<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow><mml:mi>β</mml:mi></mml:mrow><mml:mrow><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math>/electron-capture decay of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mmultiscripts><mml:mrow /><mml:mprescripts /><mml:mrow /><mml:mrow><mml:mn>192</mml:mn></mml:mrow><mml:mrow /><mml:mrow /></mml:mmultiscripts></mml:mrow></mml:math>,194,196,1

Duppen, P. Van; Coenen, E.; Deneffe, K.; Huyse, M.; Wood, John L.

doi:10.1103/physrevc.35.1861

Cited by 69 publications
(16 citation statements)

References 24 publications

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“…3(b)] is of key importance for our calculations. In this isotope, an even-spin side band exhibiting the characteristics of a collective band has been measured and is understood as a 2p-2h intruder band [10,31,35]. Similar to the previously discussed isotopes, Band I is a mainly 2p-2h band and Band II is a mainly 4p-4h band.…”

Section: Resultssupporting
confidence: 63%

Configuration mixing in the neutron-deficientPb186−196isotopes
Hellemans
¹
,
Baerdemacker
²
,
Heyde
³

2008
Phys. Rev. C
24
1
35
1
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In this article we report the results of detailed interacting boson model calculations with configuration mixing for the neutron-deficient Pb isotopes. Calculated energy levels and B(E2) values for 188−196 Pb are discussed and some care is suggested concerning the current classification on the basis of level systematics of the 4 + 1 and 6 + 1 states in 190−194 Pb. Furthermore, quadrupole deformations are extracted for 186−196 Pb and the mixing between the different families (0p-0h, 2p-2h, and 4p-4h) is discussed in detail. Finally, the experimental and the theoretical level systematics are compared.

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Section: Resultssupporting
confidence: 63%

Configuration mixing in the neutron-deficientPb186−196isotopes
Hellemans
¹
,
Baerdemacker
²
,
Heyde
³

2008
Phys. Rev. C
24
1
35
1
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show abstract

“…We have chosen the Skyrme interaction SLy6 in the mean-field channel [31] and a density-dependent zero-range pairing force with a strength of −1250 MeV fm 3 for neutrons and protons in connection with a soft cutoff at 5 MeV above and below the Fermi energy as defined in Ref. [32].…”

Section: Frameworkmentioning
confidence: 99%

Configuration mixing of angular momentum projected self-consistent mean-field states for neutron-deficient Pb isotopes
Bender
¹
,
Bonche
²
,
Duguet
³

et al. 2004
Phys. Rev. C
135
19
182
3
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We study the low-lying collective excitation spectra of the neutron-deficient lead isotopes [182][183][184][185][186][187][188][189][190][191][192][193][194] Pb by performing a configuration mixing of angular momentum and particle-number projected self-consistent meanfield states. The same effective interaction is used to generate the mean-field states and for the configuration mixing. We choose the Skyrme interaction SLy6 supplemented by a density-dependent zero-range pairing force. Our study supports the interpretation of the excitation spectra made on the grounds of more schematic models in terms of coexisting spherical, oblate, prolate, and superdeformed prolate structures. The model qualitatively reproduces the variation of the spectra with neutron number. Our results for E0 and E2 transition probabilities are compared with the few existing experimental data. Finally, we predict the presence of superdeformed bands at low excitation energy in the most neutron-deficient isotopes.

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“…Information on the mixing between the ground-state spherical and the intruder deformed configuration has been deduced for the Pb nuclei (192≤A≤196) 109,110 and for the Hg nuclei (184≤A≤190) 111,112 . For the Hg nuclei (180≤A≤188), the mixing amplitude, deduced from ρ 2 (E0) values 111 and from α-decay studies 112 , is given in Figure 28.…”

Section: E Nuclei That Exhibit Shape Coexistence and Intruder Statesmentioning
confidence: 99%

Electric monopole transitions from low energy excitations in nuclei
Wood
¹
,
Zganjar
²
,
Coster³
et al. 1999
Nuclear Physics A
233
17
223
0
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Electric monopole (E0) properties are studied across the entire nuclear mass surface. Besides an introductory discussion of various model results (shell model, geometric vibrational and rotational models, algebraic models), we point out that many of the largest E0 transition strengths, ρ 2 (E0), are associated with shape mixing. We discuss in detail the manifestation of E0 transitions and present extensive data for : single-closed shell nuclei, vibrational nuclei, well-deformed nuclei, nuclei that exhibit sudden ground-state changes, and nuclei that exhibit shape coexistence and intruder states. We also give attention to light nuclei, odd-A nuclei, and illustrate a suggested relation between ρ 2 (E0) and isotopic shifts.

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β+/electron-capture decay of192,194,196,1

Cited by 69 publications

References 24 publications

Configuration mixing in the neutron-deficientPb186−196isotopes

Configuration mixing in the neutron-deficientPb186−196isotopes

Configuration mixing of angular momentum projected self-consistent mean-field states for neutron-deficient Pb isotopes

Electric monopole transitions from low energy excitations in nuclei

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