1975
DOI: 10.1088/0305-4616/1/1/008
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Lifetime measurements in42Ca (populated in28Si(16O,2p))

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Cited by 11 publications
(1 citation statement)
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“…1, the ground states of 42Ca and 44Ca belong to the 'spherical' and soft prolate minima respectively. The positions of the 2[, 41+ and 61+ levels of 42'44'46Ca have been satisfactorily accounted for with conventional shell model calculations using effective two-body interactions assuming an inert 4~ core and predominantly lf7/2 and 2p3/2 neutrons [4,15]. However enhanced E2 transition rates (noteably the 2/~0i ~ transition) have warranted the inclusion of deformed components (specifically 4p-2h in 42Ca [16,17] and 6p -2h in 44Ca [18]) in the wave functions of these members of the ground state band in 42.4~Ca" Similarly the 03 and 2~-levels missing in this description have been interpreted as Core excited levels in analogy with the excited states (specifically the 0 5 and 21 + levels) of 4~ [4,5]; these deformed states arise mainly from a two-proton excitation from the sd-to p f-shell [19,20].…”
Section: mentioning
confidence: 99%
“…1, the ground states of 42Ca and 44Ca belong to the 'spherical' and soft prolate minima respectively. The positions of the 2[, 41+ and 61+ levels of 42'44'46Ca have been satisfactorily accounted for with conventional shell model calculations using effective two-body interactions assuming an inert 4~ core and predominantly lf7/2 and 2p3/2 neutrons [4,15]. However enhanced E2 transition rates (noteably the 2/~0i ~ transition) have warranted the inclusion of deformed components (specifically 4p-2h in 42Ca [16,17] and 6p -2h in 44Ca [18]) in the wave functions of these members of the ground state band in 42.4~Ca" Similarly the 03 and 2~-levels missing in this description have been interpreted as Core excited levels in analogy with the excited states (specifically the 0 5 and 21 + levels) of 4~ [4,5]; these deformed states arise mainly from a two-proton excitation from the sd-to p f-shell [19,20].…”
Section: mentioning
confidence: 99%