<p>This study investigates the <InlineEquation ID="IEq3"> <EquationSource Format="MATHML"><math> <mi>β</mi> </math></EquationSource> <EquationSource Format="TEX">$\beta $</EquationSource> </InlineEquation>-decay properties of <InlineEquation ID="IEq4"> <EquationSource Format="MATHML"><math> <mi>s</mi> <mi>d</mi> </math></EquationSource> <EquationSource Format="TEX">$sd$</EquationSource> </InlineEquation>-shell nuclei using the proton-neutron quasiparticle random phase approximation (pn-QRPA) model. The computed Gamow-Teller (GT) strength distributions show decent agreement with the measured data. The calculated <InlineEquation ID="IEq5"> <EquationSource Format="MATHML"><math> <mi>β</mi> </math></EquationSource> <EquationSource Format="TEX">$\beta $</EquationSource> </InlineEquation>-decay half-lives show good agreement with the previous shell model calculations. The computed log <InlineEquation ID="IEq6"> <EquationSource Format="MATHML"><math> <mtext mathvariant="italic">ft</mtext> </math></EquationSource> <EquationSource Format="TEX">$\textit{ft}$</EquationSource> </InlineEquation> values align well with the available experimental data, validating the consistency of the theoretical approach. A&#xa0;key advancement of this work is the calculation of stellar weak interaction rates performed without assuming the Brink-Axel hypothesis for the estimation of GT distributions from parent excited states. The sum of <InlineEquation ID="IEq7"> <EquationSource Format="MATHML"><math> <msup> <mi>β</mi> <mo>−</mo> </msup> </math></EquationSource> <EquationSource Format="TEX">$\beta ^{-}$</EquationSource> </InlineEquation> and positron capture (<InlineEquation ID="IEq8"> <EquationSource Format="MATHML"><math> <msup> <mi>β</mi> <mo>−</mo> </msup> </math></EquationSource> <EquationSource Format="TEX">$\beta ^{-}$</EquationSource> </InlineEquation>&#xa0;+ PC) rates were compared with earlier predictions from the shell model. The percentage contribution of <InlineEquation ID="IEq9"> <EquationSource Format="MATHML"><math> <msup> <mi>β</mi> <mo>−</mo> </msup> </math></EquationSource> <EquationSource Format="TEX">$\beta ^{-}$</EquationSource> </InlineEquation> and PC is also investigated under stellar conditions. At low density and high temperature (<InlineEquation ID="IEq10"> <EquationSource Format="MATHML"><math> <mi>ρ</mi> <mo>=</mo> <msup> <mrow> <mn>10</mn> </mrow> <mrow> <mn>7</mn> </mrow> </msup> <mtext>&#xa0;g</mtext> <mo stretchy="false">/</mo> <msup> <mtext>cm</mtext> <mn>3</mn> </msup> </math></EquationSource> <EquationSource Format="TEX">$\rho =10^{7}\text{ g}/\text{cm}^{3}$</EquationSource> </InlineEquation>, T&#xa0;=&#xa0;30 GK) the pn-QRPA calculation compare well with the shell model and differs at most by a factor 10. Our findings may provide crucial and refined nuclear inputs for astrophysical simulations of <InlineEquation ID="IEq11"> <EquationSource Format="MATHML"><math> <mi>r</mi> </math></EquationSource> <EquationSource Format="TEX">$r$</EquationSource> </InlineEquation>- and <InlineEquation ID="IEq12"> <EquationSource Format="MATHML"><math> <mi>s</mi> </math></EquationSource> <EquationSource Format="TEX">$s$</EquationSource> </InlineEquation>-process nucleosynthesis.</p>

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A re-examination of log \(\textit{ft}\) values and \(\beta \)-decay modes in sd-shell nuclei

  • Wajeeha Khalid,
  • Ammar Ahmed,
  • Anza,
  • Jameel-Un Nabi

摘要

This study investigates the β $\beta $ -decay properties of s d $sd$ -shell nuclei using the proton-neutron quasiparticle random phase approximation (pn-QRPA) model. The computed Gamow-Teller (GT) strength distributions show decent agreement with the measured data. The calculated β $\beta $ -decay half-lives show good agreement with the previous shell model calculations. The computed log ft $\textit{ft}$ values align well with the available experimental data, validating the consistency of the theoretical approach. A key advancement of this work is the calculation of stellar weak interaction rates performed without assuming the Brink-Axel hypothesis for the estimation of GT distributions from parent excited states. The sum of β $\beta ^{-}$ and positron capture ( β $\beta ^{-}$  + PC) rates were compared with earlier predictions from the shell model. The percentage contribution of β $\beta ^{-}$ and PC is also investigated under stellar conditions. At low density and high temperature ( ρ = 10 7  g / cm 3 $\rho =10^{7}\text{ g}/\text{cm}^{3}$ , T = 30 GK) the pn-QRPA calculation compare well with the shell model and differs at most by a factor 10. Our findings may provide crucial and refined nuclear inputs for astrophysical simulations of r $r$ - and s $s$ -process nucleosynthesis.