Intruder structures observed in {sup 122}Te through inelastic neutron scattering

The excited levels of {sup 122}Te to 3.3- MeV excitation have been studied using {gamma}-ray spectroscopy following inelastic neutron scattering. The decay characteristics of these levels have been determined from {gamma}-ray excitation functions, angular distributions at E{sub n}-1.72,2.80, and 3.3...

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Veröffentlicht in:Physical review. C, Nuclear physics Nuclear physics, 2005-03, Vol.71 (3)
Hauptverfasser: Hicks, S.F., Alexander, G.K., Aubin, C.A., Burns, M.C., Collard, C.J., Walbran, M.M., Vanhoy, J.R., Jensen, E., Department of Physics, United States Naval Academy, Annapolis, Maryland 21402, Garrett, P.E., Martin, A., Warr, N., Kadi, M., Yates, S.W., Department of Chemistry, University of Kentucky, Lexington, Kentucky 40506-0055
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Sprache:eng
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Zusammenfassung:The excited levels of {sup 122}Te to 3.3- MeV excitation have been studied using {gamma}-ray spectroscopy following inelastic neutron scattering. The decay characteristics of these levels have been determined from {gamma}-ray excitation functions, angular distributions at E{sub n}-1.72,2.80, and 3.35 MeV, Doppler shifts, and {gamma}{gamma} coincidences. Electromagnetic transition rates were deduced for many levels, as were multipole-mixing and branching ratios. Level energies and electromagnetic transition rates were compared to interacting boson model (IBM) calculations, both with and without intruder-state mixing, and to particle-core coupling model calculations. The energies of low-lying levels of {sup 122}Te are well described by the IBM with intruder-state mixing calculations, and observed transition rates support emerging intruder bands built on 0{sup +} levels. The other models considered do not produce enough low-lying positive parity states; however, U(5) energies to the four quadrupole-phonon level agree very well with observations when states with large intruder configurations are ignored. Mixed-symmetry and quadrupole-octupole excitations have been investigated, but mixing with other configurations and fragmentation of strength prohibit a clear identification of these states.
ISSN:0556-2813
1089-490X
DOI:10.1103/PhysRevC.71.034307