The resonant nuclear reactions D(a,y) bLi, 6Li(a,y) 1<>]3, and 7Li(a,y) liB are examined as diagnostics of the energy distribution of confined fast alpha particles in tokamak plasmas.Reaction rates for Q = I D-T plasmas are estimated. The design of and preliminary results from the prototype fusion gamma ray detector on the tokamak fusion test reactor (TFTR) will be presented. The activation reactions lOB(a,n) 13N, 14N(a,y) Hlp, 2SMg(a,p) 28Al, and 27Al(a,p) 30p are similarly examined as diagnostics offast escaping alpha particles. Count rate estimates for Q = 1 D-T plasmas will be presented.

Measurements of the burnup of fusion product tritons in TFTR are presented. Interpretation of triton burnup experiments requires three accurate components: the measurement of the 2.5 MeV neutron emission, the measurement of the 14 MeV neutron emission and a calculation of the expected burnup ratio from the measured plasma parameters. The absolute calibration for the 14 MeV neutron measurements is provided by an NE213 proton recoil spectrometer. Time dependent burnup measurements for three plasma conditions selected for optimum detector operation are shown. Measurements of the time integrated triton burnup from copper activation foils (cross-calibrated to the NE213 measurements) are presented. Descriptions are provided of the neutron detectors and the plasma diagnostics whose data are used as input to the calculation of the expected burnup. All these measurements find that the triton burnup on TFTR is 1/2 ± 1/4 the classical expectations for a wide variety of discharges. The burnup decreases for relatively longer triton slowing down times, implying possible fast ion diffusion coefficients of ∼0.1 m 2 /s. Alternatively, burnup appears to decrease with increasing major radius of the triton source and edge safety factor q cyl , implying that ripple losses may be playing a role. Triton burnup is a very sensitive measure of anomalous fast ion transport; similar levels of diffusive transport in an ignited reactor would have minimal impact on the alpha particles.

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