Low-temperature magnetic viscosity in the re-entrant ferromagnet (Fe 0.68Mn0.32)75P16B6Al 3

Y. Yeshurun; M. B. Salamon

doi:10.1088/0022-3719/14/20/003

Low-temperature magnetic viscosity in the re-entrant ferromagnet (Fe _0.68Mn_0.32)₇₅P₁₆B₆Al ₃

Y. Yeshurun, M. B. Salamon

University of Illinois at Urbana-Champaign

Research output: Contribution to journal › Article › peer-review

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Abstract

Studies of magnetic viscosity in (Fe_0.68Mn_0.32) ₇₅P₁₆B₆Al₃ are presented. The magnetisation in a constant field H is described by M=M₁+S ln t. The coefficient S(T) peaks at T_m(H). The authors show that s and the susceptibility chi scale similarly and deduce the ferromagnetic/spin glass transition temperature T_fg approximately=35K, in agreement with their previous results.

Original language	English
Article number	003
Pages (from-to)	L575-L580
Journal	Journal of Physics C: Solid State Physics
Volume	14
Issue number	20
DOIs	https://doi.org/10.1088/0022-3719/14/20/003
State	Published - 1981
Externally published	Yes

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title = "Low-temperature magnetic viscosity in the re-entrant ferromagnet (Fe 0.68Mn0.32)75P16B6Al 3",

abstract = "Studies of magnetic viscosity in (Fe0.68Mn0.32) 75P16B6Al3 are presented. The magnetisation in a constant field H is described by M=M1+S ln t. The coefficient S(T) peaks at Tm(H). The authors show that s and the susceptibility chi scale similarly and deduce the ferromagnetic/spin glass transition temperature Tfg approximately=35K, in agreement with their previous results.",

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AU - Yeshurun, Y.

AU - Salamon, M. B.

PY - 1981

Y1 - 1981

N2 - Studies of magnetic viscosity in (Fe0.68Mn0.32) 75P16B6Al3 are presented. The magnetisation in a constant field H is described by M=M1+S ln t. The coefficient S(T) peaks at Tm(H). The authors show that s and the susceptibility chi scale similarly and deduce the ferromagnetic/spin glass transition temperature Tfg approximately=35K, in agreement with their previous results.

AB - Studies of magnetic viscosity in (Fe0.68Mn0.32) 75P16B6Al3 are presented. The magnetisation in a constant field H is described by M=M1+S ln t. The coefficient S(T) peaks at Tm(H). The authors show that s and the susceptibility chi scale similarly and deduce the ferromagnetic/spin glass transition temperature Tfg approximately=35K, in agreement with their previous results.

UR - https://www.scopus.com/pages/publications/36149046731

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Low-temperature magnetic viscosity in the re-entrant ferromagnet (Fe _0.68Mn_0.32)₇₅P₁₆B₆Al ₃

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