Bajpai Utkarsh, Nikolić Branislav K
Department of Physics and Astronomy, University of Delaware, Newark, Delaware 19716, USA.
Phys Rev Lett. 2020 Oct 30;125(18):187202. doi: 10.1103/PhysRevLett.125.187202.
We analyze a quantum-classical hybrid system of steadily precessing around the fixed axis slow classical localized magnetic moments (LMMs), forming a head-to-head domain wall, surrounded by fast electrons driven out of equilibrium by LMMs and residing within a metallic wire whose connection to macroscopic reservoirs makes electronic quantum system an open one. The model captures the essence of dynamical noncollinear magnetic textures encountered in spintronics, while making it possible to obtain the exact time-dependent nonequilibrium density matrix of electronic systems and split it into four contributions. The Fermi surface contribution generates dissipative (or dampinglike in spintronics terminology) spin torque on LMMs, as the counterpart of electronic friction in nonadiabatic molecular dynamics (MD). Among two Fermi sea contributions, one generates geometric torque dominating in the adiabatic regime, which remains as the only nonzero contribution in a closed system with disconnected reservoirs. Locally geometric torque can have nondissipative (or fieldlike in spintronics terminology) component, acting as the counterpart of geometric magnetism force in nonadiabatic MD, as well as a much smaller dampinglike component acting as "geometric friction." Such current-independent geometric torque is absent from widely used micromagnetics or atomistic spin dynamics modeling of magnetization dynamics based on the Landau-Lifshitz-Gilbert equation, while previous analyses of how to include our Fermi-surface dampinglike torque have severely underestimated its total magnitude.
我们分析了一个量子 - 经典混合系统,其中缓慢的经典局域磁矩(LMMs)围绕固定轴稳定进动,形成一个对头畴壁,周围是被LMMs驱动至非平衡态的快速电子,这些电子存在于一根金属线内,该金属线与宏观储能器的连接使电子量子系统成为一个开放系统。该模型抓住了自旋电子学中遇到的动态非共线磁纹理的本质,同时能够获得电子系统精确的含时非平衡密度矩阵,并将其分解为四种贡献。费米面贡献在LMMs上产生耗散性(或自旋电子学术语中的阻尼样)自旋扭矩,这是非绝热分子动力学(MD)中电子摩擦的对应物。在两个费米海贡献中,一个产生在绝热区域占主导的几何扭矩,在具有断开储能器的封闭系统中,它是唯一的非零贡献。局部几何扭矩可以有非耗散性(或自旋电子学术语中的场样)分量,作为非绝热MD中几何磁力的对应物,以及一个小得多的阻尼样分量,作为“几何摩擦”。这种与电流无关的几何扭矩在基于朗道 - 里夫希茨 - 吉尔伯特方程的广泛使用的微磁学或原子自旋动力学磁化动力学建模中不存在,而先前关于如何纳入我们的费米面阻尼样扭矩的分析严重低估了其总量。