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
280: Trigger-less onset of NTMs with PEC and NTV effects on rotation regimePlasma RotationIstituto di Fisica del Plasma, Euratom-ENEA-CNRNoNoNo
162210RT MSE and low rotation, elevated q_min steady-state scenario discharges at high betaNSteady State Heating and Current DriveGANoNoNo
527256: SOL width and divertor peak heat flux in QH-mode plasmas with/without n=3 fieldsInductive ScenariosGANoNoNo
243256: SOL width and divertor peak heat flux in QH-mode plasmas with/without n=3 fieldsInductive ScenariosGANoNoNo
1122D imaging of small ELMsELM ControlLos Alamos National LaboratoryYesNoNo
3873-D Fields and ECH Density PumpoutTurbulence & TransportGANoNoNo
173-D Fields and ECH Density PumpoutTurbulence & TransportGANoNoNo
7803D coil based BetaN control instead of NBI based BetaN control.Steady State Heating and Current DrivePPPLNoNoNo
7283D Fields Effects on Critical Gradient and TurbulenceTurbulence & TransportGANoNoNo
4743D material migration during RMP ELM suppressionPlasma-material InterfaceU of WisconsinYesYesNo
714. ELM Characterization to Validate BOUT++ ELM SimulationsPedestal StructureLLNLNoNoNo
708444: Identify the Optimal Impurity for High Power High Performance Plasmas During Radiating Divertor OpsSteady State Heating and Current DriveGANoNoNo
686â??Born-lockedâ?? mode control by ECCD and magnetic perturbationsStability & Disruption AvoidanceColumbia UNoNoNo
364Absolute plasma response null measurement by multiple betaN stepsStability & Disruption AvoidanceColumbia UNoNoNo
611Absolute plasma response null measurement by multiple betaN stepsStability & Disruption AvoidanceColumbia UNoNoNo
284Access conditions for steady-state operation in ITERSteady State Heating and Current DriveITER OrganizationNoYesNo
405Access conditions for steady-state operation in ITERSteady State Heating and Current DriveITER OrganizationNoYesNo
285Access to advanced inductive operation in ITERInductive ScenariosITER OrganizationNoYesNo
408Access to advanced inductive operation in ITERInductive ScenariosITER OrganizationNoYesNo
321Access to low torque QH-mode using high beta low torque AI target with NRMFInductive ScenariosGANoNoNo
645Access to low torque QH-mode using high beta low torque AI target with NRMFInductive ScenariosGANoNoNo
323Access to QH-mode with low NBI torqueInductive ScenariosGANoNoNo
301Access to the small ELM regime with a shape controlELM ControlORNLYesNoNo
415Access to zero torque advanced inductive with direct stabilization of the 2/1 mode by ECCDInductive ScenariosITER OrganizationNoNoNo
651Achieve QH-mode plasmas with Te, Ti ~ 10 keV near mid-radiusTurbulence & TransportUCLANoNoNo
93Active Control of the EHO in Quiescent H-modesPlasma ControlDepartment of EnergyYesNoNo
785Active determination of angular momentum transfer process between 3D structures: NTM 2/1 and 3/2 moStability & Disruption AvoidancePPPLNoNoNo
441Active Particle Exhaust of H-mode Plasmas in the Snowflake-minus Divertor ConfigurationDivertor & SOL PhysicsGANoNoNo
81Active Particle Exhaust of H-mode Plasmas in the Snowflake-minus Divertor ConfigurationDivertor & SOL PhysicsGANoNoNo
687Add modulated ECCD to f/back or f/fwd entrainment dischargesStability & Disruption AvoidanceColumbia UNoNoNo
288Amplifying the Geodesic Acoustic Mode via Resonant Radial Field Amplification: New MethodsTurbulence & TransportU of WisconsinNoNoNo
682Amplifying the Geodesic Acoustic Mode via Resonant Radial Field Amplification: New MethodsTurbulence & TransportU of WisconsinNoNoNo
600Anomalous current diffusion in steady-state hybrid scenario with ELM suppressionSteady 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
594Aspect ratio scaling of turbulence and transport: DIII-D and NSTX-U comparisonTurbulence & TransportU of WisconsinNoNoNo
299Aspect ratio scaling of turbulence and transport: DIII-D and NSTX-U comparisonTurbulence & TransportUniv. Wisconsin (at PPPL)NoNoNo
689Assess optimal Error Field Correction by modulating I-coils at incommensurable frequenciesStability & Disruption AvoidanceColumbia UNoNoNo
716Assess the destabilization mechanism for the n = 1 tearing mode in steady-state scenario dischargesSteady State Heating and Current DriveGANoNoNo
674Assessing the Need for Using Two Impurity Species in Radiating DivertorDivertor & SOL PhysicsGANoNoNo
22Assessment of main chamber carbon sourcesDivertor & SOL PhysicsAalto UNoNoNo
778Assessment of main chamber carbon sourcesDivertor & SOL PhysicsAalto UNoNoNo
230Assessment of the degree of detachment using NIR spectroscopyDivertor & SOL PhysicsLLNLYesNoNo
440Beam Density Affects on Carbon Density ProfileTurbulence & TransportGANoNoNo
769benchmark heat flux with fast TCsDivertor & SOL PhysicsSandia National LabNoNoNo
565Benign 3/2 NTM Formation to avoid 2/1 NTM lockingStability & 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
797BetaN control with 3D CoilsPlasma ControlPPPLNoNoNo
638BetaN control with 3D Fields instead of NBIInductive ScenariosPPPLNoNoNo
533Between-shots gyrokinetic stability analysisTurbulence & TransportMassachusetts Institute of TechnologyNoNoNo
122Bid farewell to locked modes - NTM-locking avoidance by feedback synchronization assisted with ECCDStability & Disruption AvoidancePPPLYesNoNo
123Bid farewell to locked modes - NTM-locking avoidance by feedback synchronization assisted with ECCDStability & Disruption AvoidancePPPLNoNoNo
232Bifurcated helical core equilibrium - continuedStability & Disruption AvoidanceU of WisconsinYesNoNo
304Birth of ITER: the world's largest resistorGeneral PhysicsGANoNoNo
553Bootstrap Current Change During RMP ELM SuppressionELM ControlGANoNoNo
802Breakdown Optimization with ECHPlasma ControlGANoNoNo
416Burn Control in ITER Baseline ScenarioInductive ScenariosITER OrganizationNoYesNo
233C erosion and D up-take at high surface temperaturePlasma-material InterfaceGANoNoNo
1C vs I Coil NTVPlasma RotationGANoNoNo
241C-13 and background carbonPlasma-material InterfaceGANoNoNo
770Calibrated passive FIDA spectrumEnergetic ParticlesUC, IrvineNoNoNo
38Calibrated passive FIDA spectrumEnergetic ParticlesUC, IrvineNoNoNo
643Campaign to study physics at the Greenwald limitSteady State Heating and Current DrivePPPLNoNoNo
216Campaign to study physics at the Greenwald limitSteady State Heating and Current DrivePPPLYesNoNo
44Can Nitrogen impurity Seeding Improve Radiating Divertor Performance?Divertor & SOL PhysicsGANoNoNo
781Can RMP ELM Control be reliably used in ITER (or a reactor)?ELM ControlPPPLNoNoNo
348Can we obtain ELM suppression without substantial loss of density?ELM ControlUCLANoNoNo
90Carbon-13 in He Plasma erosion/deposition experiment to benchmark DIVIMP code being used by ITERPlasma-material InterfaceCommonwealth Fusion SystemsNoNoNo
128Carbon-13 in He Plasma erosion/deposition experiment to benchmark DIVIMP code being used by ITERPlasma-material InterfaceCommonwealth Fusion SystemsNoNoNo
497Cause(s) for the rotation degradation and tearing instabilities of the ITER baseline scenarioInductive ScenariosColumbia UNoNoNo
757Cause(s) for the rotation degradation and tearing instabilities of the ITER baseline scenarioStability & Disruption AvoidanceColumbia UNoNoNo
617Characterization of core/pedestal density limits for rotating tearing modesStability & Disruption AvoidanceColumbia UNoNoNo
127Characterization of Intense Bursts of Millimeter Wave Emission in QH-mode PlasmaInductive ScenariosUC, DavisYesNoNo
427Collisionality dependence of intrinsic rotationPlasma RotationUCSDNoNoNo
159Collisionality dependence of pedestal height with RMPPedestal StructureGAYesNoNo
801Collisionality dependence of pedestal height with RMPELM ControlGANoNoNo
393collisionality impact on momentum and particle transportTurbulence & TransportThe college of William and MaryNoNoNo
409Collisionality scaling of confinement in advanced inductive regimesInductive ScenariosITER OrganizationNoYesNo
286Collisionality scaling of confinement in advanced inductive regimesInductive ScenariosITER OrganizationNoYesNo
572Collisionality Scaling of High-Beta, Steady-State HybridsSteady State Heating and Current DriveGAYesNoNo
580Collisionality/density dependence and Pedestal optimization with ELM SupELM ControlGANoYesNo
