coupling in BiTeX has a significant influence on the graphene Dirac states, resulting in the topologically nontrivial band structure, which is confirmed by calculated nontrivial Z2 index and an explicit demonstration of metallic edge states. Such heterostructures offer a unique Dirac transport system that combines the 2D Dirac states from graphene and 1D Dirac edge states from the topological insulator, and it offers ideas for innovative device designs.
-----
-'''Fine structure of "zero-mode" Landau levels in HgTe/HgCdTe quantum wells'''
-Authors: M. Orlita, K. Masztalerz, C. Faugeras, M. Potemski, E. G. Novik, C. Brüne, H. Buhmann, L. W. Molenkamp
+http://pubs.acs.org/doi/abs/10.1021/nn503789v
-HgTe/HgCdTe quantum wells with the inverted band structure have been probed using far infrared magneto-spectroscopy. Realistic calculations of Landau level diagrams have been performed to identify the observed transitions. Investigations have been greatly focused on the magnetic field dependence of the peculiar pair of "zero-mode" Landau levels which characteristically split from the upper conduction and bottom valence bands, and merge under the applied magnetic field. The observed avoided crossing of these levels is tentatively attributed to the bulk inversion asymmetry of zinc blend compounds.
-arXiv:1011.5233v1
 ----
-'''Magneto-transport of large CVD-grown graphene'''
-Authors: Eric Whiteway, Victor Yu, Josianne Lefebvre, Robert Gagnon, Michael Hilke
+'''Pseudospin-driven spin relaxation mechanism in graphene'''
-We present magnetoresistance measurements on large scale monolayer graphene grown by chemical vapor deposition (CVD) on copper. The graphene layer was transferred onto SiO2/Si via PMMA and thermal release tape for transport measurements. The resulting centimeter-sized graphene samples were measured at temperatures down to 30mK in a magnetic field. We observe a very sharp peak in resistance at zero field, which is well fitted by weak localization theory. The samples exhibit conductance fluctuations symmetric in field, which are attributed to ensemble averaged conductance fluctuations due to large scale inhomogeneities consistent with the grain boundaries of copper during the CVD growth.
+'Dinh Van Tuan,	Frank Ortmann,	David Soriano,	Sergio O. Valenzuela	& Stephan Roche'
-arXiv:1011.5712v1
-----
-'''Strongly Modified Plasmon-Matter Interaction with Mesoscopic Quantum Emitters'''
-Authors: Mads Lykke Andersen, Søren Stobbe, Anders Søndberg Sørensen, Peter Lodahl
+The prospect of transporting spin information over long distances in graphene, possible because of its small intrinsic spin–orbit coupling (SOC) and vanishing hyperfine interaction, has stimulated intense research exploring spintronics applications. However, measured spin relaxation times are orders of magnitude smaller than initially predicted, while the main physical process for spin dephasing and its charge-density and disorder dependences remain unconvincingly described by conventional mechanisms. Here, we unravel a spin relaxation mechanism for non-magnetic samples that follows from an entanglement between spin and pseudospin driven by random SOC, unique to graphene. The mixing between spin and pseudospin-related Berry’s phases results in fast spin dephasing even when approaching the ballistic limit, with increasing relaxation times away from the Dirac point, as observed experimentally. The SOC can be caused by adatoms, ripples or even the substrate, suggesting novel spin manipulation strategies based on the pseudospin degree of freedom.
-Semiconductor quantum dots (QDs) provide an essential link between light and matter in emerging fields such as light-harvesting, all-solid-state quantum communication, and quantum computing. QDs are excellent single-photon sources and can store quantum bits for extended periods making them promising interconnects between light and matter in integrated quantum information networks. To this end the light-matter interaction strength must be strongly enhanced using nanophotonic structures such as photonic crystal cavities and waveguides or plasmonic nanowires. So far it has been assumed that QDs can be treated just like atomic photon emitters where the spatial properties of the wavefunction can be safely ignored. Here we demonstrate that the point-emitter description for QDs near plasmonic nanostructures breaks down. We observe that the QDs can excite plasmons eight times more efficiently depending on their orientation due to their mesoscopic character. Either enhancement or suppresion of the rate of plasmon excitation is observed depending on the geometry of the plasmonic nanostructure in full agreement with a new theory. This discovery has no equivalence in atomic systems and paves the way for novel nanophotonic devices that exploit the extended size of QDs as a resource for increasing the light-matter interaction strength.
+http://www.nature.com/nphys/journal/vaop/ncurrent/full/nphys3083.html
-arXiv:1011.5669v1
 ----
-'''Andreev reflection from non-centrosymmetric superconductors and Majorana bound state generation in half-metallic ferromagnets'''
-Authors: Mathias Duckheim, Piet W. Brouwer
+'''Observation of topological surface state quantum Hall effect in an intrinsic three-dimensional topological insulator'''
-We study Andreev reflection at an interface between a half metal and a superconductor with spin-orbit interaction. While the absence of minority carriers in the half metal makes singlet Andreev reflection impossible, the spin-orbit interaction gives rise to triplet Andreev reflection, i.e., the reflection of a majority electron into a majority hole or vice versa. As an application of our calculation, we consider a thin half metal film or wire laterally attached to a superconducting contact. If the half metal is disorder free, an excitation gap is opened that is proportional to the spin-orbit interaction strength in the superconductor. For electrons with energy below this gap a lateral half-metal--superconductor contact becomes a perfect triplet Andreev reflector. We show that the system supports localized Majorana end states in this limit.
+'Yang Xu, Ireneusz Miotkowski, Chang Liu, Jifa Tian, Hyoungdo Nam, Nasser Alidoust, Jiuning Hu, Chih-Kang Shih, M. Zahid Hasan, Yong P. Chen'
-arXiv:1011.5839v1
+A three-dimensional (3D) topological insulator (TI) is a quantum state of matter with a gapped insulating bulk yet a conducting surface hosting topologically-protected gapless surface states. One of the most distinct electronic transport signatures predicted for such topological surface states (TSS) is a well-defined half-integer quantum Hall effect (QHE) in a magnetic field, where the surface Hall conductivities become quantized in units of (1/2)e2/h (e being the electron charge, h the Planck constant) concomitant with vanishing resistance. Here, we observe well-developed QHE arising from TSS in an intrinsic TI of BiSbTeSe2. Our samples exhibit surface dominated conduction even close to room temperature, while the bulk conduction is negligible. At low temperatures and high magnetic fields perpendicular to the top and bottom surfaces, we observe well-developed integer quantized Hall plateaus, where the two parallel surfaces each contributing a half integer e2/h quantized Hall (QH) conductance, accompanied by vanishing longitudinal resistance. When the bottom surface is gated to match the top surface in carrier density, only odd integer QH plateaus are observed, representing a half-integer QHE of two degenerate Dirac gases. This system provides an excellent platform to pursue a plethora of exotic physics and novel device applications predicted for TIs, ranging from magnetic monopoles and Majorana particles to dissipationless electronics and fault-tolerant quantum computers.
-----
-'''Quantitative description of Josephson-like tunneling in $\nu_T=1$ quantum Hall bilayers'''
-Authors: Timo Hyart, Bernd Rosenow
-At total filling factor $\nu_T=1$, interlayer phase coherence in quantum Hall bilayers can result in a tunneling anomaly resembling the Josephson effect in the presence of strong fluctuations. The most robust experimental signature of this effect is a strong enhancement of the tunneling conductance at small voltages. The height and width of the conductance peak depend strongly on the area and tunneling amplitude of the samples, applied parallel magnetic field and temperature. We find that the tunneling experiments are in quantitative agreement with a theory which treats fluctuations due to meron excitations phenomenologically and takes tunneling into account perturbatively. We also discuss the qualitative changes caused by larger tunneling amplitudes, and provide a possible explanation for recently observed critical currents in counterflow geometry.
+http://xxx.lanl.gov/abs/1409.3778
-arXiv:1011.5684v1
 ----
-'''Dissipative dynamics of two-qubit system: four-level lasing'''
-Authors: E. A. Temchenko, S. N. Shevchenko, A. N. Omelyanchouk
+'''MoS2: a Choice Substrate for Accessing and Tuning the Electronic Properties of Graphene'''
-The dissipative dynamics of a two-qubit system is studied theoretically. We make use of the Bloch-Redfield formalism which explicitly includes the parameter-dependent relaxation rates. We consider the case of two flux qubits, when the controlling parameters are the partial magnetic fluxes through the qubits' loops. The strong dependence of the inter-level relaxation rates on the controlling magnetic fluxes is demonstrated for the realistic system. This allows us to propose several mechanisms for lasing in this four-level system.
+'Chih-Pin Lu, Guohong Li, K. Watanabe, T. Taniguchi, Eva Y. Andrei'
-arXiv:1011.5598v1
+One of the enduring challenges in graphene research and applications is the extreme sensitivity of its charge carriers to external perturbations, especially those introduced by the substrate. The best available substrates to date, graphite and hBN, still pose limitations: graphite being metallic does not allow gating, while both hBN and graphite having lattice structures closely matched to that of graphene, may cause significant band structure reconstruction. Here we show that the atomically smooth surface of exfoliated MoS2 provides access to the intrinsic electronic structure of graphene without these drawbacks. Using scanning tunneling microscopy and Landau-level spectroscopy in a device configuration which allows tuning the carrier concentration, we find that graphene on MoS2 is ultra-flat producing long mean free paths, while avoiding band structure reconstruction. Importantly, the screening of the MoS2 substrate can be tuned by changing the position of the Fermi energy with relatively low gate voltages. We show that shifting the Fermi energy from the gap to the edge of the conduction band gives rise to enhanced screening and to a substantial increase in the mean-free-path and quasiparticle lifetime. MoS2 substrates thus provide unique opportunities to access the intrinsic electronic properties of graphene and to study in situ the effects of screening on electron-electron interactions and transport.
-----
-'''Current noise and Coulomb effects in superconducting contacts'''
-Authors: A.V. Galaktionov, A.D. Zaikin
-We derive an effective action for contacts between superconducting terminals with arbitrary transmission distribution of conducting channels. In the case of normal-superconducting (NS) contacts we evaluate interaction correction to Andreev conductance and demonstrate a close relation between Coulomb effects and shot noise in these systems. In the case of superconducting (SS) contacts we derive the electron-electron interaction correction to the Josephson current. At $T=0$ both corrections are found to vanish for fully transparent NS and SS contacts indicating the absence of Coulomb effects in this limit.
+http://xxx.lanl.gov/abs/1409.5179
-arXiv:1011.5571v1
 ----
-'''Effects of magnetic field and transverse anisotropy on full counting statistics in single-molecule magnet'''
-Authors: Hai-Bin Xue, Y.-H. Nie, Z.-J. Li, J.-Q. Liang
+'''Aharonov-Bohm Oscillations in a Quasi-Ballistic 3D Topological Insulator Nanowire'''
-We have studied theoretically the full counting statistics of electron transport through a single-molecule magne (SMM) with an arbitrary angle between the applied magnetic field and the SMM's easy axis above the sequential tunneling threshold, since the angle $\theta$ cannot be controlled in present-day SMM experiments. In the absence of the small transverse anisotropy, when the coupling of the SMM with the incident-electrode is stronger than that with the outgoing-electrode, i.e., $\Gamma_{L}/\Gamma _{R}\gg1$, the maximum peak of shot noise firstly increase and then decrease with increasing $\theta$ from $0$ to $0.5\pi$. In particular, the shot noise can reach up to super-Poissonian value from sub-Poissonian when considering the small transverse anisotropy. For $\Gamma_{L}/\Gamma_{R}\ll1$, the maximum peaks of the shot noise and skewness can be reduced from super-Poissonian to sub-Poissonian value with increasing $\theta$ from $0$ to $0.5\pi$; and the super-Poissonian behavior of the skewness is more sensitive to the small $\theta$ than shot noise, which is suppressed when taking into account the small transverse anisotropy. These characteristics of shot noise can be qualitatively attributed to the competition between the fast and slow transport channels. The predictions regarding of the $\theta$-dependence of high order current cumulants are very interesting for better understanding electron transport through SMM, and permit experimental tests in the near future.
-arXiv:1011.5546v1
+'S. Cho, B. Dellabetta, R. D. Zhong, J. Schneeloch, T. S. Liu, G. Gu, Matthew J. Gilbert, Nadya Mason'
-----
-'''Electron-Phonon Interactions in Bilayer Graphene: A First Principles Approach'''
-Authors: K. M. Borysenko, J. T. Mullen, X. Li, Y. G. Semenov, J. M. Zavada, M. Buongiorno Nardelli, K. W. Kim
+In three-dimensional topological insulators (3D TI) nanowires, transport occurs via gapless surface states where the spin is fixed perpendicular to the momentum[1-6]. Carriers encircling the surface thus acquire a \pi Berry phase, which is predicted to open up a gap in the lowest-energy 1D surface subband. Inserting a magnetic flux ({\Phi}) of h/2e through the nanowire should cancel the Berry phase and restore the gapless 1D mode[7-8]. However, this signature has been missing in transport experiments reported to date[9-11]. Here, we report measurements of mechanically-exfoliated 3D TI nanowires which exhibit Aharonov-Bohm oscillations consistent with topological surface transport. The use of low-doped, quasi-ballistic devices allows us to observe a minimum conductance at {\Phi} = 0 and a maximum conductance reaching e^2/h at {\Phi} = h/2e near the lowest subband (i.e. the Dirac point), as well as the carrier density dependence of the transport.
-Density functional perturbation theory is used to analyze electron-phonon interaction in bilayer graphene. The results show that phonon scattering in bilayer graphene bears more resemblance with bulk graphite than monolayer graphene. In particular, electron-phonon scattering in the lowest conduction band is dominated by six lowest (acoustic and acoustic-like) phonon branches with only minor contributions from optical modes. The total scattering rate at low/moderate electron energies can be described by a simple two-phonon model in the deformation potential approximation with effective constants Dac $\approx$ 15 eV and Dop $\approx 2.8 \times 108$ eV/cm for acoustic and optical phonons, respectively. With much enhanced acoustic phonon scattering, the low field mobility of bilayer graphene is expected to be significantly smaller than that of monolayer graphene.
+http://xxx.lanl.gov/abs/1409.5095
-arXiv:1011.5521v1
 ----
-'''Interedge magnetic coupling in transition-metal terminated graphene nanoribbons'''
-Authors: Yan Wang, Hai-Ping Cheng
+'''Experimental Realization of a Three-Dimensional Dirac Semimetal'''
-The magnetic structures and interedge magnetic couplings of Fe, Co and Ni transition-metal terminated graphene nanoribbons with zigzag (ZGNR) and armchair (AGNR) edges are studied by first-principles calculations. Fe-ZGNR is found to show antiferromagnetic (AF) coupling between two edges, while the interedge coupling of Co-ZGNR is ferromagnetic (FM). For Fe-AGNRs and Co-AGNRs, increasing the interedge distance we follow oscillatory transitions from FM to AF coupling with a period of about 3.7 {\AA}. The damped oscillatory behavior indicates a Ruderman-Kittel-Kasuya-Yosida type interedge magnetic coupling and the oscillation period is determined by the critical spanning vector which connects two inequivalent Dirac points in the graphene Brillouin zone. The two edges in Ni-ZGNR are decoupled independent of the ribbon width and Ni-AGNRs are found to be nonmangetic.
+'Sergey Borisenko, Quinn Gibson, Danil Evtushinsky, Volodymyr Zabolotnyy, Bernd Büchner, and Robert J. Cava'
-arXiv:1011.6356v1
+We report the direct observation of the three-dimensional (3D) Dirac semimetal phase in cadmium arsenide (Cd3As2) by means of angle-resolved photoemission spectroscopy. We identify two momentum regions where electronic states that strongly disperse in all directions form narrow conelike structures, and thus prove the existence of the long sought 3D Dirac points. This electronic structure naturally explains why Cd3As2 has one of the highest known bulk electron mobilities. This realization of a 3D Dirac semimetal in Cd3As2 not only opens a direct path to a wide spectrum of applications, but also offers a robust platform for engineering topologically nontrivial phases including Weyl semimetals and quantum spin Hall systems.
-----
-'''Energetics and stability of vacancies in carbon nanotubes'''
-Authors: José Eduardo Padilha, Rodrigo Garcia Amorim, Alexandre Reily Rocha, Antônio José Roque da Silva, Adalberto Fazzio
+http://journals.aps.org/prl/abstract/10.1103/PhysRevLett.113.027603
-In this work we present ab initio calculations of the formation energies and stability of different types of multi-vacancies in carbon nanotubes. We demonstrate that, as in the case of graphene, the reconstruction of the defects has drastic effects on the energetics of the tubes. In particular, the formation of pentagons eliminates the dangling bonds thus lowering the formation energy. This competition leads to vacancies having an even number of carbon atoms removed to be more stable. Finally the appearance of magic numbers indicating more stable defects can be represented by a model for the formation energies that is based on the number of dangling bonds of the unreconstructed system, the pentagons and the relaxation of the final form of the defect formed after the relaxation.
-arXiv:1011.6316v1
 ----
-'''Quantum interference effects in a system of two tunnel point-contacts in the presence of single scatterer: simulation of a double-tip STM experiment'''
-Authors: N.V. Khotkevych, Yu.A. Kolesnichenko, J.M. van Ruitenbeek
+'''Terahertz Generation by Dynamical Photon Drag Effect in Graphene Excited by Femtosecond Optical Pulses'''
-The conductance of systems containing two tunnel point-contacts and a single subsurface scatterer is investigated theoretically. The problem is solved in the approximation of s-wave scattering giving analytical expressions for the wave functions and for the conductance of the system. Conductance oscillations resulting from the interference of electron waves passing through different contacts and their interference with the waves scattered by the defect are analyzed. The prospect for determining the depth of the impurity below the metal surface by using the dependence of the conductance as a function of the distance between the contacts is discussed. It is shown that the application of an external magnetic field results in Aharonov-Bohm type oscillations in the conductance, the period of which allows detection of the depth of the defect in a double tip STM experiment.
+'J. Maysonnave, S. Huppert, F. Wang, S. Maero, C. Berger, W. de Heer, T. B. Norris, L. A. De Vaulchier, S. Dhillon, J. Tignon, R. Ferreira, and J. Mangeney'
-arXiv:1011.6155v1
+Graphene has been proposed as a particularly attractive material for the achievement of strong optical nonlinearities, in particular generation of terahertz radiation. However, owing to the particular symmetries of the C-lattice, second-order nonlinear effects such as difference-frequency or rectification processes are predicted to vanish in a graphene layer for optical excitations (ℏω ≫ 2EF) involving the two relativistic dispersion bands. Here we experimentally demonstrate that graphene excited by femtosecond optical pulses generate a coherent THz radiation ranging from 0.1 to 4 THz via a second-order nonlinear effect. We fully interpret its characteristics with a model describing the electron and hole states beyond the usual massless relativistic scheme. This second-order nonlinear effect is dynamical photon drag, which relies on the transfer of light momentum to the carriers by the ponderomotive electric and magnetic forces. The model highlights the key roles of next-C-neighbor couplings and of unequal electron and hole lifetimes in the observed second-order response. Finally, our results indicate that dynamical photon drag effect in graphene can provide emission up to 60 THz, opening new routes for the generation of ultrabroadband terahertz pulses.
-----
-'''Spontaneous cross-section field in impurity graphene'''
-Authors: M.B. Belonenko, N.G. Lebedev, A.V. Pak, N.N. Yanyushkina
+http://pubs.acs.org/doi/abs/10.1021/nl502684j
-It was found that the spontaneous electric field can occur in doped graphene in an external dc electric field. The direction of the spontaneous field is perpendicular to the applied field. This effect can be connected with the nonequilibrium electron subsystem of graphene. It was also shown up the influence of problem parameters on the characteristics of the spontaneous field.
