DIII-D RESEARCH OPPORTUNITIES FORUM FOR THE 2018 EXPERIMENTAL CAMPAIGN

Author (full last name only):
Keyword:

Click here for internal detailed listing
Below is a public summary listing:

ID Title Research Area Name Affiliation Time
Req'ed
ITPA
Joint Exp
ITER IO Urgent
Research Task
385Low energy NBI for efficient angular momentum injectionTorkil Jensen AwardEidietisGAYesNoNo
387Can Pellets Completely Stabilize the deleterious 2/1 NTMs?Torkil Jensen AwardBardocziGAYesNoNo
502Exploring new reactor concepts: H-mode at negative triangularityTorkil Jensen AwardMarinoniUCSDYesNoNo
375Advanced tokamak core with Super-H pedestalTorkil Jensen AwardVictorLLNLYesNoNo
655World first deuterium poloidal rotation measurements using main ion CER spectroscopyTorkil Jensen AwardHaskeyPPPLYesNoNo
660Poloidal rotation measurements using main ion CER spectroscopyThrust 4 - Rotation PhysicsHaskeyPPPLNoNoNo
403Investigate impact of energetic particles on neoclassical toroidal viscosityThrust 4 - Rotation PhysicsWangPPPLYesNoNo
510Turbulence and core intrinsic rotation hollowingThrust 4 - Rotation PhysicsStoltzfus-DueckPPPLNoNoNo
359Effect of beam tangency on locking thresholdThrust 4 - Rotation PhysicsFerraroPPPLNoNoNo
369Role of micro-turbulence in intrinsic rotation reversals through JET DIII-D similarity experimentsThrust 4 - Rotation PhysicsNaveInstituto Superior Tecnico, Lisboa, PortugalYesNoNo
340Improved stability of counter rotating plasmasThrust 4 - Rotation PhysicsVictorLLNLYesNoNo
366Using up/down asymmetry to Increase the intrinsic rotationThrust 4 - Rotation PhysicsVictorLLNLYesNoNo
623Intrinsic rotation drive and RS asymmetries with geometry. USN/LSN and poloidal variationThrust 4 - Rotation PhysicsBoedoUCSDNoNoNo
551Intrinsic Rotation in a Negative Triangularity PlasmaThrust 4 - Rotation PhysicsAshourvanGANoNoNo
530Intrinsic Rotation and Core Transport in Wide Pedestal QH-Mode with Electron HeatingThrust 4 - Rotation PhysicsErnstMassachusetts Institute of TechnologyYesNoNo
520Intrinsic rotation in detached divertorThrust 4 - Rotation PhysicsGriersonGANoNoNo
348Intrinsic Rotation Dependence on Plasma ShapeThrust 4 - Rotation PhysicsdeGrassieGANoNoNo
469Effect of neutrals on edge momentum transportThrust 4 - Rotation PhysicsChrystalGANoNoNo
585Er dependency of NTVThrust 4 - Rotation PhysicsLeeNational Fusion Research InstituteNoNoNo
621QH-mode similarity experiment between DIII-D and AUG with co-current beamsThrust 3 - ELM ControlViezzerU of SevilleYesNoNo
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
571Imaging of the ELM suppression mechanism using MIR and ECEIThrust 3 - ELM ControlZhuUC DavisYesNoNo
427Super H-mode Access by Counter Beam Injection with n=3 RMP.Thrust 3 - ELM ControlNazikianGAYesNoNo
430Extend broad pedestal QH regime to high power and high densityThrust 3 - ELM ControlNazikianGAYesNoNo
420Low n, Low Field ELM-suppression with edge ECCDThrust 3 - ELM ControlLoganColumbia UNoNoNo
352Direct comparison of ITER similar shape (ISS) and ITER baseline scenario (IBS) plasmas for RMP-ELMThrust 3 - ELM ControlPaz-SoldanColumbia UNoNoNo
526Explore rotation thresholds with variable upper triangularityThrust 3 - ELM ControlPaz-SoldanColumbia UNoNoNo
417QH-mode with zero torque throughoutThrust 3 - ELM ControlBurrellGANoNoNo
480Magnetic topology identification by dual soft X-ray camera system during non-rotating n=2 RMPThrust 3 - ELM ControlDuGANoNoNo
518Further investigation of the saturation & underlying transport mechanism of EHO to allow ELM stableThrust 3 - ELM ControlChenGAYesNoNo
351Development of the low-torque wide-pedestal QH-mode with EHOThrust 3 - ELM ControlChenGAYesNoNo
371plasma response to n=2 rotating RMP with q95 scan between 4 and 6Thrust 3 - ELM ControlLiuGANoNoNo
583Effect of prompt and delayed fuel re-emission on apparent SP footprint during ELMsThrust 3 - ELM ControlBykovGAYesNoNo
592Toroidally-resolved lobe dynamics in ELM-mitigated and ELM-suppressed scenariosThrust 3 - ELM ControlBykovGAYesNoNo
579Wide Pedestal QH-Mode Core and Pedestal Compatibility with Electron HeatingThrust 3 - ELM ControlErnstMassachusetts Institute of TechnologyYesNoNo
501Pellet ELM pacing with field aligned tangential injectionThrust 3 - ELM ControlBaylorORNLNoNoYes
355Rotating n=2 fields with edge ECCD to reduce ELM suppression threshold amplitudeThrust 3 - ELM ControlWilcoxORNLYesNoNo
