Abstract
We study the behaviour of a universal combination of susceptibility and correlation length in the Ising model in two and three dimensions, in presence of both magnetic and thermal perturbations, in the neighbourhood of the critical point. In three dimensions we address the problem using a parametric representation of the equation of state. In two dimensions we make use of the exact integrability of the model along the thermal and the magnetic axes. Our results can be used as a sort of "reference frame" to chart the critical region of the model. While our results can be applied in principle to any possible realization of the Ising universality class, we address in particular, as specific examples, three instances of Ising behaviour in finite temperature QCD related in various ways to the deconfinement transition. In particular, in the last of these examples, we study the critical ending point in the finite density, finite temperature phase diagram of QCD. In this finite density framework, due to well know sign problem, Montecarlo simulations are not possible and thus a direct comparison of experimental results with QFT/Statmech predictions like the one we discuss in this paper may be important. Moreover in this example it is particularly difficult to disentangle "magnetic-like" from "thermal-like" observables and thus universal quantities which do not need a precise identification of the magnetic and thermal axes, like the one we address in this paper, can be particularly useful.
Highlights
Despite its apparent simplicity the Ising model is one of the cornerstones of modern statistical mechanics
We study the behavior of a universal combination of susceptibility and correlation length in the Ising model in two and three dimensions, in presence of both magnetic and thermal perturbations, in the neighborhood of the critical point
In three dimensions we address the problem using a parametric representation of the equation of state
Summary
Despite its apparent simplicity the Ising model is one of the cornerstones of modern statistical mechanics. In three dimensions we shall address the problem using a parametric representation of the equation of state [8], while in two dimensions we shall make use of the exact integrability of the model in presence of a single perturbation [5] Using these tools we shall be able to predict the value of this quantity in the whole phase space of the model in the neighborhood of the critical point. In the last of these examples, we shall address the critical ending point of finite density QCD In this case, due to the well-known sign problem, Monte Carlo simulations are not possible and a direct comparison of experimental results with QFT/statistical mechanics predictions like the one we discuss in this paper may be important. We collected in the Appendices some additional material which may be useful to reproduce our numerical analysis
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