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

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Page 70

With such a procedure one can

of Q = 5 with Q = 3 changes the amplitude of the tail by about 15%. This

patchwork procedure is however not very reliable and it remains a stumbling

block to ...

With such a procedure one can

**obtain**a rough estimate that the 15% admixtureof Q = 5 with Q = 3 changes the amplitude of the tail by about 15%. This

patchwork procedure is however not very reliable and it remains a stumbling

block to ...

Page 72

Similary by interchanging z' and X and inserting a complete set of (N + æ)

nucleon functions we

Zozo," wo,(N) = J. _ & 21, + 1 - 3, 2I-H 1 {y}osz;"|y'. 'wosz.:"|ws.' . We shall use

these ...

Similary by interchanging z' and X and inserting a complete set of (N + æ)

nucleon functions we

**obtain**an expression needed for stripping (29) (wo,(N)|XZozo," wo,(N) = J. _ & 21, + 1 - 3, 2I-H 1 {y}osz;"|y'. 'wosz.:"|ws.' . We shall use

these ...

Page 565

Using the definition of the fragment already given we have

quadrupole moment of the part of nuclear matter on one side of the symmetry

plane calculated around its centre of mass. From the curve one sees that beyond

the ...

Using the definition of the fragment already given we have

**obtained**Q' as thequadrupole moment of the part of nuclear matter on one side of the symmetry

plane calculated around its centre of mass. From the curve one sees that beyond

the ...

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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