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HIGHLIGHTED ARTICLES

Observation of large topologically trivial Fermi arcs in the candidate type-II Weyl semimetal WTe2

F. Y. Bruno, A. Tamai, Q. S. Wu, I. Cucchi, C. Barreteau, A. de la Torre, S. McKeown Walker, S. Riccò, Z. Wang, T. K. Kim, M. Hoesch, M. Shi, N. C. Plumb, E. Giannini, A. A. Soluyanov, and F. Baumberger

Phys. Rev. B 94, 121112(R) (2016) - Published 14 September, 2016

The authors present here several advances towards a comprehensive understanding of WTe2. Using microfocus laser ARPES, they resolve for the first time the distinct electronic structure of both inequivalent top and bottom (001) surfaces of WTe2. Moreover, they demonstrate for the first time the presence of large surface state Fermi arcs on both surfaces. Using surface electronic structure calculations, they further demonstrate that these Fermi arcs are topologically trivial and that their existence is independent of the presence of type-II Weyl points in the bulk band structure. Contrary to common belief, the observation of surface state Fermi arcs is thus not suitable to robustly identify a type-II Weyl semimetal. Finally, the authors use the observation of Fermi arcs and distinct top and bottom surfaces to clarify the controversial bulk electronic structure of WTe2. They show that the bulk Fermi surface is formed by three-dimensional electron and hole pockets with areas that are found to be in good agreement with transport experiments, with the exception of small hole pockets that have not been observed in quantum oscillation experiments.

Observation of Fermi arcs in the type-II Weyl semimetal candidate WTe2

Yun Wu, Daixiang Mou, Na Hyun Jo, Kewei Sun, Lunan Huang, S. L. Bud'ko, P. C. Canfield, and Adam Kaminski

Phys. Rev. B 94, 121113(R) (2016) - Published 14 September, 2016

In recently predicted type-II Weyl semimetals, the Weyl states connect hole and electron bands that would otherwise be separated by an indirect gap. The set of points in the momentum space at which both bands touch are called Weyl points and are connected by Fermi arcs at the surface of the sample. Experimental evidence confirmed existence of these exotic fermions in MoTe2 and MoxW1-xTe2. Here, the authors show that such states also exist in pure WTe2 and are very sensitive to strain. While flat undistorted portions of the sample show well defined Fermi arcs – a clear signature of Weyl fermions – strain due to bulking of the surface in other locations suppresses this state and destroys the Weyl state. Such high sensitivity to strain provides a simple way to tune properties of Weyl Fermions and explore the physics of these unusual objects.

Observation of Dirac surface states in the noncentrosymmetric superconductor BiPd

H. M. Benia, E. Rampi, C. Trainer, C. M. Yim, A. Maldonado, D. C. Peets, A. Stöhr, U. Starke, K. Kern, A. Yaresko, G. Levy, A. Damascelli, C. R. Ast, A. P. Schnyder, and P. Wahl

Phys. Rev. B 94, 121407(R) (2016) - Published 22 September, 2016

Materials with strong spin-orbit coupling often host a unique electronic structure, both in the bulk and on the surface. In particular, in systems that break inversion symmetry, spin-orbit coupling facilitates the Rashba-Dresselhaus effect, leading to a lifting of spin degeneracy in the bulk and intricate spin textures of the Bloch wave functions. Such materials could see potential applications in spintronics and quantum information technology, but these applications would benefit from a broader suite of materials, with a greater range of properties, and in particularly from very strong spin-orbit splitting. This paper’s angular-resolved photoemission and low-temperature scanning tunneling microscopy experiments, together with relativistic first-principles band structure calculations, identify several Dirac surface states in BiPd, one of which exhibits an extremely large spin splitting. Unlike the surface states in inversion-symmetric systems, the Dirac surface states of BiPd have completely different properties at opposite faces of the crystal and are not trivially linked by symmetry. The spin splitting of the surface states exhibits a strong anisotropy by itself, which can be linked to the low in-plane symmetry of the surface termination. Both may be useful to implement new functionalities for spintronic applications.

Entanglement entropy of U(1) quantum spin liquids

Michael Pretko and T. Senthil

Phys. Rev. B 94, 125112 (2016) - Published 8 September, 2016

Entanglement entropy is a powerful tool for characterizing spin liquids and other systems with long-range entanglement. For gapped spin liquids, this problem has been well-studied, finding a universal subleading constant term in the entanglement entropy, known as the topological entanglement entropy. In this paper, the idea of topological entanglement entropy is generalized to the gapless U(1) spin liquid. First, it is shown that the entanglement entropy separates into two pieces, one due to emergent charges of the theory (assumed to be gapped) and one due to the emergent gapless gauge mode. Both give universal subheading contributions to the entanglement entropy, which are logarithmic in the size of the region considered. The photon contribution is due to the local physics of the gapless mode. The particle contribution, on the other hand, is a topological term, generalizing the notion of topological entanglement entropy. A construction is presented which can isolate this topological piece by eliminating the photon contribution and other local terms, such as the area law. This topological term in the entanglement entropy can serve as a powerful diagnostic tool for U(1) spin liquids.

Section Chern number for a three-dimensional photonic crystal and the bulk-edge correspondence

Shuhei Oono, Toshikaze Kariyado, and Yasuhiro Hatsugai

Phys. Rev. B 94, 125125 (2016) - Published 14 September, 2016

Slicing the 3D Brillouin zone into 2D as a dimensional reduction makes the topological structure of the 3D Weyl point clear as a topological critical point. The Chern number of the sliced 2D system (section Chern number) changes discontinuously at the gap-closing momentum that guarantees topological stability of the Weyl point. This section Chern number is just a mathematical tool and cannot be directly measured experimentally. However, propagating edge modes of the 3D system with boundaries are necessarily momentum selective, associated with the section Chern number. This is a direct consequence of the bulk-edge correspondence. Using a localized basis with/without boundaries, the authors have demonstrated this here in a 3D helical photonic crystal without inversion symmetry

Automated construction of maximally localized Wannier functions for bands with nontrivial topology

Jamal I. Mustafa, Sinisa Coh, Marvin L. Cohen, and Steven G. Louie

Phys. Rev. B 94, 125151 (2016) - Published 30 September, 2016

Wannier functions provide a useful description of the electronic states in a crystal, providing a chemical picture for the bonding structure of a material, in addition to applications in computational materials science. Topological insulators are an interesting class of materials with spin-polarized conducting surface states alongside an insulating bulk. To date, constructing Wannier functions for topological insulators has proven difficult, relying on an educated guess for the trial orbitals or requiring the system to be parameterized in order to tune between the normal and topological phase. The authors have developed an automated approach within the optimized projection functions method for constructing localized Wannier functions for topologically nontrivial bands. They demonstrate the method on a two-dimensional tight-binding model, a strong three-dimensional topological insulator, and finally, the prototypical topological insulating material Bi2Se3. They find that the Wannier functions contain large imaginary components and are more extended than those in the topologically trivial phase.

