SU(3) Symmetry in Atomic Nuclei by V. K. B. Kota
Author:V. K. B. Kota
Language: eng
Format: epub
ISBN: 9789811536038
Publisher: Springer Singapore
7.3.1 Introduction
Important multipolarity next to the quadrupole degree of freedom, in the low-lying levels of heavy nuclei, is the octupole and obviously here in IBM description, one has to include f (octupole) bosons with besides the s and d bosons. Then, we have the sdfIBM and this appears to be a good model as long as only octupole vibrational states are present. This model was analyzed in some detail and applied in some early works [41, 42]. Here, it is possible to have SU(3) in the form of just as we have discussed in the previous section the limit (it is also possible to consider coupled to more than one f boson). However, there is strong evidence that octupole deformation will also occur in nuclei and in this situation, Iachello and collaborators found that sdfIBM is inadequate. In particular in describing the low-lying bands and enhanced E1 strengths, it is found that the cure is to include not only f bosons but also p () bosons. This led to the development of sdpfIBM [43, 44]. It is important to recognize that enhanced E1 strengths can be described using (i) octupole mode [45]; (ii) -clustering and then there will be enhanced E1 transitions due to the oscillations of the cluster relative to the remaining part of the nucleus [46]; (iii) pigmy dipole resonance [47]. See Fig. 7.4 and Ref. [40]. In the sdpfIBM, the E1 strengths arise from the octupole mode via p bosons. Also, microscopic (shell model) studies showed clearly the need to include p bosons [48]. More likely the p boson arises from the collective low-lying valence shell excitation after removing the center-of-mass motion and then the p-state is collective with respect to the operator similar to the octupole operator [43].
The sdpfIBM admits a large number of dynamical symmetries (group–subgroup chains) [49–51] and here below, we will restrict our detailed discussion to the SU(3) limit of the model.
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