DIII-D RESEARCH OPPORTUNITIES FORUM FOR THE 2019 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
Presentation ITPA
Joint Exp
ITER IO Urgent
Research Task
1Welcome to the ROF for the 2019-20 DIII-D Run CampaignGeneral PhysicsFenstermacherLLNLNoBreakoutNoNo
2testing, please ignore!Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationCovielloGANoBreakoutNoNo
5210 CCOANB Counter-direction Checkout - Including Power and Ability to Balance TorqueHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)GriersonGANoBreakoutNoNo
7Checkout of 210 CCOANB Using Visible ImagingHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)Van ZeelandGANoBreakoutNoNo
8ECH Beat Wave Generation of ICETorkil JensenGriersonGANoGeneralNoNo
11Identification of Alfven instabilities driven by REs at negative Uloop during RE plateau stageDisruption Mitigation ThrustLvovskiyGANoBreakoutNoNo
14Comparison of dispersive vs non-dispersive shell pellet payloadDisruption Mitigation ThrustHollmannUCSDNoBreakoutNoNo
15Suppression of RE seeds with W grains in shell pelletDisruption Mitigation ThrustHollmannUCSDNoBreakoutNoNo
16Dynamic measurement of impurity transport into RE plateau using carbon depositionDisruption Mitigation ThrustHollmannUCSDNoBreakoutNoNo
17Change in RE plateau vertical loss rate with low-Z injectionDisruption Mitigation ThrustHollmannUCSDNoBreakoutNoNo
18Scan of RE plateau final loss footprint with I-coil perturbationDisruption Mitigation ThrustHollmannUCSDNoBreakoutNoNo
19Scan of RE plateau impurity assimilation with auxiliary heatingDisruption Mitigation ThrustHollmannUCSDNoBreakoutNoNo
20Ignition mechanism of arc by ELMsSurface EvolutionRohdeMax Planck Institut fuer Plasmaphysiks, Garching, GermanyNoGeneralNoNo
22Optimizing of q and fast-ion profiles in high-qmin scenarioSteady State Scenarios & High qmin ThrustThomeGANoBreakoutNoNo
26Determine the cause of RE beam final loss in post disruption vertical displacement eventsDisruption Mitigation ThrustBardocziGANoBreakoutNoYes
27Dependence of Ohmic energy confinement in negative triangularity diverted plasmasTurbulence and transportThomeGANoBreakoutNoNo
42Determine accuracy of NUBEAM power and torque outside mid-radiusEnergetic Particle PhysicsChrystalGANoBreakoutNoNo
43Low and mid-Z impurity density asymmetryTurbulence and transportChrystalGANoBreakoutNoNo
44Real time measurements of impurity densityControlChrystalGANoBreakoutNoNo
46Isotope mix effects (puffing He into H plasmas) on the L-H power thresholdIsotope mass ThrustYanU of WisconsinNoBreakoutNoNo
48Identify and control pedestal turbulence modes in ELMing H-mode plasmasPedestal Physics and Pedestal Structure & QH ThrustYanU of WisconsinNoBreakoutNoNo
56Hunt the instabilities responsible for the formation of phase space holeEnergetic Particle PhysicsDuGANoGeneralNoNo
57Assess robustness of ITER baseline plasma response controlInductive ScenariosHansonColumbia UNoBreakoutNoNo
66Impact of RMP on the L-H thresholdL-H transitionDialloPPPLNoBreakoutNoNo
67Unraveling the mechanism linking the pedestal structure and its dynamics to ELM energy densities in ITER relevant regimesPedestal Physics and Pedestal Structure & QH ThrustDialloPPPLNoBreakoutNoNo
71Role of scrape-off layer electric field in L-H power threshold scalingL-H transitionSchmitzUCLANoBreakoutNoNo
73Role of pre-disruption electron temperature in runaway electron seed formationDisruption Mitigation ThrustPaz-SoldanColumbia UNoBreakoutNoNo
75RMP-ELM Suppression and Mitigation in Hydrogen PlasmasIsotope Mass ThrustPaz-SoldanColumbia UNoBreakoutNoNo
77Direct comparison of ITER similar shape (ISS) and ITER baseline scenario (IBS) plasmas for RMP-ELMInductive ScenariosPaz-SoldanColumbia UNoBreakoutNoNo
79what are those modes observed in the wide-pedestal QH edge?Pedestal Physics and Pedestal Structure & QH ThrustChenGANoBreakoutNoNo
