Nuclear Structure and Heavy-ion Collisions: Varenna on Lake Como, Villa Monastero, 9th-21st July 1979, Volume 77R. A. Broglia, R. A. Ricci, Carlo H. Dasso, Società italiana di fisica |
From inside the book
Results 1-3 of 83
Page 139
... dissipation in the § and modes as a function of time is shown for the Xe + Au system . Around 8 MeV are put in the mode at the very first stage , and then the energy dissipation takes place with a much slower rate due to the § mode ...
... dissipation in the § and modes as a function of time is shown for the Xe + Au system . Around 8 MeV are put in the mode at the very first stage , and then the energy dissipation takes place with a much slower rate due to the § mode ...
Page 237
... dissipation will not damp short - wavelength modes as much as the two - body variety will , and will , therefore , result in more contorted nuclear shapes . = 3 ) The dissipation given by ( 4 ) is strong , so that collective nuclear mo ...
... dissipation will not damp short - wavelength modes as much as the two - body variety will , and will , therefore , result in more contorted nuclear shapes . = 3 ) The dissipation given by ( 4 ) is strong , so that collective nuclear mo ...
Page 408
... dissipation is much smaller than the tangential dissipation . What comes out of the more microscopic treatments is that momentum transfer in the radial direction tends to be a more conservative process than momentum transfer in the ...
... dissipation is much smaller than the tangential dissipation . What comes out of the more microscopic treatments is that momentum transfer in the radial direction tends to be a more conservative process than momentum transfer in the ...
Contents
G WOLSCHIN Approaching equilibrium in heavyion collisions 1 Introduction | 1 |
Relative motion in a statistical treatment | 2 |
Time scales | 21 |
Copyright | |
57 other sections not shown
Other editions - View all
Common terms and phrases
alignment angular distributions angular momentum approximation average bombarding energy calculations charge classical co-ordinate coefficients components corresponding Coulomb Coulomb barrier cross-section curve damping deep inelastic deformation degrees of freedom density dependence dissipation effects elastic energy loss equation equilibration evaporation evolution operator excitation energy experimental factor Fermi fission fluctuations Fokker-Planck equation fragment spin fusion gamma-ray Hamiltonian Hartree Hartree-Fock heavy-ion collisions heavy-ion reactions impact parameters integral interaction intrinsic kinetic energy l-waves L. G. MORETTO Lett mass asymmetry mass distributions mean field measured MeV/u momenta neutron Nucl nuclear nuclei nucleon observed obtained one-body orbital out-of-plane particle phonon Phys plotted potential projectile projectilelike proton quantal quantity quasi-elastic ratio region relative motion Rendiconti S.I.F. rotation scattering angle shown in fig single-particle statistical surface target TDHF theory tion TKEL trajectories transfer velocity wave functions width yields