DIII-D RESEARCH OPPORTUNITIES FORUM FOR THE 2017 EXPERIMENTAL CAMPAIGN

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ID Title Research Area Name Affiliation Time
Req'ed
ITPA
Joint Exp
ITER IO Urgent
Research Task
1Welcome to 2017 DIII-D ROFGeneral PhysicsFenstermacherLLNLNoNoNo
3Current control VALEN based RWM feedback developmentD&C - control (apart from core stability in low torque ITER thrust)ClementPPPLNoNoNo
5Transformative Torque-less ITER similarity discharges in DIII-D with the present gyrotron set.Control and Understand Core Stability in low Torque ITER BaselinedeGrassieGANoNoNo
6ECCD and Core Intrinsic RotationDevelop Basis to Predict and Control Rotation in ITERdeGrassieGANoNoNo
7Model-Predictive Control of Magnetic/Kinetic Profiles using fast data-driven models and observersD&C - control (apart from core stability in low torque ITER thrust)MoreauCadaracheNoNoNo
8ITER Baseline ELM Suppression at Low TorqueD&C - inductive (apart from core stability in low torque ITER thrust)LuceITER OrganizationNoNoYes
9Probing stiffness with constant Ti/TeBPP - turbulence and transportLuceITER OrganizationNoNoNo
10Comparison Plasmas in Deuterium to Helium Campaign PlasmasPE - Pedestal/SOL physics and Pedestal optimizationLuceITER OrganizationNoYesYes
11Operation and performance at low P/P_LH in the ITER baseline scenarioD&C - inductive (apart from core stability in low torque ITER thrust)LuceITER OrganizationNoYesNo
12Complete q95 optimization experimentD&C - inductive (apart from core stability in low torque ITER thrust)LuceITER OrganizationNoNoNo
13Effect of closure location relative to x pointUnderstand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL DynamicsLuceITER OrganizationNoNoNo
14Characterization of the quasi-coherent fluctuations between ELMsPE - Pedestal/SOL physics and Pedestal optimizationDialloPPPLNoNoNo
16Use variable NBI voltage in high qmin scenarios to reduce AE/EPM-induced EP transportD&C - steady state (apart from core-edge SS thrust)HolcombLLNLNoNoNo
17Scaling of intrinsic rotation in ECH H-modeDevelop Basis to Predict and Control Rotation in ITERChrystalGANoNoNo
18Charge Exchange Cross Section Study with Co/counter beamsGeneral PhysicsChrystalGANoNoNo
20Quiescent runaway electron studies with refurbished gamma-ray-imaging detectorsDisruption Mitigation PhysicsPaz-SoldanColumbia UNoYesNo
21Revisit rotating n=2 fields at higher amplitude for 3D structure diagnosis during ELM suppressionUnderstand Limits and Means to Extend ELM suppression for futurePaz-SoldanColumbia UNoNoNo
22Effect of shaping on pedestal and 3D response for ELM control: aspect ratio, triangularity, X-pointUnderstand Limits and Means to Extend ELM suppression for futurePaz-SoldanColumbia UNoNoNo
23High current phase flips during rotation scans in RMP-ELM suppression in ITER baselineUnderstand Limits and Means to Extend ELM suppression for futurePaz-SoldanColumbia UNoNoNo
24Apply n=1,2,3 error field control to low torque IBS plasmaControl and Understand Core Stability in low Torque ITER BaselinePaz-SoldanColumbia UNoNoNo
25Create different yet non-dimensionally similar low torque ITER baseline plasmasControl and Understand Core Stability in low Torque ITER BaselinePaz-SoldanColumbia UNoNoNo
26Non-resonant braking for tearing mode onset studiesControl and Understand Core Stability in low Torque ITER BaselinePaz-SoldanColumbia UNoNoNo
27Effect of Fast Ion Loss on L-H TransitionBPP - L-H transitiondeGrassieGANoNoNo
29Runaway plateau impurity assimilationDisruption Mitigation PhysicsHollmannUCSDNoNoYes
30Vary runaway electron plateau wall strike phaseDisruption Mitigation PhysicsHollmannUCSDNoNoNo
31Negative Triangularity LSN ScenarioIntegrated Core-Edge Steady State SolutiondeGrassieGANoNoNo
32Asymmetry effects during SPI fast shutdownDisruption Mitigation PhysicsShirakiORNLNoNoNo
