We investigate the role of dislocations in nitride light emitters by comparing a set of laser diodes grown on GaN substrates with their counterparts grown on sapphire. Studied structures emit light in the range 383-477nm. We observe decrease in intensity of electroluminescence for samples with low indium composition and high dislocation density. To understand this effect we measured cathodoluminescence and investigated thermal stability of chosen structures. Results show that significance of dislocation related nonradiative recombination increases for low indium content structures due to shorter diffusion path of carriers. Results of TEM and SEM indicate that edge dislocations are the main source of nonradiative recombination in our structures.
In this paper, we try to resolve problems related to decreasing the size of an LED, and find a solution that would let us preserve optoelectronics parameters. The main idea is to use tunnel junctions to define the current path and, therefore, define the size of µLED. This way, during fabrication, there is no need to etch the active region. That way, it does not introduce any degradation nor problems related to surface states or differences in electrical fields inside the device.
We have fabricated such devices with sizes ranging from 100 µm-5 µm. In the characterization of these devices, it became apparent that, both electrical and optical parameters, are fully scalable with size. Most importantly, we do not observe an increase in the non-radiative recombination coefficient even for the smallest device. In addition, we observe excellent thermal stability of their light emission characteristics.
Our goal is to fabricate a laser diode 2D array which combines the properties of both VCSEL and edge emitting laser. Proposed light emitter will have a horizontal cavity with 450 deflectors. The role of these deflectors would be to deflect light perpendicular to the cavity, achieving vertical out-coupling. The most challenging part of this project is the fabrication of the micro-mirrors which act as both as beam deviating mirrors and cavity forming mirrors. Owing to the excellent thermal conductivity of GaN substrates the properties of such a 2D array should be better than of conventional nitride laser diode arrays, not even mentioning nitride-based stacked bars systems. In this paper I will describe our new device design and processing, giving insight to its possible applications and advantages over simple light emitting laser diode.
There are two physical phenomena governing the light emission in InGaN quantum structures: the internal electric fields and the In composition fluctuations. Both these effects manifest through the blue shift of the wavelength emission with the excitation intensity and both of them have the pronounced influence on the light emitting properties of these structures.
In order to discriminate between these two effects, we fabricated two identical structures: one with the quantum barriers doped with silicon (method for internal electric field screening) and the other with an undoped active region. Under the optical excitation the emission peak shifts by almost 35 nm (Si doped) and 50nm (without Si). Additionally, we studied temperature dependence of the emission peak position. In case of low temperatures and at RT and high pumping energy, emission energy position is almost the same for both samples. Our observations lead us to the conclusion that at low temperatures and at high pumping regime the Quantum Confined Stark Effect (QCSE) is totally suppressed. While this is understandable that at high carrier injection QCSE is screened, the origin of the low temperature effect is much less clear. We can speculate that at the lowest temperature the carriers are localized eliminating the spatial separation of holes and electrons wavefunctions.
Measured cathodoluminescence (CL) maps show the same level of the indium fluctuations for both samples. At higher excitation the fluctuations starts to be less visible suggesting band filling of states.
Finally we compare recombination times by means of time resolved photoluminescence.
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