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HIGHLIGHTED ARTICLES

Intertube effects on one-dimensional correlated state of metallic single-wall carbon nanotubes probed by C13 NMR

Noboru Serita, Yusuke Nakai, Kazuyuki Matsuda, Kazuhiro Yanagi, Yasumitsu Miyata, Takeshi Saito, and Yutaka Maniwa

Phys. Rev. B 95, 035128 (2017) - Published 18 January, 2017

Due to the one-dimensional nature of single-wall carbon nanotubes (SWCNTs), electron-electron interactions are of great importance because the lack of screening enhances the effective Coulomb interactions between electrons, and individual SWCNTs have been considered as an ideal realization of a Tomonaga-Luttinger liquid (TLL). In an actual SWCNT sample, SWCNTs usually pack together closely and form a bundle structure, in which intertube effects may alter the TLL state significantly. Here, the authors study the TLL effect in bundles of metallic SWCNTs using 13C nuclear magnetic resonance techniques to understand how the intertube effects alter the electron-electron interaction in the bundle form. They find a modified charge Luttinger parameter for the bundled metallic SWCNTs. Their findings give direct evidence that bundling reduces the effective Coulomb interactions via intertube interactions within bundled metallic SWCNTs.

Many-body localization in the presence of a small bath

Katharine Hyatt, James R. Garrison, Andrew C. Potter, and Bela Bauer

Phys. Rev. B 95, 035132 (2017) - Published 19 January, 2017

In the presence of strong disorder and weak interactions, closed quantum systems can enter a many-body localized phase wherein the system does not conduct heat or charge, does not equilibrate even for arbitrarily long times, and robustly violates quantum statistical mechanics. While this is well established in closed quantum systems, the interplay of such systems with delocalized degrees of freedom is much less understood. Here, the authors consider a model for which, in the noninteracting limit, some degrees of freedom are localized while others remain delocalized. Such a system can be viewed as a model for a many-body localized system brought into contact with a small bath of a comparable number of degrees of freedom. The authors numerically and analytically study the effect of interactions on this system and find that in certain parameter regimes, results are consistent with interaction-induced localization of the entire system.

Type-II Dirac surface states in topological crystalline insulators

Ching-Kai Chiu, Y.-H. Chan, Xiao Li, Y. Nohara, and A. P. Schnyder

Phys. Rev. B 95, 035151 (2017) - Published 30 January, 2017

Topological crystalline insulators are insulating in the bulk, but exhibit conducting surface states protected by crystal symmetries. Here, the authors show that the surface states of crystalline topological insulators come in two different varieties: (i) as standard Dirac cones with pointlike Fermi surfaces (type-I) and (ii) as tilted Dirac cones that appear at the contact of electron and hole pockets. They call these new tilted surface states “type-II Dirac states” in analogy to the three-dimensional type-II Weyl points that have been recently discovered in WTe2. These type-II Dirac states can exist only at the surface of topological crystalline insulators, but are absent in ordinary topological insulators, where they are forbidden by symmetry. The two types of Dirac surface states have very different physical properties, in particular with regards to their thermodynamics and magnetotransport. The authors predict that the antiperovskites A3EO are an example of a crystalline topological insulator that hosts the type-II Dirac surface states.

P·T·D symmetry-protected scattering anomaly in optics

Mário G. Silveirinha

Phys. Rev. B 95, 035153 (2017) - Published 30 January, 2017

Light waves propagating in optical fibers or other guides are usually vulnerable to defects or channel deformations, such as twisting and bending. These perturbations invariably generate undesired reflections and scattering and typically imply a power penalty. Here, building on an analogy with electronics and with the spin Hall effect, the author unveils a general theoretical solution for this dilemma. It is shown that there is a wide class of three-dimensional metamaterial platforms protected by a particular symmetry – a combination of a geometrical operation with other more subtle symmetries of the materials response – that guarantees bidirectional transport of light totally free of reflections, independent of the specific geometry of the propagation channel and other imperfections. Crucially, this scattering anomaly only requires the symmetry protection in the frequency range of interest, and hence relies on much weaker assumptions than topological theories.

Resonant optical spectroscopy and coherent control of Cr4+ spin ensembles in SiC and GaN

William F. Koehl, Berk Diler, Samuel J. Whiteley, Alexandre Bourassa, N. T. Son, Erik Janzén, and David D. Awschalom

Phys. Rev. B 95, 035207 (2017) - Published 19 January, 2017

The authors identify a new class of optically controllable, semiconductor-based defect spin that is formed from the d-orbital electrons of chromium ions in silicon carbide and gallium nitride. These ions possess a simple lambda optical structure that couples only weakly to phonons and lattice strain. Therefore, even though they probe an ensemble of many ions at once with varying strain environments, the optical transitions they observe are exceptionally narrow and possess a high radiative efficiency. These properties allow the authors to individually interrogate the magnetic sublevels of the ground-state spin using resonant optical excitation, enabling ensemble optical spin polarization as well as optically detected magnetic resonance in the time domain. Each ion species emits the majority of its luminescence within a near-infrared zero-phonon line, suggesting a capacity for efficient photonic integration. Additionally, as magnetically active d-orbital states, the spins of these ions possess a number of degrees of design freedom not available to other common defect spin species such as those based on vacancy complexes. The authors therefore expect that these studies will broaden the range of opportunities available to semiconductor-based quantum device engineering, and will motivate further explorations into the use of transition metal ions as optically active qubit states.

Quantum oscillations in a lead chalcogenide three-dimensional Dirac system

Filip Orbanić, Mario Novak, Mirko Baćani, and Ivan Kokanović

Phys. Rev. B 95, 035208 (2017) - Published 20 January, 2017

The three-dimensional (3D) Dirac materials represent a dimensional extension of the two-dimensional physics seen in graphene. Recently, two types of 3D Dirac materials have been proposed. The first type are the symmetry protected 3D Dirac materials with the Cd3As2 as the representative material. The second type are materials with accidental touching of the conduction and valence bands in a single point. In this paper, the authors are reporting bulk quantum oscillations in Pb1-xSnxSe, a latter type of material, which has also been recently identified as a topological crystalline insulator with a topological phase transition predicted to take place at x=0.17. The authors have used the quantum oscillations in resistivity and magnetization to identify the phase of the oscillation and prove that this material has the 3D Dirac linear dispersion for x=0.17. Combining the oscillations in the resistivity and magnetization, the authors provide the consistent indexing method for drawing the Landau level diagrams that are used in identifying the Berry phase.

