DIII-D RESEARCH OPPORTUNITIES FORUM FOR THE 2014 EXPERIMENTAL CAMPAIGN Review | Direct submission with log-in | Request submission without log-in

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(Proposal numbers 1-382 are from 2013)
ID Title Research Area Name Affiliation Time
Req'ed
ITPA
Joint Exp
ITER IO Urgent
Research Task
1C vs I Coil NTVPlasma RotationGANoNoNo
2Hysteresis and Turbulence Spreading in the H-L Back TransitionL-H TransitionUCLANoNoNo
3The effect of LSN Shape on the q95 windows in RMP ELM SuppressionELM ControlGANoNoYes
4Turbulence and Intrinsic RotationPlasma RotationGANoNoNo
5Measure Intrinsic Rotation Size scaling in DIII-D alone -IIPlasma RotationGANoNoNo
6Prompt torque and zonal flow dampingPlasma RotationGANoNoNo
7Investigate angular momentum diffusion and pinch using off-axis torquePlasma RotationGANoNoNo
8Compare Mach probe and CER measurements of intrinsic rotation profile of main ions in helium plasmaPlasma RotationGANoNoNo
9Test of Neoclassical Toroidal Viscosity theory using modulated I-coil currentsPlasma RotationGANoNoNo
10Maintain low-rotation QH-mode with ECH onlyInductive ScenariosGANoNoNo
11Investigate in-out density asymmetry at large toroidal rotationPlasma RotationGANoNoNo
12Diagnostic spatial cross calibration using edge sweeps in QH-modePedestal StructureGANoNoNo
13Compare edge particle transport in ELMing H-mode and QH-mode with and without NRMFInductive ScenariosGANoNoNo
14Control of toroidal mode number of EHOInductive ScenariosGANoNoNo
15Edge rotation shear threshold for QH-mode accessInductive ScenariosGANoNoNo
16Further development of QH-mode with strong co-Ip NBI torqueInductive ScenariosGANoNoNo
173-D Fields and ECH Density PumpoutTurbulence & TransportGANoNoNo
18High Collisionless NBI Torque Drive for GAMs, aka the VH-mode path?Turbulence & TransportGANoNoNo
19Effect of n=1 applied and error fields on n=3 RMP ELM suppressionELM ControlGANoNoNo
20L-H transition Trigger Physics/ Main Ion Momentum BalanceL-H TransitionUCLANoNoNo
21Magnitude of cross-field drifts in the Private Flux Region, divertor asymmetries and detachmentDivertor & SOL PhysicsAalto UNoNoNo
22Assessment of main chamber carbon sourcesDivertor & SOL PhysicsAalto UNoNoNo
23RMP ELM Suppression at q95 above 4ELM ControlGANoNoNo
25Transport mechanisms induced by RMPELM ControlUCSDNoNoYes
26Investigate the role of RS on inward momentum transportTurbulence & TransportUCSDNoNoNo
27COupling between core and SOL parallel flowDivertor & SOL PhysicsUCSDNoNoNo
28Role of profile evolution and energy transfer in L-H transitionL-H TransitionUCSDNoNoNo
29Modulation of Bootstrap CurrentELM ControlGANoNoNo
30New Optimal Plasma Shape for AT Scenario?Steady State Heating and Current DriveGANoNoNo
31Test of Turbulence Spreading Using Turbulence PropagationTurbulence & TransportGANoNoNo
32High Beta Hybrids and Pressure Profile BroadeningSteady State Heating and Current DriveGANoNoNo
33High Beta, Steady State HybridsSteady State Heating and Current DriveGANoNoNo
34Electron Critical Gradient and Heat PinchTurbulence & TransportGANoNoNo
35Non-Diffusive Heat Fluxes in the Edge "Shortfall" RegionTurbulence & TransportGANoNoNo
36Natural ELM Pacing in High-Beta, Steady-State PlasmasSteady State Heating and Current DriveGANoNoNo
38Calibrated passive FIDA spectrumEnergetic ParticlesUC, IrvineNoNoNo
39Measure and understand energetic particle profiles in steady-state plasmasSteady State Heating and Current DriveUC, IrvineNoNoNo
40MGI with applied n=1 RMP fieldsDisruption MitigationFiat Lux LLCNoNoNo
41Investigation of the effects of the EHO toroidal mode number on the edge particle transportInductive ScenariosPPPLNoNoNo
42Compatibility of High Performance Plasmas With a Puff-and-Pump Radiating DivertorSteady State Heating and Current DriveGANoNoNo
43Density Control and Active Impurity Removal from Double-null H-mode PlasmasDivertor & SOL PhysicsGANoNoNo
44Can Nitrogen impurity Seeding Improve Radiating Divertor Performance?Divertor & SOL PhysicsGANoNoNo
45Differences in Impurity Accumulation Between Resonant and Non-resonant RMP PlasmasELM ControlGANoNoNo
46Does Added Baffling From Re-Configured Tiles on the Lower Divertor Shelf Facilitate Detachment?Divertor & SOL PhysicsGANoNoNo
47Quantifying the TBM torque, both in magnitude and radial locationPlasma RotationVTT Technical Research CentreNoNoNo
48Dependence of momentum transport and intrinsic torque on rho* and betaPlasma RotationVTT Technical Research CentreNoYesNo
49Turbulent transport in detached divertorDivertor & SOL PhysicsUCSDNoNoYes
51Study of chirping Alfvén eigenmodes in DIII-DEnergetic ParticlesPPPLNoYesNo
52Control of TAE/RSAE modes via external perturbationsEnergetic ParticlesPPPLNoNoNo
53QH-mode with low torque start-upInductive ScenariosGANoNoNo
55RMP Elm Suppression in DN PlasmasELM ControlORNLNoNoNo
56Sawtooth ControlPlasma ControlORNLNoNoNo
59Effect of Changing the Grad-B Drift Direction on Snowflake Divertor Behavior, Including DetachmentDivertor & SOL PhysicsGANoNoNo
60Effective NTM control in low torque plasmasStability & Disruption AvoidanceGANoNoNo
714. ELM Characterization to Validate BOUT++ ELM SimulationsPedestal StructureLLNLNoNoNo
81Active Particle Exhaust of H-mode Plasmas in the Snowflake-minus Divertor ConfigurationDivertor & SOL PhysicsGANoNoNo
82IR Imaging of I-coil Induced Fast Ion LossesEnergetic ParticlesGANoYesNo
86Safety Factor Scaling of Turbulence and Transport in Hybrid Scenario PlasmasTurbulence & TransportU of WisconsinNoNoNo
90Carbon-13 in He Plasma erosion/deposition experiment to benchmark DIVIMP code being used by ITERPlasma-material InterfaceCommonwealth Fusion SystemsNoNoNo
94Turbulence Structure and Amplitude Variation with ExB Shear in H-mode PlasmasTurbulence & TransportU of WisconsinNoNoNo
95Experimental Validation of a Revised PCS Error Field CategoryPlasma ControlDepartment of EnergyNoNoNo
96Effect of Error Field Control Currents on Strike Point SplittingStability & Disruption AvoidanceDepartment of EnergyNoNoNo
115QH-mode at low co-Ip torque using n=2 NRMFInductive ScenariosGANoNoNo
120Optimizing non-resonant, nonaxisymmetric fields in QH-modeInductive ScenariosGANoNoNo
123Bid farewell to locked modes - NTM-locking avoidance by feedback synchronization assisted with ECCDStability & Disruption AvoidancePPPLNoNoNo
124Electron Energy Transport during q0 control using modulated EC powerInductive ScenariosORNLNoNoNo
125Observation of non-linear interactions in fast-ion loss spectraEnergetic ParticlesPPPLNoNoNo
128Carbon-13 in He Plasma erosion/deposition experiment to benchmark DIVIMP code being used by ITERPlasma-material InterfaceCommonwealth Fusion SystemsNoNoNo
130Synergy between core-localized Alfven eigenmodes and edge localized TBM fields on fast ion losses.Energetic ParticlesPPPLNoYesNo
132Dissipation & Control of RE from ITER-like LSN targetsDisruption MitigationGANoNoYes
135Measurement of RE diffusion to center postDisruption MitigationUCSDNoNoYes
136Disruption main chamber heat loadsDisruption MitigationUCSDNoYesYes
138SSI target improvement by minimizing global low-n MHD activity in 1.5 Steady State Heating and Current DrivePPPLNoNoNo
139TQ radiation distribution from R-2 MGIDisruption MitigationUCSDNoNoYes
140q0 control with Counter-ECCD in ITER Baseline DischargesInductive ScenariosRetiredNoNoNo
