The Ising model on $\mathbb{Z}^2$ is given by the Hamiltonian $$ H(\sigma)=-\sum_{\{x,y\}}\sigma_x\sigma_y $$ and the Gibbs measure as $$ \frac{\exp(-\beta H(\sigma))}{Z_\beta}\,. $$
There exists an exact solution found by Onsager and re-derived later on by others. My question is:
On Wikipedia there are explicit expressions for internal energy per site and the spontaneous magnetization (below the critical temperature). Are there any explicit formulas for the infinite-volume two point function $$ \mathbb{E}_\beta[\sigma_x\sigma_y]$$ below, at and above the critical temperature $$ \beta_c = \frac{1}{2}\log(1+\sqrt{2})?$$
In case the explicit expressions are too complicated (or too complicated to make conclusions from), I would just like to verify a few things: Above the critical temperature we have exponential decay with respect to $\|x-y\|$. Below it we have long range order and hence $$ \mathbb{E}_\beta[\sigma_x\sigma_y] \geq C \qquad(\beta>\beta_c)\,. $$ What is this constant and is it temperature dependent? Clearly it shouldn't be larger than 1. Moreover, at the critical temperature, it seems like there should be polynomial behavior $$ \mathbb{E}_{\beta_c}[\sigma_x\sigma_y] \approx \|x-y\|^{-1/{2\pi\beta_c}} \approx \|x-y\|^{-0.361152}\,. $$ Is this correct? Is there another expression?