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Phys. Rev. Lett. 101, 082502 (2008) [4 pages]

α-Particle Condensation in 16O Studied with a Full Four-Body Orthogonality Condition Model Calculation

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Y. Funaki1, T. Yamada2, H. Horiuchi3,4, G. Röpke5, P. Schuck6,7, and A. Tohsaki3
1Nishina Center for Accelerator-Based Science, The Institute of Physical and Chemical Research (RIKEN), Wako 351-0198, Japan
2Laboratory of Physics, Kanto Gakuin University, Yokohama 236-8501, Japan
3Research Center for Nuclear Physics (RCNP), Osaka University, Osaka 567-0047, Japan
4International Institute for Advanced Studies, Kizugawa 619-0225, Japan
5Institut für Physik, Universität Rostock, D-18051 Rostock, Germany
6Institut de Physique Nucléaire, CNRS, UMR 8608, Orsay, F-91406, France
7Université Paris-Sud, Orsay, F-91505, France

Received 23 February 2008; published 22 August 2008

To explore the four-α-particle condensate state in 16O, we solve a full four-body equation of motion based on the four-α-particle orthogonality condition model in a large four-α-particle model space spanned by Gaussian basis functions. A full spectrum up to the 06+ state is reproduced consistently with the lowest six 0+ states of the experimental spectrum. The 06+ state is obtained at about 2 MeV above the four-α-particle breakup threshold and has a dilute density structure, with a radius of about 5 fm. The state has an appreciably large α condensate fraction of 61%, and a large component of α+12C(02+) configuration, both features being reliable evidence for this state to be of four-α-particle condensate nature.

© 2008 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevLett.101.082502
DOI:
10.1103/PhysRevLett.101.082502
PACS:
21.10.Dr, 21.10.Gv, 21.60.Gx, 27.20.+n