Overview of ASDEX upgrade results in view of ITER and DEMO
Artikel i vetenskaplig tidskrift, 2024
Experiments on ASDEX Upgrade (AUG) in 2021 and 2022 have addressed a number of critical issues for ITER and EU DEMO. A major objective of the AUG programme is to shed light on the underlying physics of confinement, stability, and plasma exhaust in order to allow reliable extrapolation of results obtained on present day machines to these reactor-grade devices. Concerning pedestal physics, the mitigation of edge localised modes (ELMs) using resonant magnetic perturbations (RMPs) was found to be consistent with a reduction of the linear peeling-ballooning stability threshold due to the helical deformation of the plasma. Conversely, ELM suppression by RMPs is ascribed to an increased pedestal transport that keeps the plasma away from this boundary. Candidates for this increased transport are locally enhanced turbulence and a locked magnetic island in the pedestal. The enhanced D-alpha (EDA) and quasi-continuous exhaust (QCE) regimes have been established as promising ELM-free scenarios. Here, the pressure gradient at the foot of the H-mode pedestal is reduced by a quasi-coherent mode, consistent with violation of the high-n ballooning mode stability limit there. This is suggestive that the EDA and QCE regimes have a common underlying physics origin. In the area of transport physics, full radius models for both L- and H-modes have been developed. These models predict energy confinement in AUG better than the commonly used global scaling laws, representing a large step towards the goal of predictive capability. A new momentum transport analysis framework has been developed that provides access to the intrinsic torque in the plasma core. In the field of exhaust, the X-Point Radiator (XPR), a cold and dense plasma region on closed flux surfaces close to the X-point, was described by an analytical model that provides an understanding of its formation as well as its stability, i.e., the conditions under which it transitions into a deleterious MARFE with the potential to result in a disruptive termination. With the XPR close to the divertor target, a new detached divertor concept, the compact radiative divertor, was developed. Here, the exhaust power is radiated before reaching the target, allowing close proximity of the X-point to the target. No limitations by the shallow field line angle due to the large flux expansion were observed, and sufficient compression of neutral density was demonstrated. With respect to the pumping of non-recycling impurities, the divertor enrichment was found to mainly depend on the ionisation energy of the impurity under consideration. In the area of MHD physics, analysis of the hot plasma core motion in sawtooth crashes showed good agreement with nonlinear 2-fluid simulations. This indicates that the fast reconnection observed in these events is adequately described including the pressure gradient and the electron inertia in the parallel Ohm’s law. Concerning disruption physics, a shattered pellet injection system was installed in collaboration with the ITER International Organisation. Thanks to the ability to vary the shard size distribution independently of the injection velocity, as well as its impurity admixture, it was possible to tailor the current quench rate, which is an important requirement for future large devices such as ITER. Progress was also made modelling the force reduction of VDEs induced by massive gas injection on AUG. The H-mode density limit was characterised in terms of safe operational space with a newly developed active feedback control method that allowed the stability boundary to be probed several times within a single discharge without inducing a disruptive termination. Regarding integrated operation scenarios, the role of density peaking in the confinement of the ITER baseline scenario (high plasma current) was clarified. The usual energy confinement scaling ITER98(p,y) does not capture this effect, but the more recent H20 scaling does, highlighting again the importance of developing adequate physics based models. Advanced tokamak scenarios, aiming at large non-inductive current fraction due to non-standard profiles of the safety factor in combination with high normalised plasma pressure were studied with a focus on their access conditions. A method to guide the approach of the targeted safety factor profiles was developed, and the conditions for achieving good confinement were clarified. Based on this, two types of advanced scenarios (‘hybrid’ and ‘elevated’ q-profile) were established on AUG and characterised concerning their plasma performance.