141Studies of RE final lossDisruption MitigationUCSDNoNoYes
145Explore RMP ELM suppression mechanism at moderate collisionalityELM ControlUCSDNoNoNo
149Measurement of ion temperatures in the divertor region of DIII-D using the DiMES platformDivertor & SOL PhysicsU of Tennessee, KnoxvilleNoNoNo
150Sensitivity study of toroidally-asymmetric halo current to error field during VDEDisruption MitigationPPPLNoNoNo
151ITER SS Demo Discharge DocumentationsSteady State Heating and Current DriveRetiredNoNoNo
152Transport shortfall at high gyrobohm fluxTurbulence & TransportGANoNoNo
154High frequency pellet ELM pacingELM ControlORNLNoYesYes
155Investigation of pellet induced ELM heat flux footprint variation with q95ELM ControlORNLNoNoYes
157Imaging of pellet induced ELM events from mulitple simultaneous views.ELM ControlORNLNoNoYes
158Expand the high li, betaN >4 operating regime through instability avoidance and higher heating powerSteady State Heating and Current DriveGANoNoNo
160Dependence of confinement and stability on toroidal rotation in high li dischargesSteady State Heating and Current DriveGANoNoNo
161n=3 offset and ELM suppression with RMPELM ControlGANoNoYes
162210RT MSE and low rotation, elevated q_min steady-state scenario discharges at high betaNSteady State Heating and Current DriveGANoNoNo
164Produce fNI = 1 discharges at q_min near 1.5 using off-axis injection and a model guided approachSteady State Heating and Current DriveGANoNoNo
165D2 + few % Ne shattered pellets for disruption mitigationDisruption MitigationORNLNoNoYes
166Effect of q95 on SPI shutdownDisruption MitigationORNLNoNoYes
167Control of radiation asymmetries by application of external field on SPI/MGI shutdownDisruption MitigationORNLNoNoYes
168Influence of the delay time between multiple massive gas injections at different toroidal locationsDisruption MitigationORNLNoNoYes
169Runaway flattop mitigation by Neon shattered pellet injectionDisruption MitigationORNLNoNoYes
170Nature of Energy Released During H-L Back TransitionL-H TransitionGANoNoNo
171Test of the argon pellet injectorDisruption MitigationORNLNoNoYes
172High betaN with off-axis injection at reduced Bt (if 2011-level beam power is available)Steady State Heating and Current DriveGANoNoNo
173Confinement and fast ion diffusion in high betaN, steady-state scenario dischargesSteady State Heating and Current DriveGANoNoNo
174Exploration of DEFC in the feedback stabilized plasma in low-q dischargesStability & Disruption AvoidancePPPLNoNoNo
175Beta collapse avoidance in SSI discharges by de-synchronizing toroidal harmonics by using feedbackSteady State Heating and Current DrivePPPLNoNoNo
176Beta collapse avoidance in SSI discharges by de-synchronizing toroidal harmonics by using feedbackSteady State Heating and Current DrivePPPLNoNoNo
178Beta limit and bootstrap current fraction in ITER steady-state scenario dischargesSteady State Heating and Current DriveGANoNoNo
179Snowflake in AT PlasmaSteady State Heating and Current DriveLLNLNoNoNo
180Establish the incremental confinement of EC power in high betaN steady-state scenario dischargesSteady State Heating and Current DriveGANoNoNo
181Heat pulse propagation in a perturbed magnetic topologyELM ControlGANoYesYes
182Systematic test of paleoclassical transportTurbulence & TransportGANoNoNo
184Comparision DIII-D and AUG high collisionality ELM response to 3D magnetic perturbationsELM ControlGANoYesYes
188Extension of proxy error field experiments to H-mode plasmasStability & Disruption AvoidanceColumbia UNoNoNo
189Measurement of optimal n=2 phasing for RMP & ELM suppression without q95 windowsELM ControlColumbia UNoNoNo
190Measurement of n=3 error field effects in RMP phase-flip experimentsELM ControlColumbia UNoNoNo
192Measurement of heat flux on the divertor using the embedded thermocouple arrayDivertor & SOL PhysicsU of Tennessee, KnoxvilleNoNoNo
194Correlation of confinement and fluctuations with electron heating in ITER Baseline ScenarioInductive ScenariosGANoNoNo
195Correlation of confinement and fluctuations with electron heating in ITER Baseline ScenarioTurbulence & TransportGANoNoNo
204Suppression of Density Limit Disruptions with RMP FieldsTorkil Jensen AwardGANoNoYes
205SOL width in top-limited dischargesDivertor & SOL PhysicsUCSDNoNoYes
206Studies of arcing on divertor PFC surfacesPlasma-material InterfaceUCSDNoNoNo
207Dust generation from deposited layers and leading edgesPlasma-material InterfaceUCSDNoNoNo
210The Dependence of Poloidal Rotation on TurbulencePlasma RotationGANoNoNo
215Control of tungsten PFC erosion by local gas injectionPlasma-material InterfaceUCSDNoNoNo
219Establishing an experimental basis for plasma effects on magnetic islandsELM ControlGANoNoNo
220Comparison of n=2 RMP field effects on ELMs and pedestal properties in KSTAR and DIII-DELM ControlGANoYesYes
231Stabilization of NTMs with ECCDStability & Disruption AvoidanceQSTNoYesNo
233C erosion and D up-take at high surface temperaturePlasma-material InterfaceGANoNoNo
234Study fishbone-like instability at the edge of QH-modesInductive ScenariosInstituto Superior Tecnico, Lisboa, PortugalNoNoNo
235High resolution Te pedestal measurements in RMP ELM suppression experimentsELM ControlSandia National LabNoNoNo
236Wavenumber dependence of turbulence suppression in the L-H transitionL-H TransitionUCLANoNoNo
241C-13 and background carbonPlasma-material InterfaceGANoNoNo
242q95 < 2 Tokamak Operation Via Dynamic Error Field CorrectionStability & Disruption AvoidanceGANoNoNo
243256: SOL width and divertor peak heat flux in QH-mode plasmas with/without n=3 fieldsInductive ScenariosGANoNoNo
244Study NRMF driven torque in ECH-only heated plasma (ELMing H-modes)Plasma RotationGANoNoNo
245Investigate the physics of NTM suppression by large externally applied helical fieldsTorkil Jensen AwardGANoNoNo
246Develop low-torque, high normalized fusion performance QH-mode for ITER baseline scenarioInductive ScenariosGANoNoNo
247Develop low-torque, high normalized fusion performance QH-mode for FNSF-AT scenarioInductive ScenariosGANoNoNo
248Investigate elongation limit in low li discharges with/without applied 3D magnetic fieldsTorkil Jensen AwardGANoNoNo
249Steady-state high beta with NCS and qmin>2Steady State Heating and Current DriveGANoNoNo
250Plateau Ecrit with MGIDisruption MitigationGANoYesYes
251New Study of Alfven Eigenmodes Induced Fast Ion Transport/LossEnergetic ParticlesGANoNoNo
252Implement finite-state Off Normal Fault Response systemPlasma ControlGANoNoNo
253Study QH-mode with advanced fast ion diagnostics and codesInductive ScenariosGANoNoNo
254Neon SPI injection into early CQ to stunt RE formationDisruption MitigationGANoNoNo
256Fine scale stepwise q-scan: role of low-order rationales and resonance condition for ELM suppressionELM ControlU of WisconsinNoNoNo
257Transport Investigation During Slow Current Ramp-Up and Ramp-Down [for ITER]Inductive ScenariosU of WisconsinNoYesNo
258Main-ion and impurity rotation in helium plasmasPlasma RotationGANoNoNo
259Helium Campaign (D beams)General PhysicsGANoNoNo
260ITER Baseline Scenario DemonstrationInductive ScenariosITER OrganizationNoYesNo
261Demonstration of stationary inductive solutions at low and moderate q95Inductive ScenariosITER OrganizationNoNoNo
