Abstract
It is proposed that the spin-glass phase is described by two order parameters q(x)=[Si(0)Si(tx)]a v and χ(x)=0txχ(t) dt, that measure the relaxations of the average autocorrelation and susceptibility along macroscopic time scales, tx, which are parametrized in a decreasing order by x[0,1]. The function q decays from a finite value at t1 to zero at t0, while χ increases from χ(1) to a value χ(0) which is independent of temperature in the mean-field limit. The equilibrium results agree with Parisi's replica solution.
| Original language | English |
|---|---|
| Pages (from-to) | 935-938 |
| Number of pages | 4 |
| Journal | Physical Review Letters |
| Volume | 47 |
| Issue number | 13 |
| DOIs | |
| State | Published - 1981 |
| Externally published | Yes |
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