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Phys. Rev. C 76, 034305 (2007) [5 pages]

Neutron skin deduced from antiprotonic atom data

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B. Alex Brown1,4, G. Shen2,3, G. C. Hillhouse2,4, J. Meng2,4,5,6, and A. Trzcińska7
1Department of Physics and Astronomy, National Superconducting Cyclotron Laboratory, and Joint Institute for Nuclear Astrophysics, Michigan State University, East Lansing, Michigan 48824-1321, USA
2School of Physics, Peking University, Beijing 100871, People's Republic of China
3Department of Physics, Indiana University Bloomington, Indiana 47405, USA
4Department of Physics, University of Stellenbosch, Stellenbosch, South Africa
5Institute of Theoretical Physics, Chinese Academy of Science, Beijing 100080, People's Republic of China
6Center of Theoretical Nuclear Physics, National Laboratory of Heavy Ion Accelerator, Lanzhou 730000, People's Republic of China
7Heavy Ion Laboratory, Warsaw University, PL-02-093 Warsaw, Poland

Received 2 February 2006; revised 29 June 2007; published 6 September 2007

The relationship between the nucleon density at large radii and the value of the rms radius is investigated in the framework of Skyrme Hartree-Fock and relativistic mean-field models. From a comparison to the charge density we constrain the models in terms of the nuclear matter incompressibility and effective mass properties required to reproduce the density shape. The results are used to extract the rms neutron radius for 208Pb from antiprotonic atom data. The result for the difference between the neutron and proton rms radii, the so-called neutron-skin thickness, is S=0.20(±0.04)(±0.05) fm, where ±0.04 fm is experimental error from the antiprotonic line width, and ±0.05 fm is the theoretical error suggested from the comparison of the models with the experimental charge density.

© 2007 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevC.76.034305
DOI:
10.1103/PhysRevC.76.034305
PACS:
21.10.Gv, 21.60.Jz, 27.80.+w, 36.10.Gv