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Journal Article

Charge radii of neon isotopes across the sd neutron shell

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Blaum,  Klaus
Division Prof. Dr. Klaus Blaum, MPI for Nuclear Physics, Max Planck Society;

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Citation

Marinova, K., Geithner, W., Kowalska, M., Blaum, K., Kappertz, S., Keim, M., et al. (2011). Charge radii of neon isotopes across the sd neutron shell. Physical Review C, 84(3): 034313, pp. 1-13. doi:10.1103/PhysRevC.84.034313.


Cite as: https://hdl.handle.net/11858/00-001M-0000-0012-1C85-D
Abstract
We report on the changes in mean square charge radii of unstable neon nuclei relative to the stable 20Ne, based on the measurement of optical isotope shifts. The studies were carried out using collinear laser spectroscopy on a fast beam of neutral neon atoms. High sensitivity on short-lived isotopes was achieved thanks to nonoptical detection based on optical pumping and state-selective collisional ionization, which was complemented by an accurate determination of the beam kinetic energy. The new results provide information on the structural changes in the sequence of neon isotopes all across the neutron sd shell, ranging from the proton drip line nucleus and halo candidate 17Ne up to the neutron-rich 28Ne in the vicinity of the “island of inversion.” Within this range the charge radius is smallest for 24Ne with N=14 corresponding to the closure of the neutron d5/2shell, while it increases toward both neutron shell closures, N=8 and N=20. The general trend of the charge radii correlates well with the deformation effects which are known to be large for several neon isotopes. In the neutron-deficient isotopes, structural changes arise from the onset of proton-halo formation for 17Ne, shell closure in 18Ne, and clustering effects in 20,21Ne. On the neutron-rich side the transition to the island of inversion plays an important role, with the radii in the upper part of the sd shell confirming the weakening of the N=20 magic number. The results add new information to the radii systematics of light nuclei where data are scarce because of the small contribution of nuclear-size effects to the isotope shifts which are dominated by the finite-mass effect.