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C12(α,γ)O16 Capture Cross Section Below 3.2 MeV

Ronald J. Jaszczak, John H. Gibbons, and Richard L. Macklin

  • Oak Ridge National Laboratory, Oak Ridge, Tennessee 37830

Phys. Rev. C 2, 63 – Published 1 July, 1970

DOI: https://doi.org/10.1103/PhysRevC.2.63

Abstract

The C12(α,γ)O16 capture cross section was measured for α-particle energies between 1.86 MeV (σ=1.1±0.4 nb) and 3.11 MeV (σ=29±4 nb) using a pulsed He+4 beam from the ORNL 6-MV Van de Graaff accelerator and a 23- by 30-cm NaI(Tl) crystal viewed by six matched, bialkali photomultiplier tubes. An upper limit was obtained for the capture cross section at Eα=1.6 MeV. The over-all time resolution (full width at half maximum) of the system for 8-10-MeV pulses due to γ rays is 2.7 nsec. Enriched (99.94%) C12 targets ranging in thickness from 98 to 178 μg/cm2 were used. Pulses resulting from fast neutrons [from the C13(α,n)O16 reaction] interacting with the NaI(Tl) crystal were further separated from true γ pulses through the use of a new technique based on rise-time distribution differences of the respective neutron- and γ-ray-produced pulses. The face of the crystal (shielded with a 10.2 cm thickness of LiH6) was 12.2 cm from the target. The astrophysical significance of this reaction in the helium-burning sequence of stellar nucleosynthesis is also discussed.

Comments & Replies

C12(α, γ)O16 Capture Cross Section Below 4.1 MeV

Ronald J. Jaszczak and R. L. Macklin
Phys. Rev. C 2, 2452 (1970)

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