Radiative lifetime of excitons in high energy GaN/AlN quantum dots
Résumé
Self-assembled semiconductors QDs are of great interest in fundamental physics as well as in
applied physics. In GaN/AlN heterostructures, the huge band-offset and the strong excitonic
binding lead to an important exciton confinement allowing an emission even at room
temperature. GaN QDs grown along the (1000) axis are named “polar” due to their strong
internal electic field which lead to the so-called QCSE. The most important modifications due to
this electric field take place in thick QDs emitting around 330nm and more : the luminescence is
redshifted and the radiative lifetime is strongly increased [1]. On the other hand, in thin QDs
(smaller than 2.3nm), the quantum confinement plays the key role, thus leading to a significantly
smaller homogeneous linewidth and to the resolution of the exciton fine-structure splitting[2].
Concerning the radiative recombination processes, several papers reported measurements at
330nm or more either in polar[3] or non-polar[4] nanostructures. Experimental data on excitonic
radiative lifetime are also existent in thin QDs but on a limited dynamical range where the
possible influence of QCSE is not discussed [5].
In this work, we report time-resolved photoluminescence measurements in GaN/AlN QDs
emitting between 280nm and 360nm. For QDs emitting at 300nm we observe a biexponential
decay dynamics of the photoluminescence signal (Fig.1, left). The fast component (450 ps) is
interpreted as the radiative lifetime of the QDs in the absence of a noticeable redshift of the
transition. Thanks to our better signal-to-noise ratio than in Ref. 5, we are able to extract a slow
component (2 ns) which may originate either from feeding from the barrier or other processes
inside the QD. Power dependent experiments further confirm this interpretation. We observe that
the fast component remains the same as a function of excitation power (Fig.1, right) and, more
importantly, that the intensity ratio keeps the same value. This rules out any contribution from
the relaxation of multi-carriers complexes such as biexciton or trion in the short time dynamics