81Snowflake SAS divertorImpurity Radiative Divertor Dependence on Divertor ClosureSoukhanovskiiLLNLNoBreakoutNoNo
82Clarify key snowflake divertor physicsAdvanced Magnetic ConfigurationsSoukhanovskiiLLNLNoBreakoutNoNo
83Particle exhaust in snowflake divertorAdvanced Magnetic ConfigurationsSoukhanovskiiLLNLNoBreakoutNoNo
84Clarify snowflake divertor physicsAdvanced Magnetic ConfigurationsSoukhanovskiiLLNLNoBreakoutNoNo
85Can open horizontal plate divertor act as baffled vertical plate divertorImpurity Radiative Divertor Dependence on Divertor ClosureSoukhanovskiiLLNLNoBreakoutNoNo
88Exploring new reactor concepts: H-mode in negative triangularity diverted plasmasTurbulence and transportMarinoniUCSDNoBreakoutNoNo
95ELM-resolved D and D2 re-emission from C,W,and SiC: characterization by ro-vibrational spectroscopyInnovative Materials EvaluationBykovGANoBreakoutNoNo
103Comparison of high density ELM suppression in H and He to DIsotope Mass ThrustEvansGANoBreakoutNoYes
108Measure and control resistive kink mode stabilityPedestal Physics and Pedestal Structure & QH ThrustHansonColumbia UNoBreakoutNoNo
109Effects of the IPD on pedestal structure and edge fluctuations leading to ELM suppressed phasesPedestal Physics and Pedestal Structure & QH ThrustDialloPPPLNoBreakoutNoNo
115Role of fueling in determining the pedestal structureIsotope Mass ThrustMordijckThe college of William and MaryNoBreakoutYesYes
116Measuring Te-fluctuations within the pedestal of wide pedestal Quiescent H-mode plasmasPedestal Physics and Pedestal Structure & QH ThrustHoushmandyarGANoBreakoutNoNo
124Characterization of Fast-ion Diagnostic to Edge Neutral PopulationsEnergetic Particle PhysicsStagnerGANoBreakoutNoNo
138Physics of pedestal turbulence vs widthDiv/SOL Turbulence and transportBoedoUCSDNoBreakoutNoNo
139ITER pedestal turbulence propertiesTorkil JensenBoedoUCSDNoBreakoutNoNo
140Electron density up-down assymetryPedestal Physics and Pedestal Structure & QH ThrustMordijckThe college of William and MaryNoBreakoutNoNo
144Transport and turbulence in Divertor and pedestal during detachmentDiv/SOL Turbulence and transportBoedoUCSDNoBreakoutNoNo
145HFS Pellet Fueling Deposition Dynamics in H-mode PlasmasPedestal Physics and Pedestal Structure & QH ThrustBaylorORNLNoBreakoutNoNo
146Pellet Fueling of Wide Pedestal QH-mode PlasmasPedestal Physics and Pedestal Structure & QH ThrustBaylorORNLNoBreakoutNoNo
147Pellet Fueled High Density Operation of RMP ELM Mitigated PlasmasELM ControlBaylorORNLNoBreakoutNoNo
150Competition Between Intrinsic Torque and NTV for ITERRotation physicsGriersonGANoBreakoutNoNo
152Assessment of Ly-alpha opacity in fully detached divertor plasmasDissipative Divertor PhysicsGrothAalto UNoBreakoutNoNo
153Balancing the Tradeoffs Between High Performance and Core Purity & Stability in High Power HybridCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationGriersonGANoBreakoutNoNo
179Model validation of betaN > 3 in negative triangularity DIII-D dischargesTurbulence and transportAustinU of Texas, AustinNoBreakoutNoNo
180Transport vs rotation in DIII-D negative triangularity dischargesTurbulence and transportAustinU of Texas, AustinNoBreakoutNoNo
181ICE internal amplitude and radial structureEnergetic Particle PhysicsCrockerUCLANoBreakoutNoNo
182CAE suppression by more parallel injectionEnergetic Particle PhysicsCrockerUCLANoBreakoutNoNo
189Mitigation of AEs in high performance discharges using high off-axis current driveSteady State Scenarios & High qmin ThrustKramerPPPLNoBreakoutNoNo
190Impact of Current Condensation in the ECCD Stabilization of Rotating 2/1 NTMs3DSPBardocziGANoBreakoutNoNo
191What can lost fast-ions tell us about the H-mode pedestal?Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationKramerPPPLNoBreakoutNoNo
192m/n=2/1 NTM control by ECCD in IBS3DSPBardocziGANoBreakoutNoNo