262Test Pedestal Structure Model Where Paleoclassical Transport Is DominantPedestal StructureU of WisconsinNoNoNo
263Radiative divertor solutions in the ITER baseline scenarioInductive ScenariosITER OrganizationNoYesYes
264Radiative divertor solutions in the ITER baseline scenarioDivertor & SOL PhysicsITER OrganizationNoYesYes
265o Experiments using the centerpost Swing-probesDivertor & SOL PhysicsUCSDNoNoNo
266Understand resistive wall mode control physics in low-q95 plasmasInductive ScenariosColumbia UNoNoNo
267Understand and control resistive wall mode stability in high-qmin plasmasSteady State Heating and Current DriveColumbia UNoNoNo
268nu* dimensionless scalingTurbulence & TransportCEANoYesNo
278Possibility of â??Off-axis-Fishbone Mode and ELM Pacingâ?? due to Direct Energetic Particle CouplingELM ControlJAEANoNoNo
280: Trigger-less onset of NTMs with PEC and NTV effects on rotation regimePlasma RotationIstituto di Fisica del Plasma, Euratom-ENEA-CNRNoNoNo
283ITER Baseline Scenario Operation near the LH ThresholdInductive ScenariosITER OrganizationNoYesNo
284Access conditions for steady-state operation in ITERSteady State Heating and Current DriveITER OrganizationNoYesNo
285Access to advanced inductive operation in ITERInductive ScenariosITER OrganizationNoYesNo
286Collisionality scaling of confinement in advanced inductive regimesInductive ScenariosITER OrganizationNoYesNo
287High li steady-state scenario developmentSteady State Heating and Current DriveITER OrganizationNoNoNo
288Amplifying the Geodesic Acoustic Mode via Resonant Radial Field Amplification: New MethodsTurbulence & TransportU of WisconsinNoNoNo
289Demonstrate access to beta_N=5 with min(q)>2Steady State Heating and Current DriveITER OrganizationNoNoNo
290Effect of n=2 Poloidal Spectrum on NTV TorquePlasma RotationDepartment of EnergyNoNoNo
291Trigger-less onset of NTMs with P_EC and NTV effects on rotation regimeStability & Disruption AvoidanceInstituto Superior Tecnico, Lisboa, PortugalNoNoNo
292Optimize electron pedestal pressure in low-torque ITER baseline plasmasInductive ScenariosUCLANoNoNo
293Test of ETG zeff supressionTurbulence & TransportGANoNoNo
294Simulated Alpha particle dillutionTurbulence & TransportGANoNoNo
295preliminary simulated burn controlTurbulence & TransportGANoNoNo
297ITER baseline scenario with low NBI torqueInductive ScenariosGANoNoNo
298Soft landing with 2/1 TM in the ITER shapeStability & Disruption AvoidanceGANoNoNo
299Aspect ratio scaling of turbulence and transport: DIII-D and NSTX-U comparisonTurbulence & TransportUniv. Wisconsin (at PPPL)NoNoNo
300Effect of triangularity in ITER shape and improved shapingInductive ScenariosGANoNoNo
302RMP ELM Suppression at the NTV Offset RotationELM ControlGANoNoNo
303Effect on lithium wall conditioning for Co-QH-mode and edge pedestal characteristicsInductive ScenariosGANoNoNo
304Birth of ITER: the world's largest resistorGeneral PhysicsGANoNoNo
305Scaling Of Pedestal Plasma Transport With RMP I-coil CurrentELM ControlU of WisconsinNoNoNo
306Edge turbulence and blob generationDivertor & SOL PhysicsUniv. WisconsinNoNoNo
307Role of turbulent-driven and Ion pressure gradient-sustained ExB flows in Triggering H-modeL-H TransitionUCSDNoNoNo
308RMP (Resonant Magnetic Perturbation) code validation via UCLA 288 GHz polarimeterELM ControlUCLANoNoNo
309Full 3D Rotation optimization of H modeStability & Disruption AvoidanceGANoYesYes
310Energy Transport During Electron-Dominated Heating of ITER-Relevant H-Mode DischargesSteady State Heating and Current DrivePPPLNoNoNo
311Transport with qmin>2Steady State Heating and Current DriveLLNLNoNoNo
312Limits to pedestal radiation high beta dischargesSteady State Heating and Current DriveGANoNoNo
313Hybrids with co-NBI QH-mode edgeInductive ScenariosGANoNoNo
314Optimization of castellation for a new W-divertor of ITER: studies of shaped castellation in DIII-DPlasma-material InterfaceUCSDNoYesYes
315Current profile control model requirementsPlasma ControlGANoNoNo
316Model-based control of the current profile and βN for steady state scenariosPlasma ControlCadaracheNoNoNo
317Study on sawteeth in the neutral beam (NB) heated plasmasStability & Disruption AvoidanceKorea National Fusion Research CenterNoNoNo
318Current profile control for stable ITER baseline scenario plasmasInductive ScenariosColumbia UNoNoNo
319Impact of fast-ions on the RWM stability boundaryGeneral PhysicsColumbia UNoNoNo
320RWM excitation in the SSI target by reducing triangularity"Stability & Disruption AvoidancePPPLNoNoNo
321Access to low torque QH-mode using high beta low torque AI target with NRMFInductive ScenariosGANoNoNo
322ELM pacing in low torque, electron heated ITER baselineInductive ScenariosGANoNoNo
323Access to QH-mode with low NBI torqueInductive ScenariosGANoNoNo
324Document turbulence change with rotation in AI, and compare with theoryInductive ScenariosGANoNoNo
325Document turbulence change with rotation in AI, and compare with theoryTurbulence & TransportGANoNoNo
326Understand mechanisms by which ECH influences NTM stablilityStability & Disruption AvoidanceGANoNoNo
327rho* scaling of intrinsic torque between DIII-D and JETPlasma RotationGANoYesNo
328Error field correction at low rotationStability & Disruption AvoidanceGANoNoNo
329Discussion of plasma rotation transient process during OFM/ELM-driven RWM w/wo feedback usinStability & Disruption AvoidancePPPLNoNoNo
330QH-mode with TBMInductive ScenariosGANoNoNo
331QH-mode with TBM (dup 330)Stability & Disruption AvoidanceGANoNoNo
332Demonstration of noninductive Q=5 scenario in ITER shape using off-axis NBISteady State Heating and Current DriveORNLNoNoNo
333Far off-axis NBCDSteady State Heating and Current DriveORNLNoNoNo
334Measurement of neoclassical response of off-axis beam ionsSteady State Heating and Current DriveORNLNoNoNo
335Off-axis NBCD measurement in steady state scenarioSteady State Heating and Current DriveORNLNoNoNo
336Routine current profile control in operationSteady State Heating and Current DriveGANoNoNo
337Routine current profile control in operationInductive ScenariosGANoNoNo
338Local correction of the TBM error fieldStability & Disruption AvoidanceColumbia UNoNoYes
339Combined effect of TBM and NTM fields on fast-ion confinementStability & Disruption AvoidanceUC, IrvineNoYesNo
340Combined effect of TBM and Sawtooth fields on fast-ion confinementStability & Disruption AvoidanceUC, IrvineNoYesNo
342Investigation of Core Poloidal Rotation Anomaly Change at ITG -> TEM transitionPlasma RotationNational Fusion Research Institute (NFRI)NoYesYes
343Evaluating Physics of RMP Stationary Enhanced Confinement Regime Without ELMs for the 2013 JRTELM ControlLLNLNoNoYes
344Evaluating Physics of QH-mode Stationary Enhanced Confinement Regime Without ELMs for the 2013 JInductive ScenariosLLNLNoNoNo
345Evaluating Physics of I-mode Stationary Enhanced Confinement Regime Without ELMs for the 2013 JRELM ControlLLNLNoNoNo
346Control of H-L back transition via applied RMP fieldsL-H TransitionUCLANoNoNo
347Do differences in co/cnter GAM/ZF behavior affect deficit in gyrokinetic predicted Lmode transport?Turbulence & TransportUCLANoNoNo
348Can we obtain ELM suppression without substantial loss of density?ELM ControlUCLANoNoNo
349Density/current Scaling of Intrinsic Rotation and ITG/TEM TransitionTurbulence & TransportUCLANoNoNo
