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β-decay studies of neutron-rich K isotopes

F. PerrotInstitut de Recherches Subatomiques, IN2P3-CNRS et Universit Louis Pasteur, F-67037 Strasbourg Cedex 2, FranceFrançois MaréchalInstitut de Recherches Subatomiques, IN2P3-CNRS et Université Louis Pasteur, F-67037 Strasbourg Cedex 2, FranceC. JolletInstitut de Recherches Subatomiques, IN2P3-CNRS et Universit Louis Pasteur, F-67037 Strasbourg Cedex 2, FrancePh. DessagneInstitut de Recherches Subatomiques, IN2P3-CNRS et Universit Louis Pasteur, F-67037 Strasbourg Cedex 2, FranceJ. C. AngéliqueLaboratoire de Physique Corpusculaire, ENSICAEN et Université de Caen, IN2P3-CNRS, F-14050 Caen Cedex, FranceG. BanLaboratoire de Physique Corpusculaire, ENSICAEN et Universit de Caen, IN2P3-CNRS, F-14050 Caen Cedex, FranceP. BaumannInstitut de Recherches Subatomiques, IN2P3-CNRS et Universit Louis Pasteur, F-67037 Strasbourg Cedex 2, FranceF. BenrachiDepartment of Physics, Mentouri Constantine University, 25000 Constantine, AlgeriaU.C. BergmannISOLDE, Division EP, CERN, CH-1211 Geneva, SwitzerlandC. BorceaInstitute of Atomic Physics, IFIN-HH, Bucharest, RomaniaA. BuţăJ. CederkällISOLDE, Division EP, CERN, CH-1211 Geneva, SwitzerlandS. CourtinInstitut de Recherches Subatomiques, IN2P3-CNRS et Universit Louis Pasteur, F-67037 Strasbourg Cedex 2, FranceJ. M. DaugasCEA/DIF/DPTA/SPN, BP 12, F-91680 Bruyres-le-Chtel, FranceL. M. FraileISOLDE, Division EP, CERN, CH-1211 Geneva, SwitzerlandS. GrévyLaboratoire de Physique Corpusculaire, ENSICAEN et Université de Caen, IN2P3-CNRS, F-14050 Caen Cedex, FranceA. JokinenDepartment of Physics, University of Jyvskyl, FIN-40351 Jyvskyl, FinlandF.R. LecolleyLaboratoire de Physique Corpusculaire, ENSICAEN et Universit de Caen, IN2P3-CNRS, F-14050 Caen Cedex, FranceE. LiénardNuclear physicsG. Le ScornetISOLDE, Division EP, CERN, CH-1211 Geneva, SwitzerlandV. MéotCEA/DIF/DPTA/SPN, BP 12, F-91680 Bruyères-le-Châtel, FranceCh. MiehéInstitut de Recherches Subatomiques, IN2P3-CNRS et Université Louis Pasteur, F-67037 Strasbourg Cedex 2, FranceF. NegoiţăInstitute of Atomic Physics, IFIN-HH, Bucharest, RomaniaN. A. OrrLaboratoire de Physique Corpusculaire, ENSICAEN et Universit de Caen, IN2P3-CNRS, F-14050 Caen Cedex, FranceS. PiétriLaboratoire de Physique Corpusculaire, ENSICAEN et Universit de Caen, IN2P3-CNRS, F-14050 Caen Cedex, FranceÉ. PoirierInstitut de Recherches Subatomiques, IN2P3-CNRS et Universit Louis Pasteur, F-67037 Strasbourg Cedex 2, FranceM. RamdhaneNuclear physicsO. RoigCEA/DIF/DPTA/SPN, BP 12, F-91680 Bruyres-le-Chtel, FranceI. StefanInstitute of Atomic Physics, IFIN-HH, Bucharest, RomaniaWenzhong WangDepartment of Physics, University of Jyvskyl, FIN-40351 Jyvskyl, Finland
Physical Review Cjournal2006en
ABI

Abstract

The \ensuremath{\beta} decay of the neutron-rich nuclei $^{51\ensuremath{-}53}\mathrm{K}$ has been used to populate bound and unbound states in $^{50\ensuremath{-}53}\mathrm{Ca}$. Measurements of \ensuremath{\gamma} rays as well as \ensuremath{\beta}-delayed neutrons enabled detailed decay schemes to be established and levels identified in ${}^{50\ensuremath{-}53}$Ca. A delayed one-neutron emission probability ${P}_{1n}$ of $63\ifmmode\pm\else\textpm\fi{}8$% was determined for the decay of $^{51}\mathrm{K}$. A total of seven new \ensuremath{\gamma} transitions were observed following the decay of $^{51}\mathrm{K}$, and 25 neutron branches were found that enrich the level scheme of $^{51}\mathrm{Ca}$. Delayed neutron emission probabilities of ${P}_{1n}=74.4\ifmmode\pm\else\textpm\fi{}9.3$% and ${P}_{2n}=2.3\ifmmode\pm\else\textpm\fi{}0.3$% were determined for the decay of $^{52}\mathrm{K}$, and 12 new \ensuremath{\gamma} transitions were observed in $^{50,51,52}\mathrm{Ca}$. Three new \ensuremath{\gamma} transitions were observed in $^{52,53}\mathrm{Ca}$ following the \ensuremath{\beta} decay of $^{53}\mathrm{K}$. New limits on the ${P}_{1n}$ and ${P}_{2n}$ values were determined for the \ensuremath{\beta} decay of $^{53}\mathrm{K}$, and a decay scheme was established for $^{53}\mathrm{Ca}$ for the first time. The data obtained here should help clarify the structure of neutron-rich $\mathit{fp}$-shell nuclei around the $N=32\text{\ensuremath{-}}34$ subshell closures.

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