487RMP ELM mitigation and suppression in the Super H-Mode regimeThrust 3 - ELM ControlSnyderORNLYesNoNo
541Plasma Response and ELM Supssion Dependence on SN v DNThrust 3 - ELM ControlShaferORNLNoNoNo
572Imaging of the ELM suppression mechanism using MIR and ECEIThrust 3 - ELM ControlZhuUC, DavisYesNoNo
586Improve pedestal of wide-pedestal QH-mode with ECH and RMP and study the effect on LCOsThrust 3 - ELM ControlKumar BaradaUCLAYesNoNo
620QH-mode without NBIThrust 3 - ELM ControlBortolonPPPLNoNoNo
543ELMs and ELM mitigation during ITER relevant Ip ramp-up/downThrust 3 - ELM ControlBortolonPPPLNoNoNo
517n=1 RMP ELM suppression with full I+C coil optimizationThrust 3 - ELM ControlParkPPPLYesNoNo
445Effect of plasma rotation on ELM suppression threshold and density pump-out by RMPsThrust 3 - ELM ControlHuPPPLNoNoNo
563ELM suppression with rotation control with NBI voltageThrust 3 - ELM ControlKolemenPPPLNoNoNo
466Control with new real-time Pedestal CER systemThrust 3 - ELM ControlKolemenPPPLNoNoNo
478ELM pacing using impurity pellet injectionThrust 3 - ELM ControlLaggnerNorth Carolina StateNoNoNo
479The hysteresis between the access of ELM suppression and its exitThrust 3 - ELM ControlLaggnerNorth Carolina StateYesNoNo
663Role of the turbulent transport due to a broadband MHD in association with a change in Er structureThrust 3 - ELM ControlOnoQSTNoNoNo
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
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
644Impact of main ion dilution on core and edge turbulence and transport in high performance IBSsThrust 2 - Divertor DevelopmentMarinoniUCSDNoNoNo
527Comparison of pumping with private flux and shared flux pumping in attached and detached plasmasThrust 2 - Divertor DevelopmentLuceITER OrganizationNoNoNo
544Detachment dependence on neutral pressure in the SAS divertorThrust 2 - Divertor DevelopmentShaferORNLNoNoNo
678Characterizing misalignment between SAS and magnetic fieldThrust 2 - Divertor DevelopmentMoserGANoNoNo
569Effect of SAS divertor on pedestalThrust 2 - Divertor DevelopmentMoserGANoNoNo
635Convex mirror on DiMES to view upper SASThrust 2 - Divertor DevelopmentBykovGANoNoNo
627Impact of siliconization on SAS divertor performanceThrust 2 - Divertor DevelopmentAbramsGAYesNoNo
398Magnetic Balance Combined with Divertor Closure and Its Effect on Radiating Diverter PerformanceThrust 2 - Divertor DevelopmentPetrieGANoNoNo
401The Most Effective Radiating Divertor That DIII-D Can Presently Make in the DN ShapeThrust 2 - Divertor DevelopmentPetrieGANoNoNo
677Effect of RMP application on the dissipative divertor regimeThrust 2 - Divertor DevelopmentSchmitzUW MadisonNoYesYes
630ELM suppression in the SASThrust 2 - Divertor DevelopmentNazikianGAYesNoNo
587SAS meets DNThrust 2 - Divertor DevelopmentThomasGANoNoNo
464Assessing the importance of intrinsic carbon radiation and D2 molecules in SAS 1 power dissipationThrust 2 - Divertor DevelopmentCoveleGAYesNoNo
460Detachment facilitation with flux expansion in the SAS 1 slotThrust 2 - Divertor DevelopmentCoveleGAYesNoNo
426Extend robust ELM suppression to the Q=10 ITER baseline scenario.Thrust 1 - ITER Q=10 (Inductive Scenarios)NazikianGAYesYesNo
626RMP ELM suppression in the IBS with radiating divertor by Ar injectionThrust 1 - ITER Q=10 (Inductive Scenarios)TurcoColumbia UYesYesNo
512Effect of EC location and heat/CD on the confinement and stability of the IBSThrust 1 - ITER Q=10 (Inductive Scenarios)TurcoColumbia UYesNoNo
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
353Increase normalized beta of torque-free 3rd harmonic EC heated ITER baseline scenario plasmasThrust 1 - ITER Q=10 (Inductive Scenarios)Paz-SoldanColumbia UNoNoNo
368Get Advance Inductive QH Mode to Zero TorqueThrust 1 - ITER Q=10 (Inductive Scenarios)ButteryGAYesNoNo
399Access and control of QH-mode in IBS at low NBI torqueThrust 1 - ITER Q=10 (Inductive Scenarios)GarofaloGAYesNoYes
553Test compatibility of radiative divertor with QH-modeThrust 1 - ITER Q=10 (Inductive Scenarios)GarofaloGAYesNoNo
528ECCD-induced ELM suppression in low-torque ITER-baseline scenarioThrust 1 - ITER Q=10 (Inductive Scenarios)LyonsGAYesNoNo
636Safety Factor Profile Optimization of Wide Pedestal QH-Mode for Electron HeatingThrust 1 - ITER Q=10 (Inductive Scenarios)ErnstMassachusetts Institute of TechnologyYesNoNo
648Extend Zero Torque Wide Pedestal QH-Mode Operation to IBS ParametersThrust 1 - ITER Q=10 (Inductive Scenarios)ErnstMassachusetts Institute of TechnologyYesNoNo
