Publication:
Gamma Irradiation Damage Centres in KHCO3 Single Crystals

dc.authorscopusid35555793900
dc.authorscopusid6603897211
dc.contributor.authorKöksal, F.
dc.contributor.authorKarabulut, B.
dc.date.accessioned2020-06-21T15:50:30Z
dc.date.available2020-06-21T15:50:30Z
dc.date.issued1999
dc.departmentOndokuz Mayıs Üniversitesien_US
dc.department-temp[Köksal] Fevzi, Department of Physics, Ondokuz Mayis Üniversitesi, Samsun, Turkey; [Karabulut] Bünyamin, Department of Physics, Ondokuz Mayis Üniversitesi, Samsun, Turkeyen_US
dc.description.abstractPotassium bicarbonate single crystals were gamma irradiated and studied by electron paramagnetic resonance technique at room temperature. The species, responsible for the electron paramagnetic resonance spectrum, were found to be ̇CO<inf>2</inf>- and ḢCO<inf>3</inf> radicals. These species were found to be double in the unit cells of the single crystals. The principal values of the g tensors, the 13C hyperfine tensors in ̇CO<inf>2</inf>- and the hydrogen hyperfine tensors in ḢCO<inf>3</inf> were found for each site. The radicals, were found to be quite stable at room temperature and the hyperfine tensors of the 13C nucleus were well found for the crystals of natural abundancies of the constituent nuclei in ̇CO<inf>2</inf>- radical, but not in ḢCO<inf>3</inf>. This is attributed to the smallness of the hyperfine constant of the 13C nucleus in the ḢCO<inf>3</inf> radical.; Potassium bicarbonate single crystals were gamma irradiated and studied by electron paramagnetic resonance technique at room temperature. The species, responsible for the electron paramagnetic resonance spectrum, were found to be CO<inf>2</inf>- and HCO<inf>3</inf> radicals. These species were found to be double in the unit cells of the single crystals. The principal values of the g tensors, the 13C hyperfine tensors in CO<inf>2</inf>- and the hydrogen hyperfine tensors in HCO<inf>3</inf> were found for each site. The radicals, were found to be quite stable at room temperature and the hyperfine tensors of the 13C nucleus were well found for the crystals of natural abundancies of the constituent nuclei in CO<inf>2</inf>- radical, but not in HCO<inf>3</inf>. This is attributed to the smallness of the hyperfine constant of the 13C nucleus in the HCO<inf>3</inf> radical.en_US
dc.identifier.doi10.1016/S0969-806X(99)00195-4
dc.identifier.endpage376en_US
dc.identifier.issn1879-0895
dc.identifier.issue4en_US
dc.identifier.scopus2-s2.0-0345346380
dc.identifier.scopusqualityQ1
dc.identifier.startpage373en_US
dc.identifier.urihttps://doi.org/10.1016/S0969-806X(99)00195-4
dc.identifier.volume55en_US
dc.identifier.wosWOS:000081363500003
dc.identifier.wosqualityQ1
dc.language.isoenen_US
dc.publisherElsevier Science Ltden_US
dc.relation.ispartofRadiation Physics and Chemistryen_US
dc.relation.journalRadiation Physics and Chemistryen_US
dc.relation.publicationcategoryMakale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanıen_US
dc.rightsinfo:eu-repo/semantics/closedAccessen_US
dc.titleGamma Irradiation Damage Centres in KHCO3 Single Crystalsen_US
dc.typeArticleen_US
dspace.entity.typePublication

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