“…Initially, the electron and hole distributions will be non-thermal but carrier-carrier scattering [5,6,7] will result in a thermal (Fermi-Dirac) distribution of electrons and of the holes in much less than 100 fs, the time-scale of phonon motion. However, electron-hole recombination, resulting in a common chemical potential for electrons and holes, occurs on a time-scale of approximately 1 ns, which is much longer than the phonon period.…”