Emergent Non-Abelian Gauge Theory in Coupled Spin-Electron Dynamics
arXiv:2202.04694 · doi:10.1103/PhysRevB.106.094433
Abstract
A clear separation of the time scales governing the dynamics of "slow" and "fast" degrees of freedom often serves as a prerequisite for the emergence of an independent low-energy theory. Here, we consider (slow) classical spins exchange coupled to a tight-binding system of (fast) conduction electrons. The effective equations of motion are derived under the constraint that the quantum state of the electron system at any instant of time lies in the -dimensional low-energy subspace for the corresponding spin configuration at . The effective low-energy theory unfolds itself straightforwardly and takes the form of a non-abelian gauge theory with the gauge freedom given by the arbitrariness of the basis spanning the instantaneous low-energy sector. The holonomic constraint generates a gauge covariant spin-Berry curvature tensor in the equations of motion for the classical spins. In the non-abelian theory for , opposed to the adiabatic spin dynamics theory, the spin-Berry curvature is generically nonzero, even for time-reversal symmetric systems. Its expectation value with the representation of the electron state is gauge invariant and gives rise to an additional {\em geometrical} spin torque. Besides anomalous precession, the theory also captures the spin nutational motion, which is usually considered as a retardation effect. This is demonstrated by proof-of-principle numerical calculations for a minimal model with a single classical spin. Already for and in parameter regimes where the adiabatic theory breaks down, we find good agreement with results obtained from the full (unconstrained) theory.
19 pages, 12 figures, v2 with minor changes
References in corpus (26)
- Berry Phase Effects on Electronic Properties
- Atomistic spin model simulations of magnetic nanomaterials
- Microscopic approach to current-driven domain wall dynamics
- A method for atomistic spin dynamics simulations: implementation and examples
- Adiabatic Theorem without a Gap Condition
- Ab-initio calculation of the Gilbert damping parameter via linear response formalism
- Atomistic spin dynamic method with both damping and moment of inertia effects included from first principles
- Linear dynamics of quantum-classical hybrids
- Magnetization Dynamics, Gyromagnetic Relation, and Inertial Effects
- Spin Dynamics with Inertia in Metallic Ferromagnets
- Time-retarded damping and magnetic inertia in the Landau-Lifshitz-Gilbert equation self-consistently coupled to electronic time-dependent nonequilibrium Green functions
- Consistent classical and quantum mixed dynamics
- Vector Potential and Berry phase-induced Force
- Spin dynamics and relaxation in the classical-spin Kondo-impurity model beyond the Landau-Lifschitz-Gilbert equation
- Spintronics meets nonadiabatic molecular dynamics: Geometric spin torque and damping on noncollinear classical magnetism due to electronic open quantum system
- Anomalous spin precession under a geometrical torque
- Dynamics of localized spins coupled to the conduction electrons with charge/spin currents
- Exploring dynamical magnetism with time-dependent density-functional theory: from spin fluctuations to Gilbert damping
- Relaxation of a classical spin coupled to a strongly correlated electron system
- Inertia effects in the real-time dynamics of a quantum spin coupled to a Fermi sea
- Topological spin torque emerging in classical-spin systems with different time scales
- Accessing long timescales in the relaxation dynamics of spins coupled to a conduction-electron system using absorbing boundary conditions
- Long-time relaxation dynamics of a spin coupled to a Chern insulator
- Magnetic properties of a capped kagome molecule with 60 quantum spins
- Non-Hamiltonian dynamics of indirectly coupled classical impurity spins
- Controlling the real-time dynamics of a spin coupled to the helical edge states of the Kane-Mele model