DIII-D RESEARCH OPPORTUNITIES FORUM FOR THE 2019 EXPERIMENTAL CAMPAIGN

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ID Title Research Area Name Affiliation Time
Req'ed
Presentation ITPA
Joint Exp
ITER IO Urgent
Research Task
142Helical core in high performance scenarioTurbulence and transportKnolkerGAYesBreakoutNoNo
27Dependence of Ohmic energy confinement in negative triangularity diverted plasmasTurbulence and transportThomeGANoBreakoutNoNo
208Investigation of high-Z impurity pump-out mechanism inside of saturated MHD modesTurbulence and transportOdstrcilGAYesBreakoutNoNo
203Fast particle effects on transport of high Z ions with HFS asymmetryTurbulence and transportOdstrcilGAYesBreakoutNoNo
266Test of Turbulence Spreading Using Turbulence PropagationTurbulence and transportPettyGANoBreakoutNoNo
43Low and mid-Z impurity density asymmetryTurbulence and transportChrystalGANoBreakoutNoNo
402Nonlinear Effects of Impurity Dilution, Te/Ti, Safety Factor, and Magnetic Shear on TransportTurbulence and transportErnstMassachusetts Institute of TechnologyYesBreakoutNoNo
317Role of edge neoclassical particle transport and grad(B) drift direction in I-mode transitionsTurbulence and transportSciortinoMax-Planck Institute for Plasma PhysicsYesBreakoutNoNo
263Impurity temperature screening in ITBsTurbulence and transportSciortinoMax-Planck Institute for Plasma PhysicsNoBreakoutNoNo
90Impurity transport in diverted negative triangularity dischargesTurbulence and transportSciortinoMax-Planck Institute for Plasma PhysicsYesBreakoutNoNo
385Effect of 3D fields on turbulence and transport in DIII-D plasmasTurbulence and transportKumar BaradaUCLAYesBreakoutNoNo
38Role of turbulence in "No man's land" in determining pedestal structure and core profiles of H-modeTurbulence and transportKumar BaradaUCLAYesBreakoutNoNo
88Exploring new reactor concepts: H-mode in negative triangularity diverted plasmasTurbulence and transportMarinoniUCSDNoBreakoutNoNo
398Parametric Dependence of Turbulence and Transport on rho-star in low-rotation H-mode plasmasTurbulence and transportMcKeeU of WisconsinYesBreakoutNoNo
399Safety Factor Scaling of Turbulence and Transport in Hybrid Scenario PlasmasTurbulence and transportMcKeeU of WisconsinNoBreakoutNoNo
386Complete plasma turbulence measurements of DIII-D L-mode plasmasTurbulence and transportBurkeLLNLYesBreakoutNoNo
194Comparing the transport models experimentallyTurbulence and transportKolemenPPPLNoBreakoutNoNo
179Model validation of betaN > 3 in negative triangularity DIII-D dischargesTurbulence and transportAustinU of Texas, AustinNoBreakoutNoNo
180Transport vs rotation in DIII-D negative triangularity dischargesTurbulence and transportAustinU of Texas, AustinNoBreakoutNoNo
401Determine the critical gradient in negative triangularity dischargesTurbulence and transportAustinU of Texas, AustinNoBreakoutNoNo
256Avalanche-like electron heat transport events in MHD-quiescent plasmasTurbulence and transportChoiKorea Institute of Fusion EnergyYesGeneralNoNo
111Controlled ITB formation with narrow current channelTorkil JensenVictorLLNLYesBreakoutNoNo
25How fast can we go?Torkil JensenVictorLLNLYesBreakoutNoNo
534Doublet shape in DIII-DTorkil JensenAustinU of Texas, AustinYesBreakoutNoNo
139ITER pedestal turbulence propertiesTorkil JensenBoedoUCSDNoBreakoutNoNo
542LH power threshold, confinement scaling and CER calibration in carbon plasmasTorkil JensenMarinoniUCSDNoBreakoutNoNo
65Negligible background carbon via boron dropper for a closer approach to fusion reactor conditionsTorkil JensenRhodesUCLAYesBreakoutNoNo
541Soliton like Shock Front Dynamics during Pellet Deposition in H-modeTorkil JensenBaylorORNLYesBreakoutNoNo
535Demonstration of impurity control via an actively heated divertor in DIII-DTorkil JensenAbramsGAYesBreakoutNoNo
8ECH Beat Wave Generation of ICETorkil JensenGriersonGANoGeneralNoNo
460Use pellets to enable 2/1 NTM stabilization with very low gyrotron powerTorkil JensenBardocziGANoBreakoutNoNo
98A new path to ELM mitigationTorkil JensenKnolkerGAYesBreakoutNoYes
74Modify RE distribution function with externally launched helicon (whistler) wavesTorkil JensenPaz-SoldanColumbia UYesBreakoutNoNo
55Soft-landing of a major disruption using 3D fieldsTorkil JensenDuGAYesGeneralNoNo
92Decouple target inward/outward asymmetries due to ExB drift and due to finite ion gyro-radiusSurface EvolutionBykovGAYesBreakoutNoNo
20Ignition mechanism of arc by ELMsSurface EvolutionRohdeMax Planck Institut fuer Plasmaphysiks, Garching, GermanyNoGeneralNoNo
470Measuring intra-ELM D recycling on pre-exposed W surfacesSurface EvolutionSinclairOak Ridge Associated UniversitiesYesBreakoutNoNo
500Tracking erosion and redeposition of crystalline SiC in the DIII-D divertorSurface EvolutionSinclairGAYesBreakoutNoNo
491Spectroscopic inference of tungsten re-deposition fractionsSurface EvolutionAbramsGANoBreakoutNoNo
242Controlled low Z melting experiments using DiMES in support of ITERSurface EvolutionRudakovUCSDYesBreakoutYesYes
373Measuring net and gross erosion rates of SiC in DIII-D divertor at forward BtSurface EvolutionRudakovUCSDYesBreakoutNoNo
318Exploring the role of nonlinear MHD in triggering tearing modes in high-qmin and steady-state hybridSteady State Scenarios & High qmin ThrustChapmanU of WisconsinYesBreakoutNoNo
319Exploring the role of fluctuation-based dynamos in magnetic flux pumpingSteady State Scenarios & High qmin ThrustChapmanU of WisconsinYesBreakoutNoNo
447Optimizing Transport Through Magnetic ShearSteady State Scenarios & High qmin ThrustMcKeeU of WisconsinNoBreakoutNoNo
13Impact of broadened pressure profile on AE stability in qmin>2 reversed shear steady state scenarioSteady State Scenarios & High qmin ThrustCollinsORNLYesBreakoutYesNo
117Validate theory-based integrated scenario modeling for high qminSteady State Scenarios & High qmin ThrustParkORNLYesBreakoutNoNo
118High density & high qminSteady State Scenarios & High qmin ThrustParkORNLYesBreakoutNoNo
119High qmin in ITER shapeSteady State Scenarios & High qmin ThrustParkORNLYesBreakoutNoNo
121High qmin in lower elongation, Z = +10 cm plasma with far off-axis NBCDSteady State Scenarios & High qmin ThrustParkORNLYesBreakoutNoNo
125Optimize BT for high qminSteady State Scenarios & High qmin ThrustParkORNLYesBreakoutNoNo
189Mitigation of AEs in high performance discharges using high off-axis current driveSteady State Scenarios & High qmin ThrustKramerPPPLNoBreakoutNoNo
101ELM suppression by n=1 Ex-Vessel Coil at high qminSteady State Scenarios & High qmin ThrustHuPPPLYesBreakoutNoNo
221Detection of marginally stable modes in high qmin scenarios using the MM MHD spectroscopy vs q95Steady State Scenarios & High qmin ThrustMunarettoPPPLYesBreakoutNoNo
222Apply MM MHD spectroscopy results from #219/#221 experiments to achieve ELM suppression in high qminSteady State Scenarios & High qmin ThrustMunarettoPPPLYesBreakoutNoNo
223Use the multimode MHD spectroscopy in real time to control the NBI and modify the modes stabilitySteady State Scenarios & High qmin ThrustMunarettoPPPLYesBreakoutNoNo
219Detection of marginally stable modes in high qmin scenarios using the MM MHD spectroscopy vs shapeSteady State Scenarios & High qmin ThrustMunarettoPPPLYesBreakoutNoNo
3High qmin with betaN > 4Steady State Scenarios & High qmin ThrustVictorLLNLYesBreakoutNoNo
4Effect of rotation on confinement and stability in the high qmin scenarioSteady State Scenarios & High qmin ThrustVictorLLNLYesBreakoutNoNo
110Controlled ITB formation with narrow current channelSteady State Scenarios & High qmin ThrustVictorLLNLYesBreakoutNoNo
200Locking Avoidance in high q_min by Dynamic Error Field Correction Assisted by 3D Field EntrainmentSteady State Scenarios & High qmin ThrustOkabayashiPPPLYesBreakoutNoNo
298Optimize fast ion confinement in high qmin plasmas at high beta !Steady State Scenarios & High qmin ThrustNazikianGAYesBreakoutNoNo
265High Pedestal in Hybrid Scenario With Unfavorable Grad-B Drift DirectionSteady State Scenarios & High qmin ThrustPettyGANoBreakoutNoNo
336Pushing Steady-State Hybrid Scenario to Lower q95, Higher Beta and Higher Fusion GainSteady State Scenarios & High qmin ThrustPettyGANoBreakoutNoYes
488Steady-State Hybrids in Hydrogen With Higher Bootstrap FractionSteady State Scenarios & High qmin ThrustPettyGANoBreakoutNoNo
21High performance in the qmin~1.5 scenarioSteady State Scenarios & High qmin ThrustThomeGAYesBreakoutNoNo
22Optimizing of q and fast-ion profiles in high-qmin scenarioSteady State Scenarios & High qmin ThrustThomeGANoBreakoutNoNo
333Validation of Predict First Simulations using CCOANB 210Steady State Scenarios & High qmin ThrustGriersonGAYesBreakoutNoNo
228Use new off-axis CD tools to improve noninductive sustainability of high beta AT plasmaSteady State Scenarios & High qmin ThrustGarofaloGAYesBreakoutNoNo
484- Feasibility of plasma performance and stability of ITER steady-state operation with NB+EC CDSteady State Scenarios & High qmin ThrustPolevoiITER OrganizationNoBreakoutNoYes
431Profile control for high qmin steady state scenarioSteady State Scenarios & High qmin ThrustWehnerLehighNoBreakoutNoNo
432Profile control for high qmin steady state scenarioSteady State Scenarios & High qmin ThrustWehnerLehighNoBreakoutNoNo