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
625Measuring the effect of edge Z effective on RMP ELM suppression via impurity injectionThrust 1 - ITER Q=10 (Inductive Scenarios)WeisbergGANoNoNo
452ITER Baseline Scenario at Zero and Negative RotationThrust 1 - ITER Q=10 (Inductive Scenarios)LuceITER OrganizationNoYesNo
611Radiative divertor solutions in the ITER baseline scenarioThrust 1 - ITER Q=10 (Inductive Scenarios)LuceITER OrganizationNoYesNo
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
557Controlling the plasma edge rotation for QH-mode accessThrust 1 - ITER Q=10 (Inductive Scenarios)KolemenPPPLNoNoNo
442Stability of Plasma with Derivative of Current Profile Equal to zeroThrust 1 - ITER Q=10 (Inductive Scenarios)KolemenPPPLNoNoNo
647ELMs and ELM pacing in an ITER-baseline without NBIThrust 1 - ITER Q=10 (Inductive Scenarios)BortolonPPPLNoNoNo
519ELM suppression in the low torque IBS using rotating n=2 fieldsThrust 1 - ITER Q=10 (Inductive Scenarios)WangPPPLYesNoNo
410Characterize the pedestal particle transport induced by RMPPE - Pedestal/SOL Physics and Pedestal OptimizationDialloPPPLNoNoNo
605Validate EPED and Eich's ELM model in He plasmasPE - Pedestal/SOL Physics and Pedestal OptimizationBortolonPPPLNoNoNo
672Understanding the physics of RMP density pump-outPE - Pedestal/SOL Physics and Pedestal OptimizationSungKAISTNoNoNo
582Sustain and investigate EDA H-mode regime at near zero torquePE - Pedestal/SOL Physics and Pedestal OptimizationKumar BaradaUCLAYesNoNo
506Reproduce past IBS He plasmas in D to compare H-mode characteristics for ITERPE - Pedestal/SOL Physics and Pedestal OptimizationMarinoniUCSDNoNoNo
619Study of ELM Dynamics using Fast Main-Ion CERPE - Pedestal/SOL Physics and Pedestal OptimizationAshourvanGANoNoNo
421Impact of shape and q95 on QH-mode EHO behaviorPE - Pedestal/SOL Physics and Pedestal OptimizationWilksMassachusetts Institute of TechnologyYesNoNo
486Super H-Mode Pedestal Optimization: Effect of fuelling source, density and currentPE - Pedestal/SOL Physics and Pedestal OptimizationSnyderORNLYesNoNo
631Further investigation of the saturation & underlying transport mechanism of EHO to allow ELM stablePE - Pedestal/SOL Physics and Pedestal OptimizationChenGANoNoNo
367ELM studies close to LH boundaryPE - Pedestal/SOL Physics and Pedestal OptimizationKnolkerGAYesYesNo
467The effects of divertor detachment on pedestal width scalingPE - Pedestal/SOL Physics and Pedestal OptimizationWangGAYesNoNo
444Displacement between the density and temperature pedestalPE - Pedestal/SOL Physics and Pedestal OptimizationWangGAYesNoNo
492Does the edge localized pedestal particle source directly effect pedestal structurePE - Pedestal/SOL Physics and Pedestal OptimizationOsborneGANoNoNo
354Pedestal Stability in ELM free ECH H-modePE - Pedestal/SOL Physics and Pedestal OptimizationChrystalGANoNoNo
370Control of the inter-ELM pedestal fluctuationsPE - Pedestal/SOL Physics and Pedestal OptimizationLaggnerPrinceton UniverstiyYesNoNo
411Characterize the pedestal particle transport induced by RMPPE - Pedestal/SOL Physics and Pedestal OptimizationDialloPPPLNoNoNo
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
409Isotope scaling at fixed grad-teGeneral PhysicsscottPPPLYesNoNo
640Aimed visible/NIR spectroscopy for measurement of impurity flux from natural hot spotsGeneral PhysicsBykovGAYesNoNo
614Non thermal contribution to MWIR during ELMs, disruptions and in detachment (ROF2017 #177)General PhysicsBykovGANoNoNo
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
338Welcome to the 2018 ROF - note you don't need to re-enter last year's proposalsGeneral PhysicsFenstermacherLLNLNoNoNo
549Helium Campain 2018General PhysicsSamuellLLNLYesNoNo
491Boron and Boron Carbide granule injection for real time wall conditioningGeneral PhysicsLunsfordPPPLNoNoNo
578Establish in-shot boronization for low collisionality operationGeneral PhysicsBortolonPPPLNoNoNo
535Extend fully non-inductive high betap scenario to Ip~1MA towards Q=5 mission of ITEREAST - Scenarios and TransportHuangASIPPYesNoNo
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
628Understanding the limits of confinement from internal transport barriersEAST - Scenarios and TransportMcClenaghanGANoNoNo
485Investigate the Turbulence Suppression in High Betap Plasmas when Te is Close to TiEAST - Scenarios and TransportDingGAYesNoNo