350Current/Density Scaling of Intrinsic Rotation and ITG/TEM TransitionPlasma RotationUCLANoNoNo
351Confinement enhancement via impurity-seeding of H-mode plasmasTurbulence & TransportU of WisconsinNoNoNo
352Does increased turbulence in H-mode degrade agreement of GK transport/turbulence simulations?Turbulence & TransportUCLANoNoNo
353Correlation length of electron temperature turbulence measurement and comparison with simulationsTurbulence & TransportUCLANoNoNo
354Control of Major Disruptions in DIII-DStability & Disruption AvoidanceColumbia UNoNoNo
355q dependence of L-H transition power thresholdL-H TransitionUCLANoNoNo
356GAM eigenmode excitation mechanismTurbulence & TransportUCLANoNoNo
357GAM eigenmode 2D structureTurbulence & TransportUCLANoNoNo
359q95 scaling of the coupled turbulence/zonal flow during LH transitionL-H TransitionU of WisconsinNoNoNo
360density scaling and X-point position scan of LH transition power thresholdL-H TransitionU of WisconsinNoNoNo
361Dither injection for closed-loop system identification of vacuum and plasma responseStability & Disruption AvoidanceConsultantNoNoNo
362Investigation of GAMs during I-mode on D3DTurbulence & TransportMassachusetts Institute of TechnologyNoYesNo
363TBM mockup simulating ITER GDC with ferritic materialsGeneral PhysicsGANoNoNo
364Absolute plasma response null measurement by multiple betaN stepsStability & Disruption AvoidanceColumbia UNoNoNo
365Lithium dropper commissioning and ELM modificationGeneral PhysicsGANoNoNo
366Up/down Asymmetric EFCStability & Disruption AvoidanceDepartment of EnergyNoNoNo
367JET/DIII-D similarity experiment on rotation in plasmas with low momentum inputPlasma RotationInstituto Superior Tecnico, Lisboa, PortugalNoYesNo
368Investigation of extreme outer wall heating caused by the DIII-D TBMPlasma-material InterfaceLLNLNoYesYes
369First-principles-driven Model-based Current-profile Control in H-mode DischargesPlasma ControlLehigh UNoNoNo
370Particle pinch in pedestalPedestal StructureGANoNoNo
371Effect of icoil current on energy confinement in RMP ELM-suppressed dischargesELM ControlGANoNoNo
372Pedestal optimization via impurity injectionPedestal StructureORNLNoNoNo
373Pedestal optimization in VH modePedestal StructureORNLNoNoNo
374Pedestal optimization with RMP ELM ControlPedestal StructureORNLNoNoNo
375QH-mode pedestal optimizationInductive ScenariosORNLNoNoNo
376Role of q and magnetic shear of pedestal formation time and turbulent transportPedestal StructurePPPLNoNoNo
377NTM locking disruption avoidance by the EM torque with toroidal-phase forward magnetic feedDisruption MitigationPPPLNoNoNo
378Study of the connection between I-mode and low density Type III ELMs and optimization of I-modeELM ControlGANoNoNo
379Pedestal optimization of ITER baseline scenario discharges.Pedestal StructureGANoNoNo
380ELM Suppression at Lower Collisionality with Non-Resonant n=3 I-coilELM ControlGANoNoNo
381Search for turbulence at ion-cyclotron frequenciesTurbulence & TransportUCLANoNoNo
382Transport and turbulence characterization experimentSteady State Heating and Current DriveUCLANoNoNo
383Run Coordinator Test ProposalGeneral PhysicsLLNLNoNoNo
384Run Coordinator Test Proposal IIGeneral PhysicsGANoNoNo
385The effect of LSN Shape on the q95 windows in RMP ELM SuppressionELM ControlGANoNoNo
386Measure Intrinsic Rotation Size scaling in DIII-D alone -IIPlasma RotationGANoNoNo
3873-D Fields and ECH Density PumpoutTurbulence & TransportGANoNoNo
388High Collisionless NBI Torque Drive for GAMs, aka the VH-mode path?Turbulence & TransportGANoNoNo
389Effect of n=1 applied and error fields on n=3 RMP ELM suppressionELM ControlGANoNoNo
390RMP ELM Suppression at q95 above 4ELM ControlGANoNoNo
391Current/Density Scaling of Intrinsic Rotation and ITG/TEM TransitionPlasma RotationUCLANoNoNo
392Influence of rotation and rotation shear on ELM suppressionELM ControlThe college of William and MaryNoNoNo
393collisionality impact on momentum and particle transportTurbulence & TransportThe college of William and MaryNoNoNo
394Role of density and impurities on particle and momentum transportTurbulence & TransportThe college of William and MaryNoNoNo
395Rotation reversalPlasma RotationThe college of William and MaryNoNoNo
396Measurement of RE diffusion to center postDisruption MitigationUCSDNoNoNo
397Disruption main chamber heat loadsDisruption MitigationUCSDNoYesYes
398TQ radiation distribution from R-2 MGIDisruption MitigationUCSDNoNoYes
399TQ radiation distribution from R-2 MGIDisruption MitigationUCSDNoNoYes
400Studies of RE final lossDisruption MitigationUCSDNoNoNo
401ITER Baseline Scenario DemonstrationInductive ScenariosITER OrganizationNoYesNo
402Radiative divertor solutions in the ITER baseline scenarioInductive ScenariosITER OrganizationNoYesNo
403Radiative divertor solutions in the ITER baseline scenarioDivertor & SOL PhysicsITER OrganizationNoYesNo
404ITER Baseline Scenario Operation near the LH ThresholdInductive ScenariosITER OrganizationNoYesNo
405Access conditions for steady-state operation in ITERSteady State Heating and Current DriveITER OrganizationNoYesNo
406Fast-ion and thermal transport at high qminSteady State Heating and Current DriveITER OrganizationNoYesNo
407n-scaling of magnetic errors (TBM related)Plasma RotationGANoNoYes
408Access to advanced inductive operation in ITERInductive ScenariosITER OrganizationNoYesNo
409Collisionality scaling of confinement in advanced inductive regimesInductive ScenariosITER OrganizationNoYesNo
410Sensitivity of RMP ELM Suppression with Less Than 12 I-coils to I-coil ConfigurationELM ControlLLNLNoNoYes
411Demonstration of stationary inductive solutions at low and moderate q95Inductive ScenariosITER OrganizationNoNoNo
412Development of Reproducible Startup and Target q Profile Control for Steady State ScenariosSteady State Heating and Current DriveITER OrganizationNoNoNo
413Demonstrate access to beta_N=5 with min(q)>2Steady State Heating and Current DriveITER OrganizationNoNoNo
414High li steady-state scenario developmentSteady State Heating and Current DriveITER OrganizationNoNoNo
415Access to zero torque advanced inductive with direct stabilization of the 2/1 mode by ECCDInductive ScenariosITER OrganizationNoNoNo
416Burn Control in ITER Baseline ScenarioInductive ScenariosITER OrganizationNoYesNo
417Comparison of H-Mode Transport with Co- and Ctr-NBITurbulence & TransportITER OrganizationNoNoNo
418Mapping the current rise stability boundary for the ITER baseline scenarioInductive ScenariosITER OrganizationNoNoYes
419Support of ITER Research Plan for Q=10 OperationInductive ScenariosITER OrganizationNoNoNo
420Identification of I-mode through simultaneous core and edge turbulence measurementsTurbulence & TransportMassachusetts Institute of TechnologyNoNoNo
422Separation of thermal and particle transport in I-mode plasmasTurbulence & TransportMassachusetts Institute of TechnologyNoNoNo
426Investigate the role of RS on inward momentum transportPlasma RotationUCSDNoNoNo
427Collisionality dependence of intrinsic rotationPlasma RotationUCSDNoNoNo
428Scaling of L-H transiton power with Xpoint location and collisionalityL-H TransitionUCSDNoNoNo
429Investigate the role of RS on inward momentum transportPlasma RotationUCSDNoNoNo
430Test of Turbulence Spreading Using Turbulence PropagationTurbulence & TransportGANoNoNo
