ID |
Title |
Research Area |
Name |
Affiliation |
Time Req'ed |
ITPA Joint Exp |
ITER IO Urgent Research Task |
170 | Establishing the relationship between core torque, velocity profiles near the pedestal, and far-SOL flows. | Address Critical Detachment Physics Models | Samuell | LLNL | Yes | No | No |
171 | Extending CIS to the pedestal and beyond. | PE - Pedestal/SOL physics and Pedestal optimization | Samuell | LLNL | Yes | No | No |
172 | Quantifying Carbon Entrainment in H-mode plasmas | Address Critical Detachment Physics Models | Samuell | LLNL | Yes | No | No |
15 | 3D fields for ELM suppression of AT scenario plasmas | Understand Limits and Means to Extend ELM suppression for future | Victor | LLNL | Yes | No | No |
40 | Measuring Non-Axisymmetric Heat and Particle Flux Footprints in n=2 ELM Suppression | Understand Limits and Means to Extend ELM suppression for future | Briesemeister | ORNL | Yes | No | No |
65 | Commissioning of the Laser Blow-off System on DIII-D | BPP - turbulence and transport | Howard | MIT -PSFC | Yes | No | No |
261 | Effect of orbit modification on intrinsic rotation | Develop Basis to Predict and Control Rotation in ITER | Nazikian | PPPL | Yes | No | No |
133 | Validation of New W I SXB Ratios Using Ultraviolet Emission for Improved Erosion Diagnosis | AMV: Erosion/migration | Ennis | Auburn U | Yes | No | No |
134 | W II Ultraviolet Emission for Redeposition Diagnosis | AMV: Erosion/migration | Ennis | Auburn U | Yes | No | No |
95 | Use of shape driven vertical motion to probe non-axisymmetric VDE SOL currents | Disruption Mitigation Physics | Cabrera | Columbia U | Yes | No | No |
102 | Maximize performance of the low-torque ITER demonstration discharges as a function of stability | Control and Understand Core Stability in low Torque ITER Baseline | Hanson | Columbia U | Yes | No | No |
100 | Understand and control n=1 and n=2 magnetic response of low-torque ITER demonstration discharges | Control and Understand Core Stability in low Torque ITER Baseline | Hanson | Columbia U | Yes | No | No |
99 | Safe, low n NTV in Highly 3D Plasmas | Develop Basis to Predict and Control Rotation in ITER | Logan | Columbia U | Yes | No | No |
48 | Demonstrate NTV Torque Profile Control Varying 3D Field Spectra | Develop Basis to Predict and Control Rotation in ITER | Logan | Columbia U | Yes | No | No |
49 | Search for EF Driven Rotation with Positive NTV Offset | Develop Basis to Predict and Control Rotation in ITER | Logan | Columbia U | Yes | No | No |
50 | ELM Suppression Feedback using Reluctance Eigenmode Responses | Understand Limits and Means to Extend ELM suppression for future | Logan | Columbia U | Yes | No | No |
69 | Optimized lower torque hybrids | Integrated Core-Edge Steady State Solution | Turco | Columbia U | Yes | No | No |
19 | Use real time CER to test rotation actuation and 3D field effects | Develop Basis to Predict and Control Rotation in ITER | Chrystal | GA | Yes | No | No |
274 | Understand and Optimze n=2 Plasma Response for ELM Suppression in High Beta Regimes | Integrated Core-Edge Steady State Solution | Nazikian | GA | Yes | No | No |
230 | Exploring Hyteresis and Threshold Required for RMP ELM Suppression in DIII-D ISS Plasmas | Understand Limits and Means to Extend ELM suppression for future | Nazikian | GA | Yes | No | Yes |
225 | Improved Access to and Higher Performance of RMP ELM Suppressed Plasmas With Closed Divertor | Understand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL Dynamics | Nazikian | GA | Yes | No | Yes |
135 | Enhanced Hybrid Plasma Performance and Its Impact on Heat Flux Reduction | Integrated Core-Edge Steady State Solution | Petrie | GA | Yes | No | No |
104 | QH-mode with zero torque throughout | Understand Limits and Means to Extend ELM suppression for future | Burrell | GA | Yes | No | No |
194 | Physics of the high li scenario at more reactor-relevant parameters | D&C - steady state (apart from core-edge SS thrust) | Ferron | GA | Yes | No | No |
189 | Physics basis for startup of a high fNI, high betaN discharge with uniform loop voltage profile | D&C - steady state (apart from core-edge SS thrust) | Ferron | GA | Yes | No | No |
260 | Mitigation of fast ion effects in advanced scenario discharges | Integrated Core-Edge Steady State Solution | Ferron | GA | Yes | No | No |
269 | Develop, test and exploit new density feedback algorithm with dynamic target control | Scenarios and Transport | Garofalo | GA | Yes | No | No |
247 | Test nonlinear theory of EHO | Understand Limits and Means to Extend ELM suppression for future | Garofalo | GA | Yes | No | No |
283 | Develop low-torque access to QH-mode for ITER Baseline | Control and Understand Core Stability in low Torque ITER Baseline | Garofalo | GA | Yes | No | No |
229 | Measure cross phase of density, ion temperature, and radial flow fluctuations associated with EHO | Understand Limits and Means to Extend ELM suppression for future | Garofalo | GA | Yes | No | No |
182 | Understand return of ELMs in low torque QH-mode at low q95 | Understand Limits and Means to Extend ELM suppression for future | Garofalo | GA | Yes | No | No |
224 | Quantify relationship between SOL sources of fuel/impurities and pedestal profiles/transport | Understand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL Dynamics | Groebner | GA | Yes | No | No |
326 | Effect of damaged tungsten on operations | AMV: Erosion/migration | De Temmerman | ITER Organization | Yes | Yes | Yes |
