Abstract
The finite-temperature Hartree-Fock-Bogoliubov cranking equation predicts the most probable shape for Yb158 nuclei. At a spin-dependent critical temperature, there is a transition from prolate collective rotation to oblate noncollective rotation. For spins above 39, there is oblate noncollective rotation at all temperatures. However, inclusion of thermal shape fluctuations produces an average shape which is prolate collective at spins 40 and 50 and thermal excitation energy E*10 MeV.