Interplay between Auger recombination, carrier leakage, and polarization in InGaAlN multiple-quantum-well light-emitting diodes
In conventional hexagonal InGaAlN multiple-quantum-well (MQW) (h-) light-emitting diodes (LEDs), carrier leakage from QWs is the main source of internal quantum efficiency (IQE) degradation without contributing to the LED efficiency droop. Our analysis based on the newly developed Open Boundary Quan...
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creator | Tsai, Y.-C. Bayram, C. Leburton, J.-P. |
description | In conventional hexagonal InGaAlN multiple-quantum-well (MQW) (h-) light-emitting diodes (LEDs), carrier leakage from QWs is the main source of internal quantum efficiency (IQE) degradation without contributing to the LED efficiency droop. Our analysis based on the newly developed Open Boundary Quantum LED Simulator indicates that radiative recombination is hampered by the poor electron–hole wavefunction overlap induced by strong internal polarization for which QW carriers mostly recombine via Auger scattering rather than by radiative processes. By contrast, in non-polar h-LEDs, the IQE peak doubles its value compared to conventional h-LEDs while quenching the efficiency droop by 70% at current density of 100 A/cm2. Those effects are further enhanced in cubic InGaAlN MQW (c-) LEDs for which the IQE peak increases by an additional 30%, and the efficiency droop is further reduced by 80% compared to non-polar h-LEDs, thanks to the larger optical transition matrix element and the strong electron–hole wavefunction overlap in c-LEDs. Overall, a c-LED with a low efficiency droop of 3% at 100 A/cm2 is anticipated, paving a clear pathway toward ultimate solid-state lighting. |
doi_str_mv | 10.1063/5.0089463 |
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Our analysis based on the newly developed Open Boundary Quantum LED Simulator indicates that radiative recombination is hampered by the poor electron–hole wavefunction overlap induced by strong internal polarization for which QW carriers mostly recombine via Auger scattering rather than by radiative processes. By contrast, in non-polar h-LEDs, the IQE peak doubles its value compared to conventional h-LEDs while quenching the efficiency droop by 70% at current density of 100 A/cm2. Those effects are further enhanced in cubic InGaAlN MQW (c-) LEDs for which the IQE peak increases by an additional 30%, and the efficiency droop is further reduced by 80% compared to non-polar h-LEDs, thanks to the larger optical transition matrix element and the strong electron–hole wavefunction overlap in c-LEDs. Overall, a c-LED with a low efficiency droop of 3% at 100 A/cm2 is anticipated, paving a clear pathway toward ultimate solid-state lighting.</description><identifier>ISSN: 0021-8979</identifier><identifier>EISSN: 1089-7550</identifier><identifier>DOI: 10.1063/5.0089463</identifier><identifier>CODEN: JAPIAU</identifier><language>eng</language><publisher>Melville: American Institute of Physics</publisher><subject>Applied physics ; Augers ; Carrier recombination ; Efficiency ; Leakage ; Light emitting diodes ; Optical transition ; Polarization ; Quantum efficiency ; Quantum wells ; Radiative recombination ; Wave functions</subject><ispartof>Journal of applied physics, 2022-05, Vol.131 (19)</ispartof><rights>Author(s)</rights><rights>2022 Author(s). 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Our analysis based on the newly developed Open Boundary Quantum LED Simulator indicates that radiative recombination is hampered by the poor electron–hole wavefunction overlap induced by strong internal polarization for which QW carriers mostly recombine via Auger scattering rather than by radiative processes. By contrast, in non-polar h-LEDs, the IQE peak doubles its value compared to conventional h-LEDs while quenching the efficiency droop by 70% at current density of 100 A/cm2. Those effects are further enhanced in cubic InGaAlN MQW (c-) LEDs for which the IQE peak increases by an additional 30%, and the efficiency droop is further reduced by 80% compared to non-polar h-LEDs, thanks to the larger optical transition matrix element and the strong electron–hole wavefunction overlap in c-LEDs. Overall, a c-LED with a low efficiency droop of 3% at 100 A/cm2 is anticipated, paving a clear pathway toward ultimate solid-state lighting.