327 | Droplet ejection and vapour shielding during transient melting of Al | AMV: Erosion/migration | De Temmerman | ITER Organization | Yes | No | Yes |
44 | Understanding the density dependence of WI S/XB coefficients | AMV: Erosion/migration | Abrams | GA | Yes | No | No |
45 | The impact of surface temperature on high-Z/low-Z mixed material balance | AMV: Erosion/migration | Abrams | GA | Yes | No | No |
185 | Improved access and operating space for the low-torque wide-pedestal QH | Understand Limits and Means to Extend ELM suppression for future | Chen | GA | Yes | No | No |
232 | Edge momentum pinch: density scale length and strength of ITG | Develop Basis to Predict and Control Rotation in ITER | Grierson | GA | Yes | No | No |
203 | Residual stress driven rotation peaking | Develop Basis to Predict and Control Rotation in ITER | Grierson | GA | Yes | No | No |
66 | Maintaining divertor detachment through H-L back transition | DO: Detachment & control (apart from Detachment Physics Thrust) | Eldon | GA | Yes | No | No |
4 | Optimized high-qmin performance using beam ion phase space tailoring to control Alfvenic activity | D&C - steady state (apart from core-edge SS thrust) | Pace | GA | Yes | No | No |
317 | Demonstrating Plasma Performance and Technology to Increase Fusion Yield with Spin Polarized Fuel | Torkil Jensen Award | Pace | GA | Yes | No | No |
91 | Achieve detachment at low/medium core density | Understand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL Dynamics | Wang | GA | Yes | No | No |
178 | Impact of impurity detachment on pedestal | Understand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL Dynamics | Wang | GA | Yes | No | No |
266 | Modulated ECH Driven Transport During RMP | BPP - turbulence and transport | Brookman | GA | Yes | No | No |
242 | Low-field ELM-suppression with edge ECCD | Understand Limits and Means to Extend ELM suppression for future | Lyons | GA | Yes | No | No |
273 | Use edge ECCD to achieve ELM suppression with little-to-no 3D field | Torkil Jensen Award | Lyons | GA | Yes | No | No |
137 | Overdriven ELM suppression with external three-dimensional magnetic perturbations | Understand Limits and Means to Extend ELM suppression for future | Lyons | GA | Yes | No | No |
73 | Understand the role of Shafranov shift, q profile on the formation of ITB in high betap plasmas | Scenarios and Transport | Ding | GA | Yes | No | No |
136 | ELM energy scaling collisionality scan | PE - Pedestal/SOL physics and Pedestal optimization | Knolker | GA | Yes | No | No |
144 | Validation of SAS Design Concept | Understand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL Dynamics | Guo | GA | Yes | No | No |
176 | ELM-resolved fuel recycling on pre-conditioned C/metal surfaces | AMV: Erosion/migration | Bykov | GA | Yes | No | No |
177 | Non thermal contribution to edge radiation in the mid IR range in different plasma scenarios | General Physics | Bykov | GA | Yes | No | No |
275 | ELM-suppressed Hybrid Plasmas with Radiating Divertor | Integrated Core-Edge Steady State Solution | Thome | GA | Yes | No | No |
276 | Core Transport Dependence on Magnetic Shear in Hybrid Plasmas | Integrated Core-Edge Steady State Solution | Thome | GA | Yes | No | No |
118 | QH-mode edge in a hybrid plasma | Integrated Core-Edge Steady State Solution | Thome | GA | Yes | No | No |
238 | Does intrinsic stochasticity due to internal MHD drive intrinsic rotation? | Develop Basis to Predict and Control Rotation in ITER | Tobias | Los Alamos National Laboratory | Yes | No | No |
54 | correlation of stochasticity and enhanced momentum transport in multi-helicity discharges | D&C - stability (apart from core stability in low torque ITER thrust) | Tobias | Los Alamos National Laboratory | Yes | No | No |
166 | Direct measurement of core-localized MHD via toroidally separated interferometers | Control and Understand Core Stability in low Torque ITER Baseline | Davis | Massachusetts Institute of Technology | Yes | No | No |
167 | Direct measurement of core-localized MHD via toroidally separated interferometers | BPP - Energetic Particle Physics | Davis | Massachusetts Institute of Technology | Yes | No | No |
140 | Kinetic Ballooning Modes in H-Mode Inner Core | BPP - turbulence and transport | Ernst | Massachusetts Institute of Technology | Yes | No | No |
84 | Effect of Electron Heating on Momentum & Particle Transport in Reverse Shear QH-Modes | Develop Basis to Predict and Control Rotation in ITER | Ernst | Massachusetts Institute of Technology | Yes | No | No |
316 | Intrinsic Rotation and Core Transport in Wide Pedestal QH-Mode Approaching Burning Plasma Conditions | Develop Basis to Predict and Control Rotation in ITER | Ernst | Massachusetts Institute of Technology | Yes | No | No |
64 | Commissioning of the Laser Blow-off System on DIII-D | BPP - turbulence and transport | Howard | Massachusetts Institute of Technology | Yes | No | No |
138 | Multi-Scale and Multi-Channel Turbulence and Transport in the ITER Baseline Scenario | BPP - turbulence and transport | Howard | Massachusetts Institute of Technology | Yes | No | No |
196 | Control of Radial Electric Field with the Snowflake Divertor Configuration in QH-mode | Torkil Jensen Award | Wilks | Massachusetts Institute of Technology | Yes | No | No |
113 | Internal Plasma Response of n=2 RMP Suppressed Discharges | Understand Limits and Means to Extend ELM suppression for future | Shafer | ORNL | Yes | No | No |
