DIII-D RESEARCH OPPORTUNITIES FORUM FOR THE 2008 EXPERIMENTAL CAMPAIGN Login | Review | Submit | Logout | Help

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ID Title Research Area Name Affiliation Time Requested
14Develop near-balanced NBI for use in intrinsic rotation scaling experiments.Rotation Physics (2009)John DegrassieGAYes
15Intrinsic rotation in helium H-mode discharges.Rotation PhysicsJohn DegrassieGAYes
16Expand the dimensionless similarity database on intrinsic rotationRotation PhysicsJohn DegrassieGANo
17Mixed Gas MGIDisruptionsJohn C. WesleyGAYes
18Measure intrinsic rotation in the JET shapeRotation PhysicsJohn DegrassieGANo
19Use DIII-D pumping capability to separate density and temperature in Rice's scalingRotation PhysicsJohn DegrassieGANo
20RMP penetration vs rotationELM Control & Pedestal PhysicsJohn DegrassieGANo
21Does Confinement Improvement Saturate with Increasing Rotation?Rotation PhysicsMickey R. WadeGANo
22Collisionality Dependence of RMP SuppressionELM Control & Pedestal PhysicsMickey R. WadeGANo
26Commonality of Density Threshold for RMP ELM Suppression and QH-modeELM Control & Pedestal PhysicsMickey R. WadeGANo
27Disruption Statistics and PredictionDisruptionsJohn C. WesleyGAYes
28Small-sized LSN to test off axis NBCDHeating & Current DriveJohn DegrassieGANo
29ITER-AT demonstration dischargeITER Demonstration DischargesHolger ReimerdesColumbia UNo
30High beta error field thresholdRotation PhysicsHolger ReimerdesColumbia UNo
31Parametric dependencies of RWM damping in rotating plasmasRWM PhysicsHolger ReimerdesColumbia UNo
32Multiple n dynamic error field correctionRWM PhysicsHolger ReimerdesColumbia UNo
33Real-time stability measurement using active MHD spectroscopyRWM PhysicsHolger ReimerdesColumbia UNo
34Cross-machine comparison of n=2 (non-resonant) magnetic brakingRotation PhysicsHolger ReimerdesColumbia UYes
35High central fast wave current drive efficiency at high electon beta with 110 GHz EC preheatingFully Noninductive High Beta OperationRobert I. PinskerGANo
36FW-only H-mode studiesHeating & Current DriveRobert I. PinskerGANo
37FW coupling and electron heating in ELM-stabilized H-modes with RMPs - continuedELM Control & Pedestal PhysicsRobert I. PinskerGANo
38Heat transport profiles and poloidal asymmetriesThermal Transport in the Plasma BoundaryJose A. BoedoUC, San DiegoYes
39Rotation and ELMsELM Control & Pedestal PhysicsJose A. BoedoUC, San DiegoYes
40Heat Footprint active control using applied magnetic fieldsThermal Transport in the Plasma BoundaryJose A. BoedoUC, San DiegoYes
41ELM heat deposition characterization and controlThermal Transport in the Plasma BoundaryJose A. BoedoUC, San DiegoYes
42ELM Heat deposition control using detachmentThermal Transport in the Plasma BoundaryJose A. BoedoUC, San DiegoNo
43Rotation transfer across LCFSBoundaryJose A. BoedoUC, San DiegoYes
44Ploidal asymmetries of flows in the boundary/SOLBoundaryJose A. BoedoUC, San DiegoYes
45Poloidal asymmetries of turbulence and heat/particle transportBoundaryJose A. BoedoUC, San DiegoYes
46Penetration of magnetic perturbations in plasmaELM Control & Pedestal PhysicsJose A. BoedoUC, San DiegoYes
47Effect of RMPs on fluctuations and transport in edge/SOLELM Control & Pedestal PhysicsJose A. BoedoUC, San DiegoYes
48Multi-field Measurements of NTMs and Fast Ion redistribution in Hybrid PlasmasCore Integration (Advanced Inductive)Raffi NazikianPPPLYes
49Multifield Measurement of Low-n Alfven Eigenmodes in the Core of DIII-D PlasmasEnergetic ParticlesRaffi NazikianPPPLYes
50Test of a theoretical model for the irreducible minimal pedestal width scalingELM Control & Pedestal PhysicsRichard GroebnerGAYes
51Runaway electon diagnosis by impurity pellet injectionDisruptionsAlex James UC, San DiegoYes
52Determination of ITER LH Threshold powerGeneral IPPunit GohilGANo
53Test of Paleoclassical Model for Pedestal Electron Temperature ProfileELM Control & Pedestal PhysicsRichard GroebnerGAYes
54Steady State FDF Based on Hybrid ScenarioCore Integration (Steady-State Scenario)C. Craig PettyGAYes
55non-VFI Operations with RTEFITModel based ControlAlan HyattGANo
56Sustaining Low q(0) With Monster Sawtooth ControlCore Integration (Steady-State Scenario)C. Craig PettyGANo
57Gyroradius Scaling in Hybrid PlasmasCore Integration (Advanced Inductive)C. Craig PettyGANo
58ECCD in High Beta Poloidal PlasmasHeating & Current DriveC. Craig PettyGANo
59ECCD at High Electron TemperatureHeating & Current DriveC. Craig PettyGANo
60Dependence of Stiffness on ElongationTransport Model ValidationC. Craig PettyGANo
61Direct Measurement of ECCD Width from Modulated ECCDHeating & Current DriveC. Craig PettyGANo
62Measurement of Inductive Poloidal CurrentHeating & Current DriveC. Craig PettyGANo
63Extreme Off-Axis ECCDHeating & Current DriveC. Craig PettyGANo
64Sustained Monster SawteethEnergetic ParticlesC. Craig PettyGANo
65Simulation of Alpha Channeling Current DriveHeating & Current DriveC. Craig PettyGANo
66Separating Rotational Shear and rho* Scaling Effects on TransportTransport Model ValidationC. Craig PettyGANo
67High Performance Operation With Te=TiCore Integration (Steady-State Scenario)C. Craig PettyGANo
68Modulation of Bootstrap CurrentHeating & Current DriveC. Craig PettyGANo
69Electron Heat PinchTransportC. Craig PettyGANo
70Neutral Beam Current Drive ProfileHeating & Current DriveC. Craig PettyGAYes
71Well Aligned Current Drive for Sustaining High qminCore Integration (Steady-State Scenario)C. Craig PettyGANo
72Measuring the Structure of Tearing ModesStabilityC. Craig PettyGANo
73Mach Number Scan With Similar Parameters as JT-60UTransportC. Craig PettyGANo
74Is the 3/2 NTM Worth Suppressing in Hybrid Discharges?Core Integration (Advanced Inductive)C. Craig PettyGANo
75Simultaneous Suppression of 3/2 and 4/3 NTM with ECCDCore Integration (Advanced Inductive)C. Craig PettyGANo
76Voltage controlled VFI bus operationsGeneral PCOAlan HyattGANo
77Dependence of the H-L transition on toroidal rotationTransportPunit GohilGANo
78High Collisionless NBI Torque Drive for GAMs, aka the VH-mode path?TransportJohn DegrassieGANo
