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Physical Review B - January 2024

Physical Review B

covering condensed matter and materials physics
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Volume 109, Issues 1 - 4

January 2024
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Highlights

Editors' Suggestion
Bose-Einstein condensation in systems with flux equilibrium
Victor S. L'vov, Anna Pomyalov, Sergey V. Nazarenko, Dmytro A. Bozhko, Alexander J. E. Kreil, Burkard Hillebrands, and Alexander A. Serga
Phys. Rev. B 109, 014301 (2024) – Published 3 January 2024

Quasiparticles, created in dissipative nonlinear wave systems by external excitation, can form a Bose-Einstein condensate. The authors describe here the physical phenomena and conditions leading to condensation in various regimes of external excitation from weak and stationary to ultrastrong pumping. The authors have developed a stationary nonlinear theory of kinetic instability for the latter, supported by the experimental data for magnons, parametrically pumped in room-temperature films of yttrium iron garnet.

Editors' Suggestion
Variational density functional perturbation theory for metals
Xavier Gonze, Samare Rostami, and Christian Tantardini
Phys. Rev. B 109, 014317 (2024) – Published 30 January 2024

Density Functional Perturbation Theory (DFPT) is a proven method for analyzing molecular and solid responses to perturbations. For metals, challenges arise due to Fermi-Dirac statistics and electronic bands crossing the Fermi energy. This work focuses on variational DFPT for metals, examining the convexity of the entropy function of occupation numbers. It emphasizes benefits from resmearing Fermi-Dirac broadening at finite temperature, details variational expressions for free energy derivatives, and addresses inaccuracies in unperturbed wavefunctions. The formalism is implemented in the ABINIT software.

Editors' Suggestion
Exotic quantum liquids in Bose-Hubbard models with spatially modulated symmetries
Pablo Sala, Yizhi You, Johannes Hauschild, and Olexei Motrunich
Phys. Rev. B 109, 014406 (2024) – Published 9 January 2024

This work investigates the zero-temperature physics of generalized Bose-Hubbard models, which conserve finite Fourier momenta of the particle number. Analytical and numerical calculations predict a novel quasi-long-range order phase, in addition to more conventional Mott insulators. The former is characterized by a two-species Luttinger liquid in the infrared, with microscopic expectation values dressed by oscillatory contributions. The authors also conjecture that this phase is destroyed by the unbinding of topological defects along the temporal direction even when they are confined along the transverse direction.

Editors' Suggestion
Magnon interactions in the quantum paramagnetic phase of CoNb2O6
C. A. Gallegos and A. L. Chernyshev
Phys. Rev. B 109, 014424 (2024) – Published 25 January 2024

The strongly anisotropic quasi-one-dimensional ferromagnet CoNb2O6 in a transverse field has provided a spectacular realization of the magnon decay effect in its paramagnetic phase. A self-consistent theory is proposed to regularize unphysical divergences while preserving the integrity of the singular threshold phenomena of magnon decay, demonstrating quantitative agreement with the neutron scattering results throughout the field regime inaccessible by standard spin-wave theory. Phenomenological constraints on the model, connections of CoNb2O6 to the other anisotropic-exchange materials, and the effects of longitudinal fields are explored.

Editors' Suggestion
Nonlinear magnons and exchange Hamiltonians of the delafossite proximate quantum spin liquid candidates KYbSe2 and NaYbSe2
A. O. Scheie, Y. Kamiya, Hao Zhang, Sangyun Lee, A. J. Woods, M. O. Ajeesh, M. G. Gonzalez, B. Bernu, J. W. Villanova, J. Xing, Q. Huang, Qingming Zhang, Jie Ma, Eun Sang Choi, D. M. Pajerowski, Haidong Zhou, A. S. Sefat, S. Okamoto, T. Berlijn, L. Messio, R. Movshovich, C. D. Batista, and D. A. Tennant
Phys. Rev. B 109, 014425 (2024) – Published 25 January 2024

Quantum spin liquids were proposed over 50 years ago, but identifying experimental signatures is extremely difficult. Here, the authors study the Yb triangular materials KYbSe2 and NaYbSe2, and show that KYbSe2 is well described by the Heisenberg J2-J1 model. Comparing this material to NaYbSe2 and CsYbSe2, a trend emerges where the magnetic exchange interactions are correlated with chemical substitution. This allows these systems to be controllably tuned toward (and possibly into) a theoretically predicted quantum spin liquid phase.

