“…The PL can be modeled via a generalized Planck radiation law 30,31 :where, is the emitted photon energy, A is the absorptivity, Δ μ is the chemical potential or quasi-Fermi-level separation under laser excitation, and T C represents the non-equilibrium hot carrier temperature. In the simplest case, taking a linear fit to the high-energy tail of the natural logarithm of a PL spectrum determines the carrier temperature 14,15,24,25,32 . However, such an analysis can be problematic in the case of QWs, where higher carrier excitation (increased laser excitation) and/or increased temperature results in the redistribution and thermal occupation of carriers in the higher energy subbands of the QW 31,33 .…”