DIII-D RESEARCH OPPORTUNITIES FORUM FOR THE 2018 EXPERIMENTAL CAMPAIGN

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ID Title Research Area Name Affiliation Time
Req'ed
ITPA
Joint Exp
ITER IO Urgent
Research Task
340Improved stability of counter rotating plasmasThrust 4 - Rotation PhysicsVictorLLNLYesNoNo
349In-situ formation of Si-C coatings on DiMESAMV - Surface Evolution ScienceRudakovUCSDYesNoNo
351Development of the low-torque wide-pedestal QH-mode with EHOThrust 3 - ELM ControlChenGAYesNoNo
355Rotating n=2 fields with edge ECCD to reduce ELM suppression threshold amplitudeThrust 3 - ELM ControlWilcoxORNLYesNoNo
356Spectroscopic analysis of SiC preferential sputteringAMV - Material Migration and MitigationAbramsGAYesNoNo
357ELM-resolved measurements of high-Z re-deposition fractionsAMV - Material Migration and MitigationAbramsGAYesNoNo
3583D boundary effects on heavy impurity removalCore-Edge Integration Task ForceHinsonORNLYesNoNo
366Using up/down asymmetry to Increase the intrinsic rotationThrust 4 - Rotation PhysicsVictorLLNLYesNoNo
367ELM studies close to LH boundaryPE - Pedestal/SOL Physics and Pedestal OptimizationKnolkerGAYesYesNo
368Get Advance Inductive QH Mode to Zero TorqueThrust 1 - ITER Q=10 (Inductive Scenarios)ButteryGAYesNoNo
369Role of micro-turbulence in intrinsic rotation reversals through JET DIII-D similarity experimentsThrust 4 - Rotation PhysicsNaveInstituto Superior Tecnico, Lisboa, PortugalYesNoNo
370Control of the inter-ELM pedestal fluctuationsPE - Pedestal/SOL Physics and Pedestal OptimizationLaggnerPrinceton UniverstiyYesNoNo
372Radiation saturation at reduced Ne quantity by order of magnitude increase in D2 inventoryD&C - Disruption Mitigation PhysicsSweeneyMassachusetts Institute of TechnologyYesNoYes
374Aspect ratio scaling of tearing stabilityD&C - 3D and Stability PhysicsMortonU of WisconsinYesNoNo
375Advanced tokamak core with Super-H pedestalTorkil Jensen AwardVictorLLNLYesNoNo
376Super H-mode with broader current density profileD&C - Steady State ScenariosVictorLLNLYesNoNo
378Increase beta_n in high qmin plasmas with variable voltage beamsD&C - Steady State ScenariosVictorLLNLYesNoNo
379Test stability and confinement of qmin>2, q95<7 steady-state scenarioD&C - Steady State ScenariosHolcombLLNLYesNoNo
380Improved stability of high qmin plasmas through feedback control of the loop voltage profileD&C - Steady State ScenariosVictorLLNLYesNoNo
382Inside-out mitigation with B & B+W shell pelletsD&C - Disruption Mitigation PhysicsEidietisGAYesNoYes
383Measure halo & core temperatures during type I & II VDE'sD&C - Disruption Mitigation PhysicsEidietisGAYesNoYes
384Can Pellets Stabilize NTMs?D&C - 3D and Stability PhysicsBardocziGAYesNoNo
385Low energy NBI for efficient angular momentum injectionTorkil Jensen AwardEidietisGAYesNoNo
387Can Pellets Completely Stabilize the deleterious 2/1 NTMs?Torkil Jensen AwardBardocziGAYesNoNo
388Study of the thermal quench during minor disruption triggered by RMPsD&C - 3D and Stability PhysicsHuPPPLYesNoNo
396The Interplay of Magnetic Balance With Divertor Closure and Its Effect on Radiating Div PerformanceCore-Edge Integration Task ForcePetrieGAYesNoNo
397Stable Super H-mode with optimized pedestal densityCore-Edge Integration Task ForceKnolkerGAYesNoNo
399Access and control of QH-mode in IBS at low NBI torqueThrust 1 - ITER Q=10 (Inductive Scenarios)GarofaloGAYesNoYes
402Direct measurement of n=2 Multimode StabilityD&C - 3D and Stability PhysicsWangPPPLYesNoNo
403Investigate impact of energetic particles on neoclassical toroidal viscosityThrust 4 - Rotation PhysicsWangPPPLYesNoNo