Resonant optical control of the spin of a single Cr atom in a quantum dot

A. Lafuente-Sampietro, H. Utsumi, H. Boukari, S. Kuroda, and L. Besombes

Phys. Rev. B 95, 035303 (2017) - Published 10 January, 2017

A Cr atom in a semiconductor host carries a localized spin with an intrinsic large spin to strain coupling particularly promising for the development of hybrid spin-mechanical systems. The authors demonstrate here that the spin of an individual Cr atom can be controlled optically. To optically access to the spin of an individual atom, they insert it in a cadmium telluride quantum dot. With a single Cr atom introduced in the quantum dot, the energy and polarization of the photon emitted or absorbed by the dot depends on the spin state of the magnetic atom. The authors first show that excitation with a laser beam tuned to the wavelength of one of these optical transitions can be used to initialize the state of the Cr spin and to probe its dynamics optically: the Cr behaves like an optically addressable spin-based memory. Under optical excitation exactly resonant with an absorption transition one can also enter the strong coupling regime where hybrid states of matter and light are created. The spin-dependent strong coupling with the laser field is exploited to optically tune the Cr atom’s energy levels.

Light-hole exciton in a nanowire quantum dot

Mathieu Jeannin, Alberto Artioli, Pamela Rueda-Fonseca, Edith Bellet-Amalric, Kuntheak Kheng, Régis André, Serge Tatarenko, Joël Cibert, David Ferrand, and Gilles Nogues

Phys. Rev. B 95, 035305 (2017) - Published 17 January, 2017

Quantum dots are promising building blocks for future optoelectronics or quantum information applications. Many of their properties derive from the quantum state of the hole trapped in the dot. “Light” and “heavy” hole states differ by the anisotropic character of their spin and of the electric dipole they form with a trapped electron. Light holes are of particular interest as they offer extended opportunities for optical manipulation of single carriers, or the electrical manipulation of magnetic objects. Here, the authors demonstrate that the hole ground state can be engineered through a proper design of the strain built in the dot when inserted inside a nanowire of a different lattice parameter. Two complementary techniques provide evidence of a light hole state: polarization-resolved Fourier imaging, which is sensitive to the nature of the electron-hole electric dipole, and magneto-optical spectroscopy, which probes the hole spin state through its coupling to magnetic atoms.

Anomalous Fraunhofer interference in epitaxial superconductor-semiconductor Josephson junctions

H. J. Suominen, J. Danon, M. Kjaergaard, K. Flensberg, J. Shabani, C. J. Palmstrøm, F. Nichele, and C. M. Marcus

Phys. Rev. B 95, 035307 (2017) - Published 18 January, 2017

Fraunhofer interference is a paradigmatic phenomena arising due to phase coherence in diverse systems from optics to superconducting junctions. In Josephson junctions, coupling two superconductors through a weak link, such patterns arise in the maximal dissipationless current the system can sustain, oscillating as function of a perpendicular applied magnetic field. By investigating this effect in a recently realized material system epitaxially coupling a thin superconductor to a semiconducting region, the authors here discover novel effects arising due to a combination of magnetic field screening, spin physics, and disorder. In an appropriately aligned in-plane magnetic field, they find that due to screening by the superconducting leads, a flux dipole develops in the semiconducting region leading to an effective confinement of the superconducting states to edges of the intervening semiconducting region. When the out-of-plane field is swept in the presence of an in-plane field, striking asymmetries in the Fraunhofer pattern are observed. By analyzing the underlying theoretical symmetries of the system, they demonstrate that such an effect arises as a result of an intricate interplay between disorder in the junction, splitting of the spin states in the applied field, and coupling between the momentum of the electrons and their spin.

Photon echoes from (In,Ga)As quantum dots embedded in a Tamm-plasmon microcavity

M. Salewski, S. V. Poltavtsev, Yu. V. Kapitonov, J. Vondran, D. R. Yakovlev, C. Schneider, M. Kamp, S. Höfling, R. Oulton, I. A. Akimov, A. V. Kavokin, and M. Bayer

Phys. Rev. B 95, 035312 (2017) - Published 30 January, 2017

Tamm resonators are an alternate type of cavities, in which the light-matter interaction may be significantly enhanced, as required for many applications in photonics or optoelectronics. A Tamm resonator comprises at least one metal layer as mirror, in the present case combined with a distributed Bragg reflector. The metal layer may turn out to be useful, for example, for injecting carriers or applying an electric field. Here, the authors use photon echoes in the exciton four-wave mixing signal to demonstrate that the studied Tamm resonator, which contains quantum dots as the optically active medium, allows one to perform coherent manipulations on quantum-dot excitons at power levels more than one order of magnitude lower than those required for bare quantum dots. This occurs despite the moderate quality factor of about 100. Moreover, it speeds up the radiative decay of the excitons by a factor of two (the so-called “Purcell effect”). On the other hand, the coherence of the quantum dot exciton, which may become compromised by plasmon excitations in the metal, is hardly shortened. These results demonstrate that Tamm resonators are indeed prospective candidates for performing coherent optical manipulations.

Many-body theory of trion absorption features in two-dimensional semiconductors

Dmitry K. Efimkin and Allan H. MacDonald

Phys. Rev. B 95, 035417 (2017) - Published 17 January, 2017

Monolayer two-dimensional transition metal dichalcogenide (TMDCs) exhibit exceptionally strong spin-orbit and electron-electron interaction effects and have provided a rich new playground for the exploration of exciton physics. Recent experiments have demonstrated that in the presence of excess charge carriers the prominent excitonic features in optical absorption split into two separate peaks. The appearance of the additional peak is usually attributed to the presence of trions, charged fermionic quasiparticles formed by binding two electrons to one hole or two holes to one electron. The authors here argue that in the density range for which amplitudes of two peaks are comparable three-particle physics is of importance, and the appropriate picture is one of excitons interacting with the Fermi sea formed by additional charge carriers. These interactions result in the dressing of excitons into exciton-polarons. The exciton spectrum splits into a lower energy attractive exciton-polaron branch, normally identified as a trion branch, and a higher energy repulsive exciton-polaron branch, normally identified as an exciton branch. The authors provide a complete theory of absorption, which incorporates both static and dynamic effects of Fermi sea, and analyze frequency and doping dependence of optical conductivity in detail. The calculated density dependence of peak splitting and their amplitudes and widths are in agreement with recent experiments.