79Re-optimize the Breakdown processModel based ControlAlan HyattGANo
80Core transport barriers in EC-heated dischargesTransportMax AustinU of TexasYes
81ECH assisted breakdown and startup for DIII-D and ITERITER Startup, Shutdown, Vertical StabilityGary JacksonGAYes
82Optimize DIII-D startup, i.e. stop initiating on the outer wallGeneral PCOGary JacksonGAYes
83Is the Reduced L-H Threshold With Counter Beams Due to Lost Ions, or Velocity per se?Rotation PhysicsJohn DegrassieGANo
84Physics of n=3 nonresonant braking. Is there an unknown n=3 error field?RWM PhysicsGary JacksonGANo
85Current driven RWM target discharges for feedback stabilization experimentsRWM PhysicsGary JacksonGANo
86Characterization of Turbulence Associated with TEMsTransport Model ValidationJim C. DeBooGAYes
87Impact of Rotation on Incremental Diffusivity in Hybrid DischargesRotation PhysicsJim C. DeBooGANo
88Plasma rotation with Icoil rotating fieldsRotation PhysicsGary JacksonGANo
89Higher Beta ELM-Suppressed HybridsITER Demonstration DischargesC. Craig PettyGAYes
90RMP ELM-Suppression With Higher ConfinementELM Control & Pedestal PhysicsC. Craig PettyGANo
91Hybrid Beta Limit at Low RotationCore Integration (Advanced Inductive)C. Craig PettyGANo
92External n=3 RMP for ITER ELM Control TestsELM Control & Pedestal PhysicsMax E. FenstermacherLLNLNo
93Single Internal Row n=3 RMP for ELM ControlELM Control & Pedestal PhysicsMax E. FenstermacherLLNLNo
94Physics of Safety Factor Resonance for n=3 RMP ELM SuppressionELM Control & Pedestal PhysicsMax E. FenstermacherLLNLNo
95RMP Effect on Location of P-B Stability BoundaryELM Control & Pedestal PhysicsMax E. FenstermacherLLNLNo
96Determine Adiabatic Electron Response for High-n Modes in QH PlasmasEnergetic ParticlesRaffi NazikianPPPLYes
97Operational implementation of model-based shape control (MIMO)Model based ControlMichael WalkerGAYes
98Ion response to Te heat pulsesTransportJim C. DeBooGANo
99Establishment of a database for EMC3/EIRENE benchmark and direct comparison to TEXTOR (1)Thermal Transport in the Plasma BoundaryOliver SchmitzFZ JuelichNo
100Establishment of a database for EMC3/EIRENE benchmark and direct comparison to TEXTOR (2)ELM Control & Pedestal PhysicsOliver SchmitzFZ JuelichNo
101Measurements of Neutral Beam Excited State LifetimeTransportGeorge R. McKeeU of Wisconsin, MadisonYes
102Collisional damping of zonal flows/GAMsTransportGeorge R. McKeeU of Wisconsin, MadisonYes
103Turbulence and Transport dependence on Mach number in Hybrid dischargesTransportGeorge R. McKeeU of Wisconsin, MadisonYes
104Excitation of the Geodesic Acoustic Mode via Radial Field OscillationTransportGeorge R. McKeeU of Wisconsin, MadisonYes
105Comparison of EC and NBI H-mode ThresholdsTransportC. Craig PettyGANo
106Isolating particle sources and sinks in RMP H-modes with core pellet fuelingELM Control & Pedestal PhysicsTodd E. EvansGANo
107neutral beam injection for MSE calibration and comparison of NBCD with code calculationsHeating & Current DriveJay JayakumarLLNLNo
108Comparison of main ion and impurity rotation velocityRotation PhysicsRichard GroebnerGANo
109Daily Reference Shot Monitoring of Wall ConditionsBoundaryPhil WestGANo
110Role of coherent modes on edge pedestal and ELM behaviorBoundaryDmitry RudakovUC, San DiegoNo
111H-mode operation near the threshold powerITER Demonstration DischargesGuiding WangUC, Los AngelesYes
112Marginally Limited High Performance Plasmas with Density ControlCore-Edge IntegrationPhil WestGANo
113Understanding low density limit for L-H transition power thresholdGeneral IPGuiding WangUC, Los AngelesNo
114Test of TGLF transport model in pedestalELM Control & Pedestal PhysicsRichard GroebnerGANo
115Stable Impurity Enhanced Radiative Divertor Operation with Pellet PacingCore-Edge IntegrationRichard A. MoyerUC, San DiegoYes
116Access to betaN = 5 in a high li scenarioCore Integration (Steady-State Scenario)John FerronGAYes
117Investigating the Limits of Pellet pacing for ELM controlELM Control & Pedestal PhysicsRichard A. MoyerUC, San DiegoYes
118NTM stabilization and RMP in high li, high betaN dischargesCore Integration (Steady-State Scenario)John FerronGANo
119Study of moderate beta, high li transport and stabilityCore Integration (Steady-State Scenario)John FerronGANo
120H-mode power threshold in Hydrogen plasmasHydrogen DischargesPunit GohilGANo
121Reliable, flexible formation of 100% noninductive dischargesFully Noninductive High Beta OperationJohn FerronGANo
122ECCD stabilization of NTMs to improve the high beta phase of steady-state scenario dischargesFully Noninductive High Beta OperationJohn FerronGANo
123Pursue the q_min >2 path toward high noninductive fraction dischargesFully Noninductive High Beta OperationJohn FerronGANo
124Optimize the 6 gyrotron, q_min near 1.5, high noninductive fraction scenarioFully Noninductive High Beta OperationJohn FerronGAYes
125Discharges with complete 2nd stable regime accessStabilityJohn FerronGANo
126Dependence of ELM characteristics on toroidal rotation in hydrogen plasmasHydrogen DischargesPunit GohilGANo
127Intrinsic rotation vs NTVRotation PhysicsJohn DegrassieGANo
128RMP ELM-control in hydrogen plasmasHydrogen DischargesPunit GohilGANo
129Study of low-Z pellet shell ablationDisruptionsEric M. HollmannUC, San DiegoYes
130High BetaN, f_BS, ITB plasmasFully Noninductive High Beta OperationChris HolcombLLNLYes
132Momentum Transport Measurement Using Shape ModulationRotation PhysicsC. Craig PettyGANo
133Net Deuterium Retention In Unpumped and Pumped Discharges on DIII-D and Alcator C-ModHydrogenic RetentionPhil WestGAYes
134Characterization of QH-mode and EHO properties with edge toroidal rotationELM Control & Pedestal PhysicsPunit GohilGANo
135Carbon wall tritium removal using massive hydrogen injectionHydrogenic RetentionEric M. HollmannUC, San DiegoYes
136Completion of MP 2007-01-02: Dependence of Er, turbulence, and transport on RMP amplitudeELM Control & Pedestal PhysicsRichard A. MoyerUC, San DiegoYes
138Pellet induced H-mode at low toroidal rotationTransportPunit GohilGANo
139Direct Measurement of Momentum Drag from Error FieldsRotation PhysicsC. Craig PettyGANo
