‘Note: Page numbers followed by “f” indicate figures and “t” indicate tables.’
Active gas handling system (AGHS),
219Advanced Material Tokamak Experiment (AMTEX) program,
168Alcator C-Mod
compressional-Alfven wave,
313core turbulence and transport
multimachine scaling,
309nonlinear gyrokinetic turbulence models,
309particle and impurity transport,
311quantitative analysis,
309self-generated flows and momentum transport,
310–311, 310fhigh-temperature superconductors (HTS),
315–316ion cyclotron range of frequencies (ICRF),
313material erosion and tritium retention,
300pedestal and edge barrier regimes
reactor-scale device,
306plasma–material interface,
300ARIES-CS power plant
Axial symmetric divertor experiment (ASDEX) Upgrade,
17–18, 18felectron cyclotron–current drive (ECCD),
93–94L–H transition power threshold,
93–94medium-sized tokamak (MST),
93MHD modes and disruptions
electron cyclotron–current drive (ECCD),
109high thermal and mechanical loads,
110–111massive gas injection (MGI),
109plasma current evolution,
111, 111frunaway electrons (REs),
111pedestal and H-mode physics
linear peeling–ballooning stability,
100–101plasma–facing components (PFCs),
93–95plasma wall interaction
edge localized modes (ELMs),
98ionization stages,
98, 99fmagnetic perturbation coils,
98plasma wall interaction (PWI) project,
93–94technical features,
94–95TORBEAM calculations,
114Balance of plant (BOP)
energy storage system (EES),
80–81industrial steam cycle (Rankine) layout,
79, 80fintermediate heat exchanger (IHX),
81intermediate heat transport and storage system (IHTS),
80–81light water reactor technology,
81, 82fBootstrap current density,
13Broader Approach (BA) Satellite Tokamak Program,
439Contextual constraints, magnetic fusion power plants
neutral beam-based diagnostics,
568–569Edge coherent mode (ECM),
415, 416fEdge localized modes (ELMs),
21, 98control
pedestal evolution
normalised linear growth rate,
377, 377fEdge transport barriers (ETBs),
174Electron Bernstein wave (EBW)
Electron cyclotron current drive (ECCD),
23, 93–94, 109Electron cyclotron emission (ECE) measurements,
571Electron cyclotron heating (ECH),
571Electron cyclotron resonance heating (ECRH),
472–473, 473fElectron cyclotron (EC) systems
component layout and power supply circuit,
518, 519fEUROfusion consortium,
522layout and plasma side, launch system,
518, 519fshort-pulse prototype gyrotron,
522Energy storage system (EES),
80–81Enhanced reversed shear (ERS),
131Environmental constraints, magnetic fusion power plants
relativistic effects,
565stray microwave absorption,
565–566European Fusion Development Agreement (EFDA),
216European Power Plant Conceptual Study (PPCS),
580Experimental advanced superconducting tokamak (EAST)
heating and current drive system,
409, 410fhigh-performance long-pulse operation
edge coherent mode (ECM),
415, 416fGreenwald density limit,
416steady-state divertor power load,
428integrated advanced-operation scenario
beam torque and rotation-related quantities,
430–431, 431tlarge superconducting magnet application,
435long-pulse high-performance regimes,
411–412material and plasma evaluation system (MAPES),
428mission and orientation,
412neoclassical toroidal plasma viscosity (NTV),
419, 420fnonresonant magnetic braking studies,
420resonant magnetic perturbation (RMP) coil system,
409–411RF-dominated regimes,
417steady-state core plasma operation,
428–429superconducting conductors,
433, 433ftungsten (W)-based materials,
435Force-free helical reactor (FFHR)
FFHR-d1 type fusion-reactor,
585, 586fhelical divertor, advantage,
583heliotron reactor concept,
583high-temperature superconductors (HTS),
584large helical device (LHD),
581, 581flow-temperature superconductor (LTS),