431Turbulent transport in detached divertorDivertor & SOL PhysicsUCSDNoNoNo
432Transport mechanisms induced by RMPELM ControlUCSDNoNoNo
433Investigate the role of RS on inward momentum transportPlasma RotationUCSDNoNoNo
434COupling between core and SOL parallel flowDivertor & SOL PhysicsUCSDNoNoNo
435Electron Critical Gradient in H-modeTurbulence & TransportGANoNoNo
437TQ radiation distribution from R-2 MGIDisruption MitigationMassachusetts Institute of TechnologyNoNoNo
438Optimize electron pedestal pressure in ECH-heated QH-mode plasmasPedestal StructureUCLANoNoNo
439Optimize electron pedestal pressure in ECH-heated QH-mode plasmasPedestal StructureUCLANoNoNo
440Beam Density Affects on Carbon Density ProfileTurbulence & TransportGANoNoNo
441Active Particle Exhaust of H-mode Plasmas in the Snowflake-minus Divertor ConfigurationDivertor & SOL PhysicsGANoNoNo
442Measurement of Inductive Poloidal CurrentStability & Disruption AvoidanceGANoNoNo
443Effect of Changing the Grad-B Drift Direction on Snowflake Divertor Behavior, Including DetachmentDivertor & SOL PhysicsGANoNoNo
444Identify the Optimal Impurity for High Power High Performance Plasmas During Radiating Divertor OpsInductive ScenariosGANoNoNo
445Effect of Islands on ECCDStability & Disruption AvoidanceGANoNoNo
448Density Control and Active Impurity Removal from Double-null H-mode PlasmasInductive ScenariosGANoNoNo
450Hybrids with co-NBI QH-mode edgeInductive ScenariosGANoNoNo
452Source of Magnetic Flux Pumping in HybridsInductive ScenariosGANoNoNo
453Minimize Density Pumpout During RMP ELM SuppressionELM ControlLLNLNoNoYes
454Synergy between core-localized Alfven eigenmodes and edge localized TBM fields on fast ion losses.Energetic ParticlesPPPLNoYesNo
456Energy Transport During Electron-Dominated Heating of ITER Baseline Scenario H-Mode DischInductive ScenariosPPPLNoNoNo
457Prompt torque and zonal flow dampingTurbulence & TransportGANoNoNo
458Test optimized TBM error field correction at higher values of betaStability & Disruption AvoidanceCRPP-EPFLNoNoYes
459Model-based control of the current profile and βN for steady state scenariosSteady State Heating and Current DriveCadaracheNoNoNo
460Quantifying the TBM torque, both in magnitude and radial locationPlasma RotationVTT Technical Research CentreNoNoYes
461Dependence of momentum transport and intrinsic torque on rho* and betaPlasma RotationVTT Technical Research CentreNoYesNo
488Investigate angular momentum diffusion and pinch using off-axis torquePlasma RotationGANoNoNo
489Discussion of plasma rotation transient process during OFM/ELM-driven RWM w/wo feedback usinEnergetic ParticlesPPPLNoNoNo
490Maintain low-rotation QH-mode with ECH onlyInductive ScenariosGANoNoNo
491Investigate in-out density asymmetry at large toroidal rotationPlasma RotationGANoNoNo
492Diagnostic spatial cross calibration using edge sweeps in QH-modePedestal StructureGANoNoNo
493Edge rotation shear threshold for QH-mode accessELM ControlGANoNoNo
494Further development of QH-mode with strong co-Ip NBI torqueInductive ScenariosGANoNoNo
495QH-mode with low torque start-upInductive ScenariosGANoNoNo
496Impact of fast-ions on the RWM stability boundaryStability & Disruption AvoidanceColumbia UNoNoNo
497Cause(s) for the rotation degradation and tearing instabilities of the ITER baseline scenarioInductive ScenariosColumbia UNoNoNo
499Up/down Asymmetric EFCStability & Disruption AvoidanceDepartment of EnergyNoNoNo
501Energy Transport During Electron-Dominated Heating of ITER Baseline Scenario H-Mode DischargesSteady State Heating and Current DrivePPPLNoNoNo
502Energy Transport During Electron-Dominated Heating of ITER Baseline Scenario H-Mode DischargesTurbulence & TransportPPPLNoNoNo
505RMP ELM Control at ITER relevent rotation/torqueELM ControlUCSDNoNoNo
507Exploring Impurity Density Asymmetries due to NBI Fast Ions and Their Effect on Impurity TransportTorkil Jensen Award_NoNoNo
508ITER Baseline Scenario in a Radiating Divertor Environment with near-Zero Applied TorqueInductive ScenariosGANoNoYes
509Vertical positioning and stability control by means of reflectometryPlasma ControlGANoNoNo
510What can lost fast-ions tell us about the H-mode pedestal?Pedestal StructurePPPLNoNoNo
511Impact of EHO on fast ion lossesInductive ScenariosPPPLNoNoNo
512Best Impurity Specie for the Radiating Divertor in the ITER Baseline Scenario with near-Zero TorqueInductive ScenariosGANoNoYes
513Investigating the role of inter-ELM fluctuations in the ELM triggerELM ControlGANoNoNo
518Explore RMP ELM suppression mechanism at moderate collisionalityELM ControlUCSDNoNoNo
519RMP ELM-Control for Snowflake ConfigurationsDivertor & SOL PhysicsLLNLNoNoNo
521Dependence of confinement and stability on toroidal rotation in high li dischargesSteady State Heating and Current DriveGANoNoNo
522Combined effect of TBM and NTM fields on fast-ion confinementEnergetic ParticlesUC, IrvineNoYesNo
523Combined effect of TBM and Sawtooth fields on fast-ion confinementEnergetic ParticlesUC, IrvineNoYesNo
524VFI bus voltage control and the True scaled ITER shape at DIII-DPlasma ControlGANoNoNo
525Test critical gradient model for fast-ion transportEnergetic ParticlesUC, IrvineNoNoNo
526q95 < 2 Tokamak Operation Via Dynamic Error Field CorrectionStability & Disruption AvoidanceGANoNoNo
527256: SOL width and divertor peak heat flux in QH-mode plasmas with/without n=3 fieldsInductive ScenariosGANoNoNo
528Study NRMF driven torque in ECH-only heated plasma (ELMing H-modes)Plasma RotationGANoNoNo
529Investigate the physics of NTM suppression by large externally applied helical fieldsTorkil Jensen AwardGANoNoNo
530Studies of arcing on divertor PFC surfacesPlasma-material InterfaceUCSDNoNoNo
531Dust generation from deposited layers and leading edgesPlasma-material InterfaceUCSDNoNoNo
532Role of ECH Induced Mulitiscale Electron Thermal Transport in H-mode PlasmasTurbulence & TransportMassachusetts Institute of TechnologyNoNoYes
533Between-shots gyrokinetic stability analysisTurbulence & TransportMassachusetts Institute of TechnologyNoNoNo
534Develop low-torque, high normalized fusion performance QH-mode for ITER baseline scenarioInductive ScenariosGANoNoNo
535Main-ion and impurity neoclassical flows compared with the PERFECT pedestal codePedestal StructureMassachusetts Institute of TechnologyNoNoYes
536Low rotation, elevated q_min steady-state scenario discharges at high betaN and 210R MSESteady State Heating and Current DriveGANoNoNo
538Reduce fast ion transport in high qmin, high beta plasmasSteady State Heating and Current DriveLLNLNoNoNo
539Produce fNI = 1 discharges at q_min near 1.5 using off-axis injection and a model guided approachSteady State Heating and Current DriveGANoNoNo
540Establish the incremental confinement of EC power in high betaN steady-state scenario dischargesSteady State Heating and Current DriveGANoNoNo
541Support of DIII-D boundary physics experimentsDivertor & SOL PhysicsMITNoNoNo
542Investigations of advanced divertor configurations for DIII-DDivertor & SOL PhysicsMITNoNoNo
545High beta with NCS and qmin>2Steady State Heating and Current DriveGANoNoNo
546Investigate elongation limit in low li discharges with/without applied 3D magnetic fieldsTorkil Jensen AwardGANoNoNo
548Improve the optimized high li operating regime through 1/1 and 2/1 instability avoidanceSteady State Heating and Current DriveGANoNoNo
