Scaling functions in the square Ising model

preprint2014arXivOpen access

Abstract

We show and give the linear differential operators Lqscal{\cal L}^{scal}_q of order q= n^2/4+n+7/8+(-1)^n/8, for the integrals In(r)I_n(r) which appear in the two-point correlation scaling function of Ising model F±(r)=lim⁡scalingM±−2<σ0,0 σM,N>=∑nIn(r) F_{\pm}(r)= \lim_{scaling} {\cal M}_{\pm}^{-2} < σ_{0,0} \, σ_{M,N}> = \sum_{n} I_{n}(r). The integrals In(r) I_{n}(r) are given in expansion around r= 0 in the basis of the formal solutions of  Lqscal\, {\cal L}^{scal}_q with transcendental combination coefficients. We find that the expression r1/4 exp⁡(r2/8) r^{1/4}\,\exp(r^2/8) is a solution of the Painlevé VI equation in the scaling limit. Combinations of the (analytic at r=0 r= 0) solutions of Lqscal {\cal L}^{scal}_q sum to exp⁡(r2/8) \exp(r^2/8). We show that the expression r1/4exp⁡(r2/8) r^{1/4} \exp(r^2/8) is the scaling limit of the correlation function C(N,N) C(N, N) and C(N,N+1) C(N, N+1). The differential Galois groups of the factors occurring in the operators Lqscal {\cal L}^{scal}_q are given.

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