Nonlinear spin motive force driven by quantum geometry
Oral-In-person
Abstract
Quantum geometry characterizes the geometric structures of the parameter space on which electronic states depend, and these structures are called the quantum metric and Berry curvature. Such a structure in electron momentum space is known to govern both linear and nonlinear electrical responses. Extending this concept, enlarged parameter space composed of momentum k and magnetization m, namely the (k, m)-space, is considered. In the linear response, the current generated by time-varying magnetization (j ∝ ∂t m), known as the spin-motive force (SMF), is determined by the (k, m)-space Berry curvature. Such a linear SMF, however, will vanish under the one cycle of magnetization dynamics. Its nonlinear counterpart will avoid such a disappearance and are expected to be expressed in terms of the quantum metric in (k, m)-space. However, such a nonlinear SMF has remained unexplored up to date.
In this talk, we propose a theory of nonlinear SMF induced by time-varying magnetization from the viewpoint of (k, m)-space quantum geometry [1]. Using the semiclassical wave-packet theory and the perturbation expansion in the exchange interaction, we find an intrinsic second-order SMF have both rectification and second-harmonic generation, and arises from the (k, m)-space quantum metric and Berry curvature.
[1] T. Meguro, H. Ishizuka, K. Nomura, in preparation.
In this talk, we propose a theory of nonlinear SMF induced by time-varying magnetization from the viewpoint of (k, m)-space quantum geometry [1]. Using the semiclassical wave-packet theory and the perturbation expansion in the exchange interaction, we find an intrinsic second-order SMF have both rectification and second-harmonic generation, and arises from the (k, m)-space quantum metric and Berry curvature.
[1] T. Meguro, H. Ishizuka, K. Nomura, in preparation.
–
Publication: T. Meguro, H. Ishizuka, K. Nomura, in preparation.
Presenters
-
Tomonari Meguro
- Kyushu University