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 |
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Page 1
... initial conditions can be selected to some extent in the exper- iment ; only the asymptotic final states are observed , after the interaction and after the sequential decay of the excited primary products . The initial available energy ...
... initial conditions can be selected to some extent in the exper- iment ; only the asymptotic final states are observed , after the interaction and after the sequential decay of the excited primary products . The initial available energy ...
Page 273
... initial density matrix g ( x , x ' , t 。) . Although many distinct wave functions could have the same one - body ... initial condition to calculate a given observable . The spontaneous - fission lifetime is a paradigm : the naive choice ...
... initial density matrix g ( x , x ' , t 。) . Although many distinct wave functions could have the same one - body ... initial condition to calculate a given observable . The spontaneous - fission lifetime is a paradigm : the naive choice ...
Page 584
... initial conditions ( ( p , qi ) , i = 1 , ... , N ) for the oscillator amplitude q , and momentum p . , which we choose in a random manner compatible with the semi - classical phase - space distribution for the oscillator ground state ...
... initial conditions ( ( p , qi ) , i = 1 , ... , N ) for the oscillator amplitude q , and momentum p . , which we choose in a random manner compatible with the semi - classical phase - space distribution for the oscillator ground state ...
Contents
G WOLSCHIN Approaching equilibrium in heavyion collisions 1 Introduction | 1 |
Relative motion in a statistical treatment | 2 |
Time scales | 21 |
Copyright | |
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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