Beta-decay of 27/2− isomers in N =83 nuclei
Identifieur interne : 003133 ( Istex/Corpus ); précédent : 003132; suivant : 003134Beta-decay of 27/2− isomers in N =83 nuclei
Auteurs : R. Barden ; A. Plochocki ; D. Schardt ; B. Rubio ; M. Ogawa ; P. Kleinheinz ; R. Kirchner ; O. Klepper ; J. BlomqvistSource :
- Zeitschrift für Physik A Atomic Nuclei [ 0939-7922 ] ; 1988-03-01.
English descriptors
- KwdEn :
- Annual report, Atomic nuclei, Barden, Blomqvist, Channel number, Coincidence relationships, Coincidence spectra, Comparable intensities, Compound nuclei, Configuration assignments, Conversion electrons, Daughter nuclei, Decay branch, Decay branches, Decay scheme, Decay schemes, Excitation, Federal republic, Intense thulium, Isomer, Isomer decay, Isomeric, Isomeric transition, Kirchner, Kleinheinz, Klepper, Large number, Lsler, Mass separator, Miniorange spectrometer, Nucl, Nucleus, Phys, Present study, Proton shell, Respective parent nucleus, Shell model, Single particle state, Singles, Singles spectra, Singles spectrum, Tape station, Transition intensities, Transition strength, Yrast, Yrast levels, Yrast state, Yrast states.
- Teeft :
- Annual report, Atomic nuclei, Barden, Blomqvist, Channel number, Coincidence relationships, Coincidence spectra, Comparable intensities, Compound nuclei, Configuration assignments, Conversion electrons, Daughter nuclei, Decay branch, Decay branches, Decay scheme, Decay schemes, Excitation, Federal republic, Intense thulium, Isomer, Isomer decay, Isomeric, Isomeric transition, Kirchner, Kleinheinz, Klepper, Large number, Lsler, Mass separator, Miniorange spectrometer, Nucl, Nucleus, Phys, Present study, Proton shell, Respective parent nucleus, Shell model, Single particle state, Singles, Singles spectra, Singles spectrum, Tape station, Transition intensities, Transition strength, Yrast, Yrast levels, Yrast state, Yrast states.
Abstract
Abstract: In theN=83 nucleus151Er we observed the isomericE3 transition in conversion electron measurements following on-line mass separation and located its 0.6 s 27/2− isomer at 2.586 MeV. Gamma-ray data establish a 4.7(3)% Gamow-Tellerβ-decay branch proceeding to high-spin states above 2 MeV excitation in151Ho. A weakβ-decay branch of 0.7(3)% was also observed for the 0.5 s 27/2− isomer in the149Dy isotone, and it was established that a similar 27/2− E3-isomer does not occur in153Yb. First results on the151Tm and151Er ground-stateβ-decays are briefly discussed.
Url:
DOI: 10.1007/BF01294811
Links to Exploration step
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<front><div type="abstract" xml:lang="en">Abstract: In theN=83 nucleus151Er we observed the isomericE3 transition in conversion electron measurements following on-line mass separation and located its 0.6 s 27/2− isomer at 2.586 MeV. Gamma-ray data establish a 4.7(3)% Gamow-Tellerβ-decay branch proceeding to high-spin states above 2 MeV excitation in151Ho. A weakβ-decay branch of 0.7(3)% was also observed for the 0.5 s 27/2− isomer in the149Dy isotone, and it was established that a similar 27/2− E3-isomer does not occur in153Yb. First results on the151Tm and151Er ground-stateβ-decays are briefly discussed.</div>
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<abstract>Abstract: In theN=83 nucleus151Er we observed the isomericE3 transition in conversion electron measurements following on-line mass separation and located its 0.6 s 27/2− isomer at 2.586 MeV. Gamma-ray data establish a 4.7(3)% Gamow-Tellerβ-decay branch proceeding to high-spin states above 2 MeV excitation in151Ho. A weakβ-decay branch of 0.7(3)% was also observed for the 0.5 s 27/2− isomer in the149Dy isotone, and it was established that a similar 27/2− E3-isomer does not occur in153Yb. First results on the151Tm and151Er ground-stateβ-decays are briefly discussed.</abstract>
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<abstract xml:lang="en"><p>Abstract: In theN=83 nucleus151Er we observed the isomericE3 transition in conversion electron measurements following on-line mass separation and located its 0.6 s 27/2− isomer at 2.586 MeV. Gamma-ray data establish a 4.7(3)% Gamow-Tellerβ-decay branch proceeding to high-spin states above 2 MeV excitation in151Ho. A weakβ-decay branch of 0.7(3)% was also observed for the 0.5 s 27/2− isomer in the149Dy isotone, and it was established that a similar 27/2− E3-isomer does not occur in153Yb. First results on the151Tm and151Er ground-stateβ-decays are briefly discussed.</p>
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<Keyword>21.10.−k</Keyword>
<Keyword>27.60.+j</Keyword>
<Keyword>27.70.+q</Keyword>
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<ArticleNote Type="Misc"><SimplePara>This work is part of the doctoral dissertation of R. Barden, to be submitted to Johannes Gutenberg-Universität Mainz</SimplePara>
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<ArticleNote Type="Misc"><SimplePara>On leave from Tokyo Institute of Technology, Nagatsuda, Japan</SimplePara>
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Zn-beams which were vital for our measurements. For fruitful advise and productive discussions we are indebted to E. Roeckl and O. Schult.</SimplePara>
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<abstract lang="en">Abstract: In theN=83 nucleus151Er we observed the isomericE3 transition in conversion electron measurements following on-line mass separation and located its 0.6 s 27/2− isomer at 2.586 MeV. Gamma-ray data establish a 4.7(3)% Gamow-Tellerβ-decay branch proceeding to high-spin states above 2 MeV excitation in151Ho. A weakβ-decay branch of 0.7(3)% was also observed for the 0.5 s 27/2− isomer in the149Dy isotone, and it was established that a similar 27/2− E3-isomer does not occur in153Yb. First results on the151Tm and151Er ground-stateβ-decays are briefly discussed.</abstract>
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