1987
DOI: 10.1007/bf01289539
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Study of the reaction238U (?, ??f) atE ?=480 MeV

Abstract: Dedicated to Professor Theo Mayer-Kuckuk on the occasion of his 60th birthdayThe excitation function of the fission probability PI(E~) for 238U has been measured in the reaction 238U(c~, ~'f) at 480 MeV bombarding energy. The reaction mechanism of this reaction is discussed for excitation energies below B,I, the threshold for second chance fission, and above B,I up to Ex = 37 MeV. In comparing with results from fission induced by photons and by particle transfer reactions the (~, c~'f) reaction gives too low v… Show more

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Cited by 6 publications
(10 citation statements)
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“…In the following years, similar techniques were routinely used to study fission properties induced by direct reactions. Measurements were performed using ðd; pfÞ, ð; 0 fÞ, ðt; pfÞ, ðt; dfÞ, ð 3 He; dfÞ, and ð 3 He; tfÞ reactions to determine fission thresholds, the excitation-energy dependence of the fission probabilities, and/or the fission-fragment angular anisotropies for many different actinides (Wilkins, Unik, and Huizenga, 1964;Britt et al, 1965;Britt and Plasil, 1966;Specht, Fraser, and Milton, 1966;Britt, Rickey, and Hall, 1968;Wolf, Vandenbosch, and Loveland, 1968;Cramer, 1969, 1970;Cramer and Britt, 1970b;Back et al, 1974aBack et al, , 1974bGavron et al, 1975;Van Der Plicht et al, 1980;Wu et al, 1981;David et al, 1987;Sinha et al, 1992). These experiments used semiconductor detectors for both light-ion and fission-fragment detection.…”
Section: Early Surrogate Workmentioning
confidence: 99%
“…In the following years, similar techniques were routinely used to study fission properties induced by direct reactions. Measurements were performed using ðd; pfÞ, ð; 0 fÞ, ðt; pfÞ, ðt; dfÞ, ð 3 He; dfÞ, and ð 3 He; tfÞ reactions to determine fission thresholds, the excitation-energy dependence of the fission probabilities, and/or the fission-fragment angular anisotropies for many different actinides (Wilkins, Unik, and Huizenga, 1964;Britt et al, 1965;Britt and Plasil, 1966;Specht, Fraser, and Milton, 1966;Britt, Rickey, and Hall, 1968;Wolf, Vandenbosch, and Loveland, 1968;Cramer, 1969, 1970;Cramer and Britt, 1970b;Back et al, 1974aBack et al, , 1974bGavron et al, 1975;Van Der Plicht et al, 1980;Wu et al, 1981;David et al, 1987;Sinha et al, 1992). These experiments used semiconductor detectors for both light-ion and fission-fragment detection.…”
Section: Early Surrogate Workmentioning
confidence: 99%
“…The energies of muonic 2p -1 s and 3 d-1 s spontaneous fission (m) [12] and 2+lPu(n,f), E, = 1..6 MeV (,) [22] radiationless transitions responsible for prompt muonic fission lie in this region. The energies of muonic 2p -1 s and 3 d-1 s spontaneous fission (m) [12] and 2+lPu(n,f), E, = 1..6 MeV (,) [22] radiationless transitions responsible for prompt muonic fission lie in this region.…”
Section: Resultsmentioning
confidence: 91%
“…A hadron induced fission study performed for this purpose is reported in [12], the results of which are used here. A hadron induced fission study performed for this purpose is reported in [12], the results of which are used here.…”
Section: Prompt Muon Induced Fissionmentioning
confidence: 99%
See 1 more Smart Citation
“…Equation (3) has already been presented in [39] and is extended here for the average kinetic energy of the emitted neutrons. The ratios F,/F/for the final nuclei are deduced from various measurements (i.e.…”
Section: Pfc = ~ I(e) Pf(e) Dementioning
confidence: 99%