Organizations: Department of Physics, The Chinese University of Hong Kong, Shatin, Hong Kong SAR, China · State Key Laboratory of Extreme Photonics and Instrumentation, ZJU-Hangzhou Global Scientific and Technological Innovation Center, Zhejiang University, Hangzhou 310027, China. · The Electromagnetics Academy at Zhejiang University, College of Information Science and Electronic Engineering, Zhejiang University, Hangzhou 310027, China. · Zhejiang Key Lab. of Intelligent Electromagnetic Control and Advanced Electronic Integration, Jinhua Institute of Zhejiang University, Zhejiang University, Jinhua 321099, China. · State Key Laboratory of Quantum Information Technologies and Materials, The Chinese University of Hong Kong, Shatin, Hong Kong SAR, China
High-frequency artificial phononic crystals offer a low-loss platform compatible with on-chip integration, yet realizing Chern phononic phases at GHz frequencies remains challenging. Here, we propose a magnon-induced phononic Chern insulator in a honeycomb phononic crystal hybridized with ferromagnetic islands at the hexagon centers. A circularly polarized Kittel mode couples to the surrounding phonons with a phase winding, which breaks time-reversal symmetry and opens a full Chern gap. In the large-detuning regime, this mechanism leads to an effective Haldane-type phononic model with magnon-induced complex hopping. By tuning the magnon-phonon interaction, the full hybrid system accesses Chern phases with tunable Chern numbers |C|=1 and |C|=2. The predicted gaps can exceed realistic phonon and magnon linewidths, enabling their observation in GHz acoustic devices. Our work establishes chiral magnon--phonon hybridization as a route to magnetically reconfigurable topological phononics.
Figures & tables
Figure 1: (a) Schematic of Human-Agentic hybrid workflow. (b) A honeycomb phononic crystal with one phonon mode on each A and B sublattice site. A magnetic island at the plaquette center supports a right-handed circular Kittel mode. The six surrounding phononic sites are labeled in their physical counterclockwise order as A1,B1,A2,B2,A3,B3 . Their radial vectors are dα,i=a0(cosθα,i,sinθα,i) , with θA,i=2π(i−1)/3 , θB,i=(2i−1)π/3 , and a0 is the distance from the plaquette center to each surrounding phononic site. (c) Momentum-space intensity of the magnon–phonon terms ∣GA(k)∣2 and ∣GB(k)∣2 , showing that the magnon couples selectively to sublattice A at K and to sublattice B at K′ . (d) Schematic of the magnon-induced effective phonon hopping, showing Heff−Hph , where only the magnon-induced coupling between phonons is depicted. The coupling phase is illustrated in the right panel. Each NN bond receives virtual-magnon contributions from the center magnons of its two adjacent plaquettes.
Figure 2: (a) Bulk band structures in the absence (gray dashed curves) and presence (colored solid curves) of the magnon-phonon coupling, which explicitly opens a gap at the Dirac points. The lower, middle and upper bands have the Chern numbers C=(−1,+1,0) , respectively. (b) The corresponding strip spectrum for g=0.4 , with periodic boundary conditions applied along a1=a0(3,3)/2 . (c) Spatial distribution of the edge states, calculated as the sum of the probability of all localized modes within the bandgap. Parameters are set as t=1 and δω=3.2 .
Figure 3: (a) and (b) Chern-number phase diagrams of the lowest band and the middle band, respectively, as functions of the magnon detuning δω and the magnon–phonon coupling strength g , with t=1 . The dashed curve 4g2=t2+tδω , marks the gap-closing condition at the M point, while the vertical dashed line in (b) indicates the Γ -point transition at δω=3t . (c) and (d) Plots of bulk bandgaps Δ1 (gap between the lower and middle bands) and Δ2 (gap between the middle and upper bands), respectively, as functions of δω and g .