98 | ELM suppression with radiative/detached divertor condition by n=2 phase scan | Understand Limits and Means to Extend ELM suppression for future | Ahn | ORNL | Yes | No | No |
221 | AE Critical Gradient Study in H-Mode (Steady-State Scenario) | D&C - steady state (apart from core-edge SS thrust) | Collins | ORNL | Yes | No | No |
120 | Understanding the Role of Localized Gas Fueling in the SAS divertor | Understand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL Dynamics | Hinson | ORNL | Yes | No | No |
121 | Impact of 3D Sheath Boundary Condition During RMP on Material Erosion and Redeposition | AMV: 3D effects | Hinson | ORNL | Yes | No | No |
122 | Robustness of Film Adhesion of Cold-Sprayed Materials in a Tokamak Divertor Environment | AMV: Erosion/migration | Hinson | ORNL | Yes | No | No |
60 | 3D pedestal turbulence studies during ELM suppression with rotating n=2 I-coils | Understand Limits and Means to Extend ELM suppression for future | Wilcox | ORNL | Yes | No | No |
97 | Explore density pumpout mechanism and scaling | Understand Limits and Means to Extend ELM suppression for future | Wilcox | ORNL | Yes | No | No |
96 | Kick off helical core with core pressure disturbance | D&C - steady state (apart from core-edge SS thrust) | Wingen | ORNL | Yes | No | No |
92 | Scaling of helical core in high beta hybrid discharges | Integrated Core-Edge Steady State Solution | Wingen | ORNL | Yes | No | No |
93 | Scaling of helical core in high beta hybrid discharges | D&C - steady state (apart from core-edge SS thrust) | Wingen | ORNL | Yes | No | No |
94 | Kick off helical core with core pressure disturbance | Integrated Core-Edge Steady State Solution | Wingen | ORNL | Yes | No | No |
119 | High Performance Pedestal with SAS Divertor | Understand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL Dynamics | Snyder | ORNL | Yes | No | No |
149 | Role of predator-prey cycles in maintaining the transport in EHO-free wide pedestal QH-mode. | Understand Limits and Means to Extend ELM suppression for future | Kumar Barada | UCLA | Yes | No | No |
143 | Expose UFG W to DIII-D discharges to demonstrate improved properties useful in future PFCs | AMV: Erosion/migration | Barton | Sandia National Lab | Yes | No | No |
150 | Test displacement damage recovery and erosion in UFG-W | AMV: Erosion/migration | Barton | Sandia National Lab | Yes | No | No |
72 | Erosion of tungsten-alternative PFCs due to Type I ELMs in DIII-D | AMV: Erosion/migration | Coburn | Sandia National Lab | Yes | No | No |
153 | Main ion poloidal flow and hysteresis across the L-H and H-L transitions | BPP - L-H transition | Schmitz | UCLA | Yes | No | No |
154 | Mitigate L-H transition threshold increase via LFS/HFS pellet injection | BPP - L-H transition | Schmitz | UCLA | Yes | No | No |
151 | Minimize L-H transition power threshold with n=2,n=3 RMP | BPP - L-H transition | Schmitz | UCLA | Yes | No | No |
58 | Explore Electro-Magnetic turbulence by using Faraday-effect polarimeter | BPP - turbulence and transport | Chen | UCLA | Yes | No | No |
59 | Parametric dependence of micro-tearing mode and associated transport | BPP - turbulence and transport | Chen | UCLA | Yes | No | No |
299 | Role of predator-prey cycles in maintaining the transport in EHO-free wide pedestal QH-mode. | PE - QH mode (non ELM suppression thrust) | Kumar Barada | UCLA | Yes | No | No |
126 | Will discharges with SAS divertors have low P_threshold_L->H? | Understand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL Dynamics | Stangeby | U of Toronto | Yes | No | No |
128 | How to interpret SAS detachment for toroidally localized gas injection? | Understand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL Dynamics | Stangeby | U of Toronto | Yes | No | No |
204 | Infer Te at SAS target from D_αlpha/I_sat, D_beta/I_sat ratios | Understand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL Dynamics | Stangeby | U of Toronto | Yes | No | No |
205 | W-pellet injection to calibrate the Deposition Probe | AMV: Erosion/migration | Stangeby | U of Toronto | Yes | No | No |
206 | Precise measurement of the concentricity of the strike point in SAS | Understand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL Dynamics | Stangeby | U of Toronto | Yes | No | No |
46 | Qualify He exhaust capacity during RMP ELM suppression in relation to tau_E | Understand Limits and Means to Extend ELM suppression for future | Schmitz | U of Wisconsin | Yes | No | No |
218 | Investigating Flux Pumping with ELM Suppression in hybrids | D&C - steady state (apart from core-edge SS thrust) | Taylor | Oak Ridge Associated Universities | Yes | No | No |
219 | Investigating Flux Pumping in Hybrids with Applied n=2 Fields | D&C - steady state (apart from core-edge SS thrust) | Taylor | Oak Ridge Associated Universities | Yes | No | No |
270 | Investigating Flux Pumping with ELM Suppression in hybrids | Integrated Core-Edge Steady State Solution | Taylor | Oak Ridge Associated Universities | Yes | No | No |
271 | Investigating Flux Pumping in Hybrids with Applied n=2 Fields | Integrated Core-Edge Steady State Solution | Taylor | Oak Ridge Associated Universities | Yes | No | No |
123 | Test newly identified physical principles for RMP ELM suppression | Understand Limits and Means to Extend ELM suppression for future | Callen | U of Wisconsin | Yes | No | No |