405Investigation on core impurity transport in ITER-relevant ELM-y and QH-mode plasmasBPP - Turbulence and TransportSciortinoMax-Planck Institute for Plasma PhysicsYesNoNo
409Isotope scaling at fixed grad-teGeneral PhysicsscottPPPLYesNoNo
414Prospects for Suppressing Impurity Buildup at the Plasma Center During ECH Heating of AT PlasmasCore-Edge Integration Task ForcePetrieGAYesNoNo
418Quantify contribution of resistivity to external kink mode stabilityD&C - 3D and Stability PhysicsHansonColumbia UYesNoNo
419Search for path towards zero torque QH-mode for IBS and scaling of critical ExB shear requirementsThrust 1 - ITER Q=10 (Inductive Scenarios)WilksMassachusetts Institute of TechnologyYesNoNo
421Impact of shape and q95 on QH-mode EHO behaviorPE - Pedestal/SOL Physics and Pedestal OptimizationWilksMassachusetts Institute of TechnologyYesNoNo
422Low Torque n=1 Locking Threshold Scaling with RotationD&C - 3D and Stability PhysicsParkPPPLYesYesYes
423Commissioning of Laser Blow-Off (LBO) and Piggyback Studies of Impurity Transport on DIII-DBPP - Turbulence and TransportHowardMassachusetts Institute of TechnologyYesNoNo
424Studying the Ability of External Heating to Modify Impurity Transport in Reactor ScenariosBPP - Turbulence and TransportHowardMassachusetts Institute of TechnologyYesNoNo
425Extend ELM suppression to DN Hybrid Fully Non-Inductive plasmasD&C - Steady State ScenariosNazikianGAYesNoNo
426Extend robust ELM suppression to the Q=10 ITER baseline scenario.Thrust 1 - ITER Q=10 (Inductive Scenarios)NazikianGAYesYesNo
427Super H-mode Access by Counter Beam Injection with n=3 RMP.Thrust 3 - ELM ControlNazikianGAYesNoNo
429Study of cold-pulse dynamics and 'nonlocal transport effects' using perturbative LBO injectionsBPP - Turbulence and TransportRodriguez FernandezMassachusetts Institute of TechnologyYesNoNo
430Extend broad pedestal QH regime to high power and high densityThrust 3 - ELM ControlNazikianGAYesNoNo
431Exploring the avoidance of NTM-locking-induced disruption in High-beta n & low-q dischargesD&C - 3D and Stability PhysicsInoueQSTYesNoNo
432Double Tearing Mode Exploration in Reversed Shear Plasmas with 3D Fields.D&C - 3D and Stability PhysicsTakechiNational Institutes for Quantum and Radiological Science and Technology (QST)YesNoNo
433RMP ELM Suppression with Lithium Enhanced PedestalCore-Edge Integration Task ForceNazikianGAYesNoNo
444Displacement between the density and temperature pedestalPE - Pedestal/SOL Physics and Pedestal OptimizationWangGAYesNoNo
449Exploit and explore the new stable zero torque ITER Baseline ScenarioThrust 1 - ITER Q=10 (Inductive Scenarios)TurcoColumbia UYesNoNo
450Stable zero torque IBS with dominant e- heating and low collisionalityThrust 1 - ITER Q=10 (Inductive Scenarios)TurcoColumbia UYesNoNo
451ITER Baseline Scenario with zero and negative rotationThrust 1 - ITER Q=10 (Inductive Scenarios)TurcoColumbia UYesNoNo
454Scaling of Detachment Front Structure with IP, BT, Heating Power, and X-point HeightDDS - DissipationJarvinenVTT Technical Research CentreYesNoNo
455PCS Optimization of DIII-D Disruptivity Reduction via Deep Learning GuidanceD&C - 3D and Stability PhysicsTangPPPLYesNoNo
460Detachment facilitation with flux expansion in the SAS 1 slotThrust 2 - Divertor DevelopmentCoveleGAYesNoNo
462PCS Optimization of DIII-D Disruptivity Reduction via Deep Learning GuidanceD&C - 3D and Stability PhysicsKates-HarbeckPPPL/Harvard UYesNoNo
463Impurity Assisted Detachment in Moderate to High Density ConditionsDDS - DissipationJarvinenVTT Technical Research CentreYesNoNo