-arXiv:1011.6074v1
 ----
-'''Quantum dynamics of a dc-SQUID coupled to an asymmetric Cooper pair transistor'''
-Authors: A. Fay, W. Guichard, O. Buisson, F. W. J. Hekking
+'''Exceptional Charge Transport Properties of Graphene on Germanium'''
-We present a theoretical analysis of the quantum dynamics of a superconducting circuit based on a highly asymmetric Cooper pair transistor (ACPT) in parallel to a dc-SQUID. Starting from the full Hamiltonian we show that the circuit can be modeled as a charge qubit (ACPT) coupled to an anharmonic oscillator (dc-SQUID). Depending on the anharmonicity of the SQUID, the Hamiltonian can be reduced either to one that describes two coupled qubits or to the Jaynes-Cummings Hamiltonian. Here the dc-SQUID can be viewed as a tunable micron-size resonator. The coupling term, which is a combination of a capacitive and a Josephson coupling between the two qubits, can be tuned from the very strong- to the zero-coupling regimes. It describes very precisely the tunable coupling strength measured in this circuit and explains the 'quantronium' as well as the adiabatic quantum transfer read-out.
+'Francesca Cavallo, Richard Rojas Delgado, Michelle M. Kelly, José R. Sánchez Pérez, Daniel P. Schroeder, Huili Grace Xing, Mark A. Eriksson, and Max G. Lagally'
-arXiv:1011.6148v1
+The excellent charge transport properties of graphene suggest a wide range of application in analog electronics. While most practical devices will require that graphene be bonded to a substrate, such bonding generally degrades these transport properties. In contrast, when graphene is transferred to Ge(001) its conductivity is extremely high and the charge carrier mobility derived from the relevant transport measurements is, under some circumstances, higher than that of freestanding, edge-supported graphene. We measure a mobility of ∼5 × 105 cm2 V–1 s–1 at 20 K, and ∼103 cm2 V–1 s–1 at 300 K. These values are close to the theoretical limit for doped graphene. Carrier densities in the graphene are as high as 1014 cm–2 at 300 K.
-----
-'''Theoretical investigation of the four-layered self-doped high-T$_c$ superconductors: evidence of pair tunneling effect'''
-Authors: Tao Zhou
+http://pubs.acs.org/doi/abs/10.1021/nn503381m
-Based on a four-layered self-doped $t-J$ type model and the slave-boson mean-field approach, we study theoretically the superconductivity in the electron-doped and hole-doped layers. The neighbor layers are coupled through both the single electron interlayer hopping and pair tunneling effect. The superconducting gap magnitude for the electron-doped band is nearly twice of that of the hole-doped one, which contrasts to our previous understanding of the electron-hole asymmetry in high-T$_c$ superconductors but consistent with recent angle-resolved-photoemission-spectroscopy experiments in four-layered materials Ba$_2$Ca$_3$Cu$_4$O$_8$F$_2$. Our results propose that the pair tunneling effect is important to examine the multi-layered superconducting materials.
-arXiv:1011.6040v1
 ----
-'''Spin-orbit interaction and asymmetry effects on Kondo ridges at finite magnetic field'''
-Authors: S. Grap, S. Andergassen, J. Paaske, V. Meden
+'''Direct Laser Writing of Graphene Electronics'''
-We study electron transport through a serial double quantum dot with Rashba spin-orbit interaction (SOI) and Zeeman field of amplitude B in presence of local Coulomb repulsion. The linear conductance as a function of a gate voltage Vg equally shifting the levels on both dots shows two B=0 Kondo ridges which are robust against SOI as time-reversal symmetry is preserved. Resulting from the crossing of a spin-up and a spin-down level at vanishing SOI two additional Kondo plateaus appear at finite B. They are not protected by symmetry and rapidly vanish if the SOI is turned on. Left-right asymmetric level-lead couplings and detuned on-site energies lead to a simultaneous breaking of left-right and bonding-anti-bonding state symmetry. In this case the finite-B Kondo ridges in the Vg-B plane are bent with respect to the Vg-axis. For the Kondo ridge to develop different level renormalizations must be compensated by adjusting B.
+http://pubs.acs.org/doi/abs/10.1021/nn504946k
-arXiv:1011.5916v1
 ----
-'''Single Photon Near Field Emission and Revival in Quantum Dots'''
-Authors: Sergio Tafur, Michael N. Leuenberger
+'''Room-temperature coupling between electrical current and nuclear spins in OLEDs'''
-Models of the spontaneous emission of photons coupled to the electronic states of quantum dots are important for understanding quantum interactions in dielectric media as applied to proposed solid-state quantum computers, single photon emitters, and single photon detectors. The characteristic lifetime of photon emission is traditionally modeled in the Weisskopf-Wigner approximation. Here we model the fully quantized spontaneous emission, including near field effects, of a photon from the excited state of a quantum dot beyond theWeisskopf-Wigner approximation. We propose the use of discretized central-difference approximations to describe single photon states via single photon operators in 3+1 dimensions. We further show herein that one can shift from the traditional description of electrodynamics and quantum electrodynamics, in terms of electric and magnetic fields to one in terms of a photonic wave function and its operators using the Dirac equation for the propagation of single photons.
+'H. Malissa, M. Kavand, D. P. Waters, K. J. van Schooten, P. L. Burn, Z. V. Vardeny, B. Saam, J. M. Lupton, C. Boehme'
-arXiv:1011.6566v1
+The effects of external magnetic fields on the electrical conductivity of organic semiconductors have been attributed to hyperfine coupling of the spins of the charge carriers and hydrogen nuclei. We studied this coupling directly by implementation of pulsed electrically detected nuclear magnetic resonance spectroscopy in organic light-emitting diodes (OLEDs). The data revealed a fingerprint of the isotope (protium or deuterium) involved in the coherent spin precession observed in spin-echo envelope modulation. Furthermore, resonant control of the electric current by nuclear spin orientation was achieved with radiofrequency pulses in a double-resonance scheme, implying current control on energy scales one-millionth the magnitude of the thermal energy.
-----
-'''Topological superconductivity and Majorana fermions in half-metal / superconductor heterostructure'''
-Authors: Suk Bum Chung, Hai-Jun Zhang, Xiao-Liang Qi, Shou-Cheng Zhang
+http://www.sciencemag.org/content/345/6203/1487
-A half-metal is by definition spin-polarized at its Fermi level and therefore was conventionally thought to have little proximity effect with an $s$-wave superconductor. Here we show that if there is spin-orbit coupling at the interface between a single-band half-metal and an $s$-wave superconductor, $p_x +ip_y$ superconductivity would be induced on the half-metal. This can give us a topological superconductor with a single chiral Majorana edge state. We show that two atomic layers of CrO$_2$ or CrTe give us the single-band half-metal and is thus a candidate material for realizing this physics.
-arXiv:1011.6422v1
 ----
-'''Interface Landau levels in graphene monolayer-bilayer junctions'''
-Mikito Koshino1,*, Takeshi Nakanishi2, and Tsuneya Ando1
+'''Large, non-saturating magnetoresistance in WTe2'''
-Electronic structure of graphene monolayer-bilayer junction in a magnetic field is studied within an effective-mass approximation. The energy spectrum is characterized by the interface Landau levels, i.e., the locally flat bands appearing near the boundary region, resulting in a series of characteristic peaks in the local density of states. Their energies are independent of boundary types such as zigzag or armchair. In the atomic scale, the local density of states shows a Kekulé pattern due to the valley mixing in the armchair boundary while does not in the zigzag boundary.
+'Mazhar N. Ali,	Jun Xiong,	Steven Flynn,	Jing Tao,	Quinn D. Gibson,	Leslie M. Schoop,	Tian Liang,	Neel Haldolaarachchige,	Max Hirschberger,	N. P. Ong	& R. J. Cava'
-DOI: 10.1103/PhysRevB.82.205436
-----
-'''Electroluminescence from a single nanotube–molecule–nanotube junction'''
-Christoph W. Marquardt1,2, Sergio Grunder3, Alfred Baszczyk1,4, Simone Dehm1, Frank Hennrich1, Hilbert v. Löhneysen2,5,6, Marcel Mayor1,3,6 & Ralph Krupke1,6
+Magnetoresistance is the change in a material’s electrical resistance in response to an applied magnetic field. Materials with large magnetoresistance have found use as magnetic sensors1, in magnetic memory2, and in hard drives3 at room temperature, and their rarity has motivated many fundamental studies in materials physics at low temperatures4. Here we report the observation of an extremely large positive magnetoresistance at low temperatures in the non-magnetic layered transition-metal dichalcogenide WTe2: 452,700 per cent at 4.5 kelvins in a magnetic field of 14.7 teslas, and 13 million per cent at 0.53 kelvins in a magnetic field of 60 teslas. In contrast with other materials, there is no saturation of the magnetoresistance value even at very high applied fields. Determination of the origin and consequences of this effect, and the fabrication of thin films, nanostructures and devices based on the extremely large positive magnetoresistance of WTe2, will represent a significant new direction in the study of magnetoresistivity.
-The positioning of single molecules between nanoscale electrodes1, 2, 3, 4, 5, 6, 7, 8 has allowed their use as functional units in electronic devices. Although the electrical transport in such devices has been widely explored, optical measurements have been restricted to the observation of electroluminescence from nanocrystals and nanoclusters9, 10 and from molecules in a scanning tunnelling microscope setup11, 12. In this Letter, we report the observation of electroluminescence from the core of a rod-like molecule between two metallic single-walled carbon nanotube electrodes forming a rigid solid-state device. We also develop a simple model to explain the onset voltage for electroluminescence. These results suggest new characterization and functional possibilities, and demonstrate the potential of carbon nanotubes for use in molecular electronics.
+http://www.nature.com/nature/journal/vaop/ncurrent/full/nature13763.html
-doi:10.1038/nnano.2010.230
 ----
-'''High-Performance Carbon Nanotube Light-Emitting Diodes with Asymmetric Contacts'''
-Sheng Wang*†, Qingsheng Zeng†, Leijing Yang†, Zhiyong Zhang†, Zhenxing Wang†, Tian Pei†, Li Ding†, Xuelei Liang†, Min Gao†, Yan Li‡, and Lian-Mao Peng*†
+'''Fast non-thermal switching between macroscopic charge-ordered quantum states induced by charge injection'''
-Electroluminescence (EL) measurements are carried out on a two-terminal carbon nanotube (CNT) based light-emitting diode (LED). This two-terminal device is composed of an asymmetrically contacted semiconducting single-walled carbon nanotube (SWCNT). On the one end the SWCNT is contacted with Sc and on the other end with Pd. At large forward bias, with the Sc contact being grounded, electrons can be injected barrier-free into the conduction band of the SWCNT from the Sc contact and holes be injected into the valence band from the Pd electrode. The injected electrons and holes recombine radiatively in the SWCNT channel yielding a narrowly peaked emission peak with a full width at half-maximum of about 30 meV. Detailed EL spectroscopy measurements show that the emission is excitons dominated process, showing little overlap with that associated with the continuum states. The performance of the LED is compared with that based on a three-terminal field-effect transistor (FET) that is fabricated on the same SWCNT. The conversion efficiency of the two-terminal diode is shown to be more than three times higher than that of the FET based device, and the emission peak of the LED is much narrower and operation voltage is lower.
+'I. Vaskivskyi, I. A. Mihailovic, S. Brazovskii, J. Gospodaric, T. Mertelj, D. Svetin, P. Sutar, D. Mihailovic'
-Nano Lett., Article ASAP
+The functionality of logic and memory elements in current electronics is based on multi-stability, driven either by manipulating local concentrations of electrons in transistors, or by switching between equivalent states of a material with a degener- ate ground state in magnetic or ferroelectric materials. Another possibility is offered by phase transitions with switching between metallic and insulating phases, but classical phase transitions are limited in speed by slow nucleation, proliferation of domains and hysteresis. We can in principle avoid these problems by using quantum states for switching, but microscopic systems suffer from decoherence which prohibits their use in everyday devices. Macroscopic quantum states, such as the superconducting ground state have the advantage that on a fundamental level they do not suffer from decoherence plaguing microscopic systems. Here we demonstrate for the first time ultrafast non-thermal switching between different metastable electronically ordered states by pulsed electrical charge injection. The macroscopic nature of the many-body quantum states(1-4) - which are not part of the equilibrium phase diagram - gives rise to unprecedented stability and remarka- bly sharp switching thresholds. Fast sub-50 ps switching, large associated re- sistance changes, 2-terminal operation and demonstrable high fidelity of bi-stability control suggest new opportunities for the use of macroscopic quantum states in electronics, particularly for an ultrafast non-volatile quantum charge-order resistive random access memory (QCOR-RAM).
-DOI: 10.1021/nl101513z
-== Nov. 11. - nov. 25. (2010) ==
+http://xxx.lanl.gov/abs/1409.3794
-''Válogatta: Halbritter András''
 ----
-[[File:Suggestion.jpg‎]]
-'''Channel saturation and conductance quantization in single-atom gold constrictions '''
-Jason N. Armstrong, R. M. Schaub, Susan Z. Hua, and Harsh Deep Chopra*
+'''Imaging the two-component nature of Dirac–Landau levels in the topological surface state of Bi2Se3'''
-It is shown that the finite elasticity of atomic-sized gold constrictions allows for a continuous and reversible change in conductance. This is achieved by superposition of atomic-scale or subatomic-scale mechanical oscillations on a steadily retracting/approaching gold tip against a gold substrate. Through these perturbation studies, we report the direct observation of channel saturation and conductance quantization in stable, single-atom gold constrictions. In addition, the origin of peaks in conductance histograms is explained, and the peaks alone are shown to be insufficient in evaluating the stability of atomic configurations.
+'Ying-Shuang Fu,	M. Kawamura,	K. Igarashi,	H. Takagi,	T. Hanaguri	& T. Sasagawa'
-http://link.aps.org/doi/10.1103/PhysRevB.82.195416
+Massless Dirac electrons in condensed matter1, 2, 3, 4, 5, 6 are, unlike conventional electrons, described by two-component wavefunctions associated with the spin degrees of freedom in the surface state of topological insulators5, 6. Hence, the ability to observe the two-component wavefunction is useful for exploring novel spin phenomena. Here we show that the two-component nature is manifest in Landau levels, the degeneracy of which is lifted by a Coulomb potential. Using spectroscopic-imaging scanning tunnelling microscopy, we visualize energy and spatial structures of Landau levels in Bi2Se3, a prototypical topological insulator. The observed Landau-level splitting and internal structures of Landau orbits are distinct from those in a conventional electron system7 and are well reproduced by a two-component model Dirac Hamiltonian. Our model further predicts energy-dependent spin-magnetization textures in a potential variation and provides a way for manipulating spins in the topological surface state.
-----
-'''Spin Aharonov-Bohm effect and topological spin transistor'''
-Joseph Maciejko1,2, Eun-Ah Kim3, and Xiao-Liang Qi1,2
-Ever since its discovery, the electron spin has only been measured or manipulated through the application of an electromagnetic force acting on the associated magnetic moment. In this work, we propose a spin Aharonov-Bohm effect in which the electron spin is controlled by a magnetic flux while no electromagnetic field is acting on the electron. Such a nonlocal spin manipulation is realized in an Aharonov-Bohm ring made from the recently discovered quantum spin Hall insulator, by taking advantage of the defining property of the quantum spin Hall edge states: the one-to-one correspondence between spin polarization and direction of propagation. The proposed setup can be used to realize a new spintronics device, the topological spin transistor, in which the spin rotation is completely controlled by a magnetic flux of hc/2e, independently of the details of the sample.
+http://www.nature.com/nphys/journal/vaop/ncurrent/full/nphys3084.html
-http://link.aps.org/doi/10.1103/PhysRevB.82.195409
 ----
-'''Limits on Intrinsic Magnetism in Graphene'''
-M. Sepioni1, R. R. Nair1, S. Rablen1, J. Narayanan1, F. Tuna2, R. Winpenny2, A. K. Geim1,†, and I. V. Grigorieva1
+'''Ultrafast non-local control of spontaneous emission'''
-We have studied magnetization of graphene nanocrystals obtained by sonic exfoliation of graphite. No ferromagnetism is detected at any temperature down to 2 K. Neither do we find strong paramagnetism expected due to the massive amount of edge defects. Rather, graphene is strongly diamagnetic, similar to graphite. Our nanocrystals exhibit only a weak paramagnetic contribution noticeable below 50 K. The measurements yield a single species of defects responsible for the paramagnetism, with approximately one magnetic moment per typical graphene crystallite.
+http://www.nature.com/nnano/journal/vaop/ncurrent/full/nnano.2014.190.html
-http://link.aps.org/doi/10.1103/PhysRevLett.105.207205
 ----
-'''Is CrO2 Fully Spin Polarized? Analysis of Andreev Spectra and Excess Current'''
-Tomas Löfwander1, Roland Grein2, and Matthias Eschrig2,3
+http://www.sciencedirect.com/science/article/pii/S0008622314007465
-We report an extensive theoretical analysis of point-contact Andreev reflection data available in the literature on ferromagnetic CrO2. We find that the spectra can be well understood within a model of fully spin-polarized bands in CrO2 together with spin-active scattering at the contact. This is in contrast to analysis of the data within extended Blonder-Tinkham-Klapwijk models, which lead to a spin polarization varying between 50% and 100% depending on the transparency of the interface. We propose to utilize both the temperature dependence of the spectra and the excess current at voltages above the gap to resolve the spin polarization in CrO2 in a new generation of experiments.
+http://journals.aps.org/prb/abstract/10.1103/PhysRevB.90.125428
-http://link.aps.org/doi/10.1103/PhysRevLett.105.207001
 ----
-[[File:Suggestion.jpg‎]]
-'''Viewing the Interior of a Single Molecule: Vibronically Resolved Photon Imaging at Submolecular Resolution'''
-Chi Chen, Ping Chu, C. A. Bobisch, D. L. Mills, and W. Ho*
+For fun:
-We report the spatial imaging of the photon transition probability of a single molecule at submolecular resolution. Photon imaging of a ringlike pattern is further resolved as two orthogonal vibronic transitions after incorporating spectral selectivity. A theoretical model and the calculated intensity images reveal that the transition probability is dominated by the symmetry of the positions of the tip and the transition dipole moment. This imaging technique enables the probing of the electronic and optical properties in the interior of a single molecule.
+'''Spraying Quantum Dot Conjugates in the Colon of Live Animals Enabled Rapid and Multiplex Cancer Diagnosis Using Endoscopy'''
-http://link.aps.org/doi/10.1103/PhysRevLett.105.217402
+http://pubs.acs.org/doi/abs/10.1021/nn5009269
-----
-'''Tuning Energy Relaxation along Quantum Hall Channels'''
-C. Altimiras, H. le Sueur, U. Gennser, A. Cavanna, D. Mailly, and F. Pierre
-The chiral edge channels in the quantum Hall regime are considered ideal ballistic quantum channels, and have quantum information processing potentialities. Here, we demonstrate experimentally, at a filling factor of νL=2, the efficient tuning of the energy relaxation that limits quantum coherence and permits the return toward equilibrium. Energy relaxation along an edge channel is controllably enhanced by increasing its transmission toward a floating Ohmic contact, in quantitative agreement with predictions. Moreover, by forming a closed inner edge channel loop, we freeze energy exchanges in the outer channel. This result also elucidates the inelastic mechanisms at work at νL=2, informing us, in particular, that those within the outer edge channel are negligible.