193Impact of molecular processes on divertor detachment and validation of UEDGE fluid molecular modelDissipative Divertor PhysicsHolmPPPLNoBreakoutNoNo
194Comparing the transport models experimentallyTurbulence and transportKolemenPPPLNoBreakoutNoNo
196ELM cycle: induce at will and find the effect of edge current variation using burst CER/ThomsonPedestal Physics and Pedestal Structure & QH ThrustKolemenPPPLNoBreakoutNoNo
198Radial structure and identification of intermediate frequency Alfven eignemodesEnergetic Particle PhysicsCrockerUCLANoBreakoutNoNo
199Machine Learning based Instability Prediction & Avoidance3DSPKolemenPPPLNoBreakoutNoNo
201m/n=2/1 NTM control by ECCD in IBSControlBardocziGANoBreakoutNoNo
205RT stability analysis to find/avoid the instabilities with mhd calc. and feedback 3D spectroscopy3DSPKolemenPPPLNoBreakoutNoNo
206ECCD and ECH for IBS with real-time modulation control3DSPKolemenPPPLNoBreakoutNoNo
207Measure and Influence Flow with Pump and PumpCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationAllenLLNLNoBreakoutNoNo
210Puff and Pump Flow measurement in DN as a function of drsepAdvanced Magnetic ConfigurationsAllenLLNLNoBreakoutNoNo
212Minimize carbon in DIII-D AT plasmasCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationAllenLLNLNoBreakoutNoNo
213Search for SOL impurity stagnation regionSOL FlowsAllenLLNLNoBreakoutNoNo
217co-Ip QH-mode approach to super H-modeCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationChenGANoBreakoutNoNo
226Controlling ITB formation via impurity puffingDIII-D/EAST Task Force/ThrustMcClenaghanGANoBreakoutNoNo
229Measure and control resistive kink mode stabilityInductive ScenariosHansonColumbia UNoBreakoutNoNo
233Carbon flow in plasma crownSOL FlowsAllenLLNLNoBreakoutNoNo
234Search for Tungsten Accumulation in Upper divertorImpact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential ThrustAllenLLNLNoBreakoutNoNo
235Physics of real-time wall conditioning by B dust injectionMaterials Migration and MitigationBortolonPPPLNoBreakoutNoNo
236wide-pedestal QH in dominant electron-heated ITER PFPO hydrogen plasmasIsotope Mass ThrustChenGANoBreakoutNoNo
245Characterizing Detachment in H-mode Helium PlasmasIsotope mass ThrustSamuellLLNLNoBreakoutNoNo
247ExB drifts and paralel flows in divertor and SOL before/during detachmentSOL FlowsBoedoUCSDNoBreakoutNoNo
248Poloidal asymmetries of radial transport in the edge/SOLDiv/SOL Turbulence and transportBoedoUCSDNoBreakoutNoNo
249ExB drifts and paralel flows in divertor and SOL before/during detachmentSOL FlowsBoedoUCSDNoBreakoutNoNo
250Mitigate increased L-H transition threshold power in ITER PFPO hydrogen plasmas w/wo applied RMPIsotope mass ThrustSchmitzUCLANoBreakoutNoNo
251Methane Injection Changing D+ flows in SOLSOL FlowsBoedoUCSDNoBreakoutNoNo
252Effect of divertor radiation front on drifts and parallel flowDissipative Divertor PhysicsBoedoUCSDNoBreakoutNoNo
253Investigation and optimization of core and pedestal performanceCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationSolomonGANoBreakoutNoNo
258Deuterium lifecycle during ELM pacing with pellet injectionPedestal Physics and Pedestal Structure & QH ThrustBortolonPPPLNoBreakoutNoNo
259Divertor to pedestal trace impurity transportDiv/SOL Turbulence and transportBortolonPPPLNoBreakoutNoNo
262Divertor-localized turbulence and characterization of 2D profiles of divertor turbulenceDiv/SOL Turbulence and transportScottiLLNLNoBreakoutNoNo
263Impurity temperature screening in ITBsTurbulence and transportSciortinoMax-Planck Institute for Plasma PhysicsNoBreakoutNoNo
265High Pedestal in Hybrid Scenario With Unfavorable Grad-B Drift DirectionSteady State Scenarios & High qmin ThrustPettyGANoBreakoutNoNo
266Test of Turbulence Spreading Using Turbulence PropagationTurbulence and transportPettyGANoBreakoutNoNo
