Nuclear Fusion (Jan 2023)
JET D-T scenario with optimized non-thermal fusion
- M. Maslov,
- E. Lerche,
- F. Auriemma,
- E. Belli,
- C. Bourdelle,
- C.D. Challis,
- A. Chomiczewska,
- A. Dal Molin,
- J. Eriksson,
- J. Garcia,
- J. Hobirk,
- I. Ivanova-Stanik,
- Ph. Jacquet,
- A. Kappatou,
- Y. Kazakov,
- D.L. Keeling,
- D.B. King,
- V. Kiptily,
- K. Kirov,
- D. Kos,
- R. Lorenzini,
- E. De La Luna,
- C.F. Maggi,
- J. Mailloux,
- P. Mantica,
- M. Marin,
- G. Matthews,
- I. Monakhov,
- M. Nocente,
- G. Pucella,
- D. Rigamonti,
- F. Rimini,
- S. Saarelma,
- M. Salewski,
- E.R. Solano,
- Ž. Štancar,
- G. Stankunas,
- H. Sun,
- M. Tardocchi,
- D. Van Eester,
- JET Contributors
Affiliations
- M. Maslov
- ORCiD
- UKAEA, Culham Science Centre , Abingdon OX143DB, United Kingdom of Great Britain and Northern Ireland
- E. Lerche
- ORCiD
- UKAEA, Culham Science Centre , Abingdon OX143DB, United Kingdom of Great Britain and Northern Ireland; Laboratory for Plasma Physics, ERM/KMS , B-1000 Brussels, Belgium
- F. Auriemma
- ORCiD
- Consorzio RFX (CNR, ENEA, INFN, Università di Padova, Acciaierie Venete SpA) , Corso Stati Uniti 4, Padova 35127, Italy; Istituto per la Scienza e la Tecnologia dei Plasmi del CNR , Corso Stati Uniti 4, Padova 35127, Italy
- E. Belli
- ORCiD
- General Atomics , PO Box 85608, San Diego, CA 92186-5608, United States of America
- C. Bourdelle
- ORCiD
- CEA, IRFM , F-13108 St-Paul-Lez-Durance, France
- C.D. Challis
- UKAEA, Culham Science Centre , Abingdon OX143DB, United Kingdom of Great Britain and Northern Ireland
- A. Chomiczewska
- ORCiD
- Institute of Plasma Physics and Laser Microfusion , Hery 23, 01-497 Warsaw, Poland
- A. Dal Molin
- ORCiD
- Institute for Plasma Science and Technology, CNR , via Cozzi 53, 20125 Milan, Italy
- J. Eriksson
- ORCiD
- Department of Physics and Astronomy, Uppsala University , SE-75120 Uppsala, Sweden
- J. Garcia
- ORCiD
- CEA, IRFM , F-13108 St-Paul-Lez-Durance, France
- J. Hobirk
- ORCiD
- Max-Planck-Institut für Plasmaphysik , Boltzmannstr. 2, 85748 Garching, Germany
- I. Ivanova-Stanik
- ORCiD
- Institute of Plasma Physics and Laser Microfusion , Hery 23, 01-497 Warsaw, Poland
- Ph. Jacquet
- UKAEA, Culham Science Centre , Abingdon OX143DB, United Kingdom of Great Britain and Northern Ireland
- A. Kappatou
- ORCiD
- Max-Planck-Institut für Plasmaphysik , Boltzmannstr. 2, 85748 Garching, Germany
- Y. Kazakov
- Laboratory for Plasma Physics, ERM/KMS , B-1000 Brussels, Belgium
- D.L. Keeling
- ORCiD
- UKAEA, Culham Science Centre , Abingdon OX143DB, United Kingdom of Great Britain and Northern Ireland
- D.B. King
- UKAEA, Culham Science Centre , Abingdon OX143DB, United Kingdom of Great Britain and Northern Ireland
- V. Kiptily
- ORCiD
- UKAEA, Culham Science Centre , Abingdon OX143DB, United Kingdom of Great Britain and Northern Ireland
- K. Kirov
- UKAEA, Culham Science Centre , Abingdon OX143DB, United Kingdom of Great Britain and Northern Ireland
- D. Kos
- ORCiD
- UKAEA, Culham Science Centre , Abingdon OX143DB, United Kingdom of Great Britain and Northern Ireland
- R. Lorenzini
- ORCiD
- Consorzio RFX (CNR, ENEA, INFN, Università di Padova, Acciaierie Venete SpA) , Corso Stati Uniti 4, Padova 35127, Italy
- E. De La Luna
- ORCiD
- Laboratorio Nacional de Fusión, CIEMAT , 28040 Madrid, Spain
- C.F. Maggi
- ORCiD
- UKAEA, Culham Science Centre , Abingdon OX143DB, United Kingdom of Great Britain and Northern Ireland