583–584magnetohydrodynamic (MHD) stability,
581reference blanket concept,
584resonant magnetic perturbation (RMP),
584–585
edge-localized mode triggering,
541effective fuelling rate,
535unmagnetized plasma jet,
541Fusion blankets,
Fusion nuclear science facility (FNSF),
359Fusion power plant (FPP),
61Global energy economy,
high-power and long-pulse length requirements,
516high power long pulse operations,
277–278ion cyclotron resonance heating (ICRH) system,
279–280, 279flower hybrid current drive (LHCD) system,
278, 278fplasma density and temperature,
516Thomson Tubes Electroniques (THALES),
278tritium breeding ratio,
517Helical-axis advanced stellarator reactor
3-D neutronic investigations,
589European fusion program,
588Helias 5-B engineering study,
589, 591fHTS technology, application,
588Heliotron fusion power plant
bridge-type lap joint,
489high-Tc superconductor (HTS),
489self-cooled liquid breeding blanket,
489Helium-cooled pebble bed (HCPB),
65, 66fIntermediate heat exchanger (IHX),
81Intermediate heat transport and storage system (IHTS),
80–81Ion cyclotron (IC) systems
coaxial transmission lines (TL),
524EUROfusion consortium,
526near-term development program,
525
Japanese and European fusion research communities,
442Joint European Torus (JET)
carbon plasma-facing components,
215disruptions
plasma current, centroid and poloidal magnetic field,
224–225, 225fEuropean Fusion Development Agreement (EFDA),
216fusion physics
Alfvén eigenmodes (AEs),
252central electron temperature
vs. alpha power,
250f, 251–252classical Coulomb collisions,
250–251deuterium–tritium mixtures,
253–254normalised ion thermal conductivity
vs. effective mass,
252f, 253fusion reactor
active gas handling system (AGHS),
219deuterium–tritium experiment (DTE1),
218deuterium–tritium experiment (DTE2),
219–220edge localised mode (ELMs),
220–221ion cyclotron resonance heating (ICRH),
220–221lower hybrid current drive system,
219–220technical control system,
216high-fusion performance
deuterium–tritium mixtures,
244–245electron cyclotron current drive system,
247–248highest fusion energy pulse, time history,
245–246, 246fhighest fusion power pulse, time history,
245–246, 245fnonaxisymmetric magnetic fields,
247–248noninductive current drive power,
247–248optimised shear discharges,
246, 247fJET Joint Undertaking (JJU),
216plasma-wall interactions
beryllium divertor experiment,
231–232divertor plasma geometry,
233ITER-like wall (ILW),
232low-energy beryllium sputtering,
233reactor-relevant conditions,
228scrape-off layer
chamber neutral pressure,
233, 235ftransport and confinement
dimensionless thermal energy confinement time
vs. global-scaling relation,
239–240, 239fhigh-performance hybrid discharges,
238–239nonlinear electromagnetic turbulence,
238–239normalised diffusive and convective transport,
241, 241ftangential and normal injection,
240, 240f
JT-60SA
Broader Approach (BA) Satellite Tokamak Program,
439burn simulation, high-β and high-bootstrap fraction,
462–463, 463fcharacteristics
high-resolution diagnostics,
451high-temperature superconducting current leads,
446power supply systems,
447superconducting poloidal field coils,
445superconducting toroidal field coils,
445edge pedestal and edge-localized modes,
457–458high core plasma performances,
459high-energy particle physics,
459high-erosion and tritium-retention rates,
464–465initial research phase,
465integrated plasma performance,
453, 454fintegrated research phase,
465ITER and DEMO
integrated plasma performance,
442, 443fresistive wall mode (RWM),
444theoretical models and simulation codes,
444–445tritium breeding ratio (TBR),
444Japanese and European fusion research communities,