Spin and the Coulomb gap in the half-filled lowest Landau level

J. P. Eisenstein, T. Khaire, D. Nandi, A. D. K. Finck, L. N. Pfeiffer, and K. W. West

Phys. Rev. B 94, 125409 (2016) - Published 8 September, 2016

In a strong magnetic field, two-dimensional electron systems are dominated by Coulomb interactions between the electrons. While the most familiar manifestation of these interactions is the fractional quantum Hall effect, this is actually a relatively subtle variation in the strong electronic correlations that exist throughout the high-field regime. This is clearly revealed in tunneling experiments in which an uncorrelated electron is rapidly thrust into a strongly correlated electron gas. A robust Coulomb pseudogap is observed, with tunneling strongly suppressed until the energy of the incoming electron is large enough. The Coulomb gap is insensitive to the precise magnetic field and is typically much larger than the energy gap associated with the fractional quantum Hall effect. In the present paper, the authors demonstrate that the size of the Coulomb gap observed in tunneling between two parallel two-dimensional electron systems depends sensitively on their spin configuration, with larger gaps associated with a larger net spin polarization. In effect, it is easier for electrons ‘to get out of the way’ of an incoming tunneling electron when the spin polarization of the electron gas is less than complete.

RAPID COMMUNICATIONS

Electronic structure and strongly correlated systems

Hall effect within the colossal magnetoresistive semimetallic state of MoTe2

Qiong Zhou, D. Rhodes, Q. R. Zhang, S. Tang, R. Schönemann, and L. Balicas

Phys. Rev. B 94, 121101(R) (2016) - Published 1 September, 2016

Many-body breakdown of indirect gap in topological Kondo insulators

Marcin M. Wysokiński and Michele Fabrizio

Phys. Rev. B 94, 121102(R) (2016) - Published 1 September, 2016

Forbidden phonon: Dynamical signature of bond symmetry breaking in the iron chalcogenides

David M. Fobes, Igor A. Zaliznyak, John M. Tranquada, Zhijun Xu, Genda Gu, Xu-Gang He, Wei Ku, Yang Zhao, Masaaki Matsuda, V. Ovidiu Garlea, and Barry Winn

Phys. Rev. B 94, 121103(R) (2016) - Published 1 September, 2016

Evolution of electronic correlations across the rutile, perovskite, and Ruddelsden-Popper iridates with octahedral connectivity

Jason K. Kawasaki, Masaki Uchida, Hanjong Paik, Darrell G. Schlom, and Kyle M. Shen

Phys. Rev. B 94, 121104(R) (2016) - Published 6 September, 2016

Hybrid Weyl semimetal

Fei-Ye Li, Xi Luo, Xi Dai, Yue Yu, Fan Zhang, and Gang Chen

Phys. Rev. B 94, 121105(R) (2016) - Published 6 September, 2016

Type-II Weyl cone transitions in driven semimetals

Ching-Kit Chan, Yun-Tak Oh, Jung Hoon Han, and Patrick A. Lee

Phys. Rev. B 94, 121106(R) (2016) - Published 7 September, 2016

Uncovering the hidden quantum critical point in disordered massless Dirac and Weyl semimetals

J. H. Pixley, David A. Huse, and S. Das Sarma

Phys. Rev. B 94, 121107(R) (2016) - Published 8 September, 2016

Dirac-node arc in the topological line-node semimetal HfSiS

D. Takane, Zhiwei Wang, S. Souma, K. Nakayama, C. X. Trang, T. Sato, T. Takahashi, and Yoichi Ando

Phys. Rev. B 94, 121108(R) (2016) - Published 8 September, 2016

Directional Fano resonances in light scattering by a high refractive index dielectric sphere

Michael I. Tribelsky, Jean-Michel Geffrin, Amelie Litman, Christelle Eyraud, and Fernando Moreno

Phys. Rev. B 94, 121110(R) (2016) - Published 12 September, 2016

Symmetry fractionalization in the topological phase of the spin-12 J1−J2 triangular Heisenberg model

S. N. Saadatmand and I. P. McCulloch

Phys. Rev. B 94, 121111(R) (2016) - Published 13 September, 2016

Observation of large topologically trivial Fermi arcs in the candidate type-II Weyl semimetal WTe2

F. Y. Bruno, A. Tamai, Q. S. Wu, I. Cucchi, C. Barreteau, A. de la Torre, S. McKeown Walker, S. Riccò, Z. Wang, T. K. Kim, M. Hoesch, M. Shi, N. C. Plumb, E. Giannini, A. A. Soluyanov, and F. Baumberger

Phys. Rev. B 94, 121112(R) (2016) - Published 14 September, 2016

The authors present here several advances towards a comprehensive understanding of WTe2. Using microfocus laser ARPES, they resolve for the first time the distinct electronic structure of both inequivalent top and bottom (001) surfaces of WTe2. Moreover, they demonstrate for the first time the presence of large surface state Fermi arcs on both surfaces. Using surface electronic structure calculations, they further demonstrate that these Fermi arcs are topologically trivial and that their existence is independent of the presence of type-II Weyl points in the bulk band structure. Contrary to common belief, the observation of surface state Fermi arcs is thus not suitable to robustly identify a type-II Weyl semimetal. Finally, the authors use the observation of Fermi arcs and distinct top and bottom surfaces to clarify the controversial bulk electronic structure of WTe2. They show that the bulk Fermi surface is formed by three-dimensional electron and hole pockets with areas that are found to be in good agreement with transport experiments, with the exception of small hole pockets that have not been observed in quantum oscillation experiments.

Observation of Fermi arcs in the type-II Weyl semimetal candidate WTe2

Yun Wu, Daixiang Mou, Na Hyun Jo, Kewei Sun, Lunan Huang, S. L. Bud'ko, P. C. Canfield, and Adam Kaminski

Phys. Rev. B 94, 121113(R) (2016) - Published 14 September, 2016

In recently predicted type-II Weyl semimetals, the Weyl states connect hole and electron bands that would otherwise be separated by an indirect gap. The set of points in the momentum space at which both bands touch are called Weyl points and are connected by Fermi arcs at the surface of the sample. Experimental evidence confirmed existence of these exotic fermions in MoTe2 and MoxW1-xTe2. Here, the authors show that such states also exist in pure WTe2 and are very sensitive to strain. While flat undistorted portions of the sample show well defined Fermi arcs – a clear signature of Weyl fermions – strain due to bulking of the surface in other locations suppresses this state and destroys the Weyl state. Such high sensitivity to strain provides a simple way to tune properties of Weyl Fermions and explore the physics of these unusual objects.

