Electrostatic Analysis of Nuclear Reaction Energies

R. A. Douglas, J. W. Broer, Ren Chiba, D. F. Herring, and Edward A. Silverstein
Phys. Rev. 104, 1059 – Published 15 November 1956
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Abstract

Electrostatic analysis of incident and product particles has been used to measure the following reaction energies (in Mev): D(d, H3)p (4.044±0.005); D(d, He3)n (3.271±0.011); C14(d, α)B12 (0.362±0.002); C14(d, p)C15 (-1.007±0.001); B10(α, d)C12 (1.341±0.002); O16(d, p)O17*, 0.87 level (1.048±0.002); N14(d, p)N15*, 7.31 level (1.308±0.002); 7.58 level (1.045±0.002); 8.32 level (0.296±0.001) and 8.57 level (0.038±0.001); C12(d, p)C13* 3.68 level (-0.960±0.002) and 3.86 level (-1.130±0.002) and N14(d, α)C12* 9.6 level (3.933±0.014). The 30-kev width of the 9.6-Mev level of C12 limits the spin and parity assignment to 0+, 1, 2+, or 3, or possibly 4+.

  • Received 13 August 1956

DOI:https://doi.org/10.1103/PhysRev.104.1059

©1956 American Physical Society

Authors & Affiliations

R. A. Douglas*, J. W. Broer, Ren Chiba, D. F. Herring, and Edward A. Silverstein

  • University of Wisconsin, Madison, Wisconsin

  • *Now at State University of Iowa, Iowa City, Iowa.
  • Now at University of Utrecht, Netherlands.
  • On leave from Tôhoku University, Sendai, Japan.

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Issue

Vol. 104, Iss. 4 — November 1956

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