269Pushing Steady-State Hybrid Scenario to Lower q95, Higher Beta and Higher Fusion GainCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationPettyGANoBreakoutNoNo
270Evolution of edge turbulence and turbulence flow near midplane during divertor detachmentDiv/SOL Turbulence and transportWangUCLANoBreakoutNoNo
272High Density Electron Heating With O-ModeCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationPettyGANoBreakoutNoYes
273Scaling of blobby transport with divertor conditions and pedestal/SOL wideningDiv/SOL Turbulence and transportBoedoUCSDNoBreakoutNoNo
274edge/SOL turbulence with plasma isotopic mass scaling.Isotope mass ThrustBoedoUCSDNoBreakoutNoNo
275Divertor radiated power control in non-ELMing plasmasControlEldonGANoBreakoutNoNo
277Divertor radiated power control vs. ELM frequencyCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationEldonGANoBreakoutNoNo
278A Boron-Nitrogen radiative divertor for AT scenariosCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationBortolonPPPLNoBreakoutNoNo
279Isotope effect on the detachment rollover densityIsotope Mass ThrustSolokhaAalto UNoNoNo
287Validation of the NIMROD resultsPedestal Physics and Pedestal Structure & QH ThrustPankinPPPLNoBreakoutNoNo
288Exploration of IBS variation with direct gain metric regulationControlOlofssonConsultantNoBreakoutNoNo
289Shape control enabled study of IBS stability as function of edge featuresControlOlofssonConsultantNoBreakoutNoNo
297Identifying and Detecting Microtearing Modes within the Pedestal of an H-mode PlasmaPedestal Physics and Pedestal Structure & QH ThrustMajorU of WisconsinNoBreakoutNoNo
299Transient ExB flows caused by bursting fast-ion modes and secondary transport-related impactsEnergetic Particle PhysicsCrockerUCLANoBreakoutNoNo
302Measurement of EHO particle vs energy transport and phase angles with fluctuation diagnosticsPedestal Physics and Pedestal Structure & QH ThrustMortonU of WisconsinNoBreakoutNoNo
306Is krypton better than argon as a mantle seed in high power, high performance hybrid plasmas?Impurity Radiative Divertor Dependence on Divertor ClosureePetrieGANoBreakoutNoNo
307Two-impurity approach as an optimal radiating divertor solution for DIII-DImpurity Radiative Divertor Dependence on Divertor ClosureePetrieGANoBreakoutNoNo
310Two-impurity approach as an optimal radiating divertor solution for DIII-DImpurity Radiative Divertor Dependence on Divertor ClosureePetrieGANoBreakoutNoNo
314Voltage controlled SuperSpas for plasma shape controlControlHyattGANoBreakoutNoNo
315VFI-less Plasma operationsControlHyattGANoBreakoutNoNo
316A Boron-Nitrogen radiative divertor for AT scenariosCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationBortolonPPPLNoBreakoutNoNo
323Tune RMP Controlled Phase of Locked Island and Radial Alignment of ECCD Deposition for StabilizationControlReimanPPPLNoBreakoutNoNo
324Measurement of helicon wave internal amplitude and validation of simulationHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)CrockerUCLANoBreakoutNoNo
325Profile control for high qmin steady state scenarioControlWehnerLehighNoBreakoutNoNo
326Model-based rotation control developmentControlWehnerLehighNoBreakoutNoNo
334Negative Triangularity in H PlasmaIsotope Mass ThrustSmithGANoBreakoutNoNo
335High performance QH-mode in H plasma with pellet fuelingIsotope Mass ThrustSmithGANoBreakoutNoNo
336Pushing Steady-State Hybrid Scenario to Lower q95, Higher Beta and Higher Fusion GainSteady State Scenarios & High qmin ThrustPettyGANoBreakoutNoYes
337ECRH plasma production on DIII-DMaterials Migration and MitigationWautersLPP-ERM-KMS � Brussels � Belgium (EUROfusion member)NoBreakoutYesYes
338Combining variable beam energy/perveance and NTV for rotation controlControlBoyerPPPLNoBreakoutNoNo
