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Phys. Rev. C 76, 051602(R) (2007) [4 pages]

Geometry of Borromean halo nuclei

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C. A. Bertulani1,2 and M. S. Hussein3,4
1Department of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996, USA
2Department of Physics, Texas A&M University, Commerce, Texas 75429, USA
3Instituto de Física, Universidade de São Paulo, C. P. 66318, 05389-970 São Paulo, Brazil
4Max-Planck-Institut fuer Physik Komplexer Systeme, D-01187 Dresden, Germany

Received 25 May 2007; published 27 November 2007

We discuss the geometry of the highly quantal nuclear three-body systems composed of a core plus two loosely bound particles. These Borromean nuclei have no single bound two-body subsystem. Correlation plays a prominent role. From consideration of the B(E1) value extracted from electromagnetic dissociation, in conjunction with HBT-type analysis of the two valence-halo particles correlation, we show that an estimate of the over-all geometry can be deduced. In particular we find that the opening angle between the two neutrons in 6He and 11Li are, respectively, θnn=83°-10+20 and 66°-18+22. These angles are reduced by about 12% to θnn=78°-18+13 and 58°-14+10 if the laser spectroscopy values of the rms charge radii are used to obtain the rms distance between the cores and the center of mass of the two neutrons. The opening angle in the case of 11Li is more than 20% larger than recently reported by Nakamura et al. [Phys. Rev. Lett. 96, 252502 (2006)]. The analysis is extended to 14Be and the two-proton Borromean nucleus 17Ne where complete data are still not available. Using available experimental data and recent theoretical calculations we find θnn=640-10+9 and θpp=110°, respectively.

© 2007 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevC.76.051602
DOI:
10.1103/PhysRevC.76.051602
PACS:
21.45.+v, 25.60.-t, 21.10.Ky