On the origin of power-laws in equilibrium

A particle in the attractive Coulomb field has an interesting property: its specific heat is constant and negative. We show, both analytically and numerically, that when a classical Hamiltonian system stays in weak contact with one such negative specific heat object, its statistics conforms to a fat-tailed power-law distribution with power index given by $C\mathrm{/}{k}_B-1$, where $k_B$ is Boltzmann constant and $C$ is the heat capacity.