140Pellet pacing of ELMs in low toroidally rotating plasmasELM Control & Pedestal PhysicsPunit GohilGANo
141Enhanced ohmic confinemnt using edge RMPsHydrogen DischargesTodd E. EvansGANo
142High Beta, Reactor Relevant HybridCore Integration (Advanced Inductive)C. Craig PettyGANo
143Particle confinement regimes with RMP in n=3TransportOliver SchmitzFZ JuelichNo
144Resolve deviations between the measured and the EFIT predicted strike point positionModel based ControlOliver SchmitzFZ JuelichNo
145Resolve impact of mode spectrum on particle transport regimes with RMPELM Control & Pedestal PhysicsOliver SchmitzFZ JuelichNo
146Burst Disk Gas Jet for Disruption Mitigation on DIII-DDisruptionsLarry R. BaylorORNLYes
147Burst Disk Gas Jet for Disruption Mitigation on DIII-DDisruptionsLarry R. BaylorORNLYes
148electron transport in sawteethTransportEd LazarusORNLNo
149Hybrid beta limit at lower rotationRotation PhysicsRobert J. La HayeGAYes
151Test of Pellet Fueling Fast Transport TheoryGeneral IPLarry R. BaylorORNLYes
1522D Velocimetry of edge turbulence structures at the LH-transitionTransportDave SchlossbergU of Wisconsin, MadisonYes
153Simultaneous fluctuation amplitudes measured across the plasma radius in L- and H-modeTransportDave SchlossbergU of Wisconsin, MadisonYes
154Tearing Mode Beta Limits and Error Fields in Low Rotation Baseline PlasmasRotation PhysicsRichard Buttery UKAEAYes
1552/1 NTM beta limits in modest to strong counter torque plasmasRotation PhysicsRichard Buttery UKAEAYes
156ECCD control of sawteeth and monster sawteeth to avoid NTMsNTM StabilizationRichard Buttery UKAEAYes
157ELM pacing with small pelletsELM Control & Pedestal PhysicsLarry R. BaylorORNLYes
158Marginal island for 2/1 NTMsStabilityRobert J. La HayeGAYes
159Turbulence dynamics of integer q surfaces in near-sationary NCS discharges w/ off-axis ECCDTransportMorgan ShaferU of Wisconsin, MadisonYes
160Dependence of turbulence and transport on the safety factor and magnetic shearTransport Model ValidationMorgan ShaferU of Wisconsin, MadisonNo
161Multiple low-n RWM identification and feedback controlRWM PhysicsYongkyoon InFARTECH, Inc.Yes
162Can we prevent locked mode from being locked ?Rotation PhysicsYongkyoon InFARTECH, Inc.Yes
163How to maximize ELM control resources?ELM Control & Pedestal PhysicsYongkyoon InFARTECH, Inc.No
164Catastrophic MHD-affiliated non-axisymmetric fieldsError FieldsYongkyoon InFARTECH, Inc.Yes
165Dependence of Turbulence and Transport on Te/Ti in Low Rotation L & H ModesTransport Model ValidationGeorge R. McKeeU of Wisconsin, MadisonYes
166Test theory based models and empirical scaling for intrinsic rotation by changing turbulence modesRotation PhysicsEdward DoyleUC, Los AngelesYes
167Intermittency scaling for ITERBoundaryJose A. BoedoUC, San DiegoYes
168ELM supression at high densityITER Demonstration DischargesLarry R. BaylorORNLYes
169Can the RMP coils eliminate ELMs from SNs with B x gradB out of the divertor?ELM Control & Pedestal PhysicsThomas W. PetrieGANo
170Comparison of impurity screening between ELMing and ELM-suppressed plasmas?ELM Control & Pedestal PhysicsThomas W. PetrieGANo
171Completion of n=1 RMP ELM control studiesELM Control & Pedestal PhysicsRichard Buttery UKAEAYes
172Is the Radiating Divertor Scenario Compatible With ELM Suppression?ELM Control & Pedestal PhysicsThomas W. PetrieGANo
173Compatibility of ELM suppression with the radiating divertor in the hybridsELM Control & Pedestal PhysicsThomas W. PetrieGANo
174What is the nature of the heat flux outside a slot divertor and are particle drifts important?Thermal Transport in the Plasma BoundaryThomas W. PetrieGANo
175Turbulence & transport modifications in ECH plasmas and comparison to gyrokinetic simulationTransport Model ValidationTony PeeblesUC, Los AngelesNo
176Investigation of fast wave damping at 2nd and 3rd harmonics on injected hydrogen beamsHydrogen DischargesRobert I. PinskerGANo
177Compatibility of the radiative divertor with high performance plasma operationCore-Edge IntegrationThomas W. PetrieGAYes
178Optimal location for fueling pumped DN plasmasBoundaryThomas W. PetrieGANo
179Effect of particle drifts on particle exhaust in an ITER-like configurationBoundaryThomas W. PetrieGANo
180Complete ELM suppression with n=2 RMPsELM Control & Pedestal PhysicsRichard Buttery UKAEAYes
181Vertical Stability Control Physics for ITERITER Startup, Shutdown, Vertical StabilityDave HumphreysGAYes
182Measurement of the electrostatic Reynolds stress across the L-H transitionTransportRichard A. MoyerUC, San DiegoYes
183Improved Gas Jet Disruption Mitigation by I-coil-Enhanced Impurity TransportDisruptionsDave HumphreysGAYes
184Test of neoclassical toroidal viscosity (NTV) theory for magnetic brakingRotation PhysicsTed StraitGAYes
185Completion of MP 2007-01-02: test RMP effect on ELM stability and increase neped with pelletsELM Control & Pedestal PhysicsRichard A. MoyerUC, San DiegoYes
186Role of error fields in resistive wall mode stabilityRWM PhysicsTed StraitGAYes
187Stability control and disruption avoidance: initial demonstration of an integrated approachDisruptionsTed StraitGAYes
188ELM control with a single row of RMP coilsELM Control & Pedestal PhysicsTed StraitGANo
189Model Validation of Electron Transport Using Modulated ECHTransport Model ValidationKenneth GentleU of TexasNo
190Assessment of ITER startup with DIII-D similarity shapesITER Startup, Shutdown, Vertical StabilityThomas A. CasperLLNLYes
191Accessibility to AT regimes with ITER-scaled DIII-D shapesITER Startup, Shutdown, Vertical StabilityThomas A. CasperLLNLNo
192ITER controller assessmentITER Startup, Shutdown, Vertical StabilityThomas A. CasperLLNLNo
193Transport Locality and ECH DepositionTransportKenneth GentleU of TexasNo
194Current profile feedback controller verification for AT experimentsModel based ControlThomas A. CasperLLNLNo
195ECCD control of 2/1 NTM in ITER q95=3.2 shapeNTM StabilizationRobert J. La HayeGANo
196Density peaking at low collisionalityITER Demonstration DischargesThomas A. CasperLLNLNo
197Simultaneous ECCD control of 3/2 and 2/1 NTMsNTM StabilizationRobert J. La HayeGANo
