dc.date.accessioned | 2020-10-07T18:26:53Z | |
dc.date.available | 2020-10-07T18:26:53Z | |
dc.date.created | 2020-07-30T10:28:01Z | |
dc.date.issued | 2020 | |
dc.identifier.citation | Zimmermann, Christian Verhoeven, Espen Førdestrøm Frodason, Ymir Kalmann Weiser, Philip Michael Varley, Joel B Vines, Lasse . Formation and control of the E2* center in implanted b-Ga2O3 by reverse-bias and zero-bias annealing. Journal of Physics D: Applied Physics. 2020, 53(46), 464001 | |
dc.identifier.uri | http://hdl.handle.net/10852/80483 | |
dc.description.abstract | Deep-level transient spectroscopy measurements are conducted onβ-Ga2O3thin-filmsimplanted with helium and hydrogen (H) to study the formation of the defect levelE∗2(EA=0.71 eV) during heat treatments under an applied reverse-bias voltage (reverse-biasannealing). The formation ofE∗2during reverse-bias annealing is a thermally-activated processexhibiting an activation energy of around 1.0 eV to 1.3 eV, and applying larger reverse-biasvoltages during the heat treatment results in a larger concentration ofE∗2. In contrast, heattreatments without an applied reverse-bias voltage (zero-bias annealing) can be used to decreasetheE∗2concentration. The removal ofE∗2is more pronounced if zero-bias anneals are performedin the presence of H. A scenario for the formation ofE∗2is proposed, where the main effect ofreverse-bias annealing is an effective change in the Fermi-level position within the space-chargeregion, and whereE∗2is related to a defect complex involving intrinsic defects that exhibitsseveral different configurations whose relative formation energies depend on the Fermi-levelposition. One of these configurations gives rise toE∗2, and is more likely to form if theFermi-level position is further away from the conduction band edge. The defect complex relatedtoE∗2can become hydrogenated, and the corresponding hydrogenated complex is likely to formwhen the Fermi level is close to the conduction band edge. Di-vacancy defects formed byoxygen and gallium vacancies (VO−VGa) fulfill several of these requirements, and are proposedas potential candidates forE∗2. | |
dc.language | EN | |
dc.rights | Attribution 4.0 International | |
dc.rights.uri | https://creativecommons.org/licenses/by/4.0/ | |
dc.title | Formation and control of the E2* center in implanted b-Ga2O3 by reverse-bias and zero-bias annealing | |
dc.type | Journal article | |
dc.creator.author | Zimmermann, Christian | |
dc.creator.author | Verhoeven, Espen Førdestrøm | |
dc.creator.author | Frodason, Ymir Kalmann | |
dc.creator.author | Weiser, Philip Michael | |
dc.creator.author | Varley, Joel B | |
dc.creator.author | Vines, Lasse | |
cristin.unitcode | 185,15,4,90 | |
cristin.unitname | Halvlederfysikk | |
cristin.ispublished | true | |
cristin.fulltext | postprint | |
cristin.fulltext | original | |
cristin.qualitycode | 1 | |
dc.identifier.cristin | 1821026 | |
dc.identifier.bibliographiccitation | info:ofi/fmt:kev:mtx:ctx&ctx_ver=Z39.88-2004&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.jtitle=Journal of Physics D: Applied Physics&rft.volume=53&rft.spage=464001&rft.date=2020 | |
dc.identifier.jtitle | Journal of Physics D: Applied Physics | |
dc.identifier.volume | 53 | |
dc.identifier.issue | 46 | |
dc.identifier.doi | https://doi.org/10.1088/1361-6463/aba64d | |
dc.identifier.urn | URN:NBN:no-83575 | |
dc.type.document | Tidsskriftartikkel | |
dc.type.peerreviewed | Peer reviewed | |
dc.source.issn | 0022-3727 | |
dc.identifier.fulltext | Fulltext https://www.duo.uio.no/bitstream/handle/10852/80483/1/ZimmermannC.JPhysDApplPhys.53.464001.2020_E2%2Bstar%2Bcenter%2Bin%2Bimplanted%2Bb-Ga2O3.pdf | |
dc.type.version | PublishedVersion | |
cristin.articleid | 464001 | |
dc.relation.project | NOTUR/NORSTORE/NN9136K | |
dc.relation.project | NFR/245963 | |
dc.relation.project | NFR/251131 | |