2014
DOI: 10.1063/1.4901764
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Gyromagnetic ratios of excited states and nuclear structure near 132Sn

Abstract: Abstract. Several g-factor measurements have been performed recently on nuclei near the neutron-rich, double-magic nucleus 132 Sn. The focus here is on 134 Te, the N = 82 isotone which has two protons added to 132 Sn. The electromagnetic properties of 134 Te are examined. Comparisons are made with other nuclei that have two protons outside a double-magic core. The extent to which 132 Sn is an inert core is discussed based on these comparisons. The electromagnetic properties of the N = 82 isotones from 132 Sn t… Show more

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Cited by 5 publications
(3 citation statements)
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“…The calculated B(M2) values depend on the choice of proton and neutron g factors. Calculations employing g l (π ) = 1.13, g s (π ) = 4.04, g l (ν) = 0.02, and g s (ν) = −2.65, taking into account core polarization and meson-exchange currents [74,75], change the B(M2; 23/2 + → 19/2 − ) values slightly to 1.679 × 10 −3 W.u (SN100PN), 0.693 × 10 −3 W.u (GCN50:82), and 1.771 × 10 −3 W.u (SN100-KTH) in 133 Xe and similar values of 2.559 × 10 −3 W.u (SN100PN), 4.029 × 10 −3 W.u (GCN50:82), and 2.406 × 10 −3 W.u (SN100-KTH) in 135 Ba.…”
Section: Discussionmentioning
confidence: 99%
“…The calculated B(M2) values depend on the choice of proton and neutron g factors. Calculations employing g l (π ) = 1.13, g s (π ) = 4.04, g l (ν) = 0.02, and g s (ν) = −2.65, taking into account core polarization and meson-exchange currents [74,75], change the B(M2; 23/2 + → 19/2 − ) values slightly to 1.679 × 10 −3 W.u (SN100PN), 0.693 × 10 −3 W.u (GCN50:82), and 1.771 × 10 −3 W.u (SN100-KTH) in 133 Xe and similar values of 2.559 × 10 −3 W.u (SN100PN), 4.029 × 10 −3 W.u (GCN50:82), and 2.406 × 10 −3 W.u (SN100-KTH) in 135 Ba.…”
Section: Discussionmentioning
confidence: 99%
“…Table 7 shows the results of shell model calculations for the lowest five 2 + states in 132 Te. The calculations were performed with NUSHELLX [44] in the jj55 basis space and with the sn100 interactions; see Table 2 and [31,48,64,68] for additional details including the parameters of the effective M1 operator. Along with a comparison of the experimental and theoretical level energies, Table 7 lists the g factors and the decomposition of the wavefunctions into the dominant proton and neutron components coupled to 0 + and 2 + .…”
Section: Survival Of Seniority Structures Away From Closed Shellsmentioning
confidence: 99%
“…Figure 12. Shell model calculations of B(E2) and g factors in the N = 82 isotones with 50 < Z < 64.Reproduced from[31], with the permission of AIP Publishing.…”
mentioning
confidence: 99%