442nondimensional parameters,
455, 456fresearch phases and components status,
465, 466tsteady-state high-plasma-pressure operations,
439, 440fsteady-state safety factor profile,
459–460test peripheral technology,
465active MHD stability control
neoclassical tearing mode suppression,
198, 199fAdvanced Material Tokamak Experiment (AMTEX) program,
168DEMO Fusion Power Plant,
211edge transport barriers (ETBs),
174heat and particle control
heating and current drive
high-resolution measurements,
167–168high-βp mode plasmas
central heating and beam fueling,
178confinement improvement factor,
181, 181f
density and temperature profiles,
182internal transport barrier (ITB),
181, 182fsawtooth-free target plasmas,
178–180steady-state tokamak operation,
181H-mode plasmas
hot-ion enhanced confinement,
170integrated plasma performance,
176, 177fnegative-ion-based neutral beam (NNB),
168perpendicular neutral beam (PNB) injection,
170–172positive-ion-based neutral beam,
168reversed shear (RS) mode plasmas,
167Motional Stark effect (MSE) measurement,
188superconducting tokamak,
168tokamak physics experiment (TPX),
174triangularity configurations,
172–173vacuum vessel and the poloidal field coils,
170, 171fLarge helical device (LHD)
characteristics
high-temperature magnetized plasma,
485NB plasma initiation technique,
482quasi-steady state high-beta operation,
482, 483felectron cyclotron resonance heating (ECRH),
472–473, 473fion cyclotron range of frequency heating,
474, 475flocal island divertor (LID),
471neutral beam injection (NBI) heating,
474rotational transform, radial profile,
472, 472fLarge-scale clean energy,
Light water reactor technology,
81, 82fLiquid breeder concepts,
66–67Lower hybrid (LH) systems
Frascati Tokamak Upgrade,
533Toshiba Electron Tube Devices,
532–533
Magnetic fusion power plants
diagnostics
charge-exchange recombination spectroscopy (CER/CXRS),
555–556contextual constraints,
560DEMO and power plants,
569diagnostic and port plug integration,
572emerging data analysis techniques,
570–571environmental constraints,
560heat and particle exhaust,
559ITER toroidal interferometer and polarimeter (TIP),
571, 572fmagnetic equilibrium conditions,
570measurement requirements,
557motional stark effect (MSE),
553–554plasma current and density measurements,
559steady-state operation,
558edge-localized mode triggering,
541effective fuelling rate,
535unmagnetized plasma jet,
541Lawson criteria triple product,
509requirements and capabilities,
509Magnetohydrodynamic (MHD) instabilities,
10–11Magneto-hydrodynamic (MHD) pressure drops,
68–69Massive-gas injection (MGI),
45Material and plasma evaluation system (MAPES),
428Medium-sized tokamak (MST),
93Mega amp spherical tokamak (MAST)
component test facility (CTF),
359cross-field transport,
386double null (DN) configuration,
386D-shaped poloidal cross-section,
359electron Bernstein wave (EBW) heating,
362fast-ion physics and current drive
neutral beam current drive,
385, 386fself-sufficient burning plasma,
380fusion nuclear science facility (FNSF),
359heat load distribution,
386internal n = 1 kink mode
equilibrium reconstructions,
391magnetic confinement fusion research programme,
359MAST-U
Core scope, features,
399fully noninductive flat top,
402–403fully noninductive start-up,
399multibarrel pellet injector,
362plasma confinement
edge-localised modes,
363plasma start-up
HFS coils, neutron shielding,
395merging compression start-up,
395–396Small Tight Aspect Ratio Tokamak (START),
359spatiotemporal resolution,
370turbulent core transport,
370Momentum exhaust
momentum loss factor,
39, 39fmultifaceted axisymmetric radiation,
40radiated power fraction
vs. line-averaged density,
40–41, 42fNational Spherical Torus eXperiment (NSTX) Upgrade
