Variations of nuclear charge radii in mercury isotopes with<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>A</mml:mi><mml:mo>=</mml:mo><mml:mn>198</mml:mn><mml:mo>,</mml:mo><mml:mi> </mml:mi><mml:mn>1</mml:mn><mml:mn>9</mml:mn><mml:mn>9</mml:mn><mml:mo>,</mml:mo><mml:mi> </mml:mi><mml:mn>2</mml:mn><mml:mn>0</mml:mn><mml:mn>0</mml:mn><mml:mo>,</mml:mo><mml:mi> </mml:mi><mml:mn>2</mml:mn><mml:mn>0</mml:mn><mml:mn>1</mml:mn><mml:mo>,</mml:mo><mml:mi> </mml:mi><mml:mn>2</mml:m

Lee, P. L.; Boehm, F.; Hahn, A.

doi:10.1103/physrevc.17.1859

Cited by 19 publications

(9 citation statements)

References 9 publications

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“…The experimental isotope shifts are from [37] and [38]. They have been renormalized using 6v = -55.3 _+3.1 Gttz/fm 2 [40] The values of/~o~ and /3o~ used for the isotopes of platinum and osmium [51 are of the same order of magnitude as the set 2/~o~. As can be seen in Fig.…”

Section: The Calculated and Experimental Results For P(eo)mentioning

confidence: 99%

The interacting Boson Model applied to the mercury isotopes

et al. 1983

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The even isotopes of mercury have been systematically studied using the Interacting Boson Model (IBM). In order to treat shape coexistence in the light isotopes, two separate IBM calculations were performed with different configurations, which were subsequently mixed. The four Hamiltonian parameters, which were allowed to vary freely from isotope to isotope, were found to be consistent with the corresponding IBM parameters used for platinum and osmium. Overall, the calculated energy spectra and electromagnetic properties are in reasonable agreement with experiment.

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Section: The Calculated and Experimental Results For P(eo)mentioning

confidence: 99%

The interacting Boson Model applied to the mercury isotopes

et al. 1983

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“…[13] take into account a large amount of more recent results. The reference list to [21][22][23][24][25][26][27][28][29][30][31][32] Mg [20], 12 Be [21] and [63][64][65][66][67][68][69][70][71][72][73][74][75][76][77][78][79][80][81][82] Ga [22].…”

Section: Radii Changes From Optical Isotope Shiftmentioning

confidence: 99%

“…[24]. Original papers have also been taken into account [25][26][27]. Two modifications were performed in Table II of Ref.…”

Section: Radii Differences Between Isotopes From K α Isotope Shiftsmentioning

confidence: 99%

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Table of experimental nuclear ground state charge radii: An update

Angeli

Marinova

2013

Atomic Data and Nuclear Data Tables

1,512

1,163

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The present table contains experimental root-mean-square (rms) nuclear charge radii R obtained by combined analysis of two types of experimental data: (i) radii changes determined from optical and, to a lesser extent, K α X-ray isotope shifts and (ii) absolute radii measured by muonic spectra and electronic scattering experiments. The table combines the results of two working groups, using respectively two different methods of evaluation, published in ADNDT earlier. It presents an updated set of rms charge radii for 909 isotopes of 92 elements from 1 H to 96 Cm together, when available, with the radii changes from optical isotope shifts. Compared with the last published tables of R-values from 2004 (799 ground states), many new data are added due to progress recently achieved by laser spectroscopy up to early 2011. The radii changes in isotopic chains for He, Li, Be, Ne, Sc, Mn, Y, Nb, Bi have been first obtained in the last years and several isotopic sequences have been recently extended to regions far off stability, (

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“…[78]. For Hg isotopes, the experiment [3,5,79] shows an even-odd staggering in the lighter isotopes (A = 181 − 186), with larger radii in the odd-A isotopes. When we compare the data for light Hg isotopes with our calculations we see that the even-even isotopes are well described with an oblate shape, whereas the odd-A isotopes are rather associated with a prolate shape.…”

Section: A Equilibrium Deformationsmentioning

confidence: 99%

Effects of deformation on theβ-decay patterns of light even-even and odd-mass Hg and Pt isotopes

Boillos

Sarriguren

2015

Phys. Rev. C

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Bulk and decay properties, including deformation energy curves, charge mean square radii, Gamow-Teller (GT) strength distributions, and β-decay half-lives, are studied in neutron-deficient even-even and odd-A Hg and Pt isotopes. The nuclear structure is described microscopically from deformed quasiparticle random-phase approximation calculations with residual interactions in both particle-hole and particle-particle channels, performed on top of a self-consistent deformed quasiparticle Skyrme Hartree-Fock basis. The observed sensitivity of the, not yet measured, GT strength distributions to deformation is proposed as an additional complementary signature of the nuclear shape. The β-decay half-lives resulting from these distributions are compared to experiment to demonstrate the ability of the method.

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Variations of nuclear charge radii in mercury isotopes withA=198, 199, 200, 201, 2

Cited by 19 publications

References 9 publications

The interacting Boson Model applied to the mercury isotopes

The interacting Boson Model applied to the mercury isotopes

Table of experimental nuclear ground state charge radii: An update

Effects of deformation on theβ-decay patterns of light even-even and odd-mass Hg and Pt isotopes

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