Structure, optical spectroscopy and dispersion parameters of ZnGa2Se4 thin films at different annealing temperatures

dc.contributor.authorFadel, M.
dc.contributor.authorYahia, I. S.
dc.contributor.authorSakr, G. B.
dc.contributor.authorYakuphanoğlu, Fahrettin
dc.contributor.authorShenouda, S. S.
dc.date.accessioned2026-08-12T17:31:34Z
dc.date.issued2012
dc.departmentFırat Üniversitesi
dc.description.abstractThin films of ZnGa2Se4 were deposited by thermal evaporation method of pre-synthesized ingot material onto highly cleaned microscopic glass substrates. The chemical composition of the investigated compound thin film form was determined by means of energy-dispersive X-ray spectroscopy. X-ray diffraction XRD analysis revealed that the powder compound is polycrystalline and the as-deposited and the annealed films at T-a = 623 and 673 K have amorphous phase, while that annealed at T-a = 700 K is polycrystalline with a single phase of a defective chalcopyrite structure similar to that of the synthesized material. The unit-cell lattice parameters were determined and compared with the reported data. Also, the crystallite size L, the dislocation density delta and the main internal strain epsilon were calculated. Analyses of the AFM images confirm the nanostructure of the prepared annealed film at 700 K. The refractive index n and the film thickness d were determined from optical transmittance data using Swanepoel's method. It was found that the refractive index dispersion data obeys the single oscillator model from which the dispersion parameters were determined. The electric susceptibility of free carriers and the carrier concentration to the effective mass ratio were determined according to the model of Spitzer and Fan. The analysis of the optical absorption revealed both the indirect and direct energy gaps. The indirect optical gaps are presented in the amorphous films (as-deposited, annealed at 623 and 673 K), while the direct energy gap characterized the polycrystalline film at 700 K. Graphical representations of epsilon(1), epsilon(2), tan delta, - lm[1/epsilon*] and - lm[(1/epsilon* + 1)] are also presented. ZnGa2Se4 is a good candidate for optoelectronic and solar cell devices. (c) 2012 Elsevier B.V. All rights reserved.
dc.identifier.doi10.1016/j.optcom.2012.02.096
dc.identifier.endpage3161
dc.identifier.issn0030-4018
dc.identifier.issn1873-0310
dc.identifier.issue13-14
dc.identifier.orcid0000-0002-2907-1502
dc.identifier.orcid0000-0002-3156-471X
dc.identifier.orcid0000-0002-4721-268X
dc.identifier.scopus2-s2.0-84859773058
dc.identifier.scopusqualityQ2
dc.identifier.startpage3154
dc.identifier.urihttps://doi.org/10.1016/j.optcom.2012.02.096
dc.identifier.urihttps://hdl.handle.net/11508/56312
dc.identifier.volume285
dc.identifier.wosWOS:000303629900033
dc.identifier.wosqualityQ2
dc.indekslendigikaynakWeb of Science
dc.indekslendigikaynakScopus
dc.language.isoen
dc.publisherElsevier
dc.relation.ispartofOptics Communications
dc.relation.publicationcategoryMakale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanı
dc.rightsinfo:eu-repo/semantics/closedAccess
dc.snmzKA_WoS_20260511
dc.subjectDefect chalcopyrite
dc.subjectZnGa2Se4
dc.subjectOptical constants
dc.subjectOptical dispersion parameters
dc.subjectEffect of annealing
dc.titleStructure, optical spectroscopy and dispersion parameters of ZnGa2Se4 thin films at different annealing temperatures
dc.typeArticle

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