Discovery of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mmultiscripts><mml:mi>Xe</mml:mi><mml:mprescripts/><mml:none/><mml:mn>109</mml:mn></mml:mmultiscripts></mml:math>and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mmultiscripts><mml:mi>Te</mml:mi><mml:mprescripts/><mml:none/><mml:mn>105</mml:mn></mml:mmultiscripts></mml:math>: Superallowed<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>α</mml:mi></mml:math>Decay near Doubly Magic<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mmultiscripts><mml:mi>Sn</mml:mi><mml:mprescripts/><mml:none/><mml:mn>100</mml:mn></mml:mmultiscripts></mml:math>
Аннотация
Two new $\ensuremath{\alpha}$ emitters $^{109}\mathrm{Xe}$ and $^{105}\mathrm{Te}$ were identified through the observation of the $^{109}\mathrm{Xe}\ensuremath{\rightarrow}^{105}\mathrm{Te}\ensuremath{\rightarrow}^{101}\mathrm{Sn}$ $\ensuremath{\alpha}$-decay chain. The $^{109}\mathrm{Xe}$ nuclei were produced in the fusion-evaporation reaction $^{54}\mathrm{Fe}(^{58}\mathrm{Ni},3n)^{109}\mathrm{Xe}$ and studied using the Recoil Mass Spectrometer at the Holifield Radioactive Ion Beam Facility. Two transitions at ${E}_{\ensuremath{\alpha}}=4062\ifmmode\pm\else\textpm\fi{}7\text{ }\text{ }\mathrm{keV}$ and ${E}_{\ensuremath{\alpha}}=3918\ifmmode\pm\else\textpm\fi{}9\text{ }\text{ }\mathrm{keV}$ were interpreted as the $l=2$ and $l=0$ transitions from the $7/{2}^{+}$ ground state in $^{109}\mathrm{Xe}$ (${T}_{1/2}=13\ifmmode\pm\else\textpm\fi{}2\text{ }\text{ }\mathrm{ms}$) to the $5/{2}^{+}$ ground state and a $7/{2}^{+}$ excited state, located at $150\ifmmode\pm\else\textpm\fi{}13\text{ }\text{ }\mathrm{keV}$ in $^{105}\mathrm{Te}$. The observation of the subsequent decay of $^{105}\mathrm{Te}$ marks the discovery of the lightest known $\ensuremath{\alpha}$-decaying nucleus. The measured transition energy ${E}_{\ensuremath{\alpha}}=4703\ifmmode\pm\else\textpm\fi{}5\text{ }\text{ }\mathrm{keV}$ and half-life ${T}_{1/2}=620\ifmmode\pm\else\textpm\fi{}70\text{ }\text{ }\mathrm{ns}$ were used to determine the reduced $\ensuremath{\alpha}$-decay width ${\ensuremath{\delta}}^{2}$. The ratio ${\ensuremath{\delta}}_{^{105}\mathrm{Te}}^{2}/{\ensuremath{\delta}}_{^{213}\mathrm{Po}}^{2}$ of $\ensuremath{\sim}3$ indicates a superallowed character of the $\ensuremath{\alpha}$ emission from $^{105}\mathrm{Te}$.
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