  We have computed finite temperature corrections to the electron-hadron
scattering cross sections. These are based upon the renormalized electron mass
and the modified density of states due to the presence of a background thermal
bath. It is found that the electron-hadron thermal transport scattering cross
section can be much larger than the zero temperature one. In the case of
electron-neutron transport scattering, we find \sigma_{ne}(T) / \sigma_{ne}
(T=0) \simeq 5 at T \simeq 0.1 MeV.
