“…22, the E a obtained from temperature-dependent PL experiments cannot be directly compared to the electron and hole confinement energies. When aiming at describing the thermal escape of carriers from a QW, one needs to account for (i) the ionization of excitonic complexes into electron-hole pairs, 10,23) (ii) the difference in density of states between the (Al,Ga)N barriers and the GaN QW (three and two dimensional, respectively), 10) (iii) B and C excitons, as well as the excited states of the three exciton branches 22) and (iv) the disorder in both the QW plane and the (Al,Ga)N barriers. 10,23) As expected, we manage to fit the temperature dependence of PL for the different excitation spots keeping a constant E a , which we find equal to 43 meV (Fig.…”