Rendiconti della Scuola internazionale di fisica "Enrico Fermi."L. Moretto, R. A. Ricci |
Contents
Introduction | 1 |
Physical meaning of the boson model | 17 |
APPENDIX B x² distribution of 282 | 28 |
A FAESSLER | 30 |
Coupling of two quasiparticles to threeaxial rotor in | 38 |
Coupling of two quasiparticles to an IBA core in an even | 49 |
The MONSTER starts running | 57 |
Conclusions | 63 |
R H SIEMSSEN Incompletefusion reactions as fast binary | 241 |
Data on incompletefusion reactions | 260 |
Summary and outlook | 269 |
E GANSSAUGE | 272 |
H FELDMEIER Dynamics of dissipative heavyion reactions | 274 |
G MORETTO Statistics at work in heavyion reactions | 312 |
Gammaray spectra | 403 |
Gammaray multiplicity | 414 |
81 | 104 |
90 | 112 |
92 | 119 |
model | 122 |
The p n reaction as a GamowTeller probe | 130 |
Discussion of GT strength discrepancy | 137 |
P BRAUNMUNZINGER Gross intermediate and fine structure | 143 |
Structure of intermediate width | 156 |
Fine structure and compound nuclear fluctuations | 166 |
The semiclassical approximation SCA | 172 |
Quasielastic reactions between heavy ions | 182 |
LEFORT Reactions between complex nuclei Various aspects | 208 |
To fuse or not to fuse Fissionlike splitting Its main | 216 |
On the origin of the fissionlike process when fission barrier | 222 |
Gammaray angular distribution | 422 |
SIGNORINI Fusion reactions and related experimental | 454 |
The total fusion crosssection | 468 |
Evaporation residues in the mass region A 5070 | 478 |
J VERVIER Spinor symmetries and supersymmetries in | 497 |
Phaseshift analysis of elasticscattering angular distributions | 507 |
Summary | 521 |
Introduction | 551 |
The mean free path | 558 |
Data and result | 565 |
Pooling data of different charges | 571 |
CH SCHANDERA CH LAUTERBACH J DE BOER W DÜNN | 582 |
Conclusions | 590 |
Copyright | |