“…The listed values are experimental maximum cross sections if excitation functions were measured [15,17,29] or calculated maximum cross sections if only the average thick target production cross sections were measured [14,16,30]. In the latter cases the values listed in Table 2 were deduced from the target thickness and an assumed width of the corresponding excitation function.…”
Section: Resultsmentioning
confidence: 99%
“…The experimental techniques used to determine the cross sections summarized in Table 2 Table 2. Maximum cross sections for the production of fermium evaporation residues from the fusion reaction between argon and lead ; (14) ") this work b) unweighted average ~) spontaneous fission decay from 246Fm measured; assumed fission branch 8 ~o [26] otherwise detected by its c~-decay are, i) mechanical rotating wheel systems as used in this work which transport the reaction products continuously out of the beam into shielded positions where fission-track detectors register spontaneous fission decay [14][15][16]30], ii) a gas-jet system [293 which transports reaction products to collecting foils where the deposited activity is measured for c~-and spontaneous fission decay, iii) an in-beam detection system [31], where recoiling products were stopped in hydrogen gas and fission fragments detected by several ionisation chambers positioned around the stopping area, and iv) a velocity filter [32] able to separate in flight fusion products from the faster beam particles and the bulk of other reaction products [17]. Despite the very different techniques applied, the cross sections listed in Table 2 agree in general within about a factor of three.…”
The production of fermium isotopes was attempted by complete fusion of different targets and projectiles spanning a wide range of effective entrance channel fissilities below and above the predicted threshold value Xef fthr~(l'/-v... For the most asymmetric systems where fusion is expected to occur without dynamical hindrance we investigate to what extent the expected amount of sub-barrier fusion contributes to the production of fermium evaporation residues. For increasingly symmetric systems the experimental fusion barriers are found to exceed the fusion barriers predicted by the proximity formalism. The barrier heights are discussed in the framework of both the extra-push model and the surface friction model.
“…The listed values are experimental maximum cross sections if excitation functions were measured [15,17,29] or calculated maximum cross sections if only the average thick target production cross sections were measured [14,16,30]. In the latter cases the values listed in Table 2 were deduced from the target thickness and an assumed width of the corresponding excitation function.…”
Section: Resultsmentioning
confidence: 99%
“…The experimental techniques used to determine the cross sections summarized in Table 2 Table 2. Maximum cross sections for the production of fermium evaporation residues from the fusion reaction between argon and lead ; (14) ") this work b) unweighted average ~) spontaneous fission decay from 246Fm measured; assumed fission branch 8 ~o [26] otherwise detected by its c~-decay are, i) mechanical rotating wheel systems as used in this work which transport the reaction products continuously out of the beam into shielded positions where fission-track detectors register spontaneous fission decay [14][15][16]30], ii) a gas-jet system [293 which transports reaction products to collecting foils where the deposited activity is measured for c~-and spontaneous fission decay, iii) an in-beam detection system [31], where recoiling products were stopped in hydrogen gas and fission fragments detected by several ionisation chambers positioned around the stopping area, and iv) a velocity filter [32] able to separate in flight fusion products from the faster beam particles and the bulk of other reaction products [17]. Despite the very different techniques applied, the cross sections listed in Table 2 agree in general within about a factor of three.…”
The production of fermium isotopes was attempted by complete fusion of different targets and projectiles spanning a wide range of effective entrance channel fissilities below and above the predicted threshold value Xef fthr~(l'/-v... For the most asymmetric systems where fusion is expected to occur without dynamical hindrance we investigate to what extent the expected amount of sub-barrier fusion contributes to the production of fermium evaporation residues. For increasingly symmetric systems the experimental fusion barriers are found to exceed the fusion barriers predicted by the proximity formalism. The barrier heights are discussed in the framework of both the extra-push model and the surface friction model.
“…The experimental data used for the comparison are collected in Table 1. They are taken from [17][18][19][20][21] given in the fourth and sixth columns of the table.…”
Spontaneous-fission and alpha-decay half-lives are calculated for even-even nuclei with the atomic number Z = 104-110. The results reproduce rather well the existing experimental data for these nuclei and predict rather large total lifetimes for nuclei even heavier than observed up to now. The latter is mainly due to a deformed shell at the neutron number N = 162-164, obtained in calculations.
“…The final product of the reactions studied, Zg4Fm, undergoes spontaneous fission with a 100 ~o probability and has a half-life of about 4 ms [1, 71. These properties of 244Fm permitted its detection using a comparatively simple technique [3] as follows. Recoil nuclei knocked out from the target were stopped in a rotating disk and transported to mica detectors of spontaneous fission fragments.…”
Excitation functions for the reactions 2~176 2n)2~4Fm and 2~176 3n)244Fm have been measured and analysed in terms of a statistical model. The optical potential parameters have been found to be as follows: V0= -70 MeV, r o =1.26 x 10 -13 cm and d =0.36x 10-13cm. Some data on the properties of the excited compound nucleus of fermium have been obtained.
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