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A Third-order Implicit-Explicit Runge-Kutta Method for Landau-Lifshitz Equation with Arbitrary Damping Parameters

Yan Gui, Rui Du, Cheng Wang

TL;DR

This paper develops a third-order implicit-explicit Runge-Kutta (IMEX-RK3) time-stepping scheme for the Landau-Lifshitz-Gilbert equation with arbitrary damping. By introducing an artificial diffusion term and splitting the right-hand side into nonlinear (explicit) and linear (implicit) parts, the method requires only linear systems with constant coefficients at each RK stage, enabling fast Poisson-solvers. The authors establish an order-3 convergence theory that holds uniformly in the damping parameter, provide a stability analysis yielding unconditional stability with respect to $\alpha$, and demonstrate, through 1D and 3D numerical experiments, that the scheme achieves third-order temporal accuracy and second-order spatial accuracy while being robust to varying damping. The work offers a high-accuracy, efficient, and damping-parameter-insensitive tool for micromagnetics simulations and related spin dynamics problems.

Abstract

A third-order accurate implicit-explicit Runge-Kutta time marching numerical scheme is proposed and implemented for the Landau-Lifshitz-Gilbert equation, which models magnetization dynamics in ferromagnetic materials, with arbitrary damping parameters. This method has three remarkable advantages:~(1) only a linear system with constant coefficients needs to be solved at each Runge-Kutta stage, which greatly reduces the time cost and improves the efficiency; (2) the optimal rate convergence analysis does not impose any restriction on the magnitude of damping parameter, which is consistent with the third-order accuracy in time for 1-D and 3-D numerical examples; (3) its unconditional stability with respect to the damping parameter has been verified by a detailed numerical study. In comparison with many existing methods, the proposed method indicates a better performance on accuracy and efficiency, and thus provides a better option for micromagnetics simulations.

A Third-order Implicit-Explicit Runge-Kutta Method for Landau-Lifshitz Equation with Arbitrary Damping Parameters

TL;DR

This paper develops a third-order implicit-explicit Runge-Kutta (IMEX-RK3) time-stepping scheme for the Landau-Lifshitz-Gilbert equation with arbitrary damping. By introducing an artificial diffusion term and splitting the right-hand side into nonlinear (explicit) and linear (implicit) parts, the method requires only linear systems with constant coefficients at each RK stage, enabling fast Poisson-solvers. The authors establish an order-3 convergence theory that holds uniformly in the damping parameter, provide a stability analysis yielding unconditional stability with respect to , and demonstrate, through 1D and 3D numerical experiments, that the scheme achieves third-order temporal accuracy and second-order spatial accuracy while being robust to varying damping. The work offers a high-accuracy, efficient, and damping-parameter-insensitive tool for micromagnetics simulations and related spin dynamics problems.

Abstract

A third-order accurate implicit-explicit Runge-Kutta time marching numerical scheme is proposed and implemented for the Landau-Lifshitz-Gilbert equation, which models magnetization dynamics in ferromagnetic materials, with arbitrary damping parameters. This method has three remarkable advantages:~(1) only a linear system with constant coefficients needs to be solved at each Runge-Kutta stage, which greatly reduces the time cost and improves the efficiency; (2) the optimal rate convergence analysis does not impose any restriction on the magnitude of damping parameter, which is consistent with the third-order accuracy in time for 1-D and 3-D numerical examples; (3) its unconditional stability with respect to the damping parameter has been verified by a detailed numerical study. In comparison with many existing methods, the proposed method indicates a better performance on accuracy and efficiency, and thus provides a better option for micromagnetics simulations.
Paper Structure (15 sections, 5 theorems, 107 equations, 2 figures, 7 tables)

This paper contains 15 sections, 5 theorems, 107 equations, 2 figures, 7 tables.

Key Result

Lemma 4.1

For any grid functions $\boldsymbol f_h$ and $\boldsymbol g_h$, with $\boldsymbol f_h$ satisfying the discrete boundary condition eq-2, the following identity is valid:

Figures (2)

  • Figure 1: The 1-D spatial grids, where ${{x}_{-\frac{1}{2}}}$ and ${{x}_{N+\frac{1}{2}}}$ are two ghost points.
  • Figure 2: Temporal and spatial accuracy orders in the 1-D and 3-D domains computations. Top row: 1-D; Bottom row: 3-D.

Theorems & Definitions (9)

  • Remark 3.1
  • Remark 3.2
  • Definition 4.1: $\ell^2$ inner product, ${{\left\| \cdot \right\|}_{2}}$ norm
  • Definition 4.2: The discrete ${{\left\| \cdot \right\|}_{\infty}}$ and ${{\left\| \cdot \right\|}_{p}}$ norms
  • Lemma 4.1: Summation by parts
  • Lemma 4.2: Inverse inequality
  • Lemma 4.3: Discrete Gronwall inequality
  • Theorem 5.1
  • Lemma 5.1