The N-dependence of Cd mean square charge radii (54 ⩽ N ⩽72) and the nuclear moments of 103Cd

Buchinger, F.; Dabkiewicz, P.; Kluge, H.-J.; Mueller, A. C.; Otten, E.‐W.

doi:10.1016/0375-9474(87)90550-1

Cited by 37 publications

(16 citation statements)

References 39 publications

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“…The parabolic fit shown in Fig. The dashed-dotted lines show results of different Hartree-Fock approaches [41,42] behaviour is found in the indium isotopes [30] and also in the cadmium chain [31], where furthermore these parabolic features are more pronounced according to the increasing distance from the closed proton shell in the tin case. 4.…”

Section: Change Of the Mean Square Nuclear Charge Radiusmentioning

confidence: 90%

Nuclear spins, moments and charge radii of108?111Sn

Eberz

Dinger

Huber

et al. 1987

Z. Physik A - Atomic Nuclei

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The hyperfine structure splittings (hfs) and isotope shifts (IS) in the atomic transitions 5s 2 5p 2 ~So ~5s 2 5p6s 1.3p~ have been measured for the radioactive isotopes lo8 ~l~Sn and all stable ones. The tin isotopes were prepared as fast atomic beams for collinear laser spectroscopy at the GSI online mass separator following a fusion reaction. Nuclear spins, magnetic dipole, electric quadrupole moments and changes in mean square charge radii have been determined. In a~ the spin I=5/2 was measured for the nuclear ground state (Tt/2= 18 min) in contradiction to the literature value. The mean square charge radii show a parabolic behaviour with a maximum at N = 66. This is interpreted by collective effects, which are considerably stronger than accounted for by the B(E2)values.

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Section: Change Of the Mean Square Nuclear Charge Radiusmentioning

confidence: 90%

Nuclear spins, moments and charge radii of108?111Sn

Eberz

Dinger

Huber

et al. 1987

Z. Physik A - Atomic Nuclei

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“…[1]. The second estimation has consisted in determining new values for the electronic factor and the specific mass shift by doing a King plot between the optical isotope shifts measured for the stable isotopes in the 5s 2 1 S 0 → 5s 5p 3 P 1 transition at 326.1 nm [12,6] 2 c > values and the corresponding charge radii taking the same reference, 114 Cd. Lastly the comparison between the experimental isotope shifts and the δ < r 2 c > values extracted from ref.…”

Section: Cadmium Isotopesmentioning

confidence: 99%

Signs of dynamical effects for Cd, Sn, Te, Xe, Ba and Sm nuclear charge radii

2007

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The experimental charge radius values along Cd, Sn, Te, Xe, Ba and Sm isotopic series have been extracted from isotope shift measurements using different methods to calibrate the electronic factor and mass shift effects. Static and dynamic charge radii have been calculated in the framework of a microscopic configuration mixing approach on the ground of Hartree–Fock–Bogoliubov solutions obtained with the D1S Gogny effective nucleon–nucleon interaction. Low-energy spectroscopic observables have also been obtained. The theoretical and experimental results are compared and discussed. It is shown that dynamical effects must be taken into account especially for γ-soft and weakly deformed nuclei

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“…For example, similar data for medium heavy nuclei [21] prove to be insufficient for the choice of the "best" effective force (cf. Table 3), for the A = 118 series from [21] is shorter than the A = 146 series in our analysis.…”

Section: Theoretical Description Of the Isotonic And Isobaric Dependementioning

confidence: 95%

Isotonic and isobaric dependencies of nuclear charge radii for rare-earth nuclei

Barzakh

Denisov

1993

Z. Physik A - Hadrons and Nuclei

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Abstract. Isotonic and isobaric dependencies of nuclear charge radii in the region between Z = 54 and Z = 70 are obtained from the analysis of isotope shift data fi (r 2) and muonic and electron scattering data on (r2). They are compared with the predictions of the droplet model and the Hartree-Fock calculations. The isobaric dependencies of (r 2) have proven to be especially sensitive to the choice of an effective nucleon-nucleon interaction.PACS: 21.10.Ft, Ky; 31.10.Gs radii. For evaluating such dependencies one needs, besides the isotopic changes of (r 2) deduced from optical isotopic shifts, also the absolute value of(r 2) for at least one isotope in each isotopic chain. The latter can be taken from muonic spectroscopy or from electron scattering measurements on stable nuclei. In Table 1 the values with the smallest uncertainties being exploited when the data on (r 2) were available for several stable isotopes of an element involved (for example, 138Ba, 144Nd,

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The N-dependence of Cd mean square charge radii (54 ⩽ N ⩽72) and the nuclear moments of 103Cd

Cited by 37 publications

References 39 publications

Nuclear spins, moments and charge radii of108?111Sn

Nuclear spins, moments and charge radii of108?111Sn

Signs of dynamical effects for Cd, Sn, Te, Xe, Ba and Sm nuclear charge radii

Isotonic and isobaric dependencies of nuclear charge radii for rare-earth nuclei

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