Band crossing and triaxiality in <sup>129</sup>Ce
R Aryaeinejad; D J G Love; A H Nelson; P J Nolan; P J Smith; D M Todd; P J Twin; R Aryaeinejad; Oliver Lodge Lab., Univ. of Liverpool, Liverpool, UK; D J G Love; Oliver Lodge Lab., Univ. of Liverpool, Liverpool, UK; A H Nelson; Oliver Lodge Lab., Univ. of Liverpool, Liverpool, UK; P J Nolan; Oliver Lodge Lab., Univ. of Liverpool, Liverpool, UK; P J Smith; Oliver Lodge Lab., Univ. of Liverpool, Liverpool, UK; D M Todd; Oliver Lodge Lab., Univ. of Liverpool, Liverpool, UK; P J Twin; Oliver Lodge Lab., Univ. of Liverpool, Liverpool, UK
Журнал:
Journal of Physics G: Nuclear Physics
Дата:
1984-07-01
Аннотация:
Gamma-ray decays from states in <sup>129</sup>Ce have been studied using <sup>16</sup>O-induced reactions on <sup>116</sup>Sn and <sup>117</sup>Sn targets. Previously known positive- and negative-parity bands have been extended to spins of <sup>31</sup>/<sub>2</sub> and <sup>39</sup>/<sub>2</sub>, respectively. Band crossings are seen for the first time in <sup>129</sup>Ce and occur near the same rotational frequency as the h<sub>11</sub>2/ proton band crossing in <sup>130</sup>Ce. The signature splittings in the bands are discussed in terms of the cranked shell model with a prolate deformation epsilon <sub>2</sub>=0.25. The data show that the one-quasiparticle bands based on the h<sub>11/2</sub> (523) 7/2 Nilsson orbit have gamma approximately -15 degrees (signature alpha =+<sup>1</sup>/<sub>2</sub>) and gamma approximately -30 degrees ( alpha =-<sup>1</sup>/<sub>2</sub>). After the band crossing, the three-quasiparticle bands (including two h<sub>11/2</sub> quasiprotons) have gamma approximately 0 degrees for both signatures. The positive-parity states corresponds to gamma approximately 0 degrees for both the one-quasiparticle and three-quasiparticle bands. The branching ratios have been used to deduce the ratio (g<sub>K</sub>-g<sub>R</sub>)/Q<sub>0</sub> as a function of rotational frequency. This ratio shows an increase when the backbending takes place.
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