124 | Explore and test models for q_95 windows in n=2 RMP ELM suppression | Understand Limits and Means to Extend ELM suppression for future | Callen | U of Wisconsin | Yes | No | No |
157 | Characterizing the Effects of Impurity Injection on Instabilities Driving ECH Density Pumpout | BPP - turbulence and transport | Truong | Sandia National Lab | Yes | No | No |
43 | Radiative divertor physics with impurity seeding in forward and reversed BT | Address Critical Detachment Physics Models | Jarvinen | VTT Technical Research Centre | Yes | No | No |
68 | Active handling of 3D divertor power deposition with impurity seeding and gas puffing for EAST long pulse operations | Boundary | Wang | ASIPP | Yes | Yes | Yes |
82 | Understanding the effect of impurities on H-mode pedestal structure | PE - Pedestal/SOL physics and Pedestal optimization | Giroud | CCFE | Yes | Yes | No |
249 | Optimization and improvement of energy confinement of RMP ELM suppressed plasma | PE - RMP and pellets (non ELM suppression thrust) | Sung | KAIST | Yes | No | No |
180 | Solving the challenges facing modeling of divertor detachment | Address Critical Detachment Physics Models | McLean | LLNL | Yes | No | No |
240 | RMP ELM suppression of high q_min plasmas | Integrated Core-Edge Steady State Solution | Victor | LLNL | Yes | No | No |
132 | Imaging Three-Dimensional Flow Structures in ELM-suppressed H-mode plasmas. | Understand Limits and Means to Extend ELM suppression for future | Samuell | LLNL | Yes | No | No |
79 | Phase scan of n=3 RMP ELM Suppression | Understand Limits and Means to Extend ELM suppression for future | Ferraro | PPPL | Yes | No | No |
114 | Explore Threshold and Hysteresis for RMP ELM Suppression in DIII-D | Understand Limits and Means to Extend ELM suppression for future | Cui | PPPL | Yes | No | No |
263 | Exploring Dependence of Core Confinement on the RMP Amplitude and Edge Te/Ti | Integrated Core-Edge Steady State Solution | Cui | PPPL | Yes | No | No |
2 | Advanced RWM control with external coils | D&C - stability (apart from core stability in low torque ITER thrust) | Clement | PPPL | Yes | No | No |
89 | Direct identification of multi-mode plasma response for improved MHD stability control | Control and Understand Core Stability in low Torque ITER Baseline | Wang | PPPL | Yes | No | No |
90 | Optimize ELM suppression and quantify tearing drive with Nyquist optimized coil phase and frequency | Understand Limits and Means to Extend ELM suppression for future | Wang | PPPL | Yes | No | No |
142 | Effect of detachment on ELM pacing and mitigation by pellet injection | Understand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL Dynamics | Bortolon | PPPL | Yes | No | No |
145 | Stabilization of ELMs by counter beam injection | PE - Pedestal/SOL physics and Pedestal optimization | Bortolon | PPPL | Yes | No | No |
139 | ELM pacing by pellet injection in low-collisionality ITER relevant scenarios | PE - RMP and pellets (non ELM suppression thrust) | Bortolon | PPPL | Yes | No | No |
234 | Detachment of a lithiated divertor strike point | Understand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL Dynamics | Bortolon | PPPL | Yes | No | No |
284 | ECCD and ECH for IBS with real-time modulation control | Control and Understand Core Stability in low Torque ITER Baseline | Kolemen | PPPL | Yes | No | No |
141 | Adaptive Pedestal Control for ELM Free/Mitigated Scenarios | Understand Limits and Means to Extend ELM suppression for future | Kolemen | PPPL | Yes | No | No |
41 | Optimize Co-ECCD For 2/1 NTM Preemption in the Low Torque ITER Baseline | Control and Understand Core Stability in low Torque ITER Baseline | La Haye | Retired from GA | Yes | Yes | No |
39 | Near Axis Co-ECCD for ST Control in Low Torque IBS | Control and Understand Core Stability in low Torque ITER Baseline | La Haye | Retired from GA | Yes | Yes | No |
47 | Optimize Pulsed Co-ECCD "Catch & Subdue" For 2/1 NTM Stabilization in the Low Torque ITER Baseline | Control and Understand Core Stability in low Torque ITER Baseline | La Haye | Retired from GA | Yes | Yes | No |
57 | n=1 I-Coil Applied Field for Tearing Mode Probing Using Super-Spa | Control and Understand Core Stability in low Torque ITER Baseline | La Haye | Retired from GA | Yes | Yes | No |
55 | Optimize Co-ECCD for 3/2 NTM Preemption in the Low Torque ITER Baseline | Control and Understand Core Stability in low Torque ITER Baseline | La Haye | Retired from GA | Yes | Yes | No |
28 | Turbulence and transport in negative triangularity discharges at high beta_n | BPP - turbulence and transport | Austin | U of Texas, Austin | Yes | No | No |
75 | Impact deuterium molecular emission on the radiation shortfall | Address Critical Detachment Physics Models | Groth | Aalto U | Yes | No | No |
243 | Validation of SOLPS-ITER modeling of heat flux width | IBM: Core-edge integration | Meier | Zap Energy Inc. | Yes | No | No |
250 | Modeling of the effect of detachment on heat flux width using SOLPS-ITER with drifts | DO: Divertor optimization | Meier | Zap Energy Inc. | No | No | No |
125 | Wider negative shear for the confinement improvement at high Te/Ti | BPP - turbulence and transport | Yoshida | QST | No | No | No |
321 | Greenwald limit: is radiative island the cause? | Torkil Jensen Award | Kolemen | PPPL | No | No | No |
195 | Increase beta in ALfven Eigenmode mitigated high performance target discharges | D&C - steady state (apart from core-edge SS thrust) | Kramer | PPPL | No | No | No |
