Three band crossings in the yrast structure of <sup>162</sup>Hf
C R Bingham; L L Riedinger; L H Courtney; Z M Liu; A J Larabee; M Craycraft; D J G Love; P J Nolan; A Kirwan; D Thornley; P Bishop; A H Nelson; M A Riley; J C Waddington; C R Bingham; Tennessee Univ., Knoxville, TN, USA; L L Riedinger; Tennessee Univ., Knoxville, TN, USA; L H Courtney; Tennessee Univ., Knoxville, TN, USA; Z M Liu; Tennessee Univ., Knoxville, TN, USA; A J Larabee; Tennessee Univ., Knoxville, TN, USA; M Craycraft; Tennessee Univ., Knoxville, TN, USA; D J G Love; Tennessee Univ., Knoxville, TN, USA; P J Nolan; Tennessee Univ., Knoxville, TN, USA; A Kirwan; Tennessee Univ., Knoxville, TN, USA; D Thornley; Tennessee Univ., Knoxville, TN, USA; P Bishop; Tennessee Univ., Knoxville, TN, USA; A H Nelson; Tennessee Univ., Knoxville, TN, USA; M A Riley; Tennessee Univ., Knoxville, TN, USA; J C Waddington; Tennessee Univ., Knoxville, TN, USA
Журнал:
Journal of Physics G: Nuclear Physics
Дата:
1988-05-01
Аннотация:
The yrast sequence of <sup>162</sup>Hf has been observed up to a level tentatively assigned as 38<sup>+</sup> and reveals a continuing rotational character up to that spin. Sharp backbends at rotational frequencies of 0.27 and 0.42 MeV/h are attributed to i<sub>13/2</sub> neutron and h<sub>11/2</sub> proton alignments, respectively. A gradual increase in the aligned angular momentum of the yrast levels between these two sharp backbends is attributed to the rotational alignment of a pair of negative parity quasineutrons (mostly h<sub>9/2</sub> in character). The interpretation of this effect is supported by the failure of the negative parity bands, which already contain this aligned h<sub>9/2</sub> neutron, to gain alignment in the same rotational frequency range. While the alignment of the h<sub>9/2</sub> quasineutrons has been predicted in the cranked shell model to occur in the rare-earth region with a large interaction strength, this represents the first clear observation of such a band crossing.
541Кб