The critical 1-arm exponent for the ferromagnetic Ising model on the Bethe lattice

TL;DR

This paper rigorously determines the critical 1-arm exponent for the ferromagnetic Ising model on Bethe lattices, showing the root magnetization decays as n^{-1/2} at criticality, revealing precise critical behavior.

Contribution

The paper provides a rigorous proof that the critical 1-arm exponent for the Ising model on regular trees is 1/2, a key quantitative characterization of critical decay.

Findings

Root magnetization decays as n^{-1/2} at criticality.

Establishes the critical 1-arm exponent as 1/2 for the Ising model on Bethe lattices.

Provides a sharp quantitative description of the decay rate of magnetization.

Abstract

We consider the ferromagnetic nearest-neighbor Ising model on regular trees (Bethe lattice), which is well-known to undergo a phase transition in the absence of an external magnetic field. The behavior of the model at critical temperature can be described in terms of various critical exponents; one of them is the critical 1-arm exponent $\rho$, which characterizes the rate of decay of the (root) magnetization. The crucial quantity we analyze in this work is the thermal expectation of the root spin on a finite subtree, where the expected value is taken with respect to a probability measure related to the corresponding finite-volume Hamiltonian with a fixed boundary condition. The spontaneous magnetization, which is the limit of this thermal expectation in the distance between the root and the boundary (i.e. in the height of the subtree), is known to vanish at criticality. We are interested in a quantitative analysis of the rate of this convergence in terms of the critical 1-arm exponent $\rho$. Therefore, we rigorously prove that $\langle\sigma_0\rangle^+_n$, the thermal expectation of the root spin at the critical temperature and in the presence of the positive boundary condition, decays as $\langle\sigma_0\rangle^+_n\approx n^{-1/2}$ (in a rather sharp sense), where $n$ is the height of the tree. This establishes the 1-arm critical exponent for the Ising model on regular trees ($\rho=1/2$).