298 | Do Surface Patterns on the Tiles Matter? | AMV: Erosion/migration | Lasa Esquisabel | U of Tennessee, Knoxville | No | No | No |
285 | NTM Stabilization for IBS | Control and Understand Core Stability in low Torque ITER Baseline | Kolemen | PPPL | No | Yes | Yes |
256 | Detachment Control with Nitrogen (or Carbon) | Address Critical Detachment Physics Models | Kolemen | PPPL | No | No | No |
87 | Preemptive EMTI Feedback for NTM Locking Avoidance and Recovery of H-mode edge and High Confinement | Control and Understand Core Stability in low Torque ITER Baseline | Okabayashi | PPPL | No | No | No |
88 | Pre-emptive EMTI feedback-based Multi-mode (3/2 &2/1) Coupling De-phasing and Disruption Avoidance | Control and Understand Core Stability in low Torque ITER Baseline | Okabayashi | PPPL | No | No | No |
155 | Enhanced pedestal H-mode through low-Z impurity injection | PE - Pedestal/SOL physics and Pedestal optimization | Bortolon | PPPL | No | No | No |
3 | Current control VALEN based RWM feedback development | D&C - control (apart from core stability in low torque ITER thrust) | Clement | PPPL | No | No | No |
14 | Characterization of the quasi-coherent fluctuations between ELMs | PE - Pedestal/SOL physics and Pedestal optimization | Diallo | PPPL | No | No | No |
85 | Effect of the post-TQ density on runaway beam mitigation with MGI and SPI | Disruption Mitigation Physics | Fil | PPPL | No | No | No |
86 | ECCD-induced magnetic islands and impact on plasma rotation | Control and Understand Core Stability in low Torque ITER Baseline | Fil | PPPL | No | No | No |
253 | Control of toroidal rotation with NBI and NTV optimization | Develop Basis to Predict and Control Rotation in ITER | Fil | PPPL | No | No | No |
254 | Control of toroidal rotation with NBI and NTV optimization | D&C - control (apart from core stability in low torque ITER thrust) | Fil | PPPL | No | No | No |
255 | Continuous high pressure pedestal with Lithium | PE - Pedestal/SOL physics and Pedestal optimization | Fil | PPPL | No | No | No |
112 | Test Dependence of Core Confinement on the RMP Amplitude in ELM Suppressed Plasmas | BPP - turbulence and transport | Cui | PPPL | No | No | No |
207 | Clarify snowflake divertor physics | DO: Divertor optimization | Soukhanovskii | LLNL | No | No | No |
208 | Snowflake SAS divertor | Understand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL Dynamics | Soukhanovskii | LLNL | No | No | No |
258 | Collisionality dependence of the edge differential toroidal rotation between carbon and deuterium | Develop Basis to Predict and Control Rotation in ITER | Haskey | PPPL | No | No | No |
237 | D+ fueling due to cold neutral D in the pedestal at the outboard midplane using main ion CER | Understand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL Dynamics | Haskey | PPPL | No | No | No |
315 | Measurements of intrinsic torque using main ion rotation measurements | Develop Basis to Predict and Control Rotation in ITER | Haskey | PPPL | No | No | No |
307 | Optimization of n=1 RMP fields for ELM suppression | Understand Limits and Means to Extend ELM suppression for future | Park | PPPL | No | No | No |
181 | Demonstration of Divertor SPRED | Address Critical Detachment Physics Models | McLean | LLNL | No | No | No |
187 | Systematic detachment characterization in high triangularity, high performance plasmas | Address Critical Detachment Physics Models | McLean | LLNL | No | No | No |
38 | Learn how to produce qmin>2 with large rhoqmin for minimal impact of AEs using dynamic ECH and VNBI | D&C - steady state (apart from core-edge SS thrust) | Holcomb | LLNL | No | No | No |
16 | Use variable NBI voltage in high qmin scenarios to reduce AE/EPM-induced EP transport | D&C - steady state (apart from core-edge SS thrust) | Holcomb | LLNL | No | No | No |
35 | Learn how to produce qmin>2 with only positive shear for minimal impact of AEs | D&C - steady state (apart from core-edge SS thrust) | Holcomb | LLNL | No | No | No |
1 | Welcome to 2017 DIII-D ROF | General Physics | Fenstermacher | LLNL | No | No | No |
264 | Unique Code Validation through Comparison of High and Low-field-side Turbulence Measurements | BPP - turbulence and transport | Sung | KAIST | No | No | No |
330 | Control of high-Z material erosion by biasing in H mode plasma | AMV: Erosion/migration | Ding | ASIPP | No | No | No |
109 | Control of edge pedestal to extend duration and performance of high betaP scenario | Scenarios and Transport | Qian | ASIPP | No | No | No |
311 | Runaway mitigation with solid pellets | Disruption Mitigation Physics | Lehnen | ITER Organization | No | Yes | Yes |
312 | SPI with varying target plasma parameters | Disruption Mitigation Physics | Lehnen | ITER Organization | No | No | Yes |
8 | ITER Baseline ELM Suppression at Low Torque | D&C - inductive (apart from core stability in low torque ITER thrust) | Luce | ITER Organization | No | No | Yes |
9 | Probing stiffness with constant Ti/Te | BPP - turbulence and transport | Luce | ITER Organization | No | No | No |
10 | Comparison Plasmas in Deuterium to Helium Campaign Plasmas | PE - Pedestal/SOL physics and Pedestal optimization | Luce | ITER Organization | No | Yes | Yes |
11 | Operation and performance at low P/P_LH in the ITER baseline scenario | D&C - inductive (apart from core stability in low torque ITER thrust) | Luce | ITER Organization | No | Yes | No |