792Combined Core and Divertor Radiation Control: Gas Injection Feedback with Radiation MeasurementsPlasma ControlPPPLNoNoNo
339Combined effect of TBM and NTM fields on fast-ion confinementStability & Disruption AvoidanceUC, IrvineNoYesNo
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
340Combined effect of TBM and Sawtooth fields on fast-ion confinementStability & Disruption AvoidanceUC, IrvineNoYesNo
13Compare edge particle transport in ELMing H-mode and QH-mode with and without NRMFInductive ScenariosGANoNoNo
8Compare Mach probe and CER measurements of intrinsic rotation profile of main ions in helium plasmaPlasma RotationGANoNoNo
198Compare the power threshold for pre-emptive NTM suppression vs Catch and SubdueStability & Disruption AvoidancePPPLYesNoNo
718Compare the power threshold for pre-emptive NTM suppression vs Catch and SubdueStability & Disruption AvoidancePPPLNoNoNo
711Comparision DIII-D and AUG high collisionality ELM response to 3D magnetic perturbationsELM ControlGANoNoNo
104Comparision of small-ELM regimes in DIII-D and NSTXELM ControlU of WisconsinYesNoNo
417Comparison of H-Mode Transport with Co- and Ctr-NBITurbulence & TransportITER OrganizationNoNoNo
42Compatibility of High Performance Plasmas With a Puff-and-Pump Radiating DivertorSteady State Heating and Current DriveGANoNoNo
91Complete the Development of PCS n=2 Error Field Control AlgorithmStability & Disruption AvoidanceDepartment of EnergyYesNoNo
173Confinement and fast ion diffusion in high betaN, steady-state scenario dischargesSteady State Heating and Current DriveGANoNoNo
447Confinement and stability properties of 'resonant' MHD rotationPlasma RotationLos Alamos National LaboratoryYesNoNo
683Confinement enhancement via impurity-seeding of H-mode plasmasTurbulence & TransportU of WisconsinNoNoNo
351Confinement enhancement via impurity-seeding of H-mode plasmasTurbulence & TransportU of WisconsinNoNoNo
239Continuous Scan of NTV Torque Across Low Rotation PeakStability & Disruption AvoidanceColumbia UYesNoNo
211Control of experimentally simulated burning statePlasma ControlQSTYesNoNo
346Control of H-L back transition via applied RMP fieldsL-H TransitionUCLANoNoNo
543Control of high-Z PFC erosion by local gas injectionPlasma-material InterfaceUCSDYesNoNo
354Control of Major Disruptions in DIII-DStability & Disruption AvoidanceColumbia UNoNoNo
52Control of TAE/RSAE modes via external perturbationsEnergetic ParticlesPPPLNoNoNo
14Control of toroidal mode number of EHOInductive ScenariosGANoNoNo
601Control of tungsten PFC erosion by local gas injectionPlasma-material InterfaceGANoNoNo
215Control of tungsten PFC erosion by local gas injectionPlasma-material InterfaceUCSDNoNoNo
776Control/Ops Evening Development TimePlasma ControlGANoNoNo
218Controlled Snowflake Divertor StudyDivertor & SOL PhysicsPPPLYesNoNo
644Controlled Snowflake Divertor StudyDivertor & SOL PhysicsPPPLNoNoNo
156Controlling the timing and evolution of L-H and H-L with 3D fieldsPlasma ControlPPPLYesNoNo
618Controlling VH-mode with RMPs and comparison to NSTX EPH-modeELM ControlPPPLNoNoNo
153Controlling VH-mode with RMPs and comparison to NSTX EPH-modeELM ControlORNLYesNoNo
353Correlation length of electron temperature turbulence measurement and comparison with simulationsTurbulence & TransportUCLANoNoNo
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
27COupling between core and SOL parallel flowDivertor & SOL PhysicsUCSDNoNoNo
434COupling between core and SOL parallel flowDivertor & SOL PhysicsUCSDNoNoNo
423Coupling of multi-channel transport and turbulence across rotation reversalsPlasma RotationMassachusetts Institute of TechnologyYesYesNo
237Critical electric field for runaway electron growth and decay under quiescent conditionsDisruption MitigationMassachusetts Institute of TechnologyYesYesNo
191Critical electric field for runaway electron growth and decay under quiescent conditionsDisruption MitigationColumbia UYesYesNo
85Current profile control for stable ITER baseline scenario plasmasStability & Disruption AvoidanceColumbia UYesNoNo
318Current profile control for stable ITER baseline scenario plasmasInductive ScenariosColumbia UNoNoNo
315Current profile control model requirementsPlasma ControlGANoNoNo
350Current/Density Scaling of Intrinsic Rotation and ITG/TEM TransitionPlasma RotationUCLANoNoNo
391Current/Density Scaling of Intrinsic Rotation and ITG/TEM TransitionPlasma RotationUCLANoNoNo
413Demonstrate access to beta_N=5 with min(q)>2Steady State Heating and Current DriveITER OrganizationNoNoNo
289Demonstrate access to beta_N=5 with min(q)>2Steady State Heating and Current DriveITER OrganizationNoNoNo
593Demonstrating Stiffness of Electron Heat Transport in the Presence of Strong RadiationTurbulence & TransportMassachusetts Institute of TechnologyNoNoNo
332Demonstration of noninductive Q=5 scenario in ITER shape using off-axis NBISteady State Heating and Current DriveORNLNoNoNo
261Demonstration of stationary inductive solutions at low and moderate q95Inductive ScenariosITER OrganizationNoNoNo
411Demonstration of stationary inductive solutions at low and moderate q95Inductive ScenariosITER OrganizationNoNoNo
557Density (Greenwald) Limit and the Radiation Driven IslandsTorkil Jensen AwardPPPLYesNoNo
214Density (Greenwald) Limit and the Radiation Driven IslandsTorkil Jensen AwardPPPLYesNoNo
43Density Control and Active Impurity Removal from Double-null H-mode PlasmasDivertor & SOL PhysicsGANoNoNo
448Density Control and Active Impurity Removal from Double-null H-mode PlasmasInductive ScenariosGANoNoNo
798Density matching with and without ELMs.ELM ControlGANoNoNo
754density scaling and X-point position scan of LH transition power thresholdL-H TransitionU of WisconsinNoNoNo
360density scaling and X-point position scan of LH transition power thresholdL-H TransitionU of WisconsinNoNoNo
349Density/current Scaling of Intrinsic Rotation and ITG/TEM TransitionTurbulence & TransportUCLANoNoNo
160Dependence of confinement and stability on toroidal rotation in high li dischargesSteady State Heating and Current DriveGANoNoNo
521Dependence of confinement and stability on toroidal rotation in high li dischargesSteady State Heating and Current DriveGANoNoNo
111Dependence of I-mode on current direction and heating mixELM ControlMassachusetts Institute of TechnologyYesYesNo
461Dependence of momentum transport and intrinsic torque on rho* and betaPlasma RotationVTT Technical Research CentreNoYesNo
48Dependence of momentum transport and intrinsic torque on rho* and betaPlasma RotationVTT Technical Research CentreNoYesNo
660Dependence of non-axisymmetric plasma response on plasma rotationStability & Disruption AvoidanceGANoNoNo
729Dependence of pedestal structure on collisionality and Zeff in relation to JET results with ILWPedestal StructureGANoYesNo
790Detachment Control for H-modeDivertor & SOL PhysicsPPPLNoNoNo
791Detachment Control for H-modePlasma ControlPPPLNoNoNo
786Determining Particle Sources/Sinks in ITER-like NN Discharges during RMP ELM suppressionELM ControlORNLNoNoNo
57Develop a high performance L-mode plasma.General PhysicsORNLYesNoNo
705Develop feedback-controlled 3D equilibriaStability & Disruption AvoidanceColumbia UNoNoNo
98Develop feedback-controlled MHD spectroscopyStability & Disruption AvoidanceColumbia UYesNoNo
247Develop low-torque, high normalized fusion performance QH-mode for FNSF-AT scenarioInductive ScenariosGANoNoNo
246Develop low-torque, high normalized fusion performance QH-mode for ITER baseline scenarioInductive ScenariosGANoNoNo
534Develop low-torque, high normalized fusion performance QH-mode for ITER baseline scenarioInductive ScenariosGANoNoNo
799Development for PID-controlled boundary radial fieldPlasma ControlConsultantNoNoNo
470Development of Fully Noninductive High Beta EAST ScenarioSteady State Heating and Current DriveASIPPYesNoNo
783Development of Fully Noninductive High Beta EAST Scenario IISteady State Heating and Current DriveGANoNoNo
412Development of Reproducible Startup and Target q Profile Control for Steady State ScenariosSteady State Heating and Current DriveITER OrganizationNoNoNo
