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

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Page 76

However, we add them to denote the

projected. Now, if L2 denotes the square angular momentum operator, then (4.15

) L'tf = I(i+l)tf, and we write (4.14) as (4.16) H,J1, ... A)V£ = [x(e, k) + /JL*]tf* , or (

4.17) [5.

However, we add them to denote the

**intrinsic**state out of which y>f* wasprojected. Now, if L2 denotes the square angular momentum operator, then (4.15

) L'tf = I(i+l)tf, and we write (4.14) as (4.16) H,J1, ... A)V£ = [x(e, k) + /JL*]tf* , or (

4.17) [5.

Page 84

... and K are given by (6.3) and (6.4). The physical interpretation of the functions (

6.6) is the following: the quantum numbers (Xfi) describe the

axially symmetric rotator composed of independent particles in a deformed well.

... and K are given by (6.3) and (6.4). The physical interpretation of the functions (

6.6) is the following: the quantum numbers (Xfi) describe the

**intrinsic**state of anaxially symmetric rotator composed of independent particles in a deformed well.

Page 96

These

and also promotions of the lp particles into the 2s, Id shell. They are the type of

state discussed by Brown. They can also be treated in the approach considered ...

These

**intrinsic**states involve promotions of the 2s, Id particles into the 2p, 1/ shelland also promotions of the lp particles into the 2s, Id shell. They are the type of

state discussed by Brown. They can also be treated in the approach considered ...

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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