By Cyriel Wagemans, Jan Wagemans, Pierre D'Hondt
This convention is the 6th in a sequence of topical conferences facing the nuclear fission strategy, regularly at low excitation power. in the course of those conferences, genuine issues are mentioned by means of a bunch of specialists. those lawsuits supply an summary of the themes handled on the convention and allow a speedy review of the present actions within the box.
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Additional resources for Seminar on Fission: Corsendonk Priory, Belgium, 18-21 September 2007
2. Bimodaljission of 274Hs Figure 4 presents the mass yields, (TKE)(M) and variances o ~ ~ = ( M and ) o~~(TKE for) the reaction 26Mg+248Cm at energies El,b=129, 143 and 160 MeV. 3 MeV, respectively). Fig 4 a) shows the shoulders in the mass yield for MH=193-220amu and additional light fragment masses for the 31 Elab=129,143 MeV. The fit of the mass yield by the Gaussian according to the LDM model is shown by solid line. 3 MeV) J 601 40. I it i 1TKE > 220 Me Wd, mass, u Figure 5. 3MeV) fission fragments for different TKE ranges.
As regards the mechanisms for fragment spin generation in spherical nuclei, only a beginning has been made with so far only one isotope having been scrutinized. Here much work is still ahead clarifying the correlation between fragment spin and nuclear structure which - at least for the example at hand does not follow general rules having been reported. Finally the search for neutron anisotropies in the cm system of fragments should help to solve a long-standing issue. Whether this anisotropy exists or not is not a purely academic question.
25]. A new experiment is in preparation which above all will have to avoid the above mishap. To that purpose the positioning of DEMON detectors has to be elaborated where the efficiency for measuring angles A<1> is flat in 2n. But there still remains a further important task. Whether an anisotropic emission of neutrons in the cm system is present or not may at least for sizable anisotropies 22 be decided by merely having a look at the A@ dependence on angle. However, the transformation from the structure of the A@ distribution to the physically interesting degree of anisotropy in the cm system of fragments has to be calculated in a Monte Carlo simulation.
Seminar on Fission: Corsendonk Priory, Belgium, 18-21 September 2007 by Cyriel Wagemans, Jan Wagemans, Pierre D'Hondt