  We fit finite-temperature path integral Monte Carlo calculations of the
exchange-correlation energy of the 3D finite-temperature homogeneous electron
gas in the warm-dense regime (r_{s} = (3/4\pi n)^{1/3} a_{B}^{-1} < 40 and
\Theta = T/T_{F} > 0.0625). In doing so, we construct a Pad\'{e} approximant
which collapses to Debye-H\"{u}ckel theory in the high-temperature, low-density
limit. Likewise, the zero-temperature limit matches the numerical results of
ground-state quantum Monte Carlo, as well as analytical results in the
high-density limit.
