Rendiconti della Scuola internazionale di fisica "Enrico Fermi." |
Contents
B TAMAIN How is it possible to measure a nuclear temperature? | 1 |
Is it possible to deduce temperatures from gammaray or pion | 31 |
GUERREAU Lightparticle emission as a probe of reaction mecha | 37 |
Intermediate energies | 73 |
The fission step | 85 |
Conclusions | 92 |
Largeamplitude fluctuations | 119 |
J POCHODZALLA | 161 |
Nuclearlifetime measurements techniques | 275 |
Angular momentum and multifragmentation | 277 |
Highenergy yray emission | 302 |
B BLANK J J GAIMARD H GEISSEL G MÜNZENBERG K | 313 |
Experimental results | 320 |
Conclusion | 328 |
Introduction | 350 |
152 | 350 |
Dynamical correlations | 175 |
Conclusion | 182 |
Theoretical approaches | 189 |
The bounceoff fragments in the reaction plane as a barometer for | 215 |
Energy flow perpendicular to the reaction plane A direct look at | 225 |
A Lorentzinvariant moleculardynamics approach RQMD | 233 |
Conclusions | 244 |
Compoundnucleus decay | 251 |
Two or more fragments in equilibrium | 261 |
Introduction | 267 |
Angularmomentum equilibrium | 268 |
R BOUGAULT F DELAUNAY A GENOUXLUBAIN C LE BRUN J | 353 |
Prescission lifetimes | 364 |
ARDOUIN D GOUJDAMI P LAUTRIDOU R BOISGARD F GUIL | 389 |
Protonproton correlations at backward angle | 396 |
Conclusion | 402 |
171 | 428 |
187 | 454 |
W VON OERTZEN Transfer of nucleons between nuclei | 459 |
405 | 518 |
Introduction | 520 |
Copyright | |