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Fast Ion Interactions with RF Waves in IC Range of Frequencies in JET D-T Experiments

ORAL

Abstract

This work analyses synergistic interactions between radio frequency (RF) waves in the Ion Cyclotron Resonance Heating (ICRH) range and fast ion populations—both Neutral Beam Injection (NBI)-driven and fusion-born alpha particles—based on recent Deuterium-Tritium (D-T) experiments at JET [1]. These effects raise important considerations for future fusion reactors using ICRH, such as ITER and SPARC. Key issues include (i) parasitic RF power absorption by alphas and NBI ions, (ii) enhanced fast ion losses, and (iii) impacts on alpha heating efficiency. However, such interactions may also boost fusion performance by increasing reactivity between fast D or T ions and the bulk plasma.

Systematic studies during JET's D-T campaign [2, 3] using TRANSP [3] and JETTO [4], supported by neutron diagnostics, predict a 10–29% rise in fusion reactivity due to ICRH-accelerated fast ions, depending on scenario and plasma conditions. Effects on alpha orbit losses and heating were evaluated using data from the Neutral Particle Analyzer, scintillator detectors, Faraday cups, and TRANSP simulations. Results show RF-induced changes in alpha distribution without increased losses. Simulations also indicate a modest rise in electron and ion heating from alpha particles due to these synergistic effects.

Publication: 1. C.F. Maggi et al 2024 Nucl. Fusion 64 112012<br>2. K.K. Kirov et al 2024 Nucl. Fusion 64 016026<br>3. K.K. Kirov et al 2024 Nucl. Fusion 64 086011<br>4. A.Y. Pankin et al 2025 Comp Phys Coom 312 109611; https://doi.org/10.1016/j.cpc.2025.109611<br>5. M. Romanelli et al 2014 Plasma Fusion Res. 9 3403023

Presenters

  • Krassimir Kirov

    United Kingdom Atomic Energy Authority, Culham Campus, Abingdon, UK, UK Atomic Energy Authority (UKAEA)

Authors

  • Krassimir Kirov

    United Kingdom Atomic Energy Authority, Culham Campus, Abingdon, UK, UK Atomic Energy Authority (UKAEA)

  • Phillip J Bonofiglo

    Princeton Plasma Physics Laboratory (PPPL)

  • Clive D Challis

    United Kingdom Atomic Energy Authority, Culham Campus, Abingdon, UK

  • Jacob Eriksson

    Uppsala University

  • Marina Gorelenkova

    Princeton Plasma Physics Laboratory (PPPL)

  • Joerg Hobirk

    Max Planck Institute for Plasma Physics, Garching, Germany

  • Philippe Jacquet

    United Kingdom Atomic Energy Authority, Culham Campus, Abingdon, UK

  • Athina Kappatou

    Max Planck Institute for Plasma Physics

  • Yevgen Kazakov

    Laboratory for Plasma Physics, LPP-ERM/KMS, TEC Partner, 1000 Brussels, Belgium

  • David Keeling

    United Kingdom Atomic Energy Authority, Culham Science Centre, Abingdon, OX14 3DB, United Kingdom of Great Britain and Northern Ireland, United Kingdom Atomic Energy Authority, Culham Campus, Abingdon, UK

  • Damian Bryan King

    United Kingdom Atomic Energy Authority, Culham Campus, Abingdon, UK

  • Vasili Kiptily

    United Kingdom Atomic Energy Authority, Culham Campus, Abingdon, UK, UKAEA

  • Ernesto Lerche

    Laboratory for Plasma Physics LPP-ERM/KMS, B-1000 Brussels, Belgium

  • Costanza F Maggi

    United Kingdom Atomic Energy Authority, Culham Campus, Abingdon, UK

  • Joelle Mailloux

    United Kingdom Atomic Energy Authority, Culham Campus, Abingdon, UK

  • Paola Mantica

    Istituto per la Scienza e Tecnologia dei Plasmi, CNR, Milano

  • Mervi Mantsinen

    Barcelona Supercomputing Center, Barcelona, Spain

  • Mikhail Maslov

    United Kingdom Atomic Energy Authority, Culham Campus, Abingdon, UK, United Kingdom Atomic Energy Authority, Culham Centre for Fusion Energy, Culham Science Centre, Abingdon, Oxon, OX14 3DB, UK

  • Sheena Menmuir

    United Kingdom Atomic Energy Authority, Culham Campus, Abingdon, UK

  • Paula Siren

    United Kingdom Atomic Energy Authority, Culham Campus, Abingdon, UK

  • Žiga Štancar

    United Kingdom Atomic Energy Authority, Culham Campus, Abingdon, UK, UKAEA

  • Dirk Van Eester

    Laboratory for Plasma Physics LPP-ERM/KMS