| Preface to the Series |
|
xi | |
| Preface |
|
xiii | |
|
|
|
1 | (24) |
|
|
|
1 | (5) |
|
|
|
6 | (1) |
|
|
|
7 | (2) |
|
|
|
9 | (6) |
|
|
|
15 | (2) |
|
|
|
17 | (8) |
| Part 1 ZERO TEMPERATURE |
|
|
|
|
25 | (22) |
|
|
|
25 | (2) |
|
The Giant Dipole Resonance |
|
|
27 | (4) |
|
The Monopole and Quadrupole Vibrations |
|
|
31 | (4) |
|
The Decay of Giant Resonances |
|
|
35 | (1) |
|
Direct and Compound Particle-Decay |
|
|
36 | (3) |
|
Gamma-Decay of Giant Resonances |
|
|
39 | (6) |
|
Decay to Low-Lying States |
|
|
39 | (1) |
|
|
|
40 | (5) |
|
Fission Decay of Giant Resonances |
|
|
45 | (2) |
|
Random Phase Approximation |
|
|
47 | (22) |
|
|
|
47 | (4) |
|
|
|
49 | (2) |
|
Random Phase Approximation (RPA) |
|
|
51 | (16) |
|
|
|
54 | (4) |
|
|
|
58 | (3) |
|
|
|
61 | (1) |
|
Frequency of Dipole Vibrations |
|
|
62 | (3) |
|
Frequency of Quadrupole Vibrations |
|
|
65 | (2) |
|
Damping of Nuclear Motion |
|
|
67 | (2) |
|
|
|
69 | (40) |
|
|
|
69 | (10) |
|
The Dynamical Shell Model |
|
|
69 | (7) |
|
|
|
76 | (3) |
|
Relaxation of Giant Vibrations |
|
|
79 | (17) |
|
Giant Quadrupole Resonance |
|
|
84 | (6) |
|
|
|
90 | (6) |
|
Particle-Decay of Giant Resonances |
|
|
96 | (7) |
|
The Continuum---RPA Approach |
|
|
96 | (2) |
|
The Doorway-State Projection-Operator Method |
|
|
98 | (5) |
|
Gamma-Decay of Giant Resonances |
|
|
103 | (6) |
| Part 2 FINITE TEMPERATURE |
|
|
Measurement of Giant Resonances |
|
|
109 | (20) |
|
|
|
110 | (3) |
|
|
|
113 | (5) |
|
|
|
118 | (1) |
|
High-Efficiency Multidetector Arrays |
|
|
118 | (3) |
|
Statistical Model of γ-Decay |
|
|
121 | (8) |
|
|
|
125 | (4) |
|
Dipole Oscillations: Experiment |
|
|
129 | (22) |
|
Moderate Excitation Energies |
|
|
129 | (10) |
|
|
|
129 | (1) |
|
|
|
130 | (2) |
|
|
|
132 | (7) |
|
|
|
139 | (4) |
|
|
|
143 | (1) |
|
|
|
144 | (4) |
|
Search for the Giant Monopole Resonance in Hot Nuclei |
|
|
148 | (3) |
|
Concepts of Statistical Physics |
|
|
151 | (14) |
|
|
|
151 | (2) |
|
Level Density and Partition Function |
|
|
153 | (6) |
|
|
|
153 | (3) |
|
|
|
156 | (3) |
|
Applications of the SPA+RPA to Level Densities |
|
|
159 | (4) |
|
|
|
160 | (1) |
|
|
|
161 | (1) |
|
The Monte-Carlo Shell Model Method |
|
|
162 | (1) |
|
|
|
163 | (2) |
|
|
|
165 | (20) |
|
|
|
165 | (5) |
|
|
|
170 | (4) |
|
|
|
172 | (2) |
|
|
|
174 | (2) |
|
Random Phase Approximation |
|
|
176 | (9) |
|
|
|
179 | (1) |
|
|
|
179 | (6) |
|
|
|
185 | (20) |
|
The Dynamical Shell Model |
|
|
185 | (6) |
|
Single-Particle Width: Matsubara Formalism |
|
|
186 | (4) |
|
|
|
190 | (1) |
|
Relaxation of Giant Vibrations |
|
|
191 | (4) |
|
Non-Perturbative Treatment of Collisions |
|
|
195 | (10) |
|
|
|
195 | (2) |
|
The Time-Dependent Density-Matrix Formalism |
|
|
197 | (2) |
|
Damping of Giant Vibrations |
|
|
199 | (6) |
|
Dipole Oscillations: Theory |
|
|
205 | (30) |
|
Effective Charges and Centre-of-Mass Correction |
|
|
205 | (1) |
|
|
|
206 | (2) |
|
|
|
208 | (2) |
|
Temperature Dependence of the Parameters |
|
|
210 | (4) |
|
|
|
210 | (3) |
|
|
|
213 | (1) |
|
|
|
214 | (1) |
|
|
|
214 | (5) |
|
|
|
215 | (4) |
|
|
|
219 | (6) |
|
Analysis of the Experimental Data |
|
|
225 | (10) |
|
The Nuclei 120Sn and 208Pb: The Role of Temperature |
|
|
227 | (1) |
|
The Nucleus 110Sn: The Role of Angular Momentum |
|
|
227 | (3) |
|
The Nucleus 92Mo: Motional Narrowing |
|
|
230 | (5) |
|
|
|
235 | (22) |
|
|
|
235 | (3) |
|
|
|
238 | (1) |
|
Rotational Damping and NMR: An Analogy |
|
|
239 | (5) |
|
Ordered and Chaotic Motion |
|
|
242 | (2) |
|
Two-Band Model of Rotational Damping: A Primer |
|
|
244 | (2) |
|
General Formulation of Rotational Damping |
|
|
246 | (11) |
|
|
|
249 | (3) |
|
Cranked Shell Model Calculations |
|
|
252 | (5) |
| References |
|
257 | (10) |
| Index |
|
267 | |