AbstractWe defined the optimal shape which fissioning nuclei attain just before the scission and calculated the deformation energy as function of the mass asymmetry and elongation at the scission point. The calculated deformation energy is used in quasi-static approximation for estimation of the mass distribution of fission fragments, total kinetic and excitation energy of fission fragments, and the total number of prompt neutrons. The calculated results reproduce rather well the experimental data on the position of the peaks in the mass distribution of fission fragments, the total kinetic and excitation energy of fission fragments. The calculated value of neutron multiplicitiy is somewhat larger than experimental results
The main properties of the neutrons released during the neck rupture are calculated for U236 in the ...
International audienceThe potential energy of heavy nuclei has been calculated in the quasimolecular...
Prompt neutron multiplicity distributions ν(A) are generally required for prompt emission correction...
AbstractThe scission of a nucleus into two fragments is at present the least understood part of the ...
We define the optimal shape which fissioning nuclei attain just before the scission and calculate th...
AbstractFor a detailed description of the excitation energy of the fission fragments, that is used t...
International audienceThe multiplicities of scission neutrons νsc are calculated for series of U, Pu...
The total deformation energy at the moment of the neck rupture for 236U and 252Cf is calculated usin...
The experimental determination of the total excitation energy, the total kinetic energy, and the eva...
The total deformation energy at the moment of the neck rupture for 236U and 252Cf is calculated usin...
A rapidly converging 4-dimensional Fourier shape parametrization is used to model the fission proces...
AbstractThe main properties of the neutrons released during the neck rupture are calculated for U236...
The present work is dedicated to a careful investigation of the influence of the potential energy su...
Complex fission phenomena are studied in a unified way. Very general reflection asymmetrical equilib...
In nuclear fission of actinides samples, the fragments emit prompt neutrons before they reach the de...
The main properties of the neutrons released during the neck rupture are calculated for U236 in the ...
International audienceThe potential energy of heavy nuclei has been calculated in the quasimolecular...
Prompt neutron multiplicity distributions ν(A) are generally required for prompt emission correction...
AbstractThe scission of a nucleus into two fragments is at present the least understood part of the ...
We define the optimal shape which fissioning nuclei attain just before the scission and calculate th...
AbstractFor a detailed description of the excitation energy of the fission fragments, that is used t...
International audienceThe multiplicities of scission neutrons νsc are calculated for series of U, Pu...
The total deformation energy at the moment of the neck rupture for 236U and 252Cf is calculated usin...
The experimental determination of the total excitation energy, the total kinetic energy, and the eva...
The total deformation energy at the moment of the neck rupture for 236U and 252Cf is calculated usin...
A rapidly converging 4-dimensional Fourier shape parametrization is used to model the fission proces...
AbstractThe main properties of the neutrons released during the neck rupture are calculated for U236...
The present work is dedicated to a careful investigation of the influence of the potential energy su...
Complex fission phenomena are studied in a unified way. Very general reflection asymmetrical equilib...
In nuclear fission of actinides samples, the fragments emit prompt neutrons before they reach the de...
The main properties of the neutrons released during the neck rupture are calculated for U236 in the ...
International audienceThe potential energy of heavy nuclei has been calculated in the quasimolecular...
Prompt neutron multiplicity distributions ν(A) are generally required for prompt emission correction...