DIII-D RESEARCH OPPORTUNITIES FORUM FOR THE 2013 EXPERIMENTAL CAMPAIGN Review | Direct submission with log-in | Request submission without log-in

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ID Title Research Area Name Affiliation Time
Req'ed
ITPA
Joint Exp
ITER IO Urgent
Research Task
1 detailsC vs I Coil NTVPlasma RotationGANoNoNo
2 detailsHysteresis and Turbulence Spreading in the H-L Back TransitionL-H TransitionUCLANoNoNo
4 detailsTurbulence and Intrinsic RotationPlasma RotationGANoNoNo
5 detailsMeasure Intrinsic Rotation Size scaling in DIII-D alone -IIPlasma RotationGANoNoNo
6 detailsPrompt torque and zonal flow dampingPlasma RotationGANoNoNo
7 detailsInvestigate angular momentum diffusion and pinch using off-axis torquePlasma RotationGANoNoNo
8 detailsCompare Mach probe and CER measurements of intrinsic rotation profile of main ions in helium plasmaPlasma RotationGANoNoNo
9 detailsTest of Neoclassical Toroidal Viscosity theory using modulated I-coil currentsPlasma RotationGANoNoNo
10 detailsMaintain low-rotation QH-mode with ECH onlyInductive ScenariosGANoNoNo
11 detailsInvestigate in-out density asymmetry at large toroidal rotationPlasma RotationGANoNoNo
12 detailsDiagnostic spatial cross calibration using edge sweeps in QH-modePedestal StructureGANoNoNo
13 detailsCompare edge particle transport in ELMing H-mode and QH-mode with and without NRMFInductive ScenariosGANoNoNo
14 detailsControl of toroidal mode number of EHOInductive ScenariosGANoNoNo
15 detailsEdge rotation shear threshold for QH-mode accessInductive ScenariosGANoNoNo
16 detailsFurther development of QH-mode with strong co-Ip NBI torqueInductive ScenariosGANoNoNo
17 details3-D Fields and ECH Density PumpoutTurbulence & TransportGANoNoNo
18 detailsHigh Collisionless NBI Torque Drive for GAMs, aka the VH-mode path?Turbulence & TransportGANoNoNo
19 detailsEffect of n=1 applied and error fields on n=3 RMP ELM suppressionELM ControlGANoNoNo
20 detailsL-H transition Trigger Physics/ Main Ion Momentum BalanceL-H TransitionUCLANoNoNo
21 detailsMagnitude of cross-field drifts in the Private Flux Region, divertor asymmetries and detachmentDivertor & SOL PhysicsAalto UNoNoNo
22 detailsAssessment of main chamber carbon sourcesDivertor & SOL PhysicsAalto UNoNoNo
23 detailsRMP ELM Suppression at q95 above 4ELM ControlGANoNoNo
24 detailsPlasma response to 3D magnetic perturbations in the unfavorable grad-B drift directionELM ControlPPPLYesNoNo
26 detailsInvestigate the role of RS on inward momentum transportTurbulence & TransportUCSDNoNoNo
27 detailsCOupling between core and SOL parallel flowDivertor & SOL PhysicsUCSDNoNoNo
28 detailsRole of profile evolution and energy transfer in L-H transitionL-H TransitionUCSDNoNoNo
29 detailsModulation of Bootstrap CurrentELM ControlGANoNoNo
30 detailsNew Optimal Plasma Shape for AT Scenario?Steady State Heating and Current DriveGANoNoNo
31 detailsTest of Turbulence Spreading Using Turbulence PropagationTurbulence & TransportGANoNoNo
32 detailsHigh Beta Hybrids and Pressure Profile BroadeningSteady State Heating and Current DriveGANoNoNo
33 detailsHigh Beta, Steady State HybridsSteady State Heating and Current DriveGANoNoNo
34 detailsElectron Critical Gradient and Heat PinchTurbulence & TransportGANoNoNo
35 detailsNon-Diffusive Heat Fluxes in the Edge "Shortfall" RegionTurbulence & TransportGANoNoNo
36 detailsNatural ELM Pacing in High-Beta, Steady-State PlasmasSteady State Heating and Current DriveGANoNoNo
37 detailsIdentification of I-mode through simultaneous core and edge turbulence measurementsTurbulence & TransportMassachusetts Institute of TechnologyYesNoNo
38 detailsCalibrated passive FIDA spectrumEnergetic ParticlesUC, IrvineNoNoNo
39 detailsMeasure and understand energetic particle profiles in steady-state plasmasSteady State Heating and Current DriveUC, IrvineNoNoNo
40 detailsMGI with applied n=1 RMP fieldsDisruption MitigationFiat Lux LLCNoNoNo
41 detailsInvestigation of the effects of the EHO toroidal mode number on the edge particle transportInductive ScenariosPPPLNoNoNo
42 detailsCompatibility of High Performance Plasmas With a Puff-and-Pump Radiating DivertorSteady State Heating and Current DriveGANoNoNo
43 detailsDensity Control and Active Impurity Removal from Double-null H-mode PlasmasDivertor & SOL PhysicsGANoNoNo
