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
551Intrinsic Rotation in a Negative Triangularity PlasmaThrust 4 - Rotation PhysicsAshourvanGANoNoNo
619Study of ELM Dynamics using Fast Main-Ion CERPE - Pedestal/SOL Physics and Pedestal OptimizationAshourvanGANoNoNo
573Understanding improved confinement in negative triangularity dischargesBPP - Turbulence and TransportAustinU of Texas, AustinNoNoNo
413Ramp-down (dedicated+piggyback) survey for disruption avoidanceD&C - Plasma ControlBarrGANoNoNo
536Testing of a new neutral H sensor for C-X H fluxes on the wall and divertorAMV - Material Migration and MitigationBartonSandia National LabNoNoNo
537Expose UFG W to DIII-D discharges to demonstrate improved properties useful in future PFCsAMV - Innovative Materials DevelopmentBartonSandia National LabNoNoNo
501Pellet ELM pacing with field aligned tangential injectionThrust 3 - ELM ControlBaylorORNLNoNoYes
671Pellet induced H-mode with Tangential D2 Pellet InjectionBPP - L-H transitionBaylorORNLNoNoNo
389Poloidal asymmetry of RS inward momentum pinch and USN/LSN dependenceCore-Edge Integration Task ForceBoedoUCSDNoNoNo
390Study properties of the singularity that is the X-pointDDS - TurbulenceBoedoUCSDNoNoNo
391Turbulnce in detaching and detached divertorDDS - TurbulenceBoedoUCSDNoNoNo
392DIvertor and pedestal flows in attached and detached plasmasDDS - Drifts and FlowsBoedoUCSDNoNoNo
393ExB drifts in detached divertor and X-pointDDS - Drifts and FlowsBoedoUCSDNoNoNo
622Effect of divertor turbulence on upstream pedestal/SOLDDS - TurbulenceBoedoUCSDNoNoNo
623Intrinsic rotation drive and RS asymmetries with geometry. USN/LSN and poloidal variationThrust 4 - Rotation PhysicsBoedoUCSDNoNoNo
543ELMs and ELM mitigation during ITER relevant Ip ramp-up/downThrust 3 - ELM ControlBortolonPPPLNoNoNo
550Transport in the no man's land: how pedestal performance propagates to the coreCore-Edge Integration Task ForceBortolonPPPLNoNoNo
577Characterize upstream SOL impurity transport in attached/detached divertorDDS - Drifts and FlowsBortolonPPPLNoNoNo
578Establish in-shot boronization for low collisionality operationGeneral PhysicsBortolonPPPLNoNoNo
605Validate EPED and Eich's ELM model in He plasmasPE - Pedestal/SOL Physics and Pedestal OptimizationBortolonPPPLNoNoNo
609Compatibility of advanced scenarios with silicon coated PCFCore-Edge Integration Task ForceBortolonPPPLNoNoNo
620QH-mode without NBIThrust 3 - ELM ControlBortolonPPPLNoNoNo
647ELMs and ELM pacing in an ITER-baseline without NBIThrust 1 - ITER Q=10 (Inductive Scenarios)BortolonPPPLNoNoNo
446Feedback control of the edge rotation shear using variable beam voltage and perveanceD&C - Plasma ControlBoyerPPPLNoNoNo
456EPED-NN-based feedback control of pedestal parametersD&C - Plasma ControlBoyerPPPLNoNoNo
629Feedback control of current and stored energy in non-inductive scenarios on DIII-DD&C - Plasma ControlBoyerPPPLNoNoNo
598Influence of SiC Microstructure and Texture on SputteringAMV - Innovative Materials DevelopmentBringuierGANoNoNo
612Variations in Thermomechanical Stability between Amorphous and Polycrystalline SiCAMV - Innovative Materials DevelopmentBringuierGANoNoNo
417QH-mode with zero torque throughoutThrust 3 - ELM ControlBurrellGANoNoNo
614Non thermal contribution to MWIR during ELMs, disruptions and in detachment (ROF2017 #177)General PhysicsBykovGANoNoNo
635Convex mirror on DiMES to view upper SASThrust 2 - Divertor DevelopmentBykovGANoNoNo
539Detachment physics of Helium H-modesDDS - DissipationCanikORNLNoNoNo
560Understanding divertor closure's effect on power dissipation and radiation by impurity seedingThrust 2 - Divertor DevelopmentCasaliU of Tennessee, KnoxvilleNoNoNo
