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dc.contributor.authorTu, Po-Minen_US
dc.contributor.authorChang, Jet-Rungen_US
dc.contributor.authorHuang, Shih-Chengen_US
dc.contributor.authorYang, Shun-Kueien_US
dc.contributor.authorLin, Ya-wenen_US
dc.contributor.authorHung, Tzu-Chienen_US
dc.contributor.authorHsu, Chih-Pengen_US
dc.contributor.authorChang, Chun-Yenen_US
dc.date.accessioned2019-04-03T06:47:56Z-
dc.date.available2019-04-03T06:47:56Z-
dc.date.issued2012-01-01en_US
dc.identifier.isbn978-0-81948-921-0en_US
dc.identifier.issn0277-786Xen_US
dc.identifier.urihttp://dx.doi.org/10.1117/12.908266en_US
dc.identifier.urihttp://hdl.handle.net/11536/146321-
dc.description.abstractThe efficiency droop in InGaN-based 380nm UV light emitting device (LED) with n-GaN and n-AlGaN underlayer grown on sapphire substrate by metal-organic chemical vapor deposition (MOCVD) was investigated. From simulation result of high resolution x-ray diffraction (HRXRD) omega-2 theta. curve by using dynamical diffraction theory, the Al composition in the n-AlGaN layer was determined to be about 3%. The experimental results of temperature dependent photoluminescence (PL) demonstrated that the internal quantum efficiency (IQE) of n-GaN and n-AlGaN UV-LEDs are 43% and 39%, respectively, which are corresponding to an injected carrier density of 8.5 x 10(17) #/cm(3). It could be explained that the crystal quality of n-GaN is better than of n-AlGaN. In addition, the observation of pit density from atomic force microscopy (AFM) surface morphology is consistent with the interpretation. It was well-known that the pits appearing on the surface in the virtue of the threading dislocations. Thus, it means that defects induce the non-radiative centers and deteriorate the IQE of the UV-LED with n-AlGaN underlayer. Therefore, the light output power of n-GaN UV-LED is slightly higher below the forward current of 250 mA. Nevertheless, the output power was enhanced about 22% as the injection current was increased to 600 mA. Furthermore, the external quantum efficiency (EQE) of n-AlGaN UV-LED was nearly retained at the 600 mA (only 20% droop), whereas the UV-LED with n-GaN exhibits as high as 33%. We attributed this improvement to the less self-absoption by replacing n-GaN underlayer with n-AlGaN.en_US
dc.language.isoen_USen_US
dc.subjectGaNen_US
dc.subjectUV-LEDsen_US
dc.subjectDroopen_US
dc.titleInvestigation of Efficiency Droop for UV-LED with N-type AlGaN Layeren_US
dc.typeProceedings Paperen_US
dc.identifier.doi10.1117/12.908266en_US
dc.identifier.journalLIGHT-EMITTING DIODES: MATERIALS, DEVICES, AND APPLICATIONS FOR SOLID STATE LIGHTING XVIen_US
dc.citation.volume8278en_US
dc.citation.spage0en_US
dc.citation.epage0en_US
dc.contributor.department電子工程學系及電子研究所zh_TW
dc.contributor.departmentDepartment of Electronics Engineering and Institute of Electronicsen_US
dc.identifier.wosnumberWOS:000301055700020en_US
dc.citation.woscount0en_US
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