44 detailsCan Nitrogen impurity Seeding Improve Radiating Divertor Performance?Divertor & SOL PhysicsGANoNoNo
45 detailsDifferences in Impurity Accumulation Between Resonant and Non-resonant RMP PlasmasELM ControlGANoNoNo
46 detailsDoes Added Baffling From Re-Configured Tiles on the Lower Divertor Shelf Facilitate Detachment?Divertor & SOL PhysicsGANoNoNo
47 detailsQuantifying the TBM torque, both in magnitude and radial locationPlasma RotationVTT Technical Research CentreNoNoNo
48 detailsDependence of momentum transport and intrinsic torque on rho* and betaPlasma RotationVTT Technical Research CentreNoYesNo
50 detailsImproved Heat Load Reduction Using Long Outer Divertor Leg Geometry During Puff and Pump OperationDivertor & SOL PhysicsGAYesNoNo
51 detailsStudy of chirping Alfvén eigenmodes in DIII-DEnergetic ParticlesPPPLNoYesNo
52 detailsControl of TAE/RSAE modes via external perturbationsEnergetic ParticlesPPPLNoNoNo
53 detailsQH-mode with low torque start-upInductive ScenariosGANoNoNo
55 detailsRMP Elm Suppression in DN PlasmasELM ControlORNLNoNoNo
56 detailsSawtooth ControlPlasma ControlORNLNoNoNo
57 detailsDevelop a high performance L-mode plasma.General PhysicsORNLYesNoNo
59 detailsEffect of Changing the Grad-B Drift Direction on Snowflake Divertor Behavior, Including DetachmentDivertor & SOL PhysicsGANoNoNo
60 detailsEffective NTM control in low torque plasmasStability & Disruption AvoidanceGANoNoNo
61 detailsEnergy Transport During Electron-Dominated Heating of ITER-Relevant H-Mode DischargesInductive ScenariosPPPLYesNoNo
62 detailsRMP assisted snowflake divertorDivertor & SOL PhysicsU of WisconsinYesNoNo
70 detailsDIMES test of misaligned CFC tile to establish size of misalignment needed to disrupt ITERPlasma-material InterfaceU of TorontoYesNoNo
71 details4. ELM Characterization to Validate BOUT++ ELM SimulationsPedestal StructureLLNLNoNoNo
72 detailsEnergy Transport During Electron-Dominated Heating of ITER-Relevant H-Mode DischargesTurbulence & TransportPPPLYesNoNo
73 detailsTest optimized TBM error field correction at higher values of betaStability & Disruption AvoidanceCRPP-EPFLYesNoNo
74 detailsOptimize TBM error field correction against field penetration in low NBI torque H-modesStability & Disruption AvoidanceCRPP-EPFLYesNoNo
75 detailsEvaluate the potential of correcting more than one mode component of the TBM error fieldStability & Disruption AvoidanceCRPP-EPFLYesNoNo
77 detailsInfluence of rotation and rotation shear on ELM suppressionELM ControlThe college of William and MaryYesNoNo
81 detailsActive Particle Exhaust of H-mode Plasmas in the Snowflake-minus Divertor ConfigurationDivertor & SOL PhysicsGANoNoNo
82 detailsIR Imaging of I-coil Induced Fast Ion LossesEnergetic ParticlesGANoYesNo
83 detailsEstablishing stationary I-mode with high performanceELM ControlMassachusetts Institute of TechnologyYesYesNo
84 detailsInfluence of resonant/non-resonant magnetic perturbation on particle confinement with n=2ELM ControlMax-Planck Institute for Plasma PhysicsYesYesNo
85 detailsCurrent profile control for stable ITER baseline scenario plasmasStability & Disruption AvoidanceColumbia UYesNoNo
86 detailsSafety Factor Scaling of Turbulence and Transport in Hybrid Scenario PlasmasTurbulence & TransportU of WisconsinNoNoNo
90 detailsCarbon-13 in He Plasma erosion/deposition experiment to benchmark DIVIMP code being used by ITERPlasma-material InterfaceCommonwealth Fusion SystemsNoNoNo
91 detailsComplete the Development of PCS n=2 Error Field Control AlgorithmStability & Disruption AvoidanceDepartment of EnergyYesNoNo
92 detailsH-mode Optimization of n=1&2 Error Field Control CurrentsStability & Disruption AvoidanceDepartment of EnergyYesNoNo
93 detailsActive Control of the EHO in Quiescent H-modesPlasma ControlDepartment of EnergyYesNoNo
94 detailsTurbulence Structure and Amplitude Variation with ExB Shear in H-mode PlasmasTurbulence & TransportU of WisconsinNoNoNo
95 detailsExperimental Validation of a Revised PCS Error Field CategoryPlasma ControlDepartment of EnergyNoNoNo
96 detailsEffect of Error Field Control Currents on Strike Point SplittingStability & Disruption AvoidanceDepartment of EnergyNoNoNo
