Carrier injection and radiative recombination processes in InGaN/GaN blue light emitting diodes are investigated by bias-dependent cathodoluminescence. The samples are designed with a single-quantum-well SQW light emitter and an adjacent multi-quantum-well MQW carrier injector of lower In content. In unbiased samples, the MQW emission dominates over the SQW at high temperatures T160 K or low beam currents IB5 nA. This is ascribed to changes in the device energy band diagram, dependent on the field in the p-n junction and on the level of electron beam induced excitation of excess carriers. A field screening, resulting in a forward biasing of the devices, is highlighted. A maximum value of +2.65 V is reached at T=100 K for a carrier generation rate G05.41013 s−1. At a fixed electron beam power, the effects of an external applied field on the emitter efficiency are considered. The SQW emission is promoted in the forward-current regime, while in the reverse-current regime −1V2.65 at T=100 K it undergoes a quenching of at least one order of magnitude and a blueshift 60 meV at T=100 K due to a partial compensation between the junction field and the internal piezoelectric field minimum residual field of about 1.9 MV/cm at T=100 K. The observed blueshift is in a fairly good agreement with the voltage dependence predicted by calculating the energy band profiles and SQW confined states with a self-consistent Schrödinger–Poisson solver.

Field dependence of the carrier injection mechanisms in InGaN Quantum wells: Its effect on the luminescence properties of blue light emitting diodes

MENEGHINI, MATTEO;ZANONI, ENRICO;
2008

Abstract

Carrier injection and radiative recombination processes in InGaN/GaN blue light emitting diodes are investigated by bias-dependent cathodoluminescence. The samples are designed with a single-quantum-well SQW light emitter and an adjacent multi-quantum-well MQW carrier injector of lower In content. In unbiased samples, the MQW emission dominates over the SQW at high temperatures T160 K or low beam currents IB5 nA. This is ascribed to changes in the device energy band diagram, dependent on the field in the p-n junction and on the level of electron beam induced excitation of excess carriers. A field screening, resulting in a forward biasing of the devices, is highlighted. A maximum value of +2.65 V is reached at T=100 K for a carrier generation rate G05.41013 s−1. At a fixed electron beam power, the effects of an external applied field on the emitter efficiency are considered. The SQW emission is promoted in the forward-current regime, while in the reverse-current regime −1V2.65 at T=100 K it undergoes a quenching of at least one order of magnitude and a blueshift 60 meV at T=100 K due to a partial compensation between the junction field and the internal piezoelectric field minimum residual field of about 1.9 MV/cm at T=100 K. The observed blueshift is in a fairly good agreement with the voltage dependence predicted by calculating the energy band profiles and SQW confined states with a self-consistent Schrödinger–Poisson solver.
2008
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11577/2455903
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