-http://link.aps.org/doi/10.1103/PhysRevLett.105.226804
 ----
-'''Dynamic Hall Effect Driven by Circularly Polarized Light in a Graphene Layer'''
-J. Karch1, P. Olbrich1, M. Schmalzbauer1, C. Zoth1, C. Brinsteiner1, M. Fehrenbacher1, U. Wurstbauer1, M. M. Glazov2, S. A. Tarasenko2, E. L. Ivchenko2, D. Weiss1, J. Eroms1, R. Yakimova3, S. Lara-Avila4, S. Kubatkin4, and S. D. Ganichev1
+== Szept.2-12. ==
+''Tóvári Endre''
-We report the observation of the circular ac Hall effect where the current is solely driven by the crossed ac electric and magnetic fields of circularly polarized radiation. Illuminating an unbiased monolayer sheet of graphene with circularly polarized terahertz radiation at room temperature generates—under oblique incidence—an electric current perpendicular to the plane of incidence, whose sign is reversed by switching the radiation helicity. Alike the classical dc Hall effect, the voltage is caused by crossed E and B fields which are, however rotating with the light’s frequency.
+'''Fabry-Pérot Interference in Gapped Bilayer Graphene with Broken Anti-Klein Tunneling'''
-http://link.aps.org/doi/10.1103/PhysRevLett.105.227402
+'Anastasia Varlet, Ming-Hao Liu (劉明豪), Viktor Krueckl, Dominik Bischoff, Pauline Simonet, Kenji Watanabe, Takashi Taniguchi, Klaus Richter, Klaus Ensslin, and Thomas Ihn'
-----
-'''Scaling and Interaction-Assisted Transport in Graphene with One-Dimensional Defects'''
-M. Kindermann
+We report the experimental observation of Fabry-Pérot interference in the conductance of a gate-defined cavity in a dual-gated bilayer graphene device. The high quality of the bilayer graphene flake, combined with the device’s electrical robustness provided by the encapsulation between two hexagonal boron nitride layers, allows us to observe ballistic phase-coherent transport through a 1−μm-long cavity. We confirm the origin of the observed interference pattern by comparing to tight-binding calculations accounting for the gate-tunable band gap. The good agreement between experiment and theory, free of tuning parameters, further verifies that a gap opens in our device. The gap is shown to destroy the perfect reflection for electrons traversing the barrier with normal incidence (anti-Klein tunneling). The broken anti-Klein tunneling implies that the Berry phase, which is found to vary with the gate voltages, is always involved in the Fabry-Pérot oscillations regardless of the magnetic field, in sharp contrast with single-layer graphene.
-We analyze the scattering from one-dimensional defects in intrinsic graphene. The Coulomb repulsion between electrons is found to be able to induce singularities of such scattering at zero temperature as in one-dimensional conductors. In striking contrast to electrons in one space dimension, however, repulsive interactions here can enhance transport. We present explicit calculations for the scattering from vector potentials that appear when strips of the material are under strain. There the predicted effects are exponentially large for strong scatterers.
+http://journals.aps.org/prl/abstract/10.1103/PhysRevLett.113.116601
-http://link.aps.org/doi/10.1103/PhysRevLett.105.216602
 ----
-'''Enhancing the Coherence of a Spin Qubit by Operating it as a Feedback Loop That Controls its Nuclear Spin Bath'''
+'''Anomalous Sequence of Quantum Hall Liquids Revealing a Tunable Lifshitz Transition in Bilayer Graphene'''
-Hendrik Bluhm1, Sandra Foletti1, Diana Mahalu2, Vladimir Umansky2, and Amir Yacoby1,*
+'Anastasia Varlet, Dominik Bischoff, Pauline Simonet, Kenji Watanabe, Takashi Taniguchi, Thomas Ihn, Klaus Ensslin, Marcin Mucha-Kruczyński, and Vladimir I. Fal’ko'
-In many realizations of electron spin qubits the dominant source of decoherence is the fluctuating nuclear spin bath of the host material. The slowness of this bath lends itself to a promising mitigation strategy where the nuclear spin bath is prepared in a narrowed state with suppressed fluctuations. Here, this approach is realized for a two-electron spin qubit in a GaAs double quantum dot and a nearly tenfold increase in the inhomogeneous dephasing time T2* is demonstrated. Between subsequent measurements, the bath is prepared by using the qubit as a feedback loop that first measures its nuclear environment by coherent precession, and then polarizes it depending on the final state. This procedure results in a stable fixed point at a nonzero polarization gradient between the two dots, which enables fast universal qubit control.
+Bilayer graphene is a unique system where both the Fermi energy and the low-energy electron dispersion can be tuned. This is brought about by an interplay between trigonal warping and the band gap opened by a transverse electric field. Here, we drive the Lifshitz transition in bilayer graphene to experimentally controllable carrier densities by applying a large transverse electric field to a h-BN-encapsulated bilayer graphene structure. We perform magnetotransport measurements and investigate the different degeneracies in the Landau level spectrum. At low magnetic fields, the observation of filling factors −3 and −6 quantum Hall states reflects the existence of three maxima at the top of the valence-band dispersion. At high magnetic fields, all integer quantum Hall states are observed, indicating that deeper in the valence band the constant energy contours are singly connected. The fact that we observe ferromagnetic quantum Hall states at odd-integer filling factors testifies to the high quality of our sample. This enables us to identify several phase transitions between correlated quantum Hall states at intermediate magnetic fields, in agreement with the calculated evolution of the Landau level spectrum. The observed evolution of the degeneracies, therefore, reveals the presence of a Lifshitz transition in our system.
-http://link.aps.org/doi/10.1103/PhysRevLett.105.216803
+http://journals.aps.org/prl/abstract/10.1103/PhysRevLett.113.116602
-----
-''Válogatta: Makk Péter''
 ----
-'''The Uncertainty Principle Determines the Nonlocality of Quantum Mechanics'''
-Jonathan Oppenheim and Stephanie Wehner
+'''Characterizing wave functions in graphene nanodevices: Electronic transport through ultrashort graphene constrictions on a boron nitride substrate'''
-Two central concepts of quantum mechanics are Heisenberg’s uncertainty principle and a subtle form of nonlocality that Einstein famously called “spooky action at a distance.” These two fundamental features have thus far been distinct concepts. We show that they are inextricably and quantitatively linked: Quantum mechanics cannot be more nonlocal with measurements that respect the uncertainty principle. In fact, the link between uncertainty and nonlocality holds for all physical theories. More specifically, the degree of nonlocality of any theory is determined by two factors: the strength of the uncertainty principle and the strength of a property called “steering,” which determines which states can be prepared at one location given a measurement at another.
+'D. Bischoff, F. Libisch, J. Burgdörfer, T. Ihn, and K. Ensslin'
-http://www.sciencemag.org/content/330/6007/1072.full
+We present electronic transport measurements through short and narrow (30×30nm) single-layer graphene constrictions on a hexagonal boron nitride substrate. While the general observation of Coulomb blockade is compatible with earlier work, the details are not: We show that the area on which charge is localized can be significantly larger than the area of the constriction, suggesting that the localized states responsible for the Coulomb blockade leak out into the graphene bulk. The high bulk mobility of graphene on hexagonal boron nitride, however, seems to be inconsistent with the short bulk localization length required to see Coulomb blockade. To explain these findings, charge must instead be primarily localized along the imperfect edges of the devices and extend along the edge outside of the constriction. In order to better understand the mechanisms, we compare the experimental findings with tight-binding simulations of such constrictions with disordered edges. Finally, we discuss previous experiments in the light of our findings.
-----
-'''Non-Abelian operations on Majorana fermions via single charge control'''
-Karsten Flensberg
-We demonstrate that non-Abelian rotations within the degenerate groundstate manifold of a set of Majorana fermions can be realized by the addition or removal of single electrons, and propose an implementation using Coulomb blockaded quantum dots. The exchange of electrons generates rotations similar to braiding, though not in real space. Unlike braiding operations, rotations by a continuum of angles are possible, while still being partially robust against perturbations. The quantum dots can also be used for readout of the state of the Majorana system via a charge measurement.
+http://journals.aps.org/prb/abstract/10.1103/PhysRevB.90.115405
-http://arxiv.org/abs/1011.5467
 ----
-'''Fano resonances in nanoscale structures'''
-Andrey E. Miroshnichenko, Sergej Flach, Yuri S. Kivshar
+'''Twist-controlled resonant tunnelling in graphene/boron nitride/graphene heterostructures'''
+'A. Mishchenko,	J. S. Tu,	Y. Cao,	R. V. Gorbachev,	J. R. Wallbank,	M. T. Greenaway,	V. E. Morozov,	S. V. Morozov,	M. J. Zhu,	S. L. Wong,	F. Withers,	C. R. Woods,	Y-J. Kim,	K. Watanabe,	T. Taniguchi,	E. E. Vdovin,	O. Makarovsky,	T. M. Fromhold,	V. I. Fal'ko,	A. K. Geim,	L. Eaves	& K. S. Novoselov'
-Modern nanotechnology allows one to scale down various important devices (sensors, chips, fibers, etc.) and thus opens up new horizons for their applications. The efficiency of most of them is based on fundamental physical phenomena, such as transport of wave excitations and resonances. Short propagation distances make phase-coherent processes of waves important. Often the scattering of waves involves propagation along different paths and, as a consequence, results in interference phenomena, where constructive interference corresponds to resonant enhancement and destructive interference to resonant suppression of the transmission. Recently, a variety of experimental and theoretical work has revealed such patterns in different physical settings. The purpose of this review is to relate resonant scattering to Fano resonances, known from atomic physics. One of the main features of the Fano resonance is its asymmetric line profile. The asymmetry originates from a close coexistence of resonant transmission and resonant reflection and can be reduced to the interaction of a discrete (localized) state with a continuum of propagation modes. The basic concepts of Fano resonances are introduced, their geometrical and/or dynamical origin are explained, and theoretical and experimental studies of light propagation in photonic devices, charge transport through quantum dots, plasmon scattering in Josephson-junction networks, and matter-wave scattering in ultracold atom systems, among others are reviewed.
+Recent developments in the technology of van der Waals heterostructures1, 2 made from two-dimensional atomic crystals3, 4 have already led to the observation of new physical phenomena, such as the metal–insulator transition5 and Coulomb drag6, and to the realization of functional devices, such as tunnel diodes7, 8, tunnel transistors9, 10 and photovoltaic sensors11. An unprecedented degree of control of the electronic properties is available not only by means of the selection of materials in the stack12, but also through the additional fine-tuning achievable by adjusting the built-in strain and relative orientation of the component layers13, 14, 15, 16, 17. Here we demonstrate how careful alignment of the crystallographic orientation of two graphene electrodes separated by a layer of hexagonal boron nitride in a transistor device can achieve resonant tunnelling with conservation of electron energy, momentum and, potentially, chirality. We show how the resonance peak and negative differential conductance in the device characteristics induce a tunable radiofrequency oscillatory current that has potential for future high-frequency technology.
-[http://rmp.aps.org/abstract/RMP/v82/i3/p2257_1 http://rmp.aps.org/abstract/RMP/v82/i3/p2257_1]
+http://www.nature.com/nnano/journal/vaop/ncurrent/full/nnano.2014.187.html
-----
-'''Colloquium: Topological insulators'''
-M. Z. Hasan, C. L. Kane
-Topological insulators are electronic materials that have a bulk band gap like an ordinary insulator but have protected conducting states on their edge or surface. These states are possible due to the combination of spin-orbit interactions and time-reversal symmetry. The two-dimensional (2D) topological insulator is a quantum spin Hall insulator, which is a close cousin of the integer quantum Hall state. A three-dimensional (3D) topological insulator supports novel spin-polarized 2D Dirac fermions on its surface. In this Colloquium the theoretical foundation for topological insulators and superconductors is reviewed and recent experiments are described in which the signatures of topological insulators have been observed. Transport experiments on HgTe∕CdTe quantum wells are described that demonstrate the existence of the edge states predicted for the quantum spin Hall insulator. Experiments on Bi1−xSbx, Bi2Se3, Bi2Te3, and Sb2Te3 are then discussed that establish these materials as 3D topological insulators and directly probe the topology of their surface states. Exotic states are described that can occur at the surface of a 3D topological insulator due to an induced energy gap. A magnetic gap leads to a novel quantum Hall state that gives rise to a topological magnetoelectric effect. A superconducting energy gap leads to a state that supports Majorana fermions and may provide a new venue for realizing proposals for topological quantum computation. Prospects for observing these exotic states are also discussed, as well as other potential device applications of topological insulators.
-[http://rmp.aps.org/abstract/RMP/v82/i4/p3045_1 http://rmp.aps.org/abstract/RMP/v82/i4/p3045_1]
 ----
-'''Microwave Photon Counter Based on Josephson Junctions'''
-Y.-F. Chen, D. Hover, S. Sendelbach, L. Maurer, S.T. Merkel, E.J. Pritchett, F.K. Wilhelm, R. McDermott
+'''Resistance-voltage dependence of nanojunctions during electromigration in ultrahigh vacuum'''
-he strong interaction of superconducting integrated circuits with microwave photons forms the basis of circuit quantum electrodynamics (cQED), an attractive paradigm for scalable quantum computing and a test bed for quantum optics in the strong coupling regime. Most quantum optics protocols rely on photon counters to probe the state of the light field. While optical photon counters are well established, the detection of single microwave photons is exceedingly difficult due to the small energy of the photon. Here we describe a microwave photon counter based on current-biased Josephson junctions. The absorption of a single microwave photon causes a junction to transition to the voltage state, producing a large and easily measured classical signal. With a two-junction circuit, we have performed a microwave version of the Hanbury Brown and Twiss experiment and demonstrated a clear signature of microwave photon bunching for a thermal source. The design is readily scalable to tens of parallelized junctions, a configuration that would allow number-resolved counting of microwave photons.
-[http://arxiv.org/abs/1011.4329 http://arxiv.org/abs/1011.4329]
-----
-'''Mechanical control of vibrational states in single-molecule junctions'''
-Youngsang Kim, Hyunwook Song, Florian Strigl, Hans-Fridtjof Pernau, Takhee Lee, Elke Scheer
+'D. Stöffler, M. Marz, B. Kießig, T. Tomanic, R. Schäfer, H. v. Löhneysen, and R. Hoffmann-Vogel'
-We report on inelastic electron tunneling spectroscopy measurements carried out on single molecules incorporated into a mechanically controllable break-junction of Au and Pt electrodes at low temperature. Here we establish a correlation between the molecular conformation and conduction properties of a single-molecule junction. We demonstrate that the conductance through single molecules crucially depends on the contact material and configuration by virtue of their mechanical and electrical properties. Our findings prove that the charge transport via single molecules can be manipulated by varying both the molecular conformation (e.g., trans or gauche) and the contact material.
+The electrical resistance R of metallic nanocontacts subjected to controlled cyclic electromigration in ultrahigh vacuum has been investigated in situ as a function of applied voltage V. For sufficiently small contacts, i.e., large resistance, a decrease of R(V) while increasing V is observed. This effect is tentatively attributed to the presence of contacts separated by thin vacuum barriers in parallel to ohmic nanocontacts. Simple model calculations indicate that both thermal activation or tunneling can lead to this unusual behavior. We describe our data by a tunneling model whose key parameter, i.e., the tunneling distance, changes because of thermal expansion due to Joule heating and/or electrostatic strain arising from the applied voltage. Oxygen exposure during electromigration prevents the formation of negative R(V) slopes, and at the same time enhances the probability of uncontrolled melting, while other gases show little effects. In addition, indication for field emission has been observed in some samples.
-[http://arxiv.org/abs/1011.3226 http://arxiv.org/abs/1011.3226]
+http://journals.aps.org/prb/abstract/10.1103/PhysRevB.90.115406
 ----
-'''Current and noise correlations in a double dot Cooper pair beam splitter'''
+'''Quantum interference in off-resonant transport through single molecules'''
-D. Chevallier, J. Rech, T. Jonckheere, T. Martin
+'Kim G. L. Pedersen, Mikkel Strange, Martin Leijnse, Per Hedegård, Gemma C. Solomon, and Jens Paaske'
-We consider a double quantum dot coupled to two normal leads and one superconducting lead, modeling the Cooper pair beam splitter studied in two recent experiments. Starting from a microscopic Hamiltonian we derive a general expression for the branching current and the noise crossed correlations in terms of single and two-particle Green's function of the dot electrons. We then study numerically how these quantities depend on the energy configuration of the dots and the presence of direct tunneling between them, isolating the various processes which come into play. In absence of direct tunneling, the antisymmetric case (the two levels have opposite energies with respect to the superconducting chemical potential) optimizes the Crossed Andreev Reflection (CAR) process while the symmetric case (the two levels have the same energies) favors the Elastic Cotunneling (EC) process. Switching on the direct tunneling tends to suppress the CAR process, leading to negative noise crossed correlations over the whole voltage range for large enough direct tunneling.
+We provide a simple set of rules for predicting interference effects in off-resonant transport through single molecule junctions. These effects fall into two classes, showing, respectively, an odd or an even number of nodes in the linear conductance within a given molecular charge state, and we demonstrate how to decide the interference class directly from the contacting geometry. For neutral alternant hydrocarbons, we employ the Coulson-Rushbrooke-McLachlan pairing theorem to show that the interference class is decided simply by tunneling on and off the molecule from same or different sublattices. More generally, we investigate a range of smaller molecules by means of exact diagonalization combined with a perturbative treatment of the molecule-lead tunnel coupling. While these results generally agree well with GW calculations, they are shown to be at odds with simpler mean-field treatments. For molecules with spin-degenerate ground states, we show that for most junctions interference causes no transmission nodes, but we argue that it may lead to a nonstandard gate dependence of the zero-bias Kondo resonance.
-[http://arxiv.org/abs/1011.3408 http://arxiv.org/abs/1011.3408]
+http://journals.aps.org/prb/abstract/10.1103/PhysRevB.90.125413
-----
-'''Conductance fluctuations in metallic nanogaps made by electromigration'''
-P. Petit, A. Anthore, M. L. Della Rocca, P. Lafarge
-We report on low temperature conductance measurements of gold nanogaps fabricated by controlled electromigration. Fluctuations of the conductance due to quantum interferences and depending both on bias voltage and magnetic field are observed. By analyzing the voltage and magnetoconductance correlation functions we determine the type of electron trajectories generating the observed quantum interferences and the effective characteristic time of phase coherence in our device.
-[http://arxiv.org/abs/1011.5144 http://arxiv.org/abs/1011.5144]
 ----
-'''Visualization of charge transport through Landau levels in graphene'''
-G. Nazin, Y. Zhang, L. Zhang, E. Sutter  &  P. Sutter
+'''All-optical control of ferromagnetic thin films and nanostructures'''
-Band bending and the associated spatially inhomogeneous population of Landau levels play a central role in the physics of the quantum Hall effect (QHE) by constraining the pathways for charge-carrier transport and scattering1. Recent progress in understanding such effects in low-dimensional carrier gases in conventional semiconductors has been achieved by real-space mapping using local probes2, 3. Here, we use spatially resolved photocurrent measurements in the QHE regime to study the correlation between the distribution of Landau levels and the macroscopic transport characteristics in graphene. Spatial maps show that the net photocurrent is determined by hot carriers transported to the periphery of the graphene channel, where QHE edge states provide efficient pathways for their extraction to the contacts. The photocurrent is sensitive to the local filling factor, which allows us to reconstruct the local charge density in the entire conducting channel of a graphene device.
-[http://www.nature.com/nphys/journal/v6/n11/full/nphys1745.html http://www.nature.com/nphys/journal/v6/n11/full/nphys1745.html]
-----
-'''More than just room temperature'''
-Diluted magnetic semiconductors and oxides are interesting for fundamental science and applications even without room-temperature ferromagnetism.
