Publication:
Disorder in KHCO 3 as Studied by EPR and DTA in Cu 2+ Doped and Gamma-Irradiated Single Crystals

dc.authorscopusid35555793900
dc.authorscopusid6603897211
dc.authorscopusid10042932200
dc.authorscopusid10039123000
dc.authorscopusid10042745400
dc.contributor.authorKöksal, F.
dc.contributor.authorKarabulut, B.
dc.contributor.authorDemr, D.
dc.contributor.authorÇbudak, H.
dc.contributor.authorKöseolu, R.
dc.date.accessioned2020-06-21T15:31:06Z
dc.date.available2020-06-21T15:31:06Z
dc.date.issued2005
dc.departmentOndokuz Mayıs Üniversitesien_US
dc.department-temp[Köksal] Fevzi, Department of Physics, Ondokuz Mayis University Faculty of Science and Arts, Samsun, Turkey; [Karabulut] Bünyamin, Chemistry Department, Ondokuz Mayis University Faculty of Science and Arts, Samsun, Turkey; [Demr] Dlek, Department of Physics, Ondokuz Mayis University Faculty of Science and Arts, Samsun, Turkey; [Çbudak] Hasan, Chemistry Department, Ondokuz Mayis University Faculty of Science and Arts, Samsun, Turkey; [Köseolu] Rahm, Halil Bayraktar Health Services Vocational College, Erciyes Üniversitesi, Kayseri, Kayseri, Turkeyen_US
dc.description.abstractKalicinite (KHCO 3 ) single crystals were investigated by the electron paramagnetric resonance (EPR) technique in their Cu 2+ doped and gamma-irradiated states. It is observed that the behavior of the spectrum is the same at ambient and low temperatures down to 113 K in consistence with the monoclinic symmetry of the crystal. However, when the temperature is increased to 313 K, only one site signals were observed at all orientations of the magnetic field for the Cu 2+ doped samples as the site splitted signals overlap at this temperature. Furthermore, for the gamma-irradiated crystals, two sites were observed for the induced and radicals at ambient temperature for an arbitrary orientation of the magnetic field. However, when the temperature is increased to 348 K, the signals due to the radical overlap indicating only one site, but the signals due to the radical do not and continue to indicate the presence of the two sites. Therefore, we conclude that this one site transition at 313 K is due to the disordering of the proton vacancies, as the charge compensation of Cu 2+ is fulfilled by K + and proton holes. This indicates that the proton vacancies come to disorder at 313 K and the protons get disordered at 348 K. The differential thermal analysis results show two small endothermic peaks for the Cu 2+ doped and gamma-irradiated samples at 313 and 348 K that were attributed to the disorder of the proton vacancies and protons, in consistency with the EPR results.en_US
dc.identifier.doi10.1080/10420150500340926
dc.identifier.endpage319en_US
dc.identifier.issn1042-0150
dc.identifier.issue8en_US
dc.identifier.scopus2-s2.0-29144511125
dc.identifier.scopusqualityQ3
dc.identifier.startpage313en_US
dc.identifier.urihttps://doi.org/10.1080/10420150500340926
dc.identifier.volume160en_US
dc.identifier.wosWOS:000233883000001
dc.identifier.wosqualityQ3
dc.language.isoenen_US
dc.publisherTaylor & Francis Ltden_US
dc.relation.ispartofRadiation Effects and Defects in Solidsen_US
dc.relation.journalRadiation Effects and Defects in Solidsen_US
dc.relation.publicationcategoryMakale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanıen_US
dc.rightsinfo:eu-repo/semantics/closedAccessen_US
dc.subjectCu 2+en_US
dc.subjectDisorderen_US
dc.subjectDopingen_US
dc.subjectDTAen_US
dc.subjectElectron Paramagnetic Resonanceen_US
dc.subjectGamma Irradiationen_US
dc.titleDisorder in KHCO 3 as Studied by EPR and DTA in Cu 2+ Doped and Gamma-Irradiated Single Crystalsen_US
dc.typeArticleen_US
dspace.entity.typePublication

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