ARTICLES

Electronic structure and strongly correlated systems

Physical properties and crystal structure analysis of double-perovskite NdBaMn2O6 by using single crystals

S. Yamada, H. Sagayama, K. Higuchi, T. Sasaki, K. Sugimoto, and T. Arima

Phys. Rev. B 95, 035101 (2017) - Published 3 January, 2017

Topological Dirac semimetal phase in Pd and Pt oxides

Gang Li, Binghai Yan, Zhijun Wang, and Karsten Held

Phys. Rev. B 95, 035102 (2017) - Published 3 January, 2017

Signatures of an annular Fermi sea

Insun Jo, Yang Liu, L. N. Pfeiffer, K. W. West, K. W. Baldwin, M. Shayegan, and R. Winkler

Phys. Rev. B 95, 035103 (2017) - Published 3 January, 2017

Extremely high Q-factor metamaterials due to anapole excitation

Alexey A. Basharin, Vitaly Chuguevsky, Nikita Volsky, Maria Kafesaki, and Eleftherios N. Economou

Phys. Rev. B 95, 035104 (2017) - Published 3 January, 2017

Accelerated Monte Carlo simulations with restricted Boltzmann machines

Li Huang and Lei Wang

Phys. Rev. B 95, 035105 (2017) - Published 4 January, 2017

Fundamental limits of optical force and torque

A. Rahimzadegan, R. Alaee, I. Fernandez-Corbaton, and C. Rockstuhl

Phys. Rev. B 95, 035106 (2017) - Published 3 January, 2017

Fine structure of the spectra of the Kondo lattice model: Two-site cellular dynamical mean-field theory study

Žiga Osolin and Rok Žitko

Phys. Rev. B 95, 035107 (2017) - Published 3 January, 2017

Spontaneous particle-hole symmetry breaking of correlated fermions on the Lieb lattice

Martin Bercx, Johannes S. Hofmann, Fakher F. Assaad, and Thomas C. Lang

Phys. Rev. B 95, 035108 (2017) - Published 3 January, 2017

Nonuniform sampling schemes of the Brillouin zone for many-electron perturbation-theory calculations in reduced dimensionality

Felipe H. da Jornada, Diana Y. Qiu, and Steven G. Louie

Phys. Rev. B 95, 035109 (2017) - Published 3 January, 2017

NbS3: A unique quasi-one-dimensional conductor with three charge density wave transitions

S. G. Zybtsev, V. Ya. Pokrovskii, V. F. Nasretdinova, S. V. Zaitsev-Zotov, V. V. Pavlovskiy, A. B. Odobesco, Woei Wu Pai, M.-W. Chu, Y. G. Lin, E. Zupanič, H. J. P. van Midden, S. Šturm, E. Tchernychova, A. Prodan, J. C. Bennett, I. R. Mukhamedshin, O. V. Chernysheva, A. P. Menushenkov, V. B. Loginov, B. A. Loginov, A. N. Titov, and M. Abdel-Hafiez

Phys. Rev. B 95, 035110 (2017) - Published 4 January, 2017

Spectrum-splitting approach for Fermi-operator expansion in all-electron Kohn-Sham DFT calculations

Phani Motamarri, Vikram Gavini, Kaushik Bhattacharya, and Michael Ortiz

Phys. Rev. B 95, 035111 (2017) - Published 5 January, 2017

Large-scale all-electron density functional theory calculations using an enriched finite-element basis

Bikash Kanungo and Vikram Gavini

Phys. Rev. B 95, 035112 (2017) - Published 5 January, 2017

Resolving the VO2 controversy: Mott mechanism dominates the insulator-to-metal transition

O. Nájera, M. Civelli, V. Dobrosavljević, and M. J. Rozenberg

Phys. Rev. B 95, 035113 (2017) - Published 9 January, 2017

Impurity screening and stability of Fermi arcs against Coulomb and magnetic scattering in a Weyl monopnictide

Paolo Sessi, Yan Sun, Thomas Bathon, Florian Glott, Zhilin Li, Hongxiang Chen, Liwei Guo, Xiaolong Chen, Marcus Schmidt, Claudia Felser, Binghai Yan, and Matthias Bode

Phys. Rev. B 95, 035114 (2017) - Published 10 January, 2017

Dark mode–Faraday rotation synergy for enhanced magneto-optics

Y. Mazor, M. Meir, and Ben Z. Steinberg

Phys. Rev. B 95, 035115 (2017) - Published 10 January, 2017

Encoding the structure of many-body localization with matrix product operators

David Pekker and Bryan K. Clark

Phys. Rev. B 95, 035116 (2017) - Published 10 January, 2017

Dual coupling effective band model for polarons

Dominic J. J. Marchand, Philip C. E. Stamp, and Mona Berciu

Phys. Rev. B 95, 035117 (2017) - Published 11 January, 2017

Assessment of the Tao-Mo nonempirical semilocal density functional in applications to solids and surfaces

Yuxiang Mo, Roberto Car, Viktor N. Staroverov, Gustavo E. Scuseria, and Jianmin Tao

Phys. Rev. B 95, 035118 (2017) - Published 12 January, 2017

Full counting statistics in the Haldane-Shastry chain

Jean-Marie Stéphan and Frank Pollmann

Phys. Rev. B 95, 035119 (2017) - Published 13 January, 2017

Exact ensemble density functional theory for excited states in a model system: Investigating the weight dependence of the correlation energy

Killian Deur, Laurent Mazouin, and Emmanuel Fromager

Phys. Rev. B 95, 035120 (2017) - Published 13 January, 2017

Strong parameter renormalization from optimum lattice model orbitals

Valentina Brosco, Zu-Jian Ying, and José Lorenzana

Phys. Rev. B 95, 035121 (2017) - Published 13 January, 2017

Functional renormalization group approach for inhomogeneous one-dimensional Fermi systems with finite-ranged interactions

Lukas Weidinger, Florian Bauer, and Jan von Delft

Phys. Rev. B 95, 035122 (2017) - Published 13 January, 2017

Nonperturbative emergence of the Dirac fermion in a strongly correlated composite Fermi liquid

Yibin Yang, Xi Luo, and Yue Yu

Phys. Rev. B 95, 035123 (2017) - Published 17 January, 2017

Quantum critical properties of a metallic spin-density-wave transition

Max H. Gerlach, Yoni Schattner, Erez Berg, and Simon Trebst

Phys. Rev. B 95, 035124 (2017) - Published 17 January, 2017

Excitons in van der Waals materials: From monolayer to bulk hexagonal boron nitride

Jaakko Koskelo, Giorgia Fugallo, Mikko Hakala, Matteo Gatti, Francesco Sottile, and Pierluigi Cudazzo

Phys. Rev. B 95, 035125 (2017) - Published 17 January, 2017

General theory for calculating disorder-averaged Green's function correlators within the coherent potential approximation

Chenyi Zhou and Hong Guo

Phys. Rev. B 95, 035126 (2017) - Published 17 January, 2017

Anisotropic multicarrier transport at the (111) LaAlO3/SrTiO3 interface

S. Davis, V. Chandrasekhar, Z. Huang, K. Han, Ariando, and T. Venkatesan

Phys. Rev. B 95, 035127 (2017) - Published 17 January, 2017

Intertube effects on one-dimensional correlated state of metallic single-wall carbon nanotubes probed by C13 NMR