+'C-H. Lambert, S. Mangin, B. S. D. Ch. S. Varaprasad, Y. K. Takahashi, M. Hehn, M. Cinchetti, G. Malinowski, K. Hono, Y. Fainman, M. Aeschlimann, E. E. Fullerton'
+The interplay of light and magnetism allowed light to be used as a probe of magnetic materials. Now the focus has shifted to use polarized light to alter or manipulate magnetism. Here, we demonstrate optical control of ferromagnetic materials ranging from magnetic thin films to multilayers and even granular films being explored for ultra-high-density magnetic recording. Our finding shows that optical control of magnetic materials is a much more general phenomenon than previously assumed and may have a major impact on data memory and storage industries through the integration of optical control of ferromagnetic bits.
-[http://www.nature.com/nmat/journal/v9/n12/full/nmat2918.html http://www.nature.com/nmat/journal/v9/n12/full/nmat2918.html]
+http://www.sciencemag.org/content/345/6202/1337
 ----
-'''A ten-year perspective on dilute magnetic semiconductors and oxides '''
-Tomasz Dietl
+'''Ultrafast optical control of orbital and spin dynamics in a solid-state defect'''
-In 2000, a seminal study predicted ferromagnetism above room temperature in diluted magnetic semiconductors and oxides, fuelling tremendous research activity that has lasted for a decade. Tomasz Dietl reviews the progress in understanding these materials over the past ten years, with a view to the future of semiconductor spintronics.
+'Lee C. Bassett, F. Joseph Heremans, David J. Christle, Christopher G. Yale, Guido Burkard, Bob B. Buckley, David D. Awschalom'
-[http://www.nature.com/nmat/journal/v9/n12/full/nmat2898.html http://www.nature.com/nmat/journal/v9/n12/full/nmat2898.html]
+Atom-scale defects in semiconductors are promising building blocks for quantum devices, but our understanding of their material-dependent electronic structure, optical interactions, and dissipation mechanisms is lacking. Using picosecond resonant pulses of light, we study the coherent orbital and spin dynamics of a single nitrogen-vacancy center in diamond over time scales spanning six orders of magnitude. We develop a time-domain quantum tomography technique to precisely map the defect’s excited-state Hamiltonian and exploit the excited-state dynamics to control its ground-state spin with optical pulses alone. These techniques generalize to other optically addressable nanoscale spin systems and serve as powerful tools to characterize and control spin qubits for future applications in quantum technology.
-----
+http://www.sciencemag.org/content/345/6202/1333
-'''A window on the future of spintronics'''
-Hideo Ohno
-Despite low transition temperatures, ferromagnetism in diluted magnetic semiconductors has been essential in exploring new ideas and concepts in spintronics, some of which have been successfully transferred to metallic ferromagnets.
-[http://www.nature.com/nmat/journal/v9/n12/full/nmat2913.html http://www.nature.com/nmat/journal/v9/n12/full/nmat2913.html]
 ----
-'''Molecular Bridging of Silicon Nanogaps'''
-Geoffrey J. Ashwell, Laurie J. Phillips, Benjamin J. Robinson, Barbara Urasinska-Wojcik, Colin J. Lambert, Iain M. Grace, Martin R. Bryce, Rukkiat Jitchati, Mustafa Tavasli, Timothy I. Cox, Ian C. Sage, Rachel P. Tuffin, and Shona Ray
+'''Environment-assisted quantum control of a solid-state spin via coherent dark states'''
-The highly doped electrodes of a vertical silicon nanogap device have been bridged by a 5.85 nm long molecular wire, which was synthesized in situ by grafting 4-ethynylbenzaldehyde via C−Si links to the top and bottom electrodes and thereafter by coupling an amino-terminated fluorene unit to the aldehyde groups of the activated electrode surfaces. The number of bridging molecules is constrained by relying on surface roughness to match the 5.85 nm length with an electrode gap that is nominally 1 nm wider and may be controlled by varying the reaction time: the device current increases from ≤1 pA at 1 V following the initial grafting step to 10−100 nA at 1 V when reacted for 5−15 min with the amino-terminated linker and 10 μA when reacted for 16−53 h. It is the first time that both ends of a molecular wire have been directly grafted to silicon electrodes, and these molecule-induced changes are reversible. The bridges detach when the device is rinsed with dilute acid solution, which breaks the imine links of the in situ formed wire and causes the current to revert to the subpicoampere leakage value of the 4-ethynylbenzaldehyde-grafted nanogap structure.
+'Jack Hansom,	Carsten H. H. Schulte,	Claire Le Gall,	Clemens Matthiesen,	Edmund Clarke, Maxime Hugues,	Jacob M. Taylor	& Mete Atatüre'
-[http://pubs.acs.org/doi/abs/10.1021/nn102460z http://pubs.acs.org/doi/abs/10.1021/nn102460z]
+Understanding the interplay between a quantum system and its environment lies at the heart of quantum science and its applications. So far most efforts have focused on circumventing decoherence induced by the environment by either protecting the system from the associated noise1, 2, 3, 4, 5 or by manipulating the environment directly6, 7, 8, 9. Recently, parallel efforts using the environment as a resource have emerged, which could enable dissipation-driven quantum computation and coupling of distant quantum bits10, 11, 12, 13, 14. Here, we realize the optical control of a semiconductor quantum-dot spin by relying on its interaction with an adiabatically evolving spin environment. The emergence of hyperfine-induced, quasi-static optical selection rules enables the optical generation of coherent spin dark states without an external magnetic field. We show that the phase and amplitude of the lasers implement multi-axis manipulation of the basis spanned by the dark and bright states, enabling control via projection into a spin-superposition state. Our approach can be extended, within the scope of quantum control and feedback15, 16, to other systems interacting with an adiabatically evolving environment.
-----
-'''Bringing Order to the World of Nanowire Devices by Phase Shift Lithography'''
-Kittitat Subannajui, Firat Gder, and Margit Zacharias
-Semiconductor nanowire devices have several properties which match future requirements of scaling down the size of electronics. In typical microelectronics production, a number of microstructures are aligned precisely on top of each other during the fabrication process. In the case of nanowires, this mandatory condition is still hard to achieve. A technological breakthrough is needed to accurately place nanowires at any specific position and then form devices in mass production. In this article, an upscalable process combining conventional micromachining with phase shift lithography will be demonstrated as a suitable tool for nanowire device technology. Vertical Si and ZnO nanowires are demonstrated on very large (several cm2) areas. We demonstrate how the nanowire positions can be controlled, and the resulting nanowires are used for device fabrication. As an example Si/ZnO heterojunction diode arrays are fabricated. The electrical characterization of the produced devices has also been performed to confirm the functionality of the fabricated diodes.
-[http://pubs.acs.org/doi/full/10.1021/nl102103w http://pubs.acs.org/doi/full/10.1021/nl102103w]
+http://www.nature.com/nphys/journal/vaop/ncurrent/full/nphys3077.html
 ----
-'''Quantum tunnelling of the magnetization in a monolayer of oriented single-molecule magnets'''
-M. Mannini, F. Pineider, C. Danieli, F. Totti, L. Sorace, Ph. Sainctavit, M.-A. Arrio, E. Otero, L. Joly, J. C. Cezar, A. Cornia & R. Sessoli
+'''Graphene nanoribbon heterojunctions'''
-A fundamental step towards atomic- or molecular-scale spintronic devices has recently been made by demonstrating that the spin of an individual atom deposited on a surface1, or of a small paramagnetic molecule embedded in a nanojunction2, can be externally controlled. An appealing next step is the extension of such a capability to the field of information storage, by taking advantage of the magnetic bistability and rich quantum behaviour of single-molecule magnets3, 4, 5, 6 (SMMs). Recently, a proof of concept that the magnetic memory effect is retained when SMMs are chemically anchored to a metallic surface7 was provided. However, control of the nanoscale organization of these complex systems is required for SMMs to be integrated into molecular spintronic devices8, 9. Here we show that a preferential orientation of Fe4 complexes on a gold surface can be achieved by chemical tailoring. As a result, the most striking quantum feature of SMMs—their stepped hysteresis loop, which results from resonant quantum tunnelling of the magnetization5, 6—can be clearly detected using synchrotron-based spectroscopic techniques. With the aid of multiple theoretical approaches, we relate the angular dependence of the quantum tunnelling resonances to the adsorption geometry, and demonstrate that molecules predominantly lie with their easy axes close to the surface normal. Our findings prove that the quantum spin dynamics can be observed in SMMs chemically grafted to surfaces, and offer a tool to reveal the organization of matter at the nanoscale.
+http://www.nature.com/nnano/journal/vaop/ncurrent/full/nnano.2014.184.html
-[http://www.nature.com/nature/journal/v468/n7322/full/nature09478.html http://www.nature.com/nature/journal/v468/n7322/full/nature09478.html]
 ----
-'''Atomic-scale engineering of electrodes for single-molecule contacts'''
+'''Generation and electric control of spin–valley-coupled circular photogalvanic current in WSe2'''
-Guillaume Schull, Thomas Frederiksen, Andrés Arnau, Daniel Sánchez-Portal & Richard Berndt
-The transport of charge through a conducting material depends on the intrinsic ability of the material to conduct current and on the charge injection efficiency at the contacts between the conductor and the electrodes carrying current to and from the material1, 2, 3. According to theoretical considerations4, this concept remains valid down to the limit of single-molecule junctions5. Exploring this limit in experiments requires atomic-scale control of the junction geometry. Here we present a method for probing the current through a single C60 molecule while changing, one by one, the number of atoms in the electrode that are in contact with the molecule. We show quantitatively that the contact geometry has a strong influence on the conductance. We also find a crossover from a regime in which the conductance is limited by charge injection at the contact to a regime in which the conductance is limited by scattering at the molecule. Thus, the concepts of ‘good’ and ‘bad’ contacts, commonly used in macro- and mesoscopic physics, can also be applied at the molecular scale.
-[http://www.nature.com/nnano/journal/vaop/ncurrent/full/nnano.2010.215.html http://www.nature.com/nnano/journal/vaop/ncurrent/full/nnano.2010.215.html]
+http://www.nature.com/nnano/journal/vaop/ncurrent/full/nnano.2014.183.html
 ----
-''' Flexible organic transistors and circuits with extreme bending stability  '''
-Tsuyoshi Sekitani, Ute Zschieschang, Hagen Klauk  &  Takao Someya
+'''Sensitive room-temperature terahertz detection via the photothermoelectric effect in graphene'''
-Flexible electronic circuits are an essential prerequisite for the development of rollable displays, conformable sensors, biodegradable electronics and other applications with unconventional form factors. The smallest radius into which a circuit can be bent is typically several millimetres, limited by strain-induced damage to the active circuit elements. Bending-induced damage can be avoided by placing the circuit elements on rigid islands connected by stretchable wires, but the presence of rigid areas within the substrate plane limits the bending radius. Here we demonstrate organic transistors and complementary circuits that continue to operate without degradation while being folded into a radius of 100 μm. This enormous flexibility and bending stability is enabled by a very thin plastic substrate (12.5 μm), an atomically smooth planarization coating and a hybrid encapsulation stack that places the transistors in the neutral strain position. We demonstrate a potential application as a catheter with a sheet of transistors and sensors wrapped around it that enables the spatially resolved measurement of physical or chemical properties inside long, narrow tubes.
+'Xinghan Cai,	Andrei B. Sushkov,	Ryan J. Suess,	Mohammad M. Jadidi,	Gregory S. Jenkins, Luke O. Nyakiti,	Rachael L. Myers-Ward,	Shanshan Li,	Jun Yan,	D. Kurt Gaskill,	Thomas E. Murphy,	H. Dennis Drew	& Michael S. Fuhrer'
-[http://www.nature.com/nmat/journal/vaop/ncurrent/full/nmat2896.html http://www.nature.com/nmat/journal/vaop/ncurrent/full/nmat2896.html]
+Terahertz radiation has uses in applications ranging from security to medicine1. However, sensitive room-temperature detection of terahertz radiation is notoriously difficult2. The hot-electron photothermoelectric effect in graphene is a promising detection mechanism; photoexcited carriers rapidly thermalize due to strong electron–electron interactions3, 4, but lose energy to the lattice more slowly3, 5. The electron temperature gradient drives electron diffusion, and asymmetry due to local gating6, 7 or dissimilar contact metals8 produces a net current via the thermoelectric effect. Here, we demonstrate a graphene thermoelectric terahertz photodetector with sensitivity exceeding 10 V W–1 (700 V W–1) at room temperature and noise-equivalent power less than 1,100 pW Hz–1/2 (20 pW Hz–1/2), referenced to the incident (absorbed) power. This implies a performance that is competitive with the best room-temperature terahertz detectors9 for an optimally coupled device, and time-resolved measurements indicate that our graphene detector is eight to nine orders of magnitude faster than those7, 10. A simple model of the response, including contact asymmetries (resistance, work function and Fermi-energy pinning) reproduces the qualitative features of the data, and indicates that orders-of-magnitude sensitivity improvements are possible.
-== nov 3. - nov. 11. (2010) ==
+http://www.nature.com/nnano/journal/vaop/ncurrent/full/nnano.2014.182.html
-''Válogatta: Márton Attila''
-----
-'''Giant Faraday rotation in single- and multilayer graphene'''
-Iris Crassee, Julien Levallois, Andrew L. Walter, Markus Ostler, Aaron Bostwick, Eli Rotenberg, Thomas Seyller, Dirk van der Marel & Alexey B. Kuzmenko
-Nature Physics (2010) doi:10.1038/nphys1816 Received 17 May 2010 Accepted 14 September 2010 Published online 07 November 2010
-The rotation of the polarization of light after passing a medium in a magnetic field, discovered by Faraday1, is an optical analogue of the Hall effect, which combines sensitivity to the carrier type with access to a broad energy range. Up to now the thinnest structures showing the Faraday rotation were several-nanometre-thick two-dimensional electron gases2. As the rotation angle is proportional to the distance travelled by the light, an intriguing issue is the scale of this effect in two-dimensional atomic crystals or films—the ultimately thin objects in condensed matter physics. Here we demonstrate that a single atomic layer of carbon—graphene—turns the polarization by several degrees in modest magnetic fields. Such a strong rotation is due to the resonances originating from the cyclotron effect in the classical regime and the inter-Landau-level transitions in the quantum regime. Combined with the possibility of ambipolar doping3, this opens pathways to use graphene in fast tunable ultrathin infrared magneto-optical devices.
-http://www.nature.com/nphys/journal/vaop/ncurrent/abs/nphys1816.html
 ----
-'''Graphene as a quantum surface with curvature-strain preserving dynamics'''
-M. V. Karasev
+'''Polycrystalline Graphene with Single Crystalline Electronic Structure'''
-(Submitted on 10 Nov 2010)
-We discuss how the curvature and the strain density of the atomic lattice generate the quantization of graphene sheets as well as the dynamics of geometric quasiparticles propagating along the constant curvature/strain levels. The internal kinetic momentum of Riemannian oriented surface (a vector field preserving the Gaussian curvature and the area) is determined.
+http://pubs.acs.org/doi/abs/10.1021/nl502445j
-http://xxx.lanl.gov/PS_cache/arxiv/pdf/1011/1011.2339v1.pdf
 ----
-'''Tunable band gaps in bilayer graphene-BN heterostructures'''
-Ashwin Ramasubramaniam, Doron Naveh, ELias Towe
+'''Angle-dependent van Hove singularities and their breakdown in twisted graphene bilayers'''
-(Submitted on 10 Nov 2010)
-We investigate band-gap tuning of bilayer graphene between hexagonal boron nitride sheets, by external electric fields. Using density functional theory, we show that the gap is continuously tunable from 0 to 0.2 eV, and is robust to stacking disorder. Moreover, boron nitride sheets do not alter the fundamental response from that of free-standing bilayer graphene, apart from additional screening. The calculations suggest that the graphene-boron nitride heterostructures could provide a viable route to graphene-based electronic devices.
+'Wei Yan, Lan Meng, Mengxi Liu, Jia-Bin Qiao, Zhao-Dong Chu, Rui-Fen Dou, Zhongfan Liu, Jia-Cai Nie, Donald G. Naugle, and Lin He'
-http://xxx.lanl.gov/PS_cache/arxiv/pdf/1011/1011.2489v1.pdf
+The creation of van der Waals heterostructures based on a graphene monolayer and other two-dimensional crystals has attracted great interest because the atomic registry of the two-dimensional crystals can modify the electronic spectra and properties of graphene. A twisted graphene bilayer can be viewed as a special van der Waals structure composed of two mutually misoriented graphene layers, where the sublayer graphene not only plays the role of a substrate, but also acts in an equivalent role as the top graphene layer in the structure. Here we report the electronic spectra of slightly twisted graphene bilayers studied by scanning tunneling microscopy and spectroscopy. Our experiment demonstrates that twist-induced van Hove singularities are ubiquitously present for rotation angles θ of less than about 3.5°, corresponding to moiré-pattern periods D longer than 4 nm. However, they totally vanish for θ>5.5° (D<2.5nm). Such a behavior indicates that the continuum models, which capture moiré-pattern periodicity more accurately at small rotation angles, are no longer applicable at large rotation angles.
-----
-'''Energy gaps in graphene nano-constrictions with different aspect ratios'''
-B. Terrés, J. Dauber, C. Volk, S. Trellenkamp, U. Wichmann, C. Stampfer
-(Submitted on 9 Nov 2010)
-We present electron transport measurements on lithographically defined and etched graphene nano-constrictions with different aspect ratios, including different length (l) and width (w). A roughly length-independent effective energy gap can be observed around the charge neutrality point. This energy gap scales inversely with the width even in regimes where the length of the constriction is smaller than its width (l < w). In very short constrictions we observe in the gap region both, resonances due to localized states or charged islands and an elevated overall conductance level (0.1 - 1e2/h), which is strongly length-dependent. This makes very short graphene constrictions interesting for high transparent graphene tunneling barriers.
+http://journals.aps.org/prb/abstract/10.1103/PhysRevB.90.115402
-http://xxx.lanl.gov/PS_cache/arxiv/pdf/1011/1011.2091v1.pdf
 ----
-'''Tunneling conductance in strained graphene-based superconductor: Effect of asymmetric Weyl-Dirac fermions'''
-Bumned Soodchomshom
+'''Excitation of complex spin dynamics patterns in a quantum-dot electron spin ensemble'''
-(Submitted on 7 Nov 2010)
-Based on the BTK theory, we investigate the tunneling conductance in a uniaxially strained graphene-based normal metal (NG)/ barrier (I)/superconductor (SG) junctions. In the present model, we assume that depositing the conventional superconductor on the top of the uniaxially strained graphene, normal graphene may turn to superconducting graphene with the Cooper pairs formed by the asymmetric Weyl-Dirac electrons, the massless fermions with direction-dependent velocity. The highly asymmetrical velocity, vy/vx>>1, may be created by strain in the zigzag direction near the transition point between gapless and gapped graphene. In the case of the highly asymmetrical velocity, we find that the Andreev reflection strongly depends on the direction and the current perpendicular to the direction of strain can flow in the junction as if there was no barrier. Also, the current parallel to the direction of strain anomalously oscillates as a function of the gate voltage with very high frequency. Our predicted result is found as quite different from the feature of the quasiparticle tunneling in the unstrained graphene-based NG/I/SG conventional junction. This is because of the presence of the direction-dependent-velocity quasiparticles in the highly strained graphene system.