198Tearing Mode locking avoidance with toroidal phase advance in the feedbackDisruptionsMichio OkabayashiPPPLYes
199RWM: Mode non-rigidity in low/high rotation plasmasRWM PhysicsMichio OkabayashiPPPLYes
200Edge Current Control of ELMsELM Control & Pedestal PhysicsJames D. CallenU of WisconsinYes
201Improvement of Dynamic Error Filed Correction by Active MHD Spectroscopy approach in closed feedbackError FieldsMichio OkabayashiPPPLNo
202Development of Model-based Current Profile Control at DIII-DModel based ControlEugenio Schuster Lehigh UYes
203Characterization and optimization of H-mode plasmasITER Demonstration DischargesPete PolitzerGANo
204Model-based Closed-loop Current Profile Control at DIII-DModel based ControlEugenio Schuster Lehigh UYes
205Characterization and optimization of advanced inductive and hybrid plasmas in the ITER configurationITER Demonstration DischargesPete PolitzerGANo
206Intrinsic rotation and SOL flowsRotation PhysicsPete PolitzerGANo
207Perpendicular resistivity in Ohm's lawHeating & Current DrivePete PolitzerGANo
208Measure the NBCD profileHeating & Current DrivePete PolitzerGANo
209Intermediate/high-k turbulence in electron ITBs and tests of gyrokinetic code predictionsTransport Model ValidationLothar SchmitzUC, Los AngelesYes
210Effect of loop voltage fluctuations on the pedestalELM Control & Pedestal PhysicsPete PolitzerGANo
211Dependence of Zonal Flows on magnetic shear in internal transport barriersTransport Model ValidationLothar SchmitzUC, Los AngelesYes
212Burn control simulationGeneral PCOPete PolitzerGANo
213QH-mode in hydrogen plasmasHydrogen DischargesPunit GohilGANo
214Flux pumping â?? modulation of the 3/2 NTM in hybrid/AI plasmas by ELMsCore Integration (Advanced Inductive)Pete PolitzerGANo
215The n=3 RFA excitation in the ELM-induced RWM by applying the n=3 extra error fieldRWM PhysicsMichio OkabayashiPPPLNo
216Measurement of Zonal Flows in the H-mode pedestalTransportLothar SchmitzUC, Los AngelesYes
217Is q profile modification the key element in hybrid and advanced inductive plasmas?Core Integration (Advanced Inductive)Pete PolitzerGANo
218Minimum rotation for hybrid/AI plasmasCore Integration (Advanced Inductive)Pete PolitzerGANo
219Hybrid/AI plasmas rotating in the counter-Ip directionCore Integration (Advanced Inductive)Pete PolitzerGANo
220Investigation of Alfvenic Activity and Resultant Fast Ion Transport with Low NBI PowerEnergetic ParticlesMichael Van ZeelandGAYes
221Investigate Impact of ECH on Alfvenic ActivityEnergetic ParticlesMichael Van ZeelandGAYes
222Reduced beta hybrid/AI plasmas and the transition to ELM-free VH-mode-like operationCore Integration (Advanced Inductive)Pete PolitzerGANo
223Noninductive, high betap plasmas â?? lower q95Fully Noninductive High Beta OperationPete PolitzerGANo
224Noninductive, high betap plasmas â?? broadband MHD and confinementFully Noninductive High Beta OperationPete PolitzerGANo
225Edge Ti (rotation) disturbance with residual stable RWM activityRotation PhysicsMichio OkabayashiPPPLYes
226Density, Bt, and Ip dependence of toroidal rotation effect on L-H transition power thresholdTransportGuiding WangUC, Los AngelesNo
227Inter-machine comparisons for heat flux scalingThermal Transport in the Plasma BoundaryCharles LasnierLLNLYes
228Optimization of combined Dynamic Error Field Correction and Direct RWM Feedback at Low RotationRWM PhysicsMichio OkabayashiPPPLYes
229Beam Ion Excitation of Beta Induced Alfvenic Acoustic EigenmodesEnergetic ParticlesNikolai GorelenkovPPPLYes
230Modulated ECCD for 2/1 NTM suppressionNTM StabilizationAnders WelanderGAYes
231Hydrogen Confinement at Low RotationHydrogen DischargesSteve AllenLLNLNo
232Rho-star scan for transport validation studiesTransport Model ValidationChristopher HollandUC, San DiegoYes
233ELM control in hybrid dischargesELM Control & Pedestal PhysicsSteve AllenLLNLNo
234Mach number scan for transport validation studiesTransport Model ValidationChristopher HollandUC, San DiegoYes
235nu-star scan for transport validation studiesTransport Model ValidationChristopher HollandUC, San DiegoYes
236Grad-Ti/Stiffness scan for transport validation studiesTransport Model ValidationChristopher HollandUC, San DiegoYes
237Feedback Controlled Radiative DivertorBoundarySteve AllenLLNLNo
238Search for long-range correlations and non-local behavior in turbulence dynamicsTransportChristopher HollandUC, San DiegoYes
239Scaling of SOL heat fluxThermal Transport in the Plasma BoundaryCharles LasnierLLNLNo
240B-Stark Validation Using Deuterium BeamsGeneral IPNovimir PablantUC, San DiegoNo
241Evaluation of effect of double-layer Faraday screen on rf voltage standoff in ELMing H-modeHeating & Current DriveRobert I. PinskerGAYes
242Beta Scaling of turbulence and transport in low-rotation H-Mode PlasmasTransport Model ValidationGeorge R. McKeeU of Wisconsin, MadisonYes
243Assess sensitivity of ITER demonstration discharges to variations in key physics parametersITER Demonstration DischargesEdward DoyleUC, Los AngelesYes
244B-Stark Validation Using Hydrogen BeamsHydrogen DischargesNovimir PablantUC, San DiegoYes
245Real time disruption detection/mitigationDisruptionsMichael WalkerGANo
246Improve empirical error correction for right-handed plasmasError FieldsMichael J. SchafferGANo
247BetaN=5 for 2 secondsCore Integration (Steady-State Scenario)Andrea M. GarofaloColumbia UNo
248Internal Structure of n=1 MHD Activity in Low Rotation PlasmaRotation PhysicsIoan N. BogatuFAR-TECH, Inc.Yes
249Determination of intrinsic rotation using torque rampsRotation PhysicsWayne M. SolomonPPPLNo
250H-mode transition assisted by edge ECHTransportRon PraterGANo
251Dependence of intrinsic rotation on applied error fieldRotation PhysicsWayne M. SolomonPPPLYes
252Test of toroidal momentum pinch modelRotation PhysicsWayne M. SolomonPPPLNo
253Main ion rotation studiesRotation PhysicsWayne M. SolomonPPPLNo
254Rotation studies in the absence of Alfven EigenmodesRotation PhysicsWayne M. SolomonPPPLNo
255Role of turbulent momentum transport for intrinsic rotationRotation PhysicsStefan MullerUC, San DiegoYes
