On the hole accelerator for III-nitride light-emitting diodes
buir.contributor.author | Demir, Hilmi Volkan | |
buir.contributor.orcid | Demir, Hilmi Volkan|0000-0003-1793-112X | |
dc.citation.issueNumber | 15 | en_US |
dc.citation.volumeNumber | 108 | en_US |
dc.contributor.author | Zhang Z.-H. | en_US |
dc.contributor.author | Zhang, Y. | en_US |
dc.contributor.author | Bi, W. | en_US |
dc.contributor.author | Geng, C. | en_US |
dc.contributor.author | Xu S. | en_US |
dc.contributor.author | Demir, Hilmi Volkan | en_US |
dc.contributor.author | Sun, X. W. | en_US |
dc.date.accessioned | 2018-04-12T10:47:19Z | |
dc.date.available | 2018-04-12T10:47:19Z | |
dc.date.issued | 2016 | en_US |
dc.department | Department of Electrical and Electronics Engineering | en_US |
dc.department | Institute of Materials Science and Nanotechnology (UNAM) | en_US |
dc.department | Department of Physics | en_US |
dc.description.abstract | In this work, we systematically conduct parametric studies revealing the sensitivity of the hole injection on the hole accelerator (a hole accelerator is made of the polarization mismatched p-electron blocking layer (EBL)/p-GaN/p-AlxGa1-xN heterojunction) with different designs, including the AlN composition in the p-AlxGa1-xN layer, and the thickness for the p-GaN layer and the p-AlxGa1-xN layer. According to our findings, the energy that the holes obtain does not monotonically increase as the AlN incorporation in the p-AlxGa1-xN layer increases. Meanwhile, with p-GaN layer or p-AlxGa1-xN layer thickening, the energy that the holes gain increases and then reaches a saturation level. Thus, the hole injection efficiency and the device efficiency are very sensitive to the p-EBL/p-GaN/p-AlxGa1-xN design, and the hole accelerator can effectively increase the hole injection if properly designed. | en_US |
dc.description.provenance | Made available in DSpace on 2018-04-12T10:47:19Z (GMT). No. of bitstreams: 1 bilkent-research-paper.pdf: 179475 bytes, checksum: ea0bedeb05ac9ccfb983c327e155f0c2 (MD5) Previous issue date: 2016 | en |
dc.identifier.doi | 10.1063/1.4947025 | en_US |
dc.identifier.issn | 0003-6951 | |
dc.identifier.uri | http://hdl.handle.net/11693/36655 | |
dc.language.iso | English | en_US |
dc.publisher | American Institute of Physics Inc. | en_US |
dc.relation.isversionof | http://dx.doi.org/10.1063/1.4947025 | en_US |
dc.source.title | Applied Physics Letters | en_US |
dc.subject | Aluminum nitride | en_US |
dc.subject | Charge injection | en_US |
dc.subject | Electron injection | en_US |
dc.subject | Gallium nitride | en_US |
dc.subject | Heterojunctions | en_US |
dc.subject | Light emitting diodes | en_US |
dc.subject | Device efficiency | en_US |
dc.subject | Electron blocking layer | en_US |
dc.subject | GaN layers | en_US |
dc.subject | Hole injection | en_US |
dc.subject | III-Nitride | en_US |
dc.subject | N layers | en_US |
dc.subject | Parametric study | en_US |
dc.subject | Saturation levels | en_US |
dc.subject | Aluminum | en_US |
dc.title | On the hole accelerator for III-nitride light-emitting diodes | en_US |
dc.type | Article | en_US |
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