+http://journals.aps.org/prb/abstract/10.1103/PhysRevB.90.121301
-http://xxx.lanl.gov/ftp/arxiv/papers/1011/1011.1617.pdf
 ----
-'''Raman and optical characterization of multilayer turbostratic graphene grown via chemical vapor deposition'''
-Daniel R. Lenski, Michael S. Fuhrer
+'''Tunable Floquet Majorana fermions in driven coupled quantum dots'''
-(Submitted on 7 Nov 2010 (v1), last revised 9 Nov 2010 (this version, v2))
-We synthesize large-area graphene via atmospheric-pressure (AP) chemical vapor deposition (CVD) on copper, and transfer to SiO2 wafers. In contrast to low-pressure (LP) CVD on copper, optical contrast and atomic force microscopy measurements show AP-CVD graphene contains significant multi-layer areas. Raman spectroscopy always shows a single Lorentzian 2D peak, however systematic differences are observed in the 2D peak energy, width, and intensity for single- and multi-layer regions. We conclude that graphene multi-layers grown by AP-CVD on Cu are rotationally disordered.
+'Yantao Li, Arijit Kundu, Fan Zhong, and Babak Seradjeh'
-http://xxx.lanl.gov/ftp/arxiv/papers/1011/1011.1683.pdf
+We propose a system of coupled quantum dots in proximity to a superconductor and driven by separate ac potentials to realize and detect Floquet Majorana fermions. We show that the appearance of Floquet Majorana fermions can be finely controlled in the expanded parameter space of the drive frequency, amplitude, and phase difference across the two dots. While these Majorana fermions are not topologically protected, the highly tunable setup provides a realistic system for observing the exotic physics associated with Majorana fermions as well as their dynamical generation and manipulation.
-----
-'''Regularization of the spectral problem for the monolayer graphene with the separable in the angular momentum representation singular potential of defect'''
-Sergey A. Ktitorov, Yurii I. Kuzmin, Natalie E. Firsova
+http://journals.aps.org/prb/abstract/10.1103/PhysRevB.90.121401
-(Submitted on 4 Nov 2010)
-The electronic states in the monolayer graphene with the short-range perturbation asymmetric with respect to the band index are analized. The study was made for the separable in the angular momentum representation potential basing on the (2+1)-dimensional Dirac equation. The characteristic equation for bound and resonance states obtained in the present paper is compared with one derived earlier for the same problem with different approach. The momentum representation approach used in the present paper allowed us to obtain the satisfactory regularization of the Hadamar incorrect boundary problem stemming from the potential singularity.
-http://xxx.lanl.gov/PS_cache/arxiv/pdf/1011/1011.1231v1.pdf
 ----
-'''Adsorption of Cu, Ag, and Au atoms on graphene including van der Waals interactions'''
-Martin Amft, Sébastien Lebègue, Olle Eriksson, Natalia V. Skorodumova
+Unrelated:
-(Submitted on 4 Nov 2010)
-We performed a systematic density functional study of the adsorption of copper, silver, and gold adatoms on graphene, especially accounting for van der Waals interactions by the vdW-DF and the PBE+D2 methods. In particular, we analyze the preferred adsorption site (among top, bridge, and hollow positions) together with the corresponding distortion of the graphene sheet and identify diffusion paths. Both vdW schemes show that the coinage metal atoms do bind to the graphene sheet and that in some cases the buckling of the graphene can be significant. The results for silver are at variance with those obtained with GGA, which gives no binding in this case. However, we observe some quantitative differences between the vdW-DF and the PBE+D2 methods. For instance the adsorption energies calculated with the PBE+D2 method are systematically higher than the ones obtained with vdW-DF. Moreover, the equilibrium distances computed with PBE+D2 are shorter than those calculated with the vdW-DF method.
+Inventing a Modern Periscope
-http://xxx.lanl.gov/PS_cache/arxiv/pdf/1011/1011.1113v1.pdf
+http://www.tested.com/science/464266-inventing-modern-periscope/
-----
-'''Influence of electron-hole drag on conductivity of neutral and gated graphene'''
-I. I. Boiko
-(Submitted on 4 Nov 2010)
-Conductivity of monolayer and two-layer graphene is considered with due regard for mutual drag of band electrons and holes. Search of contribution of the drag in conductivity shows that this effect can sufficiently influence on mobility of carriers, which belong to different groups and have different drift velocities. In two-layer system the mutual drag can even change the di-rection of partial current in separate layer.
-http://xxx.lanl.gov/ftp/arxiv/papers/1011/1011.1105.pdf
 ----
-'''Compressibility of graphene'''
-D. S. L. Abergel, E. H. Hwang, S. Das Sarma
-(Submitted on 3 Nov 2010)
-We develop a theory for the compressibility and quantum capacitance of disordered monolayer and bilayer graphene including the full hyperbolic band structure and band gap in the latter case. We include the effects of disorder in our theory, which are of particular importance at the carrier densities near the Dirac point. We account for this disorder statistically using two different averaging procedures: first via averaging over the density of carriers directly, and then via averaging in the density of states to produce an effective density of carriers. We also compare the results of these two models with experimental data, and to do this we introduce a model for inter-layer screening which predicts the size of the band gap between the low-energy conduction and valence bands for arbitary gate potentials applied to both layers of bilayer graphene. We find that both models for disorder give qualitatively correct results for gapless systems, but when there is a band gap at charge neutrality, the density of states averaging is incorrect and disagrees with the experimental data.
-http://xxx.lanl.gov/PS_cache/arxiv/pdf/1011/1011.0995v1.pdf
-----
-'''Surface-Enhanced Raman Signal for Terbium Single-Molecule Magnets Grafted on Graphene'''
-Manuel Lopes†, Andrea Candini†‡, Matias Urdampilleta†, Antoine Reserbat-Plantey†, Valerio Bellini‡, Svetlana Klyatskaya§, Laetitia Marty†, Mario Ruben,, Marco Affronte, Wolfgang Wernsdorfer†, and Nedjma Bendiab†*
-ACS Nano, Article ASAP, Publication Date (Web): November 10, 2010
-We report the preparation and characterization of monolayer graphene decorated with functionalized single-molecule magnets (SMMs). The grafting ligands provide a homogeneous and selective deposition on graphene. The grafting is characterized by combined Raman microspectroscopy, atomic force microscopy (AFM), and electron transport measurements. We observe a surface-enhanced Raman signal that allowed us to study the grafting down to the limit of a few isolated molecules. The weak interaction through charge transfer is in agreement with ab initio DFT calculations. Our results indicate that both molecules and graphene are essentially intact and the interaction is driven by van der Waals forces.
-http://pubs.acs.org/doi/abs/10.1021/nn1018363
-----
-'''Graphene-Based Supercapacitor with an Ultrahigh Energy Density'''
-Chenguang Liu†§, Zhenning Yu‡§, David Neff†, Aruna Zhamu‡, and Bor Z. Jang*†
-Nano Lett., Article ASAP
-DOI: 10.1021/nl102661q
-Publication Date (Web): November 8, 2010
-A supercapacitor with graphene-based electrodes was found to exhibit a specific energy density of 85.6 Wh/kg at room temperature and 136 Wh/kg at 80 °C (all based on the total electrode weight), measured at a current density of 1 A/g. These energy density values are comparable to that of the Ni metal hydride battery, but the supercapacitor can be charged or discharged in seconds or minutes. The key to success was the ability to make full utilization of the highest intrinsic surface capacitance and specific surface area of single-layer graphene by preparing curved graphene sheets that will not restack face-to-face. The curved morphology enables the formation of mesopores accessible to and wettable by environmentally benign ionic liquids capable of operating at a voltage >4 V.
-http://pubs.acs.org/doi/abs/10.1021/nl102661q
-----
-'''The rise and rise of graphene'''
-Nature Nanotechnology 5, 755 (2010)
-Published online: 4 November 2010 | doi:10.1038/nnano.2010.224
-This year's Nobel Prize in Physics can be seen as part of the larger story of hexagonally bonded carbon.
-The recent award of the Nobel Prize in Physics to Andrei Geim and Konstantin Novoselov, two Russian-born physicists working at Manchester University in the United Kingdom, “for groundbreaking experiments regarding the two-dimensional material graphene”, is notable not just because it comes only six years after they and six others published their breakthrough paper in Science1, or because Novoselov is among the prize's youngest-ever winners (he is just 36). It is also notable because, together with the 1996 Nobel Prize in Chemistry (awarded for the discovery of fullerenes) and the 2008 Kavli Prize in Nanoscience (for carbon nanotubes), it completes a trifecta of mega-awards to three different topologies of what is otherwise exactly the same substance: hexagonally bonded carbon.
-http://www.nature.com/nnano/journal/v5/n11/full/nnano.2010.224.html
-----
-'''Giant Stark effect in the emission of single semiconductor quantum dots'''
-Anthony. J. Bennett, Raj. B. Patel, Joanna Skiba-Szymanska, Christine A. Nicoll, Ian Farrer, David A. Ritchie, Andrew J. Shields,
-(Submitted on 10 Nov 2010)
-We study the quantum-confined Stark effect in single InAs/GaAs quantum dots embedded within a AlGaAs/GaAs/AlGaAs quantum well. By significantly increasing the barrier height we can observe emission from a dot at electric fields of -500 kV/cm, leading to Stark shifts of up to 25 meV. Our results suggest this technique may enable future applications that require self-assembled dots with transitions at the same energy.
-http://xxx.lanl.gov/ftp/arxiv/papers/1011/1011.2436.pdf
-----
-'''Time-convolutionless master equation for quantum dots: Perturbative expansion to arbitrary order'''
-Carsten Timm
-(Submitted on 10 Nov 2010)
-The master equation describing the non-equilibrium dynamics of a quantum dot coupled to metallic leads is considered. Employing a superoperator approach, we derive an exact time-convolutionless master equation for the probabilities of dot states, i.e., a time-convolutionless Pauli master equation. The generator of this master equation is derived order by order in the hybridization between dot and leads. Although the generator turns out to be closely related to the T-matrix expressions for the transition rates, which are plagued by divergences, in the time-convolutionless generator all divergences cancel order by order. The time-convolutionless and T-matrix master equations are contrasted to the Nakajima-Zwanzig version. The absence of divergences in the Nakajima-Zwanzig master equation due to the nonexistence of secular reducible contributions becomes rather transparent in our approach, which explicitly projects out these contributions. We also show that the time-convolutionless generator contains the generator of the Nakajima-Zwanzig master equation in the Markov approximation plus corrections, which we make explicit. Furthermore, it is shown that the stationary solutions of the time-convolutionless and the Nakajima-Zwanzig master equations are identical. However, this identity neither extends to perturbative expansions truncated at finite order nor to dynamical solutions. We discuss the conditions under which the Nakajima-Zwanzig-Markov master equation nevertheless yields good results.
-http://xxx.lanl.gov/PS_cache/arxiv/pdf/1011/1011.2371v1.pdf
-----
-'''Quantum coherence versus quantum discord in two coupled semiconductor double-dot molecules via a transmission line resonator'''
-Pei Pei, Chong Li, Jia-Sen Jin, He-Shan Song
-(Submitted on 10 Nov 2010)
-We study the dynamics of quantum coherence and quantum correlations in two semiconductor double-dot molecules separated by a distance and indirectly coupled via a transmission line resonator. Dominant dissipation processes are considered. The numerical results show the sudden death of entanglement and the robustness of quantum discord to sudden death. Furthermore, the results indicate the dephasing processes in our model can lead in the revival and decay of coherence and discord with the absence of entanglement for certain initial states. By observing the dynamics of coherence versus discord for different initial states, we find that the similarities and differences of coherence and discord are not only related to the dependance of discord on optimizing the measurement set, but more importantly to the coherences in individual qubits which are captured by the adopted coherence measure.
-http://xxx.lanl.gov/PS_cache/arxiv/pdf/1011/1011.2252v1.pdf
-----
-'''Manipulation of the Lande g-factor in InAs quantum dots through application of anisotropic gate potentials'''
-Sanjay Prabhakar, James E Raynolds, Roderick Melnik
-(Submitted on 8 Nov 2010)
-We study the variation in the Lande g-factor of electron spins induced by an anisotropic gate potential in InAs quantum dots for potential use as non-charge based logic devices. In this paper, we present the numerical simulations of such spins in an electrostatically confined two-dimensional asymmetric gate potential forming a quantum dot system in a 2DEG. Using numerical techniques, we show that the broken in-plane rotational symmetry, due to Rashba spin orbit coupling in an asymmetric potential (induced by gate voltages) leads to a significant reverse effect on the tunability of the electron g-factor over a symmetric model potential (i.e. the derivative of the g-factor with respect to electric field has opposite sign in the two cases).
-http://xxx.lanl.gov/PS_cache/arxiv/pdf/1011/1011.1921v1.pdf
-----
-'''Spin-orbit coupling and phase-coherence in InAs nanowires'''
-S. Estévez Hernández, M. Akabori, K. Sladek, Ch. Volk, S. Alagha, H. Hardtdegen, N. Demarina, D. Grützmacher, Th. Schäpers, M. G. Pala
-(Submitted on 6 Nov 2010)
-We investigated the magnetotransport of InAs nanowires grown by selective area metal-organic vapor phase epitaxy. In the temperature range between 0.5 and 30 K reproducible fluctuations in the conductance upon variation of the magnetic field or the back-gate voltage are observed, which are attributed to electron interference effects in small disordered conductors. From the correlation field of the magnetoconductance fluctuations the phase-coherence length l_phi is determined. At the lowest temperatures l_phi is found to be at least 300 nm, while for temperatures exceeding 2 K a monotonous decrease of l_phi with temperature is observed. A direct observation of the weak antilocalization effect indicating the presence of spin-orbit coupling is masked by the strong magnetoconductance fluctuations. However, by averaging the magnetoconductance over a range of gate voltages a clear peak in the magnetoconductance due to the weak antilocalization effect was resolved. By comparison of the experimental data to simulations based on a recursive two-dimensional Green's function approach a spin-orbit scattering length of approximately 70 nm was extracted, indicating the presence of strong spin-orbit coupling.
-http://xxx.lanl.gov/PS_cache/arxiv/pdf/1011/1011.1556v1.pdf
-----
-'''Interactions of nanorod particles in the strong coupling regime'''
-Cheng-ping Huang, Xiao-gang Yin, Ling-bao Kong, Yong-yuan Zhu
-(Submitted on 5 Nov 2010)
-The plasmon coupling in a nanorod dimer obeys the exponential size dependence according to the Universal Plasmon Ruler Equation. However, it was shown recently that such a model does not hold at short nanorod distance (Nano Lett. 2009, 9, 1651). Here we study the nanorod coupling in various cases, including nanorod dimer with the asymmetrical lengths and symmetrical dimer with the varying gap width. The asymmetrical nanorod dimer causes two plasmon modes: one is the attractive lower- energy mode and the other the repulsive high-energy mode. Using a simple coupled LC-resonator model, the position of dimer resonance has been determined analytically. Moreover, we found that the plasmon coupling of symmetrical cylindrical (or rectangular) nanorod dimer is governed uniquely by gap width scaled for the (effective) rod radius rather than for the rod length. A new Plasmon Ruler Equation without using the fitting parameters has been proposed, which agrees well with the FDTD calculations. The method has also been extended to study the plasmonic wave-guiding in a linear chain of gold nanorod particles. A field decay length up to 2700nm with the lateral mode size about 50nm (~wavelength/28) has been suggested.
-http://xxx.lanl.gov/ftp/arxiv/papers/1011/1011.1408.pdf
-----
-'''Single-shot initialization of electron spin in a quantum dot using a short optical pulse'''
-Vivien Loo, Loic Lanco, Olivier Krebs, Pascale Senellart, Paul Voisin
-(Submitted on 4 Nov 2010)
-We propose a technique to initialize an electron spin in a semiconductor quantum dot with a single short optical pulse. It relies on the fast depletion of the initial spin state followed by a preferential, Purcell-accelerated desexcitation towards the desired state thanks to a micropillar cavity. We theoretically discuss the limits on initialization rate and fidelity, and derive the pulse area for optimal initialization. We show that spin initialization is possible using a single optical pulse down to a few tens of picoseconds wide.
-http://xxx.lanl.gov/PS_cache/arxiv/pdf/1011/1011.1156v1.pdf
-----
-'''Quantum dot-cavity strong-coupling regime measured through coherent reflection spectroscopy in a very high-Q micropillar'''
-Vivien Loo, Loic Lanco, Aristide Lemaitre, Isabelle Sagnes, Olivier Krebs, Paul Voisin, Pascale Senellart
-(Submitted on 4 Nov 2010)
-We report on the coherent reflection spectroscopy of a high-quality factor micropillar, in the strong coupling regime with a single InGaAs annealed quantum dot. The absolute reflectivity measurement is used to study the characteristics of our device at low and high excitation power. The strong coupling is obtained with a g=16 \mueV coupling strength in a 7.3\mum diameter micropillar, with a cavity spectral width kappa=20.5 \mueV (Q=65 000). The factor of merit of the strong-coupling regime, 4g/kappa=3, is the current state-of-the-art for a quantum dot-micropillar system.
-http://xxx.lanl.gov/PS_cache/arxiv/pdf/1011/1011.1155v1.pdf
-----
-'''The Kondo crossover in shot noise of a single quantum dot with orbital degeneracy'''
-Rui Sakano, Tatsuya Fujii, Akira Oguri
-(Submitted on 10 Nov 2010)
-We investigate out of equilibrium transport through an orbital Kondo system realized in a single quantum dot, described by the multiorbital impurity Anderson model. Shot noise and current are calculated up to the third order in bias voltage in the particle-hole symmetric case, using the renormalized perturbation theory. The derived expressions are asymptotically exact at low energies. The resulting Fano factor of the backscattering current $F_b$ is expressed in terms of the Wilson ratio $R$ and the orbital degeneracy $N$ as $F_b =\frac{1 + 9(N-1)(R-1)^2}{1 + 5(N-1)(R-1)^2}$ at zero temperature. Then, for small Coulomb repulsions $U$, we calculate the Fano factor exactly up to terms of order $U^5$, and also carry out the numerical renormalization group calculation for intermediate $U$ in the case of two- and four-fold degeneracy ($N=2,\,4$). As $U$ increases, the charge fluctuation in the dot is suppressed, and the Fano factor varies rapidly from the noninteracting value $F_b=1$ to the value in the Kondo limit $F_b=\frac{N+8}{N+4}$, near the crossover region $U\sim \pi \Gamma$, with the energy scale of the hybridization $\Gamma$.
-http://xxx.lanl.gov/PS_cache/arxiv/pdf/1011/1011.2343v1.pdf
-----
-'''Detection of spin injection into a double quantum dot: Violation of magnetic-field-inversion symmetry of nuclear polarization instabilities'''
-Mark S. Rudner, Emmanuel I. Rashba
-(Submitted on 10 Nov 2010)
-In mesoscopic systems with spin-orbit coupling, spin-injection into quantum dots at zero magnetic field is expected under a wide range of conditions. However, up to now, a viable approach for experimentally identifying such injection has been lacking. We show that electron spin injection into a spin-blockaded double quantum dot is dramatically manifested in the breaking of magnetic- field-inversion symmetry of nuclear polarization instabilities. Over a wide range of parameters, the asymmetry between positive and negative instability fields is extremely sensitive to the injected electron spin polarization and allows for the detection of even very weak spin injection. This phenomenon may be used to investigate the mechanisms of spin transport, and may hold implications for spin-based information processing.
-http://xxx.lanl.gov/PS_cache/arxiv/pdf/1011/1011.2247v1.pdf
-----
-'''Tomography of the two-electron spin qubits in semiconductors'''
-Zhan Su, Tao Tu, Gang Cao, Guang-Can Guo, Guo-Ping Guo
-(Submitted on 9 Nov 2010 (v1), last revised 10 Nov 2010 (this version, v2))
-We propose an approach to reconstruct two-electron spin qubit states in semiconductor quantum dots by employing tomographic techniques. This procedure exploits the combination of fast gate operations on electron spins trapped in dots and dynamical nuclear polarization of the underlying Ga and As nuclei. The presented method can be an important tool in solid state quantum computation for complete characterization of qubit states and theirs correlations.