550Probing and controlling the L->H and H->L transitions by small pellet injectionL-H TransitionKorea Institute of Fusion EnergyNoNoNo
551Test compatibility of radiative divertor with QH-modeInductive ScenariosGANoNoNo
552Modulation of Bootstrap CurrentELM ControlGANoNoNo
553Bootstrap Current Change During RMP ELM SuppressionELM ControlGANoNoNo
554The impact of increased pressure gradient on scenarios for fully noninductive operationSteady State Heating and Current DriveGANoNoNo
555Measure Plasma Response to RMPsELM ControlGANoNoNo
556Pedestal optimization with RMP ELM ControlPedestal StructureORNLNoNoNo
559SOL Width Scaling: Goldston's Heuristic Drift Model vs Critical Pressure Gradient ModelDivertor & SOL PhysicsPPPLNoNoNo
560NBI Driven Poloidal RotationPlasma RotationGANoNoNo
561Interaction of RMP Snowflake DivertorDivertor & SOL PhysicsPPPLNoNoNo
563The Role of Energetic Particles in ELM-Free H-mode PlasmasELM ControlUC, IrvineNoNoNo
565Benign 3/2 NTM Formation to avoid 2/1 NTM lockingStability & Disruption AvoidancePPPLNoNoNo
566Testing of New Hardware and Software Capabilities for NTM ControlPlasma ControlPPPLNoNoNo
567Is loss of rotation in low-torque IBS discharges due to solenoid-related error fields?Inductive ScenariosGANoNoNo
568ITER Baseline Scenario: Expand the operational limit by NTM stabilization and Time Dependent EFCInductive ScenariosPPPLNoNoNo
573Impact of EHO on fast ion lossesInductive ScenariosPPPLNoNoNo
576Slow snowflake configuration scans to clarify geometry vs physicsDivertor & SOL PhysicsLLNLNoNoNo
577MARFE limits in the snowflake configurationDivertor & SOL PhysicsLLNLNoNoNo
579Mapping of Peeling Mode Stability BoundaryPedestal StructureGANoYesNo
580Collisionality/density dependence and Pedestal optimization with ELM SupELM ControlGANoYesNo
588Plasma Response in IWL H-mode plasmasELM ControlORNLNoNoNo
589Exploration of super H-mode using high density QH-modeInductive ScenariosGANoNoNo
590Targeting Top of Pedestal in RMP ELM-suppressed plasmas with SXR ImagingELM ControlORNLNoNoNo
593Demonstrating Stiffness of Electron Heat Transport in the Presence of Strong RadiationTurbulence & TransportMassachusetts Institute of TechnologyNoNoNo
594Aspect ratio scaling of turbulence and transport: DIII-D and NSTX-U comparisonTurbulence & TransportU of WisconsinNoNoNo
595ITER steady-state scenario in USN, +BTSteady State Heating and Current DriveORNLNoNoNo
596q95 dependency of beam ion confinement in high qmin scenarioSteady State Heating and Current DriveORNLNoNoNo
597Apple-to-apple comparison of ITER steady-state scenarios: high/elevated qmin, SS hybrid, and high liSteady State Heating and Current DriveORNLNoNoNo
598Far off-axis NBCD using vertically shifted plasmaSteady State Heating and Current DriveORNLNoNoNo
599Measurement of neoclassical response of off-axis beam ionsSteady State Heating and Current DriveORNLNoNoNo
600Anomalous current diffusion in steady-state hybrid scenario with ELM suppressionSteady State Heating and Current DriveORNLNoNoNo
601Control of tungsten PFC erosion by local gas injectionPlasma-material InterfaceGANoNoNo
603Dominant poloidal modes for ELM suppression via n=2 upper/lower I-coil phase differenceELM ControlColumbia UNoNoNo
604EF optimization of low-torque low-q95 QH mode plasmasInductive ScenariosColumbia UNoNoNo
605Importance of matched poloidal spectra in most sensitive EFC conditionsStability & Disruption AvoidanceColumbia UNoNoNo
606Dominant kink-mode poloidal coupling dependence with betaN, q95Stability & Disruption AvoidanceColumbia UNoNoNo
607Direct measurement of E-coil contribution to intrinsic EFStability & Disruption AvoidanceColumbia UNoNoNo
608Quiescent runaway electron studies for 2014Disruption MitigationColumbia UNoNoNo
609MHD spectroscopy and poloidal coupling of plateau RE plasmasDisruption MitigationColumbia UNoNoNo
610Local correction of the TBM error fieldStability & Disruption AvoidanceColumbia UNoNoNo
611Absolute plasma response null measurement by multiple betaN stepsStability & Disruption AvoidanceColumbia UNoNoNo
612Investigate the Impact of ECH on Alfvenic ActivityEnergetic ParticlesGANoYesNo
613Testing for parameter space with the best fast ion confinement at high q_minSteady State Heating and Current DriveGANoNoNo
614Why Does the Heat Flux Increase in the Secondary Divertor Under the BetaN = constant Constraint?Divertor & SOL PhysicsGANoNoNo
615Increase achievable betaN in high betaP experiment using n=3 betaN feedback (ala burn control)Steady State Heating and Current DriveGANoNoNo
617Characterization of core/pedestal density limits for rotating tearing modesStability & Disruption AvoidanceColumbia UNoNoNo
618Controlling VH-mode with RMPs and comparison to NSTX EPH-modeELM ControlPPPLNoNoNo
619ELM divertor footprint and connection to ELM dynamics and effects of turbulence and modesELM ControlUCSDNoNoNo
620Measurement of heat flux on the divertor using the embedded thermocouple arrayDivertor & SOL PhysicsU of Tennessee, KnoxvilleNoNoNo
621Investigation of Sheath Power Transmission at the DIII-D Divertor using Surface ThermocouplesDivertor & SOL PhysicsU of Tennessee, KnoxvilleNoNoNo
623Trapped Electron Mode n_e / T_e Fluctuation StudyTurbulence & TransportU of Colorado, BoulderNoNoNo
624Trapped Electron Mode Study in CoreTurbulence & TransportU of Colorado, BoulderNoNoNo
625Disruption Precursor IdentificationDisruption MitigationU of Colorado, BoulderNoNoNo
634Mitigation: Reduction of toroidal-asymmetry of radiation loss by 3D-magnetic mode rotation controlDisruption MitigationPPPLNoNoYes
635Mitigation: pellet and massive gas injections in helically favorable ways for reducing asymmetryDisruption MitigationPPPLNoNoYes
636Time-resolved measurement of plasma response spectrumStability & Disruption AvoidanceColumbia UNoNoNo
637RMP Effect on ELMs: Separate the effect of density pumpoutELM ControlPPPLNoNoNo
638BetaN control with 3D Fields instead of NBIInductive ScenariosPPPLNoNoNo
639Electron thermal transport due to Compressional and Global AEs on DIII-D and projection to NSTX-UTurbulence & TransportUCLANoNoNo
640Fully Non-Inductive, Low Rotation QH-modeTorkil Jensen AwardORNLNoNoNo
641Using Magnetic Balance To Regulate Density and Impurity Accumulation Inside Double-null PlasmasDivertor & SOL PhysicsGANoNoNo
642Gas Injection Feedback with Radiation MeasurementsDivertor & SOL PhysicsPPPLNoNoNo
643Campaign to study physics at the Greenwald limitSteady State Heating and Current DrivePPPLNoNoNo
644Controlled Snowflake Divertor StudyDivertor & SOL PhysicsPPPLNoNoNo
645Access to low torque QH-mode using high beta low torque AI target with NRMFInductive ScenariosGANoNoNo
646rho* scaling of intrinsic torque between DIII-D and JETPlasma RotationGANoYesNo
647Radiating Divertor Applied to the ITER Baseline Scenario at near-Zero Applied TorqueDivertor & SOL PhysicsGANoNoYes
648Determining the Optimal Impurity Specie for the Radiating Divertor in the ITER Baseline ScenarioDivertor & SOL PhysicsGANoNoYes
649Search for high freq magnetic fluctuations with CPS diagnosticTurbulence & TransportUCLANoNoNo
650ELM Mitigation with ECCDTorkil Jensen AwardPPPLNoNoNo
651Achieve QH-mode plasmas with Te, Ti ~ 10 keV near mid-radiusTurbulence & TransportUCLANoNoNo