561Understanding divertor closure's effect on SOL impurity transportThrust 2 - Divertor DevelopmentCasaliU of Tennessee, KnoxvilleNoNoNo
631Further investigation of the saturation & underlying transport mechanism of EHO to allow ELM stablePE - Pedestal/SOL Physics and Pedestal OptimizationChenGANoNoNo
428Feedback control of 2/1 locked mode phase with RMP and synchronized ECCDD&C - 3D and Stability PhysicsChoiGANoNoNo
354Pedestal Stability in ELM free ECH H-modePE - Pedestal/SOL Physics and Pedestal OptimizationChrystalGANoNoNo
469Effect of neutrals on edge momentum transportThrust 4 - Rotation PhysicsChrystalGANoNoNo
542Effect of heated DiMES on erosion of W-alternative PFMsAMV - Innovative Materials DevelopmentCoburnSandia National LabNoNoNo
348Intrinsic Rotation Dependence on Plasma ShapeThrust 4 - Rotation PhysicsdeGrassieGANoNoNo
360L-H Transitions dynamics: Impact of the beam voltage and its effects on the edge rotation shearBPP - L-H transitionDialloPPPLNoNoNo
410Characterize the pedestal particle transport induced by RMPPE - Pedestal/SOL Physics and Pedestal OptimizationDialloPPPLNoNoNo
394Comparison of silicon and carbon erosion and migration by exposure of isotope SiC coatingAMV - Material Migration and MitigationDingASIPPNoNoNo
453Verification of Imaging Neutral Particle Analyzer and its application to the phase-space flow studyBPP - Energetic Particle PhysicsDuGANoNoNo
461Investigation of runaway electron-driven magnetized plasma wave and whistler in tokamakBPP - Energetic Particle PhysicsDuGANoNoNo
480Magnetic topology identification by dual soft X-ray camera system during non-rotating n=2 RMPThrust 3 - ELM ControlDuGANoNoNo
339Detachment onset density vs. 3D field strengthDDS - DissipationEldonGANoNoNo
341Detachment control with neonDDS - DissipationEldonGANoNoNo
342Detachment control with raw TS signals instead of analyzed TeD&C - Plasma ControlEldonGANoNoNo
343Mapping the Te cliff using detachment controlDDS - Drifts and FlowsEldonGANoNoNo
344Search for Te cliff at inner strike point in reverse BtDDS - Drifts and FlowsEldonGANoNoNo
345Detachment control performance vs. puff locationD&C - Plasma ControlEldonGANoNoNo
346Detachment control performance vs. power scans & impurity accumulationD&C - Plasma ControlEldonGANoNoNo
347Divertor radiation controlD&C - Plasma ControlEldonGANoNoNo
381Combined detachment + radiated power controlDDS - DissipationEldonGANoNoNo
443Langmuir probe based detachment controlD&C - Plasma ControlEldonGANoNoNo
661Effect of pumping on secondary strike pointDDS - Drifts and FlowsEldonGANoNoNo
676Shot-shot reproducibility against wall loading of impuritiesD&C - Plasma ControlEldonGANoNoNo
646Density Dependence of W I & W II SXB Ratios for Improved Erosion and Redeposition DiagnosisAMV - Surface Evolution ScienceEnnisAuburn UNoNoNo
338Welcome to the 2018 ROF - note you don't need to re-enter last year's proposalsGeneral PhysicsFenstermacherLLNLNoNoNo
359Effect of beam tangency on locking thresholdThrust 4 - Rotation PhysicsFerraroPPPLNoNoNo
520Intrinsic rotation in detached divertorThrust 4 - Rotation PhysicsGriersonGANoNoNo
525Global confinement and edge rotation for private, strike, and common flux pumpingCore-Edge Integration Task ForceGriersonGANoNoNo
666Validate low-k magnetic turbulence predictions relevant to the burning plasma coreBPP - Turbulence and TransportGuttenfelderPPPLNoNoNo
660Poloidal rotation measurements using main ion CER spectroscopyThrust 4 - Rotation PhysicsHaskeyPPPLNoNoNo
575Control/Ops Evening Test SessionsD&C - Plasma ControlHumphreysGANoNoNo
386Control of rotating NTM by ECCD + RMPD&C - 3D and Stability PhysicsHuPPPLNoNoNo
445Effect of plasma rotation on ELM suppression threshold and density pump-out by RMPsThrust 3 - ELM ControlHuPPPLNoNoNo
