Publication:
Thermal study and linear optical properties of (1 − x)TeO2–(x)PbF2 (x = 0.10, 0.15 and 0.25 mol) glasses

dc.contributor.coauthorKabalci I.
dc.contributor.coauthorÖzen G.
dc.contributor.coauthorÖveçoǧlu M.L.
dc.contributor.departmentDepartment of Physics
dc.contributor.facultymemberYes
dc.contributor.kuauthorSennaroğlu, Alphan
dc.contributor.schoolcollegeinstituteCollege of Sciences
dc.date.accessioned2024-11-09T22:49:26Z
dc.date.issued2006
dc.description.abstractThe (1 − x)TeO2–xPbF2 binary glass system was investigated by differential thermal analysis (DTA) and ultraviolet–visible-near-infrared (UV–VIS-NIR) absorption spectrophotometer. Samples were prepared by melting the mixture of TeO2 and PbF2 in a platinum crucible at 800 °C in air. Glass transition and the crystallization temperatures as function of the glass composition were measured by DTA. An exothermic peak of crystallization temperature was observed at about 340 ± 1 °C for all three samples. A second peak of peak crystallization temperature was observed at about 400 °C for only the sample with 0.15 mol PbF2. The mechanism and the activation energy for each crystallization peak were determined from the DTA curves measured with different heating rates between 5 and 20 °C/min. The mechanism of the crystallization was found to be surface crystallization for the first exothermic peak for only 0.15 mol PbF2 sample; on the other hand, bulk crystallization was found for all samples. Corresponding activation energies are 814, 748, and 387 kJ/mol for the samples with 0.10, 0.15 and, 0.25 mol PbF2, respectively. The mechanism and the activation energy for the second exothermic peak observed in the sample with 0.15 mol PbF2 were found to be bulk crystallization and 415 kJ/mol, respectively. The optical band gap, and Urbach energies were calculated from the absorption spectra measured between 300 and 800 nm at room temperature. The optical bandgap varies from 2.02 to 1.90 eV when the PbF2 content increases from 0.10 to 0.25 mol in the glass matrix.
dc.description.fulltextNo
dc.description.harvestedfromManual
dc.description.indexedbyWOS
dc.description.indexedbyScopus
dc.description.openaccessNO
dc.description.peerreviewstatusN/A
dc.description.publisherscopeInternational
dc.description.readpublishN/A
dc.description.sponsoredbyTubitakEuN/A
dc.description.studentonlypublicationNo
dc.description.studentpublicationNo
dc.description.versionN/A
dc.identifier.WoSQuartileQ2
dc.identifier.doi10.1016/j.jallcom.2005.09.062
dc.identifier.eissn1873-4669
dc.identifier.embargoN/A
dc.identifier.endpage298
dc.identifier.issn0925-8388
dc.identifier.issue1-2
dc.identifier.scopus2-s2.0-33745228782
dc.identifier.startpage294
dc.identifier.urihttps://doi.org/10.1016/j.jallcom.2005.09.062
dc.identifier.urihttps://hdl.handle.net/20.500.14288/6495
dc.identifier.volume419
dc.identifier.wos000238991900050
dc.keywordsTellurite glass
dc.keywordsThermal analysis
dc.keywordsActivation energy
dc.keywordsFiber laser
dc.language.isoeng
dc.publisherElsevier
dc.relation.affiliationKoç University
dc.relation.collectionKoç University Institutional Repository
dc.relation.ispartofJournal of Alloys and Compounds
dc.relation.openaccessN/A
dc.rightsN/A
dc.subjectMaterials science
dc.subjectGlass science
dc.subjectOptical materials
dc.titleThermal study and linear optical properties of (1 − x)TeO2–(x)PbF2 (x = 0.10, 0.15 and 0.25 mol) glasses
dc.typeJournal Article
dspace.entity.typePublication
local.contributor.kuauthorSennaroğlu, Alphan
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