Noboru Serita, Yusuke Nakai, Kazuyuki Matsuda, Kazuhiro Yanagi, Yasumitsu Miyata, Takeshi Saito, and Yutaka Maniwa

Phys. Rev. B 95, 035128 (2017) - Published 18 January, 2017

Due to the one-dimensional nature of single-wall carbon nanotubes (SWCNTs), electron-electron interactions are of great importance because the lack of screening enhances the effective Coulomb interactions between electrons, and individual SWCNTs have been considered as an ideal realization of a Tomonaga-Luttinger liquid (TLL). In an actual SWCNT sample, SWCNTs usually pack together closely and form a bundle structure, in which intertube effects may alter the TLL state significantly. Here, the authors study the TLL effect in bundles of metallic SWCNTs using 13C nuclear magnetic resonance techniques to understand how the intertube effects alter the electron-electron interaction in the bundle form. They find a modified charge Luttinger parameter for the bundled metallic SWCNTs. Their findings give direct evidence that bundling reduces the effective Coulomb interactions via intertube interactions within bundled metallic SWCNTs.

Generic construction of efficient matrix product operators

C. Hubig, I. P. McCulloch, and U. Schollwöck

Phys. Rev. B 95, 035129 (2017) - Published 18 January, 2017

Entanglement entropy of periodic sublattices

Temple He, Javier M. Magán, and Stefan Vandoren

Phys. Rev. B 95, 035130 (2017) - Published 19 January, 2017

Field theories for gauged symmetry-protected topological phases: Non-Abelian anyons with Abelian gauge group Z23

Huan He, Yunqin Zheng, and Curt von Keyserlingk

Phys. Rev. B 95, 035131 (2017) - Published 19 January, 2017

Many-body localization in the presence of a small bath

Katharine Hyatt, James R. Garrison, Andrew C. Potter, and Bela Bauer

Phys. Rev. B 95, 035132 (2017) - Published 19 January, 2017

In the presence of strong disorder and weak interactions, closed quantum systems can enter a many-body localized phase wherein the system does not conduct heat or charge, does not equilibrate even for arbitrarily long times, and robustly violates quantum statistical mechanics. While this is well established in closed quantum systems, the interplay of such systems with delocalized degrees of freedom is much less understood. Here, the authors consider a model for which, in the noninteracting limit, some degrees of freedom are localized while others remain delocalized. Such a system can be viewed as a model for a many-body localized system brought into contact with a small bath of a comparable number of degrees of freedom. The authors numerically and analytically study the effect of interactions on this system and find that in certain parameter regimes, results are consistent with interaction-induced localization of the entire system.

Spectral evolution with doping of an antiferromagnetic Mott state

Huan-Kuang Wu and Ting-Kuo Lee

Phys. Rev. B 95, 035133 (2017) - Published 20 January, 2017

Shift charge and spin photocurrents in Dirac surface states of topological insulator

Kun Woo Kim, Takahiro Morimoto, and Naoto Nagaosa

Phys. Rev. B 95, 035134 (2017) - Published 23 January, 2017

Two-channel Kondo physics in a Majorana island coupled to a Josephson junction

L. A. Landau and E. Sela

Phys. Rev. B 95, 035135 (2017) - Published 23 January, 2017

Quadratic band touching points and flat bands in two-dimensional topological Floquet systems

Liang Du, Xiaoting Zhou, and Gregory A. Fiete

Phys. Rev. B 95, 035136 (2017) - Published 23 January, 2017

Electrons at the monkey saddle: A multicritical Lifshitz point

A. Shtyk, G. Goldstein, and C. Chamon

Phys. Rev. B 95, 035137 (2017) - Published 23 January, 2017

Electronic properties of a heavy-fermion U(Ru0.92Rh0.08)2Si2 single crystal

K. Prokeš, Y.-K. Huang, M. Reehuis, B. Klemke, J.-U. Hoffmann, A. Sokolowski, A. de Visser, and J. A. Mydosh

Phys. Rev. B 95, 035138 (2017) - Published 23 January, 2017

Fully converged plane-wave-based self-consistent GW calculations of periodic solids

Huawei Cao, Zhongyuan Yu, Pengfei Lu, and Lin-Wang Wang

Phys. Rev. B 95, 035139 (2017) - Published 23 January, 2017

Translational symmetry breaking and the disintegration of the Hofstadter butterfly

Archana Mishra, S. R. Hassan, and R. Shankar

Phys. Rev. B 95, 035140 (2017) - Published 23 January, 2017

Chiral spin liquid and quantum criticality in extended S=12 Heisenberg models on the triangular lattice

Alexander Wietek and Andreas M. Läuchli

Phys. Rev. B 95, 035141 (2017) - Published 24 January, 2017

Nature of the metallization transition in solid hydrogen

Sam Azadi, N. D. Drummond, and W. M. C. Foulkes

Phys. Rev. B 95, 035142 (2017) - Published 24 January, 2017

Capacitance and compressibility of heterostructures with strong electronic correlations

Kevin Steffen, Raymond Frésard, and Thilo Kopp

Phys. Rev. B 95, 035143 (2017) - Published 25 January, 2017

Doping effects on the hybridization gap and antiferromagnetic order in the Kondo semiconductor CeOs2Al10 studied by break-junction experiments

J. Kawabata, T. Ekino, Y. Yamada, Y. Okada, A. Sugimoto, Y. Muro, and T. Takabatake

Phys. Rev. B 95, 035144 (2017) - Published 25 January, 2017

Frustrated spin chain physics near the Majumdar-Ghosh point in szenicsite Cu3(MoO4)(OH)4

Stefan Lebernegg, Oleg Janson, Ioannis Rousochatzakis, Satoshi Nishimoto, Helge Rosner, and Alexander A. Tsirlin

Phys. Rev. B 95, 035145 (2017) - Published 26 January, 2017

Topological phase transition coupled with spin-valley physics in ferroelectric oxide heterostructures

Kunihiko Yamauchi, Paolo Barone, and Silvia Picozzi

Phys. Rev. B 95, 035146 (2017) - Published 26 January, 2017

Small quenches and thermalization

D. M. Kennes, J. C. Pommerening, J. Diekmann, C. Karrasch, and V. Meden

Phys. Rev. B 95, 035147 (2017) - Published 26 January, 2017

Electrical anisotropy and coexistence of structural transitions and superconductivity in IrTe2

Guixin Cao, Weiwei Xie, W. Adam Phelan, J. F. DiTusa, and Rongying Jin

Phys. Rev. B 95, 035148 (2017) - Published 27 January, 2017

Topological electromagnetic responses of bosonic quantum Hall, topological insulator, and chiral semimetal phases in all dimensions