652QH-mode operation with reduced divertor interactionInductive ScenariosGANoNoNo
653High-Z Transport in QH-mode PlasmasPlasma-material InterfaceGANoNoNo
654Effect of sawteeth on QH-mode pedestal (EHO)Inductive ScenariosGANoNoNo
655ECH effects on QH-mode low or balanced torque discharges in DIII-DPlasma RotationKorea Institute of Fusion EnergyNoYesNo
657Initial n=2 error field correctionStability & Disruption AvoidanceGANoNoNo
658Plasma response to n=2 perturbationsStability & Disruption AvoidanceGANoNoNo
659n = 2 Dynamic Error Field CorrectionStability & Disruption AvoidanceGANoNoNo
660Dependence of non-axisymmetric plasma response on plasma rotationStability & Disruption AvoidanceGANoNoNo
661Massive gas injection into an unstable plasmaDisruption MitigationGANoNoNo
662NTV Collisionality Regime TestPlasma RotationColumbia UNoNoNo
663Effect of higher mode number error fields on n=1 Locking ThresholdStability & Disruption AvoidanceColumbia UNoNoNo
664Follow-up studies of fast-ion transport effects on steady-state plasmasSteady State Heating and Current DriveUC, IrvineNoNoNo
665Feedback Control to Assess the Usefulness For Using Two Impurity Species in Radiating DivertorPlasma ControlGANoNoNo
666Radiation limit in the snowflake configurationDivertor & SOL PhysicsCRPP-EPFLNoNoNo
667Effect of the snowflake configuration on the SOL width in simple plasmasDivertor & SOL PhysicsCRPP-EPFLNoNoNo
668GAM eigenmode excitation mechanism and its impact on transportTurbulence & TransportUCLANoNoNo
669Extrapolation of Low-Torque ITER Baseline Scenario With nu* and rho*Turbulence & TransportGANoNoNo
670Investigate GAM's role in the L-H transitionL-H TransitionUCLANoNoNo
671GAM eigenmode 2D structureTurbulence & TransportUCLANoNoNo
672L-H threshold in hydrogen plasmasL-H TransitionORNLNoNoNo
674Assessing the Need for Using Two Impurity Species in Radiating DivertorDivertor & SOL PhysicsGANoNoNo
675Error field correction at low rotationStability & Disruption AvoidanceGANoYesNo
676Robust NTM controlPlasma ControlCRPP-EPFLNoYesYes
677Robust NTM controlStability & Disruption AvoidanceCRPP-EPFLNoYesYes
678Understanding and Testing Methods for Producing Gentle HL TransitionsL-H TransitionGANoNoNo
679Safety Factor Scaling of Turbulence and Transport in Hybrid Scenario PlasmasTurbulence & TransportU of WisconsinNoNoNo
680Fine scale stepwise q-scan: role of low-order rationales and resonance condition for ELM suppressionELM ControlU of WisconsinNoNoNo
681Transport Investigation During Slow Current Ramp-Up and Ramp-Down [for ITER]Inductive ScenariosU of WisconsinNoNoNo
682Amplifying the Geodesic Acoustic Mode via Resonant Radial Field Amplification: New MethodsTurbulence & TransportU of WisconsinNoNoNo
683Confinement enhancement via impurity-seeding of H-mode plasmasTurbulence & TransportU of WisconsinNoNoNo
684Isotope Mass Scaling of Turbulence, Transport and Confinement in H-ModeTurbulence & TransportU of WisconsinNoNoNo
685Locked mode control at low (ITER-like) q95 and with external C-coilsStability & Disruption AvoidanceColumbia UNoNoNo
686â??Born-lockedâ?? mode control by ECCD and magnetic perturbationsStability & Disruption AvoidanceColumbia UNoNoNo
687Add modulated ECCD to f/back or f/fwd entrainment dischargesStability & Disruption AvoidanceColumbia UNoNoNo
688Measure Beam Ion Transport due to Resonance Between Applied 3D Fields and Injected Beam Ion OrbitsEnergetic ParticlesGANoYesNo
689Assess optimal Error Field Correction by modulating I-coils at incommensurable frequenciesStability & Disruption AvoidanceColumbia UNoNoNo
690EFC by ramping beta up or q95 down or NBI torque down (instead of density down) in 3-4 dischargesStability & Disruption AvoidanceColumbia UNoNoNo
691Locked-mode avoidance by magnetic f/back on saddle-loopsStability & Disruption AvoidanceColumbia UNoNoNo
692NTMs â??on demandâ??, by ECHStability & Disruption AvoidanceColumbia UNoNoNo
693NTMs â??on demandâ??, by modulated ECCDStability & Disruption AvoidanceColumbia UNoNoNo
694Image Heat Load Due to Prompt and 3D field Induced EP LossesEnergetic ParticlesGANoYesNo
695Poloidal rotation of plasma column to simulate rotating wallPlasma ControlColumbia UNoNoNo
696Measure Change in 3D Field Induced EP Losses Due to ScreeningEnergetic ParticlesGANoYesNo
697Electromagnetic Torque Waves â?? Transport of Angular MomentumPlasma RotationColumbia UNoNoNo
698Dither injection for closed-loop system identification of vacuum and plasma responseStability & Disruption AvoidanceConsultantNoNoNo
699Feedback control of mode rotation and phaseStability & Disruption AvoidanceConsultantNoNoNo
700PID-controlled boundary radial field for â??spontaneousâ?? mode-unlockingStability & Disruption AvoidanceConsultantNoNoNo
701Effect of lithium conditioning on H-mode pedestal profiles and ELM stabilityELM ControlGANoNoNo
702Measurement of hysteresis in RMP-ELM suppression thresholdsELM ControlColumbia UNoNoNo
703Use high betaP operating regime to study fast ion transportEnergetic ParticlesLLNLNoNoNo
704Use high betaP operating regime to study fast ion transportSteady State Heating and Current DriveLLNLNoNoNo
705Develop feedback-controlled 3D equilibriaStability & Disruption AvoidanceColumbia UNoNoNo
706Physics of the low density branch of the L-H power threshold scalingL-H TransitionUCLANoNoNo
707Physics of the low density branch of the L-H power threshold scalingL-H TransitionUCLANoNoNo
708444: Identify the Optimal Impurity for High Power High Performance Plasmas During Radiating Divertor OpsSteady State Heating and Current DriveGANoNoNo
709Physics of EHO control in low-torque QH-modeInductive ScenariosDepartment of EnergyNoNoNo
710RWM control using external coilsStability & Disruption AvoidanceColumbia UNoNoNo
711Comparision DIII-D and AUG high collisionality ELM response to 3D magnetic perturbationsELM ControlGANoNoNo
712D2 + few % Ne shattered pellets for disruption mitigationDisruption MitigationORNLNoNoYes
713Control of radiation asymmetries by application of external field on SPI/MGI shutdownDisruption MitigationORNLNoNoYes
714Runaway flattop mitigation by Neon shattered pellet injectionDisruption MitigationORNLNoNoYes
715Test of the upgraded SPIDisruption MitigationORNLNoNoNo
716Assess the destabilization mechanism for the n = 1 tearing mode in steady-state scenario dischargesSteady State Heating and Current DriveGANoNoNo
717Role of poloidal flux expansion to address divertor heat flux challengeDivertor & SOL PhysicsGANoNoNo
718Compare the power threshold for pre-emptive NTM suppression vs Catch and SubdueStability & Disruption AvoidancePPPLNoNoNo
719NTM Control Upgrade: Capibility to deposit EC at multiple locationsPlasma ControlPPPLNoNoNo
720Real-time Error Field CorrectionPlasma ControlPPPLNoNoNo
721qmin controlSteady State Heating and Current DrivePPPLNoNoNo
722NTM control with ECCD, Real-time Ray Tracing and real-time MirrorsPlasma ControlPPPLNoNoNo
723Physics of the Heat Flux WidthDivertor & SOL PhysicsAKIMA Infrastructure ServicesNoNoNo
724Impurity transport in ELM-suppressed regimesELM ControlGANoNoNo
725What causes density buildup at the pedestal top?Pedestal StructureU of WisconsinNoNoNo
726Test Pedestal Structure Model Where Paleoclassical Transport Is DominantPedestal StructureU of WisconsinNoNoNo
727Scaling Of Pedestal Plasma Transport With RMP I-coil CurrentELM ControlU of WisconsinNoNoNo
