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- W2010150118 abstract "Arguments are given that, for random spin systems, the density of states ensuremath{rho}(ensuremath{mu}) of the inverse of the susceptibility matrix vanishes as ensuremath{rho}(ensuremath{mu})ensuremath{sim}exp(-A/ensuremath{mu}), for ensuremath{mu}ensuremath{rightarrow}0, throughout the ``Griffiths phase.'' The amplitude A vanishes at the onset of magnetic long-range order, and diverges at the transition between ``Griffiths'' and ``paramagnetic'' phases. For an O(m) spin system, with mensuremath{rightarrow}ensuremath{infty}, the spin autocorrelation function C(t) is found to have the ``stretched-exponential'' form, lnC(t)ensuremath{sim}-(At${)}^{1/2}$, in the Griffiths phase." @default.
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- W2010150118 date "1987-08-03" @default.
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- W2010150118 title "Nature of the Griffiths phase" @default.
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- W2010150118 doi "https://doi.org/10.1103/physrevlett.59.586" @default.
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