4.4 Article

Signatures for shape coexistence and shape/phase transitions in even-even nuclei

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IOP Publishing Ltd
DOI: 10.1088/1361-6471/acd70b

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shape coexistence; shape phase transitions; B(E2) transition rates

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Systematics of B(E2) transition rates connecting the first excited 0(2)(+) state to the first excited 2(1)(+) state of the ground state band in even-even nuclei indicates that shape coexistence is expected in nuclei within certain ranges of nucleon numbers, as predicted by the dual shell mechanism of the proxy-SU(3) model.
Systematics of B(E2) transition rates connecting the first excited 0(2)(+) state to the first excited 2(1)(+) state of the ground state band in even-even nuclei indicates that shape coexistence of the ground state band and the first excited K= 0 band should be expected in nuclei lying within the stripes of nucleon numbers 7-8, 17-20, 34-40, 59-70, 96-112 predicted by the dual shell mechanism of the proxy-SU(3) model, avoiding their junctions, within which high defor-mation is expected. Systematics of the excitation energies of the 0(2)(+) states in even-even nuclei show that shape coexistence due to proton-induced neutron particle-hole excitations is related to a first-order shape/phase transition from spherical to deformed shapes, while shape coexistence due to neutron-induced proton particle-hole excitations is observed along major proton shell closures.

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