Abstract
For the first time, the frequency dependence of T f (temperature of the maximum of the a.c. susceptibility of spin-glasses) is shown to obey a Fulcher law τ = τ o exp [ E a k( T f − T f ) ] . This is observed as well in the case of dilute alloys (or R.K.K.Y. spin-glasses : Cu Mn, Au Fe, …) as for frustrated systems (Eu 1−xGd xS, Eu xSr 1−xS …). For R.K.K.Y. spin-glasses, only in the case of a very small amplitude, V o of the R.K.K.Y. interaction, this time dependence approaches an Arrhenius law. In the case of “frustrated” spin-glasses the concentration is the main parameter to determine the kind of frequency dependence of T f. These properties are evidence for a glass-like phase transition in spin-glasses. The scaling of the frequency dependence of T f with V o is justified for R.K.K.Y. spin-glasses from present data.
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