33Multiple shattered pellet injections for TQ/CQ mitigationDisruption Mitigation PhysicsShirakiORNLNoNoNo
34Ballistic transport and MHD mixing in SPI impurity assimilationDisruption Mitigation PhysicsShirakiORNLNoNoNo
35Learn how to produce qmin>2 with only positive shear for minimal impact of AEsD&C - steady state (apart from core-edge SS thrust)HolcombLLNLNoNoNo
36Alternative injection schemes for high-Z shattered pellets for dissipation of runaway electronsDisruption Mitigation PhysicsShirakiORNLNoNoNo
37Pellet ablation as a diagnostic for quiescent runaway electron growthDisruption Mitigation PhysicsShirakiORNLNoNoNo
38Learn how to produce qmin>2 with large rhoqmin for minimal impact of AEs using dynamic ECH and VNBID&C - steady state (apart from core-edge SS thrust)HolcombLLNLNoNoNo
42Role of EP transport in rotation of tearing-unstable plasmasBPP - Energetic Particle PhysicsTobiasLos Alamos National LaboratoryNoNoNo
51Identify physics mechanisms responsible for MHD-induced collapse of toroidal momentumDevelop Basis to Predict and Control Rotation in ITERTobiasLos Alamos National LaboratoryNoNoNo
52Recovery of favorable rotation profiles after MHD-induced rotation collapseDevelop Basis to Predict and Control Rotation in ITERTobiasLos Alamos National LaboratoryNoNoNo
533D pedestal turbulence studies during ELM suppression with rotating n=2 I-coilsUnderstand Limits and Means to Extend ELM suppression for futureWilcoxORNLNoNoNo
56Divertor turbulence and detachmentAddress Critical Detachment Physics ModelsBoedoUCSDNoNoNo
61Long pulse, high pedestal pressure, ELM free discharges with Li injectionScenarios and TransportOsborneGANoNoNo
62Gather evidence for Kinetic effects in SOL and DivertorDO: Divertor optimizationBoedoUCSDNoNoNo
63Intrinsic rotation scaling with collisionality, ion temperature and geometryDevelop Basis to Predict and Control Rotation in ITERBoedoUCSDNoNoNo
67RT control of H-L transition by sudden shape changeD&C - control (apart from core stability in low torque ITER thrust)EldonGANoNoNo
70Optimized lower torque hybridsD&C - steady state (apart from core-edge SS thrust)TurcoColumbia UNoNoNo
71Study and eliminate fishbones, high frequency modes and ELMs in high betaN hybridsIntegrated Core-Edge Steady State SolutionTurcoColumbia UNoNoNo
74Role of divertor geometry on confinementUnderstand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL DynamicsMordijckThe college of William and MaryNoNoNo
76Return of ELMs during RMP and low torque operationUnderstand Limits and Means to Extend ELM suppression for futureRhodesUCLANoNoNo
77Is the Coriolis Pinch the Key to Intrinsic RotationDevelop Basis to Predict and Control Rotation in ITERdeGrassieGANoNoNo
78High opacity SOL effect on pedestalUnderstand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL DynamicsMordijckThe college of William and MaryNoYesYes
80ExB and parallel flows in attached and detached divertorAddress Critical Detachment Physics ModelsBoedoUCSDNoNoNo
81Test intrinsic flow theories and edge turbulence characteristics of negtative triangularity plasmasBPP - turbulence and transportBoedoUCSDNoNoNo
83Turbulence link between detaching divertor and pedestal characteristicsUnderstand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL DynamicsBoedoUCSDNoNoNo
85Effect of the post-TQ density on runaway beam mitigation with MGI and SPIDisruption Mitigation PhysicsFilPPPLNoNoNo
86ECCD-induced magnetic islands and impact on plasma rotationControl and Understand Core Stability in low Torque ITER BaselineFilPPPLNoNoNo
87Preemptive EMTI Feedback for NTM Locking Avoidance and Recovery of H-mode edge and High ConfinementControl and Understand Core Stability in low Torque ITER BaselineOkabayashiPPPLNoNoNo
88Pre-emptive EMTI feedback-based Multi-mode (3/2 &2/1) Coupling De-phasing and Disruption AvoidanceControl and Understand Core Stability in low Torque ITER BaselineOkabayashiPPPLNoNoNo
