The pending approach of significant alpha particle populations in D-T plasmas in TFTR and JET and in the burning plasma devices, CIT and ITER, has led to detailed study of the measurement of the alpha particles both directly and through their potential effects on the plasma. The possible diagnostics of alpha particles, previously reviewed, for example, by Zweben [S. J. Zweben, Rev. Sci. Instrum. 57, 1723 (1986)], for use on such devices have been narrowed down to a relatively small number of possibilities. Small scintillator detectors at the wall have proven very effective in detecting the escaping T and p fusion products from the D-D reaction and hence mocking-up the relevant studies of loss required by ITER. Development of high-power pulsed microwave scattering systems for investigating the fast confined alphas is in progress for TFTR and JET. Selection of the right frequency and mode will be needed for CIT and ITER but this technique has the major advantage of being able to conform to readily available access. The use of a carbon impurity pellet to provide a suitably dense ablation target cloud so that the spectra of the emitted helium light will provide data on the energy distribution of these fast alphas is also being developed. For the slowing-down group (Eα≤500 keV), charge exchange recombination spectroscopy using a source beam of neutrals is the most probable diagnostic but it becomes limited by the penetration of the beams. But, in addition to the direct measurement of the alphas, or of the neutrons, to give information on their source profile and time behavior, they significantly heat the plasma and also, potentially, lead to new instability modes which could lead to enhanced loss of themselves or of the plasma. These instabilities have been extensively analyzed recently so that methods for identifying their presence can now be evaluated. These diagnostics, and some aspects of their implementation on TFTR, CIT, and ITER will be described. This work was supported by U.S. DOE contract No. DE-AC02-76-CHO-3073.