Exponential Decay of Truncated Correlations for the Ising Model in any Dimension for all but the Critical Temperature (original) (raw)

Exponential Decay for the Near‐Critical Scaling Limit of the Planar Ising Model

Communications on Pure and Applied Mathematics

We consider the Ising model at its critical temperature with external magnetic field ha 15/8 on the square lattice with lattice spacing a. We show that the truncated two-point function in this model decays exponentially with a rate independent of a. As a consequence, we show exponential decay in the near-critical scaling limit Euclidean magnetization field. For the lattice model with a = 1, the mass (inverse correlation length) is of order h 8/15 as h ↓ 0; for the Euclidean field, it equals exactly Ch 8/15 for some C. Although there has been much progress in the study of critical scaling limits, results on near-critical models are far fewer due to the lack of conformal invariance away from the critical point. Our arguments combine lattice and continuum FK representations, including coupled conformal loop and measure ensembles, showing that such ensembles can be useful even in the study of near-critical scaling limits. Thus we provide the first substantial application of measure ensembles.

A Note on Exponential Decay in the Random Field Ising Model

Journal of Statistical Physics

For the two-dimensional random field Ising model (RFIM) with bimodal (i.e., two-valued) external field, we prove exponential decay of correlations either (i) when the temperature is larger than the critical temperature of the Ising model without external field and the magnetic field strength is small or (ii) at any temperature when the magnetic field strength is sufficiently large. Unlike previous work on exponential decay, our approach is not based on cluster expansions but rather on arguably simpler methods; these combine an analysis of the Kertész line and a coupling of Ising measures (and also their random cluster representations) with different boundary conditions. We also show similar but weaker results for the RFIM with a general field distribution and in any dimension.

Exponential Decay of Correlations in the 2D Random Field Ising Model

Journal of Statistical Physics, 2019

An extension of the Ising spin configurations to continuous functions is used for an exact representation of the Random Field Ising Model's order parameter in terms of disagreement percolation. This facilitates an extension of the recent analyses of the decay of correlations to positive temperatures, at homogeneous but arbitrarily weak disorder.

On the critical behavior of the magnetization in high-dimensional Ising models

Journal of Statistical Physics, 1986

Long-range components of the interaction in statistical mechanical systems may affect the critical behavior, raising the system's 'effective dimension'. Presented here are explicit implications to this effect of a collection of rigorous results on the critical exponents in ferromagnetic models with one-component lsing (and more generally Griffiths-Simon class) spin variables. In particular, it is established that even in dimensions d < 4 if a ferromagnetic Ising spin model has a reflection-positive pair interaction with a sufficiently slow decay, e.g. as Jx = 1/Ixl a+~ with 0 < a~< d/2, then the exponents ~, 6, ? and A 4 exist and take their mean-field values. This proves rigorously an early renormalization-group prediction of Fisher, Ma and Nickel. In the converse direction: when the decay is by a similar power law with try> 2, then the long-range part of the interaction has no effect on the existent critical exponent bounds, which coincide then with those obtained for short-range models.

A note on the Ising model in high dimensions

Communications in Mathematical Physics, 1989

We consider thed-dimensional Ising model with a nearest neighbor ferromagnetic interactionJ(d)=1/4d. We show that asd→∞ the+phase (and the — phase) approaches a product measure with density given by the mean field approximation. In particular the spontaneous magnetization converges to its mean field value. A similar result holds for the unique Gibbs measure of the system subject to an external fieldh≠0.

Intermittency and correlation functions in the Ising model in two dimensions

Nuclear Physics B - Proceedings Supplements, 1989

We present results of the study of the factorial moments in the two-dimensional ]sing model. We have related their intermittent behaviour to the short distance singularity of the correlation functions. Analogies and differences with the similar phenomenon in the multiparticle production are discussed. Possible application to study the finite temperature gauge theory is also outlined.

Asymptotics of decay of correlations for lattice spin fields at high temperatures. I. The Ising model

Journal of Statistical Physics, 1996

We find the asymptotic decrease of correlations (aA +y, aB), y 9 Z" + t l Yl ~ oo, in the Ising model at high temperatures. For the case when monomials an and a n both are odd, using the saddle-point method, we find the asymptotics of the correlations for any dimension v. For even monomials aA, an we formulate a general hypothesis about the form of the asymptotics and confirm it in two cases: (1) v= 1 and the vector y has an arbitrary direction, (2) y is directed along a fixed axis and arbitrary v. Here we use besides the saddle-point method, some arguments from scattering theory.

Correlation matrices at the phase transition of the Ising model

We study spectral densities for systems on lattices, which, at a phase transition display, power-law spatial correlations. Constructing the spatial correlation matrix we prove that its eigenvalue density shows a power law that can be derived from the spatial correlations. In practice time series are short in the sense that they are either not stationary over long time intervals or that they are not available over long time intervals. Also we usually do not have time series for all variables available. We shall make numerical simulations on a 2-D Ising model with the usual Metropolis algorithm as time-evolution. Using all spins on a grid with periodic boundary conditions we find a power law, that is, for large grids, compatible with the analytic result. We still find a power law even if we choose a fairly small subset of grid points at random. The exponents of the power laws will be smaller under such circumstances. For very short time series leading to singular correlation matrices we use a recently developed technique to lift the degeneracy at zero in the spectrum and find a significant signature of critical behavior even in this case as compared to high temperature results which tend to those of random matrix models.