433Profile control for high qmin steady state scenarioSteady State Scenarios & High qmin ThrustWehnerLehighNoBreakoutNoNo
268Map and optimize the fully non-inductive operational space for the steady-state hybrid scenarioSteady State Scenarios & High qmin ThrustTurcoColumbia UYesBreakoutNoNo
286Assess the benefits of the hybrid vs the high-qmin AT scenariosSteady State Scenarios & High qmin ThrustTurcoColumbia UYesBreakoutNoNo
169Study the access to the hybrid regime, the conditions for its sustainment and its consequencesSteady State Scenarios & High qmin ThrustTurcoColumbia UYesBreakoutNoNo
165Increase the ideal MHD limits, and the passively stable operational space, of steady-state plasmasSteady State Scenarios & High qmin ThrustTurcoColumbia UYesBreakoutNoNo
166Impact of EC location and CD on current evolution, confinement and stability of steady-state plasmasSteady State Scenarios & High qmin ThrustTurcoColumbia UYesBreakoutNoNo
167Proximity of tearing mode onset to ideal limits in high-beta plasmasSteady State Scenarios & High qmin ThrustTurcoColumbia UYesBreakoutNoNo
59Assess kinetic RWM stability of ITER steady-state scenarioSteady State Scenarios & High qmin ThrustHansonColumbia UYesBreakoutNoNo
61Measure the influence of profile broadness on global stabilitySteady State Scenarios & High qmin ThrustHansonColumbia UYesBreakoutNoNo
563Probe RWM stability using off-axis NBISteady State Scenarios & High qmin ThrustHansonColumbia UNoBreakoutNoNo
23Simultaneous Control of n=1 and n=2 Resistive Wall Modes and Stability MeasurementsSteady State Scenarios & High qmin ThrustBatteyColumbia UYesBreakoutNoNo
449m/n=2/1 NTM control by ECCD in steady state hybridSteady State Scenarios & High qmin ThrustBardocziGANoBreakoutNoNo
413Redistribute plasma momentum and particles in divertor due to the coupling of drift and sheathSOL FlowsWangGAYesBreakoutNoNo
213Search for SOL impurity stagnation regionSOL FlowsAllenLLNLNoBreakoutNoNo
233Carbon flow in plasma crownSOL FlowsAllenLLNLNoBreakoutNoNo
244Are kinetics the missing piece in our ability to predict impurity velocities in the SOL?SOL FlowsSamuellLLNLYesBreakoutNoNo
251Methane Injection Changing D+ flows in SOLSOL FlowsBoedoUCSDNoBreakoutNoNo
247ExB drifts and paralel flows in divertor and SOL before/during detachmentSOL FlowsBoedoUCSDNoBreakoutNoNo
249ExB drifts and paralel flows in divertor and SOL before/during detachmentSOL FlowsBoedoUCSDNoBreakoutNoNo
422Increase "intrinsic" edge rotation via control of edge stochasticityRotation physicsSchmitzUCLANoBreakoutNoNo
479ITG and TEM's impacts on toroidal rotation profile and intrinsic rotationRotation physicsQinU of WisconsinNoBreakoutNoNo
51Deuterium poloidal rotation measurements using main ion CER spectroscopyRotation physicsHaskeyPPPLYesBreakoutNoNo
150Competition Between Intrinsic Torque and NTV for ITERRotation physicsGriersonGANoBreakoutNoNo
54NTV Electron Root as Cause of Core Velocity Hollowing with On-Axis ECH in Very High Te H-Mode CoreRotation physicsErnstMassachusetts Institute of TechnologyYesBreakoutNoNo
12Toward Initiation of Wide Pedestal QH-Mode without NBIPedestal Physics and Pedestal Structure & QH ThrustErnstMassachusetts Institute of TechnologyYesBreakoutNoNo
291Elucidate the Physics Setting the I-mode PedestalPedestal Physics and Pedestal Structure & QH ThrustHughesMassachusetts Institute of TechnologyYesBreakoutYesNo
295Pedestal Structure and Neutral Source MeasurementPedestal Physics and Pedestal Structure & QH ThrustRosenthalMassachusetts Institute of TechnologyYesBreakoutNoNo
556168: Extend Zero Torque Wide Pedestal QH-Mode Operation to IBS ParametersPedestal Physics and Pedestal Structure & QH ThrustErnstMassachusetts Institute of TechnologyNoBreakoutNoNo
29Parametric Variation of Pedestal Turbulence and Transport in Wide Pedestal QH-ModePedestal Physics and Pedestal Structure & QH ThrustErnstMassachusetts Institute of TechnologyYesBreakoutNoNo
367Wide pedestal access at high power in QH-mode and RMP Hybrid plasmas.Pedestal Physics and Pedestal Structure & QH ThrustNazikianGAYesBreakoutNoNo
280Physics requirements for high pressure staircase pedestal formationPedestal Physics and Pedestal Structure & QH ThrustNazikianGAYesBreakoutNoNo
151Test hypothesis for the cause of improved energy confinement at lower NBI torquePedestal Physics and Pedestal Structure & QH ThrustGarofaloGAYesBreakoutNoYes
548Effect of outer gap on wide-pedestal QH-modePedestal Physics and Pedestal Structure & QH ThrustGarofaloGANoBreakoutNoNo
464Effect of impurities on pedestal structure in Peeling and Ballooning dominate discharges.Pedestal Physics and Pedestal Structure & QH ThrustOsborneGANoBreakoutNoNo
216Test ExB shear importance in QH using co-Ip approachPedestal Physics and Pedestal Structure & QH ThrustChenGAYesBreakoutNoNo
353Wide pedestal QH-mode operation at lower ZeffPedestal Physics and Pedestal Structure & QH ThrustBurrellGANoBreakoutNoNo
116Measuring Te-fluctuations within the pedestal of wide pedestal Quiescent H-mode plasmasPedestal Physics and Pedestal Structure & QH ThrustHoushmandyarGANoBreakoutNoNo
79what are those modes observed in the wide-pedestal QH edge?Pedestal Physics and Pedestal Structure & QH ThrustChenGANoBreakoutNoNo
80B x gradB drift, divertor config, Carbon effects on QH-modePedestal Physics and Pedestal Structure & QH ThrustChenGAYesBreakoutNoNo
549Further investigation of the saturation & underlying transport mechanism of EHO to allow ELM stablePedestal Physics and Pedestal Structure & QH ThrustChenGANoBreakoutNoNo
550What's the physics leads to std QH, Wide Pedestal QH,or ELMing IBS from L-mode at low torque?Pedestal Physics and Pedestal Structure & QH ThrustChenGANoBreakoutNoNo
120Disentangling impacts of heating scheme and neutral sourcing on pedestal structurePedestal Physics and Pedestal Structure & QH ThrustNelsonColumbia UYesBreakoutNoNo
290Collisionality Dependence of Quasi-Coherent FluctuationsPedestal Physics and Pedestal Structure & QH ThrustAshourvanGAYesBreakoutNoNo
292Dependence of staircase pedestal formation on input power in the RMP grassy-ELM regimePedestal Physics and Pedestal Structure & QH ThrustAshourvanGAYesBreakoutNoNo
108Measure and control resistive kink mode stabilityPedestal Physics and Pedestal Structure & QH ThrustHansonColumbia UNoBreakoutNoNo
283Exploring Access Conditions to Standard QH and WPQH PedestalsPedestal Physics and Pedestal Structure & QH ThrustWilksMITYesBreakoutNoNo
49When Is Ion Thermal Transport Neoclassical in the H-mode Pedestal?Pedestal Physics and Pedestal Structure & QH ThrustHaskeyPPPLYesBreakoutNoNo
467Main-ion, impurity and electron profile evolution throughout the ELM cyclePedestal Physics and Pedestal Structure & QH ThrustHaskeyPPPLYesBreakoutNoNo
67Unraveling the mechanism linking the pedestal structure and its dynamics to ELM energy densities in ITER relevant regimesPedestal Physics and Pedestal Structure & QH ThrustDialloPPPLNoBreakoutNoNo
109Effects of the IPD on pedestal structure and edge fluctuations leading to ELM suppressed phasesPedestal Physics and Pedestal Structure & QH ThrustDialloPPPLNoBreakoutNoNo
387Local Magnetic Field Measurements of QH-mode EHOPedestal Physics and Pedestal Structure & QH ThrustBurkeLLNLNoBreakoutNoNo
383Active MHD Spectroscopy of Edge Harmonic Oscillation (EHO) Mode Control for QH-modePedestal Physics and Pedestal Structure & QH ThrustWANGASIPPYesBreakoutYesYes
140Electron density up-down assymetryPedestal Physics and Pedestal Structure & QH ThrustMordijckThe college of William and MaryNoBreakoutNoNo
301QH-mode similarity experiment between DIII-D and AUG with co-current beamsPedestal Physics and Pedestal Structure & QH ThrustViezzerU of SevilleYesBreakoutNoNo
518Dimensionless scaling of pedestal height, width and stability - a turbulence & transport perspectivePedestal Physics and Pedestal Structure & QH ThrustBanerjeePPPLNoBreakoutNoNo
287Validation of the NIMROD resultsPedestal Physics and Pedestal Structure & QH ThrustPankinPPPLNoBreakoutNoNo
519Role of poloidal rotation on pedestal instabilitiesPedestal Physics and Pedestal Structure & QH ThrustPankinPPPLYesBreakoutNoNo
102Density pump-in by RMP in H-mode plasmaPedestal Physics and Pedestal Structure & QH ThrustHuPPPLYesBreakoutNoNo
196ELM cycle: induce at will and find the effect of edge current variation using burst CER/ThomsonPedestal Physics and Pedestal Structure & QH ThrustKolemenPPPLNoBreakoutNoNo
239Pedestal structure and stability as a function of Te/Ti and momentum injectionPedestal Physics and Pedestal Structure & QH ThrustBanerjeePPPLYesBreakoutNoNo
258Deuterium lifecycle during ELM pacing with pellet injectionPedestal Physics and Pedestal Structure & QH ThrustBortolonPPPLNoBreakoutNoNo
281Perturbative study of inter-ELM pedestal localized instabilitiesPedestal Physics and Pedestal Structure & QH ThrustLaggnerNorth Carolina StateYesBreakoutNoNo
302Measurement of EHO particle vs energy transport and phase angles with fluctuation diagnosticsPedestal Physics and Pedestal Structure & QH ThrustMortonU of WisconsinNoBreakoutNoNo
297Identifying and Detecting Microtearing Modes within the Pedestal of an H-mode PlasmaPedestal Physics and Pedestal Structure & QH ThrustMajorU of WisconsinNoBreakoutNoNo