Role of Berry phase theory for describing orbital magnetism: From magnetic heterostructures to topological orbital ferromagnets

J.-P. Hanke, F. Freimuth, A. K. Nandy, H. Zhang, S. Blügel, and Y. Mokrousov

Phys. Rev. B 94, 121114(R) (2016) - Published 15 September, 2016

Resistivity plateau and negative magnetoresistance in the topological semimetal TaSb2

Yuke Li, Lin Li, Jialu Wang, Tingting Wang, Xiaofeng Xu, Chuanying Xi, Chao Cao, and Jianhui Dai

Phys. Rev. B 94, 121115(R) (2016) - Published 19 September, 2016

GWΓ+ Bethe-Salpeter equation approach for photoabsorption spectra: Importance of self-consistent GWΓ calculations in small atomic systems

Riichi Kuwahara, Yoshifumi Noguchi, and Kaoru Ohno

Phys. Rev. B 94, 121116(R) (2016) - Published 21 September, 2016

Type-II Dirac fermions in the PtSe2 class of transition metal dichalcogenides

Huaqing Huang, Shuyun Zhou, and Wenhui Duan

Phys. Rev. B 94, 121117(R) (2016) - Published 27 September, 2016

Topological edge states in correlated honeycomb materials with strong spin-orbit coupling

Andrei Catuneanu, Heung-Sik Kim, Oguzhan Can, and Hae-Young Kee

Phys. Rev. B 94, 121118(R) (2016) - Published 30 September, 2016

Semiconductors I: bulk

Magnetophonon oscillations caused by acoustic phonons in bulk conductors

O. E. Raichev

Phys. Rev. B 94, 121201(R) (2016) - Published 6 September, 2016

NV centers in 3C,4H, and 6H silicon carbide: A variable platform for solid-state qubits and nanosensors

H. J. von Bardeleben, J. L. Cantin, A. Csóré, A. Gali, E. Rauls, and U. Gerstmann

Phys. Rev. B 94, 121202(R) (2016) - Published 26 September, 2016

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

Mapping the effect of defect-induced strain disorder on the Dirac states of topological insulators

Oliver Storz, Alberto Cortijo, Stefan Wilfert, K. A. Kokh, O. E. Tereshchenko, María A. H. Vozmediano, Matthias Bode, Francisco Guinea, and Paolo Sessi

Phys. Rev. B 94, 121301(R) (2016) - Published 7 September, 2016

Hyperfine coupling of hole and nuclear spins in symmetric (111)-grown GaAs quantum dots

M. Vidal, M. V. Durnev, L. Bouet, T. Amand, M. M. Glazov, E. L. Ivchenko, P. Zhou, G. Wang, T. Mano, T. Kuroda, X. Marie, K. Sakoda, and B. Urbaszek

Phys. Rev. B 94, 121302(R) (2016) - Published 9 September, 2016

Sharp peaks in the conductance of a double quantum dot and a quantum-dot spin valve at high temperatures: A hierarchical quantum master equation approach

S. Wenderoth, J. Bätge, and R. Härtle

Phys. Rev. B 94, 121303(R) (2016) - Published 26 September, 2016

Conductance measurement of spin-orbit coupling in two-dimensional electron systems with an in-plane magnetic field

K. Kolasiński, H. Sellier, and B. Szafran

Phys. Rev. B 94, 121304(R) (2016) - Published 27 September, 2016

Giant photon gain in large-scale quantum dot-circuit QED systems

Bijay Kumar Agarwalla, Manas Kulkarni, Shaul Mukamel, and Dvira Segal

Phys. Rev. B 94, 121305(R) (2016) - Published 30 September, 2016

Surface physics, nanoscale physics, low-dimensional systems

Quantum transport in the surface states of epitaxial Bi(111) thin films

Kai Zhu, Lin Wu, Xinxin Gong, Shunhao Xiao, and Xiaofeng Jin

Phys. Rev. B 94, 121401(R) (2016) - Published 6 September, 2016

Efficiency bounds on thermoelectric transport in magnetic fields: The role of inelastic processes

Kaoru Yamamoto, Ora Entin-Wohlman, Amnon Aharony, and Naomichi Hatano

Phys. Rev. B 94, 121402(R) (2016) - Published 8 September, 2016

Control of recoil losses in nanomechanical SiN membrane resonators

A. Borrielli, L. Marconi, F. Marin, F. Marino, B. Morana, G. Pandraud, A. Pontin, G. A. Prodi, P. M. Sarro, E. Serra, and M. Bonaldi

Phys. Rev. B 94, 121403(R) (2016) - Published 8 September, 2016

Directional-dependent thickness and bending rigidity of phosphorene

Deepti Verma, Ben Hourahine, Thomas Frauenheim, Richard D. James, and Traian Dumitrică

Phys. Rev. B 94, 121404(R) (2016) - Published 13 September, 2016

Efficient single photon emission from a high-purity hexagonal boron nitride crystal

L. J. Martínez, T. Pelini, V. Waselowski, J. R. Maze, B. Gil, G. Cassabois, and V. Jacques

Phys. Rev. B 94, 121405(R) (2016) - Published 22 September, 2016

Robustness of the universal optical transmittance in monolayer and multilayer graphene flakes under Coulomb interactions

Premlata Yadav, Pawan Kumar Srivastava, Nirat Ray, and Subhasis Ghosh

Phys. Rev. B 94, 121406(R) (2016) - Published 22 September, 2016

Observation of Dirac surface states in the noncentrosymmetric superconductor BiPd

H. M. Benia, E. Rampi, C. Trainer, C. M. Yim, A. Maldonado, D. C. Peets, A. Stöhr, U. Starke, K. Kern, A. Yaresko, G. Levy, A. Damascelli, C. R. Ast, A. P. Schnyder, and P. Wahl

Phys. Rev. B 94, 121407(R) (2016) - Published 22 September, 2016

Materials with strong spin-orbit coupling often host a unique electronic structure, both in the bulk and on the surface. In particular, in systems that break inversion symmetry, spin-orbit coupling facilitates the Rashba-Dresselhaus effect, leading to a lifting of spin degeneracy in the bulk and intricate spin textures of the Bloch wave functions. Such materials could see potential applications in spintronics and quantum information technology, but these applications would benefit from a broader suite of materials, with a greater range of properties, and in particularly from very strong spin-orbit splitting. This paper’s angular-resolved photoemission and low-temperature scanning tunneling microscopy experiments, together with relativistic first-principles band structure calculations, identify several Dirac surface states in BiPd, one of which exhibits an extremely large spin splitting. Unlike the surface states in inversion-symmetric systems, the Dirac surface states of BiPd have completely different properties at opposite faces of the crystal and are not trivially linked by symmetry. The spin splitting of the surface states exhibits a strong anisotropy by itself, which can be linked to the low in-plane symmetry of the surface termination. Both may be useful to implement new functionalities for spintronic applications.

