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Dipole bands and multi-quasiparticle excitations in193Pb
Authors:L Ducroux  A Astier  R Duffait  Y Le Coz  M Meyer  S Perries  N Redon  J F Sharpey-Schafer  A N Wilson  R Lucas  V Méot  R Collatz  I Deloncle  F Hannachi  A Lopez-Martens  M G Porquet  C Schück  F Azaiez  S Bouneau  C Bourgeois  A Korichi  N Poffé  H Sergolle  B J P Gall  I Hibbert  R Wadsworth
Institution:1. Institut de Physique Nucléaire de Lyon, IN2P3/CNRS, Université C. Bernard Lyon-1, F-69622, Villeurbanne Cedex, France
3. Oliver Lodge Laboratory, University of Liverpool, PO Box 147, L69 3BX, Liverpool, UK
5. DAPNIA/SPhN, CEA Saclay, F-91191, Gif-sur-Yvette Cedex, France
6. Centre de Spectrométrie Nucléaire et de Spectroscopie de Masse, IN2P3/CNRS, Bat. 104, F-91405, Orsay Campus, France
7. Institut de Physique Nucléaire, IN2P3/CNRS, Bat. 104, F-91406, Orsay Campus, France
9. Centre de Recherches Nucléaires de Strasbourg, IN2P3/CNRS, BP 28, F-67037, Strasbourg Cedex 2, France
10. Department of Physics, University of York, PO1 5DD, Heslington, York, UK
Abstract:The nucleus193Pb was populated via the168Er(30Si,5n) reaction at a beam energy of 159 MeV and studied with the EUROGAM II spectrometer. Five new dipoleΔI=1 cascades have been found. These structures have been connected to the level scheme which has been considerably extended up to a spin of 61/2? and an excitation energy of about 8 MeV. Angular distribution coefficients,α 2, have been measured and confirm the dipole character of the in-band transitions. B(M1)/B(E2) ratios have been extracted for the two most intense cascades. The193Pb dipole bands are discussed in comparison with those known in odd lead isotopic series and the structure of the band heads is analyzed in terms of microscopic HF-BCS calculations. The proposed configurations are based on a high-K two quasiproton excitation,π(505]9/2??606]13/2+) K =11?, coupled to one or three rotation aligned quasineutrons involving thei 13/2,p 3/2,f 5/2 and/orh 9/2 subshells. The main difference, compared with the heavier lead isotopes, is the presence of largeΩ orbitals from theν (i 13/2) shell near the Fermi surface which are responsible for the increasing band-head spin as A decreases.
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