Tables of E2 transition probabilities from the first <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" altimg="si2377.gif" display="inline" overflow="scroll"><mml:msup><mml:mrow><mml:mn>2</mml:mn></mml:mrow><mml:mrow><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math> states in even–even nuclei

Pritychenko, B.; Birch, M.; Singh, Balraj; Horoi, Mihai

doi:10.1016/j.adt.2015.10.001

Cited by 379 publications

(218 citation statements)

References 43 publications

(70 reference statements)

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“…The resulting magnetic moment for the presumed 7 + state, μ(7 + , 182 Tl m2 ) = 0.54 (10)μ N , follows the general trend of magnetic moments of the states with the same spin in the heavier Tl nuclei. The magnetic moment of the presumed 4 − state, μ(4 − , 182 Tl m1 ) = −0.549 (33)μ N , coincides, within the experimental uncertainties, with the magnetic moment of 180 Tl g with the same (presumed) configuration and spin. These observations support the applicability of the fitting procedure used for the description of the mixed hfs spectra and point to the consistency of the supposed assignments.…”

mentioning

confidence: 76%

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Changes in mean-squared charge radii and magnetic moments of Tl179–184 measured by in-source laser spectroscopy

Barzakh¹,

Andreyev²,

Cocolios³

et al. 2017

Phys. Rev. C

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Hyperfine structure and isotope shifts have been measured for the ground and isomeric states in the neutrondeficient isotopes [179][180][181][182][183][184] Tl using the 276.9-nm transition. The experiment has been performed at the CERNIsotope Separator On-Line facility using the in-source resonance-ionization laser spectroscopy technique. Spins for the ground states in 179,181,183 Tl have been determined as I = 1/2. Magnetic moments and changes in the nuclear mean-square charge radii have been deduced. By applying the additivity relation for magnetic moments of the odd-odd Tl nuclei the leading configuration assignments were confirmed. A deviation of magnetic moments for isomeric states in 182,184 Tl from the trend of the heavier Tl nuclei is observed. The charge radii of the ground states of the isotopes [179][180][181][182][183][184] Tl follow the trend for isotonic (spherical) lead nuclei. The noticeable difference in charge radii for ground and isomeric states of 183,184 Tl has been observed, suggesting a larger deformation for the intruder-based 9/2 − and 10 − states compared to the ground states. An unexpected growth of the isomer shift for 183 Tl has been found.

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mentioning

confidence: 76%

“…3, the lines of δ r 2 calculated with the DM parameters from Ref. [32] and a constant mean-square deformation (setting β 2 1/2 ( 205 Tl) = β 2 1/2 ( 204 Hg) = 0.069 [33]) are also shown to provide insight into the development of the deformation across the Tl isotopic chain.…”

Section: B Changes In Mean-square Charge Radiimentioning

confidence: 99%

Changes in mean-squared charge radii and magnetic moments of Tl179–184 measured by in-source laser spectroscopy

Barzakh¹,

Andreyev²,

Cocolios³

et al. 2017

Phys. Rev. C

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“…Energies of the first-excited 2 + states [E(2 + 1 )] and the transition probabilities between the first 2 + and 0 + ground states [B(E2)] are from Ref. [9].…”

Section: Probes For Nuclear Shape Variancesmentioning

confidence: 99%

Probes of shape transitions from mass and charge radii of nuclear ground states

Sun

Liu

2016

EPJ Web Conf.

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Abstract. The masses and sizes of nuclear ground states constitute two of the most precise and extensive arrays of experimental information. These data make a model-independent view of microscopic nuclear structure possible. Relevant differential observables of nuclear mass and charge radius can be highly sensitive to nuclear shape transitions. In this contribution, we examine the correlation of these two bulk properties to nuclear shape transitions. By combining different observables, it is even possible to isolate shape transitions from nuclear shell closures.

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“…The selected fragments were transported through the ZeroDegree spectrometer (ZDS) and finally implanted into the WAS3ABi (wide-range active silicon strip stopper array for β and ion detection) Si array positioned at the focal plane of the ZDS. The WAS3ABi detector [13] consisted of five double-sided silicon-strip detectors (DSSSDs) each with an area of 40 × 60 mm 2 , and a thickness of 1 mm. The DSSSDs had segmentations of 40 × 60 strips each.…”

Section: Methodsmentioning

confidence: 99%

“…From N = 92 onwards their quadrupole deformation is close to saturation and these nuclei possess well-deformed * simpson@lpsc.in2p3.fr prolate ground-state rotational bands, as evidenced by their E(4 + )/E(2 + ) ratios of ∼3.3 [2]. The isotopes [152][153][154][155][156] Nd have exactly these properties [3][4][5] and the latter is the most neutron-rich Nd isotope with known excited states [4,6,7].…”

Section: Introductionmentioning

confidence: 99%

μs isomers of Nd158,160

Ideguchi¹,

Simpson²,

Yokoyama³

et al. 2016

Phys. Rev. C

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Tables of E2 transition probabilities from the first 2+ states in even–even nuclei

Abstract: intercomparison of different experimental techniques to obtain these data are outlined.

Cited by 379 publications

References 43 publications

Changes in mean-squared charge radii and magnetic moments of Tl179–184 measured by in-source laser spectroscopy

Changes in mean-squared charge radii and magnetic moments of Tl179–184 measured by in-source laser spectroscopy

Probes of shape transitions from mass and charge radii of nuclear ground states

μs isomers of Nd158,160

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