## Proceedings of the International School of Physics "Enrico Fermi.", Volume 23N. Zanichelli, 1963 - Nuclear physics |

### From inside the book

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Page 180

All of the dynamical effects, the relation of energy available to angular momentum

barrier, for example, have been ... The

system is measured from the A + l ground state, B* is the binding energy of the

last ...

All of the dynamical effects, the relation of energy available to angular momentum

barrier, for example, have been ... The

**excitation energy**, EX(A+1), in the A-\-lsystem is measured from the A + l ground state, B* is the binding energy of the

last ...

Page 181

If the bombarding energy Ek is sufficiently large relative to the binding energy B*,

a simplification is immediate. We can replace the ... In the Ni isotopes a neutron

with 2Ģi=2MeV has about 11 MeV of

If the bombarding energy Ek is sufficiently large relative to the binding energy B*,

a simplification is immediate. We can replace the ... In the Ni isotopes a neutron

with 2Ģi=2MeV has about 11 MeV of

**excitation energy**. Through its interaction ...Page 184

Now you recall that once you change the vertex function, you also have to

include the self-energy insertions, in a ... Both of these processes occur for

sufficiently high

states exist ...

Now you recall that once you change the vertex function, you also have to

include the self-energy insertions, in a ... Both of these processes occur for

sufficiently high

**excitation energies**of the A-\-\ system that many true compoundstates exist ...

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### Contents

Lectures | 1 |

G E Brown Collective motion and the application of manybody | 99 |

T Ep icson The compound nucleus and the random phase approximation | 142 |

Copyright | |

1 other sections not shown

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### Common terms and phrases

amplitude approximation assume calculated closed shells coefficients commutation compound configuration consider corresponding coupling cross-section define deformed describe determined diagonal dipole dipole strength discuss eigenfunctions eigenstate eigenvalues electron equation excitation energy expectation value experimental factor force gives Green's function ground Hamiltonian harmonic oscillator Hartree-Fock hermitian adjoint hole hyperfine-structure intrinsic irreducible representation isobaric spin isospin isotope shift large number lecture levels linear magnetic matrix elements Ml transitions Mottelson multipole neutron nuclear charge distribution nucleon nucleus number of particles obtained one-particle operator operator F optical potential orbitals orthogonal pair parameters particle-hole interaction perturbation theory Phys physical problem proton quadrupole qualitative quantum number quasi-particle random relation residual interaction resonant rotation rotation group scattering self-consistent shell-model shown single-particle solution spectrum spherical symmetry time-dependent tion total angular momentum two-body two-particle unperturbed variation vector vibrations wave function wave-functions width y-ray zero