2021
DOI: 10.3390/cryst11101168
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Realization of III-Nitride c-Plane microLEDs Emitting from 470 to 645 nm on Semi-Relaxed Substrates Enabled by V-Defect-Free Base Layers

Abstract: We examine full InGaN-based microLEDs on c-plane semi-relaxed InGaN substrates grown by metal organic chemical vapor deposition (MOCVD) that operate across a wide range of emission wavelengths covering nearly the entire visible spectrum. By employing a periodic InGaN base layer structure with high temperature (HT) GaN interlayers on these semi-relaxed substrates, we demonstrate robust μLED devices. A broad range of emission wavelengths ranging from cyan to deep red are realized, leveraging the indium incorpora… Show more

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Cited by 7 publications
(8 citation statements)
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“…This base layer was also designed to match the lattice constant of the substrate, maintaining the relaxed strain state present initially. With a base layer free from V-defects and with good morphology, the advantages of the relaxed InGaN substrate and increased lattice constant can be used in the realization of µLED devices [18]. Importantly, the reduction of the compositional pulling effect resulting from the reduction in strain during growth can then be applied to QW growth, allowing for higher temperatures to be used while still achieving high In content in a red-emitting device.…”
Section: Introductionmentioning
confidence: 99%
“…This base layer was also designed to match the lattice constant of the substrate, maintaining the relaxed strain state present initially. With a base layer free from V-defects and with good morphology, the advantages of the relaxed InGaN substrate and increased lattice constant can be used in the realization of µLED devices [18]. Importantly, the reduction of the compositional pulling effect resulting from the reduction in strain during growth can then be applied to QW growth, allowing for higher temperatures to be used while still achieving high In content in a red-emitting device.…”
Section: Introductionmentioning
confidence: 99%
“…Figure 3a shows the current density-voltage characteristics of the µLEDs. All the devices yielded a low forward voltage, showing voltage values between 2.00 V and 2.05 V at 20 A/cm 2 , which is the lowest voltage characteristic compared to other InGaN red emitters in the literature [9,15,19,[28][29][30]. The low voltage could be attributed to the better hole The InGaN red devices yielded exceptional electrical and optical performances, including low forward voltage and relatively high light output power (LOP) characteristics.…”
Section: Resultsmentioning
confidence: 85%
“…Nevertheless, the FWHM was very broad for display applications, and decreased from 90 nm at 5 A/cm 2 to 66 nm at 35 A/cm 2 and increased gradually to 70 nm at 100 A/cm 2 . For InGaN-based LEDs, the FWHM generally increased with wavelength emission due to indium fluctuation in the active region [9]. The reduction in electroluminescent FWHM from 5 to 35 A/cm 2 could be due to emission from delocalized band states, while the increase in FWHM at higher current densities could be attributed to bandgap normalization due to an increase in junction temperature or excited states [24,25].…”
Section: Resultsmentioning
confidence: 99%
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“…More recently, we reported InGaN red µLEDs with an EQE over 3% using similar active region design [5][6][7]. Other novel growth strategies have been proposed to achieve InGaN red µLEDs, such as InGaNOS pseudo-substrate [16][17][18][19], nano-porous GaN [20], strain relaxed InGaN buffer layer using in-situ InGaN decomposition layer [21,22]. These technologies aim to relax the strain of InGaN buffer layer and increase the indium intake efficiency in the red InGaN QWs.…”
Section: Introductionmentioning
confidence: 99%