<p>Within the context of the relativistic mean field (RMF) approach and proton-neutron quasi-particle random phase approximation (pn-QRPA) model, the nuclear ground state parameters, the Gamow Teller (GT) strength, and the stellar weak rates for <i>N</i>&#xa0;=&#xa0;60 have been analyzed. The ground-state deformation parameters (<InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\beta _2\)</EquationSource> </InlineEquation>), binding energies (BE), neutron separation energies (S<InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(_n\)</EquationSource> </InlineEquation>), nuclear radii (r<InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(_n\)</EquationSource> </InlineEquation>), neutron skin thickness (r<InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(_{np}\)</EquationSource> </InlineEquation>), and potential energy curves (PEC) were determined utilizing the RMF framework with density-dependent meson exchange interactions (DDME2). The computed <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(\beta _2\)</EquationSource> </InlineEquation> values, based on the RMF model and the finite range droplet model (FRDM) model, were used as free variables in the pn-QRPA framework to examine the GT strength distributions and stellar <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(\beta\)</EquationSource> </InlineEquation> decay rates. It is observed that the GT strength computed via the present recipe shows a good comparison with the existing data. Furthermore, the stellar electron emission (<InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(\lambda _{\beta ^{-}}\)</EquationSource> </InlineEquation>) and positron capture (<InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(\lambda _{pc}\)</EquationSource> </InlineEquation>) rates were computed for <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(^{96}\)</EquationSource> </InlineEquation>Kr, <InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(^{98}\)</EquationSource> </InlineEquation>Sr, <InlineEquation ID="IEq18"> <EquationSource Format="TEX">\(^{100}\)</EquationSource> </InlineEquation>Zr, <InlineEquation ID="IEq19"> <EquationSource Format="TEX">\(^{102}\)</EquationSource> </InlineEquation>Mo, <InlineEquation ID="IEq20"> <EquationSource Format="TEX">\(^{104}\)</EquationSource> </InlineEquation>Ru, and <InlineEquation ID="IEq21"> <EquationSource Format="TEX">\(^{106}\)</EquationSource> </InlineEquation>Pd at all densities and temperatures based on two different deformation parameters. Our analysis can be significant for the simulation of stellar weak rates near <i>N</i>&#xa0;=&#xa0;60 core nuclei.</p>

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Investigations of Nuclear Ground-State Properties and Stellar \(\beta\)-Decay Rates of N = 60 \(^{96}\)Kr, \(^{98}\)Sr, \(^{100}\)Zr, \(^{102}\)Mo, \(^{104}\)Ru and \(^{106}\)Pd Using RMF and pn-QRPA Models

  • Abdul Kabir,
  • Jameel-Un Nabi

摘要

Within the context of the relativistic mean field (RMF) approach and proton-neutron quasi-particle random phase approximation (pn-QRPA) model, the nuclear ground state parameters, the Gamow Teller (GT) strength, and the stellar weak rates for N = 60 have been analyzed. The ground-state deformation parameters ( \(\beta _2\) ), binding energies (BE), neutron separation energies (S \(_n\) ), nuclear radii (r \(_n\) ), neutron skin thickness (r \(_{np}\) ), and potential energy curves (PEC) were determined utilizing the RMF framework with density-dependent meson exchange interactions (DDME2). The computed \(\beta _2\) values, based on the RMF model and the finite range droplet model (FRDM) model, were used as free variables in the pn-QRPA framework to examine the GT strength distributions and stellar \(\beta\) decay rates. It is observed that the GT strength computed via the present recipe shows a good comparison with the existing data. Furthermore, the stellar electron emission ( \(\lambda _{\beta ^{-}}\) ) and positron capture ( \(\lambda _{pc}\) ) rates were computed for \(^{96}\) Kr, \(^{98}\) Sr, \(^{100}\) Zr, \(^{102}\) Mo, \(^{104}\) Ru, and \(^{106}\) Pd at all densities and temperatures based on two different deformation parameters. Our analysis can be significant for the simulation of stellar weak rates near N = 60 core nuclei.