361RMP ELM suppression in the high betaP scenario at lower q95EAST - Control and StabilityWeisbergGANoNoNo
552Understanding W edge transport via introducing a well-defined W sourceEAST - BoundaryDingASIPPYesNoNo
642Testing and control of radiation divertor with neon and argon seeding in high beta_p scenarioEAST - BoundaryWangASIPPYesNoNo
622Effect of divertor turbulence on upstream pedestal/SOLDDS - TurbulenceBoedoUCSDNoNoNo
390Study properties of the singularity that is the X-pointDDS - TurbulenceBoedoUCSDNoNoNo
391Turbulnce in detaching and detached divertorDDS - TurbulenceBoedoUCSDNoNoNo
607Effect on SEE on Langmuir probe measurements in the SOLDDS - TurbulenceRudakovUCSDNoNoNo
468Enhanced quasi-coherent fluctuations and associated transport in detached plasmasDDS - TurbulenceWangGANoNoNo
472Effects of radiative fluctuations and current convective instability on detachmentDDS - TurbulenceGuterlGAYesNoNo
343Mapping the Te cliff using detachment controlDDS - Drifts and FlowsEldonGANoNoNo
344Search for Te cliff at inner strike point in reverse BtDDS - Drifts and FlowsEldonGANoNoNo
661Effect of pumping on secondary strike pointDDS - Drifts and FlowsEldonGANoNoNo
584Divertor detachment in closed divertor with unfavorable BtDDS - Drifts and FlowsWangGANoNoNo
392DIvertor and pedestal flows in attached and detached plasmasDDS - Drifts and FlowsBoedoUCSDNoNoNo
393ExB drifts in detached divertor and X-pointDDS - Drifts and FlowsBoedoUCSDNoNoNo
577Characterize upstream SOL impurity transport in attached/detached divertorDDS - Drifts and FlowsBortolonPPPLNoNoNo
547Long range impurity transport in the H-mode scrape off layerDDS - Drifts and FlowsSamuellLLNLYesNoNo
548Characterizing Detachment in H-mode Helium PlasmasDDS - DissipationSamuellLLNLYesNoNo
633Scaling of Detachment and Radiative Divertor with SOL heat fluxDDS - DissipationJarvinenVTT Technical Research CentreNoNoNo
463Impurity Assisted Detachment in Moderate to High Density ConditionsDDS - DissipationJarvinenVTT Technical Research CentreYesNoNo
454Scaling of Detachment Front Structure with IP, BT, Heating Power, and X-point HeightDDS - DissipationJarvinenVTT Technical Research CentreYesNoNo
539Detachment physics of Helium H-modesDDS - DissipationCanikORNLNoNoNo
339Detachment onset density vs. 3D field strengthDDS - DissipationEldonGANoNoNo
341Detachment control with neonDDS - DissipationEldonGANoNoNo
381Combined detachment + radiated power controlDDS - DissipationEldonGANoNoNo
634Measuring poloidal variations of cross-field transport in the DIII-D SOLDDS - DissipationCoveleGANoNoNo
588Detachment Study using the Progressive Angle DivertorDDS - DissipationThomasGANoNoNo
555Helium plasma detachment behavior in closed divertorDDS - DissipationMeierZap Energy Inc.NoNoNo
416ramp-up optimization for access to high qmin SSD&C - Steady State ScenariosMaria PoliPPPLNoNoNo
425Extend ELM suppression to DN Hybrid Fully Non-Inductive plasmasD&C - Steady State ScenariosNazikianGAYesNoNo
580Steady-state hybrids with higher ideal MHD limitsD&C - Steady State ScenariosTurcoColumbia UYesNoNo
522Optimum EC and CD location in high betaN hybridsD&C - Steady State ScenariosTurcoColumbia UYesNoNo
484High Pedestal in Hybrid Scenario With Unfavorable Grad-B Drift DirectionD&C - Steady State ScenariosPettyGANoNoNo
503Avoidance of TM during target formation of high beta, high qmin scenariosD&C - Steady State ScenariosParkORNLYesNoNo
498High qmin, high beta in smaller shapeD&C - Steady State ScenariosParkORNLYesNoNo
509Optimum current profile for the integrated core/pedestal performanceD&C - Steady State ScenariosParkORNLNoNoNo
521Reduce AE induced EP transport in high q-min steady state scenarios with AE control toolsD&C - Steady State ScenariosCollinsORNLYesYesNo
499Document and reduce fast-ion transport in steady-state scenariosD&C - Steady State ScenariosThomeGAYesNoNo
376Super H-mode with broader current density profileD&C - Steady State ScenariosVictorLLNLYesNoNo
379Test stability and confinement of qmin>2, q95<7 steady-state scenarioD&C - Steady State ScenariosHolcombLLNLYesNoNo
378Increase beta_n in high qmin plasmas with variable voltage beamsD&C - Steady State ScenariosVictorLLNLYesNoNo
380Improved stability of high qmin plasmas through feedback control of the loop voltage profileD&C - Steady State ScenariosVictorLLNLYesNoNo
497Test of effect of wall stabilizationD&C - Steady State ScenariosLuceITER OrganizationNoNoNo
