  A framework for relativistic thermodynamics and statistical physics is built
by first exploiting the symmetries between energy and momentum in the
derivation of the Boltzmann distribution, then using Einstein's energy-momentum
relationship to derive a PDE for the partition function. It is shown that the
extended Boltzmann distribution implies the existence of an inverse
four-temperature, while the form of the partition function PDE implies the
existence of a quantizable field theory of classical statistics, with hints of
an associated gravity like gauge theory. An adaptation of the framework is then
used to derive a thermodynamic certainty relationship.