48Identify and control pedestal turbulence modes in ELMing H-mode plasmasPedestal Physics and Pedestal Structure & QH ThrustYanU of WisconsinNoBreakoutNoNo
145HFS Pellet Fueling Deposition Dynamics in H-mode PlasmasPedestal Physics and Pedestal Structure & QH ThrustBaylorORNLNoBreakoutNoNo
146Pellet Fueling of Wide Pedestal QH-mode PlasmasPedestal Physics and Pedestal Structure & QH ThrustBaylorORNLNoBreakoutNoNo
69EHO dominated sustained wide-pedestal QH-modePedestal Physics and Pedestal Structure & QH ThrustKumar BaradaUCLAYesBreakoutNoNo
104Radially inward propagation of pedestal after L-H transition until the first ELMPedestal Physics and Pedestal Structure & QH ThrustKumar BaradaUCLAYesBreakoutNoNo
97Inter-ELM pedestal turbulence and transport when ELMs appear in wide-pedestal QH-modePedestal Physics and Pedestal Structure & QH ThrustKumar BaradaUCLAYesBreakoutNoNo
127Identify and assess pedestal magnetic fluctuations in H-mode plasmas in DIII-DPedestal Physics and Pedestal Structure & QH ThrustChenUCLAYesBreakoutNoNo
30Multi-scale/field pedestal turbulence, transport, drive, damping just prior to ELM and inter-ELMPedestal Physics and Pedestal Structure & QH ThrustRhodesUCLAYesBreakoutNoNo
34Physics of density pump-out with application of resonant magnetic perturbations (RMP)Pedestal Physics and Pedestal Structure & QH ThrustRhodesUCLAYesBreakoutNoNo
363Assessing impact of SAS alignment on divertor particle content and transition to detachmentParticle Balance and Impact of Divertor Closure Including SAS on Detachment ThrustLoreORNLYesBreakoutNoNo
364Dependence of divertor conditions on SOL width in SAS configurationParticle Balance and Impact of Divertor Closure Including SAS on Detachment ThrustLoreORNLYesBreakoutNoNo
430How does closure impact the path to complete detachment?Particle Balance and Impact of Divertor Closure Including SAS on Detachment ThrustCanikORNLYesBreakoutNoNo
437Optimizing the pumping geometry for SAS2Particle Balance and Impact of Divertor Closure Including SAS on Detachment ThrustCanikORNLNoBreakoutNoNo
428Interplay of particle control and drifts in detached divertorsParticle Balance and Impact of Divertor Closure Including SAS on Detachment ThrustShaferORNLYesBreakoutNoNo
155Characterize the impact of 3D fields on divertor closure and detachment in SASParticle Balance and Impact of Divertor Closure Including SAS on Detachment ThrustHinsonORNLYesBreakoutNoNo
427Characterization of the impact of baffling on SOL profiles at varying plasma decay lengthsParticle Balance and Impact of Divertor Closure Including SAS on Detachment ThrustJarvinenVTT Technical Research CentreYesBreakoutNoNo
404Experimentally test edge code predictions of strong correlation between T_e_target and n_D2_targetParticle Balance and Impact of Divertor Closure Including SAS on Detachment ThrustStangebyU of TorontoYesBreakoutNoNo
423Characterizing the widths of heat flux footprint in closed diverotrParticle Balance and Impact of Divertor Closure Including SAS on Detachment ThrustRenU of Tennessee, KnoxvilleYesBreakoutNoNo
436Probing the drift effect by actively biased SAS divertorParticle Balance and Impact of Divertor Closure Including SAS on Detachment ThrustRenU of Tennessee, KnoxvilleYesBreakoutNoNo
359Neutrals: How fast are they going and where are they headed?Particle Balance and Impact of Divertor Closure Including SAS on Detachment ThrustSamuellLLNLYesBreakoutNoNo
257Detachment onset in SAS: The mysterious case of shot 173537 with a fully attached divertorParticle Balance and Impact of Divertor Closure Including SAS on Detachment ThrustMcLeanLLNLYesBreakoutNoNo
267Detachment onset in SAS: The curious case of missing neutral pressure at cold plasma onset in 175816Particle Balance and Impact of Divertor Closure Including SAS on Detachment ThrustMcLeanLLNLYesBreakoutNoNo
271Detachment onset in SAS: The peculiar case of a Te cliff in 175816 with BxgradB out of the divertorParticle Balance and Impact of Divertor Closure Including SAS on Detachment ThrustMcLeanLLNLYesBreakoutNoNo
425Characterizing the widths of heat flux footprint in closed diverotrParticle Balance and Impact of Divertor Closure Including SAS on Detachment ThrustRenUTKYesBreakoutNoNo
426Characterizing the widths of heat flux footprint in closed diverotrParticle Balance and Impact of Divertor Closure Including SAS on Detachment ThrustRenUTKYesBreakoutNoNo
440Optimizing SOL width in closed divertor for particle control and detachmentParticle Balance and Impact of Divertor Closure Including SAS on Detachment ThrustMoserGANoBreakoutNoNo
438Effect of in-divertor gas puff location in SASParticle Balance and Impact of Divertor Closure Including SAS on Detachment ThrustMoserGANoBreakoutNoNo
45Coupling of drift-closure v.s. good performance pedestal assisted with dissipative divertorParticle Balance and Impact of Divertor Closure Including SAS on Detachment ThrustWangGAYesBreakoutNoNo
40characterize divertor detachment in closed divertorParticle Balance and Impact of Divertor Closure Including SAS on Detachment ThrustWangGAYesBreakoutNoNo
441How does SAS performance depend on enclosed poloidal flux?Particle Balance and Impact of Divertor Closure Including SAS on Detachment ThrustThomasGANoBreakoutNoNo
466Plasma flow in a closed divertorParticle Balance and Impact of Divertor Closure Including SAS on Detachment ThrustLeonardGAYesBreakoutNoNo
461Pedestal and core transport comparison of SAS , upper closed, and lower open divertorParticle Balance and Impact of Divertor Closure Including SAS on Detachment ThrustOsborneGANoBreakoutNoNo
463QH-mode with detached divertorParticle Balance and Impact of Divertor Closure Including SAS on Detachment ThrustOsborneGANoBreakoutNoNo
540SAS 2 precursor experimentsParticle Balance and Detachment Characterization in Closed Divertors ThrustWatkinsSandia National LabYesBreakoutNoNo
508Understand divertor leakage & SOL accumulation using isotopic methane & main ion puff/pump methodsMaterials Migration and MitigationUnterbergORNLYesBreakoutNoNo
128Dependence of upstream low-Z impurity accumulation on ExB drift directionMaterials Migration and MitigationNicholsORNLYesBreakoutNoNo
406W-pellet injection to calibrate the DIII-D Collector ProbeMaterials Migration and MitigationStangebyU of TorontoNoBreakoutNoNo
148Impurity particle balance model in order to characterize near-SOL accumulation of carbon using 13CH4Materials Migration and MitigationDuranU of Tennessee, KnoxvilleYesBreakoutNoNo
64Liquid Metal Dust Break-up MechanismsMaterials Migration and MitigationAndrewImperial College LondonYesBreakoutNoNo
235Physics of real-time wall conditioning by B dust injectionMaterials Migration and MitigationBortolonPPPLNoBreakoutNoNo
465Test free-streaming+recycling model (FSRM) for W sputtering during ELMs at low collisionalityMaterials Migration and MitigationAbramsGAYesBreakoutNoNo
93Characterize arc ignition threshold due to ELM depositionMaterials Migration and MitigationBykovGAYesBreakoutNoNo
94Core impurity contamination by unipolar arcing on high-Z PFCs and on SiCMaterials Migration and MitigationBykovGAYesBreakoutNoNo
96High-resolved ELM filament properties: spatial frequency, q_perp, j_sat, profiles of n_e and T_eMaterials Migration and MitigationBykovGAYesBreakoutNoNo
130Time resoved measurements of CX D energy and flux density at the midplane with MiMESMaterials Migration and MitigationBykovGAYesBreakoutNoNo
91Effect of ionization in the sheath on prompt redeposition of high-Z impuritiesMaterials Migration and MitigationBykovGAYesBreakoutNoNo
337ECRH plasma production on DIII-DMaterials Migration and MitigationWautersLPP-ERM-KMS � Brussels � Belgium (EUROfusion member)NoBreakoutYesYes
112Measurement of surface incident ion direction using engineered targets on DiMES at DIII-DMaterials Migration and MitigationSkinnerPPPLYesBreakoutNoNo
246Interpret W I & W II emission to benchmark S/XB coefficients & infer prompt redeposition fractionsMaterials Migration and MitigationEnnisAuburn UYesBreakoutNoNo
520Impact of Nonresonant Magnetic Perturbations on L-H and H-L TransitionsL-H transitionLoganColumbia UYesBreakoutNoNo
352Stationary Zonal FlowsL-H transitionBurrellGANoBreakoutNoNo
551What's the physics leads to std QH, Wide Pedestal QH,or ELMing IBS from L-mode at low torque?L-H transitionChenGANoBreakoutNoNo
105L-H Transitions dynamics: Impact of the beam voltage and its effects on the edge rotation shearL-H transitionBanerjeePPPLYesBreakoutNoNo
86H-mode Access Dependence on Divertor Magnetic ConfigurationL-H transitionAndrewImperial College LondonYesBreakoutNoNo
87Density Dependence of L-H TransitionL-H transitionAndrewImperial College LondonYesBreakoutNoNo
66Impact of RMP on the L-H thresholdL-H transitionDialloPPPLNoBreakoutNoNo
47Divertor configuration effects on the L-H power thresholdL-H transitionYanU of WisconsinYesBreakoutNoNo
71Role of scrape-off layer electric field in L-H power threshold scalingL-H transitionSchmitzUCLANoBreakoutNoNo
360LH power threshold, confinement scaling and CER calibration in carbon plasmasL-H transitionMarinoniUCSDNoBreakoutNoNo
