Sum Rules for B(M1,0+ -> 1+) Strength in IBM-3 and IBM-4

Abstract

Sum rules for B(M1,0+1→1+i) strength are derived for even-even nuclei in the isospin-invariant forms of the IBM, IBM-3 and IBM-4, in the cases where the respective natural internal symmetries, isospin U(3) and U(6)⊃ SU(4), are conserved. Subsequently, the total strength is resolved into its component partial sums to the allowed isospins (and SU(4) representations in IBM-4). In cases where the usual IBM dynamical symmetries are also valid, a complete description of all B(M1,0+1→1+i) is given. In contrast to IBM-2, there is fragmentation of the strength even in the dynamical symmetry cases, for T≠ 0, over two states in IBM-3, and over three states in IBM-4. The presence of pn bosons in the ground state of the extended versions reduces the expected strength from that for IBM-2, allowing in principle the possibility of using B(M1) data for a given nucleus to infer which version is the most appropriate.

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