12 | Complete q95 optimization experiment | D&C - inductive (apart from core stability in low torque ITER thrust) | Luce | ITER Organization | No | No | No |
13 | Effect of closure location relative to x point | Understand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL Dynamics | Luce | ITER Organization | No | No | No |
293 | Test of pedestal current role in low torque ITER baseline plasmas | Control and Understand Core Stability in low Torque ITER Baseline | Luce | ITER Organization | No | Yes | No |
294 | Development of ITER-relevant rampdown scenarios | D&C - control (apart from core stability in low torque ITER thrust) | Luce | ITER Organization | No | Yes | No |
78 | High opacity SOL effect on pedestal | Understand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL Dynamics | Mordijck | The college of William and Mary | No | Yes | Yes |
74 | Role of divertor geometry on confinement | Understand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL Dynamics | Mordijck | The college of William and Mary | No | No | No |
193 | Probing X-point and inboard SOL plasma for fluctuations | Address Critical Detachment Physics Models | McLean | LLNL | No | No | No |
179 | ELM suppression in AUG-line shape with n=2 | Understand Limits and Means to Extend ELM suppression for future | Kirk | CCFE | No | Yes | No |
163 | obtain minimum core density with detached sas divertor | Understand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL Dynamics | Watkins | Sandia National Lab | No | No | No |
147 | Measure sheath power transmission factor in sas diverter | Understand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL Dynamics | Watkins | Sandia National Lab | No | No | No |
241 | Fuel Ion Mass Scaling of Transport | BPP - turbulence and transport | McKee | U of Wisconsin | No | No | No |
103 | Understand detachment access during RMP ELM suppression | Understand Limits and Means to Extend ELM suppression for future | Schmitz | U of Wisconsin | No | No | No |
101 | Understand role of plasma shape on ELM suppression | Understand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL Dynamics | Schmitz | U of Wisconsin | No | No | No |
7 | Model-Predictive Control of Magnetic/Kinetic Profiles using fast data-driven models and observers | D&C - control (apart from core stability in low torque ITER thrust) | Moreau | Cadarache | No | No | No |
239 | Intrinsic torque in ECH dominated plasma --- do we find counter-current intrinsic torque | Develop Basis to Predict and Control Rotation in ITER | Tala | VTT Technical Research Centre | No | Yes | No |
252 | Experimental NTV torque profiles in 3D fields | Develop Basis to Predict and Control Rotation in ITER | Salmi | VTT Technical Research Centre | No | No | No |
329 | Use of thin poloidal gaps to inhibit surface migration of PFC material | AMV: Erosion/migration | Stangeby | U of Toronto | No | No | No |
148 | Study the role of magnetic and ñ fluctuations in saturating pedestal gradients during type-I ELMs | PE - Pedestal/SOL physics and Pedestal optimization | Kumar Barada | UCLA | No | No | No |
209 | Study effects of SOL flows on QH-mode access | Understand Limits and Means to Extend ELM suppression for future | King | Tech-X Corporation | No | No | No |
106 | Fast-ion transport by NTMs | BPP - Energetic Particle Physics | Heidbrink | UC, Irvine | No | No | No |
108 | Fast-ion transport by NTMs in hybrid plasmas | Integrated Core-Edge Steady State Solution | Heidbrink | UC, Irvine | No | No | No |
226 | Does microturbulence control mode chirping? | BPP - Energetic Particle Physics | Heidbrink | UC, Irvine | No | Yes | No |
227 | Use resonances with 3D fields to alter the distribution function | BPP - Energetic Particle Physics | Heidbrink | UC, Irvine | No | No | No |
212 | AE critical gradient study with different modulated beams | BPP - Energetic Particle Physics | Heidbrink | UC, Irvine | No | No | No |
213 | ICE produced by beam ions in the scrapeoff layer | BPP - Energetic Particle Physics | Heidbrink | UC, Irvine | No | Yes | No |
76 | Return of ELMs during RMP and low torque operation | Understand Limits and Means to Extend ELM suppression for future | Rhodes | UCLA | No | No | No |
164 | Differentiate L-mode turbulence regimes preceding the L-H transition | BPP - L-H transition | Schmitz | UCLA | No | No | No |
228 | Establishing an experimental cyclone base case scenario for the LH transition | BPP - L-H transition | Marinoni | UCSD | No | No | No |
262 | Testing the effect of multi-scale fluctuations on steady-state profiles in IBS scenarios | BPP - turbulence and transport | Marinoni | UCSD | No | No | No |
296 | Establishing H-mode at negative triangularity | Torkil Jensen Award | Marinoni | UCSD | No | No | No |
314 | Improved core confinement of high performance steady state plasmas due to ITG turbulence dilution | Integrated Core-Edge Steady State Solution | Marinoni | UCSD | No | No | No |
300 | Studies of Arcing on Tungsten and Molybdenum PFC Surfaces | AMV: Erosion/migration | Rudakov | UCSD | No | No | No |
320 | Effect on SEE on Langmuir probe measurements in the SOL | PE - Pedestal/SOL physics and Pedestal optimization | Rudakov | UCSD | No | No | No |
322 | Dust re-mobilization studies using DiMES | AMV: Erosion/migration | Rudakov | UCSD | No | No | No |
29 | Runaway plateau impurity assimilation | Disruption Mitigation Physics | Hollmann | UCSD | No | No | Yes |
30 | Vary runaway electron plateau wall strike phase | Disruption Mitigation Physics | Hollmann | UCSD | No | No | No |