188Electron- and ion-heat dominated L-H transition regimesL-H transitionSchmitzUCLAYesBreakoutNoNo
497Reducing the L-H power threshold in D plasmas with pelletsL-H transitionWilcoxORNLYesBreakoutNoNo
39Revisit pellet triggered L-H transition and understand underlying turbulence suppression mechanismsL-H transitionKumar BaradaUCLAYesBreakoutNoNo
31Optimization of hydrogen H-mode transition targeting ITER's Pre Fusion Plasma Operation StageIsotope mass ThrustRhodesUCLAYesBreakoutNoNo
502Scaling of turbulence properties with ion mixIsotope mass ThrustCarterUCLAYesBreakoutNoNo
237Influence of isotope on H-mode density limitIsotope Mass ThrustHongUCLAYesBreakoutNoNo
250Mitigate increased L-H transition threshold power in ITER PFPO hydrogen plasmas w/wo applied RMPIsotope mass ThrustSchmitzUCLANoBreakoutNoNo
536Helium scenarios for ITERIsotope mass ThrustMarinoniUCSDNoBreakoutYesNo
357Power loading at toroidal PFC gapsIsotope Mass ThrustRudakovUCSDNoBreakoutYesYes
72H-mode access in electron-heat dominated ITER PFPO hydrogen plasmasIsotope Mass ThrustSchmitzUCLAYesBreakoutNoNo
9Improved H-mode access in mixed H/He plasmasIsotope mass ThrustSchmitzUCLAYesBreakoutNoNo
70Constrain first principles L-H transition models: Favorable/unfavorable grad-B in Helium plasmasIsotope Mass ThrustSchmitzUCLAYesBreakoutNoNo
135Reducing the L-H power threshold in H plasmas with pelletsIsotope mass ThrustWilcoxORNLYesBreakoutNoNo
362Fuel Ion Particle Transport using H/D IsotopesIsotope Mass ThrustMcKeeU of WisconsinYesBreakoutNoNo
68Isotope Mass Scaling of Turbulence, Transport and ConfinementIsotope mass ThrustMcKeeU of WisconsinYesBreakoutYesNo
348Divertor configuration effects on the L-H power threshold in H plasmasIsotope mass ThrustYanU of WisconsinNoBreakoutNoNo
46Isotope mix effects (puffing He into H plasmas) on the L-H power thresholdIsotope mass ThrustYanU of WisconsinNoBreakoutNoNo
361Simultaneous measurement of electron and ion particle transport from ITG up to TEM dominated plasmaIsotope Mass ThrustTalaVTT Technical Research CentreYesBreakoutYesNo
274edge/SOL turbulence with plasma isotopic mass scaling.Isotope mass ThrustBoedoUCSDNoBreakoutNoNo
53Power Flow Through the Ion Channel for Hydrogen and He-doped L-H transition at ITER relevant Qe/QiIsotope mass ThrustHaskeyPPPLYesBreakoutNoNo
245Characterizing Detachment in H-mode Helium PlasmasIsotope mass ThrustSamuellLLNLNoBreakoutNoNo
115Role of fueling in determining the pedestal structureIsotope Mass ThrustMordijckThe college of William and MaryNoBreakoutYesYes
446Pedestal structure in hydrogen-1 plasmas relevant for non-nuclear Iter and access to ELM suppressionIsotope mass ThrustLaggnerNorth Carolina StateNoBreakoutNoNo
141Isotope effect and the role of divertor geometryIsotope Mass ThrustCasaliU of Tennessee, KnoxvilleYesBreakoutYesYes
236wide-pedestal QH in dominant electron-heated ITER PFPO hydrogen plasmasIsotope Mass ThrustChenGANoBreakoutNoNo
334Negative Triangularity in H PlasmaIsotope Mass ThrustSmithGANoBreakoutNoNo
335High performance QH-mode in H plasma with pellet fuelingIsotope Mass ThrustSmithGANoBreakoutNoNo
209Isotope mass dependence of multichannel transportIsotope Mass ThrustOdstrcilGAYesBreakoutNoNo
341Energy Confinement dependence on massIsotope mass ThrustThomeGANoBreakoutNoNo
6H vs. D Core Transport Model Validation at High Te/TiIsotope mass ThrustGriersonGAYesGeneralYesYes
122Alfven Eigenmode Stability and Fast Ion Transport with Hydrogen and Deuterium BeamsIsotope Mass ThrustVan ZeelandGAYesBreakoutNoNo
123Alfven Eigenmode Stability and Fast Ion Transport with Helium and Deuterium BeamsIsotope Mass ThrustVan ZeelandGAYesBreakoutNoNo
28Effect of Isotopic Mass on Wide Pedestal QH-Mode Core and Pedestal Turbulence and Intrinsic RotationIsotope mass ThrustErnstMassachusetts Institute of TechnologyYesBreakoutNoNo
126Effect of Isotope Mass on Intrinsic Rotation and Momentum Transport in H-Mode PlasmasIsotope Mass ThrustErnstMassachusetts Institute of TechnologyYesBreakoutNoYes
103Comparison of high density ELM suppression in H and He to DIsotope Mass ThrustEvansGANoBreakoutNoYes
476Pedestal dimensionless parameter match DIII-D to JET for H,D,HeIsotope Mass ThrustOsborneGANoBreakoutNoNo
300Study of MHD modes near L-H transition in H, H+D and H+He plasmasIsotope Mass ThrustSolanoCiematYesBreakoutNoNo
131Isotope identity pair in H and D type I ELMy H-modesIsotope mass ThrustMaggiCCFEYesBreakoutYesNo
133Rho* scaling in Hydrogen type I ELMy H-modesIsotope mass ThrustMaggiCCFEYesBreakoutYesNo
134Validation of core and edge transport models in Hydrogen L-modeIsotope mass ThrustMaggiCCFEYesBreakoutYesNo
279Isotope effect on the detachment rollover densityIsotope Mass ThrustSolokhaAalto UNoNoNo
349isotope scaling at constant rhostarIsotope Mass ThrustscottPPPLYesBreakoutNoNo
350isotope scaling with matched kinetic profilesIsotope Mass ThrustscottPPPLNoBreakoutNoNo
365Power Threshold Studies in Mixed Ion Species PlasmasIsotope Mass ThrustPlankIPP GarchingYesBreakoutYesYes
378Impact of isotope and first wall on plasma (Te, Zeff, q) during IP ramp-upIsotope mass ThrustMaillouxUKAEAYesBreakoutYesYes
379Compare H-mode plasmas with controlled ELMs in H, He, DIsotope mass ThrustMaillouxUKAEAYesBreakoutYesYes
380Investigate impact of isotope on plasmas at low and high beta/power and at low and high torqueIsotope mass ThrustMaillouxUKAEAYesBreakoutYesYes
75RMP-ELM Suppression and Mitigation in Hydrogen PlasmasIsotope Mass ThrustPaz-SoldanColumbia UNoBreakoutNoNo
95ELM-resolved D and D2 re-emission from C,W,and SiC: characterization by ro-vibrational spectroscopyInnovative Materials EvaluationBykovGANoBreakoutNoNo
220Metastable multiphase tungsten compounds: toward new fusion friendly material?*Innovative Materials EvaluationGuterlGAYesBreakoutNoNo
553Studying the PMI properties of advanced tungsten alloys with DiMESInnovative Materials EvaluationAllainU of Illinois at Urbana-ChampaignYesBreakoutNoNo
509Exposure of Graphitic foam at DiMES and TileInnovative Materials EvaluationUnterbergORNLNoBreakoutNoNo
482Pyroid HT Material Assessment using DiMESInnovative Materials EvaluationWukitchMassachusetts Institute of TechnologyYesBreakoutNoNo
312Exploring the role of nonlinear MHD in triggering tearing modes in IBS and adv. ind. hybrid scenarioInductive ScenariosChapmanU of WisconsinYesBreakoutNoNo
313Exploring the role of fluctuation-based dynamos in magnetic flux pumpingInductive ScenariosChapmanU of WisconsinYesBreakoutNoNo
229Measure and control resistive kink mode stabilityInductive ScenariosHansonColumbia UNoBreakoutNoNo
57Assess robustness of ITER baseline plasma response controlInductive ScenariosHansonColumbia UNoBreakoutNoNo
230Study the high density branch of RMP ELM suppression in the IBSInductive ScenariosTurcoColumbia UYesBreakoutNoNo
170Tailor the T=0 IBS to achieve the fusion power and gain missionInductive ScenariosTurcoColumbia UYesBreakoutNoNo
171Assess the impact of EC power location on the performance and the stability of the T=0 IBSInductive ScenariosTurcoColumbia UYesBreakoutNoNo
172Integrate ITER relevant perturbations to the IBS, assess options to maintain stability & performanceInductive ScenariosTurcoColumbia UYesBreakoutNoNo
173Asses the benefits and impact of ohmic or heated L-mode phase in the IBS ramp-upInductive ScenariosTurcoColumbia UYesBreakoutNoNo
174Make DIII-D a W or no W machineInductive ScenariosTurcoColumbia UYesBreakoutNoNo
489Developing low-disruptivity ramp-down techniques for the ITER Baseline ScenarioInductive ScenariosBarrGANoBreakoutNoNo
76RMP-ELM Suppression Access Conditions with the actual ITER shapeInductive ScenariosPaz-SoldanColumbia UYesBreakoutNoNo
77Direct comparison of ITER similar shape (ISS) and ITER baseline scenario (IBS) plasmas for RMP-ELMInductive ScenariosPaz-SoldanColumbia UNoBreakoutNoNo
37Wide Pedestal QH-Mode Path to Super H-ModeInductive ScenariosErnstMassachusetts Institute of TechnologyYesBreakoutNoNo
168Extend Zero Torque Wide Pedestal QH-Mode Operation to IBS ParametersInductive ScenariosErnstMassachusetts Institute of TechnologyYesBreakoutNoNo
377RMP ELM suppression for inductive Hybrid plasmas relevant to the ITER Q=10 missionInductive ScenariosNazikianGAYesBreakoutNoNo
320Access super H-mode in ITER Q=10 baseline targetInductive ScenariosNazikianGAYesBreakoutNoNo
149QH-mode for Q=10 IBS at Zero NBI torque by reducing the pressure profile peakingInductive ScenariosGarofaloGAYesBreakoutNoYes
355High fusion gain in the advanced inductiveInductive ScenariosThomeGANoBreakoutNoNo
538Expanding the Wide Pedestal QH to IBS ParametersInductive ScenariosChenGANoBreakoutNoNo
304How changes in ROSP, fueling location, and dRsep during D2 injection affect hybrid performanceImpurity Radiative Divertor Dependence on Divertor ClosureePetrieGAYesBreakoutNoNo
305Effect of seed selection, ROSP, and magnetic balance on successful radiating divertor operationImpurity Radiative Divertor Dependence on Divertor ClosureePetrieGAYesBreakoutNoNo
306Is krypton better than argon as a mantle seed in high power, high performance hybrid plasmas?Impurity Radiative Divertor Dependence on Divertor ClosureePetrieGANoBreakoutNoNo