632AE control by ECH and NB voltage variationD&C - Plasma ControlHuASIPPNoNoNo
513Develop Safe Rampdown for Plasmas with High Radiative FractionD&C - Plasma ControlLuceITER OrganizationNoYesNo
413Ramp-down (dedicated+piggyback) survey for disruption avoidanceD&C - Plasma ControlBarrGANoNoNo
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
593Development of Rotation Profile Feedback Control Capability in DIII-DD&C - Plasma ControlSchusterLehigh UNoNoNo
599Actuator Sharing and Integrated Control of Magnetic and Kinetic Plasma ParametersD&C - Plasma ControlSchusterLehigh UNoNoNo
534PCS implementation of Machine Learning algorithm for disruption predictionD&C - Plasma ControlReaMassachusetts Institute of TechnologyNoNoNo
342Detachment control with raw TS signals instead of analyzed TeD&C - Plasma ControlEldonGANoNoNo
575Control/Ops Evening Test SessionsD&C - Plasma ControlHumphreysGANoNoNo
408Voltage controlled SuperSpas for plasma shape controlD&C - Plasma ControlHyattGANoNoNo
448VFI-less Plasma operationsD&C - Plasma ControlHyattGANoNoNo
676Shot-shot reproducibility against wall loading of impuritiesD&C - Plasma ControlEldonGANoNoNo
443Langmuir probe based detachment controlD&C - Plasma ControlEldonGANoNoNo
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
495Evaluation of ITER startup scenarioD&C - Plasma ControlWalkerGANoNoYes
567Actuator sharing via control supervisorD&C - Plasma ControlWalkerGANoNoYes
373helium startup characterizationD&C - Plasma ControlWalkerGANoNoYes
459Advanced Divertor Control DevelopmentD&C - Plasma ControlVailPrinceton UNoNoNo
656Real-time Stability Analysis for Stability ControlD&C - Plasma ControlKolemenPPPLNoNoNo
447Control based on Machine LearningD&C - Plasma ControlKolemenPPPLNoNoNo
457Real-time Stability Analysis for Stability ControlD&C - Plasma ControlKolemenPPPLNoNoNo
456EPED-NN-based feedback control of pedestal parametersD&C - Plasma ControlBoyerPPPLNoNoNo
446Feedback control of the edge rotation shear using variable beam voltage and perveanceD&C - Plasma ControlBoyerPPPLNoNoNo
629Feedback control of current and stored energy in non-inductive scenarios on DIII-DD&C - Plasma ControlBoyerPPPLNoNoNo
481PCS setup for proposal #370D&C - Plasma ControlLaggnerNorth Carolina StateNoNoNo
482PCS setup for proposal #477D&C - Plasma ControlLaggnerNorth Carolina StateNoNoNo
435Disruption prediction and avoidance based on Machine LearningD&C - Disruption Mitigation PhysicsKolemenPPPLNoNoNo
363Integration of Deep Learning Disruption Predictor with Plasma Control SystemD&C - Disruption Mitigation PhysicsTangPPPLNoNoNo
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
441SPI penetration depth / assimilation efficiencyD&C - Disruption Mitigation PhysicsLehnenITER OrganizationNoNoYes
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
362Effect of RMP on RE spatial gradients (in QRE)D&C - Disruption Mitigation PhysicsPaz-SoldanColumbia UNoNoNo
372Radiation saturation at reduced Ne quantity by order of magnitude increase in D2 inventoryD&C - Disruption Mitigation PhysicsSweeneyMassachusetts Institute of TechnologyYesNoYes
529Low-current runaway electron plateau dissipation by injected impuritiesD&C - Disruption Mitigation PhysicsLvovskiyGANoNoNo
377ITPA Joint Experiment on gamma-ray measurements of runaway electronsD&C - Disruption Mitigation PhysicsLvovskiyGANoYesNo
465Superposition of dual SPIs for TQ mitigation � part 2D&C - Disruption Mitigation PhysicsHerfindalORNLNoNoYes
531Impurity spreading physics and impact on fast shutdown propertiesD&C - Disruption Mitigation PhysicsShirakiORNLNoNoYes
532Fast shutdown with argon shattered pelletD&C - Disruption Mitigation PhysicsShirakiORNLNoNoNo
404RE plateau vertical loss rate during high-Z dissipationD&C - Disruption Mitigation PhysicsHollmannUCSDNoNoNo
374Aspect ratio scaling of tearing stabilityD&C - 3D and Stability PhysicsMortonU of WisconsinYesNoNo
476Onset and scaling of helical cores in hybrid plasmasD&C - 3D and Stability PhysicsWingenORNLYesNoNo
415n=2 Locking Threshold Scaling for ITERD&C - 3D and Stability PhysicsLoganColumbia UNoYesNo
418Quantify contribution of resistivity to external kink mode stabilityD&C - 3D and Stability PhysicsHansonColumbia UYesNoNo
455PCS Optimization of DIII-D Disruptivity Reduction via Deep Learning GuidanceD&C - 3D and Stability PhysicsTangPPPLYesNoNo
