Two-dimensional collective Hamiltonian for chiral and wobbling modes
arXiv:1609.06967 · doi:10.1103/PhysRevC.94.044301
Abstract
A two-dimensional collective Hamiltonian (2DCH) on both azimuth and polar motions in triaxial nuclei is proposed to investigate the chiral and wobbling modes. In the 2DCH, the collective potential and the mass parameters are determined from three-dimensional tilted axis cranking (TAC) calculations. The broken chiral and signature symmetries in the TAC solutions are restored by the 2DCH. The validity of the 2DCH is illustrated with a triaxial rotor () coupling to one proton particle and one neutron hole. By diagonalizing the 2DCH, the angular momenta and energy spectra are obtained. These results agree with the exact solutions of the particle rotor model (PRM) at high rotational frequencies. However, at low frequencies, the energies given by the 2DCH are larger than those by the PRM due to the underestimation of the mass parameters. In addition, with increasing angular momentum, the transitions from the chiral vibration to chiral rotation and further to longitudinal wobbling motion have been presented in the 2DCH.
30 pages, 12 figures
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- Recent progress in multiple chiral doublet bands
- Multi-chiral facets in symmetry restored states: Five chiral doublets candidates in even-even nucleus Nd
- A microscopic resolution of the chiral conundrum with crossing twin bands in Ag-106
- Possible chiral doublets in Ni
- Towards a new semi-classical interpretation of the wobbling motion in Lu
- The role of scalar and mass interactions in a relativistic model of the charmonium spectrum