Nonlocal topological valley transport at large valley Hall angles

Michael Beconcini, Fabio Taddei, and Marco Polini

Phys. Rev. B 94, 121408(R) (2016) - Published 22 September, 2016

Quantum Hall edge states in topological insulator nanoribbons

A. Pertsova, C. M. Canali, and A. H. MacDonald

Phys. Rev. B 94, 121409(R) (2016) - Published 26 September, 2016

Strongly coupled near-field radiative and conductive heat transfer between planar bodies

Riccardo Messina, Weiliang Jin, and Alejandro W. Rodriguez

Phys. Rev. B 94, 121410(R) (2016) - Published 26 September, 2016

Plasmon-drag-assisted terahertz generation in a graphene layer incorporating an asymmetric plasmon nanostructure

S. Mohsen Raeis-Zadeh, Behrooz Semnani, and Safieddin Safavi-Naeini

Phys. Rev. B 94, 121411(R) (2016) - Published 28 September, 2016

ARTICLES

Electronic structure and strongly correlated systems

Periodically driven three-level systems

M. B. Kenmoe and L. C. Fai

Phys. Rev. B 94, 125101 (2016) - Published 1 September, 2016

Dynamical gap generation in graphene with frequency-dependent renormalization effects

M. E. Carrington, C. S. Fischer, L. von Smekal, and M. H. Thoma

Phys. Rev. B 94, 125102 (2016) - Published 2 September, 2016

Parafermionic phases with symmetry breaking and topological order

A. Alexandradinata, N. Regnault, Chen Fang, Matthew J. Gilbert, and B. Andrei Bernevig

Phys. Rev. B 94, 125103 (2016) - Published 2 September, 2016

Thermalization of topological entropy after a quantum quench

Yu Zeng, Alioscia Hamma, and Heng Fan

Phys. Rev. B 94, 125104 (2016) - Published 2 September, 2016

Abelian Floquet symmetry-protected topological phases in one dimension

Rahul Roy and Fenner Harper

Phys. Rev. B 94, 125105 (2016) - Published 2 September, 2016

Dynamical mean-field theory for flat-band ferromagnetism

Hong-Son Nguyen and Minh-Tien Tran

Phys. Rev. B 94, 125106 (2016) - Published 6 September, 2016

Holographic duality between (2+1)-dimensional quantum anomalous Hall state and (3+1)-dimensional topological insulators

Yingfei Gu, Ching Hua Lee, Xueda Wen, Gil Young Cho, Shinsei Ryu, and Xiao-Liang Qi

Phys. Rev. B 94, 125107 (2016) - Published 6 September, 2016

Phase transitions in ensembles of solitons induced by an optical pumping or a strong electric field

P. Karpov and S. Brazovskii

Phys. Rev. B 94, 125108 (2016) - Published 6 September, 2016

Linked-cluster expansions for quantum magnets on the hypercubic lattice

Kris Coester, Darshan G. Joshi, Matthias Vojta, and Kai Phillip Schmidt

Phys. Rev. B 94, 125109 (2016) - Published 6 September, 2016

Quantum criticality in the ferromagnetic superconductor UCoGe under pressure and magnetic field

Gaël Bastien, Daniel Braithwaite, Dai Aoki, Georg Knebel, and Jacques Flouquet

Phys. Rev. B 94, 125110 (2016) - Published 7 September, 2016

Adiabatic continuity, wave-function overlap, and topological phase transitions

Jiahua Gu and Kai Sun

Phys. Rev. B 94, 125111 (2016) - Published 7 September, 2016

Entanglement entropy of U(1) quantum spin liquids

Michael Pretko and T. Senthil

Phys. Rev. B 94, 125112 (2016) - Published 8 September, 2016

Entanglement entropy is a powerful tool for characterizing spin liquids and other systems with long-range entanglement. For gapped spin liquids, this problem has been well-studied, finding a universal subleading constant term in the entanglement entropy, known as the topological entanglement entropy. In this paper, the idea of topological entanglement entropy is generalized to the gapless U(1) spin liquid. First, it is shown that the entanglement entropy separates into two pieces, one due to emergent charges of the theory (assumed to be gapped) and one due to the emergent gapless gauge mode. Both give universal subheading contributions to the entanglement entropy, which are logarithmic in the size of the region considered. The photon contribution is due to the local physics of the gapless mode. The particle contribution, on the other hand, is a topological term, generalizing the notion of topological entanglement entropy. A construction is presented which can isolate this topological piece by eliminating the photon contribution and other local terms, such as the area law. This topological term in the entanglement entropy can serve as a powerful diagnostic tool for U(1) spin liquids.

Electronic structure and magnetism of samarium and neodymium adatoms on free-standing graphene

Agnieszka L. Kozub, Alexander B. Shick, František Máca, Jindřich Kolorenč, and Alexander I. Lichtenstein

Phys. Rev. B 94, 125113 (2016) - Published 8 September, 2016

Three-dimensional Hubbard model in the thermodynamic limit

Ehsan Khatami

Phys. Rev. B 94, 125114 (2016) - Published 9 September, 2016

Kondo effect in a quantum wire with spin-orbit coupling

G. R. de Sousa, Joelson F. Silva, and E. Vernek

Phys. Rev. B 94, 125115 (2016) - Published 9 September, 2016

Identification of the fractional quantum Hall edge modes by density oscillations

Na Jiang and Zi-Xiang Hu

Phys. Rev. B 94, 125116 (2016) - Published 12 September, 2016

Theoretical concepts of unlimited-power reflectors, absorbers, and emitters with conjugately matched layers

Constantinos A. Valagiannopoulos and Sergei A. Tretyakov

Phys. Rev. B 94, 125117 (2016) - Published 12 September, 2016

Interlayer electronic transport in CaMnBi2 antiferromagnet

Aifeng Wang (王爱峰), D. Graf, Lijun Wu, Kefeng Wang (王克锋), E. Bozin, Yimei Zhu, and C. Petrovic

Phys. Rev. B 94, 125118 (2016) - Published 12 September, 2016

Zeeman-field-induced nontrivial topological phases in a one-dimensional spin-orbit-coupled dimerized lattice

Masoud Bahari and Mir Vahid Hosseini

Phys. Rev. B 94, 125119 (2016) - Published 12 September, 2016

Phase diagram and topological phases in the triangular lattice Kitaev-Hubbard model

Kai Li, Shun-Li Yu, Zhao-Long Gu, and Jian-Xin Li

Phys. Rev. B 94, 125120 (2016) - Published 13 September, 2016

Topological massive Dirac edge modes and long-range superconducting Hamiltonians

O. Viyuela, D. Vodola, G. Pupillo, and M. A. Martin-Delgado

Phys. Rev. B 94, 125121 (2016) - Published 13 September, 2016

Fractionalizing glide reflections in two-dimensional Z2 topologically ordered phases

SungBin Lee, Michael Hermele, and S. A. Parameswaran

Phys. Rev. B 94, 125122 (2016) - Published 13 September, 2016

Optical force and torque on dipolar dual chiral particles

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

Phys. Rev. B 94, 125123 (2016) - Published 13 September, 2016

Partial self-consistency and analyticity in many-body perturbation theory: Particle number conservation and a generalized sum rule