Matthew F. Lapa, Chao-Ming Jian, Peng Ye, and Taylor L. Hughes

Phys. Rev. B 95, 035149 (2017) - Published 27 January, 2017

Few-body collective excitations beyond Kohn's theorem in quantum Hall systems

R. E. Wooten, B. Yan, and Chris H. Greene

Phys. Rev. B 95, 035150 (2017) - Published 27 January, 2017

Type-II Dirac surface states in topological crystalline insulators

Ching-Kai Chiu, Y.-H. Chan, Xiao Li, Y. Nohara, and A. P. Schnyder

Phys. Rev. B 95, 035151 (2017) - Published 30 January, 2017

Topological crystalline insulators are insulating in the bulk, but exhibit conducting surface states protected by crystal symmetries. Here, the authors show that the surface states of crystalline topological insulators come in two different varieties: (i) as standard Dirac cones with pointlike Fermi surfaces (type-I) and (ii) as tilted Dirac cones that appear at the contact of electron and hole pockets. They call these new tilted surface states “type-II Dirac states” in analogy to the three-dimensional type-II Weyl points that have been recently discovered in WTe2. These type-II Dirac states can exist only at the surface of topological crystalline insulators, but are absent in ordinary topological insulators, where they are forbidden by symmetry. The two types of Dirac surface states have very different physical properties, in particular with regards to their thermodynamics and magnetotransport. The authors predict that the antiperovskites A3EO are an example of a crystalline topological insulator that hosts the type-II Dirac surface states.

Electronic structure of self-doped layered Eu3F4Bi2S4 material revealed by x-ray absorption spectroscopy and photoelectron spectromicroscopy

E. Paris, T. Sugimoto, T. Wakita, A. Barinov, K. Terashima, V. Kandyba, O. Proux, J. Kajitani, R. Higashinaka, T. D. Matsuda, Y. Aoki, T. Yokoya, T. Mizokawa, and N. L. Saini

Phys. Rev. B 95, 035152 (2017) - Published 30 January, 2017

P·T·D symmetry-protected scattering anomaly in optics

Mário G. Silveirinha

Phys. Rev. B 95, 035153 (2017) - Published 30 January, 2017

Light waves propagating in optical fibers or other guides are usually vulnerable to defects or channel deformations, such as twisting and bending. These perturbations invariably generate undesired reflections and scattering and typically imply a power penalty. Here, building on an analogy with electronics and with the spin Hall effect, the author unveils a general theoretical solution for this dilemma. It is shown that there is a wide class of three-dimensional metamaterial platforms protected by a particular symmetry – a combination of a geometrical operation with other more subtle symmetries of the materials response – that guarantees bidirectional transport of light totally free of reflections, independent of the specific geometry of the propagation channel and other imperfections. Crucially, this scattering anomaly only requires the symmetry protection in the frequency range of interest, and hence relies on much weaker assumptions than topological theories.

Non-Markovian spin-resolved counting statistics and an anomalous relation between autocorrelations and cross correlations in a three-terminal quantum dot

JunYan Luo, Yiying Yan, Yixiao Huang, Li Yu, Xiao-Ling He, and HuJun Jiao

Phys. Rev. B 95, 035154 (2017) - Published 30 January, 2017

Real-time broadening of nonequilibrium density profiles and the role of the specific initial-state realization

R. Steinigeweg, F. Jin, D. Schmidtke, H. De Raedt, K. Michielsen, and J. Gemmer

Phys. Rev. B 95, 035155 (2017) - Published 31 January, 2017

Measurement and simulation of the polarization-dependent Purcell factor in a microwave fishnet metamaterial

Kaizad Rustomji, Redha Abdeddaim, C. Martijn de Sterke, Boris Kuhlmey, and Stefan Enoch

Phys. Rev. B 95, 035156 (2017) - Published 31 January, 2017

Semiconductors I: bulk

Theoretical investigation on thermoelectric properties of Cu-based chalcopyrite compounds

Biao Wang, Hongjun Xiang, Tsuneyoshi Nakayama, Jun Zhou, and Baowen Li

Phys. Rev. B 95, 035201 (2017) - Published 3 January, 2017

Magnetoexcitons in cuprous oxide

Frank Schweiner, Jörg Main, Günter Wunner, Marcel Freitag, Julian Heckötter, Christoph Uihlein, Marc Aßmann, Dietmar Fröhlich, and Manfred Bayer

Phys. Rev. B 95, 035202 (2017) - Published 3 January, 2017

Frequency-dependent dielectric function of semiconductors with application to physisorption

Fan Zheng, Jianmin Tao, and Andrew M. Rappe

Phys. Rev. B 95, 035203 (2017) - Published 11 January, 2017

Suppressing the spin relaxation of electrons in silicon

Oleg Chalaev, Yang Song, and Hanan Dery

Phys. Rev. B 95, 035204 (2017) - Published 17 January, 2017

Intrinsic coherent acoustic phonons in the indirect band gap semiconductors Si and GaP

Kunie Ishioka, Avinash Rustagi, Ulrich Höfer, Hrvoje Petek, and Christopher J. Stanton

Phys. Rev. B 95, 035205 (2017) - Published 18 January, 2017

Homogeneous versus composite Cd1xyMnxZnySnAs2 crystals: Magnetic interactions and transport properties

L. Kilanski, P. Skupiński, S. Lewińska, E. Dynowska, A. Reszka, K. Grasza, R. Szymczak, A. Ślawska-Waniewska, M. Górska, B. J. Kowalski, and W. Dobrowolski

Phys. Rev. B 95, 035206 (2017) - Published 18 January, 2017

Resonant optical spectroscopy and coherent control of Cr4+ spin ensembles in SiC and GaN

William F. Koehl, Berk Diler, Samuel J. Whiteley, Alexandre Bourassa, N. T. Son, Erik Janzén, and David D. Awschalom

Phys. Rev. B 95, 035207 (2017) - Published 19 January, 2017

The authors identify a new class of optically controllable, semiconductor-based defect spin that is formed from the d-orbital electrons of chromium ions in silicon carbide and gallium nitride. These ions possess a simple lambda optical structure that couples only weakly to phonons and lattice strain. Therefore, even though they probe an ensemble of many ions at once with varying strain environments, the optical transitions they observe are exceptionally narrow and possess a high radiative efficiency. These properties allow the authors to individually interrogate the magnetic sublevels of the ground-state spin using resonant optical excitation, enabling ensemble optical spin polarization as well as optically detected magnetic resonance in the time domain. Each ion species emits the majority of its luminescence within a near-infrared zero-phonon line, suggesting a capacity for efficient photonic integration. Additionally, as magnetically active d-orbital states, the spins of these ions possess a number of degrees of design freedom not available to other common defect spin species such as those based on vacancy complexes. The authors therefore expect that these studies will broaden the range of opportunities available to semiconductor-based quantum device engineering, and will motivate further explorations into the use of transition metal ions as optically active qubit states.

