1983
DOI: 10.1007/bf01411616
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The 1-(1.9 MeV ?-)2+ transition in the decay of148Pm

Abstract: The non-unique first-forbidden 1-(1.9 MeV/?-)2 § transition in the decay of 148pm is studied. The nuclear matrix elements are evaluated using for the ground state of the odd-odd 148pm a phenomenological wave function derived in a previous work in the framework of the two-quasiparticle model and assuming that the first excited 2 § state in 148Sm can be described as the first quadrupole phonon state. This model provides nuclear matrix elements which are capable of describing experimental data like the spectrum s… Show more

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Cited by 3 publications
(4 citation statements)
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“…The occupation factors Vj for 148pm were taken from the solutions of the gap equations obtained with the parameters quoted in Ref. [3]. For both nuclides the magnetic dipole moments were calculated using three different approaches for the single-particle contributions #(j) as given by (7).…”
Section: Analysis and Resultsmentioning
confidence: 99%
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“…The occupation factors Vj for 148pm were taken from the solutions of the gap equations obtained with the parameters quoted in Ref. [3]. For both nuclides the magnetic dipole moments were calculated using three different approaches for the single-particle contributions #(j) as given by (7).…”
Section: Analysis and Resultsmentioning
confidence: 99%
“…More recently, the wave function singled out in Ref. [1] has been used to calculate fi-observables corresponding to the decay from the groundstate of 14SPm to the first excited state 2 + in the even-even l~SSm nucleus [3]. tn this latter work [3] the success was only partial.…”
Section: Introductionmentioning
confidence: 98%
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“…Therefore the contributions D' of [3] are given, in the present case, by the same expressions (15), after the replacement of the neutron states by proton states. Similar expressions have been reported previously for even mass superfluid systems [8,11,19]. At this point we are in condition to compute the values of the beta decay observables as they result both from the configuration mixing (10), and from the renormalization mechanism (12)-(15).…”
Section: G(u )/(E+e+w)(e+w-e) 6m(o2) = -S' S(n' N) P(n'mentioning
confidence: 66%