From butterfly wings to remnants of nuclear detonation, aperiodic order repeatedly emerges in nature, often exhibiting reduced sensitivity to boundaries and symmetry constraints. Inspired by this principle, a paradigm shift is introduced in nanomechanical resonator design from periodic to aperiodic structures, focusing on a special class: quasicrystals (QCs). Although soft clamping enabled by phononic stopbands has become a central strategy for achieving high-Qm nanomechanical resonators, its practical realization has been largely confined to periodic phononic crystals, where band structure engineering is well established. The potential of aperiodic architectures, however, has remained largely unexplored, owing to their intrinsic complexity and the lack of systematic approaches to identifying and exploiting stopband behavior. Here we demonstrate that soft clamping can be realized in quasicrystal architectures and that high-Qm nanomechanical resonators can be systematically predicted through a data-driven design framework. As a representative demonstration, the 12-fold QC-based resonator obtained numerically a quality factor Qm∼107 and an effective mass of sub-nanograms at MHz frequencies, corresponding to an exceptional force sensitivity of 26.4~aN/Hz compared to previous 2D phononic crystals. These results establish QCs as a robust platform for next-generation nanomechanical resonators and open a new design regime beyond periodic order.
Kawen Li, Hangjin Cho, Richard Norte +1
Department of Precision and Microsystems Engineering, Delft University of Technology, Delft, The Netherlands · Department of Mechanical Engineering, Pohang University of Science and Technology, Pohang, Republic of Korea
A two-dimensional electron gas in a uniform neutralizing background forms a triangular Wigner crystal at low density. In a strongly mass-asymmetric electron-hole bilayer, localized heavy holes instead provide a nonuniform positive background that supports an electron crystal at densities two orders of magnitude higher than for a homogeneous electron gas in the same material. Here we show that correlated mobile electrons can overturn the preference for triangular order, stabilizing a honeycomb electron-hole crystal. Using the powerful real-space neural-network variational Monte Carlo in the Born-Oppenheimer limit with fixed holes, we find that increasing the density drives a transition from a triangular electron-hole crystal to a honeycomb crystal, which eventually melts into itinerant electrons coexisting with the honeycomb or the triangular hole lattice at fixed interlayer separation. Relative to triangular order, honeycomb order emerges when gains in electronic kinetic energy and electron-hole attraction outweigh its higher intralayer Coulomb repulsion, a threshold never reached in the rigid point-dipole model. Moreover, the honeycomb hole lattice supports paramagnetic, antiferromagnetic, and stripe-ordered spin states. Complex polarization indicates a metal-insulator transition, while the states on the honeycomb hole lattice are consistent with a stripe-ordered Dirac semimetal and paramagnetic or antiferromagnetic Mott insulators via mapping to the half-filled Hubbard model. We further propose a BLG/hBN/WS2-WSe2 heterostructure as a platform for the predicted honeycomb crystal, at an experimentally feasible density n∼1011cm−2.
Shengdu Chai, Wangqian Miao, Yuqiang Li +3
Interdisciplinary Center for Theoretical Physics and Information Sciences (ICTPIS), Fudan University, Shanghai 200433, China · Shanghai Artificial Intelligence Laboratory, Shanghai 200232, China · Department of Physics, The Hong Kong University of Science and Technology, Clear Water Bay, Hong Kong, China +3
Discovering materials that must simultaneously satisfy multiple competing constraints remains a central challenge in computational materials design, particularly in data-scarce regimes where conventional data-driven approaches are least effective. Magnetic insulators represent a stringent example: the electronic conditions that favor magnetic order often also promote metallicity, while insulating behavior suppresses the interactions that stabilize magnetism. As a result, experimentally viable magnetic insulators are rare and difficult to identify through conventional screening. Here, we introduce MagMatLLM, a constraint-guided generative discovery framework that integrates language-model-based crystal generation with evolutionary selection, surrogate screening, and first-principles validation to target simultaneous stability, magnetism, and insulating behavior. Unlike stability-first approaches, the framework enforces functional constraints during generation and selection, steering the search toward sparsely populated regions of materials space defined by competing physical requirements. Using this workflow, we identify twelve previously unreported candidate magnetic insulators, including Tm4Co2Cr2O12 and Cr4Nb2O12. Of these, ten are dynamically stable by phonon analysis and exhibit finite band gaps and nonzero magnetic moments in spin-polarized density functional theory calculations. Beyond the specific compounds identified here, this work establishes a general constraint-guided paradigm for multi-objective materials discovery in sparse chemical spaces and provides a transferable strategy for the design of quantum materials under competing physical constraints.
Department of Math, University of Southern California, Los Angeles, CA, 90007 · Department of Computer Science, Colby College, Waterville, ME, 04901 · Department of Materials Science and Engineering, University of California, Los Angeles, Los Angeles, CA 90095, United States +1