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Theory of magnetic field stabilized compact skyrmions in thin-film ferromagnets

Anne Bernand-Mantel1,2,*, Anaïs Fondet1,2, Sarah Barnova1, Theresa M. Simon3, and Cyrill B. Muratov4,5

  • 1Université de Toulouse, Laboratoire de Physique et Chimie des Nano-Objets, UMR 5215 INSA, CNRS, UPS, 135 Avenue de Rangueil, F-31077 Toulouse Cedex 4, France
  • 2Centre d'Elaboration de Matériaux et d'Etudes Structurales, CEMES-CNRS, 29 rue Jeanne Marvig, 31055 Toulouse, France
  • 3Institut für Analysis und Numerik, Westfälische Wilhelms-Universität Münster, Einsteinstr. 62, 48149 Münster, Germany
  • 4Department of Mathematical Sciences, New Jersey Institute of Technology, Newark, New Jersey 07102, USA
  • 5Departimento di Matematica, Università di Pisa, Largo B. Pontecorvo, 5, 56127 Pisa, Italy

  • *bernandm@insa-toulouse.fr

Phys. Rev. B 108, L161405 – Published 13 October, 2023

DOI: https://doi.org/10.1103/PhysRevB.108.L161405

Abstract

We present a micromagnetic theory of compact magnetic skyrmions under applied magnetic field that accounts for the full dipolar energy and the interfacial Dzyaloshinskii-Moryia interaction (DMI) in the thin-film regime. Asymptotic analysis is used to derive analytical formulas for the parametric dependence of the skyrmion size and rotation angle, as well as the energy barriers for collapse and bursting, two processes that lead to a finite skyrmion lifetime. We demonstrate the existence of a regime at low DMI, in which the skyrmion is stabilized by a combination of nonlocal dipolar interaction and a magnetic field applied parallel to its core, and discuss the conditions for an experimental realization of such field-stabilized skyrmions.

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