632AE control by ECH and NB voltage variationD&C - Plasma ControlHuASIPPNoNoNo
408Voltage controlled SuperSpas for plasma shape controlD&C - Plasma ControlHyattGANoNoNo
448VFI-less Plasma operationsD&C - Plasma ControlHyattGANoNoNo
566Impact of Divertor Conditions on Radial Electric Field at the Pedestal-SOL BoundaryCore-Edge Integration Task ForceJarvinenVTT Technical Research CentreNoNoNo
633Scaling of Detachment and Radiative Divertor with SOL heat fluxDDS - DissipationJarvinenVTT Technical Research CentreNoNoNo
435Disruption prediction and avoidance based on Machine LearningD&C - Disruption Mitigation PhysicsKolemenPPPLNoNoNo
442Stability of Plasma with Derivative of Current Profile Equal to zeroThrust 1 - ITER Q=10 (Inductive Scenarios)KolemenPPPLNoNoNo
447Control based on Machine LearningD&C - Plasma ControlKolemenPPPLNoNoNo
457Real-time Stability Analysis for Stability ControlD&C - Plasma ControlKolemenPPPLNoNoNo
466Control with new real-time Pedestal CER systemThrust 3 - ELM ControlKolemenPPPLNoNoNo
557Controlling the plasma edge rotation for QH-mode accessThrust 1 - ITER Q=10 (Inductive Scenarios)KolemenPPPLNoNoNo
563ELM suppression with rotation control with NBI voltageThrust 3 - ELM ControlKolemenPPPLNoNoNo
638Machine Learning based Disruption Prediction & AvoidanceD&C - 3D and Stability PhysicsKolemenPPPLNoNoNo
656Real-time Stability Analysis for Stability ControlD&C - Plasma ControlKolemenPPPLNoNoNo
478ELM pacing using impurity pellet injectionThrust 3 - ELM ControlLaggnerNorth Carolina StateNoNoNo
481PCS setup for proposal #370D&C - Plasma ControlLaggnerNorth Carolina StateNoNoNo
482PCS setup for proposal #477D&C - Plasma ControlLaggnerNorth Carolina StateNoNoNo
371plasma response to n=2 rotating RMP with q95 scan between 4 and 6Thrust 3 - ELM ControlLiuGANoNoNo
601Fast-ion transport by BAAEsBPP - Energetic Particle PhysicsHeidbrinkUC, IrvineNoNoNo
604Resonant fast-ion transport by applied 3D fieldsBPP - Energetic Particle PhysicsHeidbrinkUC, IrvineNoNoNo
465Superposition of dual SPIs for TQ mitigation � part 2D&C - Disruption Mitigation PhysicsHerfindalORNLNoNoYes
564RMP effects on He confinement and exhaustCore-Edge Integration Task ForceHinsonORNLNoNoNo
658RMP effects on heavy non-recycling impurity confinement and exhaustCore-Edge Integration Task ForceHinsonORNLNoNoNo
404RE plateau vertical loss rate during high-Z dissipationD&C - Disruption Mitigation PhysicsHollmannUCSDNoNoNo
497Test of effect of wall stabilizationD&C - Steady State ScenariosLuceITER OrganizationNoNoNo
500Test advanced inductive performance vs q95 at fixed BThrust 1 - ITER Q=10 (Inductive Scenarios)LuceITER OrganizationNoNoNo
505Revisit zero torque advanced inductive scenarioThrust 1 - ITER Q=10 (Inductive Scenarios)LuceITER OrganizationNoNoNo
511Investigation of loss of linear current scaling at low q95BPP - Turbulence and TransportLuceITER OrganizationNoNoNo
420Low n, Low Field ELM-suppression with edge ECCDThrust 3 - ELM ControlLoganColumbia UNoNoNo
514Test DIII-D NB operation to 93 kVBPP - Heating & Current DriveLuceITER OrganizationNoNoNo
527Comparison of pumping with private flux and shared flux pumping in attached and detached plasmasThrust 2 - Divertor DevelopmentLuceITER OrganizationNoNoNo
556High-Z and textured surface arcing susceptibilityAMV - Surface Evolution ScienceJaworskiPPPLNoNoNo
576Understanding improved confinement in negative triangularity dischargesBPP - Turbulence and TransportAustinU. TexasNoNoNo
585Er dependency of NTVThrust 4 - Rotation PhysicsLeeNational Fusion Research InstituteNoNoNo
594Physics of Puff and PumpCore-Edge Integration Task ForceAllenLLNLNoNoNo
613Assessment of property changes in W, SiC and their composites exposed to D3D environmentsAMV - Innovative Materials DevelopmentVasudevamurthyGANoNoNo