12Diagnostic spatial cross calibration using edge sweeps in QH-modePedestal StructureGANoNoNo
492Diagnostic spatial cross calibration using edge sweeps in QH-modePedestal StructureGANoNoNo
45Differences in Impurity Accumulation Between Resonant and Non-resonant RMP PlasmasELM ControlGANoNoNo
751Dimensionless Identity Experiments in I-Mode with C-Mod and AUG (TC-18)Pedestal StructureMassachusetts Institute of TechnologyNoYesNo
70DIMES test of misaligned CFC tile to establish size of misalignment needed to disrupt ITERPlasma-material InterfaceU of TorontoYesNoNo
607Direct measurement of E-coil contribution to intrinsic EFStability & Disruption AvoidanceColumbia UNoNoNo
238Direct Measurement of NTV TorqueStability & Disruption AvoidanceColumbia UYesNoNo
329Discussion of plasma rotation transient process during OFM/ELM-driven RWM w/wo feedback usinStability & Disruption AvoidancePPPLNoNoNo
489Discussion of plasma rotation transient process during OFM/ELM-driven RWM w/wo feedback usinEnergetic ParticlesPPPLNoNoNo
108Disruption avoidance by forced magnetic spin-up of NTMsStability & Disruption AvoidanceORNLYesNoNo
451Disruption mitigation by differential rotation of internal MHDStability & Disruption AvoidanceLos Alamos National LaboratoryYesNoNo
625Disruption Precursor IdentificationDisruption MitigationU of Colorado, BoulderNoNoNo
747Dissipation & Control of RE from ITER-like LSN targetsDisruption MitigationGANoNoNo
733Distinguishing between 3d magnetic field structures and transportELM ControlORNLNoNoNo
771Distribution function inversion benchmarkEnergetic ParticlesUC, IrvineNoNoNo
361Dither injection for closed-loop system identification of vacuum and plasma responseStability & Disruption AvoidanceConsultantNoNoNo
698Dither injection for closed-loop system identification of vacuum and plasma responseStability & Disruption AvoidanceConsultantNoNoNo
272Dither injection for closed-loop system identification of vacuum and plasma responseTorkil Jensen AwardKTHYesNoNo
752Divertor detachment versus toroidal field and plasma currentDivertor & SOL PhysicsGANoYesNo
347Do differences in co/cnter GAM/ZF behavior affect deficit in gyrokinetic predicted Lmode transport?Turbulence & TransportUCLANoNoNo
324Document turbulence change with rotation in AI, and compare with theoryInductive ScenariosGANoNoNo
325Document turbulence change with rotation in AI, and compare with theoryTurbulence & TransportGANoNoNo
46Does Added Baffling From Re-Configured Tiles on the Lower Divertor Shelf Facilitate Detachment?Divertor & SOL PhysicsGANoNoNo
352Does increased turbulence in H-mode degrade agreement of GK transport/turbulence simulations?Turbulence & TransportUCLANoNoNo
118Dominant electron heated ITER baseline scenario studiesInductive ScenariosColumbia UYesNoNo
606Dominant kink-mode poloidal coupling dependence with betaN, q95Stability & Disruption AvoidanceColumbia UNoNoNo
603Dominant poloidal modes for ELM suppression via n=2 upper/lower I-coil phase differenceELM ControlColumbia UNoNoNo
449Drift wave and NTM couplingTurbulence & TransportLos Alamos National LaboratoryYesNoNo
207Dust generation from deposited layers and leading edgesPlasma-material InterfaceUCSDNoNoNo
531Dust generation from deposited layers and leading edgesPlasma-material InterfaceUCSDNoNoNo
203Dynamic plasma-wall equilibrium in ELMy H-modeDivertor & SOL PhysicsCompXYesNoNo
279ECH effects on low or balanced torque discharges in DIII-DPlasma RotationNational Fusion Research Institute (NFRI), KoreaYesYesNo
281ECH effects on low or balanced torque discharges in DIII-DPlasma RotationNational Fusion Research Institute (NFRI), KoreaYesYesNo
277ECH effects on low or balanced torque discharges in DIII-DPlasma RotationNational Fusion Research Institute (NFRI), KoreaYesYesNo
655ECH effects on QH-mode low or balanced torque discharges in DIII-DPlasma RotationKorea Institute of Fusion EnergyNoYesNo
493Edge rotation shear threshold for QH-mode accessELM ControlGANoNoNo
15Edge rotation shear threshold for QH-mode accessInductive ScenariosGANoNoNo
306Edge turbulence and blob generationDivertor & SOL PhysicsUniv. WisconsinNoNoNo
604EF optimization of low-torque low-q95 QH mode plasmasInductive ScenariosColumbia UNoNoNo
690EFC by ramping beta up or q95 down or NBI torque down (instead of density down) in 3-4 dischargesStability & Disruption AvoidanceColumbia UNoNoNo
520Effect of 3-D fields on divertor detachmentDivertor & SOL PhysicsORNLYesNoNo
59Effect of Changing the Grad-B Drift Direction on Snowflake Divertor Behavior, Including DetachmentDivertor & SOL PhysicsGANoNoNo
443Effect of Changing the Grad-B Drift Direction on Snowflake Divertor Behavior, Including DetachmentDivertor & SOL PhysicsGANoNoNo
472Effect of divertor geometry & heating scheme on the characteristic widths of heat flux footprintDivertor & SOL PhysicsASIPPYesNoNo
96Effect of Error Field Control Currents on Strike Point SplittingStability & Disruption AvoidanceDepartment of EnergyNoNoNo
663Effect of higher mode number error fields on n=1 Locking ThresholdStability & Disruption AvoidanceColumbia UNoNoNo
371Effect of icoil current on energy confinement in RMP ELM-suppressed dischargesELM ControlGANoNoNo
445Effect of Islands on ECCDStability & Disruption AvoidanceGANoNoNo
701Effect of lithium conditioning on H-mode pedestal profiles and ELM stabilityELM ControlGANoNoNo
19Effect of n=1 applied and error fields on n=3 RMP ELM suppressionELM ControlGANoNoNo
389Effect of n=1 applied and error fields on n=3 RMP ELM suppressionELM ControlGANoNoNo
290Effect of n=2 Poloidal Spectrum on NTV TorquePlasma RotationDepartment of EnergyNoNoNo
654Effect of sawteeth on QH-mode pedestal (EHO)Inductive ScenariosGANoNoNo
667Effect of the snowflake configuration on the SOL width in simple plasmasDivertor & SOL PhysicsCRPP-EPFLNoNoNo
300Effect of triangularity in ITER shape and improved shapingInductive ScenariosGANoNoNo
303Effect on lithium wall conditioning for Co-QH-mode and edge pedestal characteristicsInductive ScenariosGANoNoNo
60Effective NTM control in low torque plasmasStability & Disruption AvoidanceGANoNoNo
697Electromagnetic Torque Waves â?? Transport of Angular MomentumPlasma RotationColumbia UNoNoNo
34Electron Critical Gradient and Heat PinchTurbulence & TransportGANoNoNo
435Electron Critical Gradient in H-modeTurbulence & TransportGANoNoNo
124Electron Energy Transport during q0 control using modulated EC powerInductive ScenariosORNLNoNoNo
109Electron Heat Transport in E-Dominated Heating of ITER-like H-Mode Discharges with Modulated ECHInductive ScenariosU of WisconsinYesNoNo
110Electron Heat Transport in E-Dominated Heating of ITER-like H-Mode Discharges with Modulated ECHTurbulence & TransportU of WisconsinYesNoNo
639Electron thermal transport due to Compressional and Global AEs on DIII-D and projection to NSTX-UTurbulence & TransportUCLANoNoNo
619ELM divertor footprint and connection to ELM dynamics and effects of turbulence and modesELM ControlUCSDNoNoNo
142ELM heat transport in the snowflake divertor.Divertor & SOL PhysicsLLNLYesNoNo
650ELM Mitigation with ECCDTorkil Jensen AwardPPPLNoNoNo
322ELM pacing in low torque, electron heated ITER baselineInductive ScenariosGANoNoNo
380ELM Suppression at Lower Collisionality with Non-Resonant n=3 I-coilELM ControlGANoNoNo
146ELM suppression with Saturated wallsELM ControlUCSDYesNoNo
456Energy Transport During Electron-Dominated Heating of ITER Baseline Scenario H-Mode DischInductive ScenariosPPPLNoNoNo
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
72Energy Transport During Electron-Dominated Heating of ITER-Relevant H-Mode DischargesTurbulence & TransportPPPLYesNoNo
61Energy Transport During Electron-Dominated Heating of ITER-Relevant H-Mode DischargesInductive ScenariosPPPLYesNoNo
310Energy Transport During Electron-Dominated Heating of ITER-Relevant H-Mode DischargesSteady State Heating and Current DrivePPPLNoNoNo
736Erosion/Deposition of Aluminum with low density He L-mode Simple-As-Possible PlasmasPlasma-material InterfaceCommonwealth Fusion SystemsNoNoNo
675Error field correction at low rotationStability & Disruption AvoidanceGANoYesNo
328Error field correction at low rotationStability & Disruption AvoidanceGANoNoNo