Editors' Suggestion
Quantum magnetism in the frustrated square lattice oxyhalides YbBi2IO4 and YbBi2ClO4
Pyeongjae Park, G. Sala, Th. Proffen, Matthew B. Stone, Andrew D. Christianson, and Andrew F. May
Phys. Rev. B 109, 014426 (2024) – Published 25 January 2024

This work establishes Yb-containing oxyhalides as a new family of materials for studying quantum magnetism on a frustrated square lattice. The titular compounds appear to possess long-range magnetic order below ≈0.21 K (YbBi2lO4), but analysis of their thermodynamic properties via a J1-J2 square lattice model suggests large magnetic frustration. This places the materials near the transition to a quantum spin liquid. Thus, the impact of quantum fluctuations is expected to be strong, motivating detailed studies of these and related phases.

Editors' Suggestion
Self-induced inverse spin Hall effect in La0.67Sr0.33MnO3 films
Pushpendra Gupta, In Jun Park, Anupama Swain, Abhisek Mishra, Vivek P. Amin, and Subhankar Bedanta
Phys. Rev. B 109, 014437 (2024) – Published 29 January 2024

The authors report here the self-induced inverse spin Hall effect in epitaxial La0.67Sr0.33MnO3 (LSMO) films and perform first-principles calculations of the spin Hall conductivities of bulk LSMO. The LSMO films were prepared using pulsed laser deposition. The spin pumping voltage Vsp dominates over spin rectification effects, indicating the presence of appreciable spin-to-charge conversion in LSMO films. The spin Hall conductivity is calculated from first principles using density functional theory and the Kubo formalism, and the results qualitatively match with the experimental findings.

Editors' Suggestion
Experimental and computational study of the core-level crossing transition in iridium at high pressure
C. V. Storm, G. A. Woolman, C. M. Lonsdale, J. D. McHardy, M. J. Duff, G. J. Ackland, and M. I. McMahon
Phys. Rev. B 109, 024101 (2024) – Published 3 January 2024

This static high-pressure x-ray diffraction study of iridium investigates previous reports of a core-level crossing at 80 GPa, whereby the authors find no evidence for such a transition. Further computational investigations reveal that a core-level crossing does occur in iridium, but only at 400 GPa. In addition, the efficacy of bismuth as a pressure-transmitting medium is demonstrated, maintaining a uniaxial stress component in the sample below 2% up to 159 GPa.

Featured in Physics
Experimental investigation of the premelting process in Sn
Stephen G. Lipson and Emil Polturak
Phys. Rev. B 109, 024109 (2024) – Published 25 January 2024
Physics logo
Synopsis:Watching Defects Melt in a Crystal

Researchers have experimentally captured the melting of defects in a crystal, a process previously only understood through simulations.

Editors' Suggestion
Topological transition from nodal to nodeless Zeeman splitting in altermagnets
Rafael M. Fernandes, Vanuildo S. de Carvalho, Turan Birol, and Rodrigo G. Pereira
Phys. Rev. B 109, 024404 (2024) – Published 3 January 2024

Altermagnets are an unconventional type of magnetic state with various appealing properties, both from the fundamental and applied physics perspectives. By investigating the impact of spin-orbit coupling on these states, this work reveals that all altermagnets are intrinsically noncollinear and that their Zeeman splittings possess symmetry-protected nodal lines. These features endow altermagnets with a remarkable resilience against external magnetic fields.