101Understand role of plasma shape on ELM suppressionUnderstand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL DynamicsSchmitzU of WisconsinNoNoNo
103Understand detachment access during RMP ELM suppressionUnderstand Limits and Means to Extend ELM suppression for futureSchmitzU of WisconsinNoNoNo
105Developing new RMP physics insights based on rotating n=3 perturbation fieldsPE - RMP and pellets (non ELM suppression thrust)EvansGANoYesYes
106Fast-ion transport by NTMsBPP - Energetic Particle PhysicsHeidbrinkUC, IrvineNoNoNo
107Test radial electric field formation from ion lossDevelop Basis to Predict and Control Rotation in ITERBoedoUCSDNoNoNo
108Fast-ion transport by NTMs in hybrid plasmasIntegrated Core-Edge Steady State SolutionHeidbrinkUC, IrvineNoNoNo
109Control of edge pedestal to extend duration and performance of high betaP scenarioScenarios and TransportQianASIPPNoNoNo
110Feedback control of 2/1 locked mode phase and rotation with RMPControl and Understand Core Stability in low Torque ITER BaselineChoiGANoNoNo
111Understand and reduce fishbone activity in hybrid plasmasIntegrated Core-Edge Steady State SolutionThomeGANoNoNo
112Test Dependence of Core Confinement on the RMP Amplitude in ELM Suppressed PlasmasBPP - turbulence and transportCuiPPPLNoNoNo
115Stationary RF-dominantly heated hybrid plasmas at low torqueD&C - inductive (apart from core stability in low torque ITER thrust)ThomeGANoNoNo
116Low torque high Beta hybrid plasmasIntegrated Core-Edge Steady State SolutionThomeGANoNoNo
117Pedestal optimization of hybrid plasmasIntegrated Core-Edge Steady State SolutionThomeGANoNoNo
125Wider negative shear for the confinement improvement at high Te/TiBPP - turbulence and transportYoshidaQSTNoNoNo
127Advanced Divertor Control DevelopmentD&C - control (apart from core stability in low torque ITER thrust)VailPrinceton UNoNoNo
129Upper and Double-Null Snowflake DevelopmentD&C - control (apart from core stability in low torque ITER thrust)VailPrinceton UNoNoNo
130Advanced Divertor Detachment StudiesUnderstand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL DynamicsVailPrinceton UNoNoNo
131Effect of Advanced Divertor Magnetic Geometry on Ideal MHD Stability LimitsUnderstand Limits and Means to Extend ELM suppression for futureVailPrinceton UNoNoNo
146Effect of closed divertor on pedestal formation and divertor detachmentUnderstand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL DynamicsMoserGANoNoNo
147Measure sheath power transmission factor in sas diverterUnderstand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL DynamicsWatkinsSandia National LabNoNoNo
148Study the role of magnetic and ñ fluctuations in saturating pedestal gradients during type-I ELMsPE - Pedestal/SOL physics and Pedestal optimizationKumar BaradaUCLANoNoNo
152Quantifying detachment advantage in SAS relative to open divertorUnderstand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL DynamicsMoserGANoNoNo
155Enhanced pedestal H-mode through low-Z impurity injectionPE - Pedestal/SOL physics and Pedestal optimizationBortolonPPPLNoNoNo
156Pedestal optimization in stationary plasmasPE - Pedestal/SOL physics and Pedestal optimizationSnyderORNLNoNoNo
158Development of ECH TS-ECE Cross-CalGeneral PhysicsBrookmanGANoNoNo
159Loss of Effective Heat Flux Reduction by Puff-and-Pump Under High Power AT ConditionsUnderstand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL DynamicsPetrieGANoNoNo
160ITER Baseline Scenario in a Radiating Divertor Environment with near-Zero Applied TorqueControl and Understand Core Stability in low Torque ITER BaselinePetrieGANoNoNo
161Finish exploring the higher q95 IBS alternative, with RMP ELM suppressionControl and Understand Core Stability in low Torque ITER BaselineTurcoColumbia UNoNoNo
