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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Results 1-3 of 63
Page 538
... shell minimum and favours a drift towards the closed shell . For Kr + Er the en- trance channel configuration is most favourable due to the N = 50 neutron shell in Kr and the tendency to maintain N / Z equilibration . This interpre ...
... shell minimum and favours a drift towards the closed shell . For Kr + Er the en- trance channel configuration is most favourable due to the N = 50 neutron shell in Kr and the tendency to maintain N / Z equilibration . This interpre ...
Page 557
... shell on the nucleon diffusion such as a bump at Z1 82. Ap- parently the shell structure has become irrelevant due to the high excitation energy when the Pb fragmentation is reached . This may be accounted for in a model calculation by ...
... shell on the nucleon diffusion such as a bump at Z1 82. Ap- parently the shell structure has become irrelevant due to the high excitation energy when the Pb fragmentation is reached . This may be accounted for in a model calculation by ...
Page 562
... shell structure provides an alternative explanation of the charge drift retardation discussed in subsect . 4'2 for the Kr + Er system . Including the shell correction energy [ 84 ] in the driving potential of fig . 14 , one obtains the ...
... shell structure provides an alternative explanation of the charge drift retardation discussed in subsect . 4'2 for the Kr + Er system . Including the shell correction energy [ 84 ] in the driving potential of fig . 14 , one obtains the ...
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