Abstract:We study the carrier distribution in multi quantum well (multi-QW) InGaN light-emitting diodes. Conventional wisdom would assume that a large number of QWs lead to a smaller carrier density per QW, enabling efficient carrier recombination at high currents. We use angle-resolved far-field measurements to determine the location of spontaneous emission in a series of multi-QW samples. They reveal that, no matter how many QWs are grown, only the QW nearest the p layer emits light under electrical pumping, which ca… Show more
“…31 The "efficiency droop" is a common issue in nitride LEDs, 37,38 which is caused by a non-radiative carrier loss mechanism that has small effect at low J inject present in the active region, but becomes dominant at higher J inject. The main reason of the droop is still under debate as many different mechanisms have been proposed including Auger recombination, [39][40][41][42] "carrier overflow"/poor hole-injection efficiency, 35,43,44 and density-activated defects. 45,46 Generally, the much smaller droop of nonpolar and semipolar LEDs in comparison with polar LEDs has been attributed to the weaker polarization fields.…”
Section: Resultsmentioning
confidence: 99%
“…56 Additionally, the rough surface morphology of the PSS-LED (Fig. 1) is another issue as it can cause nonuniform carrier distribution 21,44 and compositional fluctuations. 21 It has been previously found that polished PSS-GaN substrates can strongly enhance the luminescence uniformity of QWs and the performance of PSS-LEDs.…”
Section: Discussionmentioning
confidence: 99%
“…It should be noted that in an MQW structure under PL excitation, electron-hole pairs are generated in the whole structure, whereas under EL excitation, the generated carriers are mostly distributed in the QW nearest the p-layer. 44,52 For InGaN QW structures, it is well-known that TDs strongly affect IQE as they can act as non-radiative recombination centres. 25,[53][54][55] However, it has been found that a strong ELOC can effectively reduce the QW excitons from being trapped into TDs, resulting in an enhanced luminescence efficiency from InGaN based devices.…”
We compare the optical properties and device performance of unpackaged InGaN/GaN multiple-quantum-well light-emitting diodes (LEDs) emitting at ∼430 nm grown simultaneously on a high-cost small-size bulk semipolar (112¯2) GaN substrate (Bulk-GaN) and a low-cost large-size (112¯2) GaN template created on patterned (101¯2) r-plane sapphire substrate (PSS-GaN). The Bulk-GaN substrate has the threading dislocation density (TDD) of ∼105 cm−2–106 cm−2 and basal-plane stacking fault (BSF) density of 0 cm−1, while the PSS-GaN substrate has the TDD of ∼2 × 108 cm−2 and BSF density of ∼1 × 103 cm−1. Despite an enhanced light extraction efficiency, the LED grown on PSS-GaN has two-times lower internal quantum efficiency than the LED grown on Bulk-GaN as determined by photoluminescence measurements. The LED grown on PSS-GaN substrate also has about two-times lower output power compared to the LED grown on Bulk-GaN substrate. This lower output power was attributed to the higher TDD and BSF density.
“…31 The "efficiency droop" is a common issue in nitride LEDs, 37,38 which is caused by a non-radiative carrier loss mechanism that has small effect at low J inject present in the active region, but becomes dominant at higher J inject. The main reason of the droop is still under debate as many different mechanisms have been proposed including Auger recombination, [39][40][41][42] "carrier overflow"/poor hole-injection efficiency, 35,43,44 and density-activated defects. 45,46 Generally, the much smaller droop of nonpolar and semipolar LEDs in comparison with polar LEDs has been attributed to the weaker polarization fields.…”
Section: Resultsmentioning
confidence: 99%
“…56 Additionally, the rough surface morphology of the PSS-LED (Fig. 1) is another issue as it can cause nonuniform carrier distribution 21,44 and compositional fluctuations. 21 It has been previously found that polished PSS-GaN substrates can strongly enhance the luminescence uniformity of QWs and the performance of PSS-LEDs.…”
Section: Discussionmentioning
confidence: 99%
“…It should be noted that in an MQW structure under PL excitation, electron-hole pairs are generated in the whole structure, whereas under EL excitation, the generated carriers are mostly distributed in the QW nearest the p-layer. 44,52 For InGaN QW structures, it is well-known that TDs strongly affect IQE as they can act as non-radiative recombination centres. 25,[53][54][55] However, it has been found that a strong ELOC can effectively reduce the QW excitons from being trapped into TDs, resulting in an enhanced luminescence efficiency from InGaN based devices.…”
We compare the optical properties and device performance of unpackaged InGaN/GaN multiple-quantum-well light-emitting diodes (LEDs) emitting at ∼430 nm grown simultaneously on a high-cost small-size bulk semipolar (112¯2) GaN substrate (Bulk-GaN) and a low-cost large-size (112¯2) GaN template created on patterned (101¯2) r-plane sapphire substrate (PSS-GaN). The Bulk-GaN substrate has the threading dislocation density (TDD) of ∼105 cm−2–106 cm−2 and basal-plane stacking fault (BSF) density of 0 cm−1, while the PSS-GaN substrate has the TDD of ∼2 × 108 cm−2 and BSF density of ∼1 × 103 cm−1. Despite an enhanced light extraction efficiency, the LED grown on PSS-GaN has two-times lower internal quantum efficiency than the LED grown on Bulk-GaN as determined by photoluminescence measurements. The LED grown on PSS-GaN substrate also has about two-times lower output power compared to the LED grown on Bulk-GaN substrate. This lower output power was attributed to the higher TDD and BSF density.
“…In situations where all quantum wells are identical, the relatively large effective mass of the holes, as compared to the effective mass of the electrons, tends to make hole transport the limiting factor in achieving a uniform carrier distribution. 8 The effect of barrier thickness on carrier distribution has also been studied in InGaAsP lasers where a large valence band offset is present. 9 Apart from their use in monitoring carrier distributions, multicolor LEDs are also useful as broad-spectrum LED sources.…”
“…[1][2][3] In the past decade, multiple mechanisms have been proposed to explain the efficiency droop including Auger recombination induced by multi-particle interactions, [4][5][6][7][8] electron leakage due to poor hole injection and electron overflow, 9,10 carrier loss related to reduction or saturation of carrier localization, 11,12 and other processes including the density-activated defect recombination (DADR). 13,14 Some of these factors have been found to be tightly associated with the internal polarization field.…”
Abstract:We report on the observation of carrier-diffusion-induced defect emission at high excitation density in a-plane InGaN single quantum wells. When increasing excitation density in a relatively high regime, we observed the emergence of defect-related emission together with a significant reduction in bandedge emission efficiency. The experimental results can be well explained with the density-activated carrier diffusion from localized states to defect states. Such a scenario of density-activated defect recombination, as confirmed by the dependences of photoluminescence on the excitation photon energy and temperature, is a plausible origin of efficiency droop in a-plane InGaN quantum-well light-emitting diodes. a cfzhang@nju.edu.cn b jskwak@sunchon.ac.kr c mxiao@uark.edu
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