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Highly deformed modes in the ab initio symplectic no-core shell model
T Dytrych, K D Sviratcheva, C Bahri, J P Draayer and J P Vary 2008 J. Phys. G: Nucl. Part. Phys. 35 095101 (12pp)   doi: 10.1088/0954-3899/35/9/095101


J. Phys. Soc. Jpn. (Japan) 44 (1978) 232-5

Alpha-clustering vs giant E2 excitations in 16O

K.T. Hecht
Phys. Dept., Univ. of Michigan, Ann Arbor, MI, USA

Abstract. The ( alpha +12C)-cluster model basis for 16O is compared with band systems generated by the infinitesimal operators of the noncompact group Sp(6,R), or more specifically its subgroup Sp(2,R) which generates SU(3) ladders ( lambda 0 mu 0) ( lambda 0+2, mu 0) ( lambda 0+4, mu 0)... based on np-nh states of the largest possible intrinsic deformation with n=0,...,5. Although the overlaps between the first symplectic excitations (essentially giant E2 excitations) and the corresponding alpha -cluster states range from .808 to .872, the higher symplectic excitations differ by more from the alpha -cluster states of the same ( lambda mu ). The alpha -cluster and symplectic excitations thus give a complementary description of core excitations in 16O

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