1980Physical Review CRequires access

β decay of Ca51

Alexander Huck, G. Klotz, A. Knipper, Ch. Miehé, C. Richard‐Serre, G. Walter, H.L. Ravn

Open publisher page 8 citations

Abstract

The new isotope $^{51}\mathrm{Ca}$ has been observed in the decay of $^{51}\mathrm{K}$ produced by fragmentation of a uranium target with 600-MeV protons. The half-life of $^{51}\mathrm{Ca}$ was determined to be 10.0\ifmmode\pm\else\textpm\fi{}0.8 s; the decay properties were established from $\ensuremath{\gamma}$-ray singles and coincidence measurements. The deexcitation scheme accounts for twenty-two $\ensuremath{\gamma}$ transitions between eleven levels in $^{51}\mathrm{Sc}$. Two states, located at 3039 and 3195 keV, can be related to the excitation of the odd proton in the $2p$ $\frac{3}{2}$ orbital.RADIOACTIVITY $^{51}\mathrm{Ca}$ from $p+U$ at 600 MeV $^{51}\mathrm{K}({\ensuremath{\beta}}^{\ensuremath{-}})$, natural target, mass separated, measured delayed ${E}_{\ensuremath{\gamma}}$, ${I}_{\ensuremath{\gamma}}$, $\ensuremath{\gamma}\ensuremath{-}\ensuremath{\gamma}$ coincidences, ${T}_{\frac{1}{2}}$, deduced decay scheme, $log\mathrm{ft}$, $J$, $\ensuremath{\pi}$.

About this research paper

What this paper is about

The new isotope $^{51}\mathrm{Ca}$ has been observed in the decay of $^{51}\mathrm{K}$ produced by fragmentation of a uranium target with 600-MeV protons. The half-life of $^{51}\mathrm{Ca}$ was determined to be 10.0\ifmmode\pm\else\textpm\fi{}0.8 s; the decay properties were established from $\ensuremath{\gamma}$-ray singles and coincidence measurements. The deexcitation scheme accounts for twenty-two $\ensuremath{\gamma}$ transitions between eleven levels in $^{51}\mathrm{Sc}$. Two states, located at 3039 and 3195 keV, can be related to the excitation of the odd proton in the $2p$ $\frac{3}{2}$ orbital.RADIOACTIVITY $^{51}\mathrm{Ca}$ from $p+U$ at 600 MeV $^{51}\mathrm{K}({\ensuremath{\beta}}^{\ensuremath{-}})$, natural target, mass separated, measured delayed ${E}_{\ensuremath{\gamma}}$, ${I}_{\ensuremath{\gamma}}$, $\ensuremath{\gamma}\ensuremath{-}\ensuremath{\gamma}$ coincidences, ${T}_{\frac{1}{2}}$, deduced decay scheme, $log\mathrm{ft}$, $J$, $\ensuremath{\pi}$.

Why it matters

OpenAlex reports 8 citations for this work. Citation counts describe recorded attention and do not establish research quality.

Key contribution

A contribution statement is not available in the OpenAlex record.

Method / approach

Method details are not available in the OpenAlex metadata.

Main findings

Findings are not separately available in the OpenAlex metadata.

Limitations

Limitations are not available in the OpenAlex metadata.

Applications

Application details are not available in the OpenAlex metadata.

Available abstract

The new isotope $^{51}\mathrm{Ca}$ has been observed in the decay of $^{51}\mathrm{K}$ produced by fragmentation of a uranium target with 600-MeV protons. The half-life of $^{51}\mathrm{Ca}$ was determined to be 10.0\ifmmode\pm\else\textpm\fi{}0.8 s; the decay properties were established from $\ensuremath{\gamma}$-ray singles and coincidence measurements. The deexcitation scheme accounts for twenty-two $\ensuremath{\gamma}$ transitions between eleven levels in $^{51}\mathrm{Sc}$. Two states, located at 3039 and 3195 keV, can be related to the excitation of the odd proton in the $2p$ $\frac{3}{2}$ orbital.RADIOACTIVITY $^{51}\mathrm{Ca}$ from $p+U$ at 600 MeV $^{51}\mathrm{K}({\ensuremath{\beta}}^{\ensuremath{-}})$, natural target, mass separated, measured delayed ${E}_{\ensuremath{\gamma}}$, ${I}_{\ensuremath{\gamma}}$, $\ensuremath{\gamma}\ensuremath{-}\ensuremath{\gamma}$ coincidences, ${T}_{\frac{1}{2}}$, deduced decay scheme, $log\mathrm{ft}$, $J$, $\ensuremath{\pi}$.

Key concepts: Physics, Atomic physics

Related papers

Back to paper searchBrowse research topicsOriginal source
β decay of Ca51 — Research Paper | ScholarLens