307Two-impurity approach as an optimal radiating divertor solution for DIII-DImpurity Radiative Divertor Dependence on Divertor ClosureePetrieGANoBreakoutNoNo
308Effect of reversing the grad-B drift on high betaN plasmas under radiating divertor conditionsImpurity Radiative Divertor Dependence on Divertor ClosureePetrieGAYesBreakoutNoNo
310Two-impurity approach as an optimal radiating divertor solution for DIII-DImpurity Radiative Divertor Dependence on Divertor ClosureePetrieGANoBreakoutNoNo
331Minimize upstream density for divertor detachment and test radiation detachment modelImpurity Radiative Divertor Dependence on Divertor ClosureeWangGAYesBreakoutNoNo
327Effect of drifts in Ne/N2 seeded SAS divertorImpurity Radiative Divertor Dependence on Divertor ClosureeCasaliU of Tennessee, KnoxvilleYesBreakoutYesNo
328Impurity screening in closed divertorsImpurity Radiative Divertor Dependence on Divertor ClosureeCasaliU of Tennessee, KnoxvilleYesBreakoutYesNo
330Development of high radiation scenario with dual seeding in open and closed divertorsImpurity Radiative Divertor Dependence on Divertor ClosureeCasaliU of Tennessee, KnoxvilleYesBreakoutYesNo
81Snowflake SAS divertorImpurity Radiative Divertor Dependence on Divertor ClosureSoukhanovskiiLLNLNoBreakoutNoNo
85Can open horizontal plate divertor act as baffled vertical plate divertorImpurity Radiative Divertor Dependence on Divertor ClosureSoukhanovskiiLLNLNoBreakoutNoNo
234Search for Tungsten Accumulation in Upper divertorImpact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential ThrustAllenLLNLNoBreakoutNoNo
503Impact of large area electrical biasing on material erosion and divertor leakage in SAS1-WImpact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential ThrustRenU of Tennessee, KnoxvilleNoBreakoutNoNo
63Effect of Divertor Closure on Dust TransportImpact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential ThrustAndrewImperial College LondonYesBreakoutNoNo
564Impact of high-Z PFCs on impurity seeding experiments in SASImpact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential ThrustCasaliU of Tennessee, KnoxvilleNoBreakoutNoNo
434Effect of main ion SOL flows on W impurity transportImpact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential ThrustRudakovUCSDNoBreakoutNoNo
559Impurity leakage from a closed divertor during RMP applicationImpact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential ThrustHinsonORNLYesBreakoutNoNo
129Dependence of upstream high-Z impurity accumulation on ExB drift directionImpact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential ThrustNicholsORNLYesBreakoutNoNo
562Minimizing W divertor leakage in the SASImpact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential ThrustUnterbergORNLNoBreakoutNoNo
560Using the SAS to control impurity pinchImpact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential ThrustNelsonColumbia UNoGeneralNoNo
555Toroidal symmetry of SAS tilesImpact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential ThrustBykovGANoBreakoutNoNo
424Fueling effects of metal Rings in the divertorImpact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential ThrustBykovGAYesBreakoutNoNo
390Characterization of tungsten transport and leakage in the SAS divertorImpact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential ThrustMaORAUYesBreakoutNoNo
264Impact of ELM size and footprint on W sputtering and W leakage from open & closed divertorsImpact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential ThrustAbramsGAYesBreakoutNoYes
558High-Z impurity pump-out mechanism inside of MHD modes in plasma with divertor W sourceImpact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential ThrustOdstrcilGANoBreakoutNoNo
113Characterization of SOL impurity accumulation using 13CH4 injection and collector probesImpact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential ThrustZamperiniGAYesBreakoutNoNo
114Characterizing the radial/poloidal structure of SOL impurity accumulation with collector probesImpact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential ThrustZamperiniGAYesBreakoutNoNo
388Characterization of tungsten transport and leakage in the SAS divertorImpact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential ThrustMaGAYesBreakoutNoNo
557RMP ELM suppression in the SAS shapeImpact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential ThrustEvansGANoBreakoutNoNo
5210 CCOANB Counter-direction Checkout - Including Power and Ability to Balance TorqueHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)GriersonGANoBreakoutNoNo
486Helicon Modulation and Shutdown CheckoutHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)BrookmanGANoBreakoutNoNo
487Measure Peak Current Drive Efficiency in Non-Inductive ScenerioHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)BrookmanGAYesBreakoutNoNo
157Perturbative Measurements of Helicon Power Deposition and TransportHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)BrookmanGAYesBreakoutNoNo
468absorption study of top launch ECCD schemeHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)ChenGAYesBreakoutNoNo
469compare the off-axis ECCD efficiency between top and outside launchHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)ChenGAYesBreakoutNoNo
471experimental demonstration both down-shift and up-shift top launch ECCD schemesHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)ChenGANoBreakoutNoNo
472polarization study of top launchHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)ChenGANoBreakoutNoNo
7Checkout of 210 CCOANB Using Visible ImagingHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)Van ZeelandGANoBreakoutNoNo
552Parametric instabilities during Helicon wave Iinjection in DIII-DHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)PorkolabMassachusetts Institute of TechnologyNoBreakoutNoNo
481Develop QH Mode for HFS LHCD ExperimentsHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)WukitchMassachusetts Institute of TechnologyYesBreakoutNoNo
309Validate beta_e dependence of helicon CDHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)GarofaloGAYesBreakoutNoNo
478O-mode absorption and refraction for top launch ECHHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)PettyGAYesBreakoutNoNo
498Measurement of NBCD profileHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)PettyGANoBreakoutNoNo
499Helicon Current Drive MeasurementsHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)PettyGAYesBreakoutNoNo
493Establishment of High Power Operation of Comb-line Antenna Operation with PlasmaHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)PinskerGAYesBreakoutNoNo
494Measurement of high-efficiency central current drive with helicon systemHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)PinskerGAYesBreakoutNoNo
512Parametric decay study with helicon launchHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)PinskerGAYesBreakoutNoNo
345ECRH plasma production on DIII-DHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)WautersLPP-ERM-KMS � Brussels � Belgium (EUROfusion member)NoBreakoutYesYes
485Third harmonic ECH experimentsHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)SchneiderITER OrganizationNoBreakoutNoNo
370Checkout 210 beamsHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)HeidbrinkUC, IrvineNoBreakoutNoNo
324Measurement of helicon wave internal amplitude and validation of simulationHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)CrockerUCLANoBreakoutNoNo
483Off-axis NBCD measurement with 210 CCOANBHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)ParkORNLYesBreakoutNoNo
504Helicon Launcher Checkout and ConditioningHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)ZhangASIPPNoBreakoutNoNo
1Welcome to the ROF for the 2019-20 DIII-D Run CampaignGeneral PhysicsFenstermacherLLNLNoBreakoutNoNo
561Experimental Validation of Heteroclitic magnetic Island Bifurcations in DIII-DGeneral PhysicsEvansGANoBreakoutNoNo
42Determine accuracy of NUBEAM power and torque outside mid-radiusEnergetic Particle PhysicsChrystalGANoBreakoutNoNo
501Modification of AE Drive and Nonlinear Saturation Through Variation of Beam ModulationEnergetic Particle PhysicsVan ZeelandGANoBreakoutYesNo
56Hunt the instabilities responsible for the formation of phase space holeEnergetic Particle PhysicsDuGANoGeneralNoNo
546Direct measurement of the wave-particle interactions and associated phase space flowEnergetic Particle PhysicsDuGANoBreakoutNoNo
124Characterization of Fast-ion Diagnostic to Edge Neutral PopulationsEnergetic Particle PhysicsStagnerGANoBreakoutNoNo
456Stabilization of TAEs by Localized Electron Cyclotron Current DriveEnergetic Particle PhysicsSharapovCCFENoBreakoutYesNo
547Direct measurement of the wave-particle interactions and associated phase space flowEnergetic Particle PhysicsduGeneral AtomicNoBreakoutNoNo
400Verification of Imaging Fast Ion D-Alpha and application to EP model validationEnergetic Particle PhysicsMariniORAUYesBreakoutNoNo
515Parameter scan of fast-ion critical gradient thresholdEnergetic Particle PhysicsCollinsORNLNoBreakoutNoNo
299Transient ExB flows caused by bursting fast-ion modes and secondary transport-related impactsEnergetic Particle PhysicsCrockerUCLANoBreakoutNoNo
