We report for the first time the temperature dependent PL spectra from GaInNAs/GaAs triple quantum wells, modulation doped with a 2-D carrier density of ~3x10 11 cm -2 per well. The measurements were carried out at temperatures between 10 and 300K. The results are analyzed using a Gaussian fitting technique which indicates variable nitrogen composition and/or well-width fluctuations in the wells. One of the most striking features of the results is the lack of the S-Shape temperature dependence of the PL peak energy that is commonly observed in undoped dilute nitride quantum wells and is attributed to exciton detrapping, which screens the true temperature dependence of the energy gap. Our results compare well with the predictions of the Varshni equation. The temperature dependence of the PL intensity is used to obtain the thermally activated behaviour of the non-radiative recombination processes that appear to dominate at higher temperatures. 1 Introduction Recent developments in communication technology have been stimulating an increasing demand on fast data transmission and high capacity devices operating in this area. Current devices are far from meeting the growing demand. Hence, an enormous research effort has been devoted for the development of alternative materials particularly for the 1.3 µm window of the optical-fiber communications. GaInNAs alloy is one such material system where increased nitrogen incorporation results in large band gap bowing and hence reduced band gap. However, too high a concentration of nitrogen tends to degrade the optical quality of the material [1]. Optical properties of GaInNAs alloy can be partly improved by having a tight control over the growth conditions [2], rapid thermal annealing [3] or using multiple quantum wells [4]. In undoped quantum wells temperature dependent photoluminescence has the typical exciton trapping characteristics that gives the well known S-shape behaviour [5]. Therefore experimental observation of the temperature dependence of the true band gap of dilute nitrides is not possible at low temperatures. In order to overcome this problem we have introduced modulation doping resulting in the elevation of the Fermi level, hence in the screening of the exciton trapping effects. Therefore, it was possible to observe directly a true temperature dependence of the band gap.