202Error Field Correction Improvement: Adding BetaN dependenceStability & Disruption AvoidancePPPLYesNoNo
107Error field detection by application of a "spiraling" error fieldStability & Disruption AvoidanceORNLYesNoNo
180Establish the incremental confinement of EC power in high betaN steady-state scenario dischargesSteady State Heating and Current DriveGANoNoNo
540Establish the incremental confinement of EC power in high betaN steady-state scenario dischargesSteady State Heating and Current DriveGANoNoNo
219Establishing an experimental basis for plasma effects on magnetic islandsELM ControlGANoNoNo
83Establishing stationary I-mode with high performanceELM ControlMassachusetts Institute of TechnologyYesYesNo
75Evaluate the potential of correcting more than one mode component of the TBM error fieldStability & Disruption AvoidanceCRPP-EPFLYesNoNo
345Evaluating Physics of I-mode Stationary Enhanced Confinement Regime Without ELMs for the 2013 JRELM ControlLLNLNoNoNo
344Evaluating Physics of QH-mode Stationary Enhanced Confinement Regime Without ELMs for the 2013 JInductive ScenariosLLNLNoNoNo
504Evolution of mitigation to suppression in RMP H-modes and Validation of nonlinear M3D simulationsELM ControlUCSDYesNoNo
158Expand the high li, betaN >4 operating regime through instability avoidance and higher heating powerSteady State Heating and Current DriveGANoNoNo
763Expand the high li, betaN >4 operating regime through NTM StabilizationStability & Disruption AvoidancePPPLNoNoNo
558Expand the high li, betaN >4 operating regime through NTM Stabilization and Large Sawtooth AvoidanceSteady State Heating and Current DrivePPPLYesNoNo
469Experimental guidance for the development of a predictive model of the plasma response to an RMPELM ControlPPPLYesNoNo
95Experimental Validation of a Revised PCS Error Field CategoryPlasma ControlDepartment of EnergyNoNoNo
163Exploration of DEFC in the feedback stabilized plasma in low-q dischargesStability & Disruption AvoidancePPPLYesNoNo
174Exploration of DEFC in the feedback stabilized plasma in low-q dischargesStability & Disruption AvoidancePPPLNoNoNo
589Exploration of super H-mode using high density QH-modeInductive ScenariosGANoNoNo
518Explore RMP ELM suppression mechanism at moderate collisionalityELM ControlUCSDNoNoNo
145Explore RMP ELM suppression mechanism at moderate collisionalityELM ControlUCSDNoNoNo
507Exploring Impurity Density Asymmetries due to NBI Fast Ions and Their Effect on Impurity TransportTorkil Jensen Award_NoNoNo
466Extending hybrid discharges to low noninductive fraction through flux-pumping controlInductive ScenariosDepartment of EnergyYesNoNo
188Extension of proxy error field experiments to H-mode plasmasStability & Disruption AvoidanceColumbia UNoNoNo
669Extrapolation of Low-Torque ITER Baseline Scenario With nu* and rho*Turbulence & TransportGANoNoNo
333Far off-axis NBCDSteady State Heating and Current DriveORNLNoNoNo
598Far off-axis NBCD using vertically shifted plasmaSteady State Heating and Current DriveORNLNoNoNo
406Fast-ion and thermal transport at high qminSteady State Heating and Current DriveITER OrganizationNoYesNo
699Feedback control of mode rotation and phaseStability & Disruption AvoidanceConsultantNoNoNo
665Feedback Control to Assess the Usefulness For Using Two Impurity Species in Radiating DivertorPlasma ControlGANoNoNo
680Fine scale stepwise q-scan: role of low-order rationales and resonance condition for ELM suppressionELM ControlU of WisconsinNoNoNo
256Fine scale stepwise q-scan: role of low-order rationales and resonance condition for ELM suppressionELM ControlU of WisconsinNoNoNo
734First wall heat flux and erosion due to TBM induced error fieldsPlasma-material InterfaceORNLNoNoNo
758First-principles-driven Model-based Current Profile and Internal Energy Control in H-mode DischargesPlasma ControlLehigh UNoNoNo
369First-principles-driven Model-based Current-profile Control in H-mode DischargesPlasma ControlLehigh UNoNoNo
425Flow or flow shear for m/n=2/1 tearing mode stabilization?Stability & Disruption AvoidanceRetired from GAYesYesNo
664Follow-up studies of fast-ion transport effects on steady-state plasmasSteady State Heating and Current DriveUC, IrvineNoNoNo
640Fully Non-Inductive, Low Rotation QH-modeTorkil Jensen AwardORNLNoNoNo
494Further development of QH-mode with strong co-Ip NBI torqueInductive ScenariosGANoNoNo
16Further development of QH-mode with strong co-Ip NBI torqueInductive ScenariosGANoNoNo
357GAM eigenmode 2D structureTurbulence & TransportUCLANoNoNo
671GAM eigenmode 2D structureTurbulence & TransportUCLANoNoNo
356GAM eigenmode excitation mechanismTurbulence & TransportUCLANoNoNo
668GAM eigenmode excitation mechanism and its impact on transportTurbulence & TransportUCLANoNoNo
221Gas Injection Feedback with Radiation MeasurementsDivertor & SOL PhysicsPPPLYesNoNo
642Gas Injection Feedback with Radiation MeasurementsDivertor & SOL PhysicsPPPLNoNoNo
187H-mode 3-D field optimization with purely kink-resonant and non-resonant n=1 fieldsStability & Disruption AvoidanceColumbia UYesNoNo
468H-mode access to q95<2 through 3/2 sustainment and 2/1 preemptionInductive ScenariosDepartment of EnergyYesNoNo
92H-mode Optimization of n=1&2 Error Field Control CurrentsStability & Disruption AvoidanceDepartment of EnergyYesNoNo
259Helium Campaign (D beams)General PhysicsGANoNoNo
475Helium exhaust with 3D fieldsELM ControlU of WisconsinYesNoNo
436High Beta Hybrids and Pressure Profile BroadeningSteady State Heating and Current DriveGAYesNoNo
32High Beta Hybrids and Pressure Profile BroadeningSteady State Heating and Current DriveGANoNoNo
545High beta with NCS and qmin>2Steady State Heating and Current DriveGANoNoNo
33High Beta, Steady State HybridsSteady State Heating and Current DriveGANoNoNo
569High Beta, Steady State HybridsSteady State Heating and Current DriveGAYesNoNo
172High betaN with off-axis injection at reduced Bt (if 2011-level beam power is available)Steady State Heating and Current DriveGANoNoNo
388High Collisionless NBI Torque Drive for GAMs, aka the VH-mode path?Turbulence & TransportGANoNoNo
18High Collisionless NBI Torque Drive for GAMs, aka the VH-mode path?Turbulence & TransportGANoNoNo
287High li steady-state scenario developmentSteady State Heating and Current DriveITER OrganizationNoNoNo
414High li steady-state scenario developmentSteady State Heating and Current DriveITER OrganizationNoNoNo
775High qmin transient betaN=5 demonstrationSteady State Heating and Current DriveLLNLNoNoNo
228High resolution study of collisionality and target structure in the transition to full detachmentDivertor & SOL PhysicsLLNLYesNoNo
235High resolution Te pedestal measurements in RMP ELM suppression experimentsELM ControlSandia National LabNoNoNo
653High-Z Transport in QH-mode PlasmasPlasma-material InterfaceGANoNoNo
313Hybrids with co-NBI QH-mode edgeInductive ScenariosGANoNoNo
450Hybrids with co-NBI QH-mode edgeInductive ScenariosGANoNoNo
2Hysteresis and Turbulence Spreading in the H-L Back TransitionL-H TransitionUCLANoNoNo
622Identification of entrainment threshold in I-coil amplitude/frequency spaceStability & Disruption AvoidanceMassachusetts Institute of TechnologyYesNoNo
37Identification of I-mode through simultaneous core and edge turbulence measurementsTurbulence & TransportMassachusetts Institute of TechnologyYesNoNo
420Identification of I-mode through simultaneous core and edge turbulence measurementsTurbulence & TransportMassachusetts Institute of TechnologyNoNoNo
444Identify the Optimal Impurity for High Power High Performance Plasmas During Radiating Divertor OpsInductive ScenariosGANoNoNo
694Image Heat Load Due to Prompt and 3D field Induced EP LossesEnergetic ParticlesGANoYesNo
573Impact of EHO on fast ion lossesInductive ScenariosPPPLNoNoNo
511Impact of EHO on fast ion lossesInductive ScenariosPPPLNoNoNo
496Impact of fast-ions on the RWM stability boundaryStability & Disruption AvoidanceColumbia UNoNoNo
119Impact of fast-ions on the RWM stability boundaryStability & Disruption AvoidanceColumbia UYesYesNo
319Impact of fast-ions on the RWM stability boundaryGeneral PhysicsColumbia UNoNoNo
748Implement finite-state Off Normal Fault Response systemPlasma ControlGANoNoNo
