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Highly deformed modes in the ab initio symplectic no-core shell model

T Dytrych1, K D Sviratcheva1, C Bahri1, J P Draayer1 and J P Vary2

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We show that highly deformed modes essential for nuclear dynamics modeling can readily be included in the symplectic no-core shell model (Sp-NCSM) space. In particular, a prescription for constructing general deformed k-particle–k-hole (kp–kh) translationally invariant symplectic \SpR{3} starting state configurations and symplectic excitations thereof in a fermion-based spherical harmonic oscillator basis is presented. This prescription is used to build the symplectic excitations over all possible 2\ensuremath{\hbar\Omega} \,\ph{2} as well as the most deformed 4\ensuremath{\hbar\Omega}\, \ph{4}\, \SpR{3} configurations in 12C and 16O. The extent to which these configurations enter into low-lying states for these nuclei calculated within the framework of the no-core shell model with a realistic microscopic interaction is then determined. Typically, the addition of these \ph{2} and \ph{4} representations to the leading \ph{0} results grow the overall overlap with the no-core-shell-model eigenstates by 5–10% for a total of 85–90%. And most importantly, even with the addition of these higher-order particle–hole configurations, the dimensionality of the symplectic subspace constitutes a very small fraction of the conventional full no-core shell model space, which reaffirms the relevance of the Sp-NCSM scheme.


PACS

21.60.Cs Shell model

21.10.Re Collective levels

27.20.+n 6(less-than-or-equal-to)A(less-than-or-equal-to)19

21.10.Pc Single-particle levels and strength functions

Subjects

Nuclear physics

Dates

Issue 9 (September 2008)

Received 9 May 2008

Published 25 July 2008



  1. Highly deformed modes in the ab initio symplectic no-core shell model

    T Dytrych et al 2008 J. Phys. G: Nucl. Part. Phys. 35 095101

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