256Turbulence characteristics in edge pedestal and its correlation with pedestal structure evolution from L-H transition to the first ELMELM Control & Pedestal PhysicsGuiding WangUC, Los AngelesNo
257Poloidal rotation as a function of toroidal rotationRotation PhysicsWayne M. SolomonPPPLNo
258Measurement of radial profile and radial propagation of density perturbations due to EHO in QH plasmasELM Control & Pedestal PhysicsGuiding WangUC, Los AngelesNo
259Effect of aspect ratio on momentum confinementRotation PhysicsWayne M. SolomonPPPLNo
260Poloidal spin up of plasma using off-axis neutral beam injectionTransportWayne M. SolomonPPPLNo
261Poloidal rotation comparison between forward & reverse BtTransportWayne M. SolomonPPPLNo
262Validation of GYROTransport Model ValidationRon PraterGANo
263Direct Measurement of E_rad Corrugation at Rational SurfacesTransportC. Craig PettyGANo
264Simultaneous measurement of density and temperature fluctuation level and radial correlation length in both low and high field side of L-mode plasmasTransport Model ValidationGuiding WangUC, Los AngelesNo
265Poloidal rotation comparison between forward & reverse IpTransportWayne M. SolomonPPPLNo
266"burning plasma" controlGeneral PCOPhil SnyderGANo
267Eigenmode model-based n=1 RWM feedback controlModel based ControlYongkyoon InFARTECH, Inc.Yes
268Study of turbulence effects on anomalous particle and momentum pinchesTransportLei ZengUC, Los AngelesNo
269Enhanced erosion from deuterium saturated materials during ELMsHydrogenic RetentionKarl UmstadterUC, San DiegoNo
270Simultaneous correction of B-coil bus and F-coil offset errorsError FieldsMichael J. SchafferGANo
271ECH Modification and Control of Pedestal ProfilesELM Control & Pedestal PhysicsPhil SnyderGANo
272Hydrogen Isotope Scaling of Turbulence and TransportTransport Model ValidationGeorge R. McKeeU of Wisconsin, MadisonYes
273Simultaneous correction of B-coil bus and F-coil offset errorsError FieldsMichael J. SchafferGANo
274Edge current measurementELM Control & Pedestal PhysicsPhil SnyderGANo
275Optimization w.r.t. plasma rotation of the error field correction from I-coilError FieldsAndrea M. GarofaloColumbia UNo
276Pedestal width in Hydrogen dischargesHydrogen DischargesPhil SnyderGANo
277Test of Neoclassical Toroidal Viscosity theory using modulated I-coil currentsRotation PhysicsKeith BurrellGAYes
278Density pump-out studies in USN divertored, RMP dischargesELM Control & Pedestal PhysicsZeke UnterbergORISE/ORNLNo
279Extrapolation of H-modes and Hybrids to ITERITER Demonstration DischargesC. Craig PettyGANo
280DiMES Investigation of Helium Plasma Induced Nanostructured Morphology on TungstenBoundaryMatthew BaldwinUC, San DiegoYes
281Production of a Mass gradient in DIII-D DischargesHydrogen DischargesJim LeuerGANo
282Test J-K Park theory of tokamak error field correctionError FieldsMichael J. SchafferGANo
284Test contribution of edge ion orbit loss to intrinsic toroidal rotationRotation PhysicsKeith BurrellGANo
288Measurement of internal structure of RFARWM PhysicsAndrea M. GarofaloColumbia UNo
289Main ion poloidal rotation measurements in helium plasmasRotation PhysicsKeith BurrellGANo
290Develop an L-mode error correction test plasmaError FieldsMichael J. SchafferGANo
291Prompt torque and zonal flow dampingRotation PhysicsKeith BurrellGAYes
292ELM suppression with I-coil error correctionELM Control & Pedestal PhysicsMichael J. SchafferGANo
293Minimum Contact Startup in DIII-DModel based ControlJim LeuerGANo
294Search for Structures Predicted in RMP ELM control modeingELM Control & Pedestal PhysicsRichard A. MoyerUC, San DiegoYes
295ELM suppression by single-row coil setsELM Control & Pedestal PhysicsMichael J. SchafferGANo
296Test neoclassical poloidal rotation prediction as a function of toroidal rotation speedRotation PhysicsKeith BurrellGANo
297Effect of Error Fields and RMPs on H-mode power threshold and transport barrierTransportRichard A. MoyerUC, San DiegoYes
298Balance between FW edge absorption by far-field sheaths and central absorptionHeating & Current DriveRobert I. PinskerGANo
299QH-mode studies as a function of edge rotationELM Control & Pedestal PhysicsKeith BurrellGANo
300QH-mode with co-injected neutral beamsELM Control & Pedestal PhysicsKeith BurrellGANo
301Does RMP ELM suppression have hysteresis?ELM Control & Pedestal PhysicsMichael J. SchafferGANo
302Diagnostic spatial cross calibration using edge sweeps in QH-modeELM Control & Pedestal PhysicsKeith BurrellGANo
303RF sustained QH-modeELM Control & Pedestal PhysicsKeith BurrellGANo
304Turbulence spreading experiment in plasma coreTransport Model ValidationKeith BurrellGANo
305Turbulence spreading experiment in the plasma edgeTransport Model ValidationKeith BurrellGANo
306Completion of MP 2007-01-02: Investigate direct effect of RMP on ELM StabilityELM Control & Pedestal PhysicsRichard A. MoyerUC, San DiegoYes
307ELM suppression by multi-harmonic RMPsELM Control & Pedestal PhysicsMichael J. SchafferGANo
308Resonant vs non-resonant brakingRotation PhysicsAndrea M. GarofaloColumbia UYes
309Simple as possible fast-ion transport by TAEsEnergetic ParticlesWilliam W. HeidbrinkUC, IrvineYes
310Giant sawteeth that never crashEnergetic ParticlesWilliam W. HeidbrinkUC, IrvineYes
311Off-axis NBCD with a small, upward-shifted plasmaCore Integration (Steady-State Scenario)Masanori MurakamiORNLYes
312test off-axis NBI with a small, upward-shifted plasmaHeating & Current DriveMasanori MurakamiORNLNo
313Extend full noninductive, high performance operationCore Integration (Steady-State Scenario)Masanori MurakamiORNLYes
314ITER steady state scenario demonstrationITER Demonstration DischargesMasanori MurakamiORNLNo
315L-mode RMP thermal footprintThermal Transport in the Plasma BoundaryMichael J. SchafferGANo
316effect of toroidal rotation on sawtooth periodStabilityEd LazarusORNLNo
317localized heating in the sawtooth region in oval plamasTransport Model ValidationEd LazarusORNLNo
318Bean & Oval Sawteeth without fast ionsStabilityEd LazarusORNLNo
319Stochastic thermal transport in DNDThermal Transport in the Plasma BoundaryMichael J. SchafferGANo