bootstrap and beam-driven noninductive,
352boundary physics
cross-field transport,
3413D heat-conduction solver,
344edge and SOL turbulence measurements,
344–345Princeton Plasma Physics Laboratory,
347snow flake divertor (SFD),
345energetic particles
EP-induced magnetic fluctuations,
337, 338ffishbone-like energetic particle mode,
338–340high-frequency modes,
337parallel magnetic field perturbation and electric field contours,
340–341, 340ftoroidal Alfvén eigenmodes (TAEs),
337high-flux expansion snow flake/X-divertors,
353–354macroscopic stability
neoclassical tearing modes (NTMs),
334noninductive bootstrap fraction,
332resonant field amplification (RFA),
334, 335f
Magnum-PSI divertor test stand,
353–354plasma-facing component (PFC),
326transport and turbulence
electron-gyroradius scales,
331L-mode global confinement scaling,
328–329Negative-ion-based neutral beam (NNB),
168Neoclassical toroidal plasma viscosity (NTV),
419, 420fNeutral beam current drive (NBCD) system,
402Neutral beam injection (NBI) heating,
123, 207, 474Neutral beam (NB) systems
actively cooled duct,
528Broader Approach agreement,
530EUROfusion consortium,
530multiple beam system and ITER 1-MV system,
526, 527fnegative ion-based systems,
529reliability and availability,
529Pellet injection technology
anticipated fuelling rates,
538–539differential pumping system,
538pellet acceleration methods,
537steady-state operation,
538volume and speed distribution,
538, 539fPlasma exhaust
divertor heat exhaust channel,
53–55, 54fexhaust requirements,
32–33ITER tokamak, poloidal cross-section,
32, 33fplasma–material interactions (PMI),
31, 32fblobs/intermittent plasma objects,
46–47main chamber recycling,
47steady-state peak heat flux,
55transients and 3D effects
plasma/magnetic field stored energy,
41power-producing reactors,
45shattered pellet and massive-gas injection,
45, 46fsubstantial toroidal asymmetries,
45–46Plasma facing materials,
solids
ion cyclotron radio frequency (ICRF),
48–49Plasma performance, burn and sustainment
bootstrap current density,
13energy confinement time,
8–9external heating power,
12nested magnetic surfaces,
plasma operation scenario,
13safety factor,
self-heating, α-particles,
12stability
edge localised mode (ELM),
21electron cyclotron current drive (ECCD),
23helical perturbation magnetic fields,
20–21, 20fmagnetohydrodynamic (MHD) instabilities,
10–11neoclassical tearing modes (NTMs),
11, 21–22quasi-stationary ELMing H-mode discharge,
21, 21fresistive wall mode (RWM),
20–21tokamak operational scenarios
advanced operational scenarios,
25conventional scenarios,
25pressure and safety factor,
25, 26freversed shear scenario,
27toroidal magnetic geometry,
, 7ftoroidicity-induced Alfvén eigenmodes (TAEs),
12transport
cross-field transport,
linear stability,
17, 17fquasi-linear approach,
16–17refined collisional transport,
self-consistent ab-initio turbulence simulation,
19–20Power exhaust
central line-averaged density,
106–108charge exchange process,
37dissipative process,
34–35dominant dissipative process,
37, 38fmagnetic flux expansion ratio,
36neoclassical toroidal viscosity,
105–106peak divertor heat flux,
36private flux region (PFR),
37steady-state power balance,
34–35W influx and W concentration,
106, 107f
Power extraction
components
ITER divertor, W-mono-block confi guration,
74–76, 75fneutron first wall loading,
71, 72fradial volumetric heat power distribution,
72, 73fradiative flow distribution,
73, 74fthermal conductivity,
72–73thermo-mechanic performances,
76Pressure water reactor (PWR),
65–66Resistive wall mode (RWM),
20–21Resonant magnetic perturbation (RMP) coil system,
409–411Reversed shear (RS) mode,
