Abstract

We study the free-induction decay and the spin-echo attenuation at long times for spins diffusing in a random magnetic field. We show that the decay of transverse magnetization in a Gaussian random longitudinal field is asymptotically M(t)\ensuremath{\sim}${\mathit{t}}^{\ensuremath{\gamma}\mathrm{\ensuremath{-}}1}$${\mathit{e}}^{\mathrm{\ensuremath{-}}\mathit{t}/\mathrm{\ensuremath{\tau}}}$, where \ensuremath{\gamma} is the exponent of a self-avoiding walk. The usual result given by a cumulant expansion fails due to correlations arising from multiple self-intersections in d\ensuremath{\le}4. Experimental relevance of our analysis is discussed along with the question of universality and the existence of large fluctuations in finite-size systems.

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