162Density Control and Active Middle-Z Impurity Removal from Double-null H-mode PlasmasIntegrated Core-Edge Steady State SolutionPetrieGANoNoNo
163obtain minimum core density with detached sas divertorUnderstand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL DynamicsWatkinsSandia National LabNoNoNo
164Differentiate L-mode turbulence regimes preceding the L-H transitionBPP - L-H transitionSchmitzUCLANoNoNo
165Pedestal detachment with n = 4 and 6 RMP fieldsTorkil Jensen AwardEvansGANoNoNo
168H-mode detachment data in deuterium plasma to compliment existing helium detachment dataAddress Critical Detachment Physics ModelsBriesemeisterORNLNoNoNo
169Feedback control of 2/1 locked mode phase and rotation with RMPControl and Understand Core Stability in low Torque ITER BaselineChoiColumbia UNoNoNo
173Effect of intrinsic and applied MP on error field tolerance in low torque high beta plasmasControl and StabilityWangASIPPNoNoNo
174Mixed spectrum of n=2 and 3 RMP for ELM suppressionBoundarySunASIPPNoNoNo
175Rotating n=2 RMP for ELM suppressionBoundarySunASIPPNoNoNo
179ELM suppression in AUG-line shape with n=2Understand Limits and Means to Extend ELM suppression for futureKirkCCFENoYesNo
181Demonstration of Divertor SPREDAddress Critical Detachment Physics ModelsMcLeanLLNLNoNoNo
183Transport and ELM suppression associated with the EHO in QH-modePE - QH mode (non ELM suppression thrust)WilksMassachusetts Institute of TechnologyNoNoNo
184Characterization of the radial electric field through ion orbit lossPE - Pedestal/SOL physics and Pedestal optimizationWilksMassachusetts Institute of TechnologyNoNoNo
186Electron Critical Gradient in H-modeBPP - turbulence and transportPettyGANoNoNo
187Systematic detachment characterization in high triangularity, high performance plasmasAddress Critical Detachment Physics ModelsMcLeanLLNLNoNoNo
188Test of Turbulence Spreading Using Turbulence PropagationBPP - turbulence and transportPettyGANoNoNo
190Probing the 2D flow evolution during the L/H transitionBPP - L-H transitionStaeblerGANoNoNo
191Hybrids with co-NBI QH-mode edgeIntegrated Core-Edge Steady State SolutionPettyGANoNoNo
192Effect of electron perpendicular flow variation for ELM suppression at reduced triangularityUnderstand Limits and Means to Extend ELM suppression for futureSuttropMax-Planck Institute for Plasma PhysicsNoYesNo
193Probing X-point and inboard SOL plasma for fluctuationsAddress Critical Detachment Physics ModelsMcLeanLLNLNoNoNo
195Increase beta in ALfven Eigenmode mitigated high performance target dischargesD&C - steady state (apart from core-edge SS thrust)KramerPPPLNoNoNo
197Control rotation via geometryDevelop Basis to Predict and Control Rotation in ITERBoedoUCSDNoNoNo
198Test unconstrained models of L-H transitionBPP - L-H transitionBoedoUCSDNoNoNo
199multi-scale turbuelnce validationScenarios and TransportStaeblerGANoNoNo
200Scaling of NTV Torque with Applied 3D Field Amplitude and SpectrumDevelop Basis to Predict and Control Rotation in ITERGriersonGANoNoNo
201DiMES tests of novel Mo PMI materialsAMV: Erosion/migrationThomasGANoNoNo
202Effect of divertor geometry, closure, and SOL plasma on fueling and impurity effects on pedestalUnderstand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL DynamicsOsborneGANoYesNo
207Clarify snowflake divertor physicsDO: Divertor optimizationSoukhanovskiiLLNLNoNoNo
208Snowflake SAS divertorUnderstand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL DynamicsSoukhanovskiiLLNLNoNoNo
209Study effects of SOL flows on QH-mode accessUnderstand Limits and Means to Extend ELM suppression for futureKingTech-X CorporationNoNoNo
210Improving impurity injection into RE by avoiding high energy shfited RE orbitsDisruption Mitigation PhysicsEidietisGANoNoNo
211Effect of global MHD stability on RE plateau dissipation in D3D & JETDisruption Mitigation PhysicsEidietisGANoNoYes