320Control VH-mode density rise by RMPGeneral FSMichael J. SchafferGANo
321RWM feedback control in ITER-like low rotation plasmasRWM PhysicsTed StraitGAYes
322Dynamic error field control for ITERError FieldsTed StraitGAYes
323Separating role of E x B and magnetic shear in stabilization of turbulence (DOE Milestone 166)Transport Model ValidationKeith BurrellGANo
324Dependence of non-resonant magnetic braking on nu_i and v_phi profileRotation PhysicsSteven A. SabbaghColumbia UYes
325Comparison of RWM stabilization physics in DIII-D and NSTXRWM PhysicsSteven A. SabbaghColumbia UYes
326Exploring the assumptions built in the RWM models: Hu-Bettie-Manickam and MARS codesRWM PhysicsMichio OkabayashiPPPLNo
327Understanding the role of wall sources and sinks during RMP H-modesELM Control & Pedestal PhysicsTodd E. EvansGANo
328Fast wave heating and current drive in AT plasmasCore Integration (Steady-State Scenario)Masanori MurakamiORNLNo
329Role of ECCD in sustaining steady state NCS scenarioCore Integration (Steady-State Scenario)Masanori MurakamiORNLNo
330ITER accessibility to hybrid regime using RFITER Demonstration DischargesMasanori MurakamiORNLNo
331ITB in ITER steady state scenarioITER Demonstration DischargesMasanori MurakamiORNLNo
332Comparison of high beta_p small ELM regime in DIII-D and JT-60UELM Control & Pedestal PhysicsNaoyuki OyamaJAEANo
333Turbulence dependence on rho_* via working gas species (Hydrogen and Helium)Transport Model ValidationTerry L. RhodesUC, Los AngelesYes
334Deuterium and carbon SOL flows in USN plasmas using toroidally symmetric CD4 injectionIntegrated ModelingMathias GrothLLNLYes
335Deuterium and carbon SOL flows in LSN or USN ELM-suppressed H-mode plasmasBoundaryMathias GrothLLNLNo
336Effect of core plasma rotation of deuterium and carbon SOL flowsBoundaryMathias GrothLLNLNo
337Control of SOL flows by Puff & PumpBoundaryMathias GrothLLNLNo
338Carbon migration in the divertor using the C13 methodHydrogenic RetentionMathias GrothLLNLNo
339Control of the heat and particle flux in radiative divertorsGeneral PCOMathias GrothLLNLNo
340Low triangularity, low nu*, RMP ELM controlELM Control & Pedestal PhysicsTodd E. EvansGANo
341Investigation of edge ne profile, fluctuations, and particle transport during RMPELM Control & Pedestal PhysicsLei ZengUC, Los AngelesNo
342Formation and radial propagation of ELM filament structure in DIII-DELM Control & Pedestal PhysicsLei ZengUC, Los AngelesNo
343DiMES: Exposure of CVD diamond filmBoundarySteven LisgoUKAEAYes
344Search for the critical ExB velocity shear for ITG and ETGRotation PhysicsLei ZengUC, Los AngelesNo
345Is high-k turbulence a significant contributor to the transport dynamics in the pedestal of H-mode?TransportTerry L. RhodesUC, Los AngelesNo
346Effect of ECH on low, intermediate and high k turbulence during density pumpoutTransportTerry L. RhodesUC, Los AngelesNo
347Magnetic shear dependence of low, intermediate and high k turbulence and GK simulation predictionsTransport Model ValidationTerry L. RhodesUC, Los AngelesYes
348Testing of VPS-W coating on Cu heat sink from ASIPPBoundaryClement WongGANo
349Test of importance of rotation in QH-mode using the I-coil for rotation and density controlELM Control & Pedestal PhysicsTom OsborneGANo
350Giant Sawtooth control with Alfven Eigenmodes in ITEREnergetic ParticlesGerrit J. KramerPPPLNo
351Recovery of D from thick exfoliated C-codeposits mechanically or using localized thermal oxidationHydrogenic RetentionPeter C. StangebyGA ,LLNL and U of TorontoNo
352Stabilization of Giant sawteeth by modifying the q-profile.Energetic ParticlesGerrit J. KramerPPPLNo
353Stabilization of giant sawteeth through the reduction of the fast particle pressure gradient.StabilityGerrit J. KramerPPPLNo
354The effect of plasma rotation on core-localized Alfven eigenmodes.Rotation PhysicsGerrit J. KramerPPPLNo
355Controlling q(0) with Elipticity induced Alfven Eigenmodes in DIIIDEnergetic ParticlesGerrit J. KramerPPPLNo
356Measuring the contribution of the main wall to tritium retentionHydrogenic RetentionPeter C. StangebyGA ,LLNL and U of TorontoNo
357Test the feasibility of operating ITER steady-state scenario demonstration discharges in DIII-DITER Demonstration DischargesJohn FerronGANo
358Te/Ti dependence of low, intermediate and high k turbulenceTransportTerry L. RhodesUC, Los AngelesNo
359Structure of EHO and Connection to ELM precursorELM Control & Pedestal PhysicsTom OsborneGANo
360Variation of Bootstrap Current with Collisionality in the H-Mode PedistalHeating & Current DriveBejamin F HudsonLLNLYes
361Scaling of H-mode pedestal width with rhostarELM Control & Pedestal PhysicsTom OsborneGANo
362Comparison of Bootstrap Current in ELMing and non-ELMing H-ModesHeating & Current DriveBejamin F HudsonLLNLNo
363Current versus voltage control of plasma shapeGeneral PCOBingjia XiaoASIPPNo
364Tungsten surface treatments for thermographyBoundaryCharles LasnierLLNLNo
365Visualization of 3-D SOL structures in RMP dischargesThermal Transport in the Plasma BoundaryNeil H BrooksGANo
366Effect of rotation, nonresonant field perturbation, betap, and triangularity on ELM sizeELM Control & Pedestal PhysicsTom OsborneGANo
367Deuterium retention in tungstenHydrogenic RetentionWilliam R. WamplerSandia National LaboratoriesYes
368Dependence of C deposition and D co-deposition rates on the surface temperatureHydrogenic RetentionDmitry RudakovUC, San DiegoYes
369DiMES Erosion Measurements with Detached Plasmas Induced by Argon InjectionBoundaryDmitry RudakovUC, San DiegoNo
370ECRH/ECCD Control of ELMsELM Control & Pedestal PhysicsFrancesco VolpeORAUYes
371Inducing 3/2 NTMs in hybrid discharges by means of ECRHCore Integration (Advanced Inductive)Francesco VolpeORAUYes
372Inducing 3/2 TM or NTM in hybrid discharges by means of modulated ECCDCore Integration (Advanced Inductive)Francesco VolpeORAUYes
373Prompt turn-off of ECCD when no longer required or detrimental for NTM stabilizationNTM StabilizationFrancesco VolpeORAUYes
374Assess optimal Error Field Correction by modulating I-coils at incommensurable frequenciesError FieldsFrancesco VolpeORAUYes