458�Integration of Deep Learning Disruption Predictor with Plasma Control System�D&C - 3D and Stability PhysicsTangPPPLNoNoNo
462PCS Optimization of DIII-D Disruptivity Reduction via Deep Learning GuidanceD&C - 3D and Stability PhysicsKates-HarbeckPPPL/Harvard UYesNoNo
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
473Double Tearing Mode Exploration in Reversed Shear Plasmas with 3D Fields.D&C - 3D and Stability PhysicsTakechiQSTNoNoNo
428Feedback control of 2/1 locked mode phase with RMP and synchronized ECCDD&C - 3D and Stability PhysicsChoiGANoNoNo
384Can Pellets Stabilize NTMs?D&C - 3D and Stability PhysicsBardocziGAYesNoNo
624Revisiting preemptive NTM locking avoidance with improved feedback logic in high ���²N plasmaD&C - 3D and Stability PhysicsOkabayashiPPPLNoNoNo
638Machine Learning based Disruption Prediction & AvoidanceD&C - 3D and Stability PhysicsKolemenPPPLNoNoNo
508Island suppression using real-time Thomson Scattering enhanced EFITD&C - 3D and Stability PhysicsRoelofsPPPLNoNoNo
388Study of the thermal quench during minor disruption triggered by RMPsD&C - 3D and Stability PhysicsHuPPPLYesNoNo
386Control of rotating NTM by ECCD + RMPD&C - 3D and Stability PhysicsHuPPPLNoNoNo
422Low Torque n=1 Locking Threshold Scaling with RotationD&C - 3D and Stability PhysicsParkPPPLYesYesYes
402Direct measurement of n=2 Multimode StabilityD&C - 3D and Stability PhysicsWangPPPLYesNoNo
618Better Physics Understanding of NTM SeedingD&C - 3D and Stability PhysicsLa HayeRetired from GAYesNoNo
474Particle source location and its impact on the pedestalCore-Edge Integration Task ForceLaggnerNorth Carolina StateYesNoNo
477Active control of enhanced confinement regimes with Low Z impurity Powder DroppingCore-Edge Integration Task ForceLaggnerNorth Carolina StateYesNoNo
609Compatibility of advanced scenarios with silicon coated PCFCore-Edge Integration Task ForceBortolonPPPLNoNoNo
550Transport in the no man's land: how pedestal performance propagates to the coreCore-Edge Integration Task ForceBortolonPPPLNoNoNo
396The Interplay of Magnetic Balance With Divertor Closure and Its Effect on Radiating Div PerformanceCore-Edge Integration Task ForcePetrieGAYesNoNo
525Global confinement and edge rotation for private, strike, and common flux pumpingCore-Edge Integration Task ForceGriersonGANoNoNo
414Prospects for Suppressing Impurity Buildup at the Plasma Center During ECH Heating of AT PlasmasCore-Edge Integration Task ForcePetrieGAYesNoNo
400The Most Effective Radiating Divertor That DIII-D Can Presently Make in the DN ShapeCore-Edge Integration Task ForcePetrieGANoNoNo
574Compare DN/SN vertical and shape controllabilityCore-Edge Integration Task ForceHumphreysGANoYesNo
397Stable Super H-mode with optimized pedestal densityCore-Edge Integration Task ForceKnolkerGAYesNoNo
581Effect of Divertor Geometry on High-Performance CoreCore-Edge Integration Task ForceThomeGAYesNoNo
594Physics of Puff and PumpCore-Edge Integration Task ForceAllenLLNLNoNoNo
412Prospects for Suppressing Impurity Buildup at the Plasma Center During ECH Heating of AT PlasmasCore-Edge Integration Task ForcePetrieGANoNoNo
433RMP ELM Suppression with Lithium Enhanced PedestalCore-Edge Integration Task ForceNazikianGAYesNoNo
475Onset and scaling of helical cores in hybrid plasmasCore-Edge Integration Task ForceWingenORNLYesNoNo
658RMP effects on heavy non-recycling impurity confinement and exhaustCore-Edge Integration Task ForceHinsonORNLNoNoNo
3583D boundary effects on heavy impurity removalCore-Edge Integration Task ForceHinsonORNLYesNoNo
564RMP effects on He confinement and exhaustCore-Edge Integration Task ForceHinsonORNLNoNoNo
515Core-Edge Investigations in the Super H and Near Super H RegimeCore-Edge Integration Task ForceSnyderORNLYesNoNo
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
516Effect of differing edge relaxation mechanisms on global impurity confinement timesCore-Edge Integration Task ForceHughesMassachusetts Institute of TechnologyNoYesNo
568Impact of medium Zi dilution of deuterium pasma on core and edge turbulence and transportCore-Edge Integration Task ForcePorkolabMassachusetts Institute of TechnologyNoNoNo
566Impact of Divertor Conditions on Radial Electric Field at the Pedestal-SOL BoundaryCore-Edge Integration Task ForceJarvinenVTT Technical Research CentreNoNoNo
389Poloidal asymmetry of RS inward momentum pinch and USN/LSN dependenceCore-Edge Integration Task ForceBoedoUCSDNoNoNo