212AE critical gradient study with different modulated beamsBPP - Energetic Particle PhysicsHeidbrinkUC, IrvineNoNoNo
213ICE produced by beam ions in the scrapeoff layerBPP - Energetic Particle PhysicsHeidbrinkUC, IrvineNoYesNo
214Pellet ELM triggering as a function of injection locationPE - RMP and pellets (non ELM suppression thrust)BaylorORNLNoNoNo
215Experimental test of two-threshold-field theory of RE generationDisruption Mitigation PhysicsLvovskiyORAUNoNoNo
216HFS pellet fueling compatibility with ELM mitigation scenarios and particle transportPE - RMP and pellets (non ELM suppression thrust)BaylorORNLNoNoNo
217Develop a no-ECH high betaN hybrid for radiative divertor studiesIntegrated Core-Edge Steady State SolutionTurcoColumbia UNoNoNo
220AEs in Negative Triangularity PlasmasBPP - Energetic Particle PhysicsVan ZeelandGANoNoNo
222AE Drive Due to Ions Lost on Their First OrbitBPP - Energetic Particle PhysicsVan ZeelandGANoNoNo
223AEs in Negative Triangularity PlasmasBPP - Energetic Particle PhysicsVan ZeelandGANoNoNo
226Does microturbulence control mode chirping?BPP - Energetic Particle PhysicsHeidbrinkUC, IrvineNoYesNo
227Use resonances with 3D fields to alter the distribution functionBPP - Energetic Particle PhysicsHeidbrinkUC, IrvineNoNoNo
228Establishing an experimental cyclone base case scenario for the LH transitionBPP - L-H transitionMarinoniUCSDNoNoNo
233Joint SPI experiment with JETDisruption Mitigation PhysicsGreenfieldORNLNoNoYes
235Does the P-B model accurately predict the collisionality scaling of ELM mode number (k_theta)?Understand Limits and Means to Extend ELM suppression for futureTobiasLos Alamos National LaboratoryNoNoNo
236Does nonlinear impact of ExB shear dictate the radial extent of ELMs and prevalence of filaments?Understand Limits and Means to Extend ELM suppression for futureTobiasLos Alamos National LaboratoryNoNoNo
237D+ fueling due to cold neutral D in the pedestal at the outboard midplane using main ion CERUnderstand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL DynamicsHaskeyPPPLNoNoNo
239Intrinsic torque in ECH dominated plasma --- do we find counter-current intrinsic torqueDevelop Basis to Predict and Control Rotation in ITERTalaVTT Technical Research CentreNoYesNo
241Fuel Ion Mass Scaling of TransportBPP - turbulence and transportMcKeeU of WisconsinNoNoNo
244Suppression of plasma current after plasma initializationD&C - control (apart from core stability in low torque ITER thrust)WalkerGANoNoYes
245Inward particle transport of HFS pellet fueled plasmasBPP - turbulence and transportBaylorORNLNoNoYes
246Develop low q95 post-disruption runaway electron scenarioDisruption Mitigation PhysicsPaz-SoldanColumbia UNoYesNo
248Prompt conversion of a full current into sub-MeV RE currentDisruption Mitigation PhysicsAleynikovMax-Planck Institute for Plasma PhysicsNoYesNo
250Modeling of the effect of detachment on heat flux width using SOLPS-ITER with driftsDO: Divertor optimizationMeierZap Energy Inc.NoNoNo
251Joint KSTAR/DIII-D n=2 Transport and Stability ExperimentUnderstand Limits and Means to Extend ELM suppression for futureEvansGANoNoNo
252Experimental NTV torque profiles in 3D fieldsDevelop Basis to Predict and Control Rotation in ITERSalmiVTT Technical Research CentreNoNoNo
253Control of toroidal rotation with NBI and NTV optimizationDevelop Basis to Predict and Control Rotation in ITERFilPPPLNoNoNo
254Control of toroidal rotation with NBI and NTV optimizationD&C - control (apart from core stability in low torque ITER thrust)FilPPPLNoNoNo
255Continuous high pressure pedestal with LithiumPE - Pedestal/SOL physics and Pedestal optimizationFilPPPLNoNoNo
256Detachment Control with Nitrogen (or Carbon)Address Critical Detachment Physics ModelsKolemenPPPLNoNoNo
257Density dependence of edge intrinsic rotation in USN L-mode.Develop Basis to Predict and Control Rotation in ITERAshourvanGANoNoNo
