K. Hagel et al., Light particle probes of expansion and temperature evolution: Coalescence model analyses of heavy ion collisions at 47A MeV - art. no. 034607, PHYS REV C, 6203(3), 2000, pp. 4607
The reactions C-12 + Sn-116, Ne-22 + Ag, Ar-40 + Mo-100, and Zn-64 + Y-89 h
ave been studied at 47A MeV projectile energy. For these reactions the most
violent collisions lend to increasing amounts of fragment and light partic
le emission as the projectile mass increases. This is consistent with quant
um molecular dynamics (QMD) model simulations of the collisions. Moving sou
rce fits to the light charged particle data have been used to gain a global
view of the evolution of the particle emission,Comparisons of the multipli
cities and spectra of light charged particles emitted in the reactions with
the four different projectiles indicate a common emission mechanism for ea
rly emitted ejectiles even though the deposited excitation energies differ
greatly. The spectra for such ejectiles can be characterized as emission in
the nucleon-nucleon frame. Evidence that the He-3 yield is dominated by th
is type of emission and the role of the collision dynamics in determining t
he H-3/He-3 yield ratio are discussed. Self-consistent coalescence model an
alyses are applied to the light cluster yields, in an attempt to probe emit
ter source sizes and to follow the evolution of the temperatures and densit
ies from the time of first particle emission to equilibration. These analys
es exploit correlations between ejectile energy and emission time, suggeste
d by the QMD calculations. In this analysis the degree of expansion of the
emitting system is found to increase with increasing projectile mass. The d
ouble isotope yield ratio temperature drops as the system expands. Average
densities as low as 0.36 rho(0) are reached at a time near 100 fm/c after c
ontact. Calorimetric methods were used to derive the mass and excitation en
ergy of the excited nuclei which are present after preequilibrium emission.
The derived masses range from 102 to 116 u and the derived excitation ener
gies increase from 2.6 to 6.9 MeV/nucleon with increasing projectile mass.
A caloric curve is derived for these expanded A similar to 110 nuclei. This
caloric curve exhibits a plateau at temperatures near 7 MeV. The plateau e
xtends from similar to 3.5 to 6.9 MeV/nucleon excitation energy.