7283D Fields Effects on Critical Gradient and TurbulenceTurbulence & TransportGANoNoNo
729Dependence of pedestal structure on collisionality and Zeff in relation to JET results with ILWPedestal StructureGANoYesNo
730Search for Fast Ion Critical GradientEnergetic ParticlesGANoNoNo
731Turbulent Ion Thermal Response to Electron Heat Flux and Te/Ti VariationTurbulence & TransportSandia National LabNoNoNo
732Testing ELM destabilization by 3D fields on DIII-DELM ControlORNLNoNoNo
733Distinguishing between 3d magnetic field structures and transportELM ControlORNLNoNoNo
734First wall heat flux and erosion due to TBM induced error fieldsPlasma-material InterfaceORNLNoNoNo
735ELM Suppression in Helium PlasmasELM ControlGANoNoYes
736Erosion/Deposition of Aluminum with low density He L-mode Simple-As-Possible PlasmasPlasma-material InterfaceCommonwealth Fusion SystemsNoNoNo
737n=1 and n=2 simultaneous DEFC /DFB for routine demonstration of low q << 2 RWM stable regimeStability & Disruption AvoidancePPPLNoNoNo
738The investigation of EP-kinetic effects and plasma rotation with low q and low beta operationStability & Disruption AvoidancePPPLNoNoNo
739Reduce L-H treshold power in H plasmas using pellet injectionL-H TransitionGANoNoYes
740Respond to locking by ramping IP downStability & Disruption AvoidanceColumbia UNoNoNo
741Quantifying the improved confinement achieved by NTM spinupStability & Disruption AvoidanceMassachusetts Institute of TechnologyNoNoNo
742Measurement of viscous torque on locked 2/1 modeStability & Disruption AvoidanceMassachusetts Institute of TechnologyNoNoNo
743Measurement of viscous torque on locked 2/1 modeStability & Disruption AvoidanceMassachusetts Institute of TechnologyNoNoNo
744NBI torque assisted unlocking and spinup experimentsStability & Disruption AvoidanceMassachusetts Institute of TechnologyNoNoNo
745Transport studies in I-mode plasmasPedestal StructureMassachusetts Institute of TechnologyNoNoNo
746Isotope dependence of Pthr and edge turbulence at L-H and H-L transition in DIII-D and JET-ILWL-H TransitionIPP GarchingNoNoYes
747Dissipation & Control of RE from ITER-like LSN targetsDisruption MitigationGANoNoNo
748Implement finite-state Off Normal Fault Response systemPlasma ControlGANoNoNo
749Neon SPI injection into early CQ to stunt RE formationDisruption MitigationGANoNoNo
750The role of non-local transport and avalanches in different L-H transition regimesL-H TransitionUCLANoNoNo
751Dimensionless Identity Experiments in I-Mode with C-Mod and AUG (TC-18)Pedestal StructureMassachusetts Institute of TechnologyNoYesNo
752Divertor detachment versus toroidal field and plasma currentDivertor & SOL PhysicsGANoYesNo
753q95 scaling of the coupled turbulence/zonal flow during LH transitionL-H TransitionU of WisconsinNoNoNo
754density scaling and X-point position scan of LH transition power thresholdL-H TransitionU of WisconsinNoNoNo
755Heat flux footprint with pellet-paced ELMs vs nustarELM ControlPPPLNoNoYes
756QH-mode edge sweep with helium impurity for comparison to XGC0Pedestal StructurePPPLNoNoNo
757Cause(s) for the rotation degradation and tearing instabilities of the ITER baseline scenarioStability & Disruption AvoidanceColumbia UNoNoNo
758First-principles-driven Model-based Current Profile and Internal Energy Control in H-mode DischargesPlasma ControlLehigh UNoNoNo
759Link between driven plasma response and tearing stabilityStability & Disruption AvoidanceColumbia UNoNoNo
760Marginal 2/1 island width in IBSStability & Disruption AvoidanceRetired from GANoNoNo
761Rotating Magnetic Field Current-Drive (RMFCD)Torkil Jensen AwardMassachusetts Institute of TechnologyNoNoNo
762ITER Baseline Scenario: Expand the operational limit by NTM stabilization and Time Dependent EFCStability & Disruption AvoidancePPPLNoNoNo
763Expand the high li, betaN >4 operating regime through NTM StabilizationStability & Disruption AvoidancePPPLNoNoNo
764Multiple periods of NTM suppressionStability & Disruption AvoidancePPPLNoNoNo
765Island seeding with saw teeth pacing: New method to control tearing modesStability & Disruption AvoidancePPPLNoNoNo
766Island seeding with saw teeth pacing: New method to control tearing modesPlasma ControlPPPLNoNoNo
767Radiation asymmetry measurements in opposite-handed plasmasDisruption MitigationORNLNoNoNo
768sheath physics study 2Divertor & SOL PhysicsSandia National LabNoNoNo
769benchmark heat flux with fast TCsDivertor & SOL PhysicsSandia National LabNoNoNo
770Calibrated passive FIDA spectrumEnergetic ParticlesUC, IrvineNoNoNo
771Distribution function inversion benchmarkEnergetic ParticlesUC, IrvineNoNoNo
772Unified edge and SOL rotationDivertor & SOL PhysicsUCSDNoNoNo
773Model-based control of the current profile and βN for steady state scenariosPlasma ControlGANoNoNo
774Rotating Magnetic Field Current Drive (RMFCD)Steady State Heating and Current DriveMassachusetts Institute of TechnologyNoNoNo
775High qmin transient betaN=5 demonstrationSteady State Heating and Current DriveLLNLNoNoNo
776Control/Ops Evening Development TimePlasma ControlGANoNoNo
777Magnitude of cross-field drifts in the Private Flux Region, divertor asymmetries and detachmentDivertor & SOL PhysicsAalto UNoNoNo
778Assessment of main chamber carbon sourcesDivertor & SOL PhysicsAalto UNoNoNo
779Measurement of the Heat Flux(Grad T) FunctionTurbulence & TransportU of Texas, AustinNoNoNo
7803D coil based BetaN control instead of NBI based BetaN control.Steady State Heating and Current DrivePPPLNoNoNo
781Can RMP ELM Control be reliably used in ITER (or a reactor)?ELM ControlPPPLNoNoNo
782RMP ELM Control DevelopmentPlasma ControlPPPLNoNoNo
783Development of Fully Noninductive High Beta EAST Scenario IISteady State Heating and Current DriveGANoNoNo
784Understanding the NTM Stability Limits by q-profile modificationInductive ScenariosPPPLNoNoNo
785Active determination of angular momentum transfer process between 3D structures: NTM 2/1 and 3/2 moStability & Disruption AvoidancePPPLNoNoNo
786Determining Particle Sources/Sinks in ITER-like NN Discharges during RMP ELM suppressionELM ControlORNLNoNoNo
787Optimize Radiative Divertor and Core PerformanceSteady State Heating and Current DrivePPPLNoNoNo
788Optimize Radiative Divertor and Core PerformanceDivertor & SOL PhysicsPPPLNoNoNo
789Iter Scenario: Optimize Radiative Divertor and Core PerformanceInductive ScenariosPPPLNoNoNo
790Detachment Control for H-modeDivertor & SOL PhysicsPPPLNoNoNo
791Detachment Control for H-modePlasma ControlPPPLNoNoNo
792Combined Core and Divertor Radiation Control: Gas Injection Feedback with Radiation MeasurementsPlasma ControlPPPLNoNoNo
793qmin controlPlasma ControlPPPLNoNoNo
794ITER Scenario: Understanding the NTM Stability Limits by q-profile modificationInductive ScenariosPPPLNoNoNo
795Measure NTV torque profilePlasma RotationColumbia UNoNoNo
796Snowflake ControlPlasma ControlPPPLNoNoNo
797BetaN control with 3D CoilsPlasma ControlPPPLNoNoNo
798Density matching with and without ELMs.ELM ControlGANoNoNo
799Development for PID-controlled boundary radial fieldPlasma ControlConsultantNoNoNo
800Physics of EHO control in low-torque QH-modeTorkil Jensen AwardDepartment of EnergyNoNoNo
801Collisionality dependence of pedestal height with RMPELM ControlGANoNoNo
802Breakdown Optimization with ECHPlasma ControlGANoNoNo