Theory of phonon angular momentum transport across smooth interfaces between crystals

Yuta Suzuki, Shuntaro Sumita, Yusuke Kato
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Abstract

We study the spatial profile of phonon angular momentum in a junction between a chiral crystal and a non-chiral (achiral) crystal with a smooth, flat contact at low temperatures. In this junction, the angular momentum is generated by an imbalance in non-equilibrium distributions between transverse acoustic modes. We incorporate the Fresnel coefficients for elastic waves to establish a boundary condition for the phonon distributions, for which we also provide a proof. We demonstrate that the spin angular momentum of phonon induced by a thermal gradient in the chiral crystal diffuses into the adjacent achiral crystal. This diffusion is accompanied by a finite orbital angular momentum stemming from acoustic analog of the Imbert--Fedorov shift in reflected/transmitted wave packets. Concerning angular momentum fluxes that are polarized normal to the interface, the sum of the spin and orbital components is continuous at the interface. This continuity confirms the conservation law of total phonon angular momentum.
晶体间光滑界面的声子角动量传输理论
我们研究了手性晶体与非手性(非手性)晶体之间的交界处声子角动量的空间分布,该交界处在低温下具有光滑平整的接触面。在这个交界处,角动量是由横向声波模式之间的非平衡分布产生的。我们结合弹性波的菲涅尔系数建立了声子分布的边界条件,并为此提供了证明。我们证明了手性晶体中热梯度诱导的声子自旋角动量会扩散到相邻的非手性晶体中。这种扩散伴随着有限的轨道角动量,这种轨道角动量来自反射/透射波包中类似于英伯特-费多罗夫位移的声学现象。关于界面法线极化的角动量通量,自旋和轨道分量之和在界面上是连续的。这种连续性证实了声子总角动量的守恒定律。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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