Editors' Suggestion
Distinct universality classes of diffusive transport from full counting statistics
Sarang Gopalakrishnan, Alan Morningstar, Romain Vasseur, and Vedika Khemani
Phys. Rev. B 109, 024417 (2024) – Published 12 January 2024

The authors provide an analytic theory of the transport of magnetization in a set of interacting anisotropic spin chains. Even though these are many-body systems with diffusive transport on average, the full distribution that gives rise to that average is far from Gaussian – with fluctuations that, unlike conventional diffusion, are comparable to the mean. This is an example of how systems with the same hydrodynamics can belong to distinct dynamical universality classes.

Editors' Suggestion
Magnetic antiskyrmions in two-dimensional van der Waals magnets engineered by layer stacking
Kai Huang, Edward Schwartz, Ding-Fu Shao, Alexey A. Kovalev, and Evgeny Y. Tsymbal
Phys. Rev. B 109, 024426 (2024) – Published 19 January 2024

Antiskyrmions, like skyrmions, are topologically protected magnetic quasiparticles, but exhibit greater stability and no transverse motion compared to skyrmions. This study employs ab initio calculations to investigate the polar layer stacking of two monolayers of a two-dimensional magnetic material CrI3, which can lead to the emergence of antiskyrmions. Atomistic spin dynamics simulations demonstrate the realization of antiskyrmions in Mn-doped CrI3 and shows that their spin texture can be switched by ferroelectric polarization of the polar bilayer.

Editors' Suggestion
Chiral phonons and phononic birefringence in ferromagnetic metal–bulk acoustic resonator hybrids
M. Müller, J. Weber, F. Engelhardt, V. A. S. V. Bittencourt, T. Luschmann, M. Cherkasskii, M. Opel, S. T. B. Goennenwein, S. Viola Kusminskiy, S. Geprägs, R. Gross, M. Althammer, and H. Huebl
Phys. Rev. B 109, 024430 (2024) – Published 23 January 2024

The magnetoelastic coupling of magnetic and elastic excitations enables the generation of elastic waves carrying angular momentum. In a quantum picture, this corresponds to a resonant conversion of magnons to chiral phonons and vice versa. This study showcases this conversion process using a simple and versatile experimental platform consisting of a metallic magnetic thin film on a crystalline substrate. These findings allow us to study the impact of crystal symmetry on angular momentum transport by phonons and investigate phononic birefringence.

Editors' Suggestion
Electrically sign-reversible topological Hall effect in a top-gated topological insulator (Bi,Sb)2Te3 grown on europium iron garnet
J.-F. Wong, K.-H. M. Chen, J.-M. Chia, Z.-P. Huang, S.-X. Wang, P.-T. Chen, L. B. Young, Y.-H. G. Lin, S.-F. Lee, C.-Y. Mou, M. Hong, and J. Kwo
Phys. Rev. B 109, 024432 (2024) – Published 26 January 2024

The topological Hall effect (THE) is a Hall response that arises from the deflection of motion of charge carriers flowing through nontrivial spin textures. Here, the authors observe a significant THE and investigate its interplay with the spin-polarized topological surface states in a proximity-magnetized topological insulator/ferrimagnet heterostructure. Specifically, they demonstrate a sign change in THE via a top electrical gate as the Fermi level is tuned from the electron-doped to the hole-doped region of the gapped Dirac cone.

Editors' Suggestion
Breakdown of chiral edge modes in topological magnon insulators
Jonas Habel, Alexander Mook, Josef Willsher, and Johannes Knolle
Phys. Rev. B 109, 024441 (2024) – Published 30 January 2024

Topological magnon edge modes have been proposed for the realization of robust, low-loss spintronic devices. However, ubiquitous many-body interactions that do not preserve particle number significantly compromise their topological protection. The authors show here that these interactions can lead to significant edge mode damping, hybridization with bulk modes, and coupling between edge modes on opposite sides. These findings pose challenges for the experimental realization of topological magnon edge modes, but can be overcome by the application of large magnetic fields.

