Theory of spin magnetization driven by chiral phonons
arXiv:2501.10766 · doi:10.1103/PhysRevB.111.134414
Abstract
We construct a general theory of spin magnetization driven by chiral phonons under an adiabatic process, in which atoms rotate around their equilibrium positions with a low phonon frequency. Here the spin magnetization originates from the modulated electronic states with spin-orbital coupling by atomic rotations. Under the adiabatic approximation, the time-dependent spin magnetization can be calculated by a Berry-phase method. In this paper, we focus on its time average, which is evaluated by assuming that the phonon displacement is small. As a result, the time average of the spin magnetization is concisely formulated in the form of the Berry curvature defined in the phonon-displacement space as an intrinsic property of atomic rotations. Our formula for spin magnetization reflects the chiral nature of phonons, and is convenient for calculations.
9 pages, 4 figures
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Cited by in corpus (6)
- Theory of spin Seebeck effect activated by acoustic chiral phonons
- Cavity-induced coherent magnetization and polaritons in altermagnets
- Catalogue of chiral phonon materials
- Microscopic Theory of Chiral-Phonon-Induced Orbital Selectivity in Helical Crystals
- Dynamical Orbital Angular Momentum Induced by Circularly Polarized Phonons
- Pseudo-chiral phonon splitting from octupolar magnetic order