Critical two-point functions for long-range statistical-mechanical models in high dimensions

We consider long-range self-avoiding walk, percolation and the Ising model on ${\mathbb{Z}}^d$ that are defined by power-law decaying pair potentials of the form $D(x)\asymp \mathrm{\mid }x{\mathrm{\mid }}^{-d-\alpha }$ with $\alpha >0$. The upper-critical dimension $d_{\mathrm{c}}$ is $2(\alpha \wedge 2)$ for self-avoiding walk and the Ising model, and $3(\alpha \wedge 2)$ for percolation. Let $\alpha \mathrm{\ne }2$ and assume certain heat-kernel bounds on the $n$-step distribution of the underlying random walk. We prove that, for $d>d_{\mathrm{c}}$ (and the spread-out parameter sufficiently large), the critical two-point function $G_{p_{\mathrm{c}}}(x)$ for each model is asymptotically $C\mathrm{\mid }x{\mathrm{\mid }}^{\alpha \wedge 2-d}$, where the constant $C\in (0,\mathrm{\infty })$ is expressed in terms of the model-dependent lace-expansion coefficients and exhibits crossover between $\alpha <2$ and $\alpha >2$. We also provide a class of random walks that satisfy those heat-kernel bounds.