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Overview of the MAST Upgrade physics programme: testing novel concepts at low aspect ratio to inform future devices
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Abstract
The research programme performed on the Mega Amp Spherical Tokamak (MAST) Upgrade experiment has made significant advances in developing the physics understanding of low aspect ratio tokamaks in support of the operation of ITER and design of fusion powerplants. High performance plasma scenarios have been developed to facilitate a broad programme of experiments, in which confinement is constrained by the presence of
m
/
n
= 2/1 modes that cause substantial losses of fast ions. The onset of these modes coincides with the
q
= 2 surface residing in a local minimum in the toroidal current density profile. The maximum electron temperature at the pedestal top,
T
e,ped
is limited with gas fuelling to ∼350 eV to maintain regular ELMs; higher
T
e,ped
results in a transition to a non-stationary ELM-free regime. The operational space of spherical tokamaks has been expanded into small and ELM-free regimes. Strong shaping of the last closed flux surface can induce a transition from large to small ELMs, and ELM suppression with resonant magnetic perturbations has been observed for the first time in a low aspect ratio tokamak. Negative triangularity shaping has induced a transition from ELMy H-mode to a high-performance L-mode regime for the first time in a low aspect ratio tokamak. In studies of fast ion confinement, losses of fast particles due to Global Alfvén Eigenmodes have been identified. Interactions between fast ions generated by off-axis neutral beam injection and thermal neutrals can result in significant losses of fast ions. Experiments with on- and off-axis neutral beam injection exhibit a flux pumping mechanism, where the central safety factor is held to ∼1 in the absence of sawteeth. In studies of pedestal physics, it has been found that elevated main chamber neutral pressures result in an increase in the electron density and reduction in the temperature at the pedestal top. Advances in understanding plasma exhaust include the integration of a high-performance plasma core with detached outer divertors in the
X
-point target configuration. A newly commissioned lower divertor cryopump reduces the lower divertor neutral pressure by up to 50%, with minimal effect on the main chamber or upper divertor. New measurements and SOLPS-ITER simulations emphasise the importance of plasma–neutral interactions on divertor detachment in the conditions accessible in experiments. Real-time control of the ionisation front location in both divertor chambers independently has been demonstrated in double null experiments, enabled by the tightly baffled divertor chambers.
IOP Publishing
J.R. Harrison
A. Aboutaleb
M. Aljunid
S.Y. Allan
R. Allan
A. Alli
H. Anand
Y. Andrew
L.C. Appel
A. Ash
J. Ashton
F. Auriemma
O. Bachmann
S. Bakes
P. Balazs
O. Bardsley
M. Barnes
B. Barrett
D. Baver
C. Beckley
J. Bennett
J. Bentley
J. Berkery
M. Bernert
N. Bertelli
P. Bilkova
S. Blackmore
A. Bock
W. Boeglin
P. Bohm
J. Booth
A. Bosnjak
C. Bowman
J. Bradley
L. Bramucci
D. Brida
M. Brix
P.K. Browning
D. Brunetti
P. Bryant
J. Bryant