339Detachment control w/ Te request translated to ne estimate & direct ne feedbackControlEldonGANoBreakoutNoNo
340Burn through of paced ELMs in detachmentCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationEldonGANoBreakoutNoNo
341Energy Confinement dependence on massIsotope mass ThrustThomeGANoBreakoutNoNo
342Vertical stability control with simulated horizontal interferometer channelsControlEldonGANoBreakoutNoNo
343Check for Te cliff at inner strike point in reverse BtDissipative Divertor PhysicsEldonGANoBreakoutNoNo
344Detachment onset density vs. 3D field strengthCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationEldonGANoBreakoutNoNo
345ECRH plasma production on DIII-DHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)WautersLPP-ERM-KMS � Brussels � Belgium (EUROfusion member)NoBreakoutYesYes
346Developing low-disruptivity ramp-down techniques for the ITER Baseline ScenarioControlBarrGANoBreakoutNoNo
347ITER plasma initiation and ECH assistControlWalkerGANoBreakoutYesYes
348Divertor configuration effects on the L-H power threshold in H plasmasIsotope mass ThrustYanU of WisconsinNoBreakoutNoNo
350isotope scaling with matched kinetic profilesIsotope Mass ThrustscottPPPLNoBreakoutNoNo
352Stationary Zonal FlowsL-H transitionBurrellGANoBreakoutNoNo
353Wide pedestal QH-mode operation at lower ZeffPedestal Physics and Pedestal Structure & QH ThrustBurrellGANoBreakoutNoNo
354Study of impurity ion entrainment in divertor cross-field transportDiv/SOL Turbulence and transportHollmannUCSDNoBreakoutNoNo
355High fusion gain in the advanced inductiveInductive ScenariosThomeGANoBreakoutNoNo
356ELM pacing by pellet injection in low-collisionality ITER relevant scenariosELM ControlBortolonPPPLNoBreakoutNoNo
357Power loading at toroidal PFC gapsIsotope Mass ThrustRudakovUCSDNoBreakoutYesYes
358Parallel correlation of turbulence/blobs between mid-plane and divertor SOLDiv/SOL Turbulence and transportRudakovUCSDNoBreakoutNoNo
360LH power threshold, confinement scaling and CER calibration in carbon plasmasL-H transitionMarinoniUCSDNoBreakoutNoNo
370Checkout 210 beamsHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)HeidbrinkUC, IrvineNoBreakoutNoNo
372whistler polarizationDisruption Mitigation ThrustHeidbrinkUC, IrvineNoBreakoutNoNo
374Effect on SEE on Langmuir probe measurements in the SOLDiv/SOL Turbulence and transportRudakovUCSDNoBreakoutNoNo
387Local Magnetic Field Measurements of QH-mode EHOPedestal Physics and Pedestal Structure & QH ThrustBurkeLLNLNoBreakoutNoNo
393ELM pacing by pellet injection in low-collisionality ITER relevant scenariosELM ControlBortolonPPPLNoBreakoutNoNo
394ELM pacing during ITER-like current ramp-up/downELM ControlBortolonPPPLNoBreakoutNoYes
395ELM pacing during ITER-like current ramp-up/downELM ControlBortolonPPPLNoBreakoutNoYes
397Establish ELM suppression in DND plasmaELM ControlLyonsGANoBreakoutNoNo
399Safety Factor Scaling of Turbulence and Transport in Hybrid Scenario PlasmasTurbulence and transportMcKeeU of WisconsinNoBreakoutNoNo
401Determine the critical gradient in negative triangularity dischargesTurbulence and transportAustinU of Texas, AustinNoBreakoutNoNo
403Burn Condition Emulation for ITER-relevant Control ExperimentsControlSchusterLehigh UNoBreakoutNoNo
406W-pellet injection to calibrate the DIII-D Collector ProbeMaterials Migration and MitigationStangebyU of TorontoNoBreakoutNoNo
407Divertor radiated power control vs. ELM frequencyELM ControlEldonGANoBreakoutNoNo
408Burn through of paced ELMs in detachmentELM ControlEldonGANoBreakoutNoNo
409Detachment/T_e cliff onset density vs. I_p using control to stay on the edge of the cliffCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationEldonGANoBreakoutNoNo
414Quasi-coherent fluctuations near the divertor plateDiv/SOL Turbulence and transportWangGANoBreakoutNoNo