252Implement finite-state Off Normal Fault Response systemPlasma ControlGANoNoNo
605Importance of matched poloidal spectra in most sensitive EFC conditionsStability & Disruption AvoidanceColumbia UNoNoNo
548Improve the optimized high li operating regime through 1/1 and 2/1 instability avoidanceSteady State Heating and Current DriveGANoNoNo
50Improved Heat Load Reduction Using Long Outer Divertor Leg Geometry During Puff and Pump OperationDivertor & SOL PhysicsGAYesNoNo
724Impurity transport in ELM-suppressed regimesELM ControlGANoNoNo
615Increase achievable betaN in high betaP experiment using n=3 betaN feedback (ala burn control)Steady State Heating and Current DriveGANoNoNo
547Induced L-H-L transitions in IWL plasmas with applied n=1 C-coilL-H TransitionPPPLYesNoNo
84Influence of resonant/non-resonant magnetic perturbation on particle confinement with n=2ELM ControlMax-Planck Institute for Plasma PhysicsYesYesNo
392Influence of rotation and rotation shear on ELM suppressionELM ControlThe college of William and MaryNoNoNo
77Influence of rotation and rotation shear on ELM suppressionELM ControlThe college of William and MaryYesNoNo
657Initial n=2 error field correctionStability & Disruption AvoidanceGANoNoNo
561Interaction of RMP Snowflake DivertorDivertor & SOL PhysicsPPPLNoNoNo
7Investigate angular momentum diffusion and pinch using off-axis torquePlasma RotationGANoNoNo
488Investigate angular momentum diffusion and pinch using off-axis torquePlasma RotationGANoNoNo
421Investigate Disagreements Between Thomson Scattering and ECE Measurements in High Te DischargesGeneral PhysicsMassachusetts Institute of TechnologyYesYesNo
248Investigate elongation limit in low li discharges with/without applied 3D magnetic fieldsTorkil Jensen AwardGANoNoNo
546Investigate elongation limit in low li discharges with/without applied 3D magnetic fieldsTorkil Jensen AwardGANoNoNo
670Investigate GAM's role in the L-H transitionL-H TransitionUCLANoNoNo
491Investigate in-out density asymmetry at large toroidal rotationPlasma RotationGANoNoNo
11Investigate in-out density asymmetry at large toroidal rotationPlasma RotationGANoNoNo
612Investigate the Impact of ECH on Alfvenic ActivityEnergetic ParticlesGANoYesNo
245Investigate the physics of NTM suppression by large externally applied helical fieldsTorkil Jensen AwardGANoNoNo
529Investigate the physics of NTM suppression by large externally applied helical fieldsTorkil Jensen AwardGANoNoNo
26Investigate the role of RS on inward momentum transportTurbulence & TransportUCSDNoNoNo
426Investigate the role of RS on inward momentum transportPlasma RotationUCSDNoNoNo
429Investigate the role of RS on inward momentum transportPlasma RotationUCSDNoNoNo
433Investigate the role of RS on inward momentum transportPlasma RotationUCSDNoNoNo
513Investigating the role of inter-ELM fluctuations in the ELM triggerELM ControlGANoNoNo
362Investigation of GAMs during I-mode on D3DTurbulence & TransportMassachusetts Institute of TechnologyNoYesNo
621Investigation of Sheath Power Transmission at the DIII-D Divertor using Surface ThermocouplesDivertor & SOL PhysicsU of Tennessee, KnoxvilleNoNoNo
41Investigation of the effects of the EHO toroidal mode number on the edge particle transportInductive ScenariosPPPLNoNoNo
542Investigations of advanced divertor configurations for DIII-DDivertor & SOL PhysicsMITNoNoNo
82IR Imaging of I-coil Induced Fast Ion LossesEnergetic ParticlesGANoYesNo
567Is loss of rotation in low-torque IBS discharges due to solenoid-related error fields?Inductive ScenariosGANoNoNo
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
212Island seeding with saw teeth pacing: New method to control tearing modesStability & Disruption AvoidancePPPLYesNoNo
684Isotope Mass Scaling of Turbulence, Transport and Confinement in H-ModeTurbulence & TransportU of WisconsinNoNoNo
260ITER Baseline Scenario DemonstrationInductive ScenariosITER OrganizationNoYesNo
401ITER Baseline Scenario DemonstrationInductive ScenariosITER OrganizationNoYesNo
283ITER Baseline Scenario Operation near the LH ThresholdInductive ScenariosITER OrganizationNoYesNo
404ITER Baseline Scenario Operation near the LH ThresholdInductive ScenariosITER OrganizationNoYesNo
297ITER baseline scenario with low NBI torqueInductive ScenariosGANoNoNo
762ITER Baseline Scenario: Expand the operational limit by NTM stabilization and Time Dependent EFCStability & Disruption AvoidancePPPLNoNoNo
568ITER Baseline Scenario: Expand the operational limit by NTM stabilization and Time Dependent EFCInductive ScenariosPPPLNoNoNo
789Iter Scenario: Optimize Radiative Divertor and Core PerformanceInductive ScenariosPPPLNoNoNo
794ITER Scenario: Understanding the NTM Stability Limits by q-profile modificationInductive ScenariosPPPLNoNoNo
151ITER SS Demo Discharge DocumentationsSteady State Heating and Current DriveRetiredNoNoNo
595ITER steady-state scenario in USN, +BTSteady State Heating and Current DriveORNLNoNoNo
367JET/DIII-D similarity experiment on rotation in plasmas with low momentum inputPlasma RotationInstituto Superior Tecnico, Lisboa, PortugalNoYesNo
672L-H threshold in hydrogen plasmasL-H TransitionORNLNoNoNo
20L-H transition Trigger Physics/ Main Ion Momentum BalanceL-H TransitionUCLANoNoNo
270L-mode Turbulence and L-H Transition Characterization in Snowflake Divertor PlasmasDivertor & SOL PhysicsLLNLYesNoNo
312Limits to pedestal radiation high beta dischargesSteady State Heating and Current DriveGANoNoNo
759Link between driven plasma response and tearing stabilityStability & Disruption AvoidanceColumbia UNoNoNo
365Lithium dropper commissioning and ELM modificationGeneral PhysicsGANoNoNo
514LOC/SOC StudiesTurbulence & TransportMIT PSFCYesYesNo
610Local correction of the TBM error fieldStability & Disruption AvoidanceColumbia UNoNoNo
685Locked mode control at low (ITER-like) q95 and with external C-coilsStability & Disruption AvoidanceColumbia UNoNoNo
691Locked-mode avoidance by magnetic f/back on saddle-loopsStability & Disruption AvoidanceColumbia UNoNoNo
536Low rotation, elevated q_min steady-state scenario discharges at high betaN and 210R MSESteady State Heating and Current DriveGANoNoNo
193Magnetic perturbation amplitude scan to investigate RMP-induced damping of Zonal FlowsTurbulence & TransportU of WisconsinYesNoNo
106Magnetic turbulence measurements in high beta H-mode dischargesTurbulence & TransportPPPLYesNoNo
777Magnitude of cross-field drifts in the Private Flux Region, divertor asymmetries and detachmentDivertor & SOL PhysicsAalto UNoNoNo
21Magnitude of cross-field drifts in the Private Flux Region, divertor asymmetries and detachmentDivertor & SOL PhysicsAalto UNoNoNo
258Main-ion and impurity rotation in helium plasmasPlasma RotationGANoNoNo
490Maintain low-rotation QH-mode with ECH onlyInductive ScenariosGANoNoNo
10Maintain low-rotation QH-mode with ECH onlyInductive ScenariosGANoNoNo
579Mapping of Peeling Mode Stability BoundaryPedestal StructureGANoYesNo
577MARFE limits in the snowflake configurationDivertor & SOL PhysicsLLNLNoNoNo
760Marginal 2/1 island width in IBSStability & Disruption AvoidanceRetired from GANoNoNo
661Massive gas injection into an unstable plasmaDisruption MitigationGANoNoNo
39Measure and understand energetic particle profiles in steady-state plasmasSteady State Heating and Current DriveUC, IrvineNoNoNo
688Measure Beam Ion Transport due to Resonance Between Applied 3D Fields and Injected Beam Ion OrbitsEnergetic ParticlesGANoYesNo
696Measure Change in 3D Field Induced EP Losses Due to ScreeningEnergetic ParticlesGANoYesNo
5Measure Intrinsic Rotation Size scaling in DIII-D alone -IIPlasma RotationGANoNoNo
386Measure Intrinsic Rotation Size scaling in DIII-D alone -IIPlasma RotationGANoNoNo
795Measure NTV torque profilePlasma RotationColumbia UNoNoNo
555Measure Plasma Response to RMPsELM ControlGANoNoNo
185Measure Plasma Response to RMPsELM ControlGAYesNoNo
620Measurement of heat flux on the divertor using the embedded thermocouple arrayDivertor & SOL PhysicsU of Tennessee, KnoxvilleNoNoNo
192Measurement of heat flux on the divertor using the embedded thermocouple arrayDivertor & SOL PhysicsU of Tennessee, KnoxvilleNoNoNo
702Measurement of hysteresis in RMP-ELM suppression thresholdsELM ControlColumbia UNoNoNo