Editors' Suggestion
Upper bounds on superconducting and excitonic phase stiffness for interacting isolated narrow bands
Dan Mao and Debanjan Chowdhury
Phys. Rev. B 109, 024507 (2024) – Published 10 January 2024

This work develops a systematic theoretical framework to determine the low-energy effective "diamagnetic" response associated with superconductivity and excitonic superfluidity in strongly interacting electronic models hosting isolated nearly flat bands. The results can be used to derive upper bounds on the transition temperatures for superconductivity and excitonic superfluidity without making any mean-field type approximations. The same theoretical framework can also be extended with very few modifications, to address questions related to ferromagnetism in flat bands and magnetic circular dichroism.

Editors' Suggestion
Experimental nuclear quadrupole resonance and computational study of the structurally refined topological semimetal TaSb2
T. Fujii, O. Janson, H. Yasuoka, H. Rosner, Yu. Prots, U. Burkhardt, M. Schmidt, and M. Baenitz
Phys. Rev. B 109, 035116 (2024) – Published 9 January 2024

The electric field gradient (EFG) and magnetic excitation of TaSb2 were studied using nuclear quadrupole resonance (NQR) in a single crystal. The EFG parameters determined by measuring all expected NQR lines were corroborated by density functional theory (DFT) calculations. Despite the good agreement between the measured and calculated Sommerfeld coefficients, the spin-lattice relaxation rate was not captured by the DFT band calculations. To overcome this discrepancy, the authors propose a site-dependent in-gap state with an average energy gap of ~7 meV for the Sb sites and ~22 meV for the Ta site, which are much smaller than the semimetallic gap.

Editors' Suggestion
Spin-orbit interaction enabled electronic Raman scattering from charge collective modes
Surajit Sarkar, Alexander Lee, Girsh Blumberg, and Saurabh Maiti
Phys. Rev. B 109, 035160 (2024) – Published 25 January 2024

The inelastic photon scattering process by bulk plasmon collective modes in conventional metals is restricted by conservation laws. Here, the authors demonstrate that for materials with broken SU(2) spin symmetry that is present in inversion broken systems, the restriction on the light scattering process can be removed by spin-correlation mediated coupling of light to plasmons. The theory is supported by resonant Raman scattering experiment on BiTeI, a material with a giant Rashba effect, in which the authors explicitly demonstrate this light scattering process by plasmons.

Editors' Suggestion
Spatial dispersion in silicon
Subiao Bian, Razvigor Ossikovski, Adolf Canillas, Gerald Jellison, and Oriol Arteaga
Phys. Rev. B 109, 035201 (2024) – Published 3 January 2024

Here, the complete determination of the spectroscopic permittivity tensor of crystalline silicon in consideration of spatial dispersion (SD) is presented. Using spectroscopic ellipsometry, two complex parameters, ε and p1 (wave-vector-dependent for SD), were measured, revealing significant findings. Remarkably, pronounced UV region anisotropy was observed in (110) silicon wafers, surpassing the NIR region by up to five orders of magnitude. In contrast, minimal anisotropy was detected in (100) plane measurements, supporting the proposed tensor model. Comparative analysis of (100) and (110) wafers, incorporating SD, showcased consistent ε values, contributing valuable insights into silicon's behavior.

Featured in Physics Editors' Suggestion
Composite-fermion pairing at half-filled and quarter-filled lowest Landau level
Anirban Sharma, Ajit C. Balram, and J. K. Jain
Phys. Rev. B 109, 035306 (2024) – Published 22 January 2024
Physics logo
Viewpoint:Composite Fermions Are Better Together

The physical origin of the fractional quantum Hall effect at the half-filled lowest Landau level in wide quantum wells has remained a puzzle since its discovery three decades ago. This work presents quantitative calculations supporting the formation of a p-wave topological "superconductor" of composite fermions (CFs) here. CFs are predicted to form f-wave pairs at the quarter-filled Landau level in wide quantum wells. CF pairing is thus seen as the principal mechanism underlying the even-denominator fractional quantum Hall effect.

