TY - JOUR
T1 - Probing midrapidity source characteristics with charged particles and neutrons in the [Formula Presented] reaction at 43 MeV/nucleon
AU - Larochelle, Y.
AU - St-Pierre, C.
AU - Beaulieu, L.
AU - Colonna, N.
AU - Gingras, L.
AU - Ball, G. C.
AU - Bowman, D. R.
AU - Colonna, M.
AU - D’Erasmo, G.
AU - Fiore, E.
AU - Fox, D.
AU - Galindo-Uribarri, A.
AU - Hagberg, E.
AU - Horn, D.
AU - Laforest, R.
AU - Pantaleo, A.
AU - Roy, R.
AU - Tagliente, G.
PY - 1999
Y1 - 1999
N2 - The characteristics of the midrapidity and target sources (apparent temperatures, velocities, and neutron multiplicities) extracted from the neutron energy spectra, have been measured for various quasiprojectile (QP) excitation energies, reconstructed from charged particles of well defined peripheral events in the [Formula Presented] reaction at 43 MeV/nucleon. The reconstructed excitation energy of the QP is always smaller than the excitation energy calculated from its velocity, assuming pure dissipative binary collision. The latter observation combined with the neutron multiplicity at midrapidity and the apparent temperature suggests important preequilibrium and/or dynamical effects in the entrance channel. The midrapidity source moves at a velocity lower than the nucleon-nucleon center of mass velocity showing the importance of the attractive mean-field potential from the target even at 43 MeV/nucleon. The above picture is confirmed by comparison to Boltzman-Nordheim-Vlasov (BNV) simulations.
AB - The characteristics of the midrapidity and target sources (apparent temperatures, velocities, and neutron multiplicities) extracted from the neutron energy spectra, have been measured for various quasiprojectile (QP) excitation energies, reconstructed from charged particles of well defined peripheral events in the [Formula Presented] reaction at 43 MeV/nucleon. The reconstructed excitation energy of the QP is always smaller than the excitation energy calculated from its velocity, assuming pure dissipative binary collision. The latter observation combined with the neutron multiplicity at midrapidity and the apparent temperature suggests important preequilibrium and/or dynamical effects in the entrance channel. The midrapidity source moves at a velocity lower than the nucleon-nucleon center of mass velocity showing the importance of the attractive mean-field potential from the target even at 43 MeV/nucleon. The above picture is confirmed by comparison to Boltzman-Nordheim-Vlasov (BNV) simulations.
UR - http://www.scopus.com/inward/record.url?scp=0033074670&partnerID=8YFLogxK
U2 - 10.1103/PhysRevC.59.R565
DO - 10.1103/PhysRevC.59.R565
M3 - Article
AN - SCOPUS:0033074670
SN - 0556-2813
VL - 59
SP - R565-R569
JO - Physical Review C - Nuclear Physics
JF - Physical Review C - Nuclear Physics
IS - 2
ER -