## Proceedings of the International School of Physics "Enrico Fermi.", Volume 62N. Zanichelli, 1976 - Nuclear physics |

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Page 99

The

Q-

P, ...

The

**operator**P will pick from any function p, that part that lies in the space Si-theQ-

**operator**will pick that part that lies in the complementary space S. The**operators**P and Q have the familiar properties of projection**operators**(3.7a) P* =P, ...

Page 105

(3.21) is not very useful since the r.h. s. contains the matrix element of the

effective

consistency and iterative processes, we shall use eq. (3.21) at each stage of the

iterative ...

(3.21) is not very useful since the r.h. s. contains the matrix element of the

effective

**operator**t that we are seeking. Later, when we begin to discuss self-consistency and iterative processes, we shall use eq. (3.21) at each stage of the

iterative ...

Page 118

Let us see how this first-order term emerges if we actually calculate the first-order

renormalization to the quadrupole

the general techniques of Sect. 3. Up to first order the effective

Let us see how this first-order term emerges if we actually calculate the first-order

renormalization to the quadrupole

**operator**for the spherical state Xo followingthe general techniques of Sect. 3. Up to first order the effective

**operator**i is ...### What people are saying - Write a review

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### Contents

Gruppo fotografico dei partecipanti al Corso fuori testo | 1 |

Simple ideas on reaction mechanisms | 19 |

B BUCK Nuclearstructure information from severalnucleon | 29 |

Copyright | |

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### Common terms and phrases

alpha amplitude angle angular distribution angular momentum approximation C+*C calculation centre-of-mass co-ordinates collision compound nucleus configurations continuum core corresponding Coulomb barrier coupling cross-section curve decay deformation DWBA effective eigenstates elastic scattering emission excitation energy excitation functions exit channel experimental fission form factor fragments gamma-rays ground-state Hamiltonian Hartree-Fock heavy ions heavy-ion high-spin incident energy isospin isotopes kinetic energy Lett level density mass matrix elements measured molecular moment of inertia neutron Nucl nuclear nuclei nucleons observed obtained operator optical potential orbits oscillator parameter particle peak Phys projectile proton quadrupole quasi-atom quasi-bound region renormalization residual interaction resonances rotational band shell model shown in Fig shows single-particle spectra spectroscopic spectrum spherical spherical-shell model spin structure sudden approximation target tion transfer reactions transition two-proton transfer values wave function width X-rays Y-ray yrast