634Measuring poloidal variations of cross-field transport in the DIII-D SOLDDS - DissipationCoveleGANoNoNo
441SPI penetration depth / assimilation efficiencyD&C - Disruption Mitigation PhysicsLehnenITER OrganizationNoNoYes
458�Integration of Deep Learning Disruption Predictor with Plasma Control System�D&C - 3D and Stability PhysicsTangPPPLNoNoNo
459Advanced Divertor Control DevelopmentD&C - Plasma ControlVailPrinceton UNoNoNo
473Double Tearing Mode Exploration in Reversed Shear Plasmas with 3D Fields.D&C - 3D and Stability PhysicsTakechiQSTNoNoNo
523ELM suppression in a matched KSTAR shape with n=2 fieldsThrust 3 - ELM ControlEvansGANoNoNo
524ELM suppression in a matched KSTAR shape with n=2 fieldsThrust 3 - ELM ControlEvansGANoNoNo
624Revisiting preemptive NTM locking avoidance with improved feedback logic in high ���²N plasmaD&C - 3D and Stability PhysicsOkabayashiPPPLNoNoNo
663Role of the turbulent transport due to a broadband MHD in association with a change in Er structureThrust 3 - ELM ControlOnoQSTNoNoNo
492Does the edge localized pedestal particle source directly effect pedestal structurePE - Pedestal/SOL Physics and Pedestal OptimizationOsborneGANoNoNo
509Optimum current profile for the integrated core/pedestal performanceD&C - Steady State ScenariosParkORNLNoNoNo
352Direct comparison of ITER similar shape (ISS) and ITER baseline scenario (IBS) plasmas for RMP-ELMThrust 3 - ELM ControlPaz-SoldanColumbia UNoNoNo
353Increase normalized beta of torque-free 3rd harmonic EC heated ITER baseline scenario plasmasThrust 1 - ITER Q=10 (Inductive Scenarios)Paz-SoldanColumbia UNoNoNo
362Effect of RMP on RE spatial gradients (in QRE)D&C - Disruption Mitigation PhysicsPaz-SoldanColumbia UNoNoNo
526Explore rotation thresholds with variable upper triangularityThrust 3 - ELM ControlPaz-SoldanColumbia UNoNoNo
395Prospects for Suppressing Impurity Buildup at the Plasma Center During ECH Heating of AT PlasmasBPP - Heating & Current DrivePetrieGANoNoNo
398Magnetic Balance Combined with Divertor Closure and Its Effect on Radiating Diverter PerformanceThrust 2 - Divertor DevelopmentPetrieGANoNoNo
400The Most Effective Radiating Divertor That DIII-D Can Presently Make in the DN ShapeCore-Edge Integration Task ForcePetrieGANoNoNo
401The Most Effective Radiating Divertor That DIII-D Can Presently Make in the DN ShapeThrust 2 - Divertor DevelopmentPetrieGANoNoNo
484High Pedestal in Hybrid Scenario With Unfavorable Grad-B Drift DirectionD&C - Steady State ScenariosPettyGANoNoNo
659testing the transparent materials with DIMESAMV - Innovative Materials DevelopmentPigarovCompXNoNoNo
416ramp-up optimization for access to high qmin SSD&C - Steady State ScenariosMaria PoliPPPLNoNoNo
568Impact of medium Zi dilution of deuterium pasma on core and edge turbulence and transportCore-Edge Integration Task ForcePorkolabMassachusetts Institute of TechnologyNoNoNo
570Impact of medium Zi dilution of deuterium pasma on core and edge turbulence and transportBPP - Turbulence and TransportPorkolabMassachusetts Institute of TechnologyNoNoNo
436Development of high betaP scenario with active pedestal controlEAST - Scenarios and TransportQianASIPPNoNoNo
437Exploration of Fully Non-inductive High �²p Scenarios with QH-mode EdgeEAST - Scenarios and TransportQianASIPPNoNoNo
534PCS implementation of Machine Learning algorithm for disruption predictionD&C - Plasma ControlReaMassachusetts Institute of TechnologyNoNoNo
554Boundary Ion temperature measurement based on retarding field analyzerAMV - Material Migration and MitigationRenU of Tennessee, KnoxvilleNoNoNo
508Island suppression using real-time Thomson Scattering enhanced EFITD&C - 3D and Stability PhysicsRoelofsPPPLNoNoNo