419Commissioning of a proximity-to-stability-boundary control architecture for disruption preventionControlBarrGANoBreakoutNoNo
420Commissioning of a Vertical Control proximity-to-stability-boundary algorithm for VDE preventionControlBarrGANoBreakoutNoNo
421Magnetic shear at X-point and radial turbulence transportDiv/SOL Turbulence and transportBoedoUCSDNoBreakoutNoNo
422Increase "intrinsic" edge rotation via control of edge stochasticityRotation physicsSchmitzUCLANoBreakoutNoNo
429Real time neutron controlControlHeidbrinkUC, IrvineNoBreakoutNoNo
431Profile control for high qmin steady state scenarioSteady State Scenarios & High qmin ThrustWehnerLehighNoBreakoutNoNo
432Profile control for high qmin steady state scenarioSteady State Scenarios & High qmin ThrustWehnerLehighNoBreakoutNoNo
433Profile control for high qmin steady state scenarioSteady State Scenarios & High qmin ThrustWehnerLehighNoBreakoutNoNo
434Effect of main ion SOL flows on W impurity transportImpact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential ThrustRudakovUCSDNoBreakoutNoNo
437Optimizing the pumping geometry for SAS2Particle Balance and Impact of Divertor Closure Including SAS on Detachment ThrustCanikORNLNoBreakoutNoNo
438Effect of in-divertor gas puff location in SASParticle Balance and Impact of Divertor Closure Including SAS on Detachment ThrustMoserGANoBreakoutNoNo
440Optimizing SOL width in closed divertor for particle control and detachmentParticle Balance and Impact of Divertor Closure Including SAS on Detachment ThrustMoserGANoBreakoutNoNo
441How does SAS performance depend on enclosed poloidal flux?Particle Balance and Impact of Divertor Closure Including SAS on Detachment ThrustThomasGANoBreakoutNoNo
442Access to small ELM regime in DIII-D high �²P scenarioDIII-D/EAST Task Force/ThrustQianASIPPNoBreakoutYesYes
446Pedestal structure in hydrogen-1 plasmas relevant for non-nuclear Iter and access to ELM suppressionIsotope mass ThrustLaggnerNorth Carolina StateNoBreakoutNoNo
447Optimizing Transport Through Magnetic ShearSteady State Scenarios & High qmin ThrustMcKeeU of WisconsinNoBreakoutNoNo
448Optimizing core-pedestal performance in Super H-ModeCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationSnyderORNLNoBreakoutNoNo
449m/n=2/1 NTM control by ECCD in steady state hybridSteady State Scenarios & High qmin ThrustBardocziGANoBreakoutNoNo
456Stabilization of TAEs by Localized Electron Cyclotron Current DriveEnergetic Particle PhysicsSharapovCCFENoBreakoutYesNo
457m/n=2/1 NTM control by ECCD in steady state hybrid3DSPBardocziGANoBreakoutNoNo
458m/n=2/1 NTM control by ECCD in steady state hybridControlBardocziGANoBreakoutNoNo
459Use pellets to lower the ECCD requirement for 2/1 NTM stabilization3DSPBardocziGANoBreakoutNoNo
460Use pellets to enable 2/1 NTM stabilization with very low gyrotron powerTorkil JensenBardocziGANoBreakoutNoNo
461Pedestal and core transport comparison of SAS , upper closed, and lower open divertorParticle Balance and Impact of Divertor Closure Including SAS on Detachment ThrustOsborneGANoBreakoutNoNo
462Pedestal pressure enhancement at high density through decoupling of ped peeling and ballooning modesCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationOsborneGANoBreakoutNoNo
463QH-mode with detached divertorParticle Balance and Impact of Divertor Closure Including SAS on Detachment ThrustOsborneGANoBreakoutNoNo
464Effect of impurities on pedestal structure in Peeling and Ballooning dominate discharges.Pedestal Physics and Pedestal Structure & QH ThrustOsborneGANoBreakoutNoNo
471experimental demonstration both down-shift and up-shift top launch ECCD schemesHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)ChenGANoBreakoutNoNo
472polarization study of top launchHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)ChenGANoBreakoutNoNo
