Surface, Nanomechanical, and Optical Properties of Mo-Doped GeGaAs Thin Film Deposited by Thermionic Vacuum Arc

MakaleAçık ErişimScopus SJRQ2

Özet

Mo-doped and undoped GeGaAs layers have been deposited by the thermionic vacuum arc (TVA) method, an alternative, fast plasma deposition technique. The thicknesses of the deposited layers were identical. The surface, mechanical, and optical properties of the deposited layers were studied to determine the influence of Mo doping on GeGaAs. The transparency of GeGaAs was shifted towards the near-infrared region by Mo doping. Bandgap values shifted by approximately 0.3 eV. In other words, the bandgap value of Mo-doped GeGaAs was nearly equal to that of GaAs materials. The average roughness and grain size of the Mo-doped material were smaller than for the GeGaAs layer. The particle distributions of the Mo-doped and undoped GeGaAs were almost perfect Gaussians. However, the mean height of the Mo-doped GeGaAs grains was six times that for undoped GeGaAs. The surface was homogeneous. The Mo-doped layer showed greater absorbance than the GeGaAs material. The produced Mo-doped sample showed hybrid properties.

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RDL Kalıcı Bağlantı (PID)
https://rdlopen.rawdatalibrary.net/r/bayburt/14176Resmi atıflarda kullanılan kalıcı adres
DOI
https://doi.org/10.1007/s11664-015-4140-7Yayıncı resmi DOI adresi
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1
OpenAlex
1
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AlanDeğerDil
dc.contributor.authorPat, Suat
dc.contributor.authorSenay, Volkan
dc.contributor.authorÖzen, Soner
dc.contributor.authorKorkmaz, Sadan
dc.date.accessioned2026-10-29T19:13:00.369455618Z
dc.date.available2026-10-29T19:13:00.369455618Z
dc.date.issued2016-01
dc.description.abstractMo-doped and undoped GeGaAs layers have been deposited by the thermionic vacuum arc (TVA) method, an alternative, fast plasma deposition technique. The thicknesses of the deposited layers were identical. The surface, mechanical, and optical properties of the deposited layers were studied to determine the influence of Mo doping on GeGaAs. The transparency of GeGaAs was shifted towards the near-infrared region by Mo doping. Bandgap values shifted by approximately 0.3 eV. In other words, the bandgap value of Mo-doped GeGaAs was nearly equal to that of GaAs materials. The average roughness and grain size of the Mo-doped material were smaller than for the GeGaAs layer. The particle distributions of the Mo-doped and undoped GeGaAs were almost perfect Gaussians. However, the mean height of the Mo-doped GeGaAs grains was six times that for undoped GeGaAs. The surface was homogeneous. The Mo-doped layer showed greater absorbance than the GeGaAs material. The produced Mo-doped sample showed hybrid properties.
dc.identifier.doi10.1007/s11664-015-4140-7
dc.identifier.eissn1543-186X
dc.identifier.endpage261
dc.identifier.issn0361-5235
dc.identifier.issue1
dc.identifier.startpage255
dc.identifier.urihttps://rdlopen.rawdatalibrary.net/r/bayburt/14176
dc.identifier.volume45
dc.identifier.wosWOS:000367467800030
dc.language.isoen
dc.publisherSPRINGER
dc.relation.ispartofJOURNAL OF ELECTRONIC MATERIALS
dc.rightsinfo:eu-repo/semantics/openAccess
dc.subjectMo doping
dc.subjectGe doping
dc.subjecthybrid properties
dc.subjectsurface characteristics
dc.subjectsurface free energy
dc.subject.classificationEngineering, Electrical & Electronic
dc.subject.classificationMaterials Science, Multidisciplinary
dc.subject.classificationPhysics, Applied
dc.subject.classificationEngineering
dc.subject.classificationMaterials Science
dc.subject.classificationPhysics
dc.subject.otherGAAS
dc.subject.otherDEFORMATION
dc.subject.otherINDENTATION
dc.titleSurface, Nanomechanical, and Optical Properties of Mo-Doped GeGaAs Thin Film Deposited by Thermionic Vacuum Arc
dc.typeArticle
rdl.citation.openalex1
rdl.citation.wos1
rdl.oa.statusclosed
rdl.oa.statusgreen
rdl.oa.urlhttp://hdl.handle.net/20.500.12403/3713
rdl.scopus.quartileQ2
rdl.source.indexWOS
rdl.wos.indexScience Citation Index Expanded (SCI-EXPANDED)