Quantal rotation and its coupling to intrinsic motion in nuclei
arXiv:1605.01876 · doi:10.1088/0031-8949/91/7/073008
Abstract
Symmetry breaking is an importance concept in nuclear physics and other fields of physics. Self-consistent coupling between the mean-field potential and the single-particle motion is a key ingredient in the unified model of Bohr and Mottelson, which could lead to a deformed nucleus as a consequence of spontaneous breaking of the rotational symmetry. Some remarks on the finite-size quantum effects are given. In finite nuclei, the deformation inevitably introduces the rotation as a symmetry-restoring collective motion (Anderson-Nambu-Goldstone mode), and the rotation affects the intrinsic motion. In order to investigate the interplay between the rotational and intrinsic motions in a variety of collective phenomena, we use the cranking prescription together with the quasiparticle random phase approximation. At low spin, the coupling effect can be seen in the generalized intensity relation. A feasible quantization of the cranking model is presented, which provides a microscopic approach to the higher-order intensity relation. At high spin, the semiclassical cranking prescription works well. We discuss properties of collective vibrational motions under rapid rotation and/or large deformation. The superdeformed shell structure plays a key role in emergence of a new soft mode which could lead to instability toward the octupole shape. A wobbling mode of excitation, which is a clear signature of the triviality, is discussed in terms of a microscopic point of view. A crucial role played by the quasiparticle alignment is presented.
38 pages, 11 figures, Contribution to the Focus issue to celebrate the 40 year anniversary of the 1975 Nobel Prize
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- Microscopic description of oblate-prolate shape mixing in proton-rich Se isotopes
- A further look at prolate dominance in nuclear deformation
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Cited by in corpus (7)
- Beyond the Unified Model
- Two quasiparticle wobbling in the even-even nucleus 130Ba
- Rotational motion of triaxially deformed nuclei studied by microscopic angular-momentum-projection method II: Chiral doublet band
- Rotational motion of triaxially deformed nuclei studied by microscopic angular-momentum-projection method I: Nuclear wobbling motion
- Influence of moments of inertia on transverse wobbling mode in odd-mass nuclei
- Influence of triaxial deformation on wobbling motion in even-even nuclei
- Collective inertial masses in nuclear reactions