97 detailsTime-resolved measurement of plasma response spectrumStability & Disruption AvoidanceColumbia UYesNoNo
98 detailsDevelop feedback-controlled MHD spectroscopyStability & Disruption AvoidanceColumbia UYesNoNo
99 detailsUnderstand and control resistive wall mode stability in high-qmin plasmasStability & Disruption AvoidanceColumbia UYesYesNo
100 detailsUnderstand resistive wall mode control physics in low-q95 plasmasStability & Disruption AvoidanceColumbia UYesNoNo
103 detailsProbing and controlling the L->H and H->L transitions by small pellet injectionL-H TransitionKorea Institute of Fusion EnergyYesNoNo
104 detailsComparision of small-ELM regimes in DIII-D and NSTXELM ControlU of WisconsinYesNoNo
105 detailsOptimization and exploration of the q95<2 scenario in DIII-DStability & Disruption AvoidanceConsorzio RFXYesNoNo
106 detailsMagnetic turbulence measurements in high beta H-mode dischargesTurbulence & TransportPPPLYesNoNo
107 detailsError field detection by application of a "spiraling" error fieldStability & Disruption AvoidanceORNLYesNoNo
108 detailsDisruption avoidance by forced magnetic spin-up of NTMsStability & Disruption AvoidanceORNLYesNoNo
109 detailsElectron Heat Transport in E-Dominated Heating of ITER-like H-Mode Discharges with Modulated ECHInductive ScenariosU of WisconsinYesNoNo
110 detailsElectron Heat Transport in E-Dominated Heating of ITER-like H-Mode Discharges with Modulated ECHTurbulence & TransportU of WisconsinYesNoNo
111 detailsDependence of I-mode on current direction and heating mixELM ControlMassachusetts Institute of TechnologyYesYesNo
112 details2D imaging of small ELMsELM ControlLos Alamos National LaboratoryYesNoNo
115 detailsQH-mode at low co-Ip torque using n=2 NRMFInductive ScenariosGANoNoNo
118 detailsDominant electron heated ITER baseline scenario studiesInductive ScenariosColumbia UYesNoNo
119 detailsImpact of fast-ions on the RWM stability boundaryStability & Disruption AvoidanceColumbia UYesYesNo
120 detailsOptimizing non-resonant, nonaxisymmetric fields in QH-modeInductive ScenariosGANoNoNo
121 detailsTesting Emerging Two-Fluid Model for RMP Plasma Response in Straightforward IWL PlasmasELM ControlORNLYesNoNo
122 detailsBid farewell to locked modes - NTM-locking avoidance by feedback synchronization assisted with ECCDStability & Disruption AvoidancePPPLYesNoNo
123 detailsBid farewell to locked modes - NTM-locking avoidance by feedback synchronization assisted with ECCDStability & Disruption AvoidancePPPLNoNoNo
124 detailsElectron Energy Transport during q0 control using modulated EC powerInductive ScenariosORNLNoNoNo
125 detailsObservation of non-linear interactions in fast-ion loss spectraEnergetic ParticlesPPPLNoNoNo
126 detailsTriggering ELMs at high frequency with PPPL Lithium granule injectorELM ControlRetired from PPPLYesNoNo
127 detailsCharacterization of Intense Bursts of Millimeter Wave Emission in QH-mode PlasmaInductive ScenariosUC, DavisYesNoNo
128 detailsCarbon-13 in He Plasma erosion/deposition experiment to benchmark DIVIMP code being used by ITERPlasma-material InterfaceCommonwealth Fusion SystemsNoNoNo
130 detailsSynergy between core-localized Alfven eigenmodes and edge localized TBM fields on fast ion losses.Energetic ParticlesPPPLNoYesNo
134 detailsPedestal stability and divertor transport studies with feedback-controlled snowflake configuration.Divertor & SOL PhysicsLLNLYesNoNo
138 detailsSSI target improvement by minimizing global low-n MHD activity in 1.5 Steady State Heating and Current DrivePPPLNoNoNo
140 detailsq0 control with Counter-ECCD in ITER Baseline DischargesInductive ScenariosRetiredNoNoNo
142 detailsELM heat transport in the snowflake divertor.Divertor & SOL PhysicsLLNLYesNoNo
143 detailsRMP ELM control at low torqueELM ControlUCSDYesNoNo
144 detailsValidation of kink response models with rotating n = 1 and n = 2 and phase flip n = 3 RMPsELM ControlUCSDYesNoNo
145 detailsExplore RMP ELM suppression mechanism at moderate collisionalityELM ControlUCSDNoNoNo
146 detailsELM suppression with Saturated wallsELM ControlUCSDYesNoNo
147 detailsNatural and Pellet-induced ELM behavior at low rotation/torqueELM ControlUCSDYesNoNo
148 detailsRadiative divertor control developmentDivertor & SOL PhysicsLLNLYesNoNo