442Measurement of Inductive Poloidal CurrentStability & Disruption AvoidanceGANoNoNo
149Measurement of ion temperatures in the divertor region of DIII-D using the DiMES platformDivertor & SOL PhysicsU of Tennessee, KnoxvilleNoNoNo
183Measurement of multiple mechanisms in the low-density limit via ellipticity in the compass scanStability & Disruption AvoidanceColumbia UYesNoNo
190Measurement of n=3 error field effects in RMP phase-flip experimentsELM ControlColumbia UNoNoNo
599Measurement of neoclassical response of off-axis beam ionsSteady State Heating and Current DriveORNLNoNoNo
334Measurement of neoclassical response of off-axis beam ionsSteady State Heating and Current DriveORNLNoNoNo
189Measurement of optimal n=2 phasing for RMP & ELM suppression without q95 windowsELM ControlColumbia UNoNoNo
396Measurement of RE diffusion to center postDisruption MitigationUCSDNoNoNo
779Measurement of the Heat Flux(Grad T) FunctionTurbulence & TransportU of Texas, AustinNoNoNo
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
40MGI with applied n=1 RMP fieldsDisruption MitigationFiat Lux LLCNoNoNo
609MHD spectroscopy and poloidal coupling of plateau RE plasmasDisruption MitigationColumbia UNoNoNo
773Model-based control of the current profile and βN for steady state scenariosPlasma ControlGANoNoNo
459Model-based control of the current profile and βN for steady state scenariosSteady State Heating and Current DriveCadaracheNoNoNo
316Model-based control of the current profile and βN for steady state scenariosPlasma ControlCadaracheNoNoNo
29Modulation of Bootstrap CurrentELM ControlGANoNoNo
552Modulation of Bootstrap CurrentELM ControlGANoNoNo
764Multiple periods of NTM suppressionStability & Disruption AvoidancePPPLNoNoNo
200Multiple periods of NTM suppressionStability & Disruption AvoidancePPPLYesNoNo
632Mutual alignment of gyrotrons: a new technique based on mirror-steering and anti-phase modulationSteady State Heating and Current DriveColumbia UYesNoNo
659n = 2 Dynamic Error Field CorrectionStability & Disruption AvoidanceGANoNoNo
737n=1 and n=2 simultaneous DEFC /DFB for routine demonstration of low q << 2 RWM stable regimeStability & Disruption AvoidancePPPLNoNoNo
584n=1 RMP Suppression and the role of field penetration vs kink excitationELM ControlGAYesNoNo
147Natural and Pellet-induced ELM behavior at low rotation/torqueELM ControlUCSDYesNoNo
36Natural ELM Pacing in High-Beta, Steady-State PlasmasSteady State Heating and Current DriveGANoNoNo
170Nature of Energy Released During H-L Back TransitionL-H TransitionGANoNoNo
560NBI Driven Poloidal RotationPlasma RotationGANoNoNo
744NBI torque assisted unlocking and spinup experimentsStability & Disruption AvoidanceMassachusetts Institute of TechnologyNoNoNo
749Neon SPI injection into early CQ to stunt RE formationDisruption MitigationGANoNoNo
254Neon SPI injection into early CQ to stunt RE formationDisruption MitigationGANoNoNo
30New Optimal Plasma Shape for AT Scenario?Steady State Heating and Current DriveGANoNoNo
251New Study of Alfven Eigenmodes Induced Fast Ion Transport/LossEnergetic ParticlesGANoNoNo
35Non-Diffusive Heat Fluxes in the Edge "Shortfall" RegionTurbulence & TransportGANoNoNo
201NTM Control Upgrade: Capibility to deposit EC at multiple locationsPlasma ControlPPPLYesNoNo
719NTM Control Upgrade: Capibility to deposit EC at multiple locationsPlasma ControlPPPLNoNoNo
722NTM control with ECCD, Real-time Ray Tracing and real-time MirrorsPlasma ControlPPPLNoNoNo
377NTM locking disruption avoidance by the EM torque with toroidal-phase forward magnetic feedDisruption MitigationPPPLNoNoNo
692NTMs â??on demandâ??, by ECHStability & Disruption AvoidanceColumbia UNoNoNo
693NTMs â??on demandâ??, by modulated ECCDStability & Disruption AvoidanceColumbia UNoNoNo
662NTV Collisionality Regime TestPlasma RotationColumbia UNoNoNo
268nu* dimensionless scalingTurbulence & TransportCEANoYesNo
265o Experiments using the centerpost Swing-probesDivertor & SOL PhysicsUCSDNoNoNo
125Observation of non-linear interactions in fast-ion loss spectraEnergetic ParticlesPPPLNoNoNo
335Off-axis NBCD measurement in steady state scenarioSteady State Heating and Current DriveORNLNoNoNo
186Optimal Mixing of I & C coils for n=1 EFCStability & Disruption AvoidanceColumbia UYesNoNo
571Optimal Plasma Shape for High-Beta, Steady-State Hybrid ScenarioSteady State Heating and Current DriveGAYesNoNo
105Optimization and exploration of the q95<2 scenario in DIII-DStability & Disruption AvoidanceConsorzio RFXYesNoNo
240Optimization of Applied Error Field Spectrum for NTVStability & Disruption AvoidanceColumbia UYesNoNo
438Optimize electron pedestal pressure in ECH-heated QH-mode plasmasPedestal StructureUCLANoNoNo
439Optimize electron pedestal pressure in ECH-heated QH-mode plasmasPedestal StructureUCLANoNoNo
292Optimize electron pedestal pressure in low-torque ITER baseline plasmasInductive ScenariosUCLANoNoNo
787Optimize Radiative Divertor and Core PerformanceSteady State Heating and Current DrivePPPLNoNoNo
788Optimize Radiative Divertor and Core PerformanceDivertor & SOL PhysicsPPPLNoNoNo
74Optimize TBM error field correction against field penetration in low NBI torque H-modesStability & Disruption AvoidanceCRPP-EPFLYesNoNo
120Optimizing non-resonant, nonaxisymmetric fields in QH-modeInductive ScenariosGANoNoNo
370Particle pinch in pedestalPedestal StructureGANoNoNo
373Pedestal optimization in VH modePedestal StructureORNLNoNoNo
379Pedestal optimization of ITER baseline scenario discharges.Pedestal StructureGANoNoNo
372Pedestal optimization via impurity injectionPedestal StructureORNLNoNoNo
556Pedestal optimization with RMP ELM ControlPedestal StructureORNLNoNoNo
374Pedestal optimization with RMP ELM ControlPedestal StructureORNLNoNoNo
134Pedestal stability and divertor transport studies with feedback-controlled snowflake configuration.Divertor & SOL PhysicsLLNLYesNoNo
517Physics of Crescent-shaped synchrotron emission patterns in runaway plateau discharDisruption MitigationUCSDYesNoNo
800Physics of EHO control in low-torque QH-modeTorkil Jensen AwardDepartment of EnergyNoNoNo
709Physics of EHO control in low-torque QH-modeInductive ScenariosDepartment of EnergyNoNoNo
723Physics of the Heat Flux WidthDivertor & SOL PhysicsAKIMA Infrastructure ServicesNoNoNo
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
217PID (proportional integral derivative)control of Error FieldStability & Disruption AvoidancePPPLYesNoNo
700PID-controlled boundary radial field for â??spontaneousâ?? mode-unlockingStability & Disruption AvoidanceConsultantNoNoNo
588Plasma Response in IWL H-mode plasmasELM ControlORNLNoNoNo
24Plasma response to 3D magnetic perturbations in the unfavorable grad-B drift directionELM ControlPPPLYesNoNo
658Plasma response to n=2 perturbationsStability & Disruption AvoidanceGANoNoNo
633Plasma response to small applied rotating fields as an error-field-detection methodStability & Disruption AvoidanceColumbia UYesNoNo
695Poloidal rotation of plasma column to simulate rotating wallPlasma ControlColumbia UNoNoNo
278Possibility of â??Off-axis-Fishbone Mode and ELM Pacingâ?? due to Direct Energetic Particle CouplingELM ControlJAEANoNoNo
177Possibility of â??Off-axis-Fishbone Mode and ELM Pacingâ?? due to Direct Energetic Particle CouplingELM ControlPPPLYesNoNo
295preliminary simulated burn controlTurbulence & TransportGANoNoNo
446Probe the viscosity of inter-mode couplingPlasma RotationLos Alamos National LaboratoryYesNoNo
550Probing and controlling the L->H and H->L transitions by small pellet injectionL-H TransitionKorea Institute of Fusion EnergyNoNoNo
103Probing and controlling the L->H and H->L transitions by small pellet injectionL-H TransitionKorea Institute of Fusion EnergyYesNoNo
539Produce fNI = 1 discharges at q_min near 1.5 using off-axis injection and a model guided approachSteady 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
6Prompt torque and zonal flow dampingPlasma RotationGANoNoNo
457Prompt torque and zonal flow dampingTurbulence & TransportGANoNoNo
355q dependence of L-H transition power thresholdL-H TransitionUCLANoNoNo
140q0 control with Counter-ECCD in ITER Baseline DischargesInductive ScenariosRetiredNoNoNo
