TY - JOUR

T1 - Correction to

T2 - Anisotropic magnetoresistance effect of a strong ferromagnet: magnetization direction dependence in a model with crystal field: Anisotropic magnetoresistance effect of a strong ferromagnet: magnetization direction dependence in a model with crystal field (physica status solidi (c), (2014), 11, 5-6, (1026-1032), 10.1002/pssc.201300736)

AU - Kokado, Satoshi

AU - Tsunoda, Masakiyo

N1 - Publisher Copyright:
© 2017 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim

PY - 2017/9

Y1 - 2017/9

N2 - We give a correct expression for C4 in the above paper. To be more precise, we should delete the higher-order (HO) term with (λ/δg)2 in C4. This HO term was finally ignored because of its small value in the paper. The correction therefore does not change the main results of the paper. For C4 of Eq. (29), we should delete the (λ/δg)2 term. Namely, the correct expression of C4 of Eq. (29) is given as (Formula presented.) In accordance with the revision of C4, we should delete a sentence which starts from 5th line from top in the right side of p. 1029, i.e., “Note that, from now on, we ignore the second term of the right-hand side of C4, i.e., (3/32) (λ/δg)2[(λ/∆) - λ/(|Hex| + ∆)]2, because this term is considered to be sufficiently smaller than the first term with only (λ/∆)2 and [λ/(|Hex| - ∆)]2 due to δg > |λ|.”.

AB - We give a correct expression for C4 in the above paper. To be more precise, we should delete the higher-order (HO) term with (λ/δg)2 in C4. This HO term was finally ignored because of its small value in the paper. The correction therefore does not change the main results of the paper. For C4 of Eq. (29), we should delete the (λ/δg)2 term. Namely, the correct expression of C4 of Eq. (29) is given as (Formula presented.) In accordance with the revision of C4, we should delete a sentence which starts from 5th line from top in the right side of p. 1029, i.e., “Note that, from now on, we ignore the second term of the right-hand side of C4, i.e., (3/32) (λ/δg)2[(λ/∆) - λ/(|Hex| + ∆)]2, because this term is considered to be sufficiently smaller than the first term with only (λ/∆)2 and [λ/(|Hex| - ∆)]2 due to δg > |λ|.”.

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U2 - 10.1002/pssc.201700218

DO - 10.1002/pssc.201700218

M3 - Comment/debate

AN - SCOPUS:85029368828

SN - 1862-6351

VL - 14

JO - Physica Status Solidi (C) Current Topics in Solid State Physics

JF - Physica Status Solidi (C) Current Topics in Solid State Physics

IS - 9

M1 - 1700218

ER -