149 detailsMeasurement of ion temperatures in the divertor region of DIII-D using the DiMES platformDivertor & SOL PhysicsU of Tennessee, KnoxvilleNoNoNo
150 detailsSensitivity study of toroidally-asymmetric halo current to error field during VDEDisruption MitigationPPPLNoNoNo
151 detailsITER SS Demo Discharge DocumentationsSteady State Heating and Current DriveRetiredNoNoNo
152 detailsTransport shortfall at high gyrobohm fluxTurbulence & TransportGANoNoNo
153 detailsControlling VH-mode with RMPs and comparison to NSTX EPH-modeELM ControlORNLYesNoNo
156 detailsControlling the timing and evolution of L-H and H-L with 3D fieldsPlasma ControlPPPLYesNoNo
158 detailsExpand the high li, betaN >4 operating regime through instability avoidance and higher heating powerSteady State Heating and Current DriveGANoNoNo
159 detailsCollisionality dependence of pedestal height with RMPPedestal StructureGAYesNoNo
160 detailsDependence of confinement and stability on toroidal rotation in high li dischargesSteady State Heating and Current DriveGANoNoNo
162 details210RT MSE and low rotation, elevated q_min steady-state scenario discharges at high betaNSteady State Heating and Current DriveGANoNoNo
163 detailsExploration of DEFC in the feedback stabilized plasma in low-q dischargesStability & Disruption AvoidancePPPLYesNoNo
164 detailsProduce fNI = 1 discharges at q_min near 1.5 using off-axis injection and a model guided approachSteady State Heating and Current DriveGANoNoNo
170 detailsNature of Energy Released During H-L Back TransitionL-H TransitionGANoNoNo
172 detailsHigh betaN with off-axis injection at reduced Bt (if 2011-level beam power is available)Steady State Heating and Current DriveGANoNoNo
173 detailsConfinement and fast ion diffusion in high betaN, steady-state scenario dischargesSteady State Heating and Current DriveGANoNoNo
174 detailsExploration of DEFC in the feedback stabilized plasma in low-q dischargesStability & Disruption AvoidancePPPLNoNoNo
175 detailsBeta collapse avoidance in SSI discharges by de-synchronizing toroidal harmonics by using feedbackSteady State Heating and Current DrivePPPLNoNoNo
176 detailsBeta collapse avoidance in SSI discharges by de-synchronizing toroidal harmonics by using feedbackSteady State Heating and Current DrivePPPLNoNoNo
177 detailsPossibility of â??Off-axis-Fishbone Mode and ELM Pacingâ?? due to Direct Energetic Particle CouplingELM ControlPPPLYesNoNo
178 detailsBeta limit and bootstrap current fraction in ITER steady-state scenario dischargesSteady State Heating and Current DriveGANoNoNo
179 detailsSnowflake in AT PlasmaSteady State Heating and Current DriveLLNLNoNoNo
180 detailsEstablish the incremental confinement of EC power in high betaN steady-state scenario dischargesSteady State Heating and Current DriveGANoNoNo
182 detailsSystematic test of paleoclassical transportTurbulence & TransportGANoNoNo
183 detailsMeasurement of multiple mechanisms in the low-density limit via ellipticity in the compass scanStability & Disruption AvoidanceColumbia UYesNoNo
185 detailsMeasure Plasma Response to RMPsELM ControlGAYesNoNo
186 detailsOptimal Mixing of I & C coils for n=1 EFCStability & Disruption AvoidanceColumbia UYesNoNo
187 detailsH-mode 3-D field optimization with purely kink-resonant and non-resonant n=1 fieldsStability & Disruption AvoidanceColumbia UYesNoNo
188 detailsExtension of proxy error field experiments to H-mode plasmasStability & Disruption AvoidanceColumbia UNoNoNo
189 detailsMeasurement of optimal n=2 phasing for RMP & ELM suppression without q95 windowsELM ControlColumbia UNoNoNo
190 detailsMeasurement of n=3 error field effects in RMP phase-flip experimentsELM ControlColumbia UNoNoNo
191 detailsCritical electric field for runaway electron growth and decay under quiescent conditionsDisruption MitigationColumbia UYesYesNo
192 detailsMeasurement of heat flux on the divertor using the embedded thermocouple arrayDivertor & SOL PhysicsU of Tennessee, KnoxvilleNoNoNo
193 detailsMagnetic perturbation amplitude scan to investigate RMP-induced damping of Zonal FlowsTurbulence & TransportU of WisconsinYesNoNo
194 detailsCorrelation of confinement and fluctuations with electron heating in ITER Baseline ScenarioInductive ScenariosGANoNoNo
