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dc.contributor.authorChoi, Wonjun-
dc.contributor.authorAhn, Jongtae-
dc.contributor.authorKim, Ki-Tae-
dc.contributor.authorJin, Hye-Jin-
dc.contributor.authorHong, Sungjae-
dc.contributor.authorHwang, Do Kyung-
dc.contributor.authorIm, Seongil-
dc.date.accessioned2024-01-19T14:01:00Z-
dc.date.available2024-01-19T14:01:00Z-
dc.date.created2022-01-10-
dc.date.issued2021-09-
dc.identifier.issn0935-9648-
dc.identifier.urihttps://pubs.kist.re.kr/handle/201004/116503-
dc.description.abstractHighly crystalline 2D/3D-mixed p-transition metal dichalcogenide (TMD)/n-Ga2O3 heterojunction devices are fabricated by mechanical exfoliation of each p- and n-type material. N-type beta-Ga2O3 and p-type TMD separately play as a channel for junction field effect transistors (JFETs) with each type of carriers as well as materials for a heterojunction PN diode. The work thus mainly focuses on such ambipolar channel transistors with two different types of channel in a single device architecture. For more extended applications, the transparency of high energy band gap beta-Ga2O3 (E-g approximate to 4.8 eV) is taken advantage of, firstly to measure the electrical energy gap of p-TMDs receiving visible or near infrared (NIR) photons through the beta-Ga2O3. Next, the p-TMD/n-Ga2O3 JFETs are put to high speed photo-sensing which is achieved from the p-TMD channel under reverse bias voltages on n-Ga2O3. The photo-switching cutoff frequency appears to be approximate to 16 and 29 kHz for visible red and NIR illuminations, respectively, on the basis of -3 dB photoelectric power loss. Such a high switching speed of the JFET is attributed to the fast transport of photo-carriers in TMD channels. The 2D/3D-mixed ambipolar channel JFETs and their photo-sensing applications are regarded novel, promising, and practically easy to achieve.-
dc.languageEnglish-
dc.publisherWILEY-VCH Verlag GmbH & Co. KGaA, Weinheim-
dc.titleAmbipolar Channel p-TMD/n-Ga2O3 Junction Field Effect Transistors and High Speed Photo-sensing in TMD Channel-
dc.typeArticle-
dc.identifier.doi10.1002/adma.202103079-
dc.description.journalClass1-
dc.identifier.bibliographicCitationAdvanced Materials, v.33, no.38-
dc.citation.titleAdvanced Materials-
dc.citation.volume33-
dc.citation.number38-
dc.description.isOpenAccessN-
dc.description.journalRegisteredClassscie-
dc.description.journalRegisteredClassscopus-
dc.identifier.wosid000680000800001-
dc.identifier.scopusid2-s2.0-85111633942-
dc.relation.journalWebOfScienceCategoryChemistry, Multidisciplinary-
dc.relation.journalWebOfScienceCategoryChemistry, Physical-
dc.relation.journalWebOfScienceCategoryNanoscience & Nanotechnology-
dc.relation.journalWebOfScienceCategoryMaterials Science, Multidisciplinary-
dc.relation.journalWebOfScienceCategoryPhysics, Applied-
dc.relation.journalWebOfScienceCategoryPhysics, Condensed Matter-
dc.relation.journalResearchAreaChemistry-
dc.relation.journalResearchAreaScience & Technology - Other Topics-
dc.relation.journalResearchAreaMaterials Science-
dc.relation.journalResearchAreaPhysics-
dc.type.docTypeArticle-
dc.subject.keywordPlusLAYER-
dc.subject.keywordPlusHETEROJUNCTION-
dc.subject.keywordPlusTRANSITIONS-
dc.subject.keywordPlusELECTRONICS-
dc.subject.keywordPlusMONOLAYER-
dc.subject.keywordPlusOXIDE-
dc.subject.keywordAuthorambipolar channels-
dc.subject.keywordAuthorGa-
dc.subject.keywordAuthorO-2-
dc.subject.keywordAuthor(3)-
dc.subject.keywordAuthorheterojunction devices-
dc.subject.keywordAuthorjunction field effect transistors-
dc.subject.keywordAuthorphoto-sensing-
dc.subject.keywordAuthortransition metal dichalcogenide-
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