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dc.contributor.author김은규-
dc.date.accessioned2017-10-23T02:38:07Z-
dc.date.available2017-10-23T02:38:07Z-
dc.date.issued2015-12-
dc.identifier.citationJOURNAL OF LUMINESCENCE, v. 168, Page. 288-292en_US
dc.identifier.issn0022-2313-
dc.identifier.issn1872-7883-
dc.identifier.urihttp://www.sciencedirect.com/science/article/pii/S0022231315004652?via%3Dihub-
dc.identifier.urihttp://hdl.handle.net/20.500.11754/30188-
dc.description.abstractGaN:Mn epilayers were grown on Al2O3 substrate uisng molecular beam epitaxy (MBE) and were subsequently implanted with Mn+ ions (1% and 10%). Photoluminescence (PL) with 1% of Mn showed that optical transitions related to Mn revealed the donor-Mn pair (D, Mn) at 2.5 eV and the electron-Mn pair (e, Mn) around 3.1 eV, and yellow luminescence (YL) around 2.20-2.25 eV. Photoluminescence (PL) with 10% of Mn showed the same but enhanced optical transitions as above. However, the new transitions around 1.65 eV for the sample with 10% which did not appeared with Mn of 1% were very weakly produced. The results of cathode-luminescence (CL) with 10% of Mn showed transitions related to Mn in PL together with new transitions around 1.72 eV. However, the new transitions around 1.72 eV for the sample with 10% according to high accelerating voltage were very remarkably activated in contrast with PL transitions which appeared were very weakly produced in samples with Mn of 10%. Transitions around 1.72 eV in CL correspond to though around 1.65 eV in PL This result means that deep donor (probably, V-N) is detected with increasing accelerating voltage and Mn-V-N complex is formed. This is supported by strong electron beam sensitivity of the IR emission bands. It is well known that heavy Mn doping ( ˃ similar to 10(19) C m(-3)) leads to a downshift of the Fermi level and promotes the formation of defect complexes of Mn-V-N. In our case, Mn doping concentration is ˃ similar to 10(21) C m(-3). Therefore, it is conjectured that the CL transition around 1.72 eV corresponds to Mn-V-N complex. (C) 2015 Elsevier B.V. All rights reserved.en_US
dc.description.sponsorshipThis work was supported by the National Research Foundation of Korea (NRF) Grant funded by Ministry of Education, Science and Technology (MEST) (Nos. NRF-2014R1A2A2A01007718, NRF-2014-066298, NRF-2014R1A2A1A11053936, NRF-2013R1A1A2008875, and NRF-2015R1A2A2A01004782) and by the Quntum-functional Research Center (QSRC) of Dongguk University and supported from the KIST Institutional Programme, including the Dream Project, the Converging Research Center Programme through the MEST (2012K001280).en_US
dc.language.isoenen_US
dc.publisherELSEVIER SCIENCE BVen_US
dc.subjectPhotoluminescence (PL)en_US
dc.subjectCathode-luminescence (CL)en_US
dc.subjectGaMnNen_US
dc.titleClarification of difference for transition between photoluminescence and cathode-luminescence based on GaMnNen_US
dc.typeArticleen_US
dc.relation.volume168-
dc.identifier.doi10.1016/j.jlumin.2015.08.025-
dc.relation.page288-292-
dc.relation.journalJOURNAL OF LUMINESCENCE-
dc.contributor.googleauthorLee, J. W.-
dc.contributor.googleauthorShon, Yoon-
dc.contributor.googleauthorSubramaniam, N. G.-
dc.contributor.googleauthorKwon, Y. H.-
dc.contributor.googleauthorKang, T. W.-
dc.contributor.googleauthorIm, Hyunsik-
dc.contributor.googleauthorKim, H. S.-
dc.contributor.googleauthorPark, C. S.-
dc.contributor.googleauthorKim, E. K.-
dc.contributor.googleauthorSong, J. D.-
dc.relation.code2015002474-
dc.sector.campusS-
dc.sector.daehakCOLLEGE OF NATURAL SCIENCES[S]-
dc.sector.departmentDEPARTMENT OF PHYSICS-
dc.identifier.pidek-kim-
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COLLEGE OF NATURAL SCIENCES[S](자연과학대학) > PHYSICS(물리학과) > Articles
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