ELM free scenarios
radiative exhaust
MHD stability
disruption physics
transport modelling
tokamak
Författare
H. Zohm
Max-Planck-Gesellschaft
E. Alessi
Istituto Di Fisica Del Plasma Piero Caldirola, Milan
C. Angioni
Max-Planck-Gesellschaft
N. Arden
Max-Planck-Gesellschaft
V. Artigues
Max-Planck-Gesellschaft
M. Astrain
Max-Planck-Gesellschaft
O. Asunta
Aalto-Yliopisto
M. Balden
Max-Planck-Gesellschaft
V. Bandaru
Max-Planck-Gesellschaft
A. Banon-Navarro
Max-Planck-Gesellschaft
M. Bauer
Max-Planck-Gesellschaft
A. Bergmann
Max-Planck-Gesellschaft
M. Bergmann
Max-Planck-Gesellschaft
J. Bernardo
Instituto Superior Tecnico
M. Bernert
Max-Planck-Gesellschaft
A. Biancalani
Pôle Universitaire Léonard De Vinci
R. Bielajew
Massachusetts Institute of Technology (MIT)
R. Bilato
Max-Planck-Gesellschaft
G. Birkenmeier
Max-Planck-Gesellschaft
T.C. Blanken
Technische Universiteit Eindhoven
V. Bobkov
Max-Planck-Gesellschaft
A. Bock
Max-Planck-Gesellschaft
L. Bock
Max-Planck-Gesellschaft
T. Body
Max-Planck-Gesellschaft
T. Bolzonella
Consorzio Rfx
N. Bonanomi
Max-Planck-Gesellschaft
A. Bortolon
Princeton University
B. Böswirth
Max-Planck-Gesellschaft
C. Bottereau
Le Commissariat à l’Énergie Atomique et aux Énergies Alternatives (CEA)
A. Bottino
Max-Planck-Gesellschaft
H. Van Den Brand
Technische Universiteit Eindhoven
M. Brenzke
Forschungszentrum Jülich
S. Brezinsek
Forschungszentrum Jülich
Daniele Brida
Max-Planck-Gesellschaft
F. Brochard
Institut Jean Lamour
J. Buchanan
Culham Science Centre
A. Buhler
Max-Planck-Gesellschaft
A. Burckhart
Max-Planck-Gesellschaft
Y. Camenen
Aix-Marseille Université
B. Cannas
Universita degli Studi di Cagliari
P. Cano Megías
Max-Planck-Gesellschaft
D. Carlton
Max-Planck-Gesellschaft
M. Carr
Culham Science Centre
P. Carvalho
Instituto Superior Tecnico
C. Castaldo
ENEA
A. Castillo Castillo
Max-Planck-Gesellschaft
A. Cathey
Max-Planck-Gesellschaft
M. Cavedon
Universita' degli Studi di Milano-Bicocca
C. Cazzaniga
Consorzio Rfx
C. Challis
Culham Science Centre
A. V. Chankin
Max-Planck-Gesellschaft
A. Chomiczewska
Institute of Plasma Physics & Laser Microfusion (IPPLM)
C. Cianfarani
ENEA
F. Clairet
Le Commissariat à l’Énergie Atomique et aux Énergies Alternatives (CEA)
S. Coda
Ecole Polytechnique Federale de Lausanne (EPFL)
R. Coelho
Instituto Superior Tecnico
J.W. Coenen
Forschungszentrum Jülich
L. Colas
Le Commissariat à l’Énergie Atomique et aux Énergies Alternatives (CEA)
G.D. Conway
Max-Planck-Gesellschaft
S. Costea
University of Innsbruck
D. Coster
Max-Planck-Gesellschaft
T.B. Cote
University of Wisconsin Madison
A. Creely
Massachusetts Institute of Technology (MIT)
G. Croci
Istituto Di Fisica Del Plasma Piero Caldirola, Milan
D.J. Cruz Zabala
Universidad de Sevilla
G. Cseh
Centre for Energy Research
I. Cziegler
University of York
O. D’Arcangelo
ENEA Consorzio CREATE
