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[Abstract only; full report, Armor Research Foundation Project No. A059, Supplementary Report, May 1, 1956];
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Identification of the dominant precession-damping mechanism in Fe, Co, and Ni by first-principles calculations
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K. Gilmore, Y. U. Idzerda, and M. D. Stiles, Phys. Rev. Lett. 0031-9007 10.1103/PhysRevLett.99.027204 99, 027204 (2007); (Pubitemid 47152995)
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Spin-orbit precession damping in transition metal ferromagnets (invited)
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K. Gilmore, Y. U. Idzerda, and M. D. Stiles, J. Appl. Phys. JAPIAU 0021-8979 10.1063/1.2832348 103, 07D303 (2008). (Pubitemid 351538371)
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K. Gilmore, M. D. Stiles, J. Seib, D. Steiauf, and M. Fähnle, Phys. Rev. B PRBMDO 1098-0121 10.1103/PhysRevB.81.174414 81, 174414 (2010).
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Phys. Rev. B e-print arXiv: 1104.1625v1 (to be published).
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A. A. Starikov, P. J. Kelly, A. Brataas, Y. Tserkovnyak, and G. E. W. Bauer, Phys. Rev. Lett. PRLTAO 0031-9007 10.1103/PhysRevLett.105.236601 105, 236601 (2010).
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79961219058
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In the scattering formulation, the energy loss due to Gilbert damping is related to the energy pumped into leads by the precessing magnetization. The frequency corresponding to typical Fermi velocities in metals is ~1016 Hz. Typical ferromagnetic resonance measurements from which the Gilbert damping constant is extracted are carried out at frequencies ~1010 Hz so that transport electrons see essentially frozen spins. Spin-wave (~1013 Hz) and phonon frequencies (~1012 Hz) are also much lower than the electronic frequencies, justifying the use of a frozen phonon approach.
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In the scattering formulation, the energy loss due to Gilbert damping is related to the energy pumped into leads by the precessing magnetization. The frequency corresponding to typical Fermi velocities in metals is ~ 10 16 Hz. Typical ferromagnetic resonance measurements from which the Gilbert damping constant is extracted are carried out at frequencies ~ 10 10 Hz so that transport electrons see essentially frozen spins. Spin-wave (~ 10 13 Hz) and phonon frequencies (~ 10 12 Hz) are also much lower than the electronic frequencies, justifying the use of a frozen phonon approach.
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23
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79961227881
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A similar scheme has been developed in the framework of linear response theory, implemented using the fully relativistic Korringa-Kohn-Rostoker method in combination with the coherent potential approximation, and applied to Ni by H. Ebert, S. Mankovsky, D. Ködderitzsch, and P. J. Kelly, Phys. Rev. Lett. e-print arXiv: 1102.4551v1 (to be published)
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A similar scheme has been developed in the framework of linear response theory, implemented using the fully relativistic Korringa-Kohn-Rostoker method in combination with the coherent potential approximation, and applied to Ni by H. Ebert, S. Mankovsky, D. Ködderitzsch, and P. J. Kelly, Phys. Rev. Lett. e-print arXiv: 1102.4551v1 (to be published)
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79961217627
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Ni=3.524 is used. In both cases, the fcc Cu leads are slightly stretched to match.
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Ni=3.524 is used. In both cases, the fcc Cu leads are slightly stretched to match.
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30
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79961232027
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The areas of the primitive 2D BZs for Co and Ni are almost identical and more than twice as large as that for Fe. Therefore the k-point sampling densities in the transport calculations for all three systems are very similar.
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The areas of the primitive 2D BZs for Co and Ni are almost identical and more than twice as large as that for Fe. Therefore the k -point sampling densities in the transport calculations for all three systems are very similar.
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Resistivity-like and conductivity-like regimes are determined by whether additional disorder increases or decreases the damping.
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Resistivity-like and conductivity-like regimes are determined by whether additional disorder increases or decreases the damping.
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