350Measuring net and gross erosion rates of SiC in DIII-D divertor and main chamberAMV - Surface Evolution ScienceRudakovUCSDNoNoNo
606Studies of Arcing on high-Z PFC SurfacesAMV - Surface Evolution ScienceRudakovUCSDNoNoNo
607Effect on SEE on Langmuir probe measurements in the SOLDDS - TurbulenceRudakovUCSDNoNoNo
608Dust re-mobilization studies using DiMESAMV - Surface Evolution ScienceRudakovUCSDNoNoNo
434RMP Spectrum Control to Improve H-mode AccessBPP - L-H transitionSchmitzUCLANoNoNo
593Development of Rotation Profile Feedback Control Capability in DIII-DD&C - Plasma ControlSchusterLehigh UNoNoNo
595Integrated Current Profile Control and NTM Stabilization DemonstrationD&C - Plasma ControlSchusterLehigh UNoNoNo
596Further Development of Real-time Optimization for MHD-free Steady-state OperationD&C - Plasma ControlSchusterLehigh UNoNoNo
597Development of Model-based qmin Control Capability in DIII-DD&C - Plasma ControlSchusterLehigh UNoNoNo
599Actuator Sharing and Integrated Control of Magnetic and Kinetic Plasma ParametersD&C - Plasma ControlSchusterLehigh UNoNoNo
406Investigation on impurity transport and turbulence in internal transport barriersBPP - Turbulence and TransportSciortinoMax-Planck Institute for Plasma PhysicsNoNoNo
407Effect of Injected Torque and Current Drive on Impurity TransportBPP - Turbulence and TransportSciortinoMax-Planck Institute for Plasma PhysicsNoNoNo
541Plasma Response and ELM Supssion Dependence on SN v DNThrust 3 - ELM ControlShaferORNLNoNoNo
544Detachment dependence on neutral pressure in the SAS divertorThrust 2 - Divertor DevelopmentShaferORNLNoNoNo
545Dependence of neutral pressure on detachmentCore-Edge Integration Task ForceShaferORNLNoNoNo
559Effects of divertor closure on pedestal fueling and non-diffusive transport with pellet fuelingCore-Edge Integration Task ForceShaferORNLNoNoNo
531Impurity spreading physics and impact on fast shutdown propertiesD&C - Disruption Mitigation PhysicsShirakiORNLNoNoYes
532Fast shutdown with argon shattered pelletD&C - Disruption Mitigation PhysicsShirakiORNLNoNoNo
510Turbulence and core intrinsic rotation hollowingThrust 4 - Rotation PhysicsStoltzfus-DueckPPPLNoNoNo
657Investigation of turbulence changes with ELM suppression by RMPsBPP - Turbulence and TransportSungKAISTNoNoNo
672Understanding the physics of RMP density pump-outPE - Pedestal/SOL Physics and Pedestal OptimizationSungKAISTNoNoNo
587SAS meets DNThrust 2 - Divertor DevelopmentThomasGANoNoNo
588Detachment Study using the Progressive Angle DivertorDDS - DissipationThomasGANoNoNo
589SiC versus SiC Composite Dimes TestsAMV - Innovative Materials DevelopmentThomasGANoNoNo
590Heated SiC Dimes TestsAMV - Innovative Materials DevelopmentThomasGANoNoNo
591Test of micrograin Mo mirror conceptAMV - Innovative Materials DevelopmentThomasGANoNoNo
665H-mode impurity transport dependence on beam fuelingBPP - Turbulence and TransportThomeGANoNoYes
373helium startup characterizationD&C - Plasma ControlWalkerGANoNoYes
495Evaluation of ITER startup scenarioD&C - Plasma ControlWalkerGANoNoYes
567Actuator sharing via control supervisorD&C - Plasma ControlWalkerGANoNoYes
468Enhanced quasi-coherent fluctuations and associated transport in detached plasmasDDS - TurbulenceWangGANoNoNo
584Divertor detachment in closed divertor with unfavorable BtDDS - Drifts and FlowsWangGANoNoNo
361RMP ELM suppression in the high betaP scenario at lower q95EAST - Control and StabilityWeisbergGANoNoNo
625Measuring the effect of edge Z effective on RMP ELM suppression via impurity injectionThrust 1 - ITER Q=10 (Inductive Scenarios)WeisbergGANoNoNo
662HFS LHCD Passive High Z Metallic Structure TestBPP - Heating & Current DriveWukitchMassachusetts Institute of TechnologyNoNoNo
490Triton Burn-up Study in DIII-D TokamakBPP - Energetic Particle PhysicsZhuUC, IrvineNoNoNo
