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MHD spectroscopy of JET plasmas with pellets via Alfvén eigenmodes

  • JET Contributors
  • Culham Centre for Fusion Energy
  • University of Texas at Austin
  • FORSCHUNGSZENTRUM JULICH GMBH
  • Institute for Plasma Research
  • Instituto Superior Técnico
  • Queens University
  • University of Helsinki
  • Commissariat à l'Énergie Atomique et aux Énergies Alternatives
  • VTT Technical Research Centre of Finland
  • National Institutes for Quantum and Radiological Science and Technology
  • University of Napoli 'Federico II'
  • Universidad Nacional de Educación a Distancia
  • Istituto di Fisica del Plasma Piero Caldirola
  • ITER
  • Consorzio Rfx
  • Kurchatov Institute
  • University of Napoli Parthenope
  • ENEA Centro Ricerche Frascati
  • Troitsk Insitute of Innovating and Thermonuclear Research (TRINITI)
  • Uppsala Universitet
  • The National Institute for Cryogenics and Isotopic Technology
  • Max Planck Institute for Plasma Physics
  • University of Ghent
  • Fluid and Plasma Dynamics
  • Università degli Studi di Catania
  • Fusion for Energy
  • National Institute for Fusion Science
  • Massachusetts Institute of Technology
  • Aalto University
  • University of Latvia
  • Imperial College London
  • Laboratorio Nacional de Fusión
  • University of Oxford
  • EUROfusion
  • Oak Ridge National Laboratory
  • Karlsruher Institut für Technologie
  • University of York
  • KTH Royal Institute of Technology
  • Maritime University of Szczecin
  • Institute of Nuclear Physics PAN
  • Institute of Plasma Physics, Academy of Sciences of the Czech Republic
  • University of Trento
  • École Polytechnique Fédérale de Lausanne
  • Wigner Research Centre for Physics
  • University Mlynska
  • Lviv Polytechnic National University
  • University of Milano-Bicocca
  • The National Institute for Optoelectronics
  • Fourth State Research
  • STUDIECENTRUM VOOR KERNENERGIE / CENTRE D'ETUDE DE L'ENERGIE NUCLEAIRE
  • Narodowe Centrum Badań Jadrowych
  • Princeton Plasma Physics Laboratory
  • Université Aix Marseille
  • University of Cagliari
  • University of Warwick
  • Institute of Plasma Physics and Laser Microfusion
  • FOM Institute DIFFER
  • National Institute for Laser, Plasma and Radiation Physics
  • Jozef Stefan Institute
  • Université de Lorraine
  • Institute of Plasma Physics Chinese Academy of Sciences
  • Center for Energy Research
  • The 'Horia Hulubei' National Institute for Physics and Nuclear Engineering
  • Chalmers University of Technology
  • European Commission
  • Universidad Politécnica de Madrid
  • Second University of Napoli
  • Warsaw University of Technology
  • University of Basilicata
  • Barcelona Supercomputing Center
  • University of Seville
  • Centro Brasileiro de Pesquisas Fisicas
  • University of Rome Tor Vergata
  • Ioffe Physical-Technical Institute of the Russian Academy of Sciences
  • General Atomics
  • Universitat Innsbruck
  • University of Toyama
  • University of Strathclyde
  • National Technical University of Athens
  • University of Tuscia
  • Technical University of Denmark
  • KAIST
  • Seoul National University
  • UNIVERSITY COLLEGE CORK, NATIONAL UNIVERSITY OF IRELAND, CORK
  • Vienna University of Technology
  • University of Opole
  • Daegu University
  • National Fusion Research Institute (NFRI)
  • Dublin City University
  • Pelin Llc
  • Arizona State University
  • Universidad Complutense de Madrid
  • University of Basel
  • Universidad Carlos III de Madrid
  • Consorzio CREATE
  • NCSR 'Demokritos'
  • Purdue University
  • University of California
  • Universidade de São Paulo
  • Lithuanian Energy Institute
  • HRS Fusion
  • Politecnico di Torino
  • University of Cassino
  • University of Electronic Science and Technology of China

Onderzoeksoutput: Bijdrage aan een tijdschriftArtikelpeer review

8 Citaten (Scopus)

Samenvatting

Alfvén eigenmodes (AEs) are routinely seen in present-day tokamaks and stellarators with energetic particles and they represent an attractive form of MHD spectroscopy that provides valuable information on background plasma and on the energetic particles. Possible use of AEs is assessed for MHD spectroscopy of plasma with high-velocity pellet injection employed for fuelling the plasma core. Diagnostics of temporal evolution of the ablated pellets, as well as physics effects determining the diffusion/relaxation of the post pellet profile are of high importance for validating the pellet models and extrapolating them towards ITER. In this paper, JET discharges with ICRH-driven AEs and pellets launched from outboard and inboard tracks are considered. During the pellet injection, an increase in plasma density on a time scale ≪ 50 ms occurs, and several effects on AEs are observed: (1) frequency of the AEs throughout the pellet injection sweeps down by as much as ∼30%, (2) the AE amplitudes increase during the AE frequency sweeping, and (3) spectrum of toroidal mode numbers of the AEs broadens significantly after the pellet injection. The effects observed are interpreted in terms of a rise in plasma density and an enhancement of the mode amplitude resulting from the resonance sweeping during the pellet injection.

Originele taal-2Engels
Artikelnummer082008
TijdschriftNuclear Fusion
Volume58
Nummer van het tijdschrift8
DOI's
StatusGepubliceerd - 29 jun. 2018

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