464Assessing the importance of intrinsic carbon radiation and D2 molecules in SAS 1 power dissipationThrust 2 - Divertor DevelopmentCoveleGAYesNoNo
467The effects of divertor detachment on pedestal width scalingPE - Pedestal/SOL Physics and Pedestal OptimizationWangGAYesNoNo
470Investigation of fuel recycling on tungsten in fusion-relevant conditionsAMV - Surface Evolution ScienceGuterlGAYesNoNo
471Parametric Study of Mode Stability, Frequency, and Wave Number Dependence in Mixed Species PlasmasBPP - Energetic Particle PhysicsTangOak Ridge Associated UniversitiesYesYesNo
472Effects of radiative fluctuations and current convective instability on detachmentDDS - TurbulenceGuterlGAYesNoNo
474Particle source location and its impact on the pedestalCore-Edge Integration Task ForceLaggnerNorth Carolina StateYesNoNo
475Onset and scaling of helical cores in hybrid plasmasCore-Edge Integration Task ForceWingenORNLYesNoNo
476Onset and scaling of helical cores in hybrid plasmasD&C - 3D and Stability PhysicsWingenORNLYesNoNo
477Active control of enhanced confinement regimes with Low Z impurity Powder DroppingCore-Edge Integration Task ForceLaggnerNorth Carolina StateYesNoNo
479The hysteresis between the access of ELM suppression and its exitThrust 3 - ELM ControlLaggnerNorth Carolina StateYesNoNo
483Core impurity contamination by unipolar arcing on PFCsAMV - Material Migration and MitigationBykovGAYesNoNo
485Investigate the Turbulence Suppression in High Betap Plasmas when Te is Close to TiEAST - Scenarios and TransportDingGAYesNoNo
486Super H-Mode Pedestal Optimization: Effect of fuelling source, density and currentPE - Pedestal/SOL Physics and Pedestal OptimizationSnyderORNLYesNoNo
487RMP ELM mitigation and suppression in the Super H-Mode regimeThrust 3 - ELM ControlSnyderORNLYesNoNo
488n=1 RMP ELM suppression (in conjunction with intrinsic error fields, phasing and shape dependence)Thrust 3 - ELM ControlInUlsan National Institute of Science and TechnologYesNoNo
489Arcing threshold due to ELM deposition at the strike point and in the scrape-off layerAMV - Surface Evolution ScienceBykovGAYesNoNo
493I-mode identity experiment on DIII-D and ASDEX Upgrade: access, performance and transportPE - Pedestal/SOL Physics and Pedestal OptimizationHappelMax-Planck-Institut f�¼r PlasmaphysikYesYesNo
494I-mode identity experiment on DIII-D and ASDEX Upgrade: access, performance and transportPE - Pedestal/SOL Physics and Pedestal OptimizationHappelMax-Planck-Institut f�¼r PlasmaphysikYesYesNo
4962D Isotope Scan for Energy ConfinementBPP - Turbulence and TransportThomeGAYesNoNo
498High qmin, high beta in smaller shapeD&C - Steady State ScenariosParkORNLYesNoNo
499Document and reduce fast-ion transport in steady-state scenariosD&C - Steady State ScenariosThomeGAYesNoNo
502Exploring new reactor concepts: H-mode at negative triangularityTorkil Jensen AwardMarinoniUCSDYesNoNo
503Avoidance of TM during target formation of high beta, high qmin scenariosD&C - Steady State ScenariosParkORNLYesNoNo
504Exploring new reactor concepts: H-mode at negative triangularityBPP - Turbulence and TransportMarinoniUCSDYesNoNo
507Optimization of ELMfree high-performance plasmas at negative triangularityBPP - Turbulence and TransportMarinoniUCSDYesNoNo
512Effect of EC location and heat/CD on the confinement and stability of the IBSThrust 1 - ITER Q=10 (Inductive Scenarios)TurcoColumbia UYesNoNo
515Core-Edge Investigations in the Super H and Near Super H RegimeCore-Edge Integration Task ForceSnyderORNLYesNoNo
