2006Instruments and Experimental TechniquesRequires access

A method for determining the intensity of concomitant neutron source D(d, n)3He when studying the characteristics of delayed neutrons from nuclear fission induced by neutrons from reaction T(d, n)4He

V.M. Piksaikin, V. A. Roshchenko, G. G. Korolev

Open publisher page 5 citations

Abstract

A factor that may be responsible for the discrepancies in the total delay neutron yields, the relative yields of separate groups of delayed neutrons, and half-lives of their precursors has been investigated. These discrepancies are shown to be attributable to the effect of a concomitant neutron source—reaction D( d, n ) 3 He. Such a source is unavoidably present in an experiment where reaction T( d, n ) 4 He on a solid-state target is used as a neutron source. A method has been developed to calculate the contribution of neutrons from the reaction D( d, n ) 3 He to the measured total and relative yields of delayed neutrons and the half-lives of their precursors in heavy nuclei fission induced by neutrons with energies of 14–18 MeV. The energy dependence of the parameters of delayed neutron groups from the neutron-induced fission of 238 U nuclei in the energy range of 14.2–17.9 MeV is presented.

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A factor that may be responsible for the discrepancies in the total delay neutron yields, the relative yields of separate groups of delayed neutrons, and half-lives of their precursors has been investigated. These discrepancies are shown to be attributable to the effect of a concomitant neutron source—reaction D( d, n ) 3 He. Such a source is unavoidably present in an experiment where reaction T( d, n ) 4 He on a solid-state target is used as a neutron source. A method has been developed to calculate the contribution of neutrons from the reaction D( d, n ) 3 He to the measured total and relative yields of delayed neutrons and the half-lives of their precursors in heavy nuclei fission induced by neutrons with energies of 14–18 MeV. The energy dependence of the parameters of delayed neutron groups from the neutron-induced fission of 238 U nuclei in the energy range of 14.2–17.9 MeV is presented.

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Available abstract

A factor that may be responsible for the discrepancies in the total delay neutron yields, the relative yields of separate groups of delayed neutrons, and half-lives of their precursors has been investigated. These discrepancies are shown to be attributable to the effect of a concomitant neutron source—reaction D( d, n ) 3 He. Such a source is unavoidably present in an experiment where reaction T( d, n ) 4 He on a solid-state target is used as a neutron source. A method has been developed to calculate the contribution of neutrons from the reaction D( d, n ) 3 He to the measured total and relative yields of delayed neutrons and the half-lives of their precursors in heavy nuclei fission induced by neutrons with energies of 14–18 MeV. The energy dependence of the parameters of delayed neutron groups from the neutron-induced fission of 238 U nuclei in the energy range of 14.2–17.9 MeV is presented.

Key concepts: Neutron, Neutron source, Delayed neutron, Nuclear physics, Neutron temperature, Physics, Fission, Nuclear reaction

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A method for determining the intensity of concomitant neutron source D(d, n)3He when studying the characteristics of delayed neutrons from nuclear fission induced by neutrons from reaction T(d, n)4He — Research Paper | ScholarLens