Daniel Karlsson and Robert van Leeuwen

Phys. Rev. B 94, 125124 (2016) - Published 13 September, 2016

Section Chern number for a three-dimensional photonic crystal and the bulk-edge correspondence

Shuhei Oono, Toshikaze Kariyado, and Yasuhiro Hatsugai

Phys. Rev. B 94, 125125 (2016) - Published 14 September, 2016

Slicing the 3D Brillouin zone into 2D as a dimensional reduction makes the topological structure of the 3D Weyl point clear as a topological critical point. The Chern number of the sliced 2D system (section Chern number) changes discontinuously at the gap-closing momentum that guarantees topological stability of the Weyl point. This section Chern number is just a mathematical tool and cannot be directly measured experimentally. However, propagating edge modes of the 3D system with boundaries are necessarily momentum selective, associated with the section Chern number. This is a direct consequence of the bulk-edge correspondence. Using a localized basis with/without boundaries, the authors have demonstrated this here in a 3D helical photonic crystal without inversion symmetry

Manipulating charge density waves in 1T−TaS2 by charge-carrier doping: A first-principles investigation

D. F. Shao (邵定夫), R. C. Xiao, W. J. Lu, H. Y. Lv, J. Y. Li, X. B. Zhu, and Y. P. Sun

Phys. Rev. B 94, 125126 (2016) - Published 14 September, 2016

Electric and magnetic multipoles and bond orders in excitonic insulators

Tatsuya Kaneko and Yukinori Ohta

Phys. Rev. B 94, 125127 (2016) - Published 14 September, 2016

One-step theory of two-photon photoemission

J. Braun, R. Rausch, M. Potthoff, and H. Ebert

Phys. Rev. B 94, 125128 (2016) - Published 14 September, 2016

Pressure-induced spin crossover in disordered α−LiFeO2

Samar Layek, Eran Greenberg, Weiming Xu, Gregory Kh. Rozenberg, Moshe P. Pasternak, Jean-Paul Itié, and Dániel G. Merkel

Phys. Rev. B 94, 125129 (2016) - Published 15 September, 2016

From confined spinons to emergent fermions: Observation of elementary magnetic excitations in a transverse-field Ising chain

Zhe Wang, Jianda Wu, Shenglong Xu, Wang Yang, Congjun Wu, Anup Kumar Bera, A. T. M. Nazmul Islam, Bella Lake, Dmytro Kamenskyi, Papori Gogoi, Hans Engelkamp, Nanlin Wang, Joachim Deisenhofer, and Alois Loidl

Phys. Rev. B 94, 125130 (2016) - Published 16 September, 2016

Stabilization of topological insulator emerging from electron correlations on honeycomb lattice and its possible relevance in twisted bilayer graphene

Moyuru Kurita, Youhei Yamaji, and Masatoshi Imada

Phys. Rev. B 94, 125131 (2016) - Published 16 September, 2016

Bulk spectroscopic measurement of the topological charge of Weyl nodes with resonant x rays

Stefanos Kourtis

Phys. Rev. B 94, 125132 (2016) - Published 16 September, 2016

Plaquette valence bond theory of high-temperature superconductivity

Malte Harland, Mikhail I. Katsnelson, and Alexander I. Lichtenstein

Phys. Rev. B 94, 125133 (2016) - Published 19 September, 2016

Tuning ferromagnetic BaFe2(PO4)2 through a high Chern number topological phase

Young-Joon Song, Kyo-Hoon Ahn, Warren E. Pickett, and Kwan-Woo Lee

Phys. Rev. B 94, 125134 (2016) - Published 20 September, 2016

Magnetic phases and unusual topological electronic structures of Weyl semimetals in strong interaction limit

Liang-Jun Zhai, Po-Hao Chou, and Chung-Yu Mou

Phys. Rev. B 94, 125135 (2016) - Published 20 September, 2016

Reduction of magnetic interlayer coupling in barlowite through isoelectronic substitution

Daniel Guterding, Roser Valentí, and Harald O. Jeschke

Phys. Rev. B 94, 125136 (2016) - Published 20 September, 2016

Edge Majoranas on locally flat surfaces: The cone and the Möbius band

A. Quelle, C. Morais Smith, T. Kvorning, and T. H. Hansson

Phys. Rev. B 94, 125137 (2016) - Published 21 September, 2016

Kondo effect at low electron density and high particle-hole asymmetry in 1D, 2D, and 3D

Rok Žitko and Alen Horvat

Phys. Rev. B 94, 125138 (2016) - Published 21 September, 2016

Influence of halide composition on the structural, electronic, and optical properties of mixed CH3NH3Pb(I1−xBrx)3 perovskites calculated using the virtual crystal approximation method

Un-Gi Jong, Chol-Jun Yu, Jin-Song Ri, Nam-Hyok Kim, and Guk-Chol Ri

Phys. Rev. B 94, 125139 (2016) - Published 21 September, 2016

Chemical potential asymmetry and quantum oscillations in insulators

Hridis K. Pal, Frédéric Piéchon, Jean-Noël Fuchs, Mark Goerbig, and Gilles Montambaux

Phys. Rev. B 94, 125140 (2016) - Published 21 September, 2016

Electrical transport properties of single-crystal CaB6,SrB6, and BaB6

Jolanta Stankiewicz, Priscila F. S. Rosa, Pedro Schlottmann, and Zachary Fisk

Phys. Rev. B 94, 125141 (2016) - Published 22 September, 2016

Universal corner entanglement of Dirac fermions and gapless bosons from the continuum to the lattice

Johannes Helmes, Lauren E. Hayward Sierens, Anushya Chandran, William Witczak-Krempa, and Roger G. Melko

Phys. Rev. B 94, 125142 (2016) - Published 23 September, 2016

Chirality-induced spin current through spiral magnets

Hiroki Watanabe, Koujiro Hoshi, and Jun-ichiro Ohe

Phys. Rev. B 94, 125143 (2016) - Published 23 September, 2016

Impact of nonlocal correlations over different energy scales: A dynamical vertex approximation study

G. Rohringer and A. Toschi

Phys. Rev. B 94, 125144 (2016) - Published 26 September, 2016

Topological spin liquids in the ruby lattice with anisotropic Kitaev interactions

Saeed S. Jahromi, Mehdi Kargarian, S. Farhad Masoudi, and Abdollah Langari

Phys. Rev. B 94, 125145 (2016) - Published 26 September, 2016

Spinon Majorana fermions

Rui Wang, Hong-Yan Lu, Baigeng Wang, and C. S. Ting

Phys. Rev. B 94, 125146 (2016) - Published 26 September, 2016

Hubbard interactions in iron-based pnictides and chalcogenides: Slater parametrization, screening channels, and frequency dependence

