Ren Yafei, Xiao Cong, Saparov Daniyar, Niu Qian
Department of Physics, The University of Texas at Austin, Austin, Texas 78712, USA.
Department of Materials Science and Engineering, University of Washington, Seattle, Washington 98195, USA.
Phys Rev Lett. 2021 Oct 29;127(18):186403. doi: 10.1103/PhysRevLett.127.186403.
The traditional theory of magnetic moments for chiral phonons is based on the picture of the circular motion of the Born effective charge, typically yielding a small fractional value of the nuclear magneton. Here we investigate the adiabatic evolution of electronic states induced by the lattice vibration of a chiral phonon and obtain an electronic orbital magnetization in the form of a topological second Chern form. We find that the traditional theory needs to be refined by introducing a k resolved Born effective charge, and identify another contribution from the phonon-modified electronic energy together with the momentum-space Berry curvature. The second Chern form can diverge when there is a Yang's monopole near the parameter space of interest as illustrated by considering a phonon at the Brillouin zone corner in a gapped graphene model. We also find large magnetic moments for the optical phonon in bulk topological materials where nontopological contribution is also important. Our results agree with recent observations in experiments.
传统的手性声子磁矩理论基于玻恩有效电荷圆周运动的图像,通常会产生一个小的核磁子分数值。在这里,我们研究了由手性声子的晶格振动引起的电子态绝热演化,并得到了一种拓扑第二陈数形式的电子轨道磁化强度。我们发现,传统理论需要通过引入k分辨的玻恩有效电荷来完善,并确定了声子修正电子能量与动量空间贝里曲率的另一贡献。当在感兴趣的参数空间附近存在杨振宁单极子时,第二陈数形式可能会发散,这在有能隙的石墨烯模型中布里渊区角点处的声子情况中得到了说明。我们还发现,在体拓扑材料中,光学声子的磁矩很大,其中非拓扑贡献也很重要。我们的结果与最近的实验观测结果一致。