Strachan, JD; Adler, H; Alling, P; Ancher, C; Anderson, H; Anderson, JL; Ashcroft, D; Barnes, Cris W; Barnes, G; Batha, S; Bell, MG; Bell, R; Bitter, M; Blanchard, W; Bretz, NL; Budny, R; Bush, CE; Camp, R; Caorlin, M; Cauffman, S; Chang, Z; Cheng, CZ; Collins, J; Coward, G; Darrow, DS; DeLooper, J; Duong, H; Dudek, L; Durst, R; Efthimion, PC; Ernst, D; Fisher, R; Fonck, RJ; Fredrickson, E; Fromm, N; Fu, GY; Furth, HP; Gentile, C; Gorelenkov, N; Grek, B; Grisham, LR; Hammett, G; Hanson, GR; Hawryluk, RJ; Heidbrink, W; Herrmann, HW; Hill, KW; Hosea, J; Hsuan, H; Janos, A; Jassby, DL; Jobes, FC; Johnson, DW; Johnson, LC; Kamperschroer, J; Kugel, H; Lam, NT; LaMarche, PH; Loughlin, MJ; LeBlanc, B; Leonard, M; Levinton, FM; Machuzak, J; Mansfield, DK; Martin, A; Mazzucato, E; Majeski, R; Marmar, E; McChesney, J; McCormack, B; McCune, DC; McGuire, KM; McKee, G; Meade, DM; Medley, SS; Mikkelsen, DR; Mueller, D; Murakami, M; Nagy, A; Nazikian, R; Newman, R; Nishitani, T; Norris, M; O’Connor, T; Oldaker, M

doi:10.1103/physrevlett.72.3526

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Fusion power production from TFTR plasmas fueled with deuterium and tritium

1994

Strachan, JD;
Adler, H;
Alling, P;
Ancher, C;
Anderson, H;
Anderson, JL;
Ashcroft, D;
Barnes, Cris W;
Barnes, G;
Batha, S;
Bell, MG;
Bell, R;
Bitter, M;
Blanchard, W;
Bretz, NL;
Budny, R;
Bush, CE;
Camp, R;
Caorlin, M;
Cauffman, S;
Chang, Z;
Cheng, CZ;
Collins, J;
Coward, G;
Darrow, DS;
DeLooper, J;
Duong, H;
Dudek, L;
Durst, R;
Efthimion, PC;
Ernst, D;
Fisher, R;
Fonck, RJ;
Fredrickson, E;
Fromm, N;
Fu, GY;
Furth, HP;
Gentile, C;
Gorelenkov, N;
Grek, B;
Grisham, LR;
Hammett, G;
Hanson, GR;
Hawryluk, RJ;
Heidbrink, W;
Herrmann, HW;
Hill, KW;
Hosea, J;
Hsuan, H;
Janos, A;
Jassby, DL;
Jobes, FC;
Johnson, DW;
Johnson, LC;
Kamperschroer, J;
Kugel, H;
Lam, NT;
LaMarche, PH;
Loughlin, MJ;
LeBlanc, B;
Leonard, M;
Levinton, FM;
Machuzak, J;
Mansfield, DK;
Martin, A;
Mazzucato, E;
Majeski, R;
Marmar, E;
McChesney, J;
McCormack, B;
McCune, DC;
McGuire, KM;
McKee, G;
Meade, DM;
Medley, SS;
Mikkelsen, DR;
Mueller, D;
Murakami, M;
Nagy, A;
Nazikian, R;
Newman, R;
Nishitani, T;
Norris, M;
O’Connor, T;
Oldaker, M;
Osakabe, M;
Owens, DK;
Park, H;
Park, W;
Paul, SF;
Pearson, G;
Perry, E;
Petrov, M;
Phillips, CK;
Pitcher, S;
Ramsey, AT;
Rasmussen, DA;
Redi, MH;
Roberts, D;
Rogers, J;
Rossmassler, R;
Roquemore, AL;
Ruskov, E;
Sabbagh, SA;
Sasao, M;
Schilling, G;
Schivell, J;
Schmidt, GL;
Scott, SD;
Sissingh, R;
Skinner, CH;
Snipes, JA;
Stevens, J;
Stevenson, T;
Stratton, BC;
Synakowski, E;
Tang, W;
Taylor, G;
Terry, JL;
Thompson, ME;
Tuszewski, M;
Vannoy, C;
von Halle, A;
von Goeler, S;
Voorhees, D;
Walters, RT;
Wieland, R;
Wilgen, JB;
Williams, M;
Wilson, JR;
Wong, KL;
Wurden, GA;
Yamada, M;
Young, KM;
Zarnstorff, MC;
Zweben, SJ
et al.

Published Web Location

https://doi.org/10.1103/physrevlett.72.3526

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Abstract

Peak fusion power production of 6.2±0.4 MW has been achieved in TFTR plasmas heated by deuterium and tritium neutral beams at a total power of 29.5 MW. These plasmas have an inferred central fusion alpha particle density of 1.2×1017 m-3 without the appearance of either disruptive magnetohydrodynamics events or detectable changes in Alfvén wave activity. The measured loss rate of energetic alpha particles agreed with the approximately 5% losses expected from alpha particles which are born on unconfined orbits. © 1994 The American Physical Society.

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Fusion power production from TFTR plasmas fueled with deuterium and tritium

Published Web Location