Fragment angular distributions in the fission of heavy nuclei by 103 mev helium ions and 51.5 mev deuterons

Gindler, J.E.; ̈nzel, H. Mu; Buschmann, J.; Christaller, G.; Michel, F. C.; Rohde, G.

doi:10.1016/0375-9474(70)90427-6

Cited by 16 publications

(7 citation statements)

References 16 publications

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“…2. These are in good agreement with the trends of lower energy work [10][11][12]. In Table 1 the values for the laboratory and center-of-mass anisotropies are listed along with the corresponding transformation parameters.…”

Section: II Resultssupporting

confidence: 68%

Fragment angular distributions from fission of238U,209Bi and197Au by 140-MeV4He Ions

et al. 1975

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Abstract. The fission fragment angular distributions from reactions of 140-MeV 4He ions with 23sU, 2~ and 197Au have been studied. From the anisotropies in the angular distributions, values for Jeff, the effective moment of inertia at the fission saddle point, have been estimated and compared with results obtained at lower bombarding energies. The derivation of ~ff values has included corrections for the effects of incomplete fusion mechanisms on the orbital angular momentum distribution of the fissioning nuclei and for neutron evaporation prior to fission. The results are also compared with heavy-ion-induced fission data for systems of similar fissility. Also, examination of the forward-backward symmetry of the 23su angular distribution substantiates other results which show that the fraction of fission reactions which follow complete fusion of the target and projectile is less than 0.5 for 140-MeV 4He-ion bombardment of 23su.Nuclear Reactions, Fission 23Su(o~,f), 2~197Au(o~,f), E= 140 MeV; measured cr(0); deduced effective moment of inertia.

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Section: II Resultssupporting

confidence: 68%

Fragment angular distributions from fission of238U,209Bi and197Au by 140-MeV4He Ions

et al. 1975

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“…The energies can be considered to be correct to +2.5 MeV. The errors of the absolute cross section are reported to be < 10~ [10] and 15% being ~25% in the most unfavorable cases [8]. The experimental cross section for the 197Au(4He, fission) reaction channel are available for E~=48 and 107 MeV [10,11].…”

Section: Discussionmentioning

confidence: 99%

“…Tl(x=l--ll) reaction [8,9] and two values [10,11] of the fusion-fission cross section. The xn7 data in high-energy region were measured by Djaloeis etal.…”

Section: Discussionmentioning

confidence: 99%

Fusion cross section from statistical analysis of4He+197Au reaction data

Boehev

Christov

Kutsarova

1989

Z. Physik A - Atomic Nuclei

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An approach for an estimation of the fusion cross section by combining the available experimental data with the statistical simulations is proposed. An important step is the correction of the experimental excitation functions for the noncompound contributions. The ratio of the corrected total evaporation excitation functions to the calculated ones allows to estimate the fusion cross section. The proposed scheme has been applied to the 4He + 197Au reaction data. The approach provides a basis for a consistent comparison between a particular complete-fusion model and experiment. 25.70.Jj PACS:

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“…A multitude of data on fission mechanism has been presented concerning deuterons and especially alpha particles as projectiles, but mostly at low energies [8][9][10][11][12][13][14]. Limited results are published on fission as a parallel product of high energy reaction mechanism, i.e.…”

Section: Introductionmentioning

confidence: 99%

High energy fission cross sections induced by deuteron on 232Th and proton on natPb targets

Zamani¹,

Stoulos²,

Fragopoulou³

et al. 2019

hnps

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Total fission cross sections induced by deuterons with energies 1.6, 2.5 and 4.0 GeV on 232Th targets and by protons on natPb targets at energy 2.0 GeV were measured during irradiations at the Nuclotron accelerator, JINR, Dubna. Using Solid State Nuclear Track detectors, the fission cross sections induced by deuterons on 232Th were determined as 1277±216, 1232±207 and 1153±198 mb, corresponding to the energies mentioned above. The total fission cross section of protons on natPb was estimated by the same method as 131±30 mb. These results were compared to the previous systematic parameterization of proton induced fission and new values for the parameters of deuteron-induce fission on actinides, 232Th and 238U and proton induced fission on natPb were deduced. Fitting results obtained for deuterons on actinides are discussed and compared to results for protons.

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Fragment angular distributions in the fission of heavy nuclei by 103 mev helium ions and 51.5 mev deuterons

Cited by 16 publications

References 16 publications

Fragment angular distributions from fission of238U,209Bi and197Au by 140-MeV4He Ions

Fragment angular distributions from fission of238U,209Bi and197Au by 140-MeV4He Ions

Fusion cross section from statistical analysis of4He+197Au reaction data

High energy fission cross sections induced by deuteron on 232Th and proton on natPb targets

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