Phenomenological potential calculations for cluster decays

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dc.contributor.authorAsım Soylu
dc.date.accessioned2019-08-01T13:38:39Z
dc.date.available2019-08-01T13:38:39Z
dc.date.issued2017
dc.departmentNiğde ÖHÜ
dc.description.abstractThe half-lives of cluster decays from various nuclei having experimentally measured values have been calculatedby using the Wentzel{Kramers{Brillouin method together with the Bohr{Sommerfeld quantization condition for threedifferent types of phenomenological nuclear interactions: Woods{Saxon (WS), squared Woods{Saxon (WS-2), and mixedWoods{Saxon (mWS) potentials. By comparing the results with experimental values, rms values have been calculated.The half-lives of14C,15N,16O,17O,18O,20O,22O,23F,22Ne,24Ne,25Ne,26Ne,28Mg,30Mg, and34Si decays fromvarious isotopes whose experimental half-lives are unknown have also been calculated by using the WS, WS-2, and mWSpotentials. The obtained results have been compared with results of the liquid drop model, the Christensen{Wintherpotential form, and the Coulomb and proximity potential model. Even if the logarithmic values of the half-lives havesimilar behaviors, there are differences in size between the values. The present results provide useful information andextra theoretical data for future measurements of the unknown half-lives of possible cluster emissions from various nuclei
dc.description.abstractThe half-lives of cluster decays from various nuclei having experimentally measured values have been calculatedby using the Wentzel{Kramers{Brillouin method together with the Bohr{Sommerfeld quantization condition for threedifferent types of phenomenological nuclear interactions: Woods{Saxon (WS), squared Woods{Saxon (WS-2), and mixedWoods{Saxon (mWS) potentials. By comparing the results with experimental values, rms values have been calculated.The half-lives of14C,15N,16O,17O,18O,20O,22O,23F,22Ne,24Ne,25Ne,26Ne,28Mg,30Mg, and34Si decays fromvarious isotopes whose experimental half-lives are unknown have also been calculated by using the WS, WS-2, and mWSpotentials. The obtained results have been compared with results of the liquid drop model, the Christensen{Wintherpotential form, and the Coulomb and proximity potential model. Even if the logarithmic values of the half-lives havesimilar behaviors, there are differences in size between the values. The present results provide useful information andextra theoretical data for future measurements of the unknown half-lives of possible cluster emissions from various nuclei
dc.identifier.endpage226
dc.identifier.issn1300-0101
dc.identifier.issue3
dc.identifier.scopus2-s2.0-85021059259
dc.identifier.scopusqualityQ3
dc.identifier.startpage217
dc.identifier.trdizinid244437
dc.identifier.urihttps://app.trdizin.gov.tr/makale/TWpRME5ETTNOdz09
dc.identifier.urihttps://hdl.handle.net/11480/2333
dc.identifier.volume41
dc.identifier.wosWOS:000403695400004
dc.identifier.wosqualityN/A
dc.indekslendigikaynakWeb of Science
dc.indekslendigikaynakScopus
dc.indekslendigikaynakTR-Dizin
dc.institutionauthorAsım Soylu
dc.language.isoen
dc.relation.ispartofTurkish Journal of Physics
dc.relation.publicationcategoryMakale - Ulusal Hakemli Dergi - Kurum Öğretim Elemanı
dc.rightsinfo:eu-repo/semantics/openAccess
dc.subjectFizik
dc.subjectUygulamalı
dc.titlePhenomenological potential calculations for cluster decays
dc.typeArticle

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