526q95 < 2 Tokamak Operation Via Dynamic Error Field CorrectionStability & Disruption AvoidanceGANoNoNo
242q95 < 2 Tokamak Operation Via Dynamic Error Field CorrectionStability & Disruption AvoidanceGANoNoNo
596q95 dependency of beam ion confinement in high qmin scenarioSteady State Heating and Current DriveORNLNoNoNo
753q95 scaling of the coupled turbulence/zonal flow during LH transitionL-H TransitionU of WisconsinNoNoNo
359q95 scaling of the coupled turbulence/zonal flow during LH transitionL-H TransitionU of WisconsinNoNoNo
500q95<2 tokamak operation via dynamic error field correctionStability & Disruption AvoidanceConsorzio RFXYesNoNo
115QH-mode at low co-Ip torque using n=2 NRMFInductive ScenariosGANoNoNo
756QH-mode edge sweep with helium impurity for comparison to XGC0Pedestal StructurePPPLNoNoNo
652QH-mode operation with reduced divertor interactionInductive ScenariosGANoNoNo
375QH-mode pedestal optimizationInductive ScenariosORNLNoNoNo
53QH-mode with low torque start-upInductive ScenariosGANoNoNo
495QH-mode with low torque start-upInductive ScenariosGANoNoNo
330QH-mode with TBMInductive ScenariosGANoNoNo
331QH-mode with TBM (dup 330)Stability & Disruption AvoidanceGANoNoNo
721qmin controlSteady State Heating and Current DrivePPPLNoNoNo
208qmin controlSteady State Heating and Current DrivePPPLYesNoNo
793qmin controlPlasma ControlPPPLNoNoNo
741Quantifying the improved confinement achieved by NTM spinupStability & Disruption AvoidanceMassachusetts Institute of TechnologyNoNoNo
47Quantifying the TBM torque, both in magnitude and radial locationPlasma RotationVTT Technical Research CentreNoNoNo
608Quiescent runaway electron studies for 2014Disruption MitigationColumbia UNoNoNo
767Radiation asymmetry measurements in opposite-handed plasmasDisruption MitigationORNLNoNoNo
666Radiation limit in the snowflake configurationDivertor & SOL PhysicsCRPP-EPFLNoNoNo
148Radiative divertor control developmentDivertor & SOL PhysicsLLNLYesNoNo
402Radiative divertor solutions in the ITER baseline scenarioInductive ScenariosITER OrganizationNoYesNo
403Radiative divertor solutions in the ITER baseline scenarioDivertor & SOL PhysicsITER OrganizationNoYesNo
720Real-time Error Field CorrectionPlasma ControlPPPLNoNoNo
213Real-time Ray Tracing for PCSPlasma ControlPPPLYesNoNo
538Reduce fast ion transport in high qmin, high beta plasmasSteady State Heating and Current DriveLLNLNoNoNo
199Reducing the tearing island detection timeStability & Disruption AvoidancePPPLYesNoNo
740Respond to locking by ramping IP downStability & Disruption AvoidanceColumbia UNoNoNo
646rho* scaling of intrinsic torque between DIII-D and JETPlasma RotationGANoYesNo
327rho* scaling of intrinsic torque between DIII-D and JETPlasma RotationGANoYesNo
308RMP (Resonant Magnetic Perturbation) code validation via UCLA 288 GHz polarimeterELM ControlUCLANoNoNo
473RMP assisted snowflake divertorDivertor & SOL PhysicsU of WisconsinYesNoNo
62RMP assisted snowflake divertorDivertor & SOL PhysicsU of WisconsinYesNoNo
637RMP Effect on ELMs: Separate the effect of density pumpoutELM ControlPPPLNoNoNo
505RMP ELM Control at ITER relevent rotation/torqueELM ControlUCSDNoNoNo
143RMP ELM control at low torqueELM ControlUCSDYesNoNo
782RMP ELM Control DevelopmentPlasma ControlPPPLNoNoNo
23RMP ELM Suppression at q95 above 4ELM ControlGANoNoNo
390RMP ELM Suppression at q95 above 4ELM ControlGANoNoNo
302RMP ELM Suppression at the NTV Offset RotationELM ControlGANoNoNo
55RMP Elm Suppression in DN PlasmasELM ControlORNLNoNoNo
519RMP ELM-Control for Snowflake ConfigurationsDivertor & SOL PhysicsLLNLNoNoNo
209RMP ELM-Control for Snowflake ConfigurationsTorkil Jensen AwardLLNLYesNoNo
562RMP NTM interactionStability & Disruption AvoidancePPPLYesNoNo
394Role of density and impurities on particle and momentum transportTurbulence & TransportThe college of William and MaryNoNoNo
717Role of poloidal flux expansion to address divertor heat flux challengeDivertor & SOL PhysicsGANoNoNo
28Role of profile evolution and energy transfer in L-H transitionL-H TransitionUCSDNoNoNo
376Role of q and magnetic shear of pedestal formation time and turbulent transportPedestal StructurePPPLNoNoNo
307Role of turbulent-driven and Ion pressure gradient-sustained ExB flows in Triggering H-modeL-H TransitionUCSDNoNoNo
602Rotating field current drive for NTM suppressionStability & Disruption AvoidanceMassachusetts Institute of TechnologyYesNoNo
774Rotating Magnetic Field Current Drive (RMFCD)Steady State Heating and Current DriveMassachusetts Institute of TechnologyNoNoNo
761Rotating Magnetic Field Current-Drive (RMFCD)Torkil Jensen AwardMassachusetts Institute of TechnologyNoNoNo
395Rotation reversalPlasma RotationThe college of William and MaryNoNoNo
336Routine current profile control in operationSteady State Heating and Current DriveGANoNoNo
337Routine current profile control in operationInductive ScenariosGANoNoNo
383Run Coordinator Test ProposalGeneral PhysicsLLNLNoNoNo
384Run Coordinator Test Proposal IIGeneral PhysicsGANoNoNo
710RWM control using external coilsStability & Disruption AvoidanceColumbia UNoNoNo
320RWM excitation in the SSI target by reducing triangularity"Stability & Disruption AvoidancePPPLNoNoNo
679Safety Factor Scaling of Turbulence and Transport in Hybrid Scenario PlasmasTurbulence & TransportU of WisconsinNoNoNo
86Safety Factor Scaling of Turbulence and Transport in Hybrid Scenario PlasmasTurbulence & TransportU of WisconsinNoNoNo
56Sawtooth ControlPlasma ControlORNLNoNoNo
273Sawtooth control via n=1 external magnetic perturbationTorkil Jensen AwardConsorzio RFX and Padova UYesNoNo
630Sawtooth control via n=1 external magnetic perturbation: extension to H-mode plasmasStability & Disruption AvoidanceConsorzio RFXYesNoNo
197Scaling of divertor detachment onsetDivertor & SOL PhysicsGAYesNoNo
428Scaling of L-H transiton power with Xpoint location and collisionalityL-H TransitionUCSDNoNoNo
305Scaling Of Pedestal Plasma Transport With RMP I-coil CurrentELM ControlU of WisconsinNoNoNo
727Scaling Of Pedestal Plasma Transport With RMP I-coil CurrentELM ControlU of WisconsinNoNoNo
424Search for evidence of non-local transport across slow L-H transitionsTurbulence & TransportMassachusetts Institute of TechnologyYesNoNo
730Search for Fast Ion Critical GradientEnergetic ParticlesGANoNoNo
649Search for high freq magnetic fluctuations with CPS diagnosticTurbulence & TransportUCLANoNoNo
381Search for turbulence at ion-cyclotron frequenciesTurbulence & TransportUCLANoNoNo
150Sensitivity study of toroidally-asymmetric halo current to error field during VDEDisruption MitigationPPPLNoNoNo
422Separation of thermal and particle transport in I-mode plasmasTurbulence & TransportMassachusetts Institute of TechnologyNoNoNo
768sheath physics study 2Divertor & SOL PhysicsSandia National LabNoNoNo
294Simulated Alpha particle dillutionTurbulence & TransportGANoNoNo
564Simulated of Burn Control using In-Vessel CoilsTurbulence & TransportPPPLYesNoNo
576Slow snowflake configuration scans to clarify geometry vs physicsDivertor & SOL PhysicsLLNLNoNoNo
796Snowflake ControlPlasma ControlPPPLNoNoNo
179Snowflake in AT PlasmaSteady State Heating and Current DriveLLNLNoNoNo
298Soft landing with 2/1 TM in the ITER shapeStability & Disruption AvoidanceGANoNoNo
559SOL Width Scaling: Goldston's Heuristic Drift Model vs Critical Pressure Gradient ModelDivertor & SOL PhysicsPPPLNoNoNo
452Source of Magnetic Flux Pumping in HybridsInductive ScenariosGANoNoNo
570Space, time and energy-resolved x-ray measurements for magnetically confined fusion plasmasStability & Disruption AvoidancePPPLYesNoNo
138SSI target improvement by minimizing global low-n MHD activity in 1.5 Steady State Heating and Current DrivePPPLNoNoNo
231Stabilization of NTMs with ECCDStability & Disruption AvoidanceQSTNoYesNo
249Steady-state high beta with NCS and qmin>2Steady State Heating and Current DriveGANoNoNo
530Studies of arcing on divertor PFC surfacesPlasma-material InterfaceUCSDNoNoNo
206Studies of arcing on divertor PFC surfacesPlasma-material InterfaceUCSDNoNoNo
400Studies of RE final lossDisruption MitigationUCSDNoNoNo