62 | Gather evidence for Kinetic effects in SOL and Divertor | DO: Divertor optimization | Boedo | UCSD | No | No | No |
63 | Intrinsic rotation scaling with collisionality, ion temperature and geometry | Develop Basis to Predict and Control Rotation in ITER | Boedo | UCSD | No | No | No |
56 | Divertor turbulence and detachment | Address Critical Detachment Physics Models | Boedo | UCSD | No | No | No |
80 | ExB and parallel flows in attached and detached divertor | Address Critical Detachment Physics Models | Boedo | UCSD | No | No | No |
81 | Test intrinsic flow theories and edge turbulence characteristics of negtative triangularity plasmas | BPP - turbulence and transport | Boedo | UCSD | No | No | No |
83 | Turbulence link between detaching divertor and pedestal characteristics | Understand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL Dynamics | Boedo | UCSD | No | No | No |
107 | Test radial electric field formation from ion loss | Develop Basis to Predict and Control Rotation in ITER | Boedo | UCSD | No | No | No |
197 | Control rotation via geometry | Develop Basis to Predict and Control Rotation in ITER | Boedo | UCSD | No | No | No |
198 | Test unconstrained models of L-H transition | BPP - L-H transition | Boedo | UCSD | No | No | No |
233 | Joint SPI experiment with JET | Disruption Mitigation Physics | Greenfield | ORNL | No | No | Yes |
127 | Advanced Divertor Control Development | D&C - control (apart from core stability in low torque ITER thrust) | Vail | Princeton U | No | No | No |
129 | Upper and Double-Null Snowflake Development | D&C - control (apart from core stability in low torque ITER thrust) | Vail | Princeton U | No | No | No |
130 | Advanced Divertor Detachment Studies | Understand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL Dynamics | Vail | Princeton U | No | No | No |
131 | Effect of Advanced Divertor Magnetic Geometry on Ideal MHD Stability Limits | Understand Limits and Means to Extend ELM suppression for future | Vail | Princeton U | No | No | No |
301 | Develop MIMO algorithm for detachment and radiation profile control | D&C - control (apart from core stability in low torque ITER thrust) | Vail | Princeton U | No | No | No |
302 | Characterization of detachment with MIMO detachment and radiation profile control | DO: Detachment & control (apart from Detachment Physics Thrust) | Vail | Princeton U | No | No | No |
303 | Adaptive EFC | D&C - control (apart from core stability in low torque ITER thrust) | Vail | Princeton U | No | No | No |
304 | Adaptive Error Field Correction | Control and Understand Core Stability in low Torque ITER Baseline | Vail | Princeton U | No | No | No |
305 | Adaptive ELM Control | D&C - control (apart from core stability in low torque ITER thrust) | Vail | Princeton U | No | No | No |
306 | Adaptive ELM Control | Understand Limits and Means to Extend ELM suppression for future | Vail | Princeton U | No | No | No |
289 | High-Performance, Steady-State Scenario Development Using Sustained, Broad Negative Shear q-Profiles | D&C - steady state (apart from core-edge SS thrust) | Murakami | Retired | No | No | No |
245 | Inward particle transport of HFS pellet fueled plasmas | BPP - turbulence and transport | Baylor | ORNL | No | No | Yes |
216 | HFS pellet fueling compatibility with ELM mitigation scenarios and particle transport | PE - RMP and pellets (non ELM suppression thrust) | Baylor | ORNL | No | No | No |
214 | Pellet ELM triggering as a function of injection location | PE - RMP and pellets (non ELM suppression thrust) | Baylor | ORNL | No | No | No |
332 | Detachment with varying leg length with re-directed DTS laser | Address Critical Detachment Physics Models | Canik | ORNL | No | No | No |
333 | Detachment physics at maximum heat flux | Address Critical Detachment Physics Models | Canik | ORNL | No | No | No |
156 | Pedestal optimization in stationary plasmas | PE - Pedestal/SOL physics and Pedestal optimization | Snyder | ORNL | No | No | No |
331 | Use of isotopic tracer elements to understand material migration properties | AMV: Erosion/migration | Unterberg | ORNL | No | No | No |
53 | 3D pedestal turbulence studies during ELM suppression with rotating n=2 I-coils | Understand Limits and Means to Extend ELM suppression for future | Wilcox | ORNL | No | No | No |
334 | Use deposition on 3D material structures to understand material migration on the divertor target | AMV: 3D effects | Hinson | ORNL | No | No | No |
32 | Asymmetry effects during SPI fast shutdown | Disruption Mitigation Physics | Shiraki | ORNL | No | No | No |
33 | Multiple shattered pellet injections for TQ/CQ mitigation | Disruption Mitigation Physics | Shiraki | ORNL | No | No | No |
34 | Ballistic transport and MHD mixing in SPI impurity assimilation | Disruption Mitigation Physics | Shiraki | ORNL | No | No | No |
36 | Alternative injection schemes for high-Z shattered pellets for dissipation of runaway electrons | Disruption Mitigation Physics | Shiraki | ORNL | No | No | No |
37 | Pellet ablation as a diagnostic for quiescent runaway electron growth | Disruption Mitigation Physics | Shiraki | ORNL | No | No | No |
183 | Transport and ELM suppression associated with the EHO in QH-mode | PE - QH mode (non ELM suppression thrust) | Wilks | Massachusetts Institute of Technology | No | No | No |
184 | Characterization of the radial electric field through ion orbit loss | PE - Pedestal/SOL physics and Pedestal optimization | Wilks | Massachusetts Institute of Technology | No | No | No |
