Proceedings of the International School of Physics "Enrico Fermi.", Volume 69N. Zanichelli, 1977 - Nuclear physics |
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Page 114
15 ) cannot be basis states according to rule I ) , but only intermediate states . The
quantities Šiem are the amplitudes of the physical state in the different
components of the product basis of elementary excitations . The model space
contains 22 ...
15 ) cannot be basis states according to rule I ) , but only intermediate states . The
quantities Šiem are the amplitudes of the physical state in the different
components of the product basis of elementary excitations . The model space
contains 22 ...
Page 118
4 ) A = Lamiam , - 1 : m = 1 The energy of the i - th phonon is determined by the
RPA dispersion relation ( cf . rule IV ) ) ( 7 . 5 ) ( i = 1 , 2 , . . . , 2 ) . m = 1 En The
eigenfunction corresponding to the different modes is 21 , ( 7 . 6 ) | = 1 ) = { 0 , 0 ...
4 ) A = Lamiam , - 1 : m = 1 The energy of the i - th phonon is determined by the
RPA dispersion relation ( cf . rule IV ) ) ( 7 . 5 ) ( i = 1 , 2 , . . . , 2 ) . m = 1 En The
eigenfunction corresponding to the different modes is 21 , ( 7 . 6 ) | = 1 ) = { 0 , 0 ...
Page 283
Selection rules and the distribution of excitation strength . - We have ... For
example , as a consequence of this selection rule the E2 operator can only excite
a nucleon by Oho ( excitation within a major shell ) or 2ħo ( excitation up 2 shells
) .
Selection rules and the distribution of excitation strength . - We have ... For
example , as a consequence of this selection rule the E2 operator can only excite
a nucleon by Oho ( excitation within a major shell ) or 2ħo ( excitation up 2 shells
) .
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Contents
A BOHR Some aspects of rotational motion | 3 |
B R MOTTELSON Elementary excitations in the nucleus | 42 |
R BÉs and R A BROGLIA Nuclear superfluidity | 55 |
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addition angular momentum appears approximation associated backbending band calculated closed collective compared comparison components configurations considered contributions corresponding coupling cross-sections deformation density dependence describe determined discussed distribution effects electron equations estimate evidence example excitation energy expected experiment experimental expression fact factor field given gives ground Hamiltonian hole included increase indicate inertia interaction Lett levels limit mass matrix elements measured modes moments motion neutron Nucl nuclear nuclei nucleons observed obtained operator orbits oscillator pairing parameters particle particular peak Phys physical possible potential predictions present processes protons quadrupole reaction region relation relative resonance respect rotational rule scattering seen shape shell model shown in fig shows simple single single-particle space spectra spectrum strength structure surface symmetry theory tion transfer transition values vibrational wave functions