Quantum oscillations in a lead chalcogenide three-dimensional Dirac system

Filip Orbanić, Mario Novak, Mirko Baćani, and Ivan Kokanović

Phys. Rev. B 95, 035208 (2017) - Published 20 January, 2017

The three-dimensional (3D) Dirac materials represent a dimensional extension of the two-dimensional physics seen in graphene. Recently, two types of 3D Dirac materials have been proposed. The first type are the symmetry protected 3D Dirac materials with the Cd3As2 as the representative material. The second type are materials with accidental touching of the conduction and valence bands in a single point. In this paper, the authors are reporting bulk quantum oscillations in Pb1-xSnxSe, a latter type of material, which has also been recently identified as a topological crystalline insulator with a topological phase transition predicted to take place at x=0.17. The authors have used the quantum oscillations in resistivity and magnetization to identify the phase of the oscillation and prove that this material has the 3D Dirac linear dispersion for x=0.17. Combining the oscillations in the resistivity and magnetization, the authors provide the consistent indexing method for drawing the Landau level diagrams that are used in identifying the Berry phase.

Narrow-gap semiconducting properties of KMgBi with multiband feature

Xiao Zhang (张晓), Shanshan Sun (孙珊珊), and Hechang Lei (雷和畅)

Phys. Rev. B 95, 035209 (2017) - Published 23 January, 2017

High-resolution study of the yellow excitons in Cu2O subject to an electric field

J. Heckötter, M. Freitag, D. Fröhlich, M. Aßmann, M. Bayer, M. A. Semina, and M. M. Glazov

Phys. Rev. B 95, 035210 (2017) - Published 25 January, 2017

Low-temperature semiconductor band-gap thermal shifts: T4 shifts from ordinary acoustic and T2 from piezoacoustic coupling

Philip B. Allen and Jean Paul Nery

Phys. Rev. B 95, 035211 (2017) - Published 26 January, 2017

Semiconductors II: surfaces, interfaces, microstructures, and related topics

Effect of intrinsic point defects on ferroelectric polarization behavior of SrTiO3

Konstantin Klyukin and Vitaly Alexandrov

Phys. Rev. B 95, 035301 (2017) - Published 4 January, 2017

Transition from Jaynes-Cummings to Autler-Townes ladder in a quantum dot–microcavity system

Caspar Hopfmann, Alexander Carmele, Anna Musiał, Christian Schneider, Martin Kamp, Sven Höfling, Andreas Knorr, and Stephan Reitzenstein

Phys. Rev. B 95, 035302 (2017) - Published 6 January, 2017

Resonant optical control of the spin of a single Cr atom in a quantum dot

A. Lafuente-Sampietro, H. Utsumi, H. Boukari, S. Kuroda, and L. Besombes

Phys. Rev. B 95, 035303 (2017) - Published 10 January, 2017

A Cr atom in a semiconductor host carries a localized spin with an intrinsic large spin to strain coupling particularly promising for the development of hybrid spin-mechanical systems. The authors demonstrate here that the spin of an individual Cr atom can be controlled optically. To optically access to the spin of an individual atom, they insert it in a cadmium telluride quantum dot. With a single Cr atom introduced in the quantum dot, the energy and polarization of the photon emitted or absorbed by the dot depends on the spin state of the magnetic atom. The authors first show that excitation with a laser beam tuned to the wavelength of one of these optical transitions can be used to initialize the state of the Cr spin and to probe its dynamics optically: the Cr behaves like an optically addressable spin-based memory. Under optical excitation exactly resonant with an absorption transition one can also enter the strong coupling regime where hybrid states of matter and light are created. The spin-dependent strong coupling with the laser field is exploited to optically tune the Cr atom’s energy levels.

Optical investigation of electrical spin injection into an inverted two-dimensional electron gas structure

M. Buchner, T. Kuczmik, M. Oltscher, M. Ciorga, T. Korn, J. Loher, D. Schuh, C. Schüller, D. Bougeard, D. Weiss, and C. H. Back

Phys. Rev. B 95, 035304 (2017) - Published 13 January, 2017

Light-hole exciton in a nanowire quantum dot

Mathieu Jeannin, Alberto Artioli, Pamela Rueda-Fonseca, Edith Bellet-Amalric, Kuntheak Kheng, Régis André, Serge Tatarenko, Joël Cibert, David Ferrand, and Gilles Nogues

Phys. Rev. B 95, 035305 (2017) - Published 17 January, 2017

Quantum dots are promising building blocks for future optoelectronics or quantum information applications. Many of their properties derive from the quantum state of the hole trapped in the dot. “Light” and “heavy” hole states differ by the anisotropic character of their spin and of the electric dipole they form with a trapped electron. Light holes are of particular interest as they offer extended opportunities for optical manipulation of single carriers, or the electrical manipulation of magnetic objects. Here, the authors demonstrate that the hole ground state can be engineered through a proper design of the strain built in the dot when inserted inside a nanowire of a different lattice parameter. Two complementary techniques provide evidence of a light hole state: polarization-resolved Fourier imaging, which is sensitive to the nature of the electron-hole electric dipole, and magneto-optical spectroscopy, which probes the hole spin state through its coupling to magnetic atoms.

Electron spin-flip correlations due to nuclear dynamics in driven GaAs double dots

Arijeet Pal, John M. Nichol, Michael D. Shulman, Shannon P. Harvey, Vladimir Umansky, Emmanuel I. Rashba, Amir Yacoby, and Bertrand I. Halperin

Phys. Rev. B 95, 035306 (2017) - Published 18 January, 2017

Anomalous Fraunhofer interference in epitaxial superconductor-semiconductor Josephson junctions

H. J. Suominen, J. Danon, M. Kjaergaard, K. Flensberg, J. Shabani, C. J. Palmstrøm, F. Nichele, and C. M. Marcus

Phys. Rev. B 95, 035307 (2017) - Published 18 January, 2017

Fraunhofer interference is a paradigmatic phenomena arising due to phase coherence in diverse systems from optics to superconducting junctions. In Josephson junctions, coupling two superconductors through a weak link, such patterns arise in the maximal dissipationless current the system can sustain, oscillating as function of a perpendicular applied magnetic field. By investigating this effect in a recently realized material system epitaxially coupling a thin superconductor to a semiconducting region, the authors here discover novel effects arising due to a combination of magnetic field screening, spin physics, and disorder. In an appropriately aligned in-plane magnetic field, they find that due to screening by the superconducting leads, a flux dipole develops in the semiconducting region leading to an effective confinement of the superconducting states to edges of the intervening semiconducting region. When the out-of-plane field is swept in the presence of an in-plane field, striking asymmetries in the Fraunhofer pattern are observed. By analyzing the underlying theoretical symmetries of the system, they demonstrate that such an effect arises as a result of an intricate interplay between disorder in the junction, splitting of the spin states in the applied field, and coupling between the momentum of the electrons and their spin.

