Phys. Rev. C 64, 064604 (2001) [11 pages]
Thermal excitation-energy deposition in 5–15 GeV/c hadron-induced reactions with 197Au. II. Relation between excitation energy and reaction variables
L. Beaulieu et al.
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L. Beaulieu *, T. Lefort †, K. Kwiatkowski ‡, W.-c. Hsi §, G. Wang **, D. S. Bracken ‡, E. Cornell ††, D. S. Ginger ‡‡, K. B. Morley ‡, and V. E. Viola Department of Chemistry and IUCF, Indiana University, Bloomington, Indiana 47405
F. Gimeno-Nogues, R. Laforest ¶, E. Martin, E. Ramakrishnan a, D. Rowland b, A. Ruangma, E. Winchester, and S. J. Yennello Department of Chemistry and Cyclotron Laboratory, Texas A & M University, College Station, Texas 77843
R. G. Korteling Department of Chemistry, Simon Fraser University, Burnaby, British Columbia, Canada V5A 1S6
L. Pienkowski Heavy Ion Laboratory, Warsaw University, 02-093 Warsaw, Poland
H. Breuer Department of Physics, University of Maryland, College Park, Maryland 20742
B. Back Physics Division, Argonne National Laboratory, Argonne, Illinois 60439
S. Gushue and L. P. Remsberg Department of Chemistry, Brookhaven National Laboratory, Upton, New York 11973
M. J. Huang, W. G. Lynch, M. B. Tsang, and H. Xi Department of Physics and NSCL, Michigan State University, East Lansing, Michigan 48824
Received 19 December 2000; revised 1 June 2001; published 6 November 2001
The relation between excitation energy and reaction observables has been examined for (6.0–14.6)-GeV/c protons, (5.0–9.2)-GeV π-, and 8.0-GeV/c antiprotons incident on a 197Au target. Relative to proton and π- beams, 8.0-GeV/c antiprotons are found to be the most effective projectile for depositing high excitation energies in the targetlike residue. For protons and π- the excitation-energy distributions are nearly identical and appear to be independent of beam momentum above 6–8 GeV/c. It is found that total measured charge, total thermal energy, and total charged-particle multiplicity scale most directly with excitation energy, whereas IMF multiplicity and total transverse energy exhibit large fluctuations. Correlations of the observed fragment multiplicity, charge, and kinetic-energy distributions with excitation energy indicate a transition in the reaction observables near E*/A≈4–6 MeV. These experimental signals are consistent with a multifragmentation mechanism that becomes the dominant deexcitation mode above in the range E*/A∼4–6 MeV.
©2001 The American Physical Society
URL: http://link.aps.org/doi/10.1103/PhysRevC.64.064604
DOI: 10.1103/PhysRevC.64.064604
PACS: 25.70.Pq, 25.40.-h, 25.43.+t, 25.80.Hp
* Present address: Départment de Physique, Université Laval, Laval, Quebec, Canada G1R 2J6.
† Present address: Laboratoire de Physique Corpusculaire de Caen, F-14050 Caen Cedex, France.
‡ Present address: Los Alamos National Laboratory, Los Alamos, NM 87545.
§ Present address: Rush Presbyterian, St. Luke Medical Center, Chicago, IL 60612.
** Present address: Epsilon, Inc., Dallas, TX 75240.
†† Present address: Lawrence Berkeley Laboratory, Berkeley, CA 94720.
‡‡ Present address: Department of Physics, Cambridge University, Cambridge, U.K.
¶ Present address: Barnes Hospital, Washington University, St. Louis, MO 63130.
a Present address: Microcal Software, Inc., One Roundhouse Plaza, Northampton, MA 01060.
b Present address: Mallinckrodt Institute of Radiology, Washington University, St. Louis, MO 63110.
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