-link?
-----
-'''CdSe Quantum Dots for Two-Photon Fluorescence Thermal Imaging'''
-Laura Martinez Maestro†, Emma Mart n Rodríguez‡, M. C. Iglesias-de la Cruz‡, Angeles Juarranz‡, Rafik Naccache§, Fiorenzo Vetrone, Daniel Jaque†, John A. Capobianco*, and Jose García Solé
-Nano Lett., Article ASAP
-DOI: 10.1021/nl1036098
-Publication Date (Web): November 9, 2010
-The technological development of quantum dots has ushered in a new era in fluorescence bioimaging, which was propelled with the advent of novel multiphoton fluorescence microscopes. Here, the potential use of CdSe quantum dots has been evaluated as fluorescent nanothermometers for two-photon fluorescence microscopy. In addition to the enhancement in spatial resolution inherent to any multiphoton excitation processes, two-photon (near-infrared) excitation leads to a temperature sensitivity of the emission intensity much higher than that achieved under one-photon (visible) excitation. The peak emission wavelength is also temperature sensitive, providing an additional approach for thermal imaging, which is particularly interesting for systems where nanoparticles are not homogeneously dispersed. On the basis of these superior thermal sensitivity properties of the two-photon excited fluorescence, we have demonstrated the ability of CdSe quantum dots to image a temperature gradient artificially created in a biocompatible fluid (phosphate-buffered saline) and also their ability to measure an intracellular temperature increase externally induced in a single living cell.
-http://pubs.acs.org/doi/abs/10.1021/nl1036098
-----
-'''Effect of Dephasing on Electron Transport in a Molecular Wire: Green's Function Approach'''
-Moumita Dey, Santanu K. Maiti, S. N. karmakar
-(Submitted on 9 Nov 2010)
-The effect of dephasing on electron transport through a benzene molecule is carefully examined using a phenomenological model introduced by B\"{u}ttiker. Within a tight-binding framework all the calculations are performed based on the Green's function formalism. We investigate the influence of dephasing on transmission probability and current-voltage characteristics for three different configurations ({\em ortho}, {\em meta} and {\em para}) of the molecular system depending on the locations of two contacting leads. The presence of dephasing provides a significant change in the spectral properties of the molecule and exhibits several interesting patterns that have so far remain unexplored.
-http://xxx.lanl.gov/PS_cache/arxiv/pdf/1011/1011.2033v1.pdf
-----
-'''Electrical transport through a mechanically gated molecular wire'''
-C. Toher, R. Temirov, A. Greuling, F. Pump, M. Kaczmarski, M. Rohlfing, G. Cuniberti, F.S. Tautz
-(Submitted on 5 Nov 2010)
-A surface-adsorbed molecule is contacted with the tip of a scanning tunneling microscope (STM) at a pre-defined atom. On tip retraction, the molecule is peeled off the surface. During this experiment, a two-dimensional differential conductance map is measured on the plane spanned by the bias voltage and the tip-surface distance. The conductance map demonstrates that tip retraction leads to mechanical gating of the molecular wire in the STM junction. The experiments are compared with a detailed ab initio simulation. We find that density functional theory (DFT) in the local density approximation (LDA) describes the tip-molecule contact formation and the geometry of the molecular junction throughout the peeling process with predictive power. However, a DFT-LDA-based transport simulation following the non-equilibrium Green's functions (NEGF) formalism fails to describe the behavior of the differential conductance as found in experiment. Further analysis reveals that this failure is due to the mean-field description of electron correlation in the local density approximation. The results presented here are expected to be of general validity and show that, for a wide range of common wire configurations, simulations which go beyond the mean-field level are required to accurately describe current conduction through molecules. Finally, the results of the present study illustrate that well-controlled experiments and concurrent ab initio transport simulations that systematically sample a large configuration space of molecule-electrode couplings allow the unambiguous identification of correlation signatures in experiment.
-http://xxx.lanl.gov/ftp/arxiv/papers/1011/1011.1400.pdf
-----
-'''Self consistent charge-current in a mesoscopic region attached to superconductor leads'''
-D Verrilli, F Marin
-(Submitted on 5 Nov 2010)
-We investigate the behavior of a electric potential profile inside a mesoscopic region attached to a pair of superconducting leads. It turns out that ${\rm I}-V$ characteristic curves are strongly modified by this profile. In addition, the electronic population in the mesoscopic region is affected by the profile behavior. We discuss the single particle current and the mesoscopic electronic population within the non-equilibrium Keldysh Green functions technique. The Keldysh technique results are further converted in a self consistent field (SFC) problem by introducing potential profile modifications as proposed by Datta. Evaluation of ${\rm I}-V$ characteristics are presented for several values of the model parameters and comparison with current experimental results are discussed.
-http://xxx.lanl.gov/PS_cache/arxiv/pdf/1011/1011.1372v1.pdf
-----
-'''Spin Soret effect'''
-Sylvain D. Brechet, Jean-Philippe Ansermet
-(Submitted on 10 Nov 2010)
-Using a three-current model for heat, spin-up and spin-down electrons, the thermodynamics of irreversible processes predicts that a temperature gradient gives rise to a spin current under the conditions used to measure what is called the spin Seebeck effect. A diffusive current proportional to a gradient of the chemical potential is known in thermochemistry as a Soret effect or thermophoresis.
-http://xxx.lanl.gov/PS_cache/arxiv/pdf/1011/1011.2323v1.pdf
-----
-[[file:Suggestion.jpg]]
-'''An electron jet pump: The Venturi effect of a Fermi liquid'''
-D. Taubert, G. J. Schinner, C. Tomaras, H. P. Tranitz, W. Wegscheider, S. Ludwig
-(Submitted on 10 Nov 2010)
-A three-terminal device based on a two-dimensional electron system is investigated in the regime of non-equilibrium transport. Excited electrons scatter with the cold Fermi sea and transfer energy and momentum to other electrons. A geometry analogous to a water jet pump is used to create a jet pump for electrons. Because of its phenomenological similarity we name the observed behavior "electronic Venturi effect".
-http://xxx.lanl.gov/PS_cache/arxiv/pdf/1011/1011.2289v1.pdf
-----
-'''Andreev spectroscopy and surface density of states for a three-dimensional time-reversal invariant topological superconductor'''
-Andreas P. Schnyder, P. M. R. Brydon, Dirk Manske, Carsten Timm
-(Submitted on 23 Aug 2010 (v1), last revised 10 Nov 2010 (this version, v2))
-A topological superconductor is a fully gapped superconductor that exhibits exotic zero-energy Andreev surface states at interfaces with a normal metal. In this paper we investigate the properties of a three-dimensional time reversal invariant topological superconductor by means of a two-band model with unconventional pairing in both the inter- and intraband channels. Due to the bulk-boundary correspondence the presence of Andreev surface states in this system is directly related to the topological structure of the bulk wavefunctions, which is characterized by a winding number. Using quasiclassical scattering theory we construct the spectrum of the Andreev bound states that appear near the surface and compute the surface density of states for various surface orientations. Furthermore, we consider the effects of band splitting, i.e., the breaking of an inversion-type symmetry, and demonstrate that in the absence of band splitting there is a direct transition between the fully gapped topologically trivial phase and the nontrivial phase, whereas in the presence of band splitting there exists a finite region of a gapless nodal superconducting phase between the fully gapped topologically trivial and nontrivial phases.
-http://xxx.lanl.gov/PS_cache/arxiv/pdf/1008/1008.3762v2.pdf
-----
-'''Observation of exchange Coulomb interactions in the quantum Hall state at nu=3'''
-A.B.Van'kov, T.D.Rhone, A.Pinczuk, I.V.Kukushkin, L.N.Pfeiffer, K.W.West
-(Submitted on 9 Nov 2010)
-Coulomb exchange interactions of electrons in the nu=3 quantum Hall state are determined from two inter-Landau level spin-flip excitations measured by resonant inelastic light scattering. The two coupled collective excitations are linked to inter-Landau level spin-flip transitions arising from the N=0 and N=1 Landau levels. The strong repulsion between the two spin-flip modes in the long-wave limit is clearly manifested in spectra displaying Coulomb exchange contributions that are comparable to the exchange energy for the quantum Hall state at nu=1. Theoretical calculations within the Hartree-Fock approximation are in a good agreement with measured energies of spin-flip collective excitations.
-http://xxx.lanl.gov/PS_cache/arxiv/pdf/1011/1011.2022v1.pdf
-----
-'''Electron microscopy: A new spin on electron beams'''
-Huolin L. Xin1 & David A. Muller2
-Nature Nanotechnology 5, 764 - 765 (2010)
-Published online: 4 November 2010 | doi:10.1038/nnano.2010.222
-Ideas about angular momentum that have been borrowed from optics could allow the magnetic and spin structures of materials to be studied on atomic scales with electron vortex beams.
-We are used to electrons occupying states with quantized spin and orbital angular momenta in atoms, but existing methods for generating high-energy electron beams are very inefficient at either producing or transferring states with well-defined spin and/or orbital angular momentum. This failure stems from the dominance of the direct Coulomb interaction over the spin–spin and spin–orbit interactions for high-energy electrons.
-http://www.nature.com/nnano/journal/v5/n11/full/nnano.2010.222.html
-----
-'''Biomolecular computing: Learning through play'''
-Vladimir Privman1
-Nature Nanotechnology 5, 767 - 768 (2010)
-Published online: 4 November 2010 | doi:10.1038/nnano.2010.221
-Solutions of DNA-based molecules can be taught to play a simple game in a process that does not require the operator to be familiar with the underlying molecular programming.
-As the boundaries of silicon electronics have been pushed to smaller and smaller feature sizes, a growing interest in unconventional computing has emerged. A number of alternative approaches have been considered, including quantum computing, which has grown into a major research field, but many of these rely on nanoscale features and, as such, they share the scaling-down challenges present in silicon electronics.
-http://www.nature.com/nnano/journal/v5/n11/full/nnano.2010.221.html
-----
-== Okt. 21. - nov. 3. (2010) ==
-''Válogatta: Csonka Szabolcs''
-'''Spin-orbit qubit in a semiconductor nanowire'''
-S. Nadj-Perge, S.M. Frolov, E.P.A.M. Bakkers, L.P. Kouwenhoven
-Motion of electrons can influence their spins through a fundamental effect called spin-orbit interaction. This interaction provides a way to electrically control spins and as such lies at the foundation of spintronics. Even at the level of single electrons, spin-orbit interaction has proven promising for coherent spin rotations. Here we report a spin-orbit quantum bit implemented in an InAs nanowire, where spin-orbit interaction is so strong that spin and motion can no longer be separated. In this regime we realize fast qubit rotations and universal single qubit control using only electric fields. We enhance coherence by dynamically decoupling the qubit from the environment. Our qubits are individually addressable: they are hosted in single-electron quantum dots, each of which has a different Land\'e g-factor. The demonstration of a nanowire qubit opens ways to harness the advantages of nanowires for use in quantum computing. Nanowires can serve as one-dimensional templates for scalable qubit registers. Unique to nanowires is the possibility to easily vary the material even during wire growth. Such flexibility can be used to design wires with suppressed decoherence and push semiconductor qubit fidelities towards error-correction levels. Furthermore, electrical dots can be integrated with optical dots in p-n junction nanowires. The coherence times achieved here are sufficient for the conversion of an electronic qubit into a photon, the flying qubit, for long-distance quantum communication.
-[http://xxx.lanl.gov/abs/1011.0064 arXiv:1011.0064]
-'''Cooling electrons from 1 K to 400 mK with V-based nanorefrigerators'''
-Authors: O. Quaranta, P. Spathis, F. Beltram, F. Giazotto
-(Submitted on 2 Nov 2010)
-The fabrication and operation of V-based superconducting nanorefrigerators is reported. Specifically, electrons in an Al island are cooled thanks to hot-quasiparticle extraction provided by tunnel-coupled V electrodes. Electronic temperature reduction down to 400 mK starting from 1 K is demonstrated with a cooling power ~20 pW at 1 K for a junction area of 0.3 micron^2. The present architecture extends to higher temperatures refrigeration based on tunneling between superconductors and paves the way to the implementation of a multi-stage on-chip cooling scheme operating from above 1 K down to the mK regime.
-[http://xxx.lanl.gov/abs/1011.0588 arXiv:1011.0588v1]
-'''Effect of oxygen plasma etching on graphene studied with Raman spectroscopy and electronic transport'''
-Authors: Isaac Childres, Luis A. Jauregui, Jifa Tian, Yong P. Chen
-(Submitted on 2 Nov 2010)
-Abstract: We report a study of graphene and graphene field effect devices after exposure to a series of short pulses of oxygen plasma. We present data from Raman spectroscopy, back-gated field-effect and magneto-transport measurements. The intensity ratio between Raman "D" and "G" peaks, I(D)/I(G) (commonly used to characterize disorder in graphene) is observed to increase approximately linearly with the number (N(e)) of plasma etching pulses initially, but then decreases at higher Ne. We also discuss implications of our data for extracting graphene crystalline domain sizes from I(D)/I(G). At the highest Ne measured, the "2D" peak is found to be nearly suppressed while the "D" peak is still prominent. Electronic transport measurements in plasma-etched graphene show an up-shifting of the Dirac point, indicating hole doping. We also characterize mobility, quantum Hall states, weak localization and various scattering lengths in a moderately etched sample. Our findings are valuable for understanding the effects of plasma etching on graphene and the physics of disordered graphene through artificially generated defects.
-[http://xxx.lanl.gov/abs/1011.0484 arXiv:1011.0484v1]
-'''Mesoscopic admittance of a double quantum dot'''
-Authors: Audrey Cottet, Christophe Mora, Takis Kontos
-(Submitted on 1 Nov 2010)
-Abstract: We calculate the mesoscopic admittance $G(\omega)$ of a double quantum dot, which can be measured directly using microwave techniques. This quantity shows a rich behavior. In particular, it is directly sensitive to Pauli spin blockade. We then discuss the problem of DQD coupled to a high quality photonic resonator. When the photon correlation functions can be developed along a RPA-like scheme, the behavior of the resonator can be predicted from $G(\omega)$
-[http://xxx.lanl.gov/abs/1011.0386 arXiv:1011.0386v1]
-'''Edge stability, reconstruction, zero-energy states and magnetism in triangular graphene quantum dots with zigzag edges'''
-Authors: Oleksandr Voznyy, Alev Devrim Güçlü, Pawel Potasz, Pawel Hawrylak
-(Submitted on 1 Nov 2010)
-Abstract: We present the results of ab-initio density functional theory based calculations of the stability and reconstruction of zigzag edges in triangular graphene quantum dots. We show that, while the reconstructed pentagon-heptagon zigzag edge structure is more stable in the absence of hydrogen, ideal zigzag edges are energetically favored by hydrogen passivation. Zero-energy band exists in both structures when passivated by hydrogen, however in case of pentagon-heptagon zigzag, this band is found to have stronger dispersion, leading to the loss of net magnetization.
-[http://xxx.lanl.gov/abs/1011.0369 arXiv:1011.0369v1]
-'''Interplay of the Kondo Effect and Spin-Polarized Transport in Magnetic Molecules, Adatoms and Quantum Dots'''
-Authors: Maciej Misiorny, Ireneusz Weymann, Jozef Barnas
-(Submitted on 28 Oct 2010)
-Abstract: We study the interplay of the Kondo effect and spin-polarized tunneling in a class of systems exhibiting uniaxial magnetic anisotropy, such as magnetic molecules, magnetic adatoms, or quantum dots coupled to a single localized magnetic moment. Using the numerical renormalization group method we calculate the spectral functions and linear conductance in the Kondo regime. We show that the exchange coupling between conducting electrons and localized magnetic core generally leads to suppression of the Kondo effect. We also predict a nontrivial dependence of the tunnel magnetoresistance on the strength of exchange coupling and on the anisotropy constant.
-[http://xxx.lanl.gov/abs/1010.6030 arXiv:1010.6030v1]
-'''Quantum dot spin filter in Kondo regime'''
-Authors: Mikio Eto, Tomohiro Yokoyama
-(Submitted on 28 Oct 2010)
-Abstract: A quantum dot with spin-orbit interaction can work as an efficient spin filter if it is connected to N (> 2) external leads via tunnel barriers. When an unpolarized current is injected to the quantum dot from a lead, polarized currents are ejected to the other leads. A two-level quantum dot is examined as a minimal model. First, we show that the spin polarization is remarkably enhanced by the resonant tunneling when the level spacing in the dot is smaller than the level broadening. Next, we examine the many-body resonance by the Kondo effect in the Coulomb blockade regime. A large spin current is generated in the presence of SU(4) Kondo effect when the level spacing is smaller than the Kondo temperature.
-[http://xxx.lanl.gov/abs/1010.5956 arXiv:1010.5956v1]
-'''π junction transition in InAs self-assembled quantum dot coupled with SQUID'''
-Authors: S. Kim, R. Ishiguro, M. Kamio, Y. Doda, E. Watanebe, K. Shibata, K. Hirakawa, H. Takayanagi
-(Submitted on 28 Oct 2010)
-Abstract: We report the transport measurements on the InAs self-assembled quantum dots (SAQDs) which have a unique structural zero-dimensionality, coupled to a superconducting quantum interference device (SQUID). Owing to the SQUID geometry, we directly observe a {\pi} phase shift in the current phase relation and the negative supercurrent indicating {\pi} junction behavior by not only tuning the energy level of SAQD by back-gate but also controlling the coupling between SAQD and electrodes by side-gate. Our results inspire new future quantum information devices which can link optical, spin, and superconducting state.
-[http://xxx.lanl.gov/abs/1010.5892 arXiv:1010.5892v1]
-'''Tunable Non-local Coupling between Kondo Impurities'''
-Authors: Daniel Tutuc, Bogdan Popescu, Dieter Schuh, Werner Wegscheider, Rolf J. Haug
-(Submitted on 27 Oct 2010)
-Abstract: We study the tuning mechanisms of the Ruderman-Kittel-Kasuya-Yosida (RKKY) exchange interaction between two lateral quantum dots in the Kondo regime. At zero magnetic field we observe the expected splitting of the Kondo resonance and measure the RKKY interaction strength J as a function of the asymmetry between the two Kondo temperatures. At finite magnetic fields a chiral coupling between the quantum dots is observed in the Kondo chessboard and we probe the presence of the exchange interaction by analyzing the Kondo temperature with magnetic field.
-[http://xxx.lanl.gov/abs/1010.5692 arXiv:1010.5692v1]
-'''Coupling molecular spin states by photon-assisted tunneling'''
-Authors: L. R. Schreiber, F. R. Braakman, T. Meunier, V. Calado, J. Danon, J. M. Taylor, W. Wegscheider, L. M. K. Vandersypen
-(Submitted on 27 Oct 2010)
-Abstract: Artificial molecules containing just one or two electrons provide a powerful platform for studies of orbital and spin quantum dynamics in nanoscale devices. A well-known example of these dynamics is tunneling of electrons between two coupled quantum dots triggered by microwave irradiation. So far, these tunneling processes have been treated as electric dipole-allowed spin-conserving events. Here we report that microwaves can also excite tunneling transitions between states with different spin. In this work, the dominant mechanism responsible for violation of spin conservation is the spin-orbit interaction. These transitions make it possible to perform detailed microwave spectroscopy of the molecular spin states of an artificial hydrogen molecule and open up the possibility of realizing full quantum control of a two spin system via microwave excitation.
