Published January 1962 | Version v1
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Threshold reaction interference in neutron activation analysis

  • 1. Atomic Energy of Canada Limited, Chalk River, Ontario (Canada)
  • 2. Atomic Energy Establishment, Trombay (India)
  • 3. Atomic Energy Commission, Buenos Aires (Argentina)

Description

The high energy (>0.5 MeV) component of a reactor flux can produce, via threshold reactions on the major constituents of a sample, identical activities as those produced by the thermal flux, through (n,γ) reactions, on the impurities being determined. In order to predict these interferences in thermal neutron activation analysis, it is necessary to know: 1. The cross section of the threshold reaction in a pure fission neutron flux; 2. The fraction of the reactor thermal flux, nvo, above about 0.5 MeV which has the properties of a pure fission flux. The latter has been determined in an empty fuel rod position in the NRX reactor using the reaction U-238 (n,f) as a monitor. Based on this value, fission neutron cross sections have been measured for several (n,p), (n,α), (n,2n) and (n,n') reactions. The interferences caused by the (n,p) and (n,α) reactions in this particular irradiation position are given. An example of activation by (n,2n) and (n,n') reactions, when the (n,γ) reaction is not suitable, is also discussed. (author)

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Additional details

Publishing Information

Imprint Pagination
20 p.
Report number
AECL--1434

Optional Information

Notes
19 refs., 2 tabs., 1 fig. Presented at the 1961 International Conference on Activation Analysis, A and M College of Texes, December 15-16, 1961
Secondary number(s)
CRDC--1070