195 detailsCorrelation of confinement and fluctuations with electron heating in ITER Baseline ScenarioTurbulence & TransportGANoNoNo
197 detailsScaling of divertor detachment onsetDivertor & SOL PhysicsGAYesNoNo
198 detailsCompare the power threshold for pre-emptive NTM suppression vs Catch and SubdueStability & Disruption AvoidancePPPLYesNoNo
199 detailsReducing the tearing island detection timeStability & Disruption AvoidancePPPLYesNoNo
200 detailsMultiple periods of NTM suppressionStability & Disruption AvoidancePPPLYesNoNo
201 detailsNTM Control Upgrade: Capibility to deposit EC at multiple locationsPlasma ControlPPPLYesNoNo
202 detailsError Field Correction Improvement: Adding BetaN dependenceStability & Disruption AvoidancePPPLYesNoNo
203 detailsDynamic plasma-wall equilibrium in ELMy H-modeDivertor & SOL PhysicsCompXYesNoNo
206 detailsStudies of arcing on divertor PFC surfacesPlasma-material InterfaceUCSDNoNoNo
207 detailsDust generation from deposited layers and leading edgesPlasma-material InterfaceUCSDNoNoNo
208 detailsqmin controlSteady State Heating and Current DrivePPPLYesNoNo
209 detailsRMP ELM-Control for Snowflake ConfigurationsTorkil Jensen AwardLLNLYesNoNo
210 detailsThe Dependence of Poloidal Rotation on TurbulencePlasma RotationGANoNoNo
211 detailsControl of experimentally simulated burning statePlasma ControlQSTYesNoNo
212 detailsIsland seeding with saw teeth pacing: New method to control tearing modesStability & Disruption AvoidancePPPLYesNoNo
213 detailsReal-time Ray Tracing for PCSPlasma ControlPPPLYesNoNo
214 detailsDensity (Greenwald) Limit and the Radiation Driven IslandsTorkil Jensen AwardPPPLYesNoNo
215 detailsControl of tungsten PFC erosion by local gas injectionPlasma-material InterfaceUCSDNoNoNo
216 detailsCampaign to study physics at the Greenwald limitSteady State Heating and Current DrivePPPLYesNoNo
217 detailsPID (proportional integral derivative)control of Error FieldStability & Disruption AvoidancePPPLYesNoNo
218 detailsControlled Snowflake Divertor StudyDivertor & SOL PhysicsPPPLYesNoNo
219 detailsEstablishing an experimental basis for plasma effects on magnetic islandsELM ControlGANoNoNo
221 detailsGas Injection Feedback with Radiation MeasurementsDivertor & SOL PhysicsPPPLYesNoNo
225 detailsStudy of atomic and molecular processes in deep detachment conditionsDivertor & SOL PhysicsLLNLYesNoNo
228 detailsHigh resolution study of collisionality and target structure in the transition to full detachmentDivertor & SOL PhysicsLLNLYesNoNo
230 detailsAssessment of the degree of detachment using NIR spectroscopyDivertor & SOL PhysicsLLNLYesNoNo
231 detailsStabilization of NTMs with ECCDStability & Disruption AvoidanceQSTNoYesNo
232 detailsBifurcated helical core equilibrium - continuedStability & Disruption AvoidanceU of WisconsinYesNoNo
233 detailsC erosion and D up-take at high surface temperaturePlasma-material InterfaceGANoNoNo
234 detailsStudy fishbone-like instability at the edge of QH-modesInductive ScenariosInstituto Superior Tecnico, Lisboa, PortugalNoNoNo
235 detailsHigh resolution Te pedestal measurements in RMP ELM suppression experimentsELM ControlSandia National LabNoNoNo
236 detailsWavenumber dependence of turbulence suppression in the L-H transitionL-H TransitionUCLANoNoNo
237 detailsCritical electric field for runaway electron growth and decay under quiescent conditionsDisruption MitigationMassachusetts Institute of TechnologyYesYesNo
238 detailsDirect Measurement of NTV TorqueStability & Disruption AvoidanceColumbia UYesNoNo
239 detailsContinuous Scan of NTV Torque Across Low Rotation PeakStability & Disruption AvoidanceColumbia UYesNoNo
240 detailsOptimization of Applied Error Field Spectrum for NTVStability & Disruption AvoidanceColumbia UYesNoNo
241 detailsC-13 and background carbonPlasma-material InterfaceGANoNoNo
242 detailsq95 < 2 Tokamak Operation Via Dynamic Error Field CorrectionStability & Disruption AvoidanceGANoNoNo
243 details256: SOL width and divertor peak heat flux in QH-mode plasmas with/without n=3 fieldsInductive ScenariosGANoNoNo
244 detailsStudy NRMF driven torque in ECH-only heated plasma (ELMing H-modes)Plasma RotationGANoNoNo
245 detailsInvestigate the physics of NTM suppression by large externally applied helical fieldsTorkil Jensen AwardGANoNoNo
