“…The integrated intensity of the NBE emission of ZnO/ZnMgO MQWs with L w = 1.6, 2.7, and 5.6 nm as a function of inverse temperature are given in Figure S5a. The temperature-dependent integrated PL intensity can be described as the Arrhenius expression: ,, where I 0 is the integrated intensity at 0 K, k b is Boltzmann’s constant, E b1 and E b2 are the active energies, and A and B are the corresponding constants. We found E b1 was about 5 meV and might correspond to the energy of exciton bound to a neutral donor or localization potential due to alloy fluctuation or well width variation; E b2 responsible for the high-temperature part of I ( T ) are 41, 60, and 73 meV for L w = 5.6, 2.7, and 1.6 nm samples, respectively, which correspond to the exciton binding energy in the quantum wells.…”