258Collisionality dependence of the edge differential toroidal rotation between carbon and deuteriumDevelop Basis to Predict and Control Rotation in ITERHaskeyPPPLNoNoNo
259Midplane Impurity Density AsymmetryBPP - turbulence and transportChrystalGANoNoNo
262Testing the effect of multi-scale fluctuations on steady-state profiles in IBS scenariosBPP - turbulence and transportMarinoniUCSDNoNoNo
264Unique Code Validation through Comparison of High and Low-field-side Turbulence MeasurementsBPP - turbulence and transportSungKAISTNoNoNo
265Increase the stability limits of high-betaN hybrids by optimising the plasma shapeIntegrated Core-Edge Steady State SolutionTurcoColumbia UNoNoNo
267Mixed spectrum of n=2 and 3 RMP for ELM suppressionUnderstand Limits and Means to Extend ELM suppression for futureSunASIPPNoNoNo
268Rotating n=2 RMP for ELM suppressionUnderstand Limits and Means to Extend ELM suppression for futureSunASIPPNoNoNo
272D3D/JET comparison of pure Ne SPI size scalingDisruption Mitigation PhysicsEidietisGANoNoYes
277Comparison of hybrids with open and closed divertorIntegrated Core-Edge Steady State SolutionThomeGANoNoNo
278Wall deposition of refracted ECH powerBPP - Heating & Current Drive PhysicseChenGANoNoNo
279Negative Triangularity LSN ScenarioTorkil Jensen AwarddeGrassieGANoNoNo
280Placeholder: Dedicated camrea time to get SPI solid fraction estimateDisruption Mitigation PhysicsEidietisGANoNoNo
281Develop counter-rotating analog to co-rotating ITER baseline plasma for stability studyControl and Understand Core Stability in low Torque ITER BaselinePaz-SoldanColumbia UNoNoNo
282Placeholder: Spatially resolved measurement of RE pleateau f(E) with GRIDisruption Mitigation PhysicsEidietisGANoNoNo
285NTM Stabilization for IBSControl and Understand Core Stability in low Torque ITER BaselineKolemenPPPLNoYesYes
286Off-Axis ECCD in Steady-State HybridsIntegrated Core-Edge Steady State SolutionPettyGANoNoNo
287Plasma Response in DN versus SNUnderstand Limits and Means to Extend ELM suppression for futureTurnbullGANoNoNo
288All Carbon Plasma Density MeasurementPE - RMP and pellets (non ELM suppression thrust)ChrystalGANoNoNo
289High-Performance, Steady-State Scenario Development Using Sustained, Broad Negative Shear q-ProfilesD&C - steady state (apart from core-edge SS thrust)MurakamiRetiredNoNoNo
290Improve radial control during rampupD&C - control (apart from core stability in low torque ITER thrust)EidietisGANoNoNo
291Default ONFR on all D3D shotsD&C - control (apart from core stability in low torque ITER thrust)EidietisGANoNoNo
292Plasma Control with SuperSpasD&C - control (apart from core stability in low torque ITER thrust)HyattGANoNoNo
293Test of pedestal current role in low torque ITER baseline plasmasControl and Understand Core Stability in low Torque ITER BaselineLuceITER OrganizationNoYesNo
294Development of ITER-relevant rampdown scenariosD&C - control (apart from core stability in low torque ITER thrust)LuceITER OrganizationNoYesNo
295Control EP transport in high qmin steady-state plasmas using central ECHIntegrated Core-Edge Steady State SolutionChenGANoYesNo
296Establishing H-mode at negative triangularityTorkil Jensen AwardMarinoniUCSDNoNoNo
297Understanding I-mode access and I-mode physics through identity experiments DIII-D / ASDEX UpgradePE - Pedestal/SOL physics and Pedestal optimizationHappelMax-Planck-Institut für PlasmaphysikNoYesNo
298Do Surface Patterns on the Tiles Matter?AMV: Erosion/migrationLasa EsquisabelU of Tennessee, KnoxvilleNoNoNo
300Studies of Arcing on Tungsten and Molybdenum PFC SurfacesAMV: Erosion/migrationRudakovUCSDNoNoNo
301Develop MIMO algorithm for detachment and radiation profile controlD&C - control (apart from core stability in low torque ITER thrust)VailPrinceton UNoNoNo
