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A unified description of shape coexistence and mixed-symmetry states in 98Mo using IBM-2*
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Cheng-Fu Mu(穆成富),Da-Li Zhang(张大立)
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Table 3. Same as table 2, but normalized with respect to the largest $B(E2)$ transition strength of initial states ${3}_{1}^{+}$ and ${4}_{2}^{+}$, respectively. The experimental data are taken from [5].
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${J}_{i}^{\pi }\to {J}_{f}^{\pi }$ | $B(E2)$ |
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${3}_{1}^{+}\to {2}_{1}^{+}$ | 0.04(3) | 0.004 | ${3}_{1}^{+}\to {2}_{2}^{+}$ | 1 | 1 | ${3}_{1}^{+}\to {4}_{1}^{+}$ | $\lt 0.40$ | 0.24 | ${4}_{2}^{+}\to {2}_{1}^{+}$ | 0.04(1) | 0.01 | ${4}_{2}^{+}\to {2}_{2}^{+}$ | 0.88(11) | 1.45 | ${4}_{2}^{+}\to {4}_{1}^{+}$ | 1 | 1 |
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