The Migdal-Kadanoff renormalization-group scheme is used to investigate chaotic behavior in the ordered phase of a three-dimensional Ising spin glass. The spin order is sensitive to a temperature change {δ}T at length scales L*{~}({Υ}/{σ}{δ}T)^1/ζ, where {Υ} and {σ} are temperature-dependent amplitudes associated with the interfacial free energy and entropy, respectively, {ζ}=dS/2-y is the Lyapunov exponent characterizing the chaotic behavior, dS is the fractal dimension of the interface, and -y is the scaling dimension of the temperature at the zero-temperature fixed point.
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Banavar et al. (1987) studied this question.
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