131, 167Motional Stark effect (MSE) measurement,
188Rotating electrode method,
65Shattered pellet injection (SPI),
45Small Tight Aspect Ratio Tokamak (START),
359Snow flake divertor (SFD),
345Solid breeder technology,
64Stellarator fusion power plants
Alfvénic instabilities,
596compact stellarator
Dual Coolant Lithium Lead (DCLL) configuration,
594tungsten–carbide (WC) shield,
594European Power Plant Conceptual Study (PPCS),
580neoclassical tearing modes,
577quasiaxisymmetric compact stellarator concept,
597support-structure scales,
580tritium breeding ratio (TBR),
578–579Superconducting Magnet Power Supply (SCMPS),
447Test Blanket Programme,
69–70Tokamak fusion test reactor (TFTR)
activated/contaminated components,
127cryogenic distillation system,
125alpha-driven instabilities,
159, 160falpha loss rate
vs. pitch angle and gyroradius,
152, 153ffusion power optimization,
148, 149flost-alpha detectors,
153non-sawtoothing D-T supershot,
155, 156fsupra-thermal alpha particles,
155fueling and impurity injection systems,
124heating systems
neutral beam injection (NBI),
123neoclassical resistivity,
141neoclassical tearing modes (NTMs),
145–146neutral beam injection–heated plasmas
enhanced reversed shear (ERS),
131high internal inductance regime,
130–131plasma-facing components (PFCs),
122pressure-driven MHD instabilities,
143–144pulse discharge cleaning (PDC),
122thermal energy and particle confinement
constant-current discharges,
135–136effective ion thermal diffusivity,
134, 135ffluctuation-driven transport,
136heat pulse propagation,
140ion temperature gradient (ITG) mode,
134–135nondimensional plasma parameters,
133ohmically heated plasmas,
132perturbative transport studies,
140spatial correlation functions and wave number spectra,
137, 138fthermal plasma confinement,
133transport coefficients,
134turbulent fluctuations,
136volume-average density,
134tritium gas delivery and exhaust system,
124, 125ftritium retention and removal,
125–126US Atomic Energy Commission,
119
Tore Supra
actively cooled endoscopes,
269, 270factively cooled plasma facing components
actively cooled cooper alloy,
277brazed first wall concept,
273, 275fplasma–wall interaction,
277thermal and mechanical properties,
275–276centrifugal pellet injector,
268–269European fusion roadmap,
261Frank–Condon neutrals,
269French Tokamak Tore Supra,
261high power long pulse operations,
277–278ion cyclotron resonance heating (ICRH) system,
279–280, 279flower hybrid current drive (LHCD) system,
278, 278fThomson Tubes Electroniques (THALES),
278IR thermography system,
269long pulse experiments
accumulated carbon deposits,
284–285constant retentions rate,
286cumulated gas injection and wall inventory,
286, 286fdensities and non-inductive current,
285stable plasma scenario,
284steady-state plasma control,
283lower hybrid current drive system,
266–267niobium titanium (Nb–Ti),
262plasma–wall equilibrium time-scale,
291, 291fTungsten (W) Environment in Steady-State Tokamak (WEST) project,
292limiter to divertor configuration,
288, 288flong pulse H-mode operation,
290–291water-cooled copper coils,
262Toroidal Alfvén eigenmodes (TAEs),
337Toroidicity-induced Alfvén eigenmodes (TAEs),
12Tritium production
HCLL system and T control mechanisms,
86, 86fhelium purge-gas transports,
86liquid breeder blankets,
85neutron multiplication,
85thermonuclear reaction,
84tritium breeding ratio (TBR),
84tritium residence time (TRT),
85US ARIES Programme,
68–69US Atomic Energy Commission,
119completed stellarator device,
503, 503flast closed flux surface (LCFS),
496magnetic field geometry optimization,
494physics-optimized magnetic field geometry,
494stellarator optimization,
496three-dimensional geometry,
501–502