Review of deuterium–tritium results from the Tokamak Fusion Test Reactor
Authors: McGuire K. M. , Adler H. , Alling P. , Ancher C. , Anderson H. , Anderson J. L. , Anderson J. W. , Arunasalam V. , Ascione G. , Ashcroft D. , Barnes Cris W. , Barnes G. , Batha S. , Bateman G. , Beer M. , Bell M. G. , Bell R. , Bitter M. , Blanchard W. , Bretz N. L. , Brunkhorst C. , Budny R. , Bush C. E. , Camp R. , Caorlin M. , Carnevale H. , Cauffman S. , Chang Z. , Chang C. S. , Cheng C. Z. , Chrzanowski J. , Collins J. , Coward G. , Cropper M. , Darrow D. S. , Daugert R. , DeLooper J. , Dendy R. , Dorland W. , Dudek L. , Duong H. , Durst R. , Efthimion P. C. , Ernst D. , Evenson H. , Fisch N. , Fisher R. , Fonck R. J. , Fredd E. , Fredrickson E. , Fromm N. , Fu G. Y. , Fujita T. , Furth H. P. , Garzotto V. , Gentile C. , Gilbert J. , Gioia J. , Gorelenkov N. , Grek B. , Grisham L. R. , Hammett G. , Hanson G. R. , Hawryluk R. J. , Heidbrink W. , Herrmann H. W. , Hill K. W. , Hosea J. , Hsuan H. , Hughes M. , Hulse R. , Janos A. , Jassby D. L. , Jobes F. C. , Johnson D. W. , Johnson L. C. , Kalish M. , Kamperschroer J. , Kesner J. , Kugel H. , Labik G. , Lam N. T. , LaMarche P. H. , Lawson E. , LeBlanc B. , Levine J. , Levinton F. M. , Loesser D. , Long D. , Loughlin M. J. , Machuzak J. , Majeski R. , Mansfield D. K. , Marmar E. S. , Marsala R. , Martin A. , Martin G. , Mazzucato E. , Mauel M. , McCarthy M. P. , McChesney J. , McCormack B. , McCune D. C. , McKee G. , Meade D. M. , Medley S. S. , Mikkelsen D. R. , Mirnov S. V. , Mueller D. , Murakami M. , Murphy J. A. , Nagy A. , Navratil G. A. , Nazikian R. , Newman R. , Norris M. , O’Connor T. , Oldaker M. , Ongena J. , Osakabe M. , Owens D. K. , Park H. , Park W. , Parks P. , Paul S. F. , Pearson G. , Perry E. , Persing R. , Petrov M. , Phillips C. K. , Phillips M. , Pitcher S. , Pysher R. , Qualls A. L. , Raftopoulos S. , Ramakrishnan S. , Ramsey A. , Rasmussen D. A. , Redi M. H. , Renda G. , Rewoldt G. , Roberts D. , Rogers J. , Rossmassler R. , Roquemore A. L. , Ruskov E. , Sabbagh S. A. , Sasao M. , Schilling G. , Schivell J. , Schmidt G. L. , Scillia R. , Scott S. D. , Semenov I. , Senko T. , Sesnic S. , Sissingh R. , Skinner C. H. , Snipes J. , Stencel J. , Stevens J. , Stevenson T. , Stratton B. C. , Strachan J. D. , Stodiek W. , Swanson J. , Synakowski E. , Takahashi H. , Tang W. , Taylor G. , Terry J. , Thompson M. E. , Tighe W. , Timberlake J. R. , Tobita K. , Towner H. H. , Tuszewski M. , von Halle A. , Vannoy C. , Viola M. , von Goeler S. , Voorhees D. , Walters R. T. , Wester R. , White R. , Wieland R. , Wilgen J. B. , Williams M. , Wilson J. R. , Winston J. , Wright K. , Wong K. L. , Woskov P. , Wurden G. A. , Yamada M. , Yoshikawa S. , Young K. M. , Zarnstorff M. C. , Zavereev V. , Zweben S. J. 
Published: July 2002

After many years of fusion research, the conditions needed for a D–T fusion reactor have been approached on the Tokamak Fusion Test Reactor (TFTR) [Fusion Technol. 21, 1324 (1992)]. For the first time the unique phenomena present in a D–T plasma are now being studied in a laboratory plasma.

The first magnetic fusion experiments to study plasmas using nearly equal concentrations of deuterium and tritium have been carried out on TFTR. At present the maximum fusion power of 10.7 MW, using 39.5 MW of neutral-beam heating, in a supershot discharge and 6.7 MW in a high-βp discharge following a current rampdown. The fusion power density in a core of the plasma is ≊2.8 MW m−3, exceeding that expected in the International Thermonuclear Experimental Reactor (ITER) [Plasma Physics and Controlled Nuclear Fusion Research (International Atomic Energy Agency, Vienna, 1991), Vol. 3, p. 239] at 1500 MW total fusion power. The energy confinement time, τE, is observed to increase in D–T, relative to D plasmas, by 20% and the ni(0) Ti(0) τE product by 55%. The improvement in thermal confinement is caused primarily by a decrease in ion heat conductivity in both supershot and limiter-H-mode discharges. Extensive lithium pellet injection increased the confinement time to 0.27 s and enabled higher current operation in both supershot and high-βp discharges. Ion cyclotron range of frequencies (ICRF) heating of a D–T plasma, using the second harmonic of tritium, has been demonstrated. First measurements of the confined alpha particles have been performed and found to be in good agreement with TRANSP [Nucl. Fusion 34, 1247 (1994)] simulations. Initial measurements of the alpha ash profile have been compared with simulations using particle transport coefficients from He gas puffing experiments. The loss of alpha particles to a detector at the bottom of the vessel is well described by the first-orbit loss mechanism. No loss due to alpha-particle-driven instabilities has yet been observed. D–T experiments on TFTR will continue to explore the assumptions of the ITER design and to examine some of the physics issues associated with an advanced tokamak reactor.