Spallation-Fission Competition in Heaviest Elements; HeliumIon-Induced Reactions in Uranium Isotopes

Spallation-Fission Competition in Heaviest Elements; HeliumIon-Induced Reactions in Uranium Isotopes
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Release: 1957
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A radiochemical study of fission and spallation products produced by bombardment of U233, U235, and U238 with 18-46 Mev helium ions has been made. As in the case of similar studies using isotopes of plutonium as targets, most of the reaction cross section is taken up by fission. Also, the pronounced increase of the total cross section for ([alpha], xn) reactions with increasing mass number of the target that was observed for plutonium targets is observed for uranium targets.

Spallation-Fission Competition in Heaviest Elements; Helium IonInduced Reactions in Plutonium Isotopes

Spallation-Fission Competition in Heaviest Elements; Helium IonInduced Reactions in Plutonium Isotopes
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Release: 1956
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Excitation functions have been determined for the spallation and fission reactions induced in plutonium isotopes by 20 to 50 Mev helium ions. The method employed consisted of cyclotron bombardments of plutonium oxide followed by the chemical isolation and alpha or beta counting of radioactive reaction products. Formation cross sections are given where possible for the curium and americium spallation products corresponding to ([alpha], n), ([alpha],2n), ([alpha],3n), ([alpha],4n), ([alpha]5n), ([alpha], p), ([alpha], pn or d), ([alpha], p2n or t), and ([alpha], p3n) reactions in Pu238, Pu239, and Pu242. Fission yield curves and fission cross sections for Pu238 and Pu239 serve to define the characteristics of the ([alpha], f) reaction for plutonium isotopes. Chemical procedures are outlined for the separation of both spallation and fission product elements in a sequence of operations performed on the entire dissolved target.

Spallation-Fission Competition in Heaviest Elements; TritonProduction

Spallation-Fission Competition in Heaviest Elements; TritonProduction
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Release: 1957
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Stacked f o i l s of Au197, Th232, and U238 were bombarded, i n a series of experiments, with 48-Mev helium ions, 24-Mev deuterons, and 32-Mev protons. Tritium from each f o i l was collected and then measured by a gas-counting technique. The qualitative r e s u l t s indicate t h a t high-energy t r i t o n s are emitted i n r e l a t i v e l y large abundance from a l l targets and with each of the bombarding p a r t i c l e s . Cross sections f o r t r i t o n production from fissionable U 238 and Th232 and from non-f i s s ionable Au197 are comparable. The integrated (ci, t) cross sections thus determined for and 9lk-1' are nearly the same a s the integrated cross sections f o r the '(, pZn)' reactions as determined by measuring the yield of t h e product heavy isotopes i n radiochemical experiments. A l l of the f a c t s axe consistent with a picture of emission of high-energy t r i t o n s (whether due t o a stripping, pick-up, or other mechanism) i n which fissionable intermediate nuclei are formed mainly a t l e v e l s of excitation be-low t h e i r f i s s i o n thresholds.

Nuclear Science Abstracts

Nuclear Science Abstracts
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Total Pages: 576
Release: 1959
Genre: Nuclear energy
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A/CONF.15/P

A/CONF.15/P
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Total Pages: 16
Release: 1958
Genre:
ISBN:

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