Enhanced circular photogalvanic effect in HgTe quantum wells in the heavily inverted regime

Jun Li, Wen Yang, Jiang-Tao Liu, Wei Huang, Cheng Li, and Song-Yan Chen

Phys. Rev. B 95, 035308 (2017) - Published 25 January, 2017

Atomic force microscope manipulation of Ag atom on the Si(111) surface

Batnyam Enkhtaivan and Atsushi Oshiyama

Phys. Rev. B 95, 035309 (2017) - Published 30 January, 2017

Acousto-optical phonon excitation in cubic piezoelectric slabs and crystal growth orientation effects

Lars Duggen and Morten Willatzen

Phys. Rev. B 95, 035310 (2017) - Published 30 January, 2017

Intrinsic exciton-state mixing and nonlinear optical properties in transition metal dichalcogenide monolayers

M. M. Glazov, L. E. Golub, G. Wang, X. Marie, T. Amand, and B. Urbaszek

Phys. Rev. B 95, 035311 (2017) - Published 30 January, 2017

Photon echoes from (In,Ga)As quantum dots embedded in a Tamm-plasmon microcavity

M. Salewski, S. V. Poltavtsev, Yu. V. Kapitonov, J. Vondran, D. R. Yakovlev, C. Schneider, M. Kamp, S. Höfling, R. Oulton, I. A. Akimov, A. V. Kavokin, and M. Bayer

Phys. Rev. B 95, 035312 (2017) - Published 30 January, 2017

Tamm resonators are an alternate type of cavities, in which the light-matter interaction may be significantly enhanced, as required for many applications in photonics or optoelectronics. A Tamm resonator comprises at least one metal layer as mirror, in the present case combined with a distributed Bragg reflector. The metal layer may turn out to be useful, for example, for injecting carriers or applying an electric field. Here, the authors use photon echoes in the exciton four-wave mixing signal to demonstrate that the studied Tamm resonator, which contains quantum dots as the optically active medium, allows one to perform coherent manipulations on quantum-dot excitons at power levels more than one order of magnitude lower than those required for bare quantum dots. This occurs despite the moderate quality factor of about 100. Moreover, it speeds up the radiative decay of the excitons by a factor of two (the so-called “Purcell effect”). On the other hand, the coherence of the quantum dot exciton, which may become compromised by plasmon excitations in the metal, is hardly shortened. These results demonstrate that Tamm resonators are indeed prospective candidates for performing coherent optical manipulations.

Theoretical investigation of phonon polaritons in SiC micropillar resonators

Christopher R. Gubbin, Stefan A. Maier, and Simone De Liberato

Phys. Rev. B 95, 035313 (2017) - Published 30 January, 2017

Surface physics, nanoscale physics, low-dimensional systems

Hybrid surface waves in two-dimensional Rashba-Dresselhaus materials

Dmitry Yudin, Dmitry R. Gulevich, and Ivan A. Shelykh

Phys. Rev. B 95, 035401 (2017) - Published 3 January, 2017

Copper adatoms on graphene: Theory of orbital and spin-orbital effects

Tobias Frank, Susanne Irmer, Martin Gmitra, Denis Kochan, and Jaroslav Fabian

Phys. Rev. B 95, 035402 (2017) - Published 4 January, 2017

Intraband memory function and memory-function conductivity formula in doped graphene

I. Kupčić

Phys. Rev. B 95, 035403 (2017) - Published 4 January, 2017

Influence of phonons on solid-state cavity-QED investigated using nonequilibrium Green's functions

Gaston Hornecker, Alexia Auffèves, and Thomas Grange

Phys. Rev. B 95, 035404 (2017) - Published 5 January, 2017

High-order harmonic generation from gapped graphene: Perturbative response and transition to nonperturbative regime

Darko Dimitrovski, Lars Bojer Madsen, and Thomas Garm Pedersen

Phys. Rev. B 95, 035405 (2017) - Published 9 January, 2017

High and low thermal conductivity of amorphous macromolecules

Xu Xie, Kexin Yang, Dongyao Li, Tsung-Han Tsai, Jungwoo Shin, Paul V. Braun, and David G. Cahill

Phys. Rev. B 95, 035406 (2017) - Published 9 January, 2017

Optical absorbance and band-gap engineering of (BN)1x(C2)x two-dimensional alloys: Phase separation and composition fluctuation effects

I. Guilhon, M. Marques, L. K. Teles, and F. Bechstedt

Phys. Rev. B 95, 035407 (2017) - Published 10 January, 2017

Spin blockade and coherent dynamics of high-spin states in a three-electron double quantum dot

Bao-Bao Chen, Bao-Chuan Wang, Gang Cao, Hai-Ou Li, Ming Xiao, Guang-Can Guo, Hong-Wen Jiang, Xuedong Hu, and Guo-Ping Guo

Phys. Rev. B 95, 035408 (2017) - Published 10 January, 2017

Full counting statistics of phonon-assisted Andreev tunneling through a quantum dot coupled to normal and superconducting leads

Bing Dong, G. H. Ding, and X. L. Lei

Phys. Rev. B 95, 035409 (2017) - Published 10 January, 2017

Sensitivity of mixing-current technique to detect nanomechanical motion

Yue Wang and Fabio Pistolesi

Phys. Rev. B 95, 035410 (2017) - Published 10 January, 2017

Effects of anisotropy and Coulomb interactions on quantum transport in a quadruple quantum-dot structure

M. Yu. Kagan, V. V. Val'kov, and S. V. Aksenov

Phys. Rev. B 95, 035411 (2017) - Published 11 January, 2017

Photon-assisted transport in bilayer graphene flakes

D. Zambrano, L. Rosales, A. Latgé, M. Pacheco, and P. A. Orellana

Phys. Rev. B 95, 035412 (2017) - Published 11 January, 2017

Transport gap engineering by contact geometry in graphene nanoribbons: Experimental and theoretical studies on artificial materials

Thomas Stegmann, John A. Franco-Villafañe, Ulrich Kuhl, Fabrice Mortessagne, and Thomas H. Seligman