Editors' Suggestion
Itinerant ferromagnetism in transition metal dichalcogenide moiré superlattices
Pawel Potasz, Nicolás Morales-Durán, Nai Chao Hu, and Allan H. MacDonald
Phys. Rev. B 109, 045144 (2024) – Published 23 January 2024

Moiré superlattices give a unique opportunity to investigate controllable quantum systems. Previous studies of transition metal dichalcogenide heterobilayers mainly focused on magnetic order at half-filling or charge orders at partial fillings. Here, the authors investigate itinerant ferromagnetism in the vicinity of the van Hove singularity of moiré triangular superlattices. From many-body exact diagonalization calculations that shed light on the magnon spectra and the magnetic susceptibility, the Curie temperature is estimated to vary with moiré lattice constant, from a few to a few tens of kelvins.

Editors' Suggestion
Electronic structure, magnetic correlations, and superconducting pairing in the reduced Ruddlesden-Popper bilayer La3Ni2O6 under pressure: Different role of d3z2−r2 orbital compared with La3Ni2O7
Yang Zhang, Ling-Fang Lin, Adriana Moreo, Thomas A. Maier, and Elbio Dagotto
Phys. Rev. B 109, 045151 (2024) – Published 30 January 2024

The authors investigate here two bilayer nickelates under pressure, establishing substantial qualitative differences between the two systems. They find that the d3z2−r2 orbital in La3Ni2O6 and La3Ni2O7 plays a different role: one "active" orbital (dx2−y2) vs two "active" orbitals (eg), respectively. The Fermi surface only has two sheets in La3Ni2O6, with the γ pocket absent, different from La3Ni2O7. They also find that La3Ni2O6 is far from a superconducting instability. Moreover, they do not observe changes in the electronic density in La3Ni2O6 under pressure.

Editors' Suggestion
Microwave spectroscopy of interacting Andreev spins
J. J. Wesdorp, F. J. Matute-Cañadas, A. Vaartjes, L. Grünhaupt, T. Laeven, S. Roelofs, L. J. Splitthoff, M. Pita-Vidal, A. Bargerbos, D. J. van Woerkom, P. Krogstrup, L. P. Kouwenhoven, C. K. Andersen, A. Levy Yeyati, B. van Heck, and G. de Lange
Phys. Rev. B 109, 045302 (2024) – Published 3 January 2024

Andreev bound states are fermionic states localized in weak links between superconductors, which can be occupied with spinful quasiparticles. Recently, experiments embedding a nanowire Josephson junction into a superconducting circuit have enabled coherent manipulation of a single Andreev spin. However, these experiments remained limited to small magnetic fields. Here, the authors measure the microwave spectra of a nanowire Josephson junction in magnetic fields up to ∼ 250 mT and identify singlet, doublet, and triplet states of interacting Andreev spins.

Editors' Suggestion
Gapless fluctuations and exceptional points in semiconductor lasers
N. H. Kwong, M. Em. Spotnitz, and R. Binder
Phys. Rev. B 109, 045306 (2024) – Published 23 January 2024

Semiconductor lasers have formal analogies to Bardeen-Cooper-Schrieffer (BCS) superconductors. This work shows that, in analogy to gapless superconductivity, a gapless lasing parametric regime, in which the frequency gap in the fluctuation spectrum is closed, exists for steady-state semiconductor lasers. The gap opens when the laser intensity exceeds a threshold. This gapless-to-gapped transition occurs at a third-order exceptional point.

Editors' Suggestion
Optical conductivity and damping of plasmons due to electron-electron interaction
Prachi Sharma, Alessandro Principi, Giovanni Vignale, and Dmitrii L. Maslov
Phys. Rev. B 109, 045431 (2024) – Published 24 January 2024

The calculation of the optical conductivity of electrons in two-dimensions is a classic problem of many-body theory. It is inextricably linked with the problem of plasmon damping, where plasmons are collective oscillations of the electronic density. Here, the authors resolve discrepancies that existed in the prior literature and provide definitive results for the dependence of the optical conductivity upon wavelength, frequency, and temperature. The results are interpreted in terms of bulk and shear viscosities of the electron gas.

