Proceedings of the International School of Physics "Enrico Fermi.", Volume 62N. Zanichelli, 1976 - Nuclear physics |
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Page 105
(3.21) is not very useful since the r.h. s. contains the matrix element of the
effective operator t that we are seeking. Later, when we begin to discuss self-
consistency and iterative processes, we shall use eq. (3.21) at each stage of the
iterative ...
(3.21) is not very useful since the r.h. s. contains the matrix element of the
effective operator t that we are seeking. Later, when we begin to discuss self-
consistency and iterative processes, we shall use eq. (3.21) at each stage of the
iterative ...
Page 106
in order that the effective Hamiltonian and effective operator approaches yield the
same answer. 3'4. The role of the model Hamiltonian and the kinetic energy in
determining the spectrum. – It is instructive to analyse this consistency treatment
...
in order that the effective Hamiltonian and effective operator approaches yield the
same answer. 3'4. The role of the model Hamiltonian and the kinetic energy in
determining the spectrum. – It is instructive to analyse this consistency treatment
...
Page 110
solution corresponding to the energy used to construct the effective interaction
would have meaning. To estimate the second solution a different effective
Hamiltonian would have to be constructed (corresponding to the energy of the
second ...
solution corresponding to the energy used to construct the effective interaction
would have meaning. To estimate the second solution a different effective
Hamiltonian would have to be constructed (corresponding to the energy of the
second ...
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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 | |
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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