473Evaluating the internal MHD response to shell pellet injectionDisruption Mitigation ThrustPandyaU of WisconsinNoBreakoutNoNo
474Evaluating the internal MHD response to SPIDisruption Mitigation ThrustPandyaU of WisconsinNoBreakoutNoNo
475Measuring internal MHD during the formation and evolution of a runaway electron beamDisruption Mitigation ThrustPandyaU of WisconsinNoBreakoutNoNo
476Pedestal dimensionless parameter match DIII-D to JET for H,D,HeIsotope Mass ThrustOsborneGANoBreakoutNoNo
479ITG and TEM's impacts on toroidal rotation profile and intrinsic rotationRotation physicsQinU of WisconsinNoBreakoutNoNo
484- Feasibility of plasma performance and stability of ITER steady-state operation with NB+EC CDSteady State Scenarios & High qmin ThrustPolevoiITER OrganizationNoBreakoutNoYes
485Third harmonic ECH experimentsHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)SchneiderITER OrganizationNoBreakoutNoNo
486Helicon Modulation and Shutdown CheckoutHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)BrookmanGANoBreakoutNoNo
488Steady-State Hybrids in Hydrogen With Higher Bootstrap FractionSteady State Scenarios & High qmin ThrustPettyGANoBreakoutNoNo
489Developing low-disruptivity ramp-down techniques for the ITER Baseline ScenarioInductive ScenariosBarrGANoBreakoutNoNo
490BAAE and BAE validationEnergetic Particle PhysicsHeidbrinkUC, IrvineNoBreakoutYesNo
491Spectroscopic inference of tungsten re-deposition fractionsSurface EvolutionAbramsGANoBreakoutNoNo
496Orbit Tomography (OT)Energetic Particle PhysicsGarciaUC, IrvineNoBreakoutYesNo
498Measurement of NBCD profileHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)PettyGANoBreakoutNoNo
501Modification of AE Drive and Nonlinear Saturation Through Variation of Beam ModulationEnergetic Particle PhysicsVan ZeelandGANoBreakoutYesNo
503Impact of large area electrical biasing on material erosion and divertor leakage in SAS1-WImpact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential ThrustRenU of Tennessee, KnoxvilleNoBreakoutNoNo
504Helicon Launcher Checkout and ConditioningHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)ZhangASIPPNoBreakoutNoNo
505Assessing Helicon wave current drive in high betap experimentsDIII-D/EAST Task Force/ThrustZhangASIPPNoBreakoutNoNo
506PCS supervisory algorithm for negotiating complex controller requestsControlEidietisGANoBreakoutNoNo
507ITER DMS design validationDisruption Mitigation ThrustLehnenITER OrganizationNoBreakoutNoNo
509Exposure of Graphitic foam at DiMES and TileInnovative Materials EvaluationUnterbergORNLNoBreakoutNoNo
510Superposition of identical dual SPIsDisruption Mitigation ThrustHerfindalORNLNoBreakoutNoNo
511Feedback control for divertor impurity seeding based on Surface Eroding ThermocoupleControlRenU of Tennessee, KnoxvilleNoBreakoutNoNo
515Parameter scan of fast-ion critical gradient thresholdEnergetic Particle PhysicsCollinsORNLNoBreakoutNoNo
517Penetration characterization of small pellet injection into D3D plasmasDisruption Mitigation ThrustRamanU of WashingtonNoBreakoutNoNo
518Dimensionless scaling of pedestal height, width and stability - a turbulence & transport perspectivePedestal Physics and Pedestal Structure & QH ThrustBanerjeePPPLNoBreakoutNoNo
521ECCD and ECH for IBS with real-time modulation controlControlKolemenPPPLNoBreakoutNoNo
522RT stability analysis to find/avoid the instabilities with mhd calc. and feedback 3D spectroscopyControlKolemenPPPLNoBreakoutNoNo
523Test the new method for finding the 3D perturbation needed to avoid tearingControlKolemenPPPLNoBreakoutNoNo
524Control of pressure/current profile transport models experimentallyControlKolemenPPPLNoBreakoutNoNo
525Mass scaling of shell pellet assimilationDisruption Mitigation ThrustEidietisGANoBreakoutNoNo
526Full profile measurement of shell Te profileDisruption Mitigation ThrustEidietisGANoBreakoutNoNo
