Quadrupole-quadrupole interaction calculations which include N=2 mixing

preprint1996arXivOpen access

Abstract

We carry out a study of the study of the Q⋅QQ \cdot Q interaction in a model space which consists of several nucleons in an open shell and all 2ℏω2 \hbar ω excitations. This interaction is −t(Xo/2)Q⋅Q -t (X_o/2) Q \cdot Q, where for t=1 we get the `accepted strength'. In the 0p0p space, the spectrum would scale with tt. In this space, the 21+2^+_1 and 22+2^+_2 states of 10^{10}Be are degenerate, as are the [330] and [411] sets of J=0+,1+J=0^+, 1^+ and 2+2^+ triplets. When 2ℏω2 \hbar ω admixtures are included, the degeneracies are removed. For t≥1.8t \geq 1.8 we have new ground state and a new 21+2_1^+ state. These are states in which two particles are excited from the 0p0p to the 1s−0d1s-0d shell. There is no mixing of these 2p-2h states with the other states. For these 2p-2h states the occupancy for 0s,0p,1s-0d and 1p-of are 4,4,2 and 0 respectively.

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