198Radial structure and identification of intermediate frequency Alfven eignemodesEnergetic Particle PhysicsCrockerUCLANoBreakoutNoNo
181ICE internal amplitude and radial structureEnergetic Particle PhysicsCrockerUCLANoBreakoutNoNo
182CAE suppression by more parallel injectionEnergetic Particle PhysicsCrockerUCLANoBreakoutNoNo
490BAAE and BAE validationEnergetic Particle PhysicsHeidbrinkUC, IrvineNoBreakoutYesNo
496Orbit Tomography (OT)Energetic Particle PhysicsGarciaUC, IrvineNoBreakoutYesNo
371ICE Mode StructureEnergetic Particle PhysicsDeGrandchampUC, IrvineYesBreakoutYesNo
147Pellet Fueled High Density Operation of RMP ELM Mitigated PlasmasELM ControlBaylorORNLNoBreakoutNoNo
52Pellet pacing with with peeling-limited pedestalELM ControlWilcoxORNLYesBreakoutNoNo
50D2 pellet pacing with tangential injectionELM ControlWilcoxORNLYesBreakoutNoNo
389Rotating MPs to study the change of ELMs in AUG similar shapesELM ControlWillensdorferMax-Planck Institute for Plasma PhysicsYesBreakoutNoNo
368Limits of RMP ELM Suppression Toward Double NullELM ControlShaferORNLYesBreakoutNoNo
177Evaluate the effect of penetration theory on RMP ELM suppressionELM ControlWANGASIPPYesBreakoutYesYes
543Strategy for ELM controlELM ControlLoarte-PrietoITER OrganizationYesGeneralNoYes
5443-D ELM suppressed regime access/exitELM ControlLoarte-PrietoITER OrganizationYesGeneralNoYes
5453-D ELM suppressed H-mode and pellet fuellingELM ControlLoarte-PrietoITER OrganizationYesGeneralNoYes
285Understanding the connection between ELM suppression and magnetic footprint size.ELM ControlMunarettoPPPLYesBreakoutNoNo
356ELM pacing by pellet injection in low-collisionality ITER relevant scenariosELM ControlBortolonPPPLNoBreakoutNoNo
537ELM pacing during ITER-like current ramp-up/downELM ControlBortolonPPPLNoBreakoutNoYes
554ELM pacing during ITER-like current ramp-up/downELM ControlBortolonPPPLNoBreakoutNoYes
393ELM pacing by pellet injection in low-collisionality ITER relevant scenariosELM ControlBortolonPPPLNoBreakoutNoNo
394ELM pacing during ITER-like current ramp-up/downELM ControlBortolonPPPLNoBreakoutNoYes
395ELM pacing during ITER-like current ramp-up/downELM ControlBortolonPPPLNoBreakoutNoYes
99Scaling of ELM suppression thresholdELM ControlHuPPPLYesBreakoutNoNo
100Understanding density pump-out in ELM control experimentELM ControlHuPPPLYesBreakoutNoNo
405Max-Planck-Institut f�¼r PlasmaphysikELM ControlWillensdorferMax-Planck-Institut f�¼r PlasmaphysikYesBreakoutNoNo
391Max-Planck-Institut f�¼r PlasmaphysikELM ControlWillensdorferMax-Planck-Institut f�¼r PlasmaphysikYesBreakoutNoNo
392Rotating MPs to study helically edge localized modes in AUG similar shapesELM ControlWillensdorferMax-Planck-Institut f�¼r PlasmaphysikYesBreakoutNoNo
369Limits of RMP ELM Suppression Toward Double NullELM ControlShaferORNLYesBreakoutNoNo
183Evaluate the effect of penetration theory on RMP ELM suppressionELM ControlWANGASIPPYesBreakoutYesYes
303ECEI and MIR contributionELM ControlZhuUC DavisYesBreakoutNoNo
231Study the high density branch of RMP ELM suppression in the IBSELM ControlTurcoColumbia UYesBreakoutNoNo
396Overdriven ELM SuppressionELM ControlLyonsGAYesBreakoutNoNo
397Establish ELM suppression in DND plasmaELM ControlLyonsGANoBreakoutNoNo
78RMP-ELM Control in Strongly Shaped PlasmasELM ControlPaz-SoldanColumbia UYesBreakoutYesNo
375direct detection of islands with rotating n=1 RMPELM ControlNazikianGAYesBreakoutNoNo
376Main ion rotation in ELM suppressionELM ControlNazikianGAYesBreakoutNoNo
407Divertor radiated power control vs. ELM frequencyELM ControlEldonGANoBreakoutNoNo
408Burn through of paced ELMs in detachmentELM ControlEldonGANoBreakoutNoNo
513Boundary Ion temperature measurement based on retarding field analyzerDivertor ClosureRenU of Tennessee, KnoxvilleYesBreakoutNoNo
259Divertor to pedestal trace impurity transportDiv/SOL Turbulence and transportBortolonPPPLNoBreakoutNoNo
262Divertor-localized turbulence and characterization of 2D profiles of divertor turbulenceDiv/SOL Turbulence and transportScottiLLNLNoBreakoutNoNo
270Evolution of edge turbulence and turbulence flow near midplane during divertor detachmentDiv/SOL Turbulence and transportWangUCLANoBreakoutNoNo
36Turbulence spreading from pedestal into SOL and testing models/scalings of lambda_qDiv/SOL Turbulence and transportRhodesUCLAYesBreakoutNoNo
358Parallel correlation of turbulence/blobs between mid-plane and divertor SOLDiv/SOL Turbulence and transportRudakovUCSDNoBreakoutNoNo
294Characterization of Te fluctuations in the divertor and main SOLDiv/SOL Turbulence and transportRudakovUCSDYesBreakoutNoNo
354Study of impurity ion entrainment in divertor cross-field transportDiv/SOL Turbulence and transportHollmannUCSDNoBreakoutNoNo
273Scaling of blobby transport with divertor conditions and pedestal/SOL wideningDiv/SOL Turbulence and transportBoedoUCSDNoBreakoutNoNo
248Poloidal asymmetries of radial transport in the edge/SOLDiv/SOL Turbulence and transportBoedoUCSDNoBreakoutNoNo
374Effect on SEE on Langmuir probe measurements in the SOLDiv/SOL Turbulence and transportRudakovUCSDNoBreakoutNoNo
421Magnetic shear at X-point and radial turbulence transportDiv/SOL Turbulence and transportBoedoUCSDNoBreakoutNoNo
144Transport and turbulence in Divertor and pedestal during detachmentDiv/SOL Turbulence and transportBoedoUCSDNoBreakoutNoNo
138Physics of pedestal turbulence vs widthDiv/SOL Turbulence and transportBoedoUCSDNoBreakoutNoNo
414Quasi-coherent fluctuations near the divertor plateDiv/SOL Turbulence and transportWangGANoBreakoutNoNo
296Imaging of turbulence in the divertor and SOL and poloidal asymmetriesDiv/SOL Turbulence and transportBykovGAYesBreakoutNoNo
415Power and momentum detachment in impurity seeded plasmas and test radiation detachment modelDissipative Divertor PhysicsWangGAYesBreakoutNoNo
225Detachment onset with X-point heightDissipative Divertor PhysicsMcLeanLLNLYesBreakoutNoNo
366DIII-D Experiments in Support of ITPA DSOL Detachment ResearchDissipative Divertor PhysicsReinkeORNLYesBreakoutYesNo
343Check for Te cliff at inner strike point in reverse BtDissipative Divertor PhysicsEldonGANoBreakoutNoNo
252Effect of divertor radiation front on drifts and parallel flowDissipative Divertor PhysicsBoedoUCSDNoBreakoutNoNo
410Radiative divertor with impurity seeding at moderate densityDissipative Divertor PhysicsJarvinenVTT Technical Research CentreYesBreakoutNoNo
411Impurity seeded radiative divertor in L-modeDissipative Divertor PhysicsJarvinenVTT Technical Research CentreYesBreakoutNoNo
416Characterization of pedestal/SOL coupling at X-point in detached conditionsDissipative Divertor PhysicsJarvinenVTT Technical Research CentreYesBreakoutNoNo
187Scaling of 2D structure of detachment frontDissipative Divertor PhysicsJarvinenVTT Technical Research CentreYesBreakoutNoNo
240How much protection does detachment give us from ELMs?Dissipative Divertor PhysicsSamuellLLNLYesBreakoutYesNo
243Optimizing the process for developing 2D reconstructions of divertor conditionsDissipative Divertor PhysicsSamuellLLNLYesBreakoutNoNo
227Impact of plasma opacity on divertor detachmentDissipative Divertor PhysicsMcLeanLLNLYesBreakoutNoNo
232Impact of spectral contamination of the MWIR regionDissipative Divertor PhysicsMcLeanLLNLYesBreakoutNoNo
255Contribution of molecules to radiated powerDissipative Divertor PhysicsMcLeanLLNLYesBreakoutNoNo
193Impact of molecular processes on divertor detachment and validation of UEDGE fluid molecular modelDissipative Divertor PhysicsHolmPPPLNoBreakoutNoNo
152Assessment of Ly-alpha opacity in fully detached divertor plasmasDissipative Divertor PhysicsGrothAalto UNoBreakoutNoNo
517Penetration characterization of small pellet injection into D3D plasmasDisruption Mitigation ThrustRamanU of WashingtonNoBreakoutNoNo
473Evaluating the internal MHD response to shell pellet injectionDisruption Mitigation ThrustPandyaU of WisconsinNoBreakoutNoNo
474Evaluating the internal MHD response to SPIDisruption Mitigation ThrustPandyaU of WisconsinNoBreakoutNoNo
475Measuring internal MHD during the formation and evolution of a runaway electron beamDisruption Mitigation ThrustPandyaU of WisconsinNoBreakoutNoNo
14Comparison of dispersive vs non-dispersive shell pellet payloadDisruption Mitigation ThrustHollmannUCSDNoBreakoutNoNo
15Suppression of RE seeds with W grains in shell pelletDisruption Mitigation ThrustHollmannUCSDNoBreakoutNoNo
16Dynamic measurement of impurity transport into RE plateau using carbon depositionDisruption Mitigation ThrustHollmannUCSDNoBreakoutNoNo
17Change in RE plateau vertical loss rate with low-Z injectionDisruption Mitigation ThrustHollmannUCSDNoBreakoutNoNo
18Scan of RE plateau final loss footprint with I-coil perturbationDisruption Mitigation ThrustHollmannUCSDNoBreakoutNoNo
19Scan of RE plateau impurity assimilation with auxiliary heatingDisruption Mitigation ThrustHollmannUCSDNoBreakoutNoNo
510Superposition of identical dual SPIsDisruption Mitigation ThrustHerfindalORNLNoBreakoutNoNo
514MGI-assisted-SPI for decreased radiation asymmetries and increased penetration depthDisruption Mitigation ThrustSweeneyMassachusetts Institute of TechnologyYesBreakoutNoNo
533Ballistic transport and energy/size scaling for SPIDisruption Mitigation ThrustShirakiORNLNoBreakoutNoNo
