Publication:
EPR of Gamma Irradiated (CH3)3NHClO4, (CH3)3NHBF4 and [(CH3)4N]2ZnCl4 Single Crystals

dc.authorscopusid35555793900
dc.authorscopusid6601928035
dc.contributor.authorKöksal, F.
dc.contributor.authorKartal, I.
dc.date.accessioned2020-06-21T15:53:02Z
dc.date.available2020-06-21T15:53:02Z
dc.date.issued1998
dc.departmentOndokuz Mayıs Üniversitesien_US
dc.department-temp[Köksal] Fevzi, Department of Physics, Ondokuz Mayis University Faculty of Science and Arts, Samsun, Turkey; [Kartal] Ibrahim, Department of Physics, Ondokuz Mayis University Faculty of Science and Arts, Samsun, Turkeyen_US
dc.description.abstractGamma irradiation damage centres in (CH<inf>3</inf>)<inf>3</inf>NHClO<inf>4</inf>, (CH<inf>3</inf>)<inf>3</inf>NHBF<inf>4</inf> and [(CH<inf>3</inf>)<inf>4</inf>N]<inf>2</inf>ZnCl<inf>4</inf> were investigated by electron paramagnetic resonance spectroscopy at room temperature. The centres were found to be (CH<inf>3</inf>)<inf>3</inf>N+· and the hyperfine structure parameters for methyl protons and the nitrogen nucleus were determined. The results indicated that the (CH<inf>3</inf>)<inf>3</inf>N+· radical wholly performs reorientational motions around its C(3v) axis in addition to the reorientational motions of the methyl groups around their C(3v) axes. These results were compared with the earlier studies on (CH<inf>3</inf>)<inf>3</inf>N+· radical and discussed. Low temperature measurements on the first two of the title compounds were assessed.; Gamma irradiation damage centres in (CH<inf>3</inf>)<inf>3</inf>NHClO<inf>4</inf>, (CH<inf>3</inf>)<inf>3</inf>NHBF<inf>4</inf> and [(CH<inf>3</inf>)<inf>4</inf>N]<inf>2</inf>ZnCl<inf>4</inf> were investigated by electron paramagnetic resonance spectroscopy at room temperature. The centres were found to be (CH<inf>3</inf>)<inf>3</inf>N+· and the hyperfine structure parameters for methyl protons and the nitrogen nucleus were determined. The results indicated that the (CH<inf>3</inf>)<inf>3</inf>N+· radical wholly performs reorientational motions around its C<inf>3v</inf> axis in addition to the reorientatonal motions of the methyl groups around their C<inf>3v</inf> axes. These results were compared with the earlier studies on (CH<inf>3</inf>)<inf>3</inf>N+· radical and discussed. Low temperature measurements on the first two of the title compounds were assessed.en_US
dc.identifier.doi10.1016/S0969-806X(98)00199-6
dc.identifier.endpage504en_US
dc.identifier.issn1879-0895
dc.identifier.issue5en_US
dc.identifier.scopus2-s2.0-0038231223
dc.identifier.scopusqualityQ1
dc.identifier.startpage501en_US
dc.identifier.urihttps://doi.org/10.1016/S0969-806X(98)00199-6
dc.identifier.volume53en_US
dc.identifier.wosWOS:000075883200009
dc.identifier.wosqualityQ1
dc.language.isoenen_US
dc.publisherElsevier Sci 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.titleEPR of Gamma Irradiated (CH3)3NHClO4, (CH3)3NHBF4 and [(CH3)4N]2ZnCl4 Single Crystalsen_US
dc.typeArticleen_US
dspace.entity.typePublication

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