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dc.date.accessioned2020-05-19T18:10:50Z
dc.date.available2020-09-26T22:46:17Z
dc.date.created2019-10-28T14:19:28Z
dc.date.issued2019
dc.identifier.citationSchifano, Ramon Jakiela, R Galeckas, Augustinas Kopalko, K Herklotz, Frank Johansen, Klaus Magnus H Vines, Lasse . Role of intrinsic and extrinsic defects in H implanted hydrothermally grown ZnO. Journal of Applied Physics. 2019, 126(12)
dc.identifier.urihttp://hdl.handle.net/10852/75941
dc.description.abstractThe impact of hydrogen in ZnO is revealed by combining reaction dynamics calculations with temperature dependent Hall (TDH), photoluminescence, and secondary ion mass spectrometry measurements performed on H, 2H, and He implanted ZnO. H and 2H box profiles with a concentration ranging from ∼3×1017 cm−3 to ∼1019 cm−3 and He to produce as much as damage as in the [H] ∼3×1017 cm−3 case were implanted in the samples. The formation of Li lean regions has been observed for [2H] <1019 cm−3 after annealing at 400 ∘C. This is attributed to Lii presence consequent to the diffusion of Zni created during the H/2H implantation process. Results extracted from the TDH measurements performed prior to the annealing at 400 ∘C evidence that Lii contributes to an increase in carrier concentration up to ∼1017 cm−3 by providing a donor level with an activation energy of ∼40 meV and thus is very close to the value of ∼47 meV expected for H in the oxygen site. The reaction dynamics analysis evidences that the amount of Lii introduced is decreasing at higher H implantation doses as a result of increasing VZn and H-VZn retrapping, reactions in which Lii is competing with H. Overall, due to Lii formation as well as the presence of Al the maximum percentage of the implanted H or 2H acting as a donor in the investigated range is found to be ≲ 2%, which is considerably lower than previously reported.
dc.languageEN
dc.titleRole of intrinsic and extrinsic defects in H implanted hydrothermally grown ZnO
dc.typeJournal article
dc.creator.authorSchifano, Ramon
dc.creator.authorJakiela, R
dc.creator.authorGaleckas, Augustinas
dc.creator.authorKopalko, K
dc.creator.authorHerklotz, Frank
dc.creator.authorJohansen, Klaus Magnus H
dc.creator.authorVines, Lasse
cristin.unitcode185,15,17,20
cristin.unitnameSenter for Materialvitenskap og Nanoteknologi fysikk
cristin.ispublishedtrue
cristin.fulltextoriginal
cristin.qualitycode1
dc.identifier.cristin1741236
dc.identifier.bibliographiccitationinfo:ofi/fmt:kev:mtx:ctx&ctx_ver=Z39.88-2004&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.jtitle=Journal of Applied Physics&rft.volume=126&rft.spage=&rft.date=2019
dc.identifier.jtitleJournal of Applied Physics
dc.identifier.volume126
dc.identifier.issue12
dc.identifier.doihttps://doi.org/10.1063/1.5115597
dc.identifier.urnURN:NBN:no-79089
dc.type.documentTidsskriftartikkel
dc.type.peerreviewedPeer reviewed
dc.source.issn0021-8979
dc.identifier.fulltextFulltext https://www.duo.uio.no/bitstream/handle/10852/75941/2/pubished_Schifano_JAP2019.pdf
dc.type.versionPublishedVersion
cristin.articleid125707
dc.relation.projectNFR/239895
dc.relation.projectNFR/255082


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