1997
DOI: 10.1088/0305-4470/30/21/012
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Glassy behaviour and semi-local invariance in Ising model with four-spin interaction

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Cited by 59 publications
(130 citation statements)
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“…At T g the autocorrelation time is expected to diverge because of the onset of the slow dynamics which turns the stretched exponential behaviour into a power law (with a small exponent) or a logarithm. Although that result is in good agreement with previous simulations [9], [11] the method relying on the stretched exponential fit may prove to be too risky for an exact prediction of T g due to ambiguities in the fitting process and perhaps is not trustable to that accuracy. As an alternative and a cross check, for two different temperature values, namely T = 1.720 and T = 1.695 we show the behaviour of the C spin for two very different values of the waiting time, t w = 300, 2000.…”
Section: Introductionsupporting
confidence: 87%
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“…At T g the autocorrelation time is expected to diverge because of the onset of the slow dynamics which turns the stretched exponential behaviour into a power law (with a small exponent) or a logarithm. Although that result is in good agreement with previous simulations [9], [11] the method relying on the stretched exponential fit may prove to be too risky for an exact prediction of T g due to ambiguities in the fitting process and perhaps is not trustable to that accuracy. As an alternative and a cross check, for two different temperature values, namely T = 1.720 and T = 1.695 we show the behaviour of the C spin for two very different values of the waiting time, t w = 300, 2000.…”
Section: Introductionsupporting
confidence: 87%
“…It is well known that this model exhibits a first order phase transition at T c = 1.95 along with a dynamical transition at T g ∼ 1.7, which is the temperature where the glassy behaviour shows up [9], [10], [11]. Even though our main interest is the study of the glassy characteristics by looking at the relaxation as well as the autocorrelation of the order parameters (to be defined below) in the glassy phase, the region T g < T < T c is interesting as well.…”
Section: Introductionmentioning
confidence: 99%
“…3b). Similar trapping of the system in a metastable state was observed in the three-dimensional plaquette model [11]. Energetic barriers separating metastable states from one another and from the ground states are high: for p = 3, m = 1 the distribution of hyperedges obeys the power scaling law For p = 3, m = 2 the models with random and ferromagnetic initial conditions behave in a qualitatively similar way.…”
Section: Modelsupporting
confidence: 61%
“…In general, outside the field of disordered systems Ising models with multispin interactions have been less explored [6,7], both because such interactions are less common in real materials and also because in many cases such models display first-order transitions. These might be regarded as a priori less promising subjects for numerical investigation, although the general scaling theory for first-order transitions, initiated in [8][9][10] and developed further in [11][12][13][14][15] and [16][17][18][19], is now generally well-understood.…”
Section: Introductionmentioning
confidence: 99%
“…In the isotropic case we would expect m x abs = m y abs = m z abs and similarly for the squared quantities. Lipowski had previously suggested [6] using an order parameter akin to m sq in equation (31).…”
mentioning
confidence: 99%