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

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Page 12

The

. 'y') as a whole. This is because y' may be a superregular w enough to

compensate for I'-'. The discussion is again better handled in momentum space.

Let the ...

The

**singularities**of I'-', however, do not prevent a possibly regular behaviour of (T. 'y') as a whole. This is because y' may be a superregular w enough to

compensate for I'-'. The discussion is again better handled in momentum space.

Let the ...

Page 280

... simplifies when the eigenfunctions A, e) of H, are taken as basis; then the

amplitudes a, (e) have

these

Figure 5 ...

... simplifies when the eigenfunctions A, e) of H, are taken as basis; then the

amplitudes a, (e) have

**singularities**for e & ea = E – E. The physical meaning ofthese

**singularities**is related to eq. (1.5) and will become apparent later on.Figure 5 ...

Page 421

Only the semi-classical WKB phase shift presents a

grazing wave L. = 28. different. The oscillations on the two-proton transfer data

are due to narrow width in the angular-momentum space as related before with ...

Only the semi-classical WKB phase shift presents a

**singularity**in the region of thegrazing wave L. = 28. different. The oscillations on the two-proton transfer data

are due to narrow width in the angular-momentum space as related before with ...

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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 | |

39 other sections not shown

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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