A. Dal Molin
Universita' degli Studi di Milano-Bicocca
P. David
Max-Planck-Gesellschaft
C. Day
Karlsruher Institut für Technologie (KIT)
M. De Baar
Technische Universiteit Eindhoven
P. De Marné
Max-Planck-Gesellschaft
R. Delogu
Consorzio Rfx
P. Denner
Forschungszentrum Jülich
A. Di Siena
Max-Planck-Gesellschaft
M. Dibon
Max-Planck-Gesellschaft
J. Dominguez-Palacios Durán
Universidad de Sevilla
Dániel Dunai
Centre for Energy Research
M. Dreval
National Science Center
M. Dunne
Max-Planck-Gesellschaft
B. Duval
Ecole Polytechnique Federale de Lausanne (EPFL)
R. Dux
Max-Planck-Gesellschaft
T. Eich
Max-Planck-Gesellschaft
S. Elgeti
Max-Planck-Gesellschaft
A. Encheva
ITER Organization
B. Esposito
ENEA
E. Fable
Max-Planck-Gesellschaft
M. Faitsch
Max-Planck-Gesellschaft
D. Fajardo Jimenez
Max-Planck-Gesellschaft
U. Fantz
Max-Planck-Gesellschaft
M. Farnik
Czech Academy of Sciences
H. Faugel
Max-Planck-Gesellschaft
F Felici
Ecole Polytechnique Federale de Lausanne (EPFL)
O. Ficker
Czech Academy of Sciences
A. Figueredo
Instituto Superior Tecnico
R. Fischer
Max-Planck-Gesellschaft
O. Ford
Max-Planck-Gesellschaft
L. Frassinetti
Kungliga Tekniska Högskolan (KTH)
M. Fröschle
Max-Planck-Gesellschaft
G. Fuchert
Max-Planck-Gesellschaft
J.C. Fuchs
Max-Planck-Gesellschaft
H. Fünfgelder
Max-Planck-Gesellschaft
S. Futatani
Centro Nacional de Supercomputacion
K. Galazka
Institute of Plasma Physics & Laser Microfusion (IPPLM)
J. Galdon-Quiroga
Universidad de Sevilla
D. Gallart Escolà
Centro Nacional de Supercomputacion
A. Gallo
Le Commissariat à l’Énergie Atomique et aux Énergies Alternatives (CEA)
Y. Gao
Forschungszentrum Jülich
S. Garavaglia
Istituto Di Fisica Del Plasma Piero Caldirola, Milan
M. Garcia-Munoz
Universidad de Sevilla
B. Geiger
University of Wisconsin Madison
L. Giannone
Max-Planck-Gesellschaft
S. Gibson
Durham University
L. Gil
Instituto Superior Tecnico
E. Giovannozzi
ENEA
I. Girka
Max-Planck-Gesellschaft
O. Girka
Max-Planck-Gesellschaft
T. Gleiter
Max-Planck-Gesellschaft
S. Glöggler
Max-Planck-Gesellschaft
M. Gobbin
Consorzio Rfx
J. Gonzalez
Max-Planck-Gesellschaft
J. Gonzalez Martin
Universidad de Sevilla
T. Goodman
Ecole Polytechnique Federale de Lausanne (EPFL)
G. Gorini
Universita' degli Studi di Milano-Bicocca
T. Görler
Max-Planck-Gesellschaft
D. Gradic
Max-Planck-Gesellschaft
G. Granucci
Istituto Di Fisica Del Plasma Piero Caldirola, Milan
A. Grater
Max-Planck-Gesellschaft
G. Grenfell
Max-Planck-Gesellschaft
H. Greuner
Max-Planck-Gesellschaft
M. Griener
Max-Planck-Gesellschaft
M. Groth
Aalto-Yliopisto
O. Grover
Max-Planck-Gesellschaft
A. Gude
Max-Planck-Gesellschaft
L. Guimarais
Instituto Superior Tecnico
S. Günter
Max-Planck-Gesellschaft
D. Hachmeister
Instituto Superior Tecnico
A.H. Hakola
Teknologian Tutkimuskeskus (VTT)
C. Ham
Culham Science Centre
T. Happel
