Author/Authors :
L. Donadille، نويسنده , , E. Liatard، نويسنده , , B. Benoit، نويسنده , , F. Hanappe، نويسنده , , L. Stuttge، نويسنده , , G. Rudolf، نويسنده , , E.M. Kozulin، نويسنده , , Yu.A. Lazarev، نويسنده , , P. Desesquelles، نويسنده , , L.A. Litnevsky، نويسنده , , B. Bilwes، نويسنده , , J.-F. Bruandet، نويسنده , , G.J. Costa، نويسنده , , O. Dorvaux، نويسنده , , F. Farget، نويسنده , , J. Fayot، نويسنده , , G. Guillaume، نويسنده , , A. Huck، نويسنده , , I. Itkis، نويسنده , , M.G. Itkis، نويسنده , , et al.، نويسنده ,
Abstract :
The neutron multidetector DéMoN has been used to investigate the symmetric splitting dynamics in the reactions View the MathML source with excitation energies ranging from 65 to 186 MeV for the composite system. An analysis based on the new backtracing technique has been applied on the neutron data to determine the two-dimensional correlations between the parent composite system initial thermal energy (ECNth) and the total neutron multiplicity (νtot), and between pre- and post-scission neutron multiplicities (νpre and νpost, respectively). The νpre distribution shape indicates the possible coexistence of fast-fission and fusion-fission for the system View the MathML source (Ebeam = 8.86 A MeV). The analysis of the neutron multiplicities in the framework of the combined dynamical statistical model (CDSM) gives a reduced friction coefficient β = 23 ± 1225 × 1021s−1, above the one-body dissipation limit. The corresponding fission time is τf = 40 ± 2046 × 10−21s.
Keywords :
neutron multiplicity , deduced thermal energy distribution , total , post-scission neutron multiplicity distributions , Friction coefficient , measured fission fragments mass , Kinetic energy distributions , 208Pb(58Ni , fission time , f) , Ebeam = 6.50-8.86 A MeV , 208Pb(64Ni , f) , Ebeam = 5.89-7.38 A MeV , pre-scission neutron multiplicity distributions