TY - JOUR
T1 - Anisotropic magnetoresistance effects in Fe, Co, Ni, Fe 4N, and half-metallic ferromagnet
T2 - A systematic analysis
AU - Kokado, Satoshi
AU - Tsunoda, Masakiyo
AU - Harigaya, Kikuo
AU - Sakuma, Akimasa
PY - 2012/2
Y1 - 2012/2
N2 - We theoretically analyze the anisotropic magnetoresistance (AMR) effects of bcc Fe (+), fcc Co (+), fcc Ni (+), Fe 4N (-), and a half-metallic ferromagnet (-). The sign in each parenthesis represents the sign of the AMR ratio observed experimentally. We here use the two-current model for a system consisting of a spin-polarized conduction state and localized d states with spin-orbit interaction. From the model, we first derive a general expression of the AMR ratio. The expression consists of a resistivity of the conduction state of the σ spin (σ = ↑ or ↓), ρ sσ, and resistivities due to s-d scattering processes from the conduction state to the localized d states. On the basis of this expression, we next find a relation between the sign of the AMR ratio and the s-d scattering process. In addition, we obtain expressions of the AMR ratios appropriate to the respective materials. Using the expressions, we evaluate their AMR ratios, where the expressions take into account the values of ρ s↑/ρ s↓ of the respective materials. The evaluated AMR ratios correspond well to the experimental results.
AB - We theoretically analyze the anisotropic magnetoresistance (AMR) effects of bcc Fe (+), fcc Co (+), fcc Ni (+), Fe 4N (-), and a half-metallic ferromagnet (-). The sign in each parenthesis represents the sign of the AMR ratio observed experimentally. We here use the two-current model for a system consisting of a spin-polarized conduction state and localized d states with spin-orbit interaction. From the model, we first derive a general expression of the AMR ratio. The expression consists of a resistivity of the conduction state of the σ spin (σ = ↑ or ↓), ρ sσ, and resistivities due to s-d scattering processes from the conduction state to the localized d states. On the basis of this expression, we next find a relation between the sign of the AMR ratio and the s-d scattering process. In addition, we obtain expressions of the AMR ratios appropriate to the respective materials. Using the expressions, we evaluate their AMR ratios, where the expressions take into account the values of ρ s↑/ρ s↓ of the respective materials. The evaluated AMR ratios correspond well to the experimental results.
KW - Anisotropic magnetoresistance effect
KW - Half-metallic ferromagnet
KW - S-d scattering
KW - Spin-orbit interaction
KW - Spin-polarized conduction electron
KW - Strong ferromagnet
KW - Two-current model
KW - Weak ferromagnet
UR - http://www.scopus.com/inward/record.url?scp=84856629878&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=84856629878&partnerID=8YFLogxK
U2 - 10.1143/JPSJ.81.024705
DO - 10.1143/JPSJ.81.024705
M3 - Article
AN - SCOPUS:84856629878
SN - 0031-9015
VL - 81
JO - Journal of the Physical Society of Japan
JF - Journal of the Physical Society of Japan
IS - 2
M1 - 024705
ER -