Abstract

We present the first experimental determination of the time autocorrelation C(t,t)C(t',t) of magnetization in the non-stationary regime of a spin glass. Quantitative comparison with the response, the magnetic susceptibility χ(t,t)\chi(t',t), is made using a new experimental setup allowing both measurements in the same conditions. Clearly, we observe a non-linear fluctuation-dissipation relation between CC and χ\chi, depending weakly on the waiting time tt'. Following theoretical developments on mean-field models, and lately on short range models, it is predicted that in the limit of long times, the χ(C)\chi(C) relationship should become independent on tt'. A scaling procedure allows us to extrapolate to the limit of long waiting times.Comment: 4 pages, 3 figure

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