302Characterization of detachment with MIMO detachment and radiation profile controlDO: Detachment & control (apart from Detachment Physics Thrust)VailPrinceton UNoNoNo
303Adaptive EFCD&C - control (apart from core stability in low torque ITER thrust)VailPrinceton UNoNoNo
304Adaptive Error Field CorrectionControl and Understand Core Stability in low Torque ITER BaselineVailPrinceton UNoNoNo
305Adaptive ELM ControlD&C - control (apart from core stability in low torque ITER thrust)VailPrinceton UNoNoNo
306Adaptive ELM ControlUnderstand Limits and Means to Extend ELM suppression for futureVailPrinceton UNoNoNo
307Optimization of n=1 RMP fields for ELM suppressionUnderstand Limits and Means to Extend ELM suppression for futureParkPPPLNoNoNo
308Collisionality scan for the minimum ExB shear to sustain EHO and avoid ELMsPE - QH mode (non ELM suppression thrust)ChenGANoNoYes
309Investigation of broadband EHO and the â??wide-pedestal QHâ?? broadband MHDPE - QH mode (non ELM suppression thrust)ChenGANoNoNo
310H-mode impurity transport dependence on beam fuelingBPP - turbulence and transportThomeGANoNoYes
311Runaway mitigation with solid pelletsDisruption Mitigation PhysicsLehnenITER OrganizationNoYesYes
312SPI with varying target plasma parametersDisruption Mitigation PhysicsLehnenITER OrganizationNoNoYes
313Collisionality scan for the minimum ExB shear to sustain EHO and avoid ELMsUnderstand Limits and Means to Extend ELM suppression for futureChenGANoNoYes
314Improved core confinement of high performance steady state plasmas due to ITG turbulence dilutionIntegrated Core-Edge Steady State SolutionMarinoniUCSDNoNoNo
315Measurements of intrinsic torque using main ion rotation measurementsDevelop Basis to Predict and Control Rotation in ITERHaskeyPPPLNoNoNo
318Advanced Inductive with QH Mode Edge For Path to Q=10D&C - inductive (apart from core stability in low torque ITER thrust)ButteryGANoYesYes
319Skin Current Tokamak at higher CurrentScenarios and TransportStaeblerGANoNoNo
320Effect on SEE on Langmuir probe measurements in the SOLPE - Pedestal/SOL physics and Pedestal optimizationRudakovUCSDNoNoNo
321Greenwald limit: is radiative island the cause?Torkil Jensen AwardKolemenPPPLNoNoNo
322Dust re-mobilization studies using DiMESAMV: Erosion/migrationRudakovUCSDNoNoNo
323Response of turbulence in magnetic island due to the heat pulse from modulation ECHBPP - turbulence and transportIdaNational Institute for Fusion Science, JapanNoNoNo
324Detachment control for SASD&C - control (apart from core stability in low torque ITER thrust)EldonGANoNoNo
325Combined detachment and divertor radiation controlD&C - control (apart from core stability in low torque ITER thrust)EldonGANoNoNo
328Interpretation of WII and WI emission profiles in terms of a W prompt re-deposition fractionAMV: Erosion/migrationAbramsGANoNoNo
329Use of thin poloidal gaps to inhibit surface migration of PFC materialAMV: Erosion/migrationStangebyU of TorontoNoNoNo
330Control of high-Z material erosion by biasing in H mode plasmaAMV: Erosion/migrationDingASIPPNoNoNo
331Use of isotopic tracer elements to understand material migration propertiesAMV: Erosion/migrationUnterbergORNLNoNoNo
332Detachment with varying leg length with re-directed DTS laserAddress Critical Detachment Physics ModelsCanikORNLNoNoNo
333Detachment physics at maximum heat fluxAddress Critical Detachment Physics ModelsCanikORNLNoNoNo
334Use deposition on 3D material structures to understand material migration on the divertor targetAMV: 3D effectsHinsonORNLNoNoNo
335Deposition Probe Background and Pellet Injection ExposuresAMV: Erosion/migrationDonovanU of Tennessee-KnoxvilleNoNoNo
336Test of improved 2/1 stability with reduced pedestal heightControl and Understand Core Stability in low Torque ITER BaselinePettyGANoNoNo
337Detachment control in X-divertorD&C - control (apart from core stability in low torque ITER thrust)EldonGANoNoNo