Issue |
J. Phys. I France
Volume 2, Number 12, December 1992
|
|
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Page(s) | 2299 - 2309 | |
DOI | https://doi.org/10.1051/jp1:1992282 |
J. Phys. I France 2 (1992) 2299-2309
Crossover from equilibrium to nonequilibrium dynamics in a reentrant AuFe ferromagnet
P. Mitchler, R. M. Roshko and W. RuanDepartment of Physics, University of Manitoba, Winnipeg, Manitoba, Canada R3T 2N2
(Received 26 May 1992, accepted in final form 11 August 1992)
Abstract
Measurements of the decay of the low field thermoremanent magnetization,
over four decades of observation time, 6 s
s, as a function
of temperature
T and wait time
, have been performed on two
AuFe alloys located on either side of the multicritical
point : a Au
90Fe
10 spin glass and a strongly bond-disordered
reentrant Au
83Fe
17 ferromagnet. The spin glass relaxation
isotherms exhibit the canonical symptoms of nonequilibrium ordering : below
, the isotherms are characterized by an inflection point,
on a logarithmic time perspective, which is sensitive to the wait time
, display a memory for a history of field reversals, and are
all compatible with an analytical representation based on a stretched
exponential function,
,
with
and a weakly temperature and wait time dependent
exponent
. The reentrant ferromagnet exhibits a temperature-driven
crossover between two distinct relaxation regimes : a "high temperature"
regime coincident with the ferromagnetic phase, characterized by an extremely
rapid approach to equilibrium, negligible wait time effects, and a weak power
law decay,
, with a weakly temperature dependent
exponent
, consistent with the predictions of droplet fluctuation
models of random Ising ferromagnets, and a "low temperature" regime coincident
with the reentrant phase, with nonequilibrium, age-dependent dynamics which are
virtually indistinguishable from those in the "pure" spin glass phase and describable
by the same stretched exponential relaxation function. This study represents
the first systematic comparison of relaxation dynamics in the reentrant and
ferromagnetic phases of a system with sequential transitions, and provides compelling
evidence for the equivalence of the reentrant and spin glass phases.
© Les Editions de Physique 1992