1981
DOI: 10.1103/physrevc.23.2078
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High spin states inYb156(N=86)

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Cited by 15 publications
(20 citation statements)
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“…Such a small value for ~el implies that 7 emission becomes important only when particle decay is energetically forbidden. In agreement with the results of many previous works [29][30][31] such values for the two parameters lead to the prediction of too many evaporated neutrons. For example, the maximum of the calculated 4n excitation function is shifted by ~ 5 MeV towards lower energy compared to the experimental data.…”
Section: ~2supporting
confidence: 90%
“…Such a small value for ~el implies that 7 emission becomes important only when particle decay is energetically forbidden. In agreement with the results of many previous works [29][30][31] such values for the two parameters lead to the prediction of too many evaporated neutrons. For example, the maximum of the calculated 4n excitation function is shifted by ~ 5 MeV towards lower energy compared to the experimental data.…”
Section: ~2supporting
confidence: 90%
“…The low lying odd parity yrast states in 153 Ho is reported [28] to arise from the coupling of h 11/2 proton to the yrast 2 + , 4 + , 6 + , 8 + states, probably of configuration ν(h 9/2 f 7/2 ), in 152 Dy. Similarly for 157 Lu [29], the observed level structure is almost identical with that of 156 Yb [30], upto spin 12 + .…”
Section: Discussionsupporting
confidence: 56%
“…High-spin states in 155 Yb were populated by using the fusion-evaporation reaction 144 The target consisted of a 2.89 mg/cm 2 144 Sm metallic foil with a 13.13 mg/cm 2 Pb backing. The in-beam γ rays were measured with the AFRODITE array [19], which consists of eight Compton suppressed clover detectors at the time of the experiment.…”
Section: Experiments and Resultsmentioning
confidence: 99%
“…For the eveneven Yb isotopes, the low-lying excitations exhibit a clear structural evolution with neutron number N . For instance, with N decreasing from 88 to 84, 158 Yb shows the behavior of soft rotation [1]; 156 Yb undergoes an evolution from a quasivibrational to quasirotational structure with increasing spin [2,3]; and 154 Yb is interpreted in terms of the quasiparticle coupling [4,5]. For the odd-A Yb isotopes in this transitional region, collective structures built on the f 7/2 , h 9/2 , and i 13/2 neutron orbitals have been observed in 157 Yb [6,7] and the coexistence of different nuclear shapes has been revealed.…”
Section: Introductionmentioning
confidence: 99%