Ambroise van Roekeghem, Loïg Vaugier, Hong Jiang, and Silke Biermann

Phys. Rev. B 94, 125147 (2016) - Published 27 September, 2016

Influence of k⊥ broadening on ARPES spectra of the (110) and (001) surfaces of SrVO3 films

T. Mitsuhashi, M. Minohara, R. Yukawa, M. Kitamura, K. Horiba, M. Kobayashi, and H. Kumigashira

Phys. Rev. B 94, 125148 (2016) - Published 28 September, 2016

Fast and efficient stochastic optimization for analytic continuation

F. Bao, Y. Tang, M. Summers, G. Zhang, C. Webster, V. Scarola, and T. A. Maier

Phys. Rev. B 94, 125149 (2016) - Published 28 September, 2016

Magnetic structures and magnetoelastic coupling of Fe-doped hexagonal manganites LuMn1−xFexO3(0≤x≤0.3)

Zhendong Fu, Harikrishnan S. Nair, Yinguo Xiao, Anatoliy Senyshyn, Vladimir Y. Pomjakushin, Erxi Feng, Yixi Su, W. T. Jin, and Thomas Brückel

Phys. Rev. B 94, 125150 (2016) - Published 30 September, 2016

Automated construction of maximally localized Wannier functions for bands with nontrivial topology

Jamal I. Mustafa, Sinisa Coh, Marvin L. Cohen, and Steven G. Louie

Phys. Rev. B 94, 125151 (2016) - Published 30 September, 2016

Wannier functions provide a useful description of the electronic states in a crystal, providing a chemical picture for the bonding structure of a material, in addition to applications in computational materials science. Topological insulators are an interesting class of materials with spin-polarized conducting surface states alongside an insulating bulk. To date, constructing Wannier functions for topological insulators has proven difficult, relying on an educated guess for the trial orbitals or requiring the system to be parameterized in order to tune between the normal and topological phase. The authors have developed an automated approach within the optimized projection functions method for constructing localized Wannier functions for topologically nontrivial bands. They demonstrate the method on a two-dimensional tight-binding model, a strong three-dimensional topological insulator, and finally, the prototypical topological insulating material Bi2Se3. They find that the Wannier functions contain large imaginary components and are more extended than those in the topologically trivial phase.

Topological insulators in the ordered double transition metals M2′M″C2 MXenes (M′=Mo, W; M″=Ti, Zr, Hf)

Mohammad Khazaei, Ahmad Ranjbar, Masao Arai, and Seiji Yunoki

Phys. Rev. B 94, 125152 (2016) - Published 30 September, 2016

Worm-improved estimators in continuous-time quantum Monte Carlo

P. Gunacker, M. Wallerberger, T. Ribic, A. Hausoel, G. Sangiovanni, and K. Held

Phys. Rev. B 94, 125153 (2016) - Published 30 September, 2016

Magnetotransport of multiple-band nearly antiferromagnetic metals due to hot-spot scattering

A. E. Koshelev

Phys. Rev. B 94, 125154 (2016) - Published 30 September, 2016

Semiconductors I: bulk

Electronic band structure of Mg−IV−N2 compounds in the quasiparticle-self-consistent GW approximation

Atchara Punya Jaroenjittichai and Walter R. L. Lambrecht

Phys. Rev. B 94, 125201 (2016) - Published 9 September, 2016

Characterization of oxygen defects in diamond by means of density functional theory calculations

Gergő Thiering and Adam Gali

Phys. Rev. B 94, 125202 (2016) - Published 9 September, 2016

Origin of low thermal conductivity in SnSe

Yu Xiao, Cheng Chang, Yanling Pei, Di Wu, Kunling Peng, Xiaoyuan Zhou, Shengkai Gong, Jiaqing He, Yongsheng Zhang, Zhi Zeng, and Li-Dong Zhao

Phys. Rev. B 94, 125203 (2016) - Published 12 September, 2016

Large Stark tuning of donor electron spin qubits in germanium

A. J. Sigillito, A. M. Tyryshkin, J. W. Beeman, E. E. Haller, K. M. Itoh, and S. A. Lyon

Phys. Rev. B 94, 125204 (2016) - Published 16 September, 2016

Spin dynamics and magnetic interactions of Mn dopants in the topological insulator Bi2Te3

S. Zimmermann, F. Steckel, C. Hess, H. W. Ji, Y. S. Hor, R. J. Cava, B. Büchner, and V. Kataev

Phys. Rev. B 94, 125205 (2016) - Published 21 September, 2016

All-coupling polaron optical response: Analytic approaches beyond the adiabatic approximation

S. N. Klimin, J. Tempere, and J. T. Devreese

Phys. Rev. B 94, 125206 (2016) - Published 22 September, 2016

Orbital mapping of energy bands and the truncated spin polarization in three-dimensional Rashba semiconductors

Qihang Liu, Xiuwen Zhang, J. A. Waugh, D. S. Dessau, and Alex Zunger

Phys. Rev. B 94, 125207 (2016) - Published 27 September, 2016

Self-diffusion in crystalline silicon: A single diffusion activation enthalpy down to 755∘C

Tobias Südkamp and Hartmut Bracht

Phys. Rev. B 94, 125208 (2016) - Published 29 September, 2016

Elastic and thermal properties of the layered thermoelectrics BiOCuSe and LaOCuSe

S. K. Saha and G. Dutta

Phys. Rev. B 94, 125209 (2016) - Published 30 September, 2016

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

Ab initio description of second-harmonic generation from crystal surfaces

Nicolas Tancogne-Dejean, Christine Giorgetti, and Valérie Véniard

Phys. Rev. B 94, 125301 (2016) - Published 6 September, 2016

Layer- and frequency-dependent second harmonic generation in reflection from GaSe atomic crystals

Yanhao Tang, Krishna C. Mandal, John A. McGuire, and Chih Wei Lai

Phys. Rev. B 94, 125302 (2016) - Published 6 September, 2016

Excitons in boron nitride single layer

Thomas Galvani, Fulvio Paleari, Henrique P. C. Miranda, Alejandro Molina-Sánchez, Ludger Wirtz, Sylvain Latil, Hakim Amara, and François Ducastelle

Phys. Rev. B 94, 125303 (2016) - Published 6 September, 2016

Induced spectral gap and pairing correlations from superconducting proximity effect

Ching-Kai Chiu, William S. Cole, and S. Das Sarma

Phys. Rev. B 94, 125304 (2016) - Published 6 September, 2016

Spin dynamics of hopping electrons in quantum wires: Algebraic decay and noise

A. V. Shumilin, E. Ya. Sherman, and M. M. Glazov

Phys. Rev. B 94, 125305 (2016) - Published 7 September, 2016

Spatially resolved scanning tunneling spectroscopy of single-layer steps on Si(100) surfaces

Xiqiao Wang, Pradeep Namboodiri, Kai Li, Xiao Deng, and Richard Silver

Phys. Rev. B 94, 125306 (2016) - Published 8 September, 2016

Spin polarization in the vicinity of quantum point contact with spin-orbit interaction