375Test of causality: mode rotation vs. plasma rotationRotation PhysicsFrancesco VolpeORAUYes
376RFA assisted RMP-ELM controlELM Control & Pedestal PhysicsIlon JosephUC, San DiegoNo
377Beta limits for 3/2 NTM onset and locking, as a function of rotationRotation PhysicsFrancesco VolpeORAUYes
378Counter Ip RMP-ELM suppressionELM Control & Pedestal PhysicsIlon JosephUC, San DiegoNo
379Can RMP strike point-splitting spread divertor heat flux?Thermal Transport in the Plasma BoundaryIlon JosephUC, San DiegoNo
380Calibrate separatrix deformation to ideal response theoryError FieldsIlon JosephUC, San DiegoNo
381Rapid-pulse Thomson Scattering scans in initial phase of RMP dischargesBoundaryZeke UnterbergORISE/ORNLNo
382Oblique-ECE-assisted MECCD suppression of NTMsNTM StabilizationFrancesco VolpeORAUYes
383Simultaneous control of ELMs and RWMsCore-Edge IntegrationFrancesco VolpeORAUYes
384Preferential LockingGeneral IPFrancesco VolpeORAUYes
385Sustained rotation of 2/1 for locking prevention, rotational mitigation and to assist ECCD controlNTM StabilizationFrancesco VolpeORAUYes
386Scaling of peak divertor heat flux and heat flux profile widths during MHD free L-mode operationThermal Transport in the Plasma BoundaryPhil WestGANo
387Chamber wall materials studyBoundaryClement WongGANo
388Type II ELMs and the Evolution of Profiles Between Type I ELMsELM Control & Pedestal PhysicsTom OsborneGANo
389Vertical Stability Control Using C-coil and I-coilGeneral PCODave HumphreysGANo
390Measurement of RFA using the SXR DiagnosticError FieldsMatthew LanctotColumbia UNo
391Optical Sensor for Feedback Control of Resistive Wall ModesRWM PhysicsMatthew LanctotColumbia UNo
392Resonant and Non-resonant magnetic brakingError FieldsMatthew LanctotColumbia UNo
393NSTX/DIII-D simularity experimentsEnergetic ParticlesEric FredricksonPPPLNo
394High energy confinement, low density Type III discharges and study of Type III - Type I transitionELM Control & Pedestal PhysicsTom OsborneGANo
395Turbulence dependence on rho_* via working gas species (Hydrogen and Helium) (see transport area)Hydrogen DischargesTerry L. RhodesUC, Los AngelesNo
396ELM interaction with main chamber wallBoundaryDmitry RudakovUC, San DiegoNo
397New ORNL pellet dropper to modify edge instability drivesTransportTerry L. RhodesUC, Los AngelesNo
398RMP pedestal transport and stability at normal densityELM Control & Pedestal PhysicsIlon JosephUC, San DiegoNo
399Co-Injected QH-mode access using edge EC/ECCDELM Control & Pedestal PhysicsPhil WestGANo
400Continue development of reactor optimized hybrid plasmasCore Integration (Advanced Inductive)Edward DoyleUC, Los AngelesNo
401Dedicated Experiments to Check Cross Section Correction forCER Rotation MeasurementsRotation PhysicsKeith BurrellGANo
402Comparison of Rotation Effects on Type I ELMing H-mode in DIII-Dã??and JT-60UELM Control & Pedestal PhysicsYutaka KamadaJAEANo
403Aspect Ratio Scaling of Core TurbulenceTransport Model ValidationShigeyuki KubotaUC, Los AngelesNo
404QH mode comparison in DIII-D and JT-60UELM Control & Pedestal PhysicsYoshiteru SakamotoJAEANo
405Role of pedestal on global confinement in hybrid scenario: extend beta range with AUG shapeELM Control & Pedestal PhysicsCostanza MaggiIPP GarchingNo
406Comparative study of RWM Excitation in low rotation plasmas on JT60U and DIII-DRWM PhysicsMichio OkabayashiPPPLNo
407ITER Mirror performance test. Active control over the deposition on the mirrors by the gas feed.BoundaryAndrey LitnovskyForschungszentrum JuelichNo
408Comparisons of L-mode and H-mode in hydrogen and deuteriumITER Demonstration DischargesRobert BudnyPPPLNo
409Demonstrate TokSys to Tokamak CapabilityGeneral PCOMickey R. WadeGANo
410Pedestal width dependence on BetaELM Control & Pedestal PhysicsAnthony W LeonardGANo
411Poloidal Asymmetry of Separatrix heat flux in H-modeThermal Transport in the Plasma BoundaryAnthony W LeonardGANo
412Pedestal Width dependence on Grad-B DirectionELM Control & Pedestal PhysicsAnthony W LeonardGANo
413RMP ELM suppression dependence on Grad-B drift directionELM Control & Pedestal PhysicsAnthony W LeonardGANo
414Studies of ITER-like castellation in DIII-D: impact of castellation shape on fuel retention in gapsHydrogenic RetentionAndrey LitnovskyForschungszentrum JuelichYes
415Rapid pellets for lower density radiative divertorCore-Edge IntegrationAnthony W LeonardGANo
416RWM n=1 Component Internal Structure in Low Rotation PlasmaRWM PhysicsIoan N. BogatuFAR-TECH, Inc.No
417Injection of pre-characterized dust in using DiMESBoundaryDmitry RudakovUC, San DiegoNo
418Does the Pedestasl spin the plasma?Rotation PhysicsFrancis PerkinsU of ColoradoNo
419Fluid SOL model validation for helium plasmasIntegrated ModelingMathias GrothLLNLNo
420Rotation vs Ion Loss in L-H Transition ThresholdTransportMickey R. WadeGANo
421q95 < 3 Hybrid PlasmasITER Demonstration DischargesMickey R. WadeGANo
422Monitoring dust levels following entry ventBoundaryDmitry RudakovUC, San DiegoNo
423ITER shutdown with li controlITER Startup, Shutdown, Vertical StabilityT. C. LuceGANo
424Test of thermal ion ripple loss as key parameter for L-H transitionTransportT. C. LuceGANo
425Extension of advanced inductive domain to lower q95Core Integration (Advanced Inductive)T. C. LuceGANo
426Confinement improvement or degradation with counter injectionRotation PhysicsT. C. LuceGANo
427High q95 hybrid as a test of current evolution modelsCore Integration (Advanced Inductive)T. C. LuceGANo
428Bootstrap fraction as a function of q_minCore Integration (Steady-State Scenario)T. C. LuceGANo
429Relative disruption frequency of hybrid and baseline scenarioITER Demonstration DischargesT. C. LuceGANo
430Measure rotation screening of known applied error fieldsError FieldsT. C. LuceGANo
431Develop method for optimization of error field correctionError FieldsT. C. LuceGANo
432Vertical stability of ohmic plasmas in ITER shapeITER Startup, Shutdown, Vertical StabilityT. C. LuceGANo
433ELM pacing and suppression by "plasma wobbling" 'a la TCVELM Control & Pedestal PhysicsFrancesco VolpeORAUYes
434Modulate I-coils to induce edge currents and affect/study ELMsELM Control & Pedestal PhysicsFrancesco VolpeORAUYes
