2017
DOI: 10.1103/physrevlett.118.157202
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Matching Microscopic and Macroscopic Responses in Glasses

Abstract: We first reproduce on the Janus and Janus II computers a milestone experiment that measures the spinglass coherence length through the lowering of free-energy barriers induced by the Zeeman effect. Secondly, we determine the scaling behavior that allows a quantitative analysis of a new experiment reported in the companion Letter [S. Guchhait and R. Orbach, Phys. Rev. Lett. 118, 157203 (2017)]. The value of the coherence length estimated through the analysis of microscopic correlation functions turns out to be … Show more

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Cited by 45 publications
(108 citation statements)
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“…where d f is the fractal dimension equal to d f = d − θ/2 (d = 3 is the space dimension, while θ is the socalled replicon exponent [19]). Because at the correlation lengths of interest θ ≈ 0.3, the approximation d f ≈ d made in previous work (Ref.…”
Section: Experimental Protocolmentioning
confidence: 99%
“…where d f is the fractal dimension equal to d f = d − θ/2 (d = 3 is the space dimension, while θ is the socalled replicon exponent [19]). Because at the correlation lengths of interest θ ≈ 0.3, the approximation d f ≈ d made in previous work (Ref.…”
Section: Experimental Protocolmentioning
confidence: 99%
“…As pointed out in Ref. 20 , the correlated space is in fact fractal, with a dimensionality exponent of ∼ 2.81 instead of 3. This has the effect of replacing L 3 in Eqs.…”
Section: V Analysis Of Experimental Resultsmentioning
confidence: 99%
“…By varying L, and measuring the coefficient of the H 2 reduction in ∆ max (H, L), one can uniquely detect the difference between compact and fractal growth through the measured exponent of L in Eq. (20). The relatively small value of the changes in ∆ max (H, L)/k B exhibited in Table I make this a somewhat daunting, but still possible task.…”
Section: V Analysis Of Experimental Resultsmentioning
confidence: 99%
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