Relaxational dynamics of the Edwards-Anderson model and the mean-field theory of spin-glasses

Langevin equations for the relaxation of spin fluctuations in a soft-spin version of the Edwards-Anderson model are used as a starting point for the study of the dynamic and static properties of spin-glasses. An exact uniform Lagrangian for the average dynamic correlation and response functions is derived for arbitrary range of random exchange, using a functional-integral method proposed by De Dominicis. The properties of the Lagrangian are studied in the mean-field limit which is realized by considering an infinite-ranged random exchange. In this limit, the dynamics are represented by a stochastic equation of motion of a single spin with self-consistent (bare) propagator and Gaussian noise. The low-frequency and the static properties of this equation are studied both above and below T₂. Approaching T₂ from above, spin fluctuations slow down with a relaxation time proportional to |T-{T₂|}^-1 whereas at T₂ the damping function vanishes as ^1{2}. We derive a criterion for dynamic stability below T₂. It is shown that a stable solution necessarily violates the fluctuation-dissipation theorem below T₂. Consequently, the spin-glass order parameters are the time-persistent terms which appear in both the spin correlations and the local response. This is shown to invalidate the treatment of the spin-glass order parameters as purely static quantities. Instead, one has to specify the manner in which they relax in a finite system, along time scales which diverge in the thermodynamic limit. We show that the finite-time correlations decay algebraically with time as t^- at all temperatures below T₂, with a temperature-dependent exponent. Near T₂, is given (in the Ising case) as (T) 12-^-1 (1-T{T₂}) + (1{-T{T₂}) }^2. A tentative calculation of at T=0 K is presented. We briefly discuss the physical origin of the violation of the fluctuation-dissipation theorem.