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

### From inside the book

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Page 23

In the mass

both the canonical conjugate of X and, apart from a constant, equal to the time

derivative X. It is this double property of P that simplifies the

In the mass

**problem**, one has the advantage of the very special situation that P isboth the canonical conjugate of X and, apart from a constant, equal to the time

derivative X. It is this double property of P that simplifies the

**problem**. It is easily ...Page 24

In this section, this

possible to define a canonical transformation, leading from H to a Hamiltonian (

3.2) S = exp [— iS]H exp [iS] , such that H contains a nonsingular two-body

interaction, ...

In this section, this

**problem**will be discussed from the following angle. Is itpossible to define a canonical transformation, leading from H to a Hamiltonian (

3.2) S = exp [— iS]H exp [iS] , such that H contains a nonsingular two-body

interaction, ...

Page 41

(5.15) will be considered as a new variational

equation for two sets of amplitudes ua and ... in as general a form as possible,

and only later reduce it to more special forms in connection with specific

(5.15) will be considered as a new variational

**problem**, leading to an eigenvalueequation for two sets of amplitudes ua and ... in as general a form as possible,

and only later reduce it to more special forms in connection with specific

**problems**.### What people are saying - Write a review

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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 | |

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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