246 detailsDevelop low-torque, high normalized fusion performance QH-mode for ITER baseline scenarioInductive ScenariosGANoNoNo
247 detailsDevelop low-torque, high normalized fusion performance QH-mode for FNSF-AT scenarioInductive ScenariosGANoNoNo
248 detailsInvestigate elongation limit in low li discharges with/without applied 3D magnetic fieldsTorkil Jensen AwardGANoNoNo
249 detailsSteady-state high beta with NCS and qmin>2Steady State Heating and Current DriveGANoNoNo
251 detailsNew Study of Alfven Eigenmodes Induced Fast Ion Transport/LossEnergetic ParticlesGANoNoNo
252 detailsImplement finite-state Off Normal Fault Response systemPlasma ControlGANoNoNo
253 detailsStudy QH-mode with advanced fast ion diagnostics and codesInductive ScenariosGANoNoNo
254 detailsNeon SPI injection into early CQ to stunt RE formationDisruption MitigationGANoNoNo
255 detailsSuper H-ModeTorkil Jensen AwardORNLYesNoNo
256 detailsFine scale stepwise q-scan: role of low-order rationales and resonance condition for ELM suppressionELM ControlU of WisconsinNoNoNo
257 detailsTransport Investigation During Slow Current Ramp-Up and Ramp-Down [for ITER]Inductive ScenariosU of WisconsinNoYesNo
258 detailsMain-ion and impurity rotation in helium plasmasPlasma RotationGANoNoNo
259 detailsHelium Campaign (D beams)General PhysicsGANoNoNo
260 detailsITER Baseline Scenario DemonstrationInductive ScenariosITER OrganizationNoYesNo
261 detailsDemonstration of stationary inductive solutions at low and moderate q95Inductive ScenariosITER OrganizationNoNoNo
262 detailsTest Pedestal Structure Model Where Paleoclassical Transport Is DominantPedestal StructureU of WisconsinNoNoNo
265 detailso Experiments using the centerpost Swing-probesDivertor & SOL PhysicsUCSDNoNoNo
266 detailsUnderstand resistive wall mode control physics in low-q95 plasmasInductive ScenariosColumbia UNoNoNo
267 detailsUnderstand and control resistive wall mode stability in high-qmin plasmasSteady State Heating and Current DriveColumbia UNoNoNo
268 detailsnu* dimensionless scalingTurbulence & TransportCEANoYesNo
270 detailsL-mode Turbulence and L-H Transition Characterization in Snowflake Divertor PlasmasDivertor & SOL PhysicsLLNLYesNoNo
272 detailsDither injection for closed-loop system identification of vacuum and plasma responseTorkil Jensen AwardKTHYesNoNo
273 detailsSawtooth control via n=1 external magnetic perturbationTorkil Jensen AwardConsorzio RFX and Padova UYesNoNo
277 detailsECH effects on low or balanced torque discharges in DIII-DPlasma RotationNational Fusion Research Institute (NFRI), KoreaYesYesNo
278 detailsPossibility of â??Off-axis-Fishbone Mode and ELM Pacingâ?? due to Direct Energetic Particle CouplingELM ControlJAEANoNoNo
279 detailsECH effects on low or balanced torque discharges in DIII-DPlasma RotationNational Fusion Research Institute (NFRI), KoreaYesYesNo
280 details: Trigger-less onset of NTMs with PEC and NTV effects on rotation regimePlasma RotationIstituto di Fisica del Plasma, Euratom-ENEA-CNRNoNoNo
281 detailsECH effects on low or balanced torque discharges in DIII-DPlasma RotationNational Fusion Research Institute (NFRI), KoreaYesYesNo
283 detailsITER Baseline Scenario Operation near the LH ThresholdInductive ScenariosITER OrganizationNoYesNo
284 detailsAccess conditions for steady-state operation in ITERSteady State Heating and Current DriveITER OrganizationNoYesNo
285 detailsAccess to advanced inductive operation in ITERInductive ScenariosITER OrganizationNoYesNo
286 detailsCollisionality scaling of confinement in advanced inductive regimesInductive ScenariosITER OrganizationNoYesNo
287 detailsHigh li steady-state scenario developmentSteady State Heating and Current DriveITER OrganizationNoNoNo
288 detailsAmplifying the Geodesic Acoustic Mode via Resonant Radial Field Amplification: New MethodsTurbulence & TransportU of WisconsinNoNoNo
289 detailsDemonstrate access to beta_N=5 with min(q)>2Steady State Heating and Current DriveITER OrganizationNoNoNo
290 detailsEffect of n=2 Poloidal Spectrum on NTV TorquePlasma RotationDepartment of EnergyNoNoNo
291 detailsTrigger-less onset of NTMs with P_EC and NTV effects on rotation regimeStability & Disruption AvoidanceInstituto Superior Tecnico, Lisboa, PortugalNoNoNo
