Proceedings of the International School of Physics "Enrico Fermi.", Volume 36N. Zanichelli, 1953 - Nuclear physics |
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Page 23
... orthogonal in J and M. They are not exactly orthogonal in K , however ; we shall calculate the overlap integral in some detail , since it serves to demonstrate a technique which is needed again and again : ( 40 ) Jar ( * ) v { xx ( x ) ...
... orthogonal in J and M. They are not exactly orthogonal in K , however ; we shall calculate the overlap integral in some detail , since it serves to demonstrate a technique which is needed again and again : ( 40 ) Jar ( * ) v { xx ( x ) ...
Page 161
... orthogonal to all P19 .. Then again Pq ' are eigenfunctions of H and , since the value of ( 22+ μ ' ) must be less than ( 22 + μ ) , this « band » of levels will lie higher in energy than those first constructed . The explicit ...
... orthogonal to all P19 .. Then again Pq ' are eigenfunctions of H and , since the value of ( 22+ μ ' ) must be less than ( 22 + μ ) , this « band » of levels will lie higher in energy than those first constructed . The explicit ...
Page 332
... orthogonal » parts using the same classification . As a very simple case the multipole sepa- ration of the two - body H is of this form : for example the multipole spectra plotted in Fig . 6 are orthogonal , satisfying 3 ( 5.111 ) Σ [ J ] ...
... orthogonal » parts using the same classification . As a very simple case the multipole sepa- ration of the two - body H is of this form : for example the multipole spectra plotted in Fig . 6 are orthogonal , satisfying 3 ( 5.111 ) Σ [ J ] ...
Contents
Gruppo fotografico dei partecipanti al Corso | 1 |
F VILLARS Rotational states and general theory of collective | 10 |
Introduction | 13 |
Copyright | |
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a-clusters amplitude angular momentum antisymmetrized approximation calculations closed shell closed-shell coefficients commutation configurations consider corresponding coupling defined deformed denotes density matrix diagonal diagrams effective field eigenfunctions eigenstates eigenvalue equation example excitation expansion experimental expression external field Fermi level formalism given gives graphs Green's function ground-state Hamiltonian Hartree-Fock hole integral isospin isotopes matrix elements method multipole neutron Nucl nuclear nuclei nucleons number of particles obtain occupation numbers one-body operator orbit orthogonal P₁ pairing force parameters parity particle-hole pair perturbation Phys potential properties protons quadrupole quantity quantum number quasi-particle Rendiconti S.I.F. representation residual interaction rotational scalar Sect secular problem self-consistent shell-model simple Slater determinants solution space spherical spin sum rules symmetry t₁ tensor theory transformation transition rates two-body unperturbed vacuum values vector wave functions zero