Excess velocity of magnetic domain walls close to the depinning field

Magnetic field driven domain wall velocities in [Co/Ni] based multilayers thin films have been measured using polar magneto-optic Kerr effect microscopy. The low field results are shown to be consistent with the universal creep regime of domain wall motion, characterized by a stretched exponential g...

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Detalles Bibliográficos
Autores: Caballero, Nirvana Belén, Fernández Aguirre, Iván, Albornoz, Lucas Javier, Kolton, Alejandro Benedykt, Rojas Sanchez, Juan Carlos, Collin, Sophie, George, Jean Marie, Diaz Pardo, Rebeca, Jeudy, Vincent, Bustingorry, Sebastián, Curiale, Carlos Javier
Tipo de recurso: artículo
Estado:Versión publicada
Fecha de publicación:2017
País:Argentina
Institución:Consejo Nacional de Investigaciones Científicas y Técnicas
Repositorio:CONICET Digital (CONICET)
Idioma:inglés
OAI Identifier:oai:ri.conicet.gov.ar:11336/68304
Acceso en línea:http://hdl.handle.net/11336/68304
Access Level:acceso abierto
Palabra clave:NANOMAGNETISM
MULTILAYERS
DOMAIN WALL
https://purl.org/becyt/ford/1.3
https://purl.org/becyt/ford/1
https://purl.org/becyt/ford/2.10
https://purl.org/becyt/ford/2
Descripción
Sumario:Magnetic field driven domain wall velocities in [Co/Ni] based multilayers thin films have been measured using polar magneto-optic Kerr effect microscopy. The low field results are shown to be consistent with the universal creep regime of domain wall motion, characterized by a stretched exponential growth of the velocity with the inverse of the applied field. Approaching the depinning field from below results in an unexpected excess velocity with respect to the creep law. We analyze these results using scaling theory to show that this speeding up of domain wall motion can be interpreted as due to the increase of the size of the deterministic relaxation close to the depinning transition. We propose a phenomenological model to accurately fit the observed excess velocity and to obtain characteristic values for the depinning field Hd, the depinning temperature Td, and the characteristic velocity scale v0 for each sample.