Rendiconti della Scuola internazionale di fisica "Enrico Fermi."North-Holland, 1953 - Physics |
Contents
LEZIONI | 1 |
The B C S BogoliubovValatin pairing theory | 3 |
R ARVIEU | 4 |
Deuteron transfer reactions | 11 |
The surface delta interaction | 15 |
New regions of deformation | 23 |
Comparison of T D A and R P A from applications | 43 |
Vibrations of odd A nuclei | 53 |
Rules for Feynman diagrams | 515 |
Feynman diagrams for a manybody system | 516 |
FeynmanGoldstone diagrams | 519 |
Special pitfalls | 520 |
Questions of antisymmetry signs and coefficients | 522 |
The Pauli principle may be disregarded in intermediate states | 523 |
The singleparticle propagator formalism | 525 |
110 Difference between the two formalisms | 527 |
Appendix A Surface vibrations of a charged droplet nucleus | 63 |
Appendix B Quadrupole harmonic vibrations of eveneven | 70 |
Quadrupole and octupole excitations in eveneven nuclei | 99 |
Singleparticle and hole states in f nuclei | 108 |
Deformations in the 1f shell | 127 |
S G NILSSON Nucleonic structure at equilibrium and fission | 142 |
BROMLEY | 148 |
Singleparticle energies | 149 |
The distortion | 159 |
The barrierpenetration problem | 165 |
JEAN | 171 |
Elastic scattering | 244 |
Neutron transfer reactions at low energies | 264 |
Neutrontransfer reactions on heavy nuclei | 283 |
N K GLENDENNING Inelastic scattering and nuclear structure | 332 |
Twophonon states | 358 |
B F BAYMAN Isobaric analogue states | 380 |
R H LEMMER Nuclear reactions | 429 |
171 | 456 |
Introduction pag | 457 |
The assumptions and aims of nuclear shell theory | 458 |
The singleparticle potential and the model space of shell theory | 459 |
Equations for the effective interaction | 463 |
Separation of core and valence energies | 468 |
The reaction matrix as effective interaction | 475 |
Core excitation in twoparticle shellmodel systems | 483 |
Deformed states and statedependence of the effective inter action in 180 and 18F | 488 |
The manyparticle shell model | 490 |
Phenomenological shellmodel interactions | 491 |
Phenomenological study of deformed states in 180 and 18F The anatomy of a forced fit | 496 |
Moments and transition rates | 499 |
Future prospects for nuclear shell theory | 501 |
BARANGER Recent progress in the understanding of finite nuclei from the twonucleon interaction Introduction | 511 |
Diagrams | 513 |
Goldstones theorem | 528 |
The groundstate wave function | 529 |
23 Calculation of the energy | 530 |
The contribution of a single cluster | 531 |
The linked cluster expansion | 532 |
Use of the singleparticle energy propagator | 533 |
The twonucleon interaction | 534 |
The twonucleon potential | 535 |
Proof of the BBP theorem | 550 |
55 | 559 |
The effect of U insertions in particle lines | 579 |
Some recent calculations | 602 |
Conclusion | 610 |
173 | 623 |
Structure of the wave functions of nondegenerate systems | 634 |
E UREY BARANGER Shellmodel calculations with a smooth | 643 |
P CAMIZ Binding energies of light nuclei with pairing plus | 654 |
E GRYPEOS A variational approach to twobody correla | 661 |
Noncentral forces | 674 |
176 | 682 |
of 160 | 683 |
The Erepresentation | 689 |
Information on nuclear structure given by | 695 |
p 2p reaction | 701 |
General results given by the spectroscopy of proton holes | 713 |
J SAWICKI Microscopic theories of vibrational states of even | 721 |
The nuclear manybody problem and nuclear spectra | 730 |
180 | 737 |
Some numerical results on even parity states of even | 744 |
Results | 747 |
H A WEIDENMÜLLER Isobaric analogue resonances | 780 |
Generalizations | 787 |
The stretch wave function | 808 |
Copyright | |