292 detailsOptimize electron pedestal pressure in low-torque ITER baseline plasmasInductive ScenariosUCLANoNoNo
293 detailsTest of ETG zeff supressionTurbulence & TransportGANoNoNo
294 detailsSimulated Alpha particle dillutionTurbulence & TransportGANoNoNo
295 detailspreliminary simulated burn controlTurbulence & TransportGANoNoNo
297 detailsITER baseline scenario with low NBI torqueInductive ScenariosGANoNoNo
298 detailsSoft landing with 2/1 TM in the ITER shapeStability & Disruption AvoidanceGANoNoNo
299 detailsAspect ratio scaling of turbulence and transport: DIII-D and NSTX-U comparisonTurbulence & TransportUniv. Wisconsin (at PPPL)NoNoNo
300 detailsEffect of triangularity in ITER shape and improved shapingInductive ScenariosGANoNoNo
301 detailsAccess to the small ELM regime with a shape controlELM ControlORNLYesNoNo
302 detailsRMP ELM Suppression at the NTV Offset RotationELM ControlGANoNoNo
303 detailsEffect on lithium wall conditioning for Co-QH-mode and edge pedestal characteristicsInductive ScenariosGANoNoNo
304 detailsBirth of ITER: the world's largest resistorGeneral PhysicsGANoNoNo
305 detailsScaling Of Pedestal Plasma Transport With RMP I-coil CurrentELM ControlU of WisconsinNoNoNo
306 detailsEdge turbulence and blob generationDivertor & SOL PhysicsUniv. WisconsinNoNoNo
307 detailsRole of turbulent-driven and Ion pressure gradient-sustained ExB flows in Triggering H-modeL-H TransitionUCSDNoNoNo
308 detailsRMP (Resonant Magnetic Perturbation) code validation via UCLA 288 GHz polarimeterELM ControlUCLANoNoNo
310 detailsEnergy Transport During Electron-Dominated Heating of ITER-Relevant H-Mode DischargesSteady State Heating and Current DrivePPPLNoNoNo
311 detailsTransport with qmin>2Steady State Heating and Current DriveLLNLNoNoNo
312 detailsLimits to pedestal radiation high beta dischargesSteady State Heating and Current DriveGANoNoNo
313 detailsHybrids with co-NBI QH-mode edgeInductive ScenariosGANoNoNo
315 detailsCurrent profile control model requirementsPlasma ControlGANoNoNo
316 detailsModel-based control of the current profile and βN for steady state scenariosPlasma ControlCadaracheNoNoNo
317 detailsStudy on sawteeth in the neutral beam (NB) heated plasmasStability & Disruption AvoidanceKorea National Fusion Research CenterNoNoNo
318 detailsCurrent profile control for stable ITER baseline scenario plasmasInductive ScenariosColumbia UNoNoNo
319 detailsImpact of fast-ions on the RWM stability boundaryGeneral PhysicsColumbia UNoNoNo
320 detailsRWM excitation in the SSI target by reducing triangularity"Stability & Disruption AvoidancePPPLNoNoNo
321 detailsAccess to low torque QH-mode using high beta low torque AI target with NRMFInductive ScenariosGANoNoNo
322 detailsELM pacing in low torque, electron heated ITER baselineInductive ScenariosGANoNoNo
323 detailsAccess to QH-mode with low NBI torqueInductive ScenariosGANoNoNo
324 detailsDocument turbulence change with rotation in AI, and compare with theoryInductive ScenariosGANoNoNo
325 detailsDocument turbulence change with rotation in AI, and compare with theoryTurbulence & TransportGANoNoNo
326 detailsUnderstand mechanisms by which ECH influences NTM stablilityStability & Disruption AvoidanceGANoNoNo
327 detailsrho* scaling of intrinsic torque between DIII-D and JETPlasma RotationGANoYesNo
328 detailsError field correction at low rotationStability & Disruption AvoidanceGANoNoNo
329 detailsDiscussion of plasma rotation transient process during OFM/ELM-driven RWM w/wo feedback usinStability & Disruption AvoidancePPPLNoNoNo
330 detailsQH-mode with TBMInductive ScenariosGANoNoNo
331 detailsQH-mode with TBM (dup 330)Stability & Disruption AvoidanceGANoNoNo
332 detailsDemonstration of noninductive Q=5 scenario in ITER shape using off-axis NBISteady State Heating and Current DriveORNLNoNoNo
333 detailsFar off-axis NBCDSteady State Heating and Current DriveORNLNoNoNo
334 detailsMeasurement of neoclassical response of off-axis beam ionsSteady State Heating and Current DriveORNLNoNoNo
335 detailsOff-axis NBCD measurement in steady state scenarioSteady State Heating and Current DriveORNLNoNoNo
336 detailsRoutine current profile control in operationSteady State Heating and Current DriveGANoNoNo