234Study fishbone-like instability at the edge of QH-modesInductive ScenariosInstituto Superior Tecnico, Lisboa, PortugalNoNoNo
244Study NRMF driven torque in ECH-only heated plasma (ELMing H-modes)Plasma RotationGANoNoNo
528Study NRMF driven torque in ECH-only heated plasma (ELMing H-modes)Plasma RotationGANoNoNo
225Study of atomic and molecular processes in deep detachment conditionsDivertor & SOL PhysicsLLNLYesNoNo
51Study of chirping Alfvén eigenmodes in DIII-DEnergetic ParticlesPPPLNoYesNo
378Study of the connection between I-mode and low density Type III ELMs and optimization of I-modeELM ControlGANoNoNo
317Study on sawteeth in the neutral beam (NB) heated plasmasStability & Disruption AvoidanceKorea National Fusion Research CenterNoNoNo
253Study QH-mode with advanced fast ion diagnostics and codesInductive ScenariosGANoNoNo
255Super H-ModeTorkil Jensen AwardORNLYesNoNo
537Super H-Mode: Pedestal Evolution and OptimizationPedestal StructureORNLYesNoNo
544Super H-Mode: Scenario DevelopmentSteady State Heating and Current DriveORNLYesNoNo
541Support of DIII-D boundary physics experimentsDivertor & SOL PhysicsMITNoNoNo
419Support of ITER Research Plan for Q=10 OperationInductive ScenariosITER OrganizationNoNoNo
467Sustainment of q<2 through pseudo wall rotationInductive ScenariosDepartment of EnergyYesNoNo
130Synergy between core-localized Alfven eigenmodes and edge localized TBM fields on fast ion losses.Energetic ParticlesPPPLNoYesNo
454Synergy between core-localized Alfven eigenmodes and edge localized TBM fields on fast ion losses.Energetic ParticlesPPPLNoYesNo
182Systematic test of paleoclassical transportTurbulence & TransportGANoNoNo
590Targeting Top of Pedestal in RMP ELM-suppressed plasmas with SXR ImagingELM ControlORNLNoNoNo
363TBM mockup simulating ITER GDC with ferritic materialsGeneral PhysicsGANoNoNo
551Test compatibility of radiative divertor with QH-modeInductive ScenariosGANoNoNo
525Test critical gradient model for fast-ion transportEnergetic ParticlesUC, IrvineNoNoNo
293Test of ETG zeff supressionTurbulence & TransportGANoNoNo
9Test of Neoclassical Toroidal Viscosity theory using modulated I-coil currentsPlasma RotationGANoNoNo
715Test of the upgraded SPIDisruption MitigationORNLNoNoNo
430Test of Turbulence Spreading Using Turbulence PropagationTurbulence & TransportGANoNoNo
31Test of Turbulence Spreading Using Turbulence PropagationTurbulence & TransportGANoNoNo
73Test optimized TBM error field correction at higher values of betaStability & Disruption AvoidanceCRPP-EPFLYesNoNo
726Test Pedestal Structure Model Where Paleoclassical Transport Is DominantPedestal StructureU of WisconsinNoNoNo
262Test Pedestal Structure Model Where Paleoclassical Transport Is DominantPedestal StructureU of WisconsinNoNoNo
732Testing ELM destabilization by 3D fields on DIII-DELM ControlORNLNoNoNo
121Testing Emerging Two-Fluid Model for RMP Plasma Response in Straightforward IWL PlasmasELM ControlORNLYesNoNo
613Testing for parameter space with the best fast ion confinement at high q_minSteady State Heating and Current DriveGANoNoNo
566Testing of New Hardware and Software Capabilities for NTM ControlPlasma ControlPPPLNoNoNo
210The Dependence of Poloidal Rotation on TurbulencePlasma RotationGANoNoNo
385The effect of LSN Shape on the q95 windows in RMP ELM SuppressionELM ControlGANoNoNo
471The experiment on generalized hybrid scenario with qmin > 2 at low density and relatively high q95Inductive ScenariosASIPPYesNoNo
554The impact of increased pressure gradient on scenarios for fully noninductive operationSteady State Heating and Current DriveGANoNoNo
738The investigation of EP-kinetic effects and plasma rotation with low q and low beta operationStability & Disruption AvoidancePPPLNoNoNo
563The Role of Energetic Particles in ELM-Free H-mode PlasmasELM ControlUC, IrvineNoNoNo
750The role of non-local transport and avalanches in different L-H transition regimesL-H TransitionUCLANoNoNo
636Time-resolved measurement of plasma response spectrumStability & Disruption AvoidanceColumbia UNoNoNo
97Time-resolved measurement of plasma response spectrumStability & Disruption AvoidanceColumbia UYesNoNo
437TQ radiation distribution from R-2 MGIDisruption MitigationMassachusetts Institute of TechnologyNoNoNo
382Transport and turbulence characterization experimentSteady State Heating and Current DriveUCLANoNoNo
257Transport Investigation During Slow Current Ramp-Up and Ramp-Down [for ITER]Inductive ScenariosU of WisconsinNoYesNo
681Transport Investigation During Slow Current Ramp-Up and Ramp-Down [for ITER]Inductive ScenariosU of WisconsinNoNoNo
432Transport mechanisms induced by RMPELM ControlUCSDNoNoNo
152Transport shortfall at high gyrobohm fluxTurbulence & TransportGANoNoNo
745Transport studies in I-mode plasmasPedestal StructureMassachusetts Institute of TechnologyNoNoNo
629Transport study using Modulation RMP (M-RMP)ELM ControlZhejiang UYesNoNo
311Transport with qmin>2Steady State Heating and Current DriveLLNLNoNoNo
623Trapped Electron Mode n_e / T_e Fluctuation StudyTurbulence & TransportU of Colorado, BoulderNoNoNo
624Trapped Electron Mode Study in CoreTurbulence & TransportU of Colorado, BoulderNoNoNo
291Trigger-less onset of NTMs with P_EC and NTV effects on rotation regimeStability & Disruption AvoidanceInstituto Superior Tecnico, Lisboa, PortugalNoNoNo
126Triggering ELMs at high frequency with PPPL Lithium granule injectorELM ControlRetired from PPPLYesNoNo
4Turbulence and Intrinsic RotationPlasma RotationGANoNoNo
94Turbulence Structure and Amplitude Variation with ExB Shear in H-mode PlasmasTurbulence & TransportU of WisconsinNoNoNo
731Turbulent Ion Thermal Response to Electron Heat Flux and Te/Ti VariationTurbulence & TransportSandia National LabNoNoNo
431Turbulent transport in detached divertorDivertor & SOL PhysicsUCSDNoNoNo
267Understand and control resistive wall mode stability in high-qmin plasmasSteady State Heating and Current DriveColumbia UNoNoNo
99Understand and control resistive wall mode stability in high-qmin plasmasStability & Disruption AvoidanceColumbia UYesYesNo
326Understand mechanisms by which ECH influences NTM stablilityStability & Disruption AvoidanceGANoNoNo
100Understand resistive wall mode control physics in low-q95 plasmasStability & Disruption AvoidanceColumbia UYesNoNo
266Understand resistive wall mode control physics in low-q95 plasmasInductive ScenariosColumbia UNoNoNo
678Understanding and Testing Methods for Producing Gentle HL TransitionsL-H TransitionGANoNoNo
784Understanding the NTM Stability Limits by q-profile modificationInductive ScenariosPPPLNoNoNo
506Understanding the synchrotron emission patterns in QRE dischargesDisruption MitigationUCSDYesNoNo
772Unified edge and SOL rotationDivertor & SOL PhysicsUCSDNoNoNo
366Up/down Asymmetric EFCStability & Disruption AvoidanceDepartment of EnergyNoNoNo
499Up/down Asymmetric EFCStability & Disruption AvoidanceDepartment of EnergyNoNoNo
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
641Using Magnetic Balance To Regulate Density and Impurity Accumulation Inside Double-null PlasmasDivertor & SOL PhysicsGANoNoNo
656Validating Critical Gradient Model for Burning PlasmasEnergetic ParticlesPPPLYesNoNo
144Validation of kink response models with rotating n = 1 and n = 2 and phase flip n = 3 RMPsELM ControlUCSDYesNoNo
503Validation of M3D nonlinear MHD simulations of ELMsPedestal StructureUCSDYesNoNo
616Validation of nonlinear models of ELMs and RMP ELM mitigationELM ControlMassachusetts Institute of TechnologyYesNoNo
498Validation of single-mode model of error field correction for n=2 fieldsStability & Disruption AvoidanceDepartment of EnergyYesYesNo
509Vertical positioning and stability control by means of reflectometryPlasma ControlGANoNoNo
524VFI bus voltage control and the True scaled ITER shape at DIII-DPlasma ControlGANoNoNo
236Wavenumber dependence of turbulence suppression in the L-H transitionL-H TransitionUCLANoNoNo
510What can lost fast-ions tell us about the H-mode pedestal?Pedestal StructurePPPLNoNoNo
725What causes density buildup at the pedestal top?Pedestal StructureU of WisconsinNoNoNo
614Why Does the Heat Flux Increase in the Secondary Divertor Under the BetaN = constant Constraint?Divertor & SOL PhysicsGANoNoNo