{"title":"应变补偿InGaAs/InAlAs量子级联激光器结构的自洽设计:短波方向","authors":"Y. Ko, J. S. Yu, K. Chung","doi":"10.1109/NUSOD.2009.5297246","DOIUrl":null,"url":null,"abstract":"We designed In<inf>x</inf>Ga<inf>1−x</inf>As/InyAl<inf>1−y</inf>As quantum cascade laser (QCL) structures, based on the four-quantum well active region operating at λ ~ 2.8−3.3 μm in terms of an objective function, i.e., zg<inf>L</inf>(l − t<inf>l</inf>/t<inf>ul</inf>)tu, related to the optical gain, including dipole matrix element (z<inf>UL</inf>) and population inversion between electron transitions. For shorter wavelength emission, the higher conduction band discontinuity (ΔE<inf>C</inf>) was achieved by changing the In mole fraction of In<inf>x</inf>Ga<inf>1−x</inf>As/InyAl<inf>1−y</inf>As strain-compensated layers. The use of strain-compensated In<inf>0</inf>.7<inf>2</inf>Ga<inf>0</inf>.<inf>28</inf>As/In<inf>0</inf>.3Al<inf>0</inf>.<inf>7</inf>As pair (i.e, ΔE<inf>C</inf> = 857 meV) leads to the shortest wavelength up to λ ~ 2.84 μm with τ<inf>43</inf> = 3.96 ps, τ<inf>4</inf> = 1.21 ps, τ<inf>3</inf> = 0.55 ps and z<inf>43</inf> = 0.57 nm under an electric field of 94 kV/cm.","PeriodicalId":120796,"journal":{"name":"2009 9th International Conference on Numerical Simulation of Optoelectronic Devices","volume":"65 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2009-10-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Self-consistent design of strain-compensated InGaAs/InAlAs quantum cascade laser structures: Towards short wavelengths\",\"authors\":\"Y. Ko, J. S. Yu, K. Chung\",\"doi\":\"10.1109/NUSOD.2009.5297246\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We designed In<inf>x</inf>Ga<inf>1−x</inf>As/InyAl<inf>1−y</inf>As quantum cascade laser (QCL) structures, based on the four-quantum well active region operating at λ ~ 2.8−3.3 μm in terms of an objective function, i.e., zg<inf>L</inf>(l − t<inf>l</inf>/t<inf>ul</inf>)tu, related to the optical gain, including dipole matrix element (z<inf>UL</inf>) and population inversion between electron transitions. For shorter wavelength emission, the higher conduction band discontinuity (ΔE<inf>C</inf>) was achieved by changing the In mole fraction of In<inf>x</inf>Ga<inf>1−x</inf>As/InyAl<inf>1−y</inf>As strain-compensated layers. The use of strain-compensated In<inf>0</inf>.7<inf>2</inf>Ga<inf>0</inf>.<inf>28</inf>As/In<inf>0</inf>.3Al<inf>0</inf>.<inf>7</inf>As pair (i.e, ΔE<inf>C</inf> = 857 meV) leads to the shortest wavelength up to λ ~ 2.84 μm with τ<inf>43</inf> = 3.96 ps, τ<inf>4</inf> = 1.21 ps, τ<inf>3</inf> = 0.55 ps and z<inf>43</inf> = 0.57 nm under an electric field of 94 kV/cm.\",\"PeriodicalId\":120796,\"journal\":{\"name\":\"2009 9th International Conference on Numerical Simulation of Optoelectronic Devices\",\"volume\":\"65 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2009-10-30\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2009 9th International Conference on Numerical Simulation of Optoelectronic Devices\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/NUSOD.2009.5297246\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2009 9th International Conference on Numerical Simulation of Optoelectronic Devices","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/NUSOD.2009.5297246","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Self-consistent design of strain-compensated InGaAs/InAlAs quantum cascade laser structures: Towards short wavelengths
We designed InxGa1−xAs/InyAl1−yAs quantum cascade laser (QCL) structures, based on the four-quantum well active region operating at λ ~ 2.8−3.3 μm in terms of an objective function, i.e., zgL(l − tl/tul)tu, related to the optical gain, including dipole matrix element (zUL) and population inversion between electron transitions. For shorter wavelength emission, the higher conduction band discontinuity (ΔEC) was achieved by changing the In mole fraction of InxGa1−xAs/InyAl1−yAs strain-compensated layers. The use of strain-compensated In0.72Ga0.28As/In0.3Al0.7As pair (i.e, ΔEC = 857 meV) leads to the shortest wavelength up to λ ~ 2.84 μm with τ43 = 3.96 ps, τ4 = 1.21 ps, τ3 = 0.55 ps and z43 = 0.57 nm under an electric field of 94 kV/cm.