Charge density waves in the 2.5-dimensional quantum heterostructure
F. Z. Yang, T. T. Zhang, F. Y. Meng, H. C. Lei, C. Nelson, Y. Q. Cai, E. Vescovo, A. H. Said, P. M. Lozano, G. Fabbris, and H. Miao
Phys. Rev. B 111, L041101 (2025) - Published 2 January, 2025
Ab initio study on heavy-fermion behavior in : Role of Hund's coupling and stability
Steffen Backes, Yusuke Nomura, Ryotaro Arita, and Hiroshi Shinaoka
Phys. Rev. B 111, L041102 (2025) - Published 2 January, 2025
Winding Berry dipoles on uniaxially strained graphene/insulator moiré superlattices
Angiolo Huamán and Salvador Barraza-Lopez
Phys. Rev. B 111, L041103 (2025) - Published 7 January, 2025
Emergent cross-product-type spin-orbit coupling under ferroaxial ordering
Akane Inda and Satoru Hayami
Phys. Rev. B 111, L041104 (2025) - Published 7 January, 2025
Ferroaxial ordering, which is characterized as a ferroic alignment of a time-reversal-even axial vector, is often caused by vertical mirror symmetry breaking according to a rotational distortion of the lattice structure. The authors theoretically clarify here the emergent cross-product-type spin-orbit coupling under ferroaxial ordering based on a - tetragonal cluster model. Such unconventional spin-orbit entanglement originates from the interplay between the atomic spin-orbit coupling and the - hybridization according to vertical mirror symmetry breaking.
Topological triviality of flat Hamiltonians
Pratik Sathe and Rahul Roy
Phys. Rev. B 111, L041105 (2025) - Published 9 January, 2025
Landau levels have played a pivotal role in advancing our understanding of topological phases of matter. Motivated by Landau levels, which are flat and topological, the authors answer here the following question: can a tight-binding Hamiltonian that exclusively has flat bands be topologically nontrivial? The authors show that, under broad conditions, energy levels in such flat-band Hamiltonians have vanishing Chern numbers. They also identify the exotic condition that is necessary for topologically nontrivial flat-band Hamiltonians. Importantly, all the proofs extend even to Hamiltonians that lack translational invariance.
Diagrammatic Monte Carlo scheme for dielectric losses in metals
I. S. Tupitsyn and N. V. Prokof'ev
Phys. Rev. B 111, L041106 (2025) - Published 10 January, 2025
Kohn's theorem applied to quantum oscillations in cuprates
Sudip Chakravarty
Phys. Rev. B 111, L041107 (2025) - Published 13 January, 2025
Kardar-Parisi-Zhang universality at the edge of Laughlin states
Gustavo M. Monteiro, Dylan Reynolds, Paolo Glorioso, and Sriram Ganeshan
Phys. Rev. B 111, L041108 (2025) - Published 14 January, 2025
Constraints on the orbital flux phase in from the polar Kerr effect
Hao-Tian Liu, Junkang Huang, Tao Zhou, and Wen Huang
Phys. Rev. B 111, L041109 (2025) - Published 16 January, 2025
Snell's law in multirefringent systems
József Cserti, Áron Holló, and László Oroszlány
Phys. Rev. B 111, L041110 (2025) - Published 16 January, 2025
Microscopic theory of field-tuned topological transitions in the Kitaev honeycomb model
Jagannath Das, Aman Kumar, and Vikram Tripathi
Phys. Rev. B 111, L041111 (2025) - Published 21 January, 2025
Photonic realization of chiral hinge states in a Chern-insulator stack
Han-Rong Xia, Jia-Zheng Li, Si-Yu Yuan, and Meng Xiao
Phys. Rev. B 111, L041112 (2025) - Published 21 January, 2025
Probing Fermi surface parity with spin-resolved transverse magnetic focusing
M. J. Rendell, S. D. Liles, S. Bladwell, A. Srinivasan, O. Klochan, I. Farrer, D. A. Ritchie, O. P. Sushkov, and A. R. Hamilton
Phys. Rev. B 111, L041113 (2025) - Published 22 January, 2025
Fermi surface measurements are critical for determining the electrical and magnetic properties of solids. Typical techniques used in 2D systems such as Shubnikov–de Haas and commensurability oscillations are unable to detect changes in the parity of the Fermi surface, i.e., when (+) (-). In this work, the authors show that transverse magnetic focusing can be used to detect changes in Fermi surface parity, as focusing only measures a well defined section of the Fermi surface.
Direct free energy calculation from ab initio path integral Monte Carlo simulations of warm dense matter
Tobias Dornheim, Zhandos A. Moldabekov, Sebastian Schwalbe, and Jan Vorberger
Phys. Rev. B 111, L041114 (2025) - Published 23 January, 2025
Fermi-liquid behavior of nonaltermagnetic
Maxim Wenzel, Ece Uykur, Sahana Rößler, Marcus Schmidt, Oleg Janson, Achyut Tiwari, Martin Dressel, and Alexander A. Tsirlin
Phys. Rev. B 111, L041115 (2025) - Published 28 January, 2025
Disorder-induced instability of a Weyl nodal loop semimetal towards a diffusive topological metal with protected multifractal surface states
João S. Silva, Miguel Gonçalves, Eduardo V. Castro, Pedro Ribeiro, and Miguel A. N. Araújo
Phys. Rev. B 111, L041116 (2025) - Published 28 January, 2025
Axion insulator, Weyl points, quantum anomalous Hall effect, and magnetic topological phase transition in
Jingyu Yao, Ruihan Zhang, Sheng Zhang, Haohao Sheng, Youguo Shi, Zhong Fang, Hongming Weng, and Zhijun Wang
Phys. Rev. B 111, L041117 (2025) - Published 29 January, 2025
Quantum kinetic theory of the linear response for weakly disordered multiband systems
T. Valet and R. Raimondi
Phys. Rev. B 111, L041118 (2025) - Published 30 January, 2025











