Abstract:We study dynamic fluctuations in non-disordered finite dimensional ferromagnetic systems quenched to the critical point and the low-temperature phase. We investigate the fluctuations of two two-time quantities, called χ and C, the averages of which yield the self linear response and correlation function. We introduce a restricted average of the χ's, summing over all configurations with a given value of C. We find that the restricted average χ C obeys a scaling form, and that the slope of the scaling function a… Show more
“…This mechanism makes lim tw →∞ lim t→∞ V C k=0 (t, t w ) = ∞, and in this sense the limit ( 22) is recovered, bearing in mind that ξ = ∞. Moreover, lim tw→∞ lim t→∞ V Cχ k=0 (t, t w )/V C k=0 (t, t w ), is a t w -independent constant as was found in [21]. We also observe that V Cχ k=0 going to a constant value is a different behavior with respect to the spherical model [22], where this quantity vanishes for t → ∞.…”
Section: Critical Quenchsupporting
confidence: 62%
“…(58) or Eq. (61)) this implies that the fluctuations χ and C cannot be constrained to follow the χ(C) curve, at least in this particular order of the large time limits, as already noticed in [21]. Hence the interpretation of [18,19] cannot be strictly obeyed.…”
“…For V C k=0 (∞) and V χ k=0 (∞) the same result holds true also below (but close to) T c , since the terms containing the magnetization in Eqs. (21) can be neglected. Interestingly, the behavior of V Cχ k=0 (∞), on the other hand, is discontinuous around the critical temperature: It vanishes identically for T > T c while it diverges as −(T c − T ) 2β−γ (where γ = (2 − η)ν and β are the usual critical exponents) on approaching T c from below.…”
We study the fluctuations of the autocorrelation and autoresponse functions and, in particular, their variances and co-variance. In a first general part of the Article, we show the equivalence of the variance of the response function with the second-order susceptibility of a composite operator, and we derive an equilibrium fluctuation-dissipation theorem beyond-linear order relating it to the other variances. In a second part of the paper we apply the formalism to the study to non-disordered ferromagnets, in equilibrium or in the coarsening kinetics following a critical or sub-critical quench. We show numerically that the variances and the non-linear susceptibility obey scaling with respect to the coherence length ξ in equilibrium, and with respect to the growing length L(t) after a quench, similarly to what is known for the autocorrelation and the autoresponse functions.
“…This mechanism makes lim tw →∞ lim t→∞ V C k=0 (t, t w ) = ∞, and in this sense the limit ( 22) is recovered, bearing in mind that ξ = ∞. Moreover, lim tw→∞ lim t→∞ V Cχ k=0 (t, t w )/V C k=0 (t, t w ), is a t w -independent constant as was found in [21]. We also observe that V Cχ k=0 going to a constant value is a different behavior with respect to the spherical model [22], where this quantity vanishes for t → ∞.…”
Section: Critical Quenchsupporting
confidence: 62%
“…(58) or Eq. (61)) this implies that the fluctuations χ and C cannot be constrained to follow the χ(C) curve, at least in this particular order of the large time limits, as already noticed in [21]. Hence the interpretation of [18,19] cannot be strictly obeyed.…”
“…For V C k=0 (∞) and V χ k=0 (∞) the same result holds true also below (but close to) T c , since the terms containing the magnetization in Eqs. (21) can be neglected. Interestingly, the behavior of V Cχ k=0 (∞), on the other hand, is discontinuous around the critical temperature: It vanishes identically for T > T c while it diverges as −(T c − T ) 2β−γ (where γ = (2 − η)ν and β are the usual critical exponents) on approaching T c from below.…”
We study the fluctuations of the autocorrelation and autoresponse functions and, in particular, their variances and co-variance. In a first general part of the Article, we show the equivalence of the variance of the response function with the second-order susceptibility of a composite operator, and we derive an equilibrium fluctuation-dissipation theorem beyond-linear order relating it to the other variances. In a second part of the paper we apply the formalism to the study to non-disordered ferromagnets, in equilibrium or in the coarsening kinetics following a critical or sub-critical quench. We show numerically that the variances and the non-linear susceptibility obey scaling with respect to the coherence length ξ in equilibrium, and with respect to the growing length L(t) after a quench, similarly to what is known for the autocorrelation and the autoresponse functions.
“…For a generic fluctuating observable X, besides the standard full average X = X we also introduce the restricted average X C = X C , namely an average taken only over the instances (realizations) with a given value C of the fluctuating autocorrelation, as suggested in [16]. Clearly one has…”
This article is a contribution to the understanding of fluctuations in the out of equilibrium dynamics of glassy systems. By extending theoretical ideas based on the assumption that timereparametrization invariance develops asymptotically we deduce the scaling properties of diverse high-order correlation functions. We examine these predictions with numerical tests in a standard glassy model, the 3d Edwards-Anderson spin-glass, and in a system where time-reparametrization invariance is not expected to hold, the 2d ferromagnetic Ising model, both at low temperatures. Our results enlighten a qualitative difference between the fluctuation properties of the two models and show that scaling properties conform to the time-reparametrization invariance scenario in the former but not in the latter.
“…In this context the theoretical study of perfect, i.e. nondisordered, models has been most fruitful, see, for example, [5,6,7,8,9,10,11,12,13,14,15,16,17,18,19,20,21,22].…”
Abstract. Using extensive Monte Carlo simulations we study aging properties of two disordered systems quenched below their critical point, namely the two-dimensional random-bond Ising model and the threedimensional Edwards-Anderson Ising spin glass with a bimodal distribution of the coupling constants. We study the two-times autocorrelation and space-time correlation functions and show that in both systems a simple aging scenario prevails in terms of the scaling variable L(t)/L(s), where L is the time-dependent correlation length, whereas s is the waiting time and t is the observation time. The investigation of the space-time correlation function for the random-bond Ising model allows us to address some issues related to superuniversality.
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.