Sunwoo Kim, Yoshiaki Hashimoto, Taketomo Nakamura, and Shingo Katsumoto

Phys. Rev. B 94, 125307 (2016) - Published 9 September, 2016

Theoretical analysis of influence of random alloy fluctuations on the optoelectronic properties of site-controlled (111)-oriented InGaAs/GaAs quantum dots

R. Benchamekh, S. Schulz, and E. P. O'Reilly

Phys. Rev. B 94, 125308 (2016) - Published 9 September, 2016

Light propagation in tunable exciton-polariton one-dimensional photonic crystals

E. S. Sedov, E. D. Cherotchenko, S. M. Arakelian, and A. V. Kavokin

Phys. Rev. B 94, 125309 (2016) - Published 16 September, 2016

Dipolar polaritons in microcavity-embedded coupled quantum wells in electric and magnetic fields

J. Wilkes and E. A. Muljarov

Phys. Rev. B 94, 125310 (2016) - Published 19 September, 2016

Electric control of spin transport in GaAs (111) quantum wells

A. Hernández-Mínguez, K. Biermann, R. Hey, and P. V. Santos

Phys. Rev. B 94, 125311 (2016) - Published 21 September, 2016

Projected equations of motion approach to hybrid quantum/classical dynamics in dielectric-metal composites

Ryan J. McMillan, Lorenzo Stella, and Myrta Grüning

Phys. Rev. B 94, 125312 (2016) - Published 30 September, 2016

Surface physics, nanoscale physics, low-dimensional systems

Longitudinal spin relaxation of donor-bound electrons in direct band-gap semiconductors

Xiayu Linpeng, Todd Karin, M. V. Durnev, Russell Barbour, M. M. Glazov, E. Ya. Sherman, S. P. Watkins, Satoru Seto, and Kai-Mei C. Fu

Phys. Rev. B 94, 125401 (2016) - Published 1 September, 2016

RKKY-like contributions to the magnetic anisotropy energy: 3d adatoms on Pt(111) surface

Mohammmed Bouhassoune, Manuel dos Santos Dias, Bernd Zimmermann, Peter H. Dederichs, and Samir Lounis

Phys. Rev. B 94, 125402 (2016) - Published 1 September, 2016

Drag of electrons in graphene by substrate surface polar phonons

S. V. Koniakhin and A. V. Nalitov

Phys. Rev. B 94, 125403 (2016) - Published 2 September, 2016

Magnetoresistivity plateau of graphene in proximity to superconducting NbSe2

Xiaoqiang Zhang, Ran Tao, Laiming Wei, Jiangang Xu, Haixing Liang, Lijun Zhu, Yi Zhang, Naizhou Wang, Xianhui Chen, and Changgan Zeng

Phys. Rev. B 94, 125404 (2016) - Published 2 September, 2016

Coupled-layer description of topological crystalline insulators

I. C. Fulga, N. Avraham, H. Beidenkopf, and A. Stern

Phys. Rev. B 94, 125405 (2016) - Published 2 September, 2016

Modified emission of extended light emitting layers by selective coupling to collective lattice resonances

Mohammad Ramezani, Gabriel Lozano, Marc A. Verschuuren, and Jaime Gómez-Rivas

Phys. Rev. B 94, 125406 (2016) - Published 6 September, 2016

Quantum charge fluctuations of a proximitized nanowire

Roman M. Lutchyn, Karsten Flensberg, and Leonid I. Glazman

Phys. Rev. B 94, 125407 (2016) - Published 6 September, 2016

Generalized Aubry-André-Harper model with p-wave superconducting pairing

Qi-Bo Zeng, Shu Chen, and Rong Lü

Phys. Rev. B 94, 125408 (2016) - Published 7 September, 2016

Spin and the Coulomb gap in the half-filled lowest Landau level

J. P. Eisenstein, T. Khaire, D. Nandi, A. D. K. Finck, L. N. Pfeiffer, and K. W. West

Phys. Rev. B 94, 125409 (2016) - Published 8 September, 2016

In a strong magnetic field, two-dimensional electron systems are dominated by Coulomb interactions between the electrons. While the most familiar manifestation of these interactions is the fractional quantum Hall effect, this is actually a relatively subtle variation in the strong electronic correlations that exist throughout the high-field regime. This is clearly revealed in tunneling experiments in which an uncorrelated electron is rapidly thrust into a strongly correlated electron gas. A robust Coulomb pseudogap is observed, with tunneling strongly suppressed until the energy of the incoming electron is large enough. The Coulomb gap is insensitive to the precise magnetic field and is typically much larger than the energy gap associated with the fractional quantum Hall effect. In the present paper, the authors demonstrate that the size of the Coulomb gap observed in tunneling between two parallel two-dimensional electron systems depends sensitively on their spin configuration, with larger gaps associated with a larger net spin polarization. In effect, it is easier for electrons ‘to get out of the way’ of an incoming tunneling electron when the spin polarization of the electron gas is less than complete.

Effect of the edge states on the conductance and thermopower in zigzag phosphorene nanoribbons

R. Ma, H. Geng, W. Y. Deng, M. N. Chen, L. Sheng, and D. Y. Xing

Phys. Rev. B 94, 125410 (2016) - Published 8 September, 2016

Photovoltage detection of edge magnetoplasmon oscillations and giant magnetoplasmon resonances in a two-dimensional hole system

Jian Mi, Jianli Wang, L. N. Pfeiffer, K. W. West, K. W. Baldwin, and Chi Zhang

Phys. Rev. B 94, 125411 (2016) - Published 9 September, 2016

Peculiar half-metallic state in zigzag nanoribbons of MoS2: Spin filtering

F. Khoeini, Kh. Shakouri, and F. M. Peeters

Phys. Rev. B 94, 125412 (2016) - Published 9 September, 2016

Energy losses and transition radiation produced by the interaction of charged particles with a graphene sheet

Zoran L. Mišković, Silvina Segui, Juana L. Gervasoni, and Néstor R. Arista

Phys. Rev. B 94, 125414 (2016) - Published 12 September, 2016

Tunable anomalous Andreev reflection and triplet pairings in spin-orbit-coupled graphene

Razieh Beiranvand, Hossein Hamzehpour, and Mohammad Alidoust

Phys. Rev. B 94, 125415 (2016) - Published 12 September, 2016

Simultaneously giant enhancement of Förster resonance energy transfer rate and efficiency based on plasmonic excitations

Jun Ren, Tong Wu, Bing Yang, and Xiangdong Zhang

Phys. Rev. B 94, 125416 (2016) - Published 12 September, 2016

Electromechanical transition in quantum dots

G. Micchi, R. Avriller, and F. Pistolesi

Phys. Rev. B 94, 125417 (2016) - Published 13 September, 2016

Time-dependent scattering of a composite particle: A local self-energy approach for internal excitations

