Nuclear Data Sheets for A = 119

Symochko, Dmytro; Browne, E.; Tuli, J.K.

doi:10.1016/j.nds.2009.10.003

Cited by 61 publications

(42 citation statements)

References 188 publications

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“…119 Cd was assigned a spin of I = 3 /2 based on γ-ray studies [14]. This is consistent with conclusions drawn from the measurements on Cd + ions published previously [10].…”

Section: Nuclear Spinsupporting

confidence: 90%

Collinear laser spectroscopy of atomic cadmium

et al. 2015

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Abstract. Hyperfine structure A and B factors of the atomic 5s 5p 3 P2 → 5s 6s 3 S1 transition are determined from collinear laser spectroscopy data of 107−123 Cd and 111m−123m Cd. Nuclear magnetic moments and electric quadrupole moments are extracted using reference dipole moments and calculated electric field gradients, respectively. The hyperfine structure anomaly for isotopes with s1 /2 and d5 /2 nuclear ground states and isomeric h11 /2 states is evaluated and a linear relationship is observed for all nuclear states except s1 /2 . This corresponds to the Moskowitz-Lombardi rule that was established in the mercury region of the nuclear chart but in the case of cadmium the slope is distinctively smaller than for mercury. In total four atomic and ionic levels were analyzed and all of them exhibit a similar behaviour. The electric field gradient for the atomic 5s 5p 3 P2 level is derived from multi-configuration Dirac-Hartree-Fock calculations in order to evaluate the spectroscopic nuclear quadrupole moments. The results are consistent with those obtained in an ionic transition and based on a similar calculation.

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“…119 Cd was assigned a spin of I = 3 /2 based on γ-ray studies [14]. This is consistent with conclusions drawn from the measurements on Cd + ions published previously [10].…”

Section: Nuclear Spinsupporting

confidence: 90%

Collinear laser spectroscopy of atomic cadmium

et al. 2015

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“…Examples of typical excitation functions obtained for previously known transitions of 117−123 Sn [7,9,10,[28][29][30][31] in Experiment IV are shown in Figs. 6, 7 and 8.…”

Section: Bmentioning

confidence: 99%

States built on the 10+isomers in118,120,122,124Sn

et al. 2011

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“…The level scheme of 96 Nb deduced in the present work is shown in Fig. 3 [15], 94 Nb [16], and 95 Nb [17] isotopes, with respect to reactions in the target, and the complementary 117 Sn [20], 118 Sn [21], and 119 Sn [22], with respect to reactions in the backing, are indicated. 96 Nb is also a complementary fragment to itself.…”

Section: B Levels and Transitions In 96 Nbmentioning

confidence: 71%

High-spin states inNb96,97

et al. 2010

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The high-spin level structures of the 96,97 Nb isotopes have been studied. The isotopes were produced in the fission of the compound systems formed in two heavy-ion-induced reactions, 24 Mg (134.5 MeV) + 173 Yb and 23 Na (129 MeV) + 176 Yb. Gamma-ray spectroscopy was accomplished with the Gammasphere array. High-spin states are observed for the first time in both isotopes with excitation energies up to 5.2 and 6.6 MeV in 96,97 Nb, respectively. The coupling of the odd proton occupying the g 9/2 orbital to the yrast states in the subshell closure nucleus of 96 Zr can account for the first excited states of 97 Nb. A comparison with the first excited states in 95 Zr is also attempted. The addition of a neutron hole in 96 Nb results in a much more fragmented level scheme.

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Nuclear Data Sheets for A = 119

Cited by 61 publications

References 188 publications

Collinear laser spectroscopy of atomic cadmium

Collinear laser spectroscopy of atomic cadmium

States built on the 10+isomers in118,120,122,124Sn

High-spin states inNb96,97

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