Giant Anisotropy of Gilbert Damping in Epitaxial CoFe Films

Giant Anisotropy of Gilbert Damping in Epitaxial CoFe Films

Tailoring Gilbert damping of metallic ferromagnetic thin films is one of the central interests in spintronics applications. Here we report a giant Gilbert damping anisotropy in epitaxial Co_{50}Fe_{50} thin films with a maximum-minimum damping ratio of 400%, determined by broadband spin-torque ferro...

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Published in:Physical review letters Vol. 122; no. 11; p. 117203
Main Authors: Li, Yi, Zeng, Fanlong, Zhang, Steven S-L, Shin, Hyeondeok, Saglam, Hilal, Karakas, Vedat, Ozatay, Ozhan, Pearson, John E, Heinonen, Olle G, Wu, Yizheng, Hoffmann, Axel, Zhang, Wei
Format: Journal Article
Language:English
Published: United States American Physical Society 21-03-2019
American Physical Society (APS)
Subjects:
Anisotropy
Broadband
CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY
Cubic lattice
Damping ratio
Ferromagnetic materials
Ferromagnetic resonance
Magnetism
magnetization dynamics
Magnetoresistance
Magnetoresistivity
spin-orbit coupling
Spintronics
Thin films
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Abstract Tailoring Gilbert damping of metallic ferromagnetic thin films is one of the central interests in spintronics applications. Here we report a giant Gilbert damping anisotropy in epitaxial Co_{50}Fe_{50} thin films with a maximum-minimum damping ratio of 400%, determined by broadband spin-torque ferromagnetic resonance as well as inductive ferromagnetic resonance. We conclude that the origin of this damping anisotropy is the variation of the spin orbit coupling for different magnetization orientations in the cubic lattice, which is further corroborated from the magnitude of the anisotropic magnetoresistance in Co_{50}Fe_{50}.
AbstractList Tailoring Gilbert damping of metallic ferromagnetic thin films is one of the central interests in spintronics applications. Here we report a giant Gilbert damping anisotropy in epitaxial Co50Fe50 thin films with a maximum-minimum damping ratio of 400%, determined by broadband spin-torque ferromagnetic resonance as well as inductive ferromagnetic resonance. We conclude that the origin of this damping anisotropy is the variation of the spin orbit coupling for different magnetization orientations in the cubic lattice, which is further corroborated from the magnitude of the anisotropic magnetoresistance in Co50Fe50.
Tailoring Gilbert damping of metallic ferromagnetic thin films is one of the central interests in spintronics applications. We report a giant Gilbert damping anisotropy in epitaxial ${\mathrm{Co}}_{50}{\mathrm{Fe}}_{50}$ thin films with a maximum-minimum damping ratio of 400%, determined by broadband spin-torque ferromagnetic resonance as well as inductive ferromagnetic resonance. We conclude that the origin of this damping anisotropy is the variation of the spin orbit coupling for different magnetization orientations in the cubic lattice, which is further corroborated from the magnitude of the anisotropic magnetoresistance in ${\mathrm{Co}}_{50}{\mathrm{Fe}}_{50}$.
Tailoring Gilbert damping of metallic ferromagnetic thin films is one of the central interests in spintronics applications. Here we report a giant Gilbert damping anisotropy in epitaxial Co_{50}Fe_{50} thin films with a maximum-minimum damping ratio of 400%, determined by broadband spin-torque ferromagnetic resonance as well as inductive ferromagnetic resonance. We conclude that the origin of this damping anisotropy is the variation of the spin orbit coupling for different magnetization orientations in the cubic lattice, which is further corroborated from the magnitude of the anisotropic magnetoresistance in Co_{50}Fe_{50}.
ArticleNumber 117203
Author Zhang, Steven S-L
Ozatay, Ozhan
Shin, Hyeondeok
Zhang, Wei
Zeng, Fanlong
Heinonen, Olle G
Hoffmann, Axel
Li, Yi
Pearson, John E
Saglam, Hilal
Karakas, Vedat
Wu, Yizheng
Author_xml – sequence: 1
  givenname: Yi
  surname: Li
  fullname: Li, Yi
  organization: Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439, USA
– sequence: 2
  givenname: Fanlong
  surname: Zeng
  fullname: Zeng, Fanlong
  organization: State Key Laboratory of Surface Physics, Department of Physics, Fudan University, Shanghai 200433, China
– sequence: 3
  givenname: Steven S-L
  surname: Zhang
  fullname: Zhang, Steven S-L
  organization: Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439, USA
– sequence: 4
  givenname: Hyeondeok
  surname: Shin
  fullname: Shin, Hyeondeok
  organization: Computational Sciences Division, Argonne National Laboratory, Argonne, Illinois 60439, USA
– sequence: 5
  givenname: Hilal
  surname: Saglam
  fullname: Saglam, Hilal
  organization: Department of Physics, Illinois Institute of Technology, Chicago Illinois 60616, USA
– sequence: 6
  givenname: Vedat
  surname: Karakas
  fullname: Karakas, Vedat
  organization: Department of Physics, Bogazici University, Bebek 34342, Istanbul, Turkey
– sequence: 7
  givenname: Ozhan
  surname: Ozatay
  fullname: Ozatay, Ozhan
  organization: Department of Physics, Bogazici University, Bebek 34342, Istanbul, Turkey
– sequence: 8
  givenname: John E
  surname: Pearson
  fullname: Pearson, John E
  organization: Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439, USA
– sequence: 9
  givenname: Olle G
  surname: Heinonen
  fullname: Heinonen, Olle G
  organization: Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439, USA
– sequence: 10
  givenname: Yizheng
  surname: Wu
  fullname: Wu, Yizheng
  organization: Collaborative Innovation Center of Advanced Microstructures, Nanjing 210093, China
– sequence: 11
  givenname: Axel
  surname: Hoffmann
  fullname: Hoffmann, Axel
  organization: Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439, USA
– sequence: 12
  givenname: Wei
  surname: Zhang
  fullname: Zhang, Wei
  organization: Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439, USA
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Fudan Univ., Shanghai (China)
Argonne National Lab. (ANL), Argonne, IL (United States)
Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States)
Oakland Univ., Rochester, MI (United States)
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Snippet Tailoring Gilbert damping of metallic ferromagnetic thin films is one of the central interests in spintronics applications. Here we report a giant Gilbert...
Tailoring Gilbert damping of metallic ferromagnetic thin films is one of the central interests in spintronics applications. We report a giant Gilbert damping...
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StartPage 117203
SubjectTerms Anisotropy
Broadband
CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY
Cubic lattice
Damping ratio
Ferromagnetic materials
Ferromagnetic resonance
Magnetism
magnetization dynamics
Magnetoresistance
Magnetoresistivity
spin-orbit coupling
Spintronics
Thin films
Title Giant Anisotropy of Gilbert Damping in Epitaxial CoFe Films
URI https://www.ncbi.nlm.nih.gov/pubmed/30951326
https://www.proquest.com/docview/2207144066
https://search.proquest.com/docview/2204696192
https://www.osti.gov/servlets/purl/1505133
Volume 122
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