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dc.contributor.authorCheng, Chih-Hsienen_US
dc.contributor.authorTzou, An-Jyeen_US
dc.contributor.authorChang, Jung-Hungen_US
dc.contributor.authorChi, Yu-Chiehen_US
dc.contributor.authorLin, Yung-Hsiangen_US
dc.contributor.authorShih, Min-Hsiungen_US
dc.contributor.authorLee, Chao-Kueien_US
dc.contributor.authorWu, Chih-Ien_US
dc.contributor.authorKuo, Hao-Chungen_US
dc.contributor.authorChang, Chun-Yenen_US
dc.contributor.authorLin, Gong-Ruen_US
dc.date.accessioned2019-04-03T06:44:50Z-
dc.date.available2019-04-03T06:44:50Z-
dc.date.issued2016-01-22en_US
dc.identifier.issn2045-2322en_US
dc.identifier.urihttp://dx.doi.org/10.1038/srep19757en_US
dc.identifier.urihttp://hdl.handle.net/11536/129658-
dc.description.abstractThe epitaxy of high-power gallium nitride (GaN) light-emitting diode (LED) on amorphous silicon carbide (a-SixC1-x) buffer is demonstrated. The a-SixC1-x buffers with different nonstoichiometric C/Si composition ratios are synthesized on SiO2/Si substrate by using a low-temperature plasma enhanced chemical vapor deposition. The GaN LEDs on different SixC1-x buffers exhibit different EL and C-V characteristics because of the extended strain induced interfacial defects. The EL power decays when increasing the Si content of SixC1-x buffer. The C-rich SixC1-x favors the GaN epitaxy and enables the strain relaxation to suppress the probability of Auger recombination. When the SixC1-x buffer changes from Si-rich to C-rich condition, the EL peak wavelengh shifts from 446 nm to 450 nm. Moreover, the uniform distribution contour of EL intensity spreads between the anode and the cathode because the traping density of the interfacial defect gradually reduces. In comparison with the GaN LED grown on Sirich SixC1-x buffer, the device deposited on C-rich SixC1-x buffer shows a lower turn-on voltage, a higher output power, an external quantum efficiency, and an efficiency droop of 2.48 V, 106 mW, 42.3%, and 7%, respectively.en_US
dc.language.isoen_USen_US
dc.titleGrowing GaN LEDs on amorphous SiC buffer with variable C/Si compositionsen_US
dc.typeArticleen_US
dc.identifier.doi10.1038/srep19757en_US
dc.identifier.journalSCIENTIFIC REPORTSen_US
dc.citation.volume6en_US
dc.citation.spage0en_US
dc.citation.epage0en_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.department電子工程學系及電子研究所zh_TW
dc.contributor.department光電工程學系zh_TW
dc.contributor.department光電工程研究所zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.contributor.departmentDepartment of Electronics Engineering and Institute of Electronicsen_US
dc.contributor.departmentDepartment of Photonicsen_US
dc.contributor.departmentInstitute of EO Enginerringen_US
dc.identifier.wosnumberWOS:000368667700003en_US
dc.citation.woscount20en_US
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