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Multifragmentation of gold nuclei by light relativistic ions: Thermal breakup versus dynamical disintegration
Authors:S. P. Avdeyev  V. A. Karnaukhov  L. A. Petrov  V. K. Rodionov  V. D. Toneev  H. Oeschler  O. V. Bochkarev  L. V. Chulkov  E. A. Kuzmin  A. Budzanowsk  W. Karcz  M. Janicki  E. Norbeck  A. S. Botvina  W. A. Friedman  K. K. Gudima  P. A. Rukoyatkin
Affiliation:8. Joint Institute for Nuclear Research, Dubna, Moscow oblast, 141980, Russia
1. Institut für Kernphysik, Technische Universit?t Darmstadt, 64289, Darmstadt, Germany
2. Russian Research Centre Kurchatov Institute, pl. Kurchatova 1, Moscow, 123182, Russia
3. Niewodniczanski Institute of Nuclear Physics, PL-31-342, Cracow, Poland
4. University of Iowa, Iowa City, IA, 52242, USA
5. Istituto Nazionale di Fisica Nucleare, Sezione di Bologna and Dipartimento di Fisica, Università di Bologna, Viale C. Berti Pichat, n. 6/2, I-40127, Bologna, Italy
6. Physics Department, University of Wisconsin, Madison, WI, 53706, USA
7. Institute of Applied Physics, Chisinau, Moldova
Abstract:The multiple emission of intermediate-mass fragments (IMF) is studied for collisions of p, 4He, and 12C on Au with the 4π FASA setup. The mean multiplicities of IMF saturate at a value of around 2 for incident energies above 6 GeV. An attempt at describing the observed IMF multiplicities in the two-stage scenario, a fast cascade followed by a statistical multifragmentation, fails. Agreement with the measured IMF multiplicities is obtained by introducing an intermediate expansion phase and modifying empirically the excitation energies and masses of remnants. The angular distributions and energy spectra from p-induced collisions are in agreement with the scenario of “thermal” multifragmentation of a hot and expanded target spectator. In the case of 12C + Au(22.4 GeV) and 4He (14.6 GeV) + Au collisions, deviations from a pure thermal breakup are seen in the fragment energy spectra, which are harder than those both from model calculations and from the measured ones for p-induced collisions. This difference is attributed to a collective flow with the expansion velocity at the surface of about 0.1c (for 12C + Au collisions).
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