<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>α</mml:mi></mml:math>Decay of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mmultiscripts><mml:mi mathvariant="normal">I</mml:mi><mml:mprescripts/><mml:none/><mml:mn>109</mml:mn></mml:mmultiscripts></mml:math>and Its Implications for the Proton Decay of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mmultiscripts><mml:mi>Sb</mml:mi><mml:mprescripts/><mml:none/><mml:mn>105</mml:mn></mml:mmultiscripts></mml:math>and the Astrophysical Rapid Proton-Capture Process
Аннотация
An $\ensuremath{\alpha}$-decay branch of $(1.4\ifmmode\pm\else\textpm\fi{}0.4)\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}4}$ has been discovered in the decay of $^{109}\mathrm{I}$, which predominantly decays via proton emission. The measured ${Q}_{\ensuremath{\alpha}}$ value of $3918\ifmmode\pm\else\textpm\fi{}21\text{ }\text{ }\mathrm{keV}$ allows the indirect determination of the $Q$ value for proton emission from $^{105}\mathrm{Sb}$ of $356\ifmmode\pm\else\textpm\fi{}22\text{ }\text{ }\mathrm{keV}$, which is approximately of 130 keV more bound than previously reported. This result is relevant for the astrophysical rapid proton-capture process, which would terminate in the $^{105}\mathrm{Sn}(p,\ensuremath{\gamma})^{106}\mathrm{Sb}(p,\ensuremath{\gamma})^{107}\mathrm{Te}(\ensuremath{\alpha}\mathrm{\text{decay}})^{103}\mathrm{Sn}$ cycle at the densities expected in explosive hydrogen burning scenarios, unless unusually strong pairing effects result in a $^{103}\mathrm{Sn}(p,\ensuremath{\gamma})^{104}\mathrm{Sb}(p,\ensuremath{\gamma})^{105}\mathrm{Te}(\ensuremath{\alpha}\mathrm{\text{decay}})^{101}\mathrm{Sn})$ cycle.
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