1991
DOI: 10.1103/physrevc.43.484
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Shape coexistence inHg190

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Cited by 28 publications
(15 citation statements)
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“…Absolute monopole transition probabilities between the excited 0 + states and the groundstate have been measured in 19o-192-19~pb [81, and were used to deduce the mixing. [61, [7], [10] and [11]) and one would expect these bands to occur in the even Po isotopes as well. * Present address: CERN, CH-1211 Geneva, Switzerland Further away from the Z = 82 shell gap, coexisting bands have been observed in the Hg and Pt nuclei (see e.g.…”
Section: Introductionmentioning
confidence: 99%
“…Absolute monopole transition probabilities between the excited 0 + states and the groundstate have been measured in 19o-192-19~pb [81, and were used to deduce the mixing. [61, [7], [10] and [11]) and one would expect these bands to occur in the even Po isotopes as well. * Present address: CERN, CH-1211 Geneva, Switzerland Further away from the Z = 82 shell gap, coexisting bands have been observed in the Hg and Pt nuclei (see e.g.…”
Section: Introductionmentioning
confidence: 99%
“…Examples of such bands can be found in the even Hg and Pt isotopes where one band is built on the groundstate while the other one has a low-lying 0 § state as bandhead. [4]) and Pt (see e.g. Decay studies can be used for the identification and study of the low-spin members of the coexisting bands.…”
Section: Introductionmentioning
confidence: 99%
“…Recently, Gade et al [11] + states having different deformations are mixed because the E0 matrix element is sensitive to changes in the mean-square radius [12]. Strong E0 0 + 2 →0 + 1 transitions have been ob-served, for example, in 184,186,188,190 Hg [13,14,15,16] and 114,116,118,120,122 Sn [12] isotopes related to the shape coexistences. The relatively weak 984.8 keV transition in Fig.…”
mentioning
confidence: 99%