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dc.contributor.authorIlik, E.en
dc.contributor.authorKilic, G.en
dc.contributor.authorIssever, U. G.en
dc.contributor.authorIssa, S. A. M.en
dc.contributor.authorZakaly, H. M. H.en
dc.contributor.authorTekin, H. O.en
dc.date.accessioned2022-05-12T08:21:38Z-
dc.date.available2022-05-12T08:21:38Z-
dc.date.issued2022-
dc.identifier.citationCerium (IV) Oxide Reinforced Lithium-Borotellurite Glasses: A Characterization Study Through Physical, Optical, Structural and Radiation Shielding Properties / E. Ilik, G. Kilic, U. G. Issever et al. // Ceramics International. — 2022. — Vol. 48. — Iss. 1. — P. 1152-1165.en
dc.identifier.issn0272-8842-
dc.identifier.otherAll Open Access, Bronze3
dc.identifier.urihttp://elar.urfu.ru/handle/10995/111732-
dc.description.abstractThe purpose of this study was to characterize the structural, optical, and physical properties of various kinds of glasses based on the 50TeO2–30B2O3-(20-x)Li2O-xCeO2 system (x = 0, 0.5, 1, 2, 3, 4, 5, 10, 15, 20). Consequently, ten glass samples were produced by melting-annealing. Calculations of the densities of the synthesized glasses were performed using the Archimedes technique. The sample's structural, optical, physical, and radiation interaction properties were determined using XRD analysis, Raman spectroscopy, and advanced modelling techniques with FLUKA code, yielding optical band gap, refractive index, and Urbach energy values. By increasing the CeO2 reinforcement from 0 to 20 mol %, the glass densities rose from 4.0614 to 4.7519 g cm−3. The transmittance spectra of TBLC glasses were found in the range of 200–1100 nm. Our findings showed that the lowest Urbach energy belonged to the TBLC1 sample, and the highest Urbach energy belonged to the TBLC20 sample. When the CeO2 ratio was raised, the optical transmittance and absorption characteristics changed nearly monotonically, suggesting that these qualities may be calculated and controlled using the CeO2 additive, as shown in this experiment. By substituting CeO2 for Li2O inside the structure, it was possible to substantially enhance the optical band gap. Additionally, at simulated energies greater than 0.02 MeV, the gamma-ray linear attenuation coefficient rises monotonically with CeO2 reinforcement. Consequently, linear attenuation coefficients were reported as 125.843 cm−1, 127.601 cm−1, 129.211 cm−1, 132.312 cm−1, 135.166 cm−1, 138.705 cm−1, 141.288 cm−1, 156.690 cm−1, 172.393 cm−1, 186.811 cm−1 for TBLC0, TBLC0.5, TBLC1, TBLC2, TBLC3, TBLC4, TBLC5, TBL10, TBLC15 and TBLC20 at 0.015 MeV, respectively. It can be concluded that combination of high-concentration CeO2 and TeO2–B2O3 glass is an excellent synergetic tool for combining structural, optical, and radiation properties when combined with other materials. © 2021 Elsevier Ltd and Techna Group S.r.l.en
dc.description.sponsorshipThe research activity is supported by Eskisehir Osmangazi University, Scientific Research Council with grant number 202019D20.en
dc.format.mimetypeapplication/pdfen
dc.language.isoenen
dc.publisherElsevier Ltden1
dc.publisherElsevier BVen
dc.rightsinfo:eu-repo/semantics/openAccessen
dc.sourceCeram Int2
dc.sourceCeramics Internationalen
dc.subjectCERIUM (IV) OXIDEen
dc.subjectFLUKAen
dc.subjectGAMMA-RAY SHIELDINGen
dc.subjectOPTICAL PROPERTIESen
dc.subjectRAMAN SPECTRAen
dc.subjectXRDen
dc.subjectCERIUM OXIDEen
dc.subjectGAMMA RAYSen
dc.subjectGLASSen
dc.subjectOPTICAL BAND GAPSen
dc.subjectQUALITY CONTROLen
dc.subjectRAMAN SCATTERINGen
dc.subjectREFRACTIVE INDEXen
dc.subjectREINFORCEMENTen
dc.subjectX RAY DIFFRACTIONen
dc.subjectCHARACTERIZATION STUDIESen
dc.subjectFLUKAen
dc.subjectGAMMA-RAY SHIELDINGen
dc.subjectGLASS SAMPLESen
dc.subjectLINEAR ATTENUATION COEFFICIENTSen
dc.subjectOPTICAL-en
dc.subjectSHIELDING PROPERTIESen
dc.subjectSYNTHESISEDen
dc.subjectURBACH ENERGYen
dc.subjectXRDen
dc.subjectENERGY GAPen
dc.titleCerium (IV) Oxide Reinforced Lithium-Borotellurite Glasses: A Characterization Study Through Physical, Optical, Structural and Radiation Shielding Propertiesen
dc.typeArticleen
dc.typeinfo:eu-repo/semantics/articleen
dc.typeinfo:eu-repo/semantics/publishedVersionen
dc.identifier.rsi47524845-
dc.identifier.doi10.1016/j.ceramint.2021.09.200-
dc.identifier.scopus85118799368-
local.contributor.employeeIlik, E., Eskisehir Osmangazi University, Faculty of Science and Letters, Department of Physics, Eskisehir, TR-26040, Turkey; Kilic, G., Eskisehir Osmangazi University, Faculty of Science and Letters, Department of Physics, Eskisehir, TR-26040, Turkey; Issever, U.G., Eskisehir Osmangazi University, Faculty of Science and Letters, Department of Physics, Eskisehir, TR-26040, Turkey; Issa, S.A.M., Department of Physics, Faculty of Science, University of Tabuk, Tabuk, Saudi Arabia, Physics Department, Faculty of Science, Al-Azhar University, Assiut, 71452, Egypt; Zakaly, H.M.H., Physics Department, Faculty of Science, Al-Azhar University, Assiut, 71452, Egypt, Institute of Physics and Technology, Ural Federal University, Ekaterinburg, 620000, Russian Federation; Tekin, H.O., Medical Diagnostic Imaging Department, College of Health Sciences, University of Sharjah, Sharjah, 27272, United Arab Emirates, Medical Radiation Research Center (USMERA), Uskudar University, Istanbul, 34672, Turkeyen
local.description.firstpage1152-
local.description.lastpage1165-
local.issue1-
local.volume48-
dc.identifier.wos000722522600001-
local.contributor.departmentEskisehir Osmangazi University, Faculty of Science and Letters, Department of Physics, Eskisehir, TR-26040, Turkey; Department of Physics, Faculty of Science, University of Tabuk, Tabuk, Saudi Arabia; Physics Department, Faculty of Science, Al-Azhar University, Assiut, 71452, Egypt; Institute of Physics and Technology, Ural Federal University, Ekaterinburg, 620000, Russian Federation; Medical Diagnostic Imaging Department, College of Health Sciences, University of Sharjah, Sharjah, 27272, United Arab Emirates; Medical Radiation Research Center (USMERA), Uskudar University, Istanbul, 34672, Turkeyen
local.identifier.pure28944784-
local.identifier.eid2-s2.0-85118799368-
local.identifier.wosWOS:000722522600001-
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