517n=1 RMP ELM suppression with full I+C coil optimizationThrust 3 - ELM ControlParkPPPLYesNoNo
518Further investigation of the saturation & underlying transport mechanism of EHO to allow ELM stableThrust 3 - ELM ControlChenGAYesNoNo
519ELM suppression in the low torque IBS using rotating n=2 fieldsThrust 1 - ITER Q=10 (Inductive Scenarios)WangPPPLYesNoNo
521Reduce AE induced EP transport in high q-min steady state scenarios with AE control toolsD&C - Steady State ScenariosCollinsORNLYesYesNo
522Optimum EC and CD location in high betaN hybridsD&C - Steady State ScenariosTurcoColumbia UYesNoNo
528ECCD-induced ELM suppression in low-torque ITER-baseline scenarioThrust 1 - ITER Q=10 (Inductive Scenarios)LyonsGAYesNoNo
530Intrinsic Rotation and Core Transport in Wide Pedestal QH-Mode with Electron HeatingThrust 4 - Rotation PhysicsErnstMassachusetts Institute of TechnologyYesNoNo
533Reduce AE induced EP transport in high q-min steady state scenarios with AE control toolsBPP - Energetic Particle PhysicsCollinsORNLYesYesNo
535Extend fully non-inductive high betap scenario to Ip~1MA towards Q=5 mission of ITEREAST - Scenarios and TransportHuangASIPPYesNoNo
538Electron Temperature Profile Stiffness in Wide Pedestal QH-ModeBPP - Turbulence and TransportErnstMassachusetts Institute of TechnologyYesNoNo
540Erosion Characterization of W-alternative PFMs under L-mode & H-mode using Micro-Trench TechniqueAMV - Innovative Materials DevelopmentCoburnSandia National LabYesNoNo
546Dependence of L-H power threshold on X-point heightBPP - L-H transitionSamuellLLNLYesNoNo
547Long range impurity transport in the H-mode scrape off layerDDS - Drifts and FlowsSamuellLLNLYesNoNo
548Characterizing Detachment in H-mode Helium PlasmasDDS - DissipationSamuellLLNLYesNoNo
549Helium Campain 2018General PhysicsSamuellLLNLYesNoNo
552Understanding W edge transport via introducing a well-defined W sourceEAST - BoundaryDingASIPPYesNoNo
553Test compatibility of radiative divertor with QH-modeThrust 1 - ITER Q=10 (Inductive Scenarios)GarofaloGAYesNoNo
562Measurement of local erosion/redeposition impulse functionAMV - Surface Evolution ScienceHinsonORNLYesNoNo
565Understand effect of resonant vs non-resonant magnetic perturbations on L-H transition dynamicsBPP - L-H transitionKrieteU of WisconsinYesNoNo
571Imaging of the ELM suppression mechanism using MIR and ECEIThrust 3 - ELM ControlZhuUC DavisYesNoNo
572Imaging of the ELM suppression mechanism using MIR and ECEIThrust 3 - ELM ControlZhuUC, DavisYesNoNo
579Wide Pedestal QH-Mode Core and Pedestal Compatibility with Electron HeatingThrust 3 - ELM ControlErnstMassachusetts Institute of TechnologyYesNoNo
580Steady-state hybrids with higher ideal MHD limitsD&C - Steady State ScenariosTurcoColumbia UYesNoNo
581Effect of Divertor Geometry on High-Performance CoreCore-Edge Integration Task ForceThomeGAYesNoNo
582Sustain and investigate EDA H-mode regime at near zero torquePE - Pedestal/SOL Physics and Pedestal OptimizationKumar BaradaUCLAYesNoNo
583Effect of prompt and delayed fuel re-emission on apparent SP footprint during ELMsThrust 3 - ELM ControlBykovGAYesNoNo
586Improve pedestal of wide-pedestal QH-mode with ECH and RMP and study the effect on LCOsThrust 3 - ELM ControlKumar BaradaUCLAYesNoNo
592Toroidally-resolved lobe dynamics in ELM-mitigated and ELM-suppressed scenariosThrust 3 - ELM ControlBykovGAYesNoNo
602Performance of irradiated W, SiC, and SiC/W composites as a PFC materialAMV - Surface Evolution ScienceAbramsGAYesNoNo
603Measure D retention/recycling properties of bulk SiC versus fibrous SiC/SiC in DIII-D divertorAMV - Innovative Materials DevelopmentAbramsGAYesNoNo