Max-Planck-Gesellschaft
N. Den Harder
Max-Planck-Gesellschaft
G.F. Harrer
Technische Universität Wien
J.R. Harrison
Culham Science Centre
V. Hauer
Karlsruher Institut für Technologie (KIT)
T. Hayward-Schneider
Max-Planck-Gesellschaft
B. Heinemann
Max-Planck-Gesellschaft
P. Heinrich
Max-Planck-Gesellschaft
T. Hellsten
General Atomics
S.S. Henderson
Culham Science Centre
P. Hennequin
École polytechnique
M. Herschel
Max-Planck-Gesellschaft
S. Heuraux
Institut Jean Lamour
A. Herrmann
Max-Planck-Gesellschaft
E. Heyn
Technische Universität Graz
F. Hitzler
Max-Planck-Gesellschaft
J. Hobirk
Max-Planck-Gesellschaft
K. Höfler
Max-Planck-Gesellschaft
S. Hörmann
Max-Planck-Gesellschaft
J.H. Holm
Danmarks Tekniske Universitet (DTU)
M. Hölzl
Max-Planck-Gesellschaft
C. Hopf
Max-Planck-Gesellschaft
L. Horváth
University of York
T. Höschen
Max-Planck-Gesellschaft
A. Houben
Institut Jean Lamour
A. Hubbard
Massachusetts Institute of Technology (MIT)
A. Huber
Forschungszentrum Jülich
K. Hunger
Max-Planck-Gesellschaft
V. Igochine
Max-Planck-Gesellschaft
M. Iliasova
Russian Academy of Sciences
J. Illerhaus
Max-Planck-Gesellschaft
Klara Insulander Björk
Chalmers, Fysik, Subatomär, högenergi- och plasmafysik
C. Ionita Schrittwieser
University of Innsbruck
I. Ivanova-Stanik
Institute of Plasma Physics & Laser Microfusion (IPPLM)
S. Jachmich
ITER Organization
W. Jacob
Max-Planck-Gesellschaft
N. Jaksic
Max-Planck-Gesellschaft
A. Jansen Van Vuuren
Universidad de Sevilla
F. Jaulmes
Czech Academy of Sciences
Frank Jenko
Max-Planck-Gesellschaft
T. Jensen
Danmarks Tekniske Universitet (DTU)
E. Joffrin
Le Commissariat à l’Énergie Atomique et aux Énergies Alternatives (CEA)
A. Kallenbach
Max-Planck-Gesellschaft
J. Kalis
Max-Planck-Gesellschaft
A. Kappatou
Max-Planck-Gesellschaft
J. Karhunen
Aalto-Yliopisto
C.-P. Kasemann
Max-Planck-Gesellschaft
S. Kasilov
Technische Universität Graz
Y. Kazakov
Koninklijke Militaire School
A. Kendl
University of Innsbruck
W. Kernbichler
Technische Universität Wien
E. Khilkevitch
Russian Academy of Sciences
M. Kircher
Max-Planck-Gesellschaft
A. Kirk
Culham Science Centre
S. Kjer Hansen
Massachusetts Institute of Technology (MIT)
V. Klevarova
Universiteit Gent
F. Klossek
Max-Planck-Gesellschaft
G. Kocsis
Centre for Energy Research
M. Koleva
Max-Planck-Gesellschaft
M. Komm
Czech Academy of Sciences
M. Kong
Ecole Polytechnique Federale de Lausanne (EPFL)
A. Kramer-Flecken
Forschungszentrum Jülich
M. Krause
Max-Planck-Gesellschaft
I. Krebs
Technische Universiteit Eindhoven
A. Kreuzeder
Max-Planck-Gesellschaft
K. Krieger
Max-Planck-Gesellschaft
O. Kudlacek
Max-Planck-Gesellschaft
D. Kulla
Max-Planck-Gesellschaft
Taina Kurki-Suonio
Aalto-Yliopisto
B. Kurzan
Max-Planck-Gesellschaft
B. Labit
Ecole Polytechnique Federale de Lausanne (EPFL)
K. Lackner
Max-Planck-Gesellschaft
F. Laggner