527Test Li coating for "ideal" shell pelletDisruption Mitigation ThrustEidietisGANoBreakoutNoNo
528Ablation measurments of single snall Ne pelletDisruption Mitigation ThrustEidietisGANoBreakoutNoNo
529Effect of D admixture in SPIDisruption Mitigation ThrustEidietisGANoBreakoutNoNo
530dilution cooling in SPI superpositionDisruption Mitigation ThrustEidietisGANoBreakoutNoNo
531Scaling of fragment penetration depth with energy:Disruption Mitigation ThrustEidietisGANoBreakoutNoNo
532JET SPI similarity experimentsDisruption Mitigation ThrustEidietisGANoBreakoutNoNo
533Ballistic transport and energy/size scaling for SPIDisruption Mitigation ThrustShirakiORNLNoBreakoutNoNo
536Helium scenarios for ITERIsotope mass ThrustMarinoniUCSDNoBreakoutYesNo
537ELM pacing during ITER-like current ramp-up/downELM ControlBortolonPPPLNoBreakoutNoYes
538Expanding the Wide Pedestal QH to IBS ParametersInductive ScenariosChenGANoBreakoutNoNo
539Effect of underlying non-axisymmetric (NA) fields on disruption mitigation processDisruption Mitigation ThrustEidietisGANoBreakoutNoNo
542LH power threshold, confinement scaling and CER calibration in carbon plasmasTorkil JensenMarinoniUCSDNoBreakoutNoNo
546Direct measurement of the wave-particle interactions and associated phase space flowEnergetic Particle PhysicsDuGANoBreakoutNoNo
547Direct measurement of the wave-particle interactions and associated phase space flowEnergetic Particle PhysicsduGeneral AtomicNoBreakoutNoNo
548Effect of outer gap on wide-pedestal QH-modePedestal Physics and Pedestal Structure & QH ThrustGarofaloGANoBreakoutNoNo
549Further investigation of the saturation & underlying transport mechanism of EHO to allow ELM stablePedestal Physics and Pedestal Structure & QH ThrustChenGANoBreakoutNoNo
550What's the physics leads to std QH, Wide Pedestal QH,or ELMing IBS from L-mode at low torque?Pedestal Physics and Pedestal Structure & QH ThrustChenGANoBreakoutNoNo
551What's the physics leads to std QH, Wide Pedestal QH,or ELMing IBS from L-mode at low torque?L-H transitionChenGANoBreakoutNoNo
552Parametric instabilities during Helicon wave Iinjection in DIII-DHeating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)PorkolabMassachusetts Institute of TechnologyNoBreakoutNoNo
554ELM pacing during ITER-like current ramp-up/downELM ControlBortolonPPPLNoBreakoutNoYes
555Toroidal symmetry of SAS tilesImpact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential ThrustBykovGANoBreakoutNoNo
556168: Extend Zero Torque Wide Pedestal QH-Mode Operation to IBS ParametersPedestal Physics and Pedestal Structure & QH ThrustErnstMassachusetts Institute of TechnologyNoBreakoutNoNo
557RMP ELM suppression in the SAS shapeImpact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential ThrustEvansGANoBreakoutNoNo
558High-Z impurity pump-out mechanism inside of MHD modes in plasma with divertor W sourceImpact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential ThrustOdstrcilGANoBreakoutNoNo
560Using the SAS to control impurity pinchImpact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential ThrustNelsonColumbia UNoGeneralNoNo
561Experimental Validation of Heteroclitic magnetic Island Bifurcations in DIII-DGeneral PhysicsEvansGANoBreakoutNoNo
562Minimizing W divertor leakage in the SASImpact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential ThrustUnterbergORNLNoBreakoutNoNo
563Probe RWM stability using off-axis NBISteady State Scenarios & High qmin ThrustHansonColumbia UNoBreakoutNoNo
564Impact of high-Z PFCs on impurity seeding experiments in SASImpact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential ThrustCasaliU of Tennessee, KnoxvilleNoBreakoutNoNo
565Measure lambda-q during rotation scans at constant heating power in super H mode plasmasCore-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario OptimizationGarofaloGANoBreakoutNoNo