-[http://xxx.lanl.gov/abs/1010.5682 arXiv:1010.5682v1]
-'''Spatially probed electron-electron scattering in a two-dimensional electron gas'''
-M. P. Jura, M. Grobis, M. A. Topinka, L. N. Pfeiffer, K. W. West, D. Goldhaber-Gordon
-Using scanning gate microscopy (SGM), we probe the scattering between a beam of electrons and a two-dimensional electron gas (2DEG) as a function of the beam's injection energy, and distance from the injection point. At low injection energies, we find electrons in the beam scatter by small-angles, as has been previously observed. At high injection energies, we find a surprising result: placing the SGM tip where it back-scatters electrons increases the differential conductance through the system. This effect is explained by a non-equilibrium distribution of electrons in a localized region of 2DEG near the injection point. Our data indicate that the spatial extent of this highly non-equilibrium distribution is within ~1 micrometer of the injection point. We approximate the non-equilibrium region as having an effective temperature that depends linearly upon injection energy.
-[http://xxx.lanl.gov/abs/1011.0106 arXiv:1011.0106v1]
-'''Cooling electrons from 1 K to 400 mK with V-based nanorefrigerators'''
-O. Quaranta, P. Spathis, F. Beltram, F. Giazotto
-The fabrication and operation of V-based superconducting nanorefrigerators is reported. Specifically, electrons in an Al island are cooled thanks to hot-quasiparticle extraction provided by tunnel-coupled V electrodes. Electronic temperature reduction down to 400 mK starting from 1 K is demonstrated with a cooling power ~20 pW at 1 K for a junction area of 0.3 micron^2. The present architecture extends to higher temperatures refrigeration based on tunneling between superconductors and paves the way to the implementation of a multi-stage on-chip cooling scheme operating from above 1 K down to the mK regime.
-[http://xxx.lanl.gov/abs/1011.0588 arXiv:1011.0588v1]
-----
-''Válogatta: Halbritter András''
-'''Large-Diameter Graphene Nanotubes Synthesized Using Ni Nanowire Templates'''
-Rui Wang†, Yufeng Hao†, Ziqian Wang†, Hao Gong‡, and John T. L. Thong
-We report a method to synthesize tubular graphene structures by chemical vapor deposition (CVD) on Ni nanowire templates, using ethylene as a precursor at growth temperature of around 750 °C. Unlike carbon nanotubes that are synthesized via conventional routes, the number of graphene layers is determined by the growth time and is independent of the tube diameter and tube length, which follow those of the nanowire template. This allows us to realize large-diameter tubes with shells comprising a few or many layers of graphene as desired. Thin graphene layers are observed to be highly crystalline, and of uniform thickness throughout the length of the nanowire. Raman analysis shows the presence of a small level of defects typical of CVD-grown graphene. The metallic core could be removed by chemical etching to result in a collapsed tube. Backgated field-effect transistor measurements were conducted on the collapsed graphene tube. This approach to the realization of tubular graphene offers new opportunities for graphene-based nanodevices.
-[http://dx.doi.org/10.1021/nl102445x Nano Letter ASAP October 28, 2010]
-'''Graphene Islands on Cu Foils: The Interplay between Shape, Orientation, and Defects'''
-Joseph M. Wofford†‡, Shu Nie§, Kevin F. McCarty§, Norman C. Bartelt§, and Oscar D. Dubon
-We have observed the growth of monolayer graphene on Cu foils using low-energy electron microscopy. On the (100)-textured surface of the foils, four-lobed, 4-fold-symmetric islands nucleate and grow. The graphene in each of the four lobes has a different crystallographic alignment with respect to the underlying Cu substrate. These “polycrystalline” islands arise from complex heterogeneous nucleation events at surface imperfections. The shape evolution of the lobes is well explained by an angularly dependent growth velocity. Well-ordered graphene forms only above 790 °C. Sublimation-induced motion of Cu steps during growth at this temperature creates a rough surface, where large Cu mounds form under the graphene islands. Strategies for improving the quality of monolayer graphene grown on Cu foils must address these fundamental defect-generating processes.
-[http://dx.doi.org/10.1021/nl102788f Nano Letters ASAP October 27, 2010]
-'''Controllable N-Doping of Graphene'''
-Beidou Guo†‡, Qian Liu†, Erdan Chen†, Hewei Zhu†, Liang Fang‡, and Jian Ru Gong*†
-Opening and tuning an energy gap in graphene are central to many electronic applications of graphene. Here we report N-doped graphene obtained by NH3 annealing after N+-ion irradiation of graphene samples. First, the evolution of the graphene microstructure was investigated following N+-ion irradiation at different fluences using Raman spectroscopy, showing that defects were introduced in plane after irradiation and then restored after annealing in N2 or in NH3. Auger electron spectroscopy (AES) of the graphene annealed in NH3 after irradiation showed N signal, however, no N signal was observed after annealing in N2. Last, the field-effect transistor (FET) was fabricated using N-doped graphene and monitored by the source−drain conductance and back-gate voltage (Gsd−Vg) curves in the measurement. The transport property changed compared to that of the FET made by intrinsic graphene, that is, the Dirac point position moved from positive Vg to negative Vg, indicating the transition of graphene from p-type to n-type after annealing in NH3. Our approach, which provides a physical mechanism for the introduction of defect and subsequent hetero dopant atoms into the graphene material in a controllable fashion, will be promising for producing graphene-based devices for multiple applications.
-[http://dx.doi.org/10.1021/nl103079j Nano Letters ASAP October 22, 2010]
-'''Surface State Transport and Ambipolar Electric Field Effect in Bi2Se3 Nanodevices'''
-Hadar Steinberg, Dillon R. Gardner, Young S. Lee, and Pablo Jarillo-Herrero
-Electronic transport experiments involving the topologically protected states found at the surface of Bi2Se3 and other topological insulators require fine control over carrier density, which is challenging with existing bulk-doped material. Here we report on electronic transport measurements on thin (<100 nm) Bi2Se3 devices and show that the density of the surface states can be modulated via the electric field effect by using a top-gate with a high-k dielectric insulator. The conductance dependence on geometry, gate voltage, and temperature all indicate that transport is governed by parallel surface and bulk contributions. Moreover, the conductance dependence on top-gate voltage is ambipolar, consistent with tuning between electrons and hole carriers at the surface.
-[http://dx.doi.org/10.1021/nl1032183 Nano Letters ASAP November 1, 2010]
-'''Ice Lithography for Nanodevices'''
-Anpan Han†, Dimitar Vlassarev†, Jenny Wang†, Jene A. Golovchenko†‡, and Daniel Branton
-We report the successful application of a new approach, ice lithography (IL), to fabricate nanoscale devices. The entire IL process takes place inside a modified scanning electron microscope (SEM), where a vapor-deposited film of water ice serves as a resist for e-beam lithography, greatly simplifying and streamlining device fabrication. We show that labile nanostructures such as carbon nanotubes can be safely imaged in an SEM when coated in ice. The ice film is patterned at high e-beam intensity and serves as a mask for lift-off without the device degradation and contamination associated with e-beam imaging and polymer resist residues. We demonstrate the IL preparation of carbon nanotube field effect transistors with high-quality trans-conductance properties.
-[http://dx.doi.org/10.1021/nl1032815 Nano Letter ASAP November 1, 2010]
-'''Nanoelectronics: Nanoribbons on the edge'''
-John A. Rogers
-Arrays of graphene nanoribbons are fabricated on structured silicon carbide substrates using self-organized growth, without lithography and with well-controlled widths.
-Graphene is attractive for electronics because of its exceptional properties and the relative ease with which it can be integrated into transistors and circuits. In the form of large-area planar sheets, it can be processed using straightforward adaptations of methods that are already in widespread use by the semiconductor industry.
-[http://www.nature.com/nnano/journal/v5/n10/full/nnano.2010.200.html Nature Nanotechnology News and Views 6 October 2010]
-'''Quantum tunnelling of the magnetization in a monolayer of oriented single-molecule magnets'''
-M. Mannini, F. Pineider, C. Danieli, F. Totti, L. Sorace, Ph. Sainctavit, M.-A. Arrio, E. Otero, L. Joly, J. C. Cezar, A. Cornia
-A fundamental step towards atomic- or molecular-scale spintronic devices has recently been made by demonstrating that the spin of an individual atom deposited on a surface1, or of a small paramagnetic molecule embedded in a nanojunction2, can be externally controlled. An appealing next step is the extension of such a capability to the field of information storage, by taking advantage of the magnetic bistability and rich quantum behaviour of single-molecule magnets3, 4, 5, 6 (SMMs). Recently, a proof of concept that the magnetic memory effect is retained when SMMs are chemically anchored to a metallic surface7 was provided. However, control of the nanoscale organization of these complex systems is required for SMMs to be integrated into molecular spintronic devices8, 9. Here we show that a preferential orientation of Fe4 complexes on a gold surface can be achieved by chemical tailoring. As a result, the most striking quantum feature of SMMs—their stepped hysteresis loop, which results from resonant quantum tunnelling of the magnetization5, 6—can be clearly detected using synchrotron-based spectroscopic techniques. With the aid of multiple theoretical approaches, we relate the angular dependence of the quantum tunnelling resonances to the adsorption geometry, and demonstrate that molecules predominantly lie with their easy axes close to the surface normal. Our findings prove that the quantum spin dynamics can be observed in SMMs chemically grafted to surfaces, and offer a tool to reveal the organization of matter at the nanoscale.
-[http://www.nature.com/nature/journal/vaop/ncurrent/full/nature09478.html Nature online 27 October 2010]
-'''Quantum physics: Tripping the light fantastic'''
-Geoff Pryde about the book "Dance of Photon: From Einstein to Quantum Teleportation" by Anton Zeilinger
-The only way to understand the quantum world is to measure it. This empirical view is dear to the heart of Anton Zeilinger, now at the University of Vienna, a leading figure in quantum physics through his work on correlated photons. In Dance of the Photons, he explores the phenomenon of quantum entanglement, the quantum correlations in the properties of particles.
-...
-Dance of the Photons is an enjoyable introduction to the strange world of quantum phenomena and the technologies they empower. It gives a foundation from which to ponder the nature of randomness and reality — and whether, in Vienna, the photon dance is performed to a Strauss waltz. Maybe Rupert can tell us over a lager, if he's ever allowed out of the tunnels.
-[http://www.nature.com/nature/journal/v467/n7319/full/4671042a.html Nature online 27 October 2010]
-== Okt. 14. - okt. 20. (2010) ==
-''Válogatta: Bordács Sándor''
-----
-'''Raman Scattering at Pure Graphene Zigzag Edges'''
-Benjamin Krauss, Péter Nemes-Incze, Viera Skakalova, László P. Biro, Klaus von Klitzing, and Jurgen H. Smet
-Theory has predicted rich and very distinct physics for graphene devices with boundaries that follow either the armchair or the zigzag crystallographic directions. A prerequisite to disclose this physics in experiment is to be able to produce devices with boundaries of pure chirality. Exfoliated flakes frequently exhibit corners with an odd multiple of 30°, which raised expectations that their boundaries follow pure zigzag and armchair directions. The predicted Raman behavior at such crystallographic edges however failed to confirm pure edge chirality. Here, we perform confocal Raman spectroscopy on hexagonal holes obtained after the anisotropic etching of prepatterned pits using carbothermal decomposition of SiO2. The boundaries of the hexagonal holes are aligned along the zigzag crystallographic direction and leave hardly any signature in the Raman map indicating unprecedented purity of the edge chirality. This work offers the first opportunity to experimentally confirm the validity of the Raman theory for graphene edges.
-[http://pubs.acs.org/doi/abs/10.1021/nl102526s Nano Letters ASAP (2010)]
-----
-'''Selective darkening of degenerate transitions demonstrated with two superconducting quantum bits'''
-P. C. de Groot, J. Lisenfeld, R. N. Schouten, S. Ashhab, A. Lupaşcu, C. J. P. M. Harmans & J. E. Mooij
-A new technique for controlling the quantum state of a superconducting qubit is now presented. Microwave pulses are applied in such a way that they excite only one of a pair of degenerate states. The concept enables construction of a controlled-NOT gate, a device important for quantum logic.
-[http://www.nature.com/nphys/journal/v6/n10/full/nphys1733.html Nature Physics 6, 763 (2010)]
-----
-'''Real-space mapping of magnetically quantized graphene states'''
-David L. Miller, Kevin D. Kubista, Gregory M. Rutter, Ming Ruan, Walt A. de Heer, Markus Kindermann, Phillip N. First & Joseph A. Stroscio
-Real-space mapping of the quantum Hall state at the Dirac point in epitaxial graphene reveals unexpected localized lifting of the degeneracy of this level. This could be the result of moiré interference caused by the twisting of the top layer with respect to underlying layers, suggesting possible new ways to understand and control the unusual properties of graphene.
-[http://www.nature.com/nphys/journal/v6/n10/full/nphys1736.html Nature Physics 6, 811 (2010)]
-----
-'''Andreev reflection between a normal metal and the FFLO superconductor II: a self-consistent approach'''
-J. Kaczmarczyk, M. Sadzikowski, J. Spałek
-We consider Andreev reflection in a two dimensional junction between a normal metal and a heavy fermion superconductor in the Fulde-Ferrell (FF) type of the Fulde-Ferrell-Larkin-Ovchinnikov (FFLO) state. We assume s-wave symmetry of the superconducting gap. The parameters of the superconductor: the gap magnitude, the chemical potential, and the Cooper pair center-of-mass momentum Q, are all determined self-consistently within a mean-field (BCS) scheme. The Cooper pair momentum Q is chosen as perpendicular to the junction interface. We calculate the junction conductance for a series of barrier strengths. In the case of incoming electron with spin \sigma = 1 only for magnetic fields close to the upper critical field H_{c2}, we obtain the so-called Andreev window i.e. the energy interval in which the reflection probability is maximal, which in turn is indicated by a peak in the conductance. The last result differs with other non-self-consistent calculations existing in the literature.
-[http://arxiv.org/abs/1010.4136 arXiv:1010.4136]
-----
-'''Low-field magnetoelectric effect at room temperature'''
-Yutaro Kitagawa, Yuji Hiraoka, Takashi Honda, Taishi Ishikura, Hiroyuki Nakamura & Tsuyoshi Kimura
-Only few magnetoelectric materials, where magnetism and ferroelectricity are coupled, are known to exist at room temperature, and in most cases the magnetoelectric coupling is weak. The discovery of strong room-temperature magnetoelectric coupling in Sr3Co2Fe24O41 at low magnetic fields is therefore a significant advance towards the practical application of multiferroics.
-[http://www.nature.com/nmat/journal/v9/n10/full/nmat2826.html Nature Materials 9, 797 (2010)]
-----
-'''Two-dimensional superconductivity at a Mott insulator/band insulator interface LaTiO3/SrTiO3'''
-J. Biscaras , N. Bergeal , A. Kushwaha , T. Wolf , A. Rastogi , R.C. Budhani & J. Lesueur
-Transition metal oxides show a great variety of quantum electronic behaviours where correlations often have an important role. The achievement of high-quality epitaxial interfaces involving such materials gives a unique opportunity to engineer artificial structures where new electronic orders take place. One of the most striking result in this area is the recent observation of a two-dimensional electron gas at the interface between a strongly correlated Mott insulator LaTiO3 and a band insulator SrTiO3. The mechanism responsible for such a behaviour is still under debate. In particular, the influence of the nature of the insulator has to be clarified. In this article, we show that despite the expected electronic correlations, LaTiO3/SrTiO3 heterostructures undergo a superconducting transition at a critical temperature Tconset~300 mK. We have found that the superconducting electron gas is confined over a typical thickness of 12 nm and is located mostly on the SrTiO3 substrate.
-[http://www.nature.com/ncomms/journal/v1/n7/full/ncomms1084.html Nature Communications 1, (2010)]
-----
-'''Chiral Charge-Density Waves'''
-J. Ishioka, Y. H. Liu, K. Shimatake, T. Kurosawa, K. Ichimura, Y. Toda, M. Oda, S. Tanda
-We discovered the chirality of charge-density waves (CDW) in 1T-TiSe2 by using STM and time-domain optical polarimetry. We found that the CDW intensity becomes Ia1∶Ia2∶Ia3=1∶0.7±0.1∶0.5±0.1, where Iai (i=1,2,3) is the amplitude of the tunneling current contributed by the CDWs. There were two states, in which the three intensity peaks of the CDW decrease clockwise and anticlockwise. The chirality in CDW results in the threefold symmetry breaking. Macroscopically, twofold symmetry was indeed observed in optical measurement. We propose the new generalized CDW chirality HCDW≡q1•(q2×q3), where qi are the CDW q vectors, which is independent of the symmetry of components. The nonzero HCDW—the triple-q vectors do not exist in an identical plane in the reciprocal space—should induce a real-space chirality in CDW system.
-[http://prl.aps.org/abstract/PRL/v105/i17/e176401 Physical Review Letters 105, 176401 (2010)]
-----
-'''Theory of electric polarization in multi-orbital Mott insulators'''
-Maxim Mostovoy, Kentaro Numura, Naoto Nagaosa
-The interaction between the electric field, E, and spins in multi-orbital Mott insulators is studied theoretically. We find a generic dynamical coupling mechanism, which works for all crystal lattices and which does not involve relativistic effects. The general form of the coupling is -T_ab E_a e_b, where e is the `internal' electric field originating from the dynamical Berry phase of electrons and T_ab is a tensor determined by lattice symmetry. We discuss several effects of this interaction: (i) an unusual electron spin resonance induced by an oscillating electric field, (ii) the displacement of spin textures in an applied electric field, and (iii) the resonant absorption of circularly polarized light by Skyrmions, magnetic bubbles, and magnetic vortices.
-[http://arxiv.org/abs/1010.3687 arXiv:1010.3687v1]
-== Okt. 7. - okt. 13. (2010) ==
-''Válogatta: Makk Péter''
-----
-'''An All-Electric Single-Molecule Motor'''
-Johannes S. Seldenthuis, Ferry Prins, Joseph M. Thijssen, and Herre S. J. van der Zant
-Many types of molecular motors have been proposed and synthesized in recent years, displaying different kinds of motion, and fueled by different driving forces such as light, heat, or chemical reactions. We propose a new type of molecular motor based on electric field actuation and electric current detection of the rotational motion of a molecular dipole embedded in a three-terminal single-molecule device. The key aspect of this all-electronic design is the conjugated backbone of the molecule, which simultaneously provides the potential landscape of the rotor orientation and a real-time measure of that orientation through the modulation of the conductivity. Using quantum chemistry calculations, we show that this approach provides full control over the speed and continuity of motion, thereby combining electrical and mechanical control at the molecular level over a wide range of temperatures. Moreover, chemistry can be used to change all key parameters of the device, enabling a variety of new experiments on molecular motors.
-[http://pubs.acs.org/doi/abs/10.1021/nn1021499 ACS Nano ASAP(2010)]
-----
-'''Time-resolved detection of spin-transfer-driven ferromagnetic resonance and spin torque measurement in magnetic tunnel junctions'''
-Chen Wang, Yong-Tao Cui, Jordan A. Katine, Robert A. Buhrman, Daniel C. Ralph
-Several experimental techniques have been introduced in recent years in attempts to measure spin transfer torque in magnetic tunnel junctions (MTJs). The dependence of spin torque on bias is important for understanding fundamental spin physics in magnetic devices and for applications. However, previous techniques have provided only indirect measures of the torque and their results to date for the bias dependence are qualitatively and quantitatively inconsistent. Here we demonstrate that spin torque in MTJs can be measured directly by using time-domain techniques to detect resonant magnetic precession in response to an oscillating spin torque. The technique is accurate in the high-bias regime relevant for applications, and because it detects directly small-angle linear-response magnetic dynamics caused by spin torque it is relatively immune to artifacts affecting competing techniques. At high bias we find that the spin torque vector differs markedly from the simple lowest-order Taylor series approximations commonly assumed.