6153D spectrum dependence on L-H transition in DIII-DBPP - L-H transitionKoNational Fusion Research InstituteYesNoNo
6163D spectrum dependence on L-H transition in DIII-DBPP - L-H transitionKoNational Fusion Research InstituteYesNoNo
617D2 re-emission from prospective materials: characterization by ro-vibrational sp. in H-modeAMV - Innovative Materials DevelopmentBykovGAYesNoNo
618Better Physics Understanding of NTM SeedingD&C - 3D and Stability PhysicsLa HayeRetired from GAYesNoNo
621QH-mode similarity experiment between DIII-D and AUG with co-current beamsThrust 3 - ELM ControlViezzerU of SevilleYesNoNo
626RMP ELM suppression in the IBS with radiating divertor by Ar injectionThrust 1 - ITER Q=10 (Inductive Scenarios)TurcoColumbia UYesYesNo
627Impact of siliconization on SAS divertor performanceThrust 2 - Divertor DevelopmentAbramsGAYesNoNo
630ELM suppression in the SASThrust 2 - Divertor DevelopmentNazikianGAYesNoNo
636Safety Factor Profile Optimization of Wide Pedestal QH-Mode for Electron HeatingThrust 1 - ITER Q=10 (Inductive Scenarios)ErnstMassachusetts Institute of TechnologyYesNoNo
637ELM filament footprint in j, q_perp, Da etc. (#583 for AMV)AMV - Surface Evolution ScienceBykovGAYesNoNo
639Measurement of 3D ion impact geometry by erosion of med-Z spherical micro particlesAMV - Material Migration and MitigationBykovGAYesNoNo
640Aimed visible/NIR spectroscopy for measurement of impurity flux from natural hot spotsGeneral PhysicsBykovGAYesNoNo
641Visible spectroscopy for impurity flux from and temperature of leading edges on DiMES (#640 for AMV)AMV - Material Migration and MitigationBykovGAYesNoNo
642Testing and control of radiation divertor with neon and argon seeding in high beta_p scenarioEAST - BoundaryWangASIPPYesNoNo
643Steady-state, high beta_pol plasma utilizing the SAS divertorCore-Edge Integration Task ForceVictorLLNLYesNoNo
648Extend Zero Torque Wide Pedestal QH-Mode Operation to IBS ParametersThrust 1 - ITER Q=10 (Inductive Scenarios)ErnstMassachusetts Institute of TechnologyYesNoNo
649Exposure of graphitic foam with CVI SiC coatingsAMV - Innovative Materials DevelopmentUnterbergORNLYesNoNo
650Influence of thin in-situ Si coatings on SOL carbon contentAMV - Material Migration and MitigationUnterbergORNLYesNoNo
651Impact of gaps/trenches on high-Z material migrationAMV - Material Migration and MitigationUnterbergORNLYesNoNo
652W deposition from a complete core source with shell pellets and collector probeAMV - Material Migration and MitigationUnterbergORNLYesNoNo
653Preferential sputtering of Si or C from SiC versus temperatureAMV - Surface Evolution ScienceUnterbergORNLYesNoNo
655World first deuterium poloidal rotation measurements using main ion CER spectroscopyTorkil Jensen AwardHaskeyPPPLYesNoNo
664Unique Code Validation via Comparison of HFS/LFS and exploring up/down asymmetry in turbulenceBPP - Turbulence and TransportSungKAISTYesNoNo
667Measurement of poloidal flow structuresBPP - Turbulence and TransportBortolonPPPLYesNoNo
668Measurement of poloidal flow structuresBPP - Turbulence and TransportBortolonPPPLYesNoNo
669Study of Electro-Magnetic quasi-coherent fluctuation under various plasma conditionsBPP - Turbulence and TransportChenUCLAYesNoNo
670Validation of high-Z dust ablation models in edge plasmaGeneral PhysicsGuterlGAYesNoNo
675Compare Er measured by DBS and CER in important DIII-D plasmasGeneral PhysicsKumar BaradaUCLAYesNoNo
679SiC Sputtering and Near-surface Characterization Under He BombardmentAMV - Surface Evolution ScienceBringuierGAYesNoNo