Editors' Suggestion Letter
Non-Hermitian Hamiltonians violate the eigenstate thermalization hypothesis
Giorgio Cipolloni and Jonah Kudler-Flam
Phys. Rev. B 109, L020201 (2024) – Published 3 January 2024

The eigenstate thermalization hypothesis (ETH) represents a cornerstone in the theoretical understanding of the emergence of thermal behavior in closed quantum systems. Here, the authors investigate to what extent the ETH holds for non-Hermitian Hamiltonians, relevant for open and monitored quantum systems, and come to the surprising conclusion that fluctuations are greatly enhanced, indicating the breakdown of thermalization.

Editors' Suggestion Letter
Experimental determination of the spin Hamiltonian of the cubic chiral magnet MnSi
P. Dalmas de Réotier, A. Yaouanc, G. Lapertot, C. Wang, A. Amato, and D. Andreica
Phys. Rev. B 109, L020408 (2024) – Published 25 January 2024

The authors determine here the minimal spin Hamiltonian of manganese silicide from analysis of muon spin rotation experimental data measured in its helical and conical phases. The model includes Heisenberg and Dzyaloshinskii-Moriya interactions between the Mn nearest neighbors. In particular, information is derived on the orientation of the Moriya vector that cannot be inferred from the symmetry of the Mn-Mn bond. This result enforces constraints for future theoretical works, e.g., on the origin of the stability of the magnetic skyrmions phase.

Editors' Suggestion Letter
Spin-mediated direct photon scattering by plasmons in BiTeI
A. C. Lee, S. Sarkar, K. Du, H.-H. Kung, C. J. Won, K. Wang, S.-W. Cheong, S. Maiti, and G. Blumberg
Phys. Rev. B 109, L041111 (2024) – Published 25 January 2024

It has been long established that collective charge oscillations of electron density relative to nuclei lattice – the bulk plasmons in metals – are typically unobservable by light scattering spectroscopy. Here, the authors report the unexpected observation of a distinct long-lived plasmon mode in the Raman spectrum of BiTeI, a material with a giant Rashba spin-orbit coupling. In contrast to conventional expectations, the findings reveal strong and direct light scattering by bulk plasmons even in the long-wavelength limit. The authors also establish the basic criteria enabling the discovered observation.

Editors' Suggestion Letter
Emergence of composite many-body exciton states in WS2 and MoSe2 monolayers
J. Choi, J. Li, D. Van Tuan, H. Dery, and S. A. Crooker
Phys. Rev. B 109, L041304 (2024) – Published 30 January 2024

When electron-hole pairs (excitons) are photoexcited into semiconductors containing a Fermi sea of mobile charges, they can form bound states known variously as trions, tetrons, or exciton-polarons. Crucially, the interaction occurs with those mobile carriers possessing distinguishable quantum numbers (e.g., spin). In monolayer TMD semiconductors, the availability of both spin and valley quantum numbers allows excitons to interact, simultaneously, with more than one type of quantum-mechanically distinguishable carrier. This leads to new types of composite excitons (e.g., six-particle "hexcitons"), which appear as distinct resonances in optical spectra.

Editors' Suggestion Letter
Employing quasidegenerate optical modes for chiral sensing
S. F. Almousa, T. Weiss, and E. A. Muljarov
Phys. Rev. B 109, L041410 (2024) – Published 26 January 2024

The authors demonstrate here a linear splitting of quasidegenerate modes in the presence of chirality in optical systems. Employing the resonant-state expansion and two quasidegenerate modes, they reveal the transformation of the chirality effect on mode splitting from second to first order in the Pasteur parameter (ϰ). This linear effect is demonstrated for individual chiral particles and homogeneous chiral perturbations of metasurfaces. These findings deepen our understanding of chirality-induced mode splitting, opening prospects for innovative sensing schemes.

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