Princeton University
A. Lahtinen
Aalto-Yliopisto
P. Lainer
Technische Universität Wien
P.T. Lang
Max-Planck-Gesellschaft
Ph Lauber
Max-Planck-Gesellschaft
M Lehnen
ITER Organization
L. Leppin
Max-Planck-Gesellschaft
E. Lerche
Max-Planck-Gesellschaft
N. Leuthold
General Atomics
Li Li
Forschungszentrum Jülich
J. Likonen
Teknologian Tutkimuskeskus (VTT)
O. Linder
Max-Planck-Gesellschaft
H. Lindl
Max-Planck-Gesellschaft
B. Lipschultz
University of York
Yueqiang Liu
General Atomics
Z. Lu
Max-Planck-Gesellschaft
T. Luda Di Cortemiglia
Max-Planck-Gesellschaft
N.C. Luhmann
University of California
T. Lunt
Max-Planck-Gesellschaft
A Lyssoivan
Koninklijke Militaire School
T. Maceina
Max-Planck-Gesellschaft
J. Madsen
Danmarks Tekniske Universitet (DTU)
A. Magnanimo
Max-Planck-Gesellschaft
H. Maier
Max-Planck-Gesellschaft
J. Mailloux
Culham Science Centre
R. Maingi
Princeton University
O. Maj
Max-Planck-Gesellschaft
E. Maljaars
Technische Universiteit Eindhoven
V. Maquet
Koninklijke Militaire School
Andrea Mancini
Istituto Di Fisica Del Plasma Piero Caldirola, Milan
A. Manhard
Max-Planck-Gesellschaft
P. Mantica
Istituto Di Fisica Del Plasma Piero Caldirola, Milan
M. Mantsinen
Centro Nacional de Supercomputacion
P. Manz
Universität Greifswald
Mark Maraschek
Max-Planck-Gesellschaft
C. Marchetto
Politecnico di Torino
M. Markl
Technische Universität Wien
L. Marrelli
Consorzio Rfx
P. Martin
Consorzio Rfx
F. Matos
Max-Planck-Gesellschaft
M. Mayer
Max-Planck-Gesellschaft
P. McCarthy
University College Cork
R. McDermott
Max-Planck-Gesellschaft
G. Meng
Max-Planck-Gesellschaft
R. Merkel
Max-Planck-Gesellschaft
A. Merle
Ecole Polytechnique Federale de Lausanne (EPFL)
H.F. Meyer
Culham Science Centre
M. Michelini
Max-Planck-Gesellschaft
D. Milanesio
Politecnico di Torino
V. Mitterauer
Max-Planck-Gesellschaft
P.A. Molina Cabrera
Max-Planck-Gesellschaft
M. Muraca
Max-Planck-Gesellschaft
F. Nabais
Instituto Superior Tecnico
V Naulin
Danmarks Tekniske Universitet (DTU)
R. Nazikian
Princeton University
R.D. Nem
Danmarks Tekniske Universitet (DTU)
R. Neu
Max-Planck-Gesellschaft
A.H. Nielsen
Danmarks Tekniske Universitet (DTU)
S. K. Nielsen
Danmarks Tekniske Universitet (DTU)
T. Nishizawa
Max-Planck-Gesellschaft
M. Nocente
Universita' degli Studi di Milano-Bicocca
I. Novikau
Max-Planck-Gesellschaft
S. Nowak
Istituto Di Fisica Del Plasma Piero Caldirola, Milan
R. Ochoukov
Max-Planck-Gesellschaft
J. Olsen
Danmarks Tekniske Universitet (DTU)
P. Oyola
Universidad de Sevilla
O. Pan
Max-Planck-Gesellschaft
Gergely Papp
Max-Planck-Gesellschaft
A. Pau
Ecole Polytechnique Federale de Lausanne (EPFL)
G Pautasso
Max-Planck-Gesellschaft
C. Paz-Soldan
General Atomics
M. Peglau
Max-Planck-Gesellschaft
E. Peluso
University of Rome
P. Petersson
Kungliga Tekniska Högskolan (KTH)
C. Piron
Consorzio Rfx
U. Plank