</description><subject>Applied physics</subject><subject>Augers</subject><subject>Carrier recombination</subject><subject>Efficiency</subject><subject>Leakage</subject><subject>Light emitting diodes</subject><subject>Optical transition</subject><subject>Polarization</subject><subject>Quantum efficiency</subject><subject>Quantum wells</subject><subject>Radiative recombination</subject><subject>Wave functions</subject><issn>0021-8979</issn><issn>1089-7550</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><recordid>eNp90EFLwzAUB_AgCs7pwW8Q8KSsM2matDmOoXMw9KLnkravMzNNuzR1zItf3boNPQie3uPx473HH6FLSsaUCHbLx4QkMhLsCA1o3wUx5-QYDQgJaZDIWJ6is7ZdEUJpwuQAfc6tB9cYtcUZ-A2AxZNuCQ47yOsq01Z5XdsRzpVzuh8bUG9qCSOsbIGb2iinP3YEa4vndqYm5hFXnfG6MRCsO2V9VwUbMAYbvXz1AVTae22XuNB1Ae05OimVaeHiUIfo5f7uefoQLJ5m8-lkEeQsjH0gM14UjAsqk4yIpH8_yQREuVBQhpKRKFM8k1JENBFQclJAFKo4powDzfKoYEN0td_buHrdQevTVd05259MQyE4Y5wmvFfXe5W7um0dlGnjdKXcNqUk_c435ekh397e7G2ba7-L4Ae_1-4Xpk1R_of_bv4CwWSKkw</recordid><startdate>20220521</startdate><enddate>20220521</enddate><creator>Tsai, Y.-C.</creator><creator>Bayram, C.</creator><creator>Leburton, J.-P.</creator><general>American Institute of Physics</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0002-3987-1132</orcidid><orcidid>https://orcid.org/0000-0002-8183-5581</orcidid><orcidid>https://orcid.org/0000-0003-2658-9397</orcidid></search><sort><creationdate>20220521</creationdate><title>Interplay between Auger recombination, carrier leakage, and polarization in InGaAlN multiple-quantum-well light-emitting diodes</title><author>Tsai, Y.-C. ; Bayram, C. ; Leburton, J.-P.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c327t-9b5dd356198b0680018b6e4c6aef29304ba5b9964186ef50de42a77135e1bc4d3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><topic>Applied physics</topic><topic>Augers</topic><topic>Carrier recombination</topic><topic>Efficiency</topic><topic>Leakage</topic><topic>Light emitting diodes</topic><topic>Optical transition</topic><topic>Polarization</topic><topic>Quantum efficiency</topic><topic>Quantum wells</topic><topic>Radiative recombination</topic><topic>Wave functions</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Tsai, Y.-C.</creatorcontrib><creatorcontrib>Bayram, C.</creatorcontrib><creatorcontrib>Leburton, J.-P.</creatorcontrib><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of applied physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Tsai, Y.-C.</au><au>Bayram, C.</au><au>Leburton, J.-P.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Interplay between Auger recombination, carrier leakage, and polarization in InGaAlN multiple-quantum-well light-emitting diodes</atitle><jtitle>Journal of applied physics</jtitle><date>2022-05-21</date><risdate>2022</risdate><volume>131</volume><issue>19</issue><issn>0021-8979</issn><eissn>1089-7550</eissn><coden>JAPIAU</coden><abstract>In conventional hexagonal InGaAlN multiple-quantum-well (MQW) (h-) light-emitting diodes (LEDs), carrier leakage from QWs is the main source of internal quantum efficiency (IQE) degradation without contributing to the LED efficiency droop. Our analysis based on the newly developed Open Boundary Quantum LED Simulator indicates that radiative recombination is hampered by the poor electron–hole wavefunction overlap induced by strong internal polarization for which QW carriers mostly recombine via Auger scattering rather than by radiative processes. By contrast, in non-polar h-LEDs, the IQE peak doubles its value compared to conventional h-LEDs while quenching the efficiency droop by 70% at current density of 100 A/cm2. Those effects are further enhanced in cubic InGaAlN MQW (c-) LEDs for which the IQE peak increases by an additional 30%, and the efficiency droop is further reduced by 80% compared to non-polar h-LEDs, thanks to the larger optical transition matrix element and the strong electron–hole wavefunction overlap in c-LEDs. 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subjects | Applied physics Augers Carrier recombination Efficiency Leakage Light emitting diodes Optical transition Polarization Quantum efficiency Quantum wells Radiative recombination Wave functions |
title | Interplay between Auger recombination, carrier leakage, and polarization in InGaAlN multiple-quantum-well light-emitting diodes |
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