Phys. Rev. B 95, 035413 (2017) - Published 12 January, 2017

Frequency-dependent magneto-optical conductivity in the generalized αT3 model

Áron Dániel Kovács, Gyula Dávid, Balázs Dóra, and József Cserti

Phys. Rev. B 95, 035414 (2017) - Published 12 January, 2017

Conductance fluctuations and disorder induced ν=0 quantum Hall plateau in topological insulator nanowires

Emmanouil Xypakis and Jens H. Bardarson

Phys. Rev. B 95, 035415 (2017) - Published 13 January, 2017

Theory of plasmonic effects in nonlinear optics: The case of graphene

Habib Rostami, Mikhail I. Katsnelson, and Marco Polini

Phys. Rev. B 95, 035416 (2017) - Published 17 January, 2017

Many-body theory of trion absorption features in two-dimensional semiconductors

Dmitry K. Efimkin and Allan H. MacDonald

Phys. Rev. B 95, 035417 (2017) - Published 17 January, 2017

Monolayer two-dimensional transition metal dichalcogenide (TMDCs) exhibit exceptionally strong spin-orbit and electron-electron interaction effects and have provided a rich new playground for the exploration of exciton physics. Recent experiments have demonstrated that in the presence of excess charge carriers the prominent excitonic features in optical absorption split into two separate peaks. The appearance of the additional peak is usually attributed to the presence of trions, charged fermionic quasiparticles formed by binding two electrons to one hole or two holes to one electron. The authors here argue that in the density range for which amplitudes of two peaks are comparable three-particle physics is of importance, and the appropriate picture is one of excitons interacting with the Fermi sea formed by additional charge carriers. These interactions result in the dressing of excitons into exciton-polarons. The exciton spectrum splits into a lower energy attractive exciton-polaron branch, normally identified as a trion branch, and a higher energy repulsive exciton-polaron branch, normally identified as an exciton branch. The authors provide a complete theory of absorption, which incorporates both static and dynamic effects of Fermi sea, and analyze frequency and doping dependence of optical conductivity in detail. The calculated density dependence of peak splitting and their amplitudes and widths are in agreement with recent experiments.

Plasmonic shock waves and solitons in a nanoring

K. L. Koshelev, V. Yu. Kachorovskii, M. Titov, and M. S. Shur

Phys. Rev. B 95, 035418 (2017) - Published 18 January, 2017

Poisson-like height distribution of Ag nanoislands on Si(111) 7×7

Yiyao Chen, M. W. Gramlich, S. T. Hayden, and P. F. Miceli

Phys. Rev. B 95, 035419 (2017) - Published 20 January, 2017

Electrical transport in nanothick ZrTe5 sheets: From three to two dimensions

Jingjing Niu, Jingyue Wang, Zhijie He, Chenglong Zhang, Xinqi Li, Tuocheng Cai, Xiumei Ma, Shuang Jia, Dapeng Yu, and Xiaosong Wu

Phys. Rev. B 95, 035420 (2017) - Published 23 January, 2017

Bulk-boundary correspondence from the intercellular Zak phase

Jun-Won Rhim, Jan Behrends, and Jens H. Bardarson

Phys. Rev. B 95, 035421 (2017) - Published 23 January, 2017

Spin-orbit torque in two-dimensional antiferromagnetic topological insulators

S. Ghosh and A. Manchon

Phys. Rev. B 95, 035422 (2017) - Published 23 January, 2017

Energy transfer in strained graphene assisted by discrete breathers excited by external ac driving

Iman Evazzade, Ivan P. Lobzenko, Elena A. Korznikova, Ilya A. Ovid'ko, Mahmood Rezaee Roknabadi, and Sergey V. Dmitriev

Phys. Rev. B 95, 035423 (2017) - Published 24 January, 2017

Kinetics of copper growth on graphene revealed by time-resolved small-angle x-ray scattering

M. Hodas, P. Siffalovic, M. Jergel, M. Pelletta, Y. Halahovets, K. Vegso, M. Kotlar, and E. Majkova

Phys. Rev. B 95, 035424 (2017) - Published 24 January, 2017

Optical properties of dielectric plates coated with gapped graphene

G. L. Klimchitskaya and V. M. Mostepanenko

Phys. Rev. B 95, 035425 (2017) - Published 25 January, 2017

Role of band-index-dependent transport relaxation times in anomalous Hall effect

Cong Xiao, Dingping Li, and Zhongshui Ma

Phys. Rev. B 95, 035426 (2017) - Published 25 January, 2017

Transformation optics for surface phenomena: Engineering the Goos-Hänchen effect

Lieve Lambrechts, Vincent Ginis, Jan Danckaert, and Philippe Tassin

Phys. Rev. B 95, 035427 (2017) - Published 26 January, 2017

Finite coupling effects in double quantum dots near equilibrium

Xiansong Xu, Juzar Thingna, and Jian-Sheng Wang

Phys. Rev. B 95, 035428 (2017) - Published 26 January, 2017

Electronic transport in disordered MoS2 nanoribbons

Emilia Ridolfi, Leandro R. F. Lima, Eduardo R. Mucciolo, and Caio H. Lewenkopf

Phys. Rev. B 95, 035430 (2017) - Published 30 January, 2017

Coulomb-blockade and Pauli-blockade magnetometry

Gábor Széchenyi and András Pályi

Phys. Rev. B 95, 035431 (2017) - Published 30 January, 2017

Harmonic model of corrugations of incommensurate two-dimensional layers

Konrad Thürmer and Catalin D. Spataru

Phys. Rev. B 95, 035432 (2017) - Published 30 January, 2017

ERRATA

Erratum: Analytic model of the energy spectrum of a graphene quantum dot in a perpendicular magnetic field [Phys. Rev. B 78, 195427 (2008)]

S. Schnez, Klaus Ensslin, M. Sigrist, and T. Ihn

Phys. Rev. B 95, 039901 (2017) - Published 10 January, 2017

Erratum: Rashba scattering in the low-energy limit [Phys. Rev. B 93, 245309 (2016)]

Joel Hutchinson and Joseph Maciejko

Phys. Rev. B 95, 039902 (2017) - Published 11 January, 2017

Publisher's Note: Interpenetrating graphene networks: Three-dimensional node-line semimetals with massive negative linear compressibilities [Phys. Rev. B 94, 245422 (2016)]

Yangzheng Lin, Zhisheng Zhao, Timothy A. Strobel, and R. E. Cohen

Phys. Rev. B 95, 039903 (2017) - Published 17 January, 2017

Erratum: Quantum heat engines based on electronic Mach-Zehnder interferometers [Phys. Rev. B 91, 195406 (2015)]

Patrick P. Hofer and Björn Sothmann

Phys. Rev. B 95, 039904 (2017) - Published 30 January, 2017

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