372whistler polarizationDisruption Mitigation ThrustHeidbrinkUC, IrvineNoBreakoutNoNo
539Effect of underlying non-axisymmetric (NA) fields on disruption mitigation processDisruption Mitigation ThrustEidietisGANoBreakoutNoNo
525Mass scaling of shell pellet assimilationDisruption Mitigation ThrustEidietisGANoBreakoutNoNo
526Full profile measurement of shell Te profileDisruption Mitigation ThrustEidietisGANoBreakoutNoNo
527Test Li coating for "ideal" shell pelletDisruption Mitigation ThrustEidietisGANoBreakoutNoNo
528Ablation measurments of single snall Ne pelletDisruption Mitigation ThrustEidietisGANoBreakoutNoNo
529Effect of D admixture in SPIDisruption Mitigation ThrustEidietisGANoBreakoutNoNo
530dilution cooling in SPI superpositionDisruption Mitigation ThrustEidietisGANoBreakoutNoNo
531Scaling of fragment penetration depth with energy:Disruption Mitigation ThrustEidietisGANoBreakoutNoNo
532JET SPI similarity experimentsDisruption Mitigation ThrustEidietisGANoBreakoutNoNo
10The role of RE-driven kinetic instabilities on formation of post-disruption RE beamDisruption Mitigation ThrustLvovskiyGAYesBreakoutNoNo
11Identification of Alfven instabilities driven by REs at negative Uloop during RE plateau stageDisruption Mitigation ThrustLvovskiyGANoBreakoutNoNo
73Role of pre-disruption electron temperature in runaway electron seed formationDisruption Mitigation ThrustPaz-SoldanColumbia UNoBreakoutNoNo
507ITER DMS design validationDisruption Mitigation ThrustLehnenITER OrganizationNoBreakoutNoNo
26Determine the cause of RE beam final loss in post disruption vertical displacement eventsDisruption Mitigation ThrustBardocziGANoBreakoutNoYes
417Collisionality effects on ELM dynamics in the high-betaP scenarioDIII-D/EAST Task Force/ThrustWeisbergGAYesBreakoutNoNo
418Investigating RWM stability in the high-betaP scenarioDIII-D/EAST Task Force/ThrustWeisbergGAYesBreakoutNoNo
226Controlling ITB formation via impurity puffingDIII-D/EAST Task Force/ThrustMcClenaghanGANoBreakoutNoNo
450Explore the Basis of Realizing ITER Q=10 at Ip<=9MA on DIII-DDIII-D/EAST Task Force/ThrustDingGAYesBreakoutNoNo
452Develop High Betap Scenario toward High Non-Inductive Current Fraction at q95~6 on DIII-DDIII-D/EAST Task Force/ThrustDingGAYesBreakoutNoNo
453Investigate the Turbulence Suppression in High Betap Plasmas when Te is Close to TiDIII-D/EAST Task Force/ThrustDingGAYesBreakoutNoNo
480Radiative divertor in high-betap plasma by utilizing SAS and local impurity injectionDIII-D/EAST Task Force/ThrustWangGAYesBreakoutNoNo
454Validating Dominant Micro-Turbulence Instabilities in DIII-D high BetaP ScenariosDIII-D/EAST Task Force/ThrustJianGAYesBreakoutNoNo
32Testing and validating low pedestal height with high core confinement plasmasDIII-D/EAST Task Force/ThrustRhodesUCLAYesBreakoutNoNo
33Is core ITB in high-betap plasmas due to ExB velocity shear or magnetic shear?DIII-D/EAST Task Force/ThrustRhodesUCLAYesBreakoutNoNo
443Compatibility of highly radiative divertor with high beta_p scenarioDIII-D/EAST Task Force/ThrustWangASIPPYesBreakoutNoYes
439Exploring high-frequency small-ELM regime in hybrid scenario on DIII-DDIII-D/EAST Task Force/ThrustWangASIPPYesBreakoutNoNo
455Detection of marginally stable modes in high betaP scenarios using the MM MHD spectroscopyDIII-D/EAST Task Force/ThrustMunarettoPPPLYesBreakoutNoNo
282Explore the use of the RMP to control the heat flux peak in high BetaP plasmas.DIII-D/EAST Task Force/ThrustMunarettoPPPLYesBreakoutNoNo
384Active MHD Spectroscopy of Edge Harmonic Oscillation (EHO) Mode Control for QH-modeDIII-D/EAST Task Force/ThrustWANGASIPPYesBreakoutYesYes
381Evaluate the effect of penetration theory on RMP ELM suppressionDIII-D/EAST Task Force/ThrustWANGASIPPYesBreakoutYesYes
382Use NBI to evaluate n=2 RMP penetration positionDIII-D/EAST Task Force/ThrustWANGASIPPYesBreakoutYesYes
505Assessing Helicon wave current drive in high betap experimentsDIII-D/EAST Task Force/ThrustZhangASIPPNoBreakoutNoNo
435Fully non-inductive high betap scenario at q95~6-7DIII-D/EAST Task Force/ThrustHuangASIPPYesBreakoutNoNo
442Access to small ELM regime in DIII-D high �²P scenarioDIII-D/EAST Task Force/ThrustQianASIPPNoBreakoutYesYes
207Measure and Influence Flow with Pump and PumpCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationAllenLLNLNoBreakoutNoNo
212Minimize carbon in DIII-D AT plasmasCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationAllenLLNLNoBreakoutNoNo
195Obtaining High Core Confinement with High Edge Confinement using Pedestal ControlCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationKolemenPPPLYesBreakoutNoNo
143Development of high radiation scenario with dual seeding in open and closed divertorsCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationCasaliU of Tennessee, KnoxvilleYesBreakoutYesNo
260Wide pedestal QH-mode at low Zeff through real-time boronizationCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationBortolonPPPLYesBreakoutNoNo
278A Boron-Nitrogen radiative divertor for AT scenariosCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationBortolonPPPLNoBreakoutNoNo
238Mapping the Super H-mode Boundary and BifurcationCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationBortolonPPPLYesBreakoutNoNo
316A Boron-Nitrogen radiative divertor for AT scenariosCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationBortolonPPPLNoBreakoutNoNo
241High performance core at high radiative fraction with real-time impurity feedback controlCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationAbbatePPPLYesGeneralNoNo
191What can lost fast-ions tell us about the H-mode pedestal?Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationKramerPPPLNoBreakoutNoNo
261Exploring the role of nonlinear MHD in triggering tearing modes in Core-Edge Scenario OptimizationCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationChapmanU of WisconsinYesBreakoutNoNo
35Reduction of background carbon via boron dropper for a closer approach to fusion reactor conditionsCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationRhodesUCLAYesBreakoutNoNo
156Impact of magnetic perturbations on SOL force balanceCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationHinsonORNLYesBreakoutNoNo
106Dependence of core-edge impurity transport on plasma shaping in Ti~Te and Ti>>Te regimesCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationSciortinoMax-Planck Institute for Plasma PhysicsYesBreakoutNoNo
107Optimization of impurity transport in RMP ELM-suppressed discharges with variable ECH locationCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationSciortinoMax-Planck Institute for Plasma PhysicsYesBreakoutNoNo
448Optimizing core-pedestal performance in Super H-ModeCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationSnyderORNLNoBreakoutNoNo
211Shape Thresholds for Super H Access and Application to JET DT CampaignCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationSnyderORNLYesBreakoutNoNo
215Core-Edge Compatibility of Super H Mode with Closed DivertorCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationSnyderORNLYesBreakoutNoNo
204Understanding the Impact of the Tokamak Edge on Rf PropagationCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationBrookmanGAYesBreakoutNoNo
202Pedestal and core impurity transport in super H-mode dischargesCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationOdstrcilGAYesBreakoutNoNo
276Super QH-mode with feedback controlled radiationCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationEldonGAYesBreakoutNoNo
277Divertor radiated power control vs. ELM frequencyCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationEldonGANoBreakoutNoNo
344Detachment onset density vs. 3D field strengthCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationEldonGANoBreakoutNoNo
340Burn through of paced ELMs in detachmentCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationEldonGANoBreakoutNoNo
409Detachment/T_e cliff onset density vs. I_p using control to stay on the edge of the cliffCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationEldonGANoBreakoutNoNo
217co-Ip QH-mode approach to super H-modeCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationChenGANoBreakoutNoNo
153Balancing the Tradeoffs Between High Performance and Core Purity & Stability in High Power HybridCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationGriersonGANoBreakoutNoNo
412Test H-L back transition transient mitigation strategies in detachmentCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationEldonGAYesBreakoutNoNo
253Investigation and optimization of core and pedestal performanceCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationSolomonGANoBreakoutNoNo
136Impurity Transport from Core to Edge in IBS-like ConditionsCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationHowardMassachusetts Institute of TechnologyYesBreakoutNoNo
137Impurity Transport from Core to Edge in Steady State Hybrid ConditionsCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationHowardMassachusetts Institute of TechnologyYesBreakoutNoNo
41Impurity Transport and Carbon Reduction in Wide Pedestal QH-ModeCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationErnstMassachusetts Institute of TechnologyYesBreakoutNoNo