558Transport alteration and confinement improvement via radiative impurity-seedingCore-Edge Integration Task ForceMcKeeU of WisconsinNoNoNo
645H-mode at negative triangularity as a feasibility study for future machinesCore-Edge Integration Task ForceMarinoniUCSDNoNoNo
643Steady-state, high beta_pol plasma utilizing the SAS divertorCore-Edge Integration Task ForceVictorLLNLYesNoNo
364Role of divertor geometry on confinementCore-Edge Integration Task ForceMordijckThe college of William and MaryNoNoNo
365High opacity SOL effect on pedestalCore-Edge Integration Task ForceMordijckThe college of William and MaryNoYesYes
667Measurement of poloidal flow structuresBPP - Turbulence and TransportBortolonPPPLYesNoNo
669Study of Electro-Magnetic quasi-coherent fluctuation under various plasma conditionsBPP - Turbulence and TransportChenUCLAYesNoNo
576Understanding improved confinement in negative triangularity dischargesBPP - Turbulence and TransportAustinU. TexasNoNoNo
511Investigation of loss of linear current scaling at low q95BPP - Turbulence and TransportLuceITER OrganizationNoNoNo
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
507Optimization of ELMfree high-performance plasmas at negative triangularityBPP - Turbulence and TransportMarinoniUCSDYesNoNo
504Exploring new reactor concepts: H-mode at negative triangularityBPP - Turbulence and TransportMarinoniUCSDYesNoNo
657Investigation of turbulence changes with ELM suppression by RMPsBPP - Turbulence and TransportSungKAISTNoNoNo
664Unique Code Validation via Comparison of HFS/LFS and exploring up/down asymmetry in turbulenceBPP - Turbulence and TransportSungKAISTYesNoNo
570Impact of medium Zi dilution of deuterium pasma on core and edge turbulence and transportBPP - Turbulence and TransportPorkolabMassachusetts Institute of TechnologyNoNoNo
538Electron Temperature Profile Stiffness in Wide Pedestal QH-ModeBPP - Turbulence and TransportErnstMassachusetts Institute of TechnologyYesNoNo
429Study of cold-pulse dynamics and 'nonlocal transport effects' using perturbative LBO injectionsBPP - Turbulence and TransportRodriguez FernandezMassachusetts Institute of TechnologyYesNoNo
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
405Investigation on core impurity transport in ITER-relevant ELM-y and QH-mode plasmasBPP - Turbulence and TransportSciortinoMax-Planck Institute for Plasma PhysicsYesNoNo
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
4962D Isotope Scan for Energy ConfinementBPP - Turbulence and TransportThomeGAYesNoNo
665H-mode impurity transport dependence on beam fuelingBPP - Turbulence and TransportThomeGANoNoYes
668Measurement of poloidal flow structuresBPP - Turbulence and TransportBortolonPPPLYesNoNo
666Validate low-k magnetic turbulence predictions relevant to the burning plasma coreBPP - Turbulence and TransportGuttenfelderPPPLNoNoNo
573Understanding improved confinement in negative triangularity dischargesBPP - Turbulence and TransportAustinU of Texas, AustinNoNoNo
360L-H Transitions dynamics: Impact of the beam voltage and its effects on the edge rotation shearBPP - L-H transitionDialloPPPLNoNoNo
671Pellet induced H-mode with Tangential D2 Pellet InjectionBPP - L-H transitionBaylorORNLNoNoNo
565Understand effect of resonant vs non-resonant magnetic perturbations on L-H transition dynamicsBPP - L-H transitionKrieteU of WisconsinYesNoNo
434RMP Spectrum Control to Improve H-mode AccessBPP - L-H transitionSchmitzUCLANoNoNo
546Dependence of L-H power threshold on X-point heightBPP - L-H transitionSamuellLLNLYesNoNo
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
395Prospects for Suppressing Impurity Buildup at the Plasma Center During ECH Heating of AT PlasmasBPP - Heating & Current DrivePetrieGANoNoNo
514Test DIII-D NB operation to 93 kVBPP - Heating & Current DriveLuceITER OrganizationNoNoNo
662HFS LHCD Passive High Z Metallic Structure TestBPP - Heating & Current DriveWukitchMassachusetts Institute of TechnologyNoNoNo
533Reduce AE induced EP transport in high q-min steady state scenarios with AE control toolsBPP - Energetic Particle PhysicsCollinsORNLYesYesNo
490Triton Burn-up Study in DIII-D TokamakBPP - Energetic Particle PhysicsZhuUC, IrvineNoNoNo
600BAE/BAAE validationBPP - Energetic Particle PhysicsHeidbrinkUC, IrvineNoYesNo
601Fast-ion transport by BAAEsBPP - Energetic Particle PhysicsHeidbrinkUC, IrvineNoNoNo