Max-Planck-Gesellschaft
B. Plaum
Universität Stuttgart
B. Plöckl
Max-Planck-Gesellschaft
V V Plyusnin
Instituto Superior Tecnico
G. Pokol
Centre for Energy Research
E. Poli
Max-Planck-Gesellschaft
A. Popa
Max-Planck-Gesellschaft
L. Porte
Ecole Polytechnique Federale de Lausanne (EPFL)
J. Puchmayr
Max-Planck-Gesellschaft
T. Pütterich
Max-Planck-Gesellschaft
L. Radovanovic
Technische Universität Wien
M. Ramisch
Universität Stuttgart
J. Rasmussen
Danmarks Tekniske Universitet (DTU)
G.A. Rattá
Laboratorio Nacional de Fusion
S. Ratynskaia
Kungliga Tekniska Högskolan (KTH)
G. Raupp
Max-Planck-Gesellschaft
A. Redl
Universita degli Studi della Tuscia
D. Refy
Centre for Energy Research
M. Reich
Max-Planck-Gesellschaft
F. Reimold
Max-Planck-Gesellschaft
D. Reiser
Forschungszentrum Jülich
M. Reisner
Max-Planck-Gesellschaft
D. Reiter
Forschungszentrum Jülich
B. Rettino
Max-Planck-Gesellschaft
T. Ribeiro
Max-Planck-Gesellschaft
D. Ricci
Istituto Di Fisica Del Plasma Piero Caldirola, Milan
R. Riedl
Max-Planck-Gesellschaft
J. Riesch
Max-Planck-Gesellschaft
J.F. Rivero-Rodriguez
Universidad de Sevilla
G. Rocchi
ENEA
P. Rodriguez-Fernandez
Massachusetts Institute of Technology (MIT)
V. Rohde
Max-Planck-Gesellschaft
G. Ronchi
Technische Universiteit Eindhoven
M. Rott
Max-Planck-Gesellschaft
M. Rubel
Kungliga Tekniska Högskolan (KTH)
D. Ryan
Culham Science Centre
F. Ryter
Max-Planck-Gesellschaft
S. Saarelma
Culham Science Centre
M. Salewski
Danmarks Tekniske Universitet (DTU)
A. Salmi
Aalto-Yliopisto
O. Samoylov
Max-Planck-Gesellschaft
L. Sanchis-Sanchez
Universidad de Sevilla
J. Santos
Instituto Superior Tecnico
O. Sauter
Ecole Polytechnique Federale de Lausanne (EPFL)
G. Schall
Max-Planck-Gesellschaft
A. Schlüter
Max-Planck-Gesellschaft
J. Scholte
Technische Universiteit Eindhoven
K. Schmid
Max-Planck-Gesellschaft
O. Schmitz
University of Wisconsin Madison
P.A. Schneider
Max-Planck-Gesellschaft
R. Schrittwieser
University of Innsbruck
M. Schubert
Max-Planck-Gesellschaft
C. Schuster
Max-Planck-Gesellschaft
N. Schwarz
Max-Planck-Gesellschaft
T. Schwarz-Selinger
Max-Planck-Gesellschaft
Josef Schweinzer
Max-Planck-Gesellschaft
F. Sciortino
Max-Planck-Gesellschaft
O. Seibold-Benjak
Max-Planck-Gesellschaft
A. Shabbir
Universiteit Gent
A. Shalpegin
Ecole Polytechnique Federale de Lausanne (EPFL)
S. E. Sharapov
Culham Science Centre
U. Sheikh
Ecole Polytechnique Federale de Lausanne (EPFL)
A. Shevelev
Russian Academy of Sciences
G. Sias
Universita degli Studi di Cagliari
M. Siccinio
Max-Planck-Gesellschaft
B. Sieglin
Max-Planck-Gesellschaft
A. Sigalov
Max-Planck-Gesellschaft
A. Silva
Instituto Superior Tecnico
Carlos Silva
Instituto Superior Tecnico
D. Silvagni
Max-Planck-Gesellschaft
J. Simpson
Culham Science Centre
S. Sipila
Aalto-Yliopisto
A. Snicker
Aalto-Yliopisto
E. R. Solano
Laboratorio Nacional de Fusion