J. Buchanan
M. Bull
M. Bulman
N. Bulmer
D. Burke
P. Cahill
P. Cano-Megías
M. Carpita
A. Carruthers
L. Casali
A. Cassidy
F. Causa
M. Cecconello
A. Celora
M. Cha
B. Chamberlain
B. Chapman
B. Chapman-Oplopoiou
R. Chazal
X. Chen
J. Clark
M. Clark
T. Clayton
K. Collie
D. Collishaw-Schepman
J.W. Connor
M. Coy
S. Cramp
N. Crocker
D. Cruse
G. Cunningham
M. Czarski
I. Cziegler
Y. Damizia
P. Davies
K. Davies
I. Day
E. Delabie
G.L. Derks
S. Dixon
J. Dobrashian
M. Dreval
X. Du
H. Dudding
D. Dunai
M. Dunne
F. Ebrahimi
J. Edmond
J. Edwards
H. El-Haroun
S. Elmore
Y. Enters
M. Faitsch
F. Federici
N. Fedorczak
F. Felici
N. Ferraro
A.R. Field
P. Figueiredo
I. FitzGerald
M. Fitzgerald
R. Fitzpatrick
C. Fitzpatrick
S. Frankel
L. Frassinetti
D. Frattolillo
S. Freethy
W. Fuller
R. Futtersack
S. Gabriellini
K. Gage
J. Galdon
J. Galdon-Quiroga
M. Gambrioli
C. Garner
L. Garzotti
T.E. Gheorghiu
K.J. Gibson
C. Gibson
E. Giovannozzi
C. Giroud
J. Goatley
A. Goodyear
M. Gorelenkova
S. Gosden
G. Grassler
J.P. Graves
D. Greenhouse
R. Griffiths
V.H. Hall-Chen
C.J. Ham
E. Harrington
R. Harrison
A. Haupt
J. Hawes
S. Hegedus
S.S. Henderson
C. Heo
C. Hickling
M. Hill
B. Hnat
C. Hogben
B. Honey
L. Howlett
Z. Huang
A. Hudoba
J. Hughes
R. Hussain
K. Imada
P. Ivanov
A. Jackson
P. Jacquet
F. Jaulmes
P. Jepson
T. Jones
P. Jones
M. Juvonen
V. Kachkanov
B. Kandan
I. Katramados
S. Kaye
Y.O. Kazakov
D. Keeling
D. Kennedy
A. Kenny
H-T. Kim
D. King
R. King
A. King
V. Kiptily
A. Kirjasuo
A. Kirk
A. Kit
A. Kleiner
M. Knolker
S. Kobussen
M. Kochan
L. Kogan
B. Kool
D. Kos
M. Kotschenreuther
M. Lampert
A. Lawson
K. Lawson
K.-W. Lee
G. Lee
J. Lee
M. Lees
S. Leigh
A.W. Leonard
G. Liddiard
B. Lipschultz
E. Litherland-Smith
Y.Q. Liu
B.A. Lomanowski
J. Lombardo
N. Lonigro
J. Lore
J. Lovell
R. Lucock
T. Luong
A. Lvovskiy
J. Macdonald
T. Macwan
S. Mahajan
F. Maiden
R. Maingi
C. Man-Friel
F. Mansfield
M. Markl
S. Marsden
R. Martin
R. Mathew
R. Maurizio
U. Mazzarese
S. Mazzi
R. McAdams
G. McArdle
J. McBride
K. McClements
J. McClenaghan
D. McConville
K. McKay
C. McKnight
P. McKnight
A. McLean
B.F. McMillan
A. McShee
J. Measures
N. Mehay
S. Menmuir
H.F. Meyer
C.A. Michael
F. Militello
I.G. Miron
R. Mishra
J. Mitchell
D. Moiraf
P. Monaghan
R. Mooney
N. Mooring
R. Morales Gomes
D. Morbey
S. Mordijck
C. Morgan
J. Morris
D. Moulton
S. Munaretto
A. Munasinghe
A. Muraro
O. Myatra
Y.-S. Na
T.F. Neiser
A.O. Nelson
S.L. Newton
M. Nicassio
M.G. O’Mullane
C. Olde
H.J. Oliver
P. Ollus
J. Omotani
M. Ono
F.P. Orsitto
R. Osawa
N. Osborne
T. Osborne
R. Otin
E. Ozturk
F. Palermo
A. Pankin
I. Paradela Pérez
J. Parisi
E. Parr
B. Parry
B.S. Patel
E. Pawelec
D. Payne
C. Paz-Soldan
A. Phelps
L. Piron
C. Piron
G. Pokol
R. Preece
M. Price
B. Pritchard
R. Proudfoot
G. Pucella
T. Pumfrett
D.-Y. Pyo
H. Reimerdes
T. Rhodes
E. Ribeiro
D. Rigamonti
J. Riquezes
J.F. Rivero-Rodriguez
J. Roberts
M. Robson
K. Ronald
E. Rose
D. Ryan
P. Ryan
S. Saarelma
S. Sabbagh
A. Salmi
R. Sarwar
P. Saunders
O. Sauter
R. Scannell
R. Sealey
R. Seath
S. Sharapov
R. Sharma
H. Sheikh
S. Shiraiwa
B. Sieglin
S.A. Silburn
M. Simmonds
J. Simpson
A. Sladkomedova
J. Smith
P. Smith
M. Sos
V.A. Soukhanovskii
D. Speirs
C. Srinivasan
G. Staebler
R. Stephen
P. Stevenson
J. Stobbs
C. Stroud
H. Sun
H. Sun
G. Szepesi
D.M. Takács
T. Tala
C. Tame
C. Theiler
