Abstract:A generalized finite-range liquid-drop model based on the Yukawa-plusexponential potential was applied to describe fission dynamics of hot rotating nuclei. The potential energy, level-density parameter and Helmholtz free energy are calculated in a consistent way by using the generalized finiterange liquid-drop model. The level-density parameter was approximated by a leptodermous-type expression. The coefficients of this expansion are in surprisingly good agreement with those obtained earlier by Ignatyuk and co… Show more
“…The temperature of the heat bath T has been determined by the Fermi-gas formula T = (E int /a(q)) 1/2 , where E int is the internal excitation energy of the nucleus and a(q) is the level-density parameter, which has been taken from the work of Ignatyuk et al [16]. It should be noted that the asymptotic level-density parameter obtained by Ignatyuk and his co-workers is in surprisingly good agreement with the level-density parameter, calculated [17] in a consistent way by using a temperature-dependent finite-range liquid drop model [18]. The repeated indices in the equation above imply summation over the collective coordinates from 1 to 3.…”
A dynamical approach to the treatment of fission fragment angular distribution is developed. The approach is based on three-dimensional Langevin dynamics for shape collective coordinates joined with the Monte Carlo algorithm for the degree of freedom associated with the projection K of the total angular momentum of the fissioning system on the symmetry axis. The relaxation time of the tilting mode τ K is estimated. From fits to experimental data on the fission fragment angular distribution of heavy fissioning compound systems, the K equilibration time is deduced to be ∼4 × 10 −21 s for temperatures ∼1-2 MeV. A modified one-body mechanism of nuclear viscosity with the reduction coefficient of the contribution from the 'wall' formula k s = 0.25 has been used in calculations.
“…The temperature of the heat bath T has been determined by the Fermi-gas formula T = (E int /a(q)) 1/2 , where E int is the internal excitation energy of the nucleus and a(q) is the level-density parameter, which has been taken from the work of Ignatyuk et al [16]. It should be noted that the asymptotic level-density parameter obtained by Ignatyuk and his co-workers is in surprisingly good agreement with the level-density parameter, calculated [17] in a consistent way by using a temperature-dependent finite-range liquid drop model [18]. The repeated indices in the equation above imply summation over the collective coordinates from 1 to 3.…”
A dynamical approach to the treatment of fission fragment angular distribution is developed. The approach is based on three-dimensional Langevin dynamics for shape collective coordinates joined with the Monte Carlo algorithm for the degree of freedom associated with the projection K of the total angular momentum of the fissioning system on the symmetry axis. The relaxation time of the tilting mode τ K is estimated. From fits to experimental data on the fission fragment angular distribution of heavy fissioning compound systems, the K equilibration time is deduced to be ∼4 × 10 −21 s for temperatures ∼1-2 MeV. A modified one-body mechanism of nuclear viscosity with the reduction coefficient of the contribution from the 'wall' formula k s = 0.25 has been used in calculations.
“…The use of the Kramers factor allows one to match the fission rate (width) calculated by Eq. (20) and the quasistationary fission rate obtained in dynamical calculations (see, e.g., [26][27][28]). The appearance of the temperature in the denominator of Eq.…”
Section: Decay Of Excited Sh Nucleus and Its Survival Probabilitymentioning
confidence: 99%
“…Energy, angular and mass distributions of primary reaction fragments are given by formula (28) and Eqs. (25).…”
Section: Formation Of Superheavy Nuclei In Multinucleon Transfer Reacmentioning
“…The deformation dependence of the level-density parameter has been discussed in references [33,34,36,35]. In our case, the ratio a f /a n is calculated considering volume and surface dependencies as proposed in reference [36] .…”
Section: Dynamical Description Of Fission By the Abrabla Codementioning
confidence: 99%
“…[37]. A recent work of Karpov et al [35] has shown that equation (44) is well adapted by comparing it to several derivations: in the framework of the liquid-drop model including a Coulomb term [38], with the finite-range liquid-drop model [39] and within the relativistic mean-field theory [40]. The angularmomentum-dependent fission barriers are taken from the finite-range liquid-drop model predictions of Sierk [41].…”
Section: Dynamical Description Of Fission By the Abrabla Codementioning
Abstract:We examine the manifestation of transient effects in fission by analysing experimental data where fission is induced by peripheral heavy-ion collisions at relativistic energies. Available total nuclear fission cross sections of 238 U at 1⋅A GeV on gold and uranium targets are compared with a nuclear-reaction code, where transient effects in fission are modelled using different approximations to the numerical time-dependent fission-decay width: a new analytical description based on the solution of the Fokker-Planck equation and two widely used but less realistic descriptions, a step function and an exponential-like function. The experimental data are only reproduced when transient effects are considered. The deduced value of the dissipation strength β depends strongly on the approximation applied for the time-dependent fission-decay width and is estimated to be of the order of 2·10 21 s -1. A careful analysis sheds severe doubts on the use of the exponential-like in-growth function largely used in the past. Finally, we discuss which should be the characteristics of experimental observables to be most sensitive to transient effects in fission.
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