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Indeed, if we take ε=2, then for T≳0.6 notable finite-time corrections to simple aging are seen, which may be accounted for by including a finite-time correction term (Refs.). C (t,s) = FC (t/s) - s- b′ GC (t/s) and a new correction exponent b′ >0.
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Indeed, if we take ε=2, then for T≳0.6 notable finite-time corrections to simple aging are seen, which may be accounted for by including a finite-time correction term (Refs.). C (t,s) = FC (t/s) - s- b′ GC (t/s) and a new correction exponent b′ >0.
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If one uses a scaling form C (t,s) =C [(t-s) s-μ], it can be shown that the superaging case μ>1 is incompatible with basic requirements from probability theory.
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If one uses a scaling form C (t,s) =C [(t-s) s-μ], it can be shown that the superaging case μ>1 is incompatible with basic requirements from probability theory.
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The consideration of the spatiotemporal response allows for a much more demanding test of dynamical scaling than is possible by merely considering the autoresponse alone. Our results hence strengthen the conclusions of a simple power-law scaling in the disordered Ising model reached earlier (Refs.).
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The consideration of the spatiotemporal response allows for a much more demanding test of dynamical scaling than is possible by merely considering the autoresponse alone. Our results hence strengthen the conclusions of a simple power-law scaling in the disordered Ising model reached earlier (Refs.).
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It is conceivable that our finding of a distinct behavior for ε=2 might be a sort of borderline behavior when going from ferromagnets to frustrated magnet.
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It is conceivable that our finding of a distinct behavior for ε=2 might be a sort of borderline behavior when going from ferromagnets to frustrated magnet.
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