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Universal critical exponents of the magnetic domain wall depinning transition

L. J. Albornoz1,2,3, E. E. Ferrero1, A. B. Kolton3,4, V. Jeudy2, S. Bustingorry1, and J. Curiale1,3,*

  • 1Instituto de Nanociencia y Nanotecnología, CNEA–CONICET, Centro Atómico Bariloche, Avenida E. Bustillo 9500 (R8402AGP), San Carlos de Bariloche, Río Negro, Argentina
  • 2Université Paris-Saclay, CNRS, Laboratoire de Physique des Solides, 91405 Orsay, France
  • 3Instituto Balseiro, Universidad Nacional de Cuyo–CNEA, Centro Atómico Bariloche, Avenida E. Bustillo 9500 (R8402AGP), San Carlos de Bariloche, Río Negro, Argentina
  • 4Centro Atómico Bariloche, Comisión Nacional de Energía Atómica (CNEA), Consejo Nacional de Investigaciones Científicas y Técnicas (CONICET), Avenida E. Bustillo 9500 (R8402AGP), San Carlos de Bariloche, Río Negro, Argentina

  • *curiale@cab.cnea.gov.ar, he/him/his

Phys. Rev. B 104, L060404 – Published 5 August, 2021

DOI: https://doi.org/10.1103/PhysRevB.104.L060404

Abstract

Magnetic-field-driven domain wall dynamics in a ferrimagnetic GdFeCo thin film with perpendicular magnetic anisotropy is studied using low-temperature magneto-optical Kerr microscopy. Measurements performed in a practically athermal condition allow for the direct experimental determination of the velocity (β=0.30±0.03) and correlation length (ν=1.3±0.3) exponents of the depinning transition. The whole family of exponents characterizing the transition is deduced, providing evidence that the depinning of magnetic domain walls is better described by the quenched Edwards-Wilkinson universality class.

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