192 | Effect of electron perpendicular flow variation for ELM suppression at reduced triangularity | Understand Limits and Means to Extend ELM suppression for future | Suttrop | Max-Planck Institute for Plasma Physics | No | Yes | No |
248 | Prompt conversion of a full current into sub-MeV RE current | Disruption Mitigation Physics | Aleynikov | Max-Planck Institute for Plasma Physics | No | Yes | No |
323 | Response of turbulence in magnetic island due to the heat pulse from modulation ECH | BPP - turbulence and transport | Ida | National Institute for Fusion Science, Japan | No | No | No |
51 | Identify physics mechanisms responsible for MHD-induced collapse of toroidal momentum | Develop Basis to Predict and Control Rotation in ITER | Tobias | Los Alamos National Laboratory | No | No | No |
52 | Recovery of favorable rotation profiles after MHD-induced rotation collapse | Develop Basis to Predict and Control Rotation in ITER | Tobias | Los Alamos National Laboratory | No | No | No |
42 | Role of EP transport in rotation of tearing-unstable plasmas | BPP - Energetic Particle Physics | Tobias | Los Alamos National Laboratory | No | No | No |
235 | Does the P-B model accurately predict the collisionality scaling of ELM mode number (k_theta)? | Understand Limits and Means to Extend ELM suppression for future | Tobias | Los Alamos National Laboratory | No | No | No |
236 | Does nonlinear impact of ExB shear dictate the radial extent of ELMs and prevalence of filaments? | Understand Limits and Means to Extend ELM suppression for future | Tobias | Los Alamos National Laboratory | No | No | No |
111 | Understand and reduce fishbone activity in hybrid plasmas | Integrated Core-Edge Steady State Solution | Thome | GA | No | No | No |
277 | Comparison of hybrids with open and closed divertor | Integrated Core-Edge Steady State Solution | Thome | GA | No | No | No |
310 | H-mode impurity transport dependence on beam fueling | BPP - turbulence and transport | Thome | GA | No | No | Yes |
257 | Density dependence of edge intrinsic rotation in USN L-mode. | Develop Basis to Predict and Control Rotation in ITER | Ashourvan | GA | No | No | No |
115 | Stationary RF-dominantly heated hybrid plasmas at low torque | D&C - inductive (apart from core stability in low torque ITER thrust) | Thome | GA | No | No | No |
116 | Low torque high Beta hybrid plasmas | Integrated Core-Edge Steady State Solution | Thome | GA | No | No | No |
117 | Pedestal optimization of hybrid plasmas | Integrated Core-Edge Steady State Solution | Thome | GA | No | No | No |
158 | Development of ECH TS-ECE Cross-Cal | General Physics | Brookman | GA | No | No | No |
110 | Feedback control of 2/1 locked mode phase and rotation with RMP | Control and Understand Core Stability in low Torque ITER Baseline | Choi | GA | No | No | No |
146 | Effect of closed divertor on pedestal formation and divertor detachment | Understand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL Dynamics | Moser | GA | No | No | No |
152 | Quantifying detachment advantage in SAS relative to open divertor | Understand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL Dynamics | Moser | GA | No | No | No |
67 | RT control of H-L transition by sudden shape change | D&C - control (apart from core stability in low torque ITER thrust) | Eldon | GA | No | No | No |
324 | Detachment control for SAS | D&C - control (apart from core stability in low torque ITER thrust) | Eldon | GA | No | No | No |
325 | Combined detachment and divertor radiation control | D&C - control (apart from core stability in low torque ITER thrust) | Eldon | GA | No | No | No |
337 | Detachment control in X-divertor | D&C - control (apart from core stability in low torque ITER thrust) | Eldon | GA | No | No | No |
200 | Scaling of NTV Torque with Applied 3D Field Amplitude and Spectrum | Develop Basis to Predict and Control Rotation in ITER | Grierson | GA | No | No | No |
199 | multi-scale turbuelnce validation | Scenarios and Transport | Staebler | GA | No | No | No |
190 | Probing the 2D flow evolution during the L/H transition | BPP - L-H transition | Staebler | GA | No | No | No |
328 | Interpretation of WII and WI emission profiles in terms of a W prompt re-deposition fraction | AMV: Erosion/migration | Abrams | GA | No | No | No |
335 | Deposition Probe Background and Pellet Injection Exposures | AMV: Erosion/migration | Donovan | U of Tennessee-Knoxville | No | No | No |
292 | Plasma Control with SuperSpas | D&C - control (apart from core stability in low torque ITER thrust) | Hyatt | GA | No | No | No |
313 | Collisionality scan for the minimum ExB shear to sustain EHO and avoid ELMs | Understand Limits and Means to Extend ELM suppression for future | Chen | GA | No | No | Yes |
295 | Control EP transport in high qmin steady-state plasmas using central ECH | Integrated Core-Edge Steady State Solution | Chen | GA | No | Yes | No |
308 | Collisionality scan for the minimum ExB shear to sustain EHO and avoid ELMs | PE - QH mode (non ELM suppression thrust) | Chen | GA | No | No | Yes |
309 | Investigation of broadband EHO and the â??wide-pedestal QHâ?? broadband MHD | PE - QH mode (non ELM suppression thrust) | Chen | GA | No | No | No |
278 | Wall deposition of refracted ECH power | BPP - Heating & Current Drive Physicse | Chen | GA | No | No | No |
318 | Advanced Inductive with QH Mode Edge For