Critical two-point function for long-range $O(n)$ models below the upper critical dimension

Abstract

We consider the $n$-component $|\phi {|}^4$ lattice spin model ($n\ge 1$) and the weakly self-avoiding walk ($n=0$) on ${\mathbb{Z}}^d$, in dimensions $d=1,2,3$. We study long-range models based on the fractional Laplacian, with spin-spin interactions or walk step probabilities decaying with distance $r$ as $r^{-(d+\alpha )}$ with $\alpha \in (0,2)$. The upper critical dimension is $d_c=2\alpha$. For $\epsilon >0$, and $\alpha =\frac{1}{2}(d+\epsilon )$, the dimension $d=d_c-\epsilon$ is below the upper critical dimension. For small $\epsilon$, weak coupling, and all integers $n\ge 0$, we prove that the two-point function at the critical point decays with distance as $r^{-(d-\alpha )}$. This "sticking" of the critical exponent at its mean-field value was first predicted in the physics literature in 1972. Our proof is based on a rigorous renormalisation group method. The treatment of observables differs from that used in recent work on the nearest-neighbour 4-dimensional case, via our use of a cluster expansion.

arXiv comment32 pages

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