214Hybrid approac to Super H-modeCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationNazikianGAYesBreakoutNoNo
565Measure lambda-q during rotation scans at constant heating power in super H mode plasmasCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationGarofaloGANoBreakoutNoNo
462Pedestal pressure enhancement at high density through decoupling of ped peeling and ballooning modesCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationOsborneGANoBreakoutNoNo
158Effect of O-mode deposition radius on tearing mode onset and impurity profiles in high betaN plasmasCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationPetrieGAYesBreakoutNoNo
159Low level RMP feedback to control deuterium/impurity buildup in high power, high performance plasmasCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationPetrieGAYesBreakoutNoNo
160How changes in ROSP, fueling location, and dRsep during D2 injection affect hybrid performanceCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationPetrieGAYesBreakoutNoNo
161Effect of seed selection, ROSP, and magnetic balance on successful radiating divertor operationCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationPetrieGAYesBreakoutNoNo
162Is krypton better than argon as a mantle seed in high power, high performance hybrid plasmas?Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationPetrieGAYesBreakoutNoNo
163Two-impurity approach as an optimal radiating divertor solution for DIII-DCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationPetrieGAYesBreakoutNoNo
164Effect of reversing the grad-B drift on high betaN plasmas under radiating divertor conditionsCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationPetrieGAYesBreakoutNoNo
272High Density Electron Heating With O-ModeCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationPettyGANoBreakoutNoYes
269Pushing Steady-State Hybrid Scenario to Lower q95, Higher Beta and Higher Fusion GainCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationPettyGANoBreakoutNoNo
176Reversing the direction of the impurity pinch at ITER-relevant edge conditionsCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationNelsonColumbia UYesBreakoutNoNo
154How does divertor drift affect upstream profiles?Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationWangGAYesBreakoutNoNo
224Integrate a divertor solution in the T=0 IBSCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationTurcoColumbia UYesBreakoutNoNo
89Sustainment of high Super H core confinementCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationKnolkerGAYesBreakoutNoNo
2testing, please ignore!Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationCovielloGANoBreakoutNoNo
175Make DIII-D a W or no W machineCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationTurcoColumbia UYesBreakoutNoNo
254Compatibility of QH-mode with Radiative DivertprCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationWilksMITYesBreakoutNoNo
284ELM-phase dependence on transport for different experimental conditionsCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationIzacardPrinceton UYesBreakoutNoNo
321Further PCS Development on q-profile Control and NTM SuppressionControlPajaresLehigh UYesBreakoutNoNo
322Integrated Control of Individual ScalarsControlPajaresLehigh UYesBreakoutNoNo
325Profile control for high qmin steady state scenarioControlWehnerLehighNoBreakoutNoNo
326Model-based rotation control developmentControlWehnerLehighNoBreakoutNoNo
458m/n=2/1 NTM control by ECCD in steady state hybridControlBardocziGANoBreakoutNoNo
346Developing low-disruptivity ramp-down techniques for the ITER Baseline ScenarioControlBarrGANoBreakoutNoNo
419Commissioning of a proximity-to-stability-boundary control architecture for disruption preventionControlBarrGANoBreakoutNoNo
420Commissioning of a Vertical Control proximity-to-stability-boundary algorithm for VDE preventionControlBarrGANoBreakoutNoNo
218The Disruption Free ProtocolControlBarrGAYesBreakoutNoNo
288Exploration of IBS variation with direct gain metric regulationControlOlofssonConsultantNoBreakoutNoNo
289Shape control enabled study of IBS stability as function of edge featuresControlOlofssonConsultantNoBreakoutNoNo
293Divertor detachment control based on Langmuir Probes measurementControlWangGAYesBreakoutNoNo
24Tuning of Controller/Observer Gains for n=1 and n=2 Resistive Wall Mode ControlControlBatteyColumbia UYesBreakoutNoNo
314Voltage controlled SuperSpas for plasma shape controlControlHyattGANoBreakoutNoNo
315VFI-less Plasma operationsControlHyattGANoBreakoutNoNo
44Real time measurements of impurity densityControlChrystalGANoBreakoutNoNo
403Burn Condition Emulation for ITER-relevant Control ExperimentsControlSchusterLehigh UNoBreakoutNoNo
347ITER plasma initiation and ECH assistControlWalkerGANoBreakoutYesYes
342Vertical stability control with simulated horizontal interferometer channelsControlEldonGANoBreakoutNoNo
275Divertor radiated power control in non-ELMing plasmasControlEldonGANoBreakoutNoNo
339Detachment control w/ Te request translated to ne estimate & direct ne feedbackControlEldonGANoBreakoutNoNo
506PCS supervisory algorithm for negotiating complex controller requestsControlEidietisGANoBreakoutNoNo
201m/n=2/1 NTM control by ECCD in IBSControlBardocziGANoBreakoutNoNo
429Real time neutron controlControlHeidbrinkUC, IrvineNoBreakoutNoNo
511Feedback control for divertor impurity seeding based on Surface Eroding ThermocoupleControlRenU of Tennessee, KnoxvilleNoBreakoutNoNo
351Machine Learning based Instability Prediction & AvoidanceControlKolemenPPPLYesBreakoutNoNo
521ECCD and ECH for IBS with real-time modulation controlControlKolemenPPPLNoBreakoutNoNo
522RT stability analysis to find/avoid the instabilities with mhd calc. and feedback 3D spectroscopyControlKolemenPPPLNoBreakoutNoNo
523Test the new method for finding the 3D perturbation needed to avoid tearingControlKolemenPPPLNoBreakoutNoNo
524Control of pressure/current profile transport models experimentallyControlKolemenPPPLNoBreakoutNoNo
338Combining variable beam energy/perveance and NTV for rotation controlControlBoyerPPPLNoBreakoutNoNo
323Tune RMP Controlled Phase of Locked Island and Radial Alignment of ECCD Deposition for StabilizationControlReimanPPPLNoBreakoutNoNo
210Puff and Pump Flow measurement in DN as a function of drsepAdvanced Magnetic ConfigurationsAllenLLNLNoBreakoutNoNo
82Clarify key snowflake divertor physicsAdvanced Magnetic ConfigurationsSoukhanovskiiLLNLNoBreakoutNoNo
83Particle exhaust in snowflake divertorAdvanced Magnetic ConfigurationsSoukhanovskiiLLNLNoBreakoutNoNo
329Magnetic geometry as an actuator for detachment stability and controlAdvanced Magnetic ConfigurationsSamuellLLNLYesBreakoutNoNo
495SAS, meet DNAdvanced Magnetic ConfigurationsThomasGAYesBreakoutNoNo
332Detachment at horizontal and vertical targetsAdvanced Magnetic ConfigurationsWangGAYesBreakoutNoNo
84Clarify snowflake divertor physicsAdvanced Magnetic ConfigurationsSoukhanovskiiLLNLNoBreakoutNoNo
184Use NBI to evaluate n=2 RMP penetration position3DSPWANGASIPPYesYesYes
60Measure and control resistive kink mode stability3DSPHansonColumbia UYesBreakoutNoNo
311Proximity of tearing mode onset to ideal limits in high-beta plasmas3DSPTurcoColumbia UYesBreakoutNoNo
58Assess robustness of ITER baseline plasma response control3DSPHansonColumbia UYesBreakoutNoNo
457m/n=2/1 NTM control by ECCD in steady state hybrid3DSPBardocziGANoBreakoutNoNo
192m/n=2/1 NTM control by ECCD in IBS3DSPBardocziGANoBreakoutNoNo
190Impact of Current Condensation in the ECCD Stabilization of Rotating 2/1 NTMs3DSPBardocziGANoBreakoutNoNo
459Use pellets to lower the ECCD requirement for 2/1 NTM stabilization3DSPBardocziGANoBreakoutNoNo
477Optimizing NTV torque profiles with multi-modal 3D control3DSPWeisbergGAYesBreakoutNoNo
178Use NBI to evaluate n=2 RMP penetration position3DSPWANGASIPPYesBreakoutYesYes
62Disruption Avoidance via ECCD Stabilization of Locked Islands and the Impact of Current Condensation3DSPReimanPPPLYesBreakoutNoNo
199Machine Learning based Instability Prediction & Avoidance3DSPKolemenPPPLNoBreakoutNoNo
205RT stability analysis to find/avoid the instabilities with mhd calc. and feedback 3D spectroscopy3DSPKolemenPPPLNoBreakoutNoNo
206ECCD and ECH for IBS with real-time modulation control3DSPKolemenPPPLNoBreakoutNoNo
492Understanding outliers of ITER error field correction criteria3DSPParkPPPLYesBreakoutYesYes
197Test the new method for finding the 3D perturbation needed to avoid tearing3DSPKolemenPPPLYesBreakoutNoNo
451Combine the MM MHD spectroscopy, ML, RT DCON to control q95 and beta and modify the modes stability3DSPMunarettoPPPLYesBreakoutNoNo
516Role of Quasi-symmetric Magnetic Perturbations on LH-transition and pedestal transport3DSPZarnstorffPrinceton UYesBreakoutNoNo
132Disruption Prediction via Random Forests v2.0 and Interpretability3DSPReaMassachusetts Institute of TechnologyYesBreakoutNoNo
185Exploring the role of nonlinear MHD in triggering tearing modes3DSPChapmanU of WisconsinYesBreakoutNoNo
186Exploring the role of fluctuation-based dynamos in magnetic flux pumping3DSPChapmanU of WisconsinYesBreakoutNoNo