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- W2991826915 startingPage "1365" @default.
- W2991826915 abstract "Lifetimes were measured for ${mathrm{K}}^{39}$, ${mathrm{Ca}}^{41}$, and ${mathrm{Ca}}^{43}$ states formed by promoting a particle from the ${d}_{frac{3}{2}}$ shell to the ${f}_{frac{7}{2}}$ shell. In ${mathrm{Ca}}^{43}$, this state occurs at 990-keV excitation and has a mean life of 0.12 ifmmodepmelsetextpmfi{} 0.04 nsec. By taking account of the branching ratio we find that the partial mean life for the transition ${frac{3}{2}}^{+}ensuremath{rightarrow}{frac{7}{2}}^{ensuremath{-}}$ is 45 ifmmodepmelsetextpmfi{} 16 nsec. which represents an inhibition of 120 relative to the single-particle estimate. In ${mathrm{Ca}}^{41}$, the hole state occurs at 2010 keV and has a lifetime of 0.8 ifmmodepmelsetextpmfi{} 0.2 nsec. No other branch is observed, so this is the mean life for the ${frac{3}{2}}^{+}ensuremath{rightarrow}{frac{7}{2}}^{ensuremath{-}}$ transition. It is inhibited by a factor 62 relative to the single-particle estimate. In ${mathrm{K}}^{39}$ the state occurs at 2820 keV and the mean life for this ${frac{7}{2}}^{ensuremath{-}}ensuremath{rightarrow}{frac{3}{2}}^{+}$ transition is less than 0.08 nsec; the inhibition here is less than 18. All of the above rates are consistent with the theoretical model of Kurath and Lawson. From additional data on ${mathrm{Ca}}^{43}$, we find that the partial mean life for the 612-keV ${frac{3}{2}}^{+}ensuremath{rightarrow}{frac{5}{2}}^{ensuremath{-}}$ transition is 1.4 nsec. This is 0.06 times the single-particle value and is not explainable in the scheme of Kurath and Lawson." @default.
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- W2991826915 date "1970-10-01" @default.
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- W2991826915 title "Radiative Decay ofd32- Hole States" @default.
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- W2991826915 doi "https://doi.org/10.1103/physrevc.2.1365" @default.
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