- J. Mailloux
- UKAEA, Culham Science Centre , Abingdon OX143DB, United Kingdom of Great Britain and Northern Ireland
- P. Mantica
- ORCiD
- Institute for Plasma Science and Technology, CNR , via Cozzi 53, 20125 Milan, Italy
- M. Marin
- EPFL, Swiss Plasma Center (SPC) , CH—1015 Lausanne, Switzerland
- G. Matthews
- UKAEA, Culham Science Centre , Abingdon OX143DB, United Kingdom of Great Britain and Northern Ireland
- I. Monakhov
- UKAEA, Culham Science Centre , Abingdon OX143DB, United Kingdom of Great Britain and Northern Ireland
- M. Nocente
- ORCiD
- Institute for Plasma Science and Technology, CNR , via Cozzi 53, 20125 Milan, Italy; Department of Physics, University of Milano-Bicocca , Piazza della Scienza 3, 20126 Milan, Italy
- G. Pucella
- ORCiD
- ENEA C. R. Frascati , via E. Fermi 45, 00044 Frascati (Roma), Italy
- D. Rigamonti
- ORCiD
- Institute for Plasma Science and Technology, CNR , via Cozzi 53, 20125 Milan, Italy
- F. Rimini
- UKAEA, Culham Science Centre , Abingdon OX143DB, United Kingdom of Great Britain and Northern Ireland
- S. Saarelma
- UKAEA, Culham Science Centre , Abingdon OX143DB, United Kingdom of Great Britain and Northern Ireland
- M. Salewski
- ORCiD
- Department of Physics, Technical University of Denmark , Kgs. Lyngby, Denmark
- E.R. Solano
- ORCiD
- Laboratorio Nacional de Fusión, CIEMAT , 28040 Madrid, Spain
- Ž. Štancar
- ORCiD
- UKAEA, Culham Science Centre , Abingdon OX143DB, United Kingdom of Great Britain and Northern Ireland
- G. Stankunas
- ORCiD
- Lithuanian Energy Institute, Laboratory of Nuclear Installation Safety , Kaunas, Lithuania
- H. Sun
- ORCiD
- UKAEA, Culham Science Centre , Abingdon OX143DB, United Kingdom of Great Britain and Northern Ireland
- M. Tardocchi
- Institute for Plasma Science and Technology, CNR , via Cozzi 53, 20125 Milan, Italy
- D. Van Eester
- ORCiD
- Laboratory for Plasma Physics, ERM/KMS , B-1000 Brussels, Belgium
- JET Contributors
- DOI
- https://doi.org/10.1088/1741-4326/ace2d8
- Journal volume & issue
-
Vol. 63,
no. 11
p. 112002
Abstract
In JET deuterium-tritium (D-T) plasmas, the fusion power is produced through thermonuclear reactions and reactions between thermal ions and fast particles generated by neutral beam injection (NBI) heating or accelerated by electromagnetic wave heating in the ion cyclotron range of frequencies (ICRFs). To complement the experiments with 50/50 D/T mixtures maximizing thermonuclear reactivity, a scenario with dominant non-thermal reactivity has been developed and successfully demonstrated during the second JET deuterium-tritium campaign DTE2, as it was predicted to generate the highest fusion power in JET with a Be/W wall. It was performed in a 15/85 D/T mixture with pure D-NBI heating combined with ICRF heating at the fundamental deuterium resonance. In steady plasma conditions, a record 59 MJ of fusion energy has been achieved in a single pulse, of which 50.5 MJ were produced in a 5 s time window ( P _fus = 10.1 MW) with average Q = 0.33, confirming predictive modelling in preparation of the experiment. The highest fusion power in these experiments, P _fus = 12.5 MW with average Q = 0.38, was achieved over a shorter 2 s time window, with the period of sustainment limited by high-Z impurity accumulation. This scenario provides unique data for the validation of physics-based models used to predict D-T fusion power.
Keywords