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Energy-selective confinement of fusion-born alpha particles during internal relaxations in a tokamak plasma.
Bierwage, A; Shinohara, K; Kazakov, Ye O; Kiptily, V G; Lauber, Ph; Nocente, M; Stancar, Z; Sumida, S; Yagi, M; Garcia, J; Ide, S.
Afiliação
  • Bierwage A; National Institutes for Quantum Science and Technology (QST), Rokkasho Fusion Institute, Rokkasho, Aomori, Japan. bierwage.andreas@qst.go.jp.
  • Shinohara K; National Institutes for Quantum Science and Technology (QST), Naka Fusion Institute, Naka, Ibaraki, Japan. bierwage.andreas@qst.go.jp.
  • Kazakov YO; National Institutes for Quantum Science and Technology (QST), Naka Fusion Institute, Naka, Ibaraki, Japan.
  • Kiptily VG; Department of Complexity Science and Engineering, The University of Tokyo, Kashiwa, Chiba, Japan.
  • Lauber P; Laboratory for Plasma Physics, LPP-ERM/KMS, Partner in the Trilateral Euregio Cluster (TEC), Brussels, Belgium.
  • Nocente M; United Kingdom Atomic Energy Authority, CCFE, Culham Science Centre, Abingdon, United Kingdom.
  • Stancar Z; Max-Planck-Institut für Plasmaphysik, Garching, Germany.
  • Sumida S; Dipartimento di Fisica 'G. Occhialini', Università di Milano-Bicocca, Milano, Italy.
  • Yagi M; Institute for Plasma Science and Technology, National Research Council, Milan, Italy.
  • Garcia J; United Kingdom Atomic Energy Authority, CCFE, Culham Science Centre, Abingdon, United Kingdom.
  • Ide S; Jozef Stefan Institute, Ljubljana, Slovenia.
Nat Commun ; 13(1): 3941, 2022 Jul 08.
Article em En | MEDLINE | ID: mdl-35803936
ABSTRACT
Long-pulse operation of a self-sustained fusion reactor using toroidal magnetic containment requires control over the content of alpha particles produced by D-T fusion reactions. On the one hand, MeV-class alpha particles must stay confined to heat the plasma. On the other hand, decelerated helium ash must be expelled before diluting the fusion fuel. Here, we report results of kinetic-magnetohydrodynamic hybrid simulations of a large tokamak plasma that confirm the existence of a parameter window where such energy-selective confinement can be accomplished by exploiting internal relaxation events known as sawtooth crashes. The physical picture - a synergy between magnetic geometry, optimal crash duration and rapid particle motion - is completed by clarifying the role of magnetic drifts. Besides causing asymmetry between co- and counter-going particle populations, magnetic drifts determine the size of the confinement window by dictating where and how much reconnection occurs in particle orbit topology.

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2022 Tipo de documento: Article

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2022 Tipo de documento: Article