Phys. Rev. C
72,
024603
(2005)
[9 pages]
Tracing the evolution of temperature in near Fermi energy heavy ion collisions
J. Wang et al. NIMROD Collaboration
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J. Wang1,*, R. Wada1,2,†, T. Keutgen1,‡, K. Hagel1, Y. G. Ma1,§, M. Murray1,**, L. Qin1, A. Botvina1, S. Kowalski1, T. Materna1, J. B. Natowitz1, R. Alfarro3, J. Cibor4, M. Cinausero5, Y. El Masri6, D. Fabris7, E. Fioretto7, A. Keksis1, M. Lunardon7, A. Makeev1, N. Marie1,††, E. Martin1, Z. Majka8, A. Martinez-Davalos3, A. Menchaca-Rocha3, G. Nebbia7, G. Prete5, V. Rizzi7, A. Ruangma1, D. V. Shetty1, G. Souliotis1, P. Staszel8, M. Veselsky1, G. Viesti7, E. M. Winchester1, S. J. Yennello1, and W. Zipper9 (NIMROD Collaboration)
1Cyclotron Institute, Texas A&M University, College Station, Texas 77843, USA 2Riken, Cyclotron Center, 2-1 Hirosawa, Wako, Saitama, Japan 351-0198 3Instituto de Fisica, Universidad National Autonoma de Mexico, Apactado Postal 20-364 01000, Mexico City, Mexico 4Institute of Nuclear Physics, ul. Radzikowskiego 152, PL-31-342 Krakow, Poland 5Instituto Nazionale di Fisica Nucleare, Laboratori Nazionali di Legnaro, I-35020 Legnaro, Italy 6Fonds National de la Recherche Scientifique de Belgique and Institut de Physique Nucleaire, Université Catholique de Louvain, B-1348 Louvain-Neuve, Belgium 7Instituto Nazionale di Fisica Nucleare and Dipartimento di Fisica dell’ Universitá di Padova, I-35131 Padova, Italy 8Jagellonian University, M Smoluchowski Institute of Physics, PL-30059, Krakow, Poland 9Institute of Physics, University of Silesia, PL-40007, Katowice, Poland
A. Ono
Department of Physics, Tohoku University, Sendai 980-8578, Japan
Received 2 September 2004; published 11 August 2005
The kinetic-energy variation of emitted light clusters has been employed as a clock to explore the time evolution of the temperature for thermalizing composite systems produced in the reactions of 26A, 35A, and 47A MeV 64Zn with 58Ni, 92Mo, and 197Au. For each system investigated, the double-isotope ratio temperature curve exhibits a high maximum apparent temperature, in the range of 10–25 MeV, at high ejectile velocity. These maximum values increase with increasing projectile energy and decrease with increasing target mass. The time at which the maximum in the temperature curve is reached ranges from 80 to 130 fm/c after contact. For each different target, the subsequent cooling curves for all three projectile energies are quite similar. Temperatures comparable with those of limiting temperature systematics are reached 30 to 40 fm/c after the times corresponding to the maxima, at a time when antisymmetrized molecular dynamics transport model calculations predict entry into the final evaporative or fragmentation stage of deexcitation of the hot composite systems. Evidence for the establishment of thermal and chemical equilibrium is discussed.
© 2005 The American Physical Society
URL:
http://link.aps.org/doi/10.1103/PhysRevC.72.024603
DOI:
10.1103/PhysRevC.72.024603
PACS:
25.70.Pq, 24.60.Ky, 05.70.Jk
*On leave from the Institute of Modern Physics, Chinese Academy of Science, Lanzhou 73, China. Email address:wang@comp.tamu.edu †Riken Collaborative Scientist, Beam Technology Division, Cyclotron Center. ‡Now at FNRS IPN, Université Catholique de Louvain, B-1348 Louvain-Neuve, Belgium. §On leave from Shanghai Institute of Nuclear Research, Chinese Academy of Sciences, Shanghai 201800, China. **Now at University of Kansas, Lawrence, Kansas 66045-7582, USA. ††Now at LCP Caen ISMRA IN2P3-Centre National de la Rechuche Scientifique, F-14050 Caen, France.
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