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Phys. Rev. Lett. 76, 372–375 (1996)

Phase Coexistence in Multifragmentation?

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L. G. Moretto, L. Phair, R. Ghetti, K. Tso, N. Colonna, W. Skulski, and G. J. Wozniak
Nuclear Science Division, Lawrence Berkeley Laboratory, Berkeley, California 94720

D. R. Bowman, N. Carlin, M. Chartier, C. K. Gelbke, W. G. Gong, W. C. Hsi, Y. D. Kim, M. A. Lisa, W. G. Lynch, G. F. Peaslee, C. Schwarz, R. T. de Souza, M. B. Tsang, and F. Zhu
National Superconducting Cyclotron Laboratory and Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824

Received 1 May 1995; published in the issue dated 15 January 1996

The charge ( Z) distributions from intermediate energy heavy-ion reactions depend upon the multiplicity n of intermediate mass fragments through a factor of the form e-cnZ. Experimentally c starts from zero at low values of the transverse energy Et and reaches a saturation value at high Et. In a liquid-gas phase diagram c = 0 for the saturated vapor, while c>0 for the unsaturated vapor. It is suggested that in the c0 regime the source evaporates down to a sizable remnant, while for c>0 the source vaporizes completely. Percolation of finite systems and nuclear evaporation portray a behavior similar to that observed experimentally.

© 1996 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevLett.76.372
DOI:
10.1103/PhysRevLett.76.372
PACS:
25.70.Pq, 05.70.Jk