Multiferrons are defined as elementary excitations with both electric and magnetic character that tilt polarization, generate magnetization via dynamical multiferroicity, and carry quadrupole and octupole moments, as computed for LiNbO3.
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4 Pith papers cite this work. Polarity classification is still indexing.
representative citing papers
DFT+U models of cubic/hexagonal NiO, monoclinic/trigonal Ni(OH)2, and NiOOH supply vibrational references that align with operando Raman spectra and TEM observations for OER-relevant phases.
Spin-orbit coupling enriches spin-phonon interactions in α-RuCl₃ to produce finite phonon Berry curvatures and a thermal Hall effect that qualitatively matches measured κ_xy field dependence.
Sn incorporation in MBA₂SnₓPb₁₋ₓI₄ distorts octahedra with only minor effect on structural chirality while substantially enhancing phonon chirality, yet without increasing temperature-gradient angular momentum due to mode compensation.
citing papers explorer
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Lattice excitations with finite polarization and magnetization
Multiferrons are defined as elementary excitations with both electric and magnetic character that tilt polarization, generate magnetization via dynamical multiferroicity, and carry quadrupole and octupole moments, as computed for LiNbO3.
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DFT-Guided Operando Raman Characterization of Ni-Based Phases Relevant to Electrochemical Systems
DFT+U models of cubic/hexagonal NiO, monoclinic/trigonal Ni(OH)2, and NiOOH supply vibrational references that align with operando Raman spectra and TEM observations for OER-relevant phases.
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Theory of Intrinsic Phonon Thermal Hall Effect in $\alpha$-RuCl$_3$
Spin-orbit coupling enriches spin-phonon interactions in α-RuCl₃ to produce finite phonon Berry curvatures and a thermal Hall effect that qualitatively matches measured κ_xy field dependence.
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Impact of Metal Cation on Chiral Properties of 2D Halide Perovskites
Sn incorporation in MBA₂SnₓPb₁₋ₓI₄ distorts octahedra with only minor effect on structural chirality while substantially enhancing phonon chirality, yet without increasing temperature-gradient angular momentum due to mode compensation.