Federico Grasselli, Andrea Bertoni, and Guido Goldoni

Phys. Rev. B 94, 125418 (2016) - Published 14 September, 2016

Near-field radiative heat transfer between graphene and anisotropic magneto-dielectric hyperbolic metamaterials

Jinlin Song and Qiang Cheng

Phys. Rev. B 94, 125419 (2016) - Published 15 September, 2016

Helical gaps in interacting Rashba wires at low electron densities

Thomas L. Schmidt and Christopher J. Pedder

Phys. Rev. B 94, 125420 (2016) - Published 15 September, 2016

Effects of a magnetic Fe monolayer on the structural and surface electronic properties of Sb2Te3

Farideh Hajiheidari, Wei Zhang, and Riccardo Mazzarello

Phys. Rev. B 94, 125421 (2016) - Published 15 September, 2016

Strained fold-assisted transport in graphene systems

R. Carrillo-Bastos, C. León, D. Faria, A. Latgé, E. Y. Andrei, and N. Sandler

Phys. Rev. B 94, 125422 (2016) - Published 15 September, 2016

Time-domain quantum interference in graphene

François Fillion-Gourdeau, Denis Gagnon, Catherine Lefebvre, and Steve MacLean

Phys. Rev. B 94, 125423 (2016) - Published 16 September, 2016

Exciton Stark shift and electroabsorption in monolayer transition-metal dichalcogenides

Thomas Garm Pedersen

Phys. Rev. B 94, 125424 (2016) - Published 16 September, 2016

Transport in quantum spin Hall edges in contact to a quantum dot

Bruno Rizzo, Alberto Camjayi, and Liliana Arrachea

Phys. Rev. B 94, 125425 (2016) - Published 16 September, 2016

Unveiling Majorana quasiparticles by a quantum phase transition: Proposal of a current switch

F. A. Dessotti, L. S. Ricco, Y. Marques, L. H. Guessi, M. Yoshida, M. S. Figueira, M. de Souza, Pasquale Sodano, and A. C. Seridonio

Phys. Rev. B 94, 125426 (2016) - Published 16 September, 2016

Hall viscosity and electromagnetic response of electrons in graphene

Mohammad Sherafati, Alessandro Principi, and Giovanni Vignale

Phys. Rev. B 94, 125427 (2016) - Published 16 September, 2016

Tunable Majorana fermion from Landau quantization in 2D topological superconductors

R. S. Akzyanov, A. L. Rakhmanov, A. V. Rozhkov, and Franco Nori

Phys. Rev. B 94, 125428 (2016) - Published 19 September, 2016

Free and trapped hybrid charge transfer excitons at a ZnO/small-molecule heterojunction

Anurag Panda, Kan Ding, Xiao Liu, and Stephen R. Forrest

Phys. Rev. B 94, 125429 (2016) - Published 20 September, 2016

Coherent magneto-optical effects in topological insulators: Excitation near the absorption edge

Wang-Kong Tse

Phys. Rev. B 94, 125430 (2016) - Published 21 September, 2016

Near-field radiative heat transfer between metasurfaces: A full-wave study based on two-dimensional grooved metal plates

Jin Dai, Sergey A. Dyakov, Sergey I. Bozhevolnyi, and Min Yan

Phys. Rev. B 94, 125431 (2016) - Published 21 September, 2016

Exciton-polariton gap soliton dynamics in moving acoustic square lattices

J. V. T. Buller, R. E. Balderas-Navarro, K. Biermann, E. A. Cerda-Méndez, and P. V. Santos

Phys. Rev. B 94, 125432 (2016) - Published 22 September, 2016

Short-time counting statistics of charge transfer in Coulomb-blockade systems

Philipp Stegmann and Jürgen König

Phys. Rev. B 94, 125433 (2016) - Published 22 September, 2016

Changing anyonic ground degeneracy with engineered gauge fields

Emilio Cobanera, Jascha Ulrich, and Fabian Hassler

Phys. Rev. B 94, 125434 (2016) - Published 22 September, 2016

Magnetic properties of the α−T3 model: Magneto-optical conductivity and the Hofstadter butterfly

E. Illes and E. J. Nicol

Phys. Rev. B 94, 125435 (2016) - Published 23 September, 2016

Adsorption geometry and interface states: Relaxed and compressed phases of NTCDA/Ag(111)

P. Jakob, N. L. Zaitsev, A. Namgalies, R. Tonner, I. A. Nechaev, F. S. Tautz, U. Höfer, and D. Sánchez-Portal

Phys. Rev. B 94, 125436 (2016) - Published 26 September, 2016

Absence of superconductivity in ultrathin layers of FeSe synthesized on a topological insulator

Andreas Eich, Nils Rollfing, Fabian Arnold, Charlotte Sanders, Pascal R. Ewen, Marco Bianchi, Maciej Dendzik, Matteo Michiardi, Jian-Li Mi, Martin Bremholm, Daniel Wegner, Philip Hofmann, and Alexander A. Khajetoorians

Phys. Rev. B 94, 125437 (2016) - Published 26 September, 2016

Zero-line modes at stacking faulted domain walls in multilayer graphene

Changhee Lee, Gunn Kim, Jeil Jung, and Hongki Min

Phys. Rev. B 94, 125438 (2016) - Published 26 September, 2016

Path-integral description of combined Hamiltonian and non-Hamiltonian dynamics in quantum dissipative systems

A. M. Barth, A. Vagov, and V. M. Axt

Phys. Rev. B 94, 125439 (2016) - Published 26 September, 2016

Role of interlayer coupling for the power factor of CuSbS2 and CuSbSe2

Najebah M. Alsaleh, Nirpendra Singh, and Udo Schwingenschlögl

Phys. Rev. B 94, 125440 (2016) - Published 26 September, 2016

Effective production of orbital quantum entanglement in chaotic quantum dots with nonideal contacts

E. H. Santos and F. A. G. Almeida

Phys. Rev. B 94, 125441 (2016) - Published 27 September, 2016

Fano resonance engineering in slanted cavities with hyperbolic metamaterials

Fabio Vaianella and Bjorn Maes

Phys. Rev. B 94, 125442 (2016) - Published 28 September, 2016

Layer-dependent properties of SnS2 and SnSe2 two-dimensional materials

Joseph M. Gonzalez and Ivan I. Oleynik

Phys. Rev. B 94, 125443 (2016) - Published 29 September, 2016

Band-gap control in phosphorene/BN structures from first-principles calculations

Lukas Eugen Marsoner Steinkasserer, Simon Suhr, and Beate Paulus

Phys. Rev. B 94, 125444 (2016) - Published 29 September, 2016

Nonlinear response of a ballistic graphene transistor with an ac-driven gate: High harmonic generation and terahertz detection

Y. Korniyenko, O. Shevtsov, and T. Löfwander

Phys. Rev. B 94, 125445 (2016) - Published 30 September, 2016

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