435Modulate Ip to modulate edge current above/below peeling limitELM Control & Pedestal PhysicsFrancesco VolpeORAUYes
436Sheath factor measurement in Pisces compared with DIII-DThermal Transport in the Plasma BoundaryCharles LasnierLLNLNo
437Study of turbulence during RMPsELM Control & Pedestal PhysicsJose A. BoedoUC, San DiegoNo
438Momentum transfer across separatrixRotation PhysicsJose A. BoedoUC, San DiegoNo
439SHeath physics studiesThermal Transport in the Plasma BoundaryJose A. BoedoUC, San DiegoNo
440Plasma startup with compensating n=1(=3) error magnetic field components before the plasma ignition with I-coil feedbackGeneral PCOMichio OkabayashiPPPLNo
441Does the LH threshold go back up with strong ctr-NBI?TransportT. C. LuceGANo
442Rho* scaling of the LH thresholdTransportT. C. LuceGANo
443Run hybrid plasmas to the ideal MHD limitCore Integration (Advanced Inductive)T. C. LuceGANo
444Rho* scaling in hydrogen L modeHydrogen DischargesT. C. LuceGANo
445Effect of ECCD on sawteeth in H modeStabilityT. C. LuceGANo
446Hydrogen Sensor Diagnostic for DIII-DHydrogenic RetentionDean BuchenauerSandia National LaboratoriesNo
447Rho* Scaling of Alfvenic Activity Using Hydrogen DischargeHydrogen DischargesMichael Van ZeelandGANo
448Sensitivity of ELMs and Particle Control to TriangularityITER Demonstration DischargesC. Craig PettyGANo
449Target Plate Heat flux, sheath power transmission factor, and Power AccountingBoundaryJonathan G. WatkinsSandia National LaboratoriesNo
450Search for a window of RWM instability at high rotationRWM PhysicsHolger ReimerdesColumbia UNo
451Systematic study of in-situ boronizationBoundaryClement WongGANo
452Systematic study of in-situ boronizationBoundaryClement WongGANo
453Edge Ti (rotation) disturbance with residual stable RWM activityRWM PhysicsMichio OkabayashiPPPLNo
454The n=3 RFA excitation in the ELM-induced RWM by applying the n=3 extra error fieldRWM PhysicsMichio OkabayashiPPPLNo
455Tearing Mode locking avoidance with toroidal phase advance in the feedbackRWM PhysicsMichio OkabayashiPPPLNo
456Improvement of Dynamic Error Filed Correction by Active MHD Spectroscopy approach in closed feedbackRWM PhysicsMichio OkabayashiPPPLNo
457Plasma startup with compensating n=1(=3) error magnetic field components before the plasma ignition with I-coil feedbackRWM PhysicsMichio OkabayashiPPPLNo
458Massive Gas Injection during Ip RampdownDisruptionsTom JerniganORNLNo
459Massive Gas Injection of ECH Heated PlasmaDisruptionsTom JerniganORNLNo
460Performance sensitivity studies of steady-state scenario (low rotation, Te~Ti)Core Integration (Steady-State Scenario)Edward DoyleUC, Los AngelesNo
461Affect of MHD stability on pedestal width at low triangularityELM Control & Pedestal PhysicsRichard GroebnerGANo
462Modulated ECH to study pedestal electron thermal transport in ELM-stabilized discharges via RMPELM Control & Pedestal PhysicsRichard GroebnerGANo
463Real-time q and Te profile control based on dynamical model approachModel based ControlDidier J MazonCEA CadaracheNo
464Measurement of RFA using the SXR DiagnosticRWM PhysicsMatthew LanctotColumbia UNo
465Gas Puff ImagingBoundaryJonathan YuUC, San DiegoNo
466ECCD stabilization of non-rotating mode in high beta, low-torque plasmasRWM PhysicsHolger ReimerdesColumbia UNo
467NTM (de)stabilization by co-/ctr-ECCD in island O-/X-pointNTM StabilizationFrancesco VolpeORAUNo
468Pair formation during disruptionsDisruptionsFrancesco VolpeORAUNo
469Prompt Beam Ion Loss Reduction & SuppressionEnergetic ParticlesYubao ZhuUC, IrvineNo
470Experimental emulation of ITER port-plug RWM coil asymmetriesRWM PhysicsMichael WalkerGANo
471Dependence of core rotation on dRsepRotation PhysicsWayne M. SolomonPPPLNo
472"Simple as possible" tests of TEM to ITG transitionsTransport Model ValidationEdward DoyleUC, Los AngelesNo
473Comparison of particle and momentum diffusivities and pinches in helium dischargesRotation PhysicsRajesh MaingiORNLNo
474L-H transition threshold with ECH induced H-modesTransportEdward DoyleUC, Los AngelesNo
475Studies of C deposition and D co-deposition in tile gapsHydrogenic RetentionDmitry RudakovUC, San DiegoNo
476ECCD profile in presence of magnetic islandHeating & Current DriveRon PraterGANo
477Dust Generation at Tile Leading EdgesBoundaryPhil WestGANo
478W Rod Armor Plasma ExposureBoundaryClement WongGANo
479Thermal Energy Scan for Helium MGIDisruptionsJohn C. WesleyGANo
480Physics and Power Threshold of Low Rotation L- to H-mode TransitionsTransportLothar SchmitzUC, Los AngelesNo
481Physics and Power Threshold of Low Rotation L- to H-mode TransitionsTransportLothar SchmitzUC, Los AngelesNo
482Test of resistive MHD linear stability threshold and saturated island structure against modelsIntegrated ModelingLang L LaoGANo
483Parasitic edge losses during Fast Wave Current Drive and HeatingHeating & Current DriveMiklos PorkolabMass. Inst. of TechnologyNo
484The unexplored SN/DN transition zone in the SOLBoundaryJonathan G. WatkinsSandia National LaboratoriesNo
485Sheath Factor measurement in unbalanced Double NullBoundaryJonathan G. WatkinsSandia National LaboratoriesNo
486RMP fueling effect on pressure profile and ELMsELM Control & Pedestal PhysicsJonathan G. WatkinsSandia National LaboratoriesNo
487Target plate conditions during ELM suppressionELM Control & Pedestal PhysicsJonathan G. WatkinsSandia National LaboratoriesNo
488Role of pedestal in beta scaling of confinementTransportAnthony W LeonardGANo
489Relativistic effects on profile reflectometry and a new potential Te measurementGeneral IPLei ZengUC, Los AngelesNo
490Optimal Density Control in Double-null and near Double-null High Performance PlasmasCore-Edge IntegrationThomas W. PetrieGANo
492Particle balance in hybrid plasmas over a full day of operations with no helium glow conditioningHydrogenic RetentionPhil WestGANo
493Does Intrinsic Rotation Depend on Beam Ions?Rotation PhysicsC. Craig PettyGANo
494RWM thresholds without tearing modesRWM PhysicsRichard Buttery UKAEANo
495Can n=3 fields raise n=1 error field thresholds?Error FieldsRichard Buttery UKAEANo