337 detailsRoutine current profile control in operationInductive ScenariosGANoNoNo
339 detailsCombined effect of TBM and NTM fields on fast-ion confinementStability & Disruption AvoidanceUC, IrvineNoYesNo
340 detailsCombined effect of TBM and Sawtooth fields on fast-ion confinementStability & Disruption AvoidanceUC, IrvineNoYesNo
344 detailsEvaluating Physics of QH-mode Stationary Enhanced Confinement Regime Without ELMs for the 2013 JInductive ScenariosLLNLNoNoNo
345 detailsEvaluating Physics of I-mode Stationary Enhanced Confinement Regime Without ELMs for the 2013 JRELM ControlLLNLNoNoNo
346 detailsControl of H-L back transition via applied RMP fieldsL-H TransitionUCLANoNoNo
347 detailsDo differences in co/cnter GAM/ZF behavior affect deficit in gyrokinetic predicted Lmode transport?Turbulence & TransportUCLANoNoNo
348 detailsCan we obtain ELM suppression without substantial loss of density?ELM ControlUCLANoNoNo
349 detailsDensity/current Scaling of Intrinsic Rotation and ITG/TEM TransitionTurbulence & TransportUCLANoNoNo
350 detailsCurrent/Density Scaling of Intrinsic Rotation and ITG/TEM TransitionPlasma RotationUCLANoNoNo
351 detailsConfinement enhancement via impurity-seeding of H-mode plasmasTurbulence & TransportU of WisconsinNoNoNo
352 detailsDoes increased turbulence in H-mode degrade agreement of GK transport/turbulence simulations?Turbulence & TransportUCLANoNoNo
353 detailsCorrelation length of electron temperature turbulence measurement and comparison with simulationsTurbulence & TransportUCLANoNoNo
354 detailsControl of Major Disruptions in DIII-DStability & Disruption AvoidanceColumbia UNoNoNo
355 detailsq dependence of L-H transition power thresholdL-H TransitionUCLANoNoNo
356 detailsGAM eigenmode excitation mechanismTurbulence & TransportUCLANoNoNo
357 detailsGAM eigenmode 2D structureTurbulence & TransportUCLANoNoNo
359 detailsq95 scaling of the coupled turbulence/zonal flow during LH transitionL-H TransitionU of WisconsinNoNoNo
360 detailsdensity scaling and X-point position scan of LH transition power thresholdL-H TransitionU of WisconsinNoNoNo
361 detailsDither injection for closed-loop system identification of vacuum and plasma responseStability & Disruption AvoidanceConsultantNoNoNo
362 detailsInvestigation of GAMs during I-mode on D3DTurbulence & TransportMassachusetts Institute of TechnologyNoYesNo
363 detailsTBM mockup simulating ITER GDC with ferritic materialsGeneral PhysicsGANoNoNo
364 detailsAbsolute plasma response null measurement by multiple betaN stepsStability & Disruption AvoidanceColumbia UNoNoNo
365 detailsLithium dropper commissioning and ELM modificationGeneral PhysicsGANoNoNo
366 detailsUp/down Asymmetric EFCStability & Disruption AvoidanceDepartment of EnergyNoNoNo
367 detailsJET/DIII-D similarity experiment on rotation in plasmas with low momentum inputPlasma RotationInstituto Superior Tecnico, Lisboa, PortugalNoYesNo
369 detailsFirst-principles-driven Model-based Current-profile Control in H-mode DischargesPlasma ControlLehigh UNoNoNo
370 detailsParticle pinch in pedestalPedestal StructureGANoNoNo
371 detailsEffect of icoil current on energy confinement in RMP ELM-suppressed dischargesELM ControlGANoNoNo
372 detailsPedestal optimization via impurity injectionPedestal StructureORNLNoNoNo
373 detailsPedestal optimization in VH modePedestal StructureORNLNoNoNo
374 detailsPedestal optimization with RMP ELM ControlPedestal StructureORNLNoNoNo
375 detailsQH-mode pedestal optimizationInductive ScenariosORNLNoNoNo
376 detailsRole of q and magnetic shear of pedestal formation time and turbulent transportPedestal StructurePPPLNoNoNo
377 detailsNTM locking disruption avoidance by the EM torque with toroidal-phase forward magnetic feedDisruption MitigationPPPLNoNoNo
378 detailsStudy of the connection between I-mode and low density Type III ELMs and optimization of I-modeELM ControlGANoNoNo
379 detailsPedestal optimization of ITER baseline scenario discharges.Pedestal StructureGANoNoNo
380 detailsELM Suppression at Lower Collisionality with Non-Resonant n=3 I-coilELM ControlGANoNoNo
381 detailsSearch for turbulence at ion-cyclotron frequenciesTurbulence & TransportUCLANoNoNo
382 detailsTransport and turbulence characterization experimentSteady State Heating and Current DriveUCLANoNoNo