529Low-current runaway electron plateau dissipation by injected impuritiesD&C - Disruption Mitigation PhysicsLvovskiyGANoNoNo
506Reproduce past IBS He plasmas in D to compare H-mode characteristics for ITERPE - Pedestal/SOL Physics and Pedestal OptimizationMarinoniUCSDNoNoNo
644Impact of main ion dilution on core and edge turbulence and transport in high performance IBSsThrust 2 - Divertor DevelopmentMarinoniUCSDNoNoNo
645H-mode at negative triangularity as a feasibility study for future machinesCore-Edge Integration Task ForceMarinoniUCSDNoNoNo
673LH power threshold, confinement scaling and CER calibration in C plasmasBPP - Turbulence and TransportMarinoniUCSDNoNoNo
674Investigating the link between electron scale fluctuations and the ECH density pump-outBPP - Turbulence and TransportMarinoniUCSDNoNoNo
628Understanding the limits of confinement from internal transport barriersEAST - Scenarios and TransportMcClenaghanGANoNoNo
558Transport alteration and confinement improvement via radiative impurity-seedingCore-Edge Integration Task ForceMcKeeU of WisconsinNoNoNo
555Helium plasma detachment behavior in closed divertorDDS - DissipationMeierZap Energy Inc.NoNoNo
364Role of divertor geometry on confinementCore-Edge Integration Task ForceMordijckThe college of William and MaryNoNoNo
491Boron and Boron Carbide granule injection for real time wall conditioningGeneral PhysicsLunsfordPPPLNoNoNo
569Effect of SAS divertor on pedestalThrust 2 - Divertor DevelopmentMoserGANoNoNo
678Characterizing misalignment between SAS and magnetic fieldThrust 2 - Divertor DevelopmentMoserGANoNoNo
363Integration of Deep Learning Disruption Predictor with Plasma Control SystemD&C - Disruption Mitigation PhysicsTangPPPLNoNoNo
411Characterize the pedestal particle transport induced by RMPPE - Pedestal/SOL Physics and Pedestal OptimizationDialloPPPLNoNoNo
412Prospects for Suppressing Impurity Buildup at the Plasma Center During ECH Heating of AT PlasmasCore-Edge Integration Task ForcePetrieGANoNoNo
438Shallow injection with shards onlyD&C - Disruption Mitigation PhysicsMichaelITER OrganizationNoNoYes
439Optimisation of multiple SPID&C - Disruption Mitigation PhysicsLehnenITER OrganizationNoNoYes
440SPI injection into the early current quenchD&C - Disruption Mitigation PhysicsLehnenITER OrganizationNoNoYes
677Effect of RMP application on the dissipative divertor regimeThrust 2 - Divertor DevelopmentSchmitzUW MadisonNoYesYes
654Fast-ion and AE control via externally applied 3D fieldsBPP - Energetic Particle PhysicsGarcia MunozU of SevilleNoYesNo
377ITPA Joint Experiment on gamma-ray measurements of runaway electronsD&C - Disruption Mitigation PhysicsLvovskiyGANoYesNo
365High opacity SOL effect on pedestalCore-Edge Integration Task ForceMordijckThe college of William and MaryNoYesYes
610Power loading at toroidal PFC gapsAMV - Material Migration and MitigationRudakovUCSDNoYesYes
611Radiative divertor solutions in the ITER baseline scenarioThrust 1 - ITER Q=10 (Inductive Scenarios)LuceITER OrganizationNoYesNo
452ITER Baseline Scenario at Zero and Negative RotationThrust 1 - ITER Q=10 (Inductive Scenarios)LuceITER OrganizationNoYesNo
513Develop Safe Rampdown for Plasmas with High Radiative FractionD&C - Plasma ControlLuceITER OrganizationNoYesNo
516Effect of differing edge relaxation mechanisms on global impurity confinement timesCore-Edge Integration Task ForceHughesMassachusetts Institute of TechnologyNoYesNo
574Compare DN/SN vertical and shape controllabilityCore-Edge Integration Task ForceHumphreysGANoYesNo
415n=2 Locking Threshold Scaling for ITERD&C - 3D and Stability PhysicsLoganColumbia UNoYesNo
600BAE/BAAE validationBPP - Energetic Particle PhysicsHeidbrinkUC, IrvineNoYesNo