B. Thomas
S. Thomas
S. Thomas
N. Thomas-Davies
A.J. Thornton
A. Tilley
I. Tirkova
M. Tobin
E. Tomasina
A. Tonel
P. Tonner
A. Tookey
G. Tvalashvili
M. Vallar
M. Valovic
R.G.L. Vann
L. Velarde
L. Velarde
K. Verhaegh
E. Viezzer
C. Vincent
M. Walsh
T. Walsh
M. Warr
S. Wiesen
T.A. Wijkamp
D. Wilkins
J. Willis
T. Wilson
H.R. Wilson
N. Winston
G. Withenshaw
H. Wong
M. Wood
R. Worrall
Q. Xia
G. Xia
L. Xiang
G. Xiang
T. Xu
J.H. Yu
V. Zamkovska
M. Zerbini
V.K. Zotta
M. Zurita
L.E. di Grazia
Title: Overview of the MAST Upgrade physics programme: testing novel concepts at low aspect ratio to inform future devices
Description:
Abstract
The research programme performed on the Mega Amp Spherical Tokamak (MAST) Upgrade experiment has made significant advances in developing the physics understanding of low aspect ratio tokamaks in support of the operation of ITER and design of fusion powerplants.
High performance plasma scenarios have been developed to facilitate a broad programme of experiments, in which confinement is constrained by the presence of
m
/
n
= 2/1 modes that cause substantial losses of fast ions.
The onset of these modes coincides with the
q
= 2 surface residing in a local minimum in the toroidal current density profile.
The maximum electron temperature at the pedestal top,
T
e,ped
is limited with gas fuelling to ∼350 eV to maintain regular ELMs; higher
T
e,ped
results in a transition to a non-stationary ELM-free regime.
The operational space of spherical tokamaks has been expanded into small and ELM-free regimes.
Strong shaping of the last closed flux surface can induce a transition from large to small ELMs, and ELM suppression with resonant magnetic perturbations has been observed for the first time in a low aspect ratio tokamak.
Negative triangularity shaping has induced a transition from ELMy H-mode to a high-performance L-mode regime for the first time in a low aspect ratio tokamak.
In studies of fast ion confinement, losses of fast particles due to Global Alfvén Eigenmodes have been identified.
Interactions between fast ions generated by off-axis neutral beam injection and thermal neutrals can result in significant losses of fast ions.
Experiments with on- and off-axis neutral beam injection exhibit a flux pumping mechanism, where the central safety factor is held to ∼1 in the absence of sawteeth.
In studies of pedestal physics, it has been found that elevated main chamber neutral pressures result in an increase in the electron density and reduction in the temperature at the pedestal top.
Advances in understanding plasma exhaust include the integration of a high-performance plasma core with detached outer divertors in the
X
-point target configuration.
A newly commissioned lower divertor cryopump reduces the lower divertor neutral pressure by up to 50%, with minimal effect on the main chamber or upper divertor.
New measurements and SOLPS-ITER simulations emphasise the importance of plasma–neutral interactions on divertor detachment in the conditions accessible in experiments.
Real-time control of the ionisation front location in both divertor chambers independently has been demonstrated in double null experiments, enabled by the tightly baffled divertor chambers.
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