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dc.contributor.authorJiao, Z.en
dc.contributor.authorYao, Q.en
dc.contributor.authorRudenko, A. N.en
dc.contributor.authorZhang, L.en
dc.contributor.authorZandvliet, H. J. W.en
dc.date.accessioned2021-08-31T15:08:39Z-
dc.date.available2021-08-31T15:08:39Z-
dc.date.issued2020-
dc.identifier.citationGermanium/MoS2: Competition between the growth of germanene and intercalation / Z. Jiao, Q. Yao, A. N. Rudenko, et al. — DOI 10.1103/PhysRevB.102.205419 // Physical Review B. — 2020. — Vol. 102. — Iss. 20. — 205419.en
dc.identifier.issn24699950-
dc.identifier.otherFinal2
dc.identifier.otherAll Open Access, Green3
dc.identifier.otherhttps://www.scopus.com/inward/record.uri?eid=2-s2.0-85097151365&doi=10.1103%2fPhysRevB.102.205419&partnerID=40&md5=3e62d2fb71566c0b439ebaa883340fce
dc.identifier.otherhttps://repository.ubn.ru.nl/bitstream/handle/2066/227108/1/227108.pdfm
dc.identifier.urihttp://elar.urfu.ru/handle/10995/103261-
dc.description.abstractWe have scrutinized the growth of germanium (Ge) on molybdenum disulfide (MoS2) using scanning tunneling microscopy and density functional theory calculations in order to resolve the still outstanding question whether Ge atoms prefer to intercalate between the MoS2 layers or rather form germanene islands on top of the MoS2 substrate. We found that, at a fixed growth temperature, germanene islands are formed on top of the MoS2 substrate at high deposition rates, whereas at low deposition rates the Ge intercalates between the MoS2 layers. Scanning tunneling spectra recorded on the germanene islands reveal a V-shaped density of states, which is one of the hallmarks of a two-dimensional Dirac material. The intercalated Ge clusters have a band gap of 0.5-0.6 eV. Density functional theory calculations have been conducted in order to study the stability and electronic band structure of several intercalated Ge cluster configurations. Based on these calculations we are able to identify two promising stable configurations that have a band gap that compares favorably well with the experimental observations. Scanning tunneling spectroscopy measurement recorded on the intercalated Ge clusters reveals signatures of Coulomb blockade. © 2020 American Physical Society.en
dc.description.sponsorshipThis work is part of the research program on 2D semiconductor crystals with Project No. FV157-TWOD, which is financed by the Netherlands Organization for Scientific Research (NWO). Z.J. thanks the China Scholarship Council for financial support. L.Z. acknowledges the financial support from the National Natural Science Foundation of China (Grants No. 11904094 and No. 51972106) and the Natural Science Foundation of Hunan, China (Grant No. 2019JJ50034).en
dc.format.mimetypeapplication/pdfen
dc.language.isoenen
dc.publisherAmerican Physical Societyen
dc.rightsinfo:eu-repo/semantics/openAccessen
dc.sourcePhys. Rev. B2
dc.sourcePhysical Review Ben
dc.subjectDENSITY FUNCTIONAL THEORYen
dc.subjectDEPOSITION RATESen
dc.subjectENERGY GAPen
dc.subjectGERMANIUM COMPOUNDSen
dc.subjectGERMANIUM METALLOGRAPHYen
dc.subjectLAYERED SEMICONDUCTORSen
dc.subjectMOLYBDENUM COMPOUNDSen
dc.subjectMOLYBDENUM METALLOGRAPHYen
dc.subjectSCANNING TUNNELING MICROSCOPYen
dc.subjectSUBSTRATESen
dc.subjectDENSITY OF STATEen
dc.subjectELECTRONIC BAND STRUCTUREen
dc.subjectGERMANIUMS (GE)en
dc.subjectHIGH DEPOSITION RATESen
dc.subjectMOLYBDENUM DISULFIDEen
dc.subjectSCANNING TUNNELING SPECTROSCOPYen
dc.subjectSTABLE CONFIGURATIONen
dc.subjectTUNNELING SPECTRAen
dc.subjectSULFUR COMPOUNDSen
dc.titleGermanium/MoS2: Competition between the growth of germanene and intercalationen
dc.typeArticleen
dc.typeinfo:eu-repo/semantics/articleen
dc.typeinfo:eu-repo/semantics/publishedVersionen
dc.identifier.doi10.1103/PhysRevB.102.205419-
dc.identifier.scopus85097151365-
local.contributor.employeeJiao, Z., Physics of Interfaces and Nanomaterials, MESA+ Institute for Nanotechnology, University of Twente, P.O. Box 217, Enschede, 7500AE, Netherlands
local.contributor.employeeYao, Q., Physics of Interfaces and Nanomaterials, MESA+ Institute for Nanotechnology, University of Twente, P.O. Box 217, Enschede, 7500AE, Netherlands
local.contributor.employeeRudenko, A.N., School of Physics and Technology, Wuhan University, Wuhan, 430072, China, Theoretical Physics and Applied Mathematics Department, Ural Federal University, Mira Strasse 19, Ekaterinburg, 620002, Russian Federation, Radboud University, Institute for Molecules and Materials, Heijendaalseweg 135, Nijmegen, 6525 AJ, Netherlands
local.contributor.employeeZhang, L., Hunan Provincial Key Laboratory of Low-Dimensional Structural Physics and Devices, School of Physics and Electronics, Hunan University, Changsha, 410082, China
local.contributor.employeeZandvliet, H.J.W., Physics of Interfaces and Nanomaterials, MESA+ Institute for Nanotechnology, University of Twente, P.O. Box 217, Enschede, 7500AE, Netherlands
local.issue20-
local.volume102-
dc.identifier.wos000589602000006-
local.contributor.departmentPhysics of Interfaces and Nanomaterials, MESA+ Institute for Nanotechnology, University of Twente, P.O. Box 217, Enschede, 7500AE, Netherlands
local.contributor.departmentSchool of Physics and Technology, Wuhan University, Wuhan, 430072, China
local.contributor.departmentTheoretical Physics and Applied Mathematics Department, Ural Federal University, Mira Strasse 19, Ekaterinburg, 620002, Russian Federation
local.contributor.departmentRadboud University, Institute for Molecules and Materials, Heijendaalseweg 135, Nijmegen, 6525 AJ, Netherlands
local.contributor.departmentHunan Provincial Key Laboratory of Low-Dimensional Structural Physics and Devices, School of Physics and Electronics, Hunan University, Changsha, 410082, China
local.identifier.pure826edc88-40d6-4afe-98d4-7c6ed5488523uuid
local.identifier.pure20231665-
local.description.order205419-
local.identifier.eid2-s2.0-85097151365-
local.identifier.wosWOS:000589602000006-
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