1992
DOI: 10.1016/0370-1573(92)90095-h
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Coexistence in even-mass nuclei

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Cited by 685 publications
(545 citation statements)
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References 508 publications
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“…The appearance of shape coexistence in nuclei has attracted a lot of attention in recent decades [1,2,3] and compelling evidence has been obtained, in particular, at and very near to proton or neutron closed shells. The Pb region takes a prominent position because in addition to specific shell-model excitations established close to the N = 126 neutron shell closure, collective excitations have been observed for the neutron-deficient nuclei [4].…”
Section: Introductionmentioning
confidence: 99%
“…The appearance of shape coexistence in nuclei has attracted a lot of attention in recent decades [1,2,3] and compelling evidence has been obtained, in particular, at and very near to proton or neutron closed shells. The Pb region takes a prominent position because in addition to specific shell-model excitations established close to the N = 126 neutron shell closure, collective excitations have been observed for the neutron-deficient nuclei [4].…”
Section: Introductionmentioning
confidence: 99%
“…A rapid expansion of applications of the mean-field methods both with [1,2,3,4,5,6,7] and without [8,9,10,11] self-consistency gives rise to various important theoretical issues in the microscopic theory of many-body system. Among others, a property change in the single-particle states and its dynamical relation to the mean-field, a stability of the excited mean-field, a restoration dynamics of broken symmetries for the excited mean-fields and a dynamics of the single-particle level crossing are interesting subjects to be explored.…”
Section: Introductionmentioning
confidence: 99%
“…11 and 12, combined with the existing information on shape coexistence in the Pb region [1,3,4,5,6,7,8,9,10,11,12,13,14], stresses the conclusion that secondary minima in the PES (shape coexistence) are related to the distinct balance of prolate and oblate energy di erence of both protons and neutrons for a given con guration. Based on this observation, it is interesting to note that the Rn isotopes should beexpected to exhibit the same variety of coexisting shapes as the Po and Pb isotopes (close to spherical, oblate and prolate).…”
Section: Potential Energy Surface Calculationsmentioning
confidence: 82%
“…Its PCM wave function has a main (1h 9=2 1i 13=2 ) component in all the Po isotopes with N<126, but also a non-negligible ( 25%) 2 + (core) (1h 9=2 1i 13=2 ) admixture. The slight disagreement b e t w een the calculated and experimental energy of the 11 1 state, as shown in gure 4, is probably due to the reduced numberof model con gurations leading to this rather high spin, which results in some basis truncation e ects. A slightly lower single-particle energy for the 1i 13=2 orbital will improve the agreement for the 11 states.…”
Section: Resultsmentioning
confidence: 98%
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