604Resonant fast-ion transport by applied 3D fieldsBPP - Energetic Particle PhysicsHeidbrinkUC, IrvineNoNoNo
654Fast-ion and AE control via externally applied 3D fieldsBPP - Energetic Particle PhysicsGarcia MunozU of SevilleNoYesNo
471Parametric Study of Mode Stability, Frequency, and Wave Number Dependence in Mixed Species PlasmasBPP - Energetic Particle PhysicsTangOak Ridge Associated UniversitiesYesYesNo
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
470Investigation of fuel recycling on tungsten in fusion-relevant conditionsAMV - Surface Evolution ScienceGuterlGAYesNoNo
637ELM filament footprint in j, q_perp, Da etc. (#583 for AMV)AMV - Surface Evolution ScienceBykovGAYesNoNo
556High-Z and textured surface arcing susceptibilityAMV - Surface Evolution ScienceJaworskiPPPLNoNoNo
602Performance of irradiated W, SiC, and SiC/W composites as a PFC materialAMV - Surface Evolution ScienceAbramsGAYesNoNo
646Density Dependence of W I & W II SXB Ratios for Improved Erosion and Redeposition DiagnosisAMV - Surface Evolution ScienceEnnisAuburn UNoNoNo
608Dust re-mobilization studies using DiMESAMV - Surface Evolution ScienceRudakovUCSDNoNoNo
349In-situ formation of Si-C coatings on DiMESAMV - Surface Evolution ScienceRudakovUCSDYesNoNo
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
653Preferential sputtering of Si or C from SiC versus temperatureAMV - Surface Evolution ScienceUnterbergORNLYesNoNo
562Measurement of local erosion/redeposition impulse functionAMV - Surface Evolution ScienceHinsonORNLYesNoNo
489Arcing threshold due to ELM deposition at the strike point and in the scrape-off layerAMV - Surface Evolution ScienceBykovGAYesNoNo
679SiC Sputtering and Near-surface Characterization Under He BombardmentAMV - Surface Evolution ScienceBringuierGAYesNoNo
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
536Testing of a new neutral H sensor for C-X H fluxes on the wall and divertorAMV - Material Migration and MitigationBartonSandia National LabNoNoNo
394Comparison of silicon and carbon erosion and migration by exposure of isotope SiC coatingAMV - Material Migration and MitigationDingASIPPNoNoNo
610Power loading at toroidal PFC gapsAMV - Material Migration and MitigationRudakovUCSDNoYesYes
483Core impurity contamination by unipolar arcing on PFCsAMV - Material Migration and MitigationBykovGAYesNoNo
641Visible spectroscopy for impurity flux from and temperature of leading edges on DiMES (#640 for AMV)AMV - Material Migration and MitigationBykovGAYesNoNo
639Measurement of 3D ion impact geometry by erosion of med-Z spherical micro particlesAMV - Material Migration and MitigationBykovGAYesNoNo
356Spectroscopic analysis of SiC preferential sputteringAMV - Material Migration and MitigationAbramsGAYesNoNo
357ELM-resolved measurements of high-Z re-deposition fractionsAMV - Material Migration and MitigationAbramsGAYesNoNo
554Boundary Ion temperature measurement based on retarding field analyzerAMV - Material Migration and MitigationRenU of Tennessee, KnoxvilleNoNoNo
617D2 re-emission from prospective materials: characterization by ro-vibrational sp. in H-modeAMV - Innovative Materials DevelopmentBykovGAYesNoNo
659testing the transparent materials with DIMESAMV - Innovative Materials DevelopmentPigarovCompXNoNoNo
603Measure D retention/recycling properties of bulk SiC versus fibrous SiC/SiC in DIII-D divertorAMV - Innovative Materials DevelopmentAbramsGAYesNoNo
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
613Assessment of property changes in W, SiC and their composites exposed to D3D environmentsAMV - Innovative Materials DevelopmentVasudevamurthyGANoNoNo
537Expose UFG W to DIII-D discharges to demonstrate improved properties useful in future PFCsAMV - Innovative Materials DevelopmentBartonSandia National LabNoNoNo
542Effect of heated DiMES on erosion of W-alternative PFMsAMV - Innovative Materials DevelopmentCoburnSandia National LabNoNoNo
540Erosion Characterization of W-alternative PFMs under L-mode & H-mode using Micro-Trench TechniqueAMV - Innovative Materials DevelopmentCoburnSandia National LabYesNoNo
649Exposure of graphitic foam with CVI SiC coatingsAMV - Innovative Materials DevelopmentUnterbergORNLYesNoNo
612Variations in Thermomechanical Stability between Amorphous and Polycrystalline SiCAMV - Innovative Materials DevelopmentBringuierGANoNoNo
598Influence of SiC Microstructure and Texture on SputteringAMV - Innovative Materials DevelopmentBringuierGANoNoNo