Adiabatic spin-transfer-torque-induced domain wall creep in a magnetic metal

The creep motion of domain walls in magnetic metals can belong to different universality classes depending on whether they are driven by magnetic fields or spin-polarized currents. The dynamics of elastic interfaces is a general field of interest in statistical physics, where magnetic domain wall ha...

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Published inNature physics Vol. 12; no. 4; pp. 333 - 336
Main Authors DuttaGupta, S., Fukami, S., Zhang, C., Sato, H., Yamanouchi, M., Matsukura, F., Ohno, H.
Format Journal Article
LanguageEnglish
Published London Nature Publishing Group UK 01.04.2016
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Abstract The creep motion of domain walls in magnetic metals can belong to different universality classes depending on whether they are driven by magnetic fields or spin-polarized currents. The dynamics of elastic interfaces is a general field of interest in statistical physics, where magnetic domain wall has served as a prototypical example. Domain wall ‘creep’ under the action of sub-threshold driving forces with thermal activation is known to be described by a scaling law with a certain universality class 1 , 2 , 3 , 4 , 5 , 6 , 7 , 8 , 9 , 10 , which represents the mechanism of the interaction of domain walls with the applied forces over the disorder of the system. Here we show different universality classes depending on the driving forces, magnetic field or spin-polarized current, in a metallic system, which have hitherto been seen only in a magnetic semiconductor 3 , 6 . We reveal that an adiabatic spin-transfer torque plays a major role in determining the universality class of current-induced creep, which does not depend on the intricacies of material disorder. Our results shed light on the physics of the creep motion of domain walls and other elastic systems.
AbstractList The dynamics of elastic interfaces is a general field of interest in statistical physics, where magnetic domain wall has served as a prototypical example. Domain wall 'creep' under the action of sub-threshold driving forces with thermal activation is known to be described by a scaling law with a certain universality class1, 2, 3, 4, 5, 6, 7, 8, 9, 10, which represents the mechanism of the interaction of domain walls with the applied forces over the disorder of the system. Here we show different universality classes depending on the driving forces, magnetic field or spin-polarized current, in a metallic system, which have hitherto been seen only in a magnetic semiconductor3, 6. We reveal that an adiabatic spin-transfer torque plays a major role in determining the universality class of current-induced creep, which does not depend on the intricacies of material disorder. Our results shed light on the physics of the creep motion of domain walls and other elastic systems.
The creep motion of domain walls in magnetic metals can belong to different universality classes depending on whether they are driven by magnetic fields or spin-polarized currents. The dynamics of elastic interfaces is a general field of interest in statistical physics, where magnetic domain wall has served as a prototypical example. Domain wall ‘creep’ under the action of sub-threshold driving forces with thermal activation is known to be described by a scaling law with a certain universality class 1 , 2 , 3 , 4 , 5 , 6 , 7 , 8 , 9 , 10 , which represents the mechanism of the interaction of domain walls with the applied forces over the disorder of the system. Here we show different universality classes depending on the driving forces, magnetic field or spin-polarized current, in a metallic system, which have hitherto been seen only in a magnetic semiconductor 3 , 6 . We reveal that an adiabatic spin-transfer torque plays a major role in determining the universality class of current-induced creep, which does not depend on the intricacies of material disorder. Our results shed light on the physics of the creep motion of domain walls and other elastic systems.
The dynamics of elastic interfaces is a general field of interest in statistical physics, where magnetic domain wall has served as a prototypical example. Domain wall 'creep' under the action of sub-threshold driving forces with thermal activation is known to be described by a scaling law with a certain universality class, which represents the mechanism of the interaction of domain walls with the applied forces over the disorder of the system. Here we show different universality classes depending on the driving forces, magnetic field or spin-polarized current, in a metallic system, which have hitherto been seen only in a magnetic semiconductor. We reveal that an adiabatic spin-transfer torque plays a major role in determining the universality class of current-induced creep, which does not depend on the intricacies of material disorder. Our results shed light on the physics of the creep motion of domain walls and other elastic systems.
Author Zhang, C.
Fukami, S.
Sato, H.
DuttaGupta, S.
Yamanouchi, M.
Ohno, H.
Matsukura, F.
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  surname: Fukami
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  surname: Zhang
  fullname: Zhang, C.
  organization: Laboratory for Nanoelectronics and Spintronics, Research Institute of Electrical Communication, Tohoku University
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  email: ohno@riec.tohoku.ac.jp
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Snippet The creep motion of domain walls in magnetic metals can belong to different universality classes depending on whether they are driven by magnetic fields or...
The dynamics of elastic interfaces is a general field of interest in statistical physics, where magnetic domain wall has served as a prototypical example....
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SubjectTerms 639/766/119/1001
639/766/530/2803
639/925/357/997
Adiabatic flow
Atomic
Classical and Continuum Physics
Complex Systems
Condensed Matter Physics
Creep (materials)
Disorders
Domain walls
Elastic systems
letter
Magnetic domains
Magnetic fields
Magnetism
Mathematical and Computational Physics
Metals
Molecular
Optical and Plasma Physics
Physics
Statistics
Theoretical
Walls
Title Adiabatic spin-transfer-torque-induced domain wall creep in a magnetic metal
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