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This research investigates the emergence of a temperature-dependent non-Abelian thermal gauge potential within ferromagnetic systems driven by spin-polarized currents, linking time evolution operators to SU(2) and SU(3) gauge transformations. By deriving an analytical solution for the Landau-Lifshitz-Gilbert equation in the semi-classical limit, the study provides a theoretical framework for understanding magnetization dynamics under specific thermal conditions. While grounded in condensed matter physics, the work contributes directly to the fundamental understanding of spin transport and quantum coherence mechanisms relevant to quantum information processing.
The temperature-dependent non-Abelian gauge potential
arXiv:2608.25437v1 Announce Type: new Abstract: This study shows that the usual time evolution operator can act as a U(1) gauge transformation on the initial wavefuntion. When considering the spin freedom in the system, the time evolution operator corresponds to a non-Abelian SU(2) gauge transformation for spin-1/2 particles and a SU(3) gauge transformation for spin-1 particles. If we adopt the adiabatic approximation in the magnetization dynamics of a ferromagnetic system driven by a spin-polarized current, a temperature-dependent non-Abelian thermal gauge potential will appear. We can employ a temperature-dependent Landau-Lifshitz-Gilbert (LLG) equation to describe the magnetization dynamics in the semi-classical limit, a linear approximated solution for this equation is given analytically.
Abstract:This study shows that the usual time evolution operator can act as a U(1) gauge transformation on the initial wavefuntion. When considering the spin freedom in the system, the time evolution operator corresponds to a non-Abelian SU(2) gauge transformation for spin-1/2 particles and a SU(3) gauge transformation for spin-1 particles. If we adopt the adiabatic approximation in the magnetization dynamics of a ferromagnetic system driven by a spin-polarized current, a temperature-dependent non-Abelian thermal gauge potential will appear. We can employ a temperature-dependent Landau-Lifshitz-Gilbert (LLG) equation to describe the magnetization dynamics in the semi-classical limit, a linear approximated solution for this equation is given analytically.
Quantum Physics (quant-ph); Mesoscale and Nanoscale Physics (cond-mat.mes-hall)
arXiv:2608.25437 [quant-ph]
(or arXiv:2608.25437v1 [quant-ph] for this version)
https://doi.org/10.48550/arXiv.2608.25437 Focus to learn more arXiv-issued DOI via DataCite (pending registration)
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