-[http://arxiv.org/abs/1010.1777v1 arXiv:1010.1777v1]
-----
-'''Gate-Defined Graphene Quantum Point Contact in the Quantum Hall Regime'''
-S. Nakaharai, J. R. Williams, C. M. Marcus
-We investigate transport in a gate-defined graphene quantum point contact in the quantum Hall regime. Edge states confined to the interface of p and n regions in the graphene sheet are controllably brought together from opposite sides of the sample and allowed to mix in this split-gate geometry. Among the expected quantum Hall features, an unexpected additional plateau at 0.5 h/e^2 is observed. We propose that chaotic mixing of edge channels gives rise to the extra plateau.
-[http://arxiv.org/abs/1010.1919v1 arXiv:1010.1919v1]
-----
-'''Spin-polarization of platinum (111) induced by the proximity to cobalt nanostripes'''
-Focko Meier, Samir Lounis, Jens Wiebe, Lihui Zhou, Swantje Heers, Phivos Mavropoulos, Peter H. Dederichs, Stefan Blügel, Roland Wiesendanger
-We measured a spin polarization above a Pt (111) surface in the vicinity of a Co nanostripe by spin-polarized scanning tunneling spectroscopy. The spin polarization is exponentially decaying away from the Pt/Co interface and is detectable at distances larger than 1 nm. By performing self-consistent ab-initio calculations of the electronic-structure for a related model system we reveal the interplay between the induced magnetic moments within the Pt surface and the spin-resolved electronic density of states above the surface.
-[http://arxiv.org/abs/1010.2109v1 arXiv:1010.2109v1]
-----
-'''Coulomb-driven broken-symmetry states in doubly gated suspended bilayer graphene'''
-R. Thomas Weitz, Monica T. Allen, Benjamin E. Feldman, Jens Martin, Amir Yacoby
-The non-interacting energy spectrum of graphene and its bilayer counterpart consists of multiple degeneracies owing to the inherent spin, valley and layer symmetries. Interactions among charge carriers are expected to spontaneously break these symmetries, leading to gapped ordered states. In the quantum Hall regime these states are predicted to be ferromagnetic in nature whereby the system becomes spin polarized, layer polarized or both. In bilayer graphene, due to its parabolic dispersion, interaction-induced symmetry breaking is already expected at zero magnetic field. In this work, the underlying order of the various broken-symmetry states is investigated in bilayer graphene that is suspended between top and bottom gate electrodes. By controllably breaking the spin and sublattice symmetries we are able to deduce the order parameter of the various quantum Hall ferromagnetic states. At small carrier densities, we identify for the first time three distinct broken symmetry states, one of which is consistent with either spontaneously broken time-reversal symmetry or spontaneously broken rotational symmetry.
-[http://arxiv.org/abs/1010.0989v1 arXiv:1010.0989v1]
-----
-'''Measurement of the \nu= 1/3 fractional quantum Hall energy gap in suspended graphene'''
-Fereshte Ghahari, Yue Zhao, Paul Cadden-Zimansky, Kirill Bolotin, Philip Kim
-We report on magnetotransport measurements of multi-terminal suspended graphene devices. Fully developed integer quantum Hall states appear in magnetic fields as low as 2 T. At higher fields the formation of longitudinal resistance minima and transverse resistance plateaus are seen corresponding to fractional quantum Hall states, most strongly for \nu= 1/3. By measuring the temperature dependence of these resistance minima, the energy gap for the 1/3 fractional state in graphene is determined to be at ~20 K at 14 T. This gap is at least 3 times larger than the observed gaps for the corresponding state in the best quality semiconductor heterostructures.
-[http://arxiv.org/abs/1010.1187v1 arXiv:1010.1187v1]
-----
-'''Multicomponent fractional quantum Hall effect in graphene'''
-C.R. Dean, A.F. Young, P. Cadden-Zimansky, L. Wang, H. Ren, K. Watanabe, T. Taniguchi, P. Kim, J.
-Hone, K.L. Shepard
-We report observation of the fractional quantum Hall effect (FQHE) in high mobility multi-terminal graphene devices, fabricated on a single crystal boron nitride substrate. We observe an unexpected hierarchy in the emergent FQHE states that may be explained by strongly interacting composite Fermions with full SU(4) symmetric underlying degrees of freedom. The FQHE gaps are measured from temperature dependent transport to be up 10 times larger than in any other semiconductor system. The remarkable strength and unusual hierarcy of the FQHE described here provides a unique opportunity to probe correlated behavior in the presence of expanded quantum degrees of freedom.
-[http://arxiv.org/abs/1010.1179v1 arXiv:1010.1179v1]
-----
-'''Mean-field quantum phase transition in graphene and in general gapless systems '''
-Ádám Bácsi, Attila Virosztek, László Borda, and Balázs Dóra
-We study the quantum-critical properties of antiferromagnetism in graphene at T=0 within mean-field (MF) theory. The resulting exponents differ from the conventional MF exponents, describing finite-temperature transitions. Motivated by this, we have developed the MF theory of general gapless phases with density of states ρ(ε)∼|ε|r, r>−1, with the interaction as control parameter. For r>2, the conventional MF exponents à la Landau are recovered, while for −1<r<2, the exponents vary significantly with r. The critical interaction is finite for r>0, therefore no weak-coupling solution exists in this range. This generalizes the results on quantum criticality of the gapless Kondo systems to bulk correlated phases.
-[http://prb.aps.org/abstract/PRB/v82/i15/e153406 Phys. Rev. B 82, 153406 (2010)]
-----
-'''Josephson current in ballistic superconductor-graphene systems'''
-Imre Hagymási, Andor Kormányos, and József Cserti
-We calculate the phase, the temperature and the junction length dependence of the supercurrent for ballistic graphene Josephson junctions. For low temperatures we find nonsinusoidal dependence of the supercurrent on the superconductor phase difference for both short and long junctions. The skewness, which characterizes the deviaton of the current-phase relation from a simple sinusoidal one, shows a linear dependence on the critical current for small currents. We discuss the similarities and differences with respect to the classical theory of Josephson junctions, where the weak link is formed by a diffusive or ballistic metal. The relation to other recent theoretical results on graphene Josephson junctions is pointed out and the possible experimental relevance of our work is considered as well.
-[http://prb.aps.org/abstract/PRB/v82/i13/e134516 Phys. Rev. B 82, 134516 (2010)]
-----
-'''Wafer Scale Homogeneous Bilayer Graphene Films by Chemical Vapor Deposition'''
-Seunghyun Lee, Kyunghoon Lee, and Zhaohui Zhong
-The discovery of electric field induced band gap opening in bilayer graphene opens a new door for making semiconducting graphene without aggressive size scaling or using expensive substrates. However, bilayer graphene samples have been limited to μm2 size scale thus far, and synthesis of wafer scale bilayer graphene poses a tremendous challenge. Here we report homogeneous bilayer graphene films over at least a 2 in. × 2 in. area, synthesized by chemical vapor deposition on copper foil and subsequently transferred to arbitrary substrates. The bilayer nature of graphene film is verified by Raman spectroscopy, atomic force microscopy, and transmission electron microscopy. Importantly, spatially resolved Raman spectroscopy confirms a bilayer coverage of over 99%. The homogeneity of the film is further supported by electrical transport measurements on dual-gate bilayer graphene transistors, in which a band gap opening is observed in 98% of the devices.
-[http://pubs.acs.org/doi/abs/10.1021/nl1029978#cor1 Nano Lett.,, Article ASAP,  DOI: 10.1021/nl1029978]
-----
-'''The Relation between Structure and Quantum Interference in Single Molecule Junctions'''
-Troels Markussen, Robert Stadler, and Kristian S. Thygesen
-Quantum interference (QI) of electron pathways has recently attracted increased interest as an enabling tool for single-molecule electronic devices. Although various molecular systems have been shown to exhibit QI effects and a number of methods have been proposed for its analysis, simple guidelines linking the molecular structure to QI effects in the phase-coherent transport regime have until now been lacking. In the present work we demonstrate that QI in aromatic molecules is intimately related to the topology of the molecule’s π system and establish a simple graphical scheme to predict the existence of QI-induced transmission antiresonances. The generality of the scheme, which is exact for a certain class of tight-binding models, is proved by a comparison to first-principles transport calculations for 10 different configurations of anthraquinone as well as a set of cross-conjugated molecular wires.
-[http://pubs.acs.org/doi/abs/10.1021/nl101688a Nano Lett., Article ASAP, DOI: 10.1021/nl101688a]
-----
-'''Hybrid superconductor–quantum dot devices'''
-Silvano De Franceschi, Leo Kouwenhoven, Christian Schönenberger & Wolfgang Wernsdorfer
-Advances in nanofabrication techniques have made it possible to make devices in which superconducting electrodes are connected to non-superconducting nanostructures such as quantum dots. The properties of these hybrid devices result from a combination of a macroscopic quantum phenomenon involving large numbers of electrons (superconductivity) and the ability to control single electrons, offered by quantum dots. Here we review research into electron transport and other fundamental processes that have been studied in these devices. We also describe potential applications, such as a transistor in which the direction of a supercurrent can be reversed by adding just one electron to a quantum dot.
-[http://www.nature.com/nnano/journal/v5/n10/pdf/nnano.2010.173.pdf Nature Nanotechnology 5, 703 - 711 (2010)]
-----
-'''Boron nitride substrates for high-quality graphene electronics'''
-C. R. Dean, A. F. Young, I. Meric, C. Lee, L. Wang, S. Sorgenfrei, K. Watanabe, T. Taniguchi, P. Kim, K. L. Shepard & J. Hone
-Graphene devices on standard SiO2 substrates are highly disordered, exhibiting characteristics that are far inferior to the expected intrinsic properties of graphene. Although suspending the graphene above the substrate leads to a substantial improvement in device quality, this geometry imposes severe limitations on device architecture and functionality. There is a growing need, therefore, to identify dielectrics that allow a substrate-supported geometry while retaining the quality achieved with a suspended sample. Hexagonal boron nitride (h-BN) is an appealing substrate, because it has an atomically smooth surface that is relatively free of dangling bonds and charge traps. It also has a lattice constant similar to that of graphite, and has large optical phonon modes and a large electrical bandgap. Here we report the fabrication and characterization of high-quality exfoliated mono- and bilayer graphene devices on single-crystal h-BN substrates, by using a mechanical transfer process. Graphene devices on h-BN substrates have mobilities and carrier inhomogeneities that are almost an order of magnitude better than devices on SiO2. These devices also show reduced roughness, intrinsic doping and chemical reactivity. The ability to assemble crystalline layered materials in a controlled way permits the fabrication of graphene devices on other promising dielectrics and allows for the realization of more complex graphene heterostructures.
-[http://www.nature.com/nnano/journal/v5/n10/abs/nnano.2010.172.html Nature Nanotechnology 5,722–726 (2010)]
-----
-'''Direct observation of single-charge-detection capability of nanowire field-effect transistors'''
-J. Salfi I. G. Savelyev, M. Blumin, S. V. Nair  &  H. E. Ruda
-A single localized charge can quench the luminescence of a semiconductor nanowire, but relatively little is known about the effect of single charges on the conductance of the nanowire. In one-dimensional nanostructures embedded in a material with a low dielectric permittivity, the Coulomb interaction and excitonic binding energy are much larger than the corresponding values when embedded in a material with the same dielectric permittivity. The stronger Coulomb interaction is also predicted to limit the carrier mobility in nanowires. Here, we experimentally isolate and study the effect of individual localized electrons on carrier transport in InAs nanowire field-effect transistors, and extract the equivalent charge sensitivity. In the low carrier density regime, the electrostatic potential produced by one electron can create an insulating weak link in an otherwise conducting nanowire field-effect transistor, modulating its conductance by as much as 4,200% at 31 K. The equivalent charge sensitivity, 4 × 10−5 e Hz−1/2 at 25 K and 6 × 10−5 e Hz−1/2 at 198 K, is orders of magnitude better than conventional field-effect transistors5 and nanoelectromechanical systems, and is just a factor of 20–30 away from the record sensitivity for state-of-the-art single-electron transistors operating below 4 K (ref. 8). This work demonstrates the feasibility of nanowire-based single-electron memories and illustrates a physical process of potential relevance for high performance chemical sensors. The charge-state-detection capability we demonstrate also makes the nanowire field-effect transistor a promising host system for impurities (which may be introduced intentionally or unintentionally) with potentially long spin lifetimes, because such transistors offer more sensitive spin-to-charge conversion readout than schemes based on conventional field-effect transistors.
-[http://www.nature.com/nnano/journal/v5/n10/full/nnano.2010.180.html Nature Nanotechnology 5, 737 - 741 (2010)]
-----
-'''Hybrid InAs nanowire-vanadium proximity SQUID'''
-Panayotis Spathis, Subhajit Biswas, Stefano Roddaro, L.Sorba, F.Giazotto, Fabio Beltram
-We report the fabrication and characterization of superconducting quantum interference devices (SQUIDs) based on InAs nanowires and vanadium superconducting electrodes. These mesoscopic devices are found to be extremely robust against thermal cycling and to operate up to temperatures of $\sim2.5$~K with reduced power dissipation. We show that our geometry allows to obtain nearly-symmetric devices with very large magnetic-field modulation of the critical current. All these properties make these devices attractive for on-chip quantum-circuit implementation.
-[http://arxiv.org/abs/1010.2545v1 arXiv:1010.2545v1]
-----
-'''Chemical Functionalization of Graphene Enabled by Phage Displayed Peptides'''
-Yue Cui†, Sang N. Kim, Sharon E. Jones, L.L. Wissler, Rajesh R. Naik, and Michael C. McAlpine
-The development of a general approach for the nondestructive chemical and biological functionalization of graphene could expand opportunities for graphene in both fundamental studies and a variety of device platforms. Graphene is a delicate single-layer, two-dimensional network of carbon atoms whose properties can be affected by covalent modification. One method for functionalizing materials without fundamentally changing their inherent structure is using biorecognition moieties. In particular, oligopeptides are molecules containing a broad chemical diversity that can be achieved within a relatively compact size. Phage display is a dominant method for identifying peptides that possess enhanced selectivity toward a particular target. Here, we demonstrate a powerful yet benign approach for chemical functionalization of graphene via comprehensively screened phage displayed peptides. Our results show that graphene can be selectively recognized even in nanometer-defined strips. Further, modification of graphene with bifunctional peptides reveals both the ability to impart selective recognition of gold nanoparticles and the development of an ultrasensitive graphene-based TNT sensor. We anticipate that these results could open exciting opportunities in the use of graphene in fundamental biochemical recognition studies, as well as applications ranging from sensors to energy storage devices.
-[http://pubs.acs.org/doi/abs/10.1021/nl102564d Nano Lett., Article ASAP, DOI: 10.1021/nl102564d]
-== Szept. 30. - okt. 6. (2010) ==
-''Válogatta: Geresdi Attila''
-----
-'''Spin Seebeck insulator'''
-K. Uchida, J. Xiao, H. Adachi, J. Ohe, S. Takahashi, J. Ieda, T. Ota, Y. Kajiwara, H. Umezawa, H. Kawai, G. E.W. Bauer, S. Maekawa and E. Saitoh
-Thermoelectric generation is an essential function in future energy-saving technologies. However, it has so far been an exclusive feature of electric conductors, a situation which limits its application; conduction electrons are often problematic in the thermal design of devices. Here we report electric voltage generation from heat flowing in an insulator. We reveal that, despite the absence of conduction electrons, the magnetic insulator LaY2Fe5O12 can convert a heat flow into a spin voltage. Attached Pt films can then transform this spin voltage into an electric voltage as a result of the inverse spin Hall effect. The experimental results require us to introduce a thermally activated interface spin exchange between LaY2Fe5O12 and Pt. Our findings extend the range of potential materials for thermoelectric applications and provide a crucial piece of information for understanding the physics of the spin Seebeck effect.
-Nature Materials, DOI:[http://dx.doi.org/10.1038/NMAT2856 10.1038/NMAT2856]
-----
-'''Nobel Prize 2010: Geim and Novoselov'''
-Ed Gerstner
-The 2010 Nobel Prize in Physics has been awarded to Andre Geim and Konstantin Novoselov, “for groundbreaking experiments regarding the two-dimensional material graphene”.
-Nature Physics, DOI:[http://dx.doi.org/10.1038/nphys1836 10.1038/nphys1836]
-----
-'''Electrical Measurement of the Direct Spin Hall Effect in Fe/InxGa1-xAs Heterostructures'''
-E. S. Garlid, Q. O. Hu, M. K. Chan, C. J. Palmstrøm, and P. A. Crowell
-We report on an all-electrical measurement of the spin Hall effect in epitaxial Fe/InxGa1-xAs heterostructures with n-type (Si) channel doping and highly doped Schottky tunnel barriers. A transverse spin current generated by an ordinary charge current flowing in the InxGa1_xAs is detected by measuring the spin accumulation at the edges of the channel. The spin accumulation is identified through the observation of a Hanle effect in the voltage measured by pairs of ferromagnetic Hall contacts. We investigate the bias and temperature dependence of the resulting Hanle signal and determine the skew and side-jump contributions to the total spin Hall conductivity.
-Phys. Rev. Letters, DOI:[http://dx.doi.org/10.1103/PhysRevLett.105.156602 10.1103/PhysRevLett.105.156602]
-----
-'''Fast domain wall motion in magnetic comb structures'''
-E. R. Lewis, D. Petit, L. O’Brien, A. Fernandez-Pacheco, J. Sampaio, A-V. Jausovec, H. T. Zeng, D. E. Read and R. P. Cowburn
-Modern fabrication technology has enabled the study of submicron ferromagnetic strips with a particularly simple domain structure, allowing single, well-defined domain walls to be isolated and characterized. However, these domain walls have complex field-driven dynamics. The wall velocity initially increases with field, but above a certain threshold the domain wall abruptly slows down, accompanied by periodic transformations of the domain wall structure. This behaviour is potentially detrimental to the speed and proper functioning of proposed domain-wall-based devices, and although methods for suppression of the breakdown have been demonstrated in simulations, a convincing experimental demonstration is lacking. Here, we show experimentally that a series of crossshaped traps acts to prevent transformations of the domain wall structure and increase the domain wall velocity by a factor of four compared to the maximum velocity on a plain strip. Our results suggest a route to faster and more reliable domain wall devices for memory, logic and sensing.
-Nature Materials, DOI:[http://dx.doi.org/10.1038/NMAT2857 10.1038/NMAT2857]
-----
-'''Nanomaterials: Graphene rests easy'''
-R. Thomas Weitz & Amir Yacoby
-Samples of graphene supported on boron nitride demonstrate superior electrical  properties, achieving levels of performance that are comparable to those observed with suspended samples.
-Nature Nano, DOI:[http://dx.doi.org/10.1038/nnano.2010.201 10.1038/nnano.2010.201]
-----
-'''Nanoelectronics: Nanoribbons on the edge'''
-John A. Rogers
-Arrays of graphene nanoribbons are fabricated on structured silicon carbide substrates using self-organized growth, without lithography and with well-controlled widths.
-Nature Nano, DOI:[http://dx.doi.org/10.1038/nnano.2010.200 10.1038/nnano.2010.200]
-----
-'''Nanopores: Graphene opens up to DNA'''
-Zuzanna S. Siwy & Matthew Davenport
-It might be possible to sequence DNA by passing the molecule through a small hole in a sheet of graphene. The nanopores that are found in the membranes of cells have an important role in biology and, along with artificial nanopores fabricated in materials such as silicon nitride, they have also been used to detect single molecules and, in some cases, extract more detailed information such as the size and shape of the molecules1. The capabilities of these systems are influenced by the diameter of the nanopore and also by the thickness of the membrane that contains it.
-Nature Nano, DOI:[http://dx.doi.org/10.1038/nnano.2010.198 10.1038/nnano.2010.198]