C. Sommariva
Ecole Polytechnique Federale de Lausanne (EPFL)
C. Sozzi
Istituto Di Fisica Del Plasma Piero Caldirola, Milan
M. Spacek
Max-Planck-Gesellschaft
G. Spizzo
Consorzio Rfx
M. Spolaore
Consorzio Rfx
A. Stegmeir
Max-Planck-Gesellschaft
M. Stejner
Danmarks Tekniske Universitet (DTU)
D. Stieglitz
Max-Planck-Gesellschaft
J. Stober
Max-Planck-Gesellschaft
U. Stroth
Max-Planck-Gesellschaft
E. Strumberger
Max-Planck-Gesellschaft
G. Suarez Lopez
Max-Planck-Gesellschaft
W. Suttrop
Max-Planck-Gesellschaft
T. Szepesi
Centre for Energy Research
B. Tál
Max-Planck-Gesellschaft
T. Tala
Teknologian Tutkimuskeskus (VTT)
W. Tang
Max-Planck-Gesellschaft
G. Tardini
Max-Planck-Gesellschaft
M. Tardocchi
Istituto Di Fisica Del Plasma Piero Caldirola, Milan
D. Terranova
Consorzio Rfx
M. Teschke
Max-Planck-Gesellschaft
E. Thorén
Kungliga Tekniska Högskolan (KTH)
W. Tierens
Max-Planck-Gesellschaft
Daniel Told
Max-Planck-Gesellschaft
W. Treutterer
Max-Planck-Gesellschaft
G.L. Trevisan
Consorzio Rfx
M. Tripský
Koninklijke Militaire School
P. Ulbl
Max-Planck-Gesellschaft
G. Urbanczyk
Max-Planck-Gesellschaft
M. Usoltseva
Max-Planck-Gesellschaft
M. Valisa
Consorzio Rfx
Martin Valovic
Culham Science Centre
S. Van Mulders
Ecole Polytechnique Federale de Lausanne (EPFL)
M.A. Van Zeeland
General Atomics
F. Vannini
Max-Planck-Gesellschaft
B. Vanovac
Massachusetts Institute of Technology (MIT)
P. Varela
Instituto Superior Tecnico
S. Varoutis
Karlsruher Institut für Technologie (KIT)
T. Verdier
Danmarks Tekniske Universitet (DTU)
Geert Verdoolaege
Universiteit Gent
N. Vianello
Consorzio Rfx
J. Vicente
Instituto Superior Tecnico
T. Vierle
Max-Planck-Gesellschaft
E. Viezzer
Universidad de Sevilla
I. Voitsekhovitch
Culham Science Centre
U. Von Toussaint
Max-Planck-Gesellschaft
D. Wagner
Max-Planck-Gesellschaft
X. Wang
Max-Planck-Gesellschaft
M. Weiland
Max-Planck-Gesellschaft
D. Wendler
Max-Planck-Gesellschaft
A.E. White
Massachusetts Institute of Technology (MIT)
M. Willensdorfer
Max-Planck-Gesellschaft
B. Wiringer
Max-Planck-Gesellschaft
M. Wischmeier
Max-Planck-Gesellschaft
R C Wolf
Max-Planck-Gesellschaft
E. Wolfrum
Max-Planck-Gesellschaft
Q. Yang
Chinese Academy of Sciences
C. Yoo
Massachusetts Institute of Technology (MIT)
Q. Yu
Max-Planck-Gesellschaft
R. Zagórski
Institute of Plasma Physics & Laser Microfusion (IPPLM)
I. Zammuto
Max-Planck-Gesellschaft
T. Zehetbauer
Max-Planck-Gesellschaft
W. Zhang
Chinese Academy of Sciences
W. Zholobenko
Max-Planck-Gesellschaft
A. Zibrov
Max-Planck-Gesellschaft
M. Zilker
Max-Planck-Gesellschaft
C. Zimmermann
Max-Planck-Gesellschaft
A. Zito
Max-Planck-Gesellschaft
S. Zoletnik
Centre for Energy Research
Nuclear Fusion
00295515 (ISSN) 17414326 (eISSN)
Vol. 64 11 112001Ämneskategorier
Annan fysik
Fusion, plasma och rymdfysik
DOI
10.1088/1741-4326/ad249d