Periodic micromagnetic finite element method

The periodic micromagnetic finite element method (PM-FEM) is introduced to solve periodic unit cell problems using the Landau–Lifshitz–Gilbert equation. PM-FEM is applicable to general problems with 1D, 2D, and 3D periodicities. PM-FEM is based on a nonperiodic FEM-based micromagnetic solver and ext...

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Published inJournal of magnetism and magnetic materials Vol. 615; no. C; p. 172776
Main Authors Ai, Fangzhou, Duan, Jiawei, Lomakin, Vitaliy
Format Journal Article
LanguageEnglish
Published Netherlands Elsevier B.V 01.03.2025
Elsevier
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ISSN0304-8853
1873-4766
DOI10.1016/j.jmmm.2025.172776

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Abstract The periodic micromagnetic finite element method (PM-FEM) is introduced to solve periodic unit cell problems using the Landau–Lifshitz–Gilbert equation. PM-FEM is applicable to general problems with 1D, 2D, and 3D periodicities. PM-FEM is based on a nonperiodic FEM-based micromagnetic solver and extends it in several aspects to account for periodicities, including the computation of exchange and magnetostatic fields. For the exchange field, PM-FEM modifies the sparse matrix construction for computing the Laplace operator to include additional elements arising due to the periodicities. For the magnetostatic field, the periodic extensions include modifications in the local operators, such as gradient, divergence, and surface magnetic charges, as well as the long-range superposition operator for computing the periodic scalar potential. The local operators are extended to account for the periodicities similar to handling the Laplace operator. For the long-range superposition operator, PM-FEM utilizes a periodic Green’s function (PGF) and fast spatial convolutions. The PGF is computed rapidly via exponentially rapidly convergent sums. The spatial convolutions are accomplished via a modified fast Fourier transform based adaptive integral method that allows calculating spatial convolutions with nonuniform meshes in O(NlogN) numerical operations. PM-FEM is implemented on CPU and GPU based computer architectures. PM-FEM allows efficiently handling cases of structures contained within the periodic unit cell touching or not touching its boundaries as well as structures that protrude beyond the unit cell boundaries. PM-FEM is demonstrated to have about the same or even higher performance than its parent nonperiodic code. The demonstrated numerical examples show the efficiency of PM-FEM for highly complex structures with 1D, 2D, and 3D periodicities. •Finite element method micromagnetic solver with periodic boundaries is introduced.•Arbitrary 1D, 2D, and 3D periodic boundary conditions are allowed at high accuracy.•The method is based on superposition integrals with no need in air layers.•High performance is achieved on CPUs and GPUs.•Large highly complex problems can be handled.
AbstractList The periodic micromagnetic finite element method (PM-FEM) is introduced to solve periodic unit cell problems using the Landau–Lifshitz–Gilbert equation. PM-FEM is applicable to general problems with 1D, 2D, and 3D periodicities. PM-FEM is based on a nonperiodic FEM-based micromagnetic solver and extends it in several aspects to account for periodicities, including the computation of exchange and magnetostatic fields. For the exchange field, PM-FEM modifies the sparse matrix construction for computing the Laplace operator to include additional elements arising due to the periodicities. For the magnetostatic field, the periodic extensions include modifications in the local operators, such as gradient, divergence, and surface magnetic charges, as well as the long-range superposition operator for computing the periodic scalar potential. The local operators are extended to account for the periodicities similar to handling the Laplace operator. For the long-range superposition operator, PM-FEM utilizes a periodic Green’s function (PGF) and fast spatial convolutions. The PGF is computed rapidly via exponentially rapidly convergent sums. The spatial convolutions are accomplished via a modified fast Fourier transform based adaptive integral method that allows calculating spatial convolutions with nonuniform meshes in O(NlogN) numerical operations. PM-FEM is implemented on CPU and GPU based computer architectures. PM-FEM allows efficiently handling cases of structures contained within the periodic unit cell touching or not touching its boundaries as well as structures that protrude beyond the unit cell boundaries. PM-FEM is demonstrated to have about the same or even higher performance than its parent nonperiodic code. The demonstrated numerical examples show the efficiency of PM-FEM for highly complex structures with 1D, 2D, and 3D periodicities. •Finite element method micromagnetic solver with periodic boundaries is introduced.•Arbitrary 1D, 2D, and 3D periodic boundary conditions are allowed at high accuracy.•The method is based on superposition integrals with no need in air layers.•High performance is achieved on CPUs and GPUs.•Large highly complex problems can be handled.
ArticleNumber 172776
Author Lomakin, Vitaliy
Ai, Fangzhou
Duan, Jiawei
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Issue C
Keywords Finite element method
Landau–Lifshitz–Gilbert equation
Magnetostatic field
Micromagnetics
High-performance computing
Periodic structures
Language English
License This is an open access article under the CC BY license.
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  doi: 10.1109/8.774139
– year: 1993
  ident: 10.1016/j.jmmm.2025.172776_b41
– volume: 105
  start-page: 07D541
  issue: 7
  year: 2009
  ident: 10.1016/j.jmmm.2025.172776_b45
  article-title: Nonuniform grid algorithm for fast calculation of magnetostatic interactions in micromagnetics
  publication-title: J. Appl. Phys.
  doi: 10.1063/1.3076048
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Snippet The periodic micromagnetic finite element method (PM-FEM) is introduced to solve periodic unit cell problems using the Landau–Lifshitz–Gilbert equation. PM-FEM...
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StartPage 172776
SubjectTerms Finite element method
High-performance computing
Landau–Lifshitz–Gilbert equation
Magnetostatic field
Micromagnetics
Periodic structures
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Title Periodic micromagnetic finite element method
URI https://dx.doi.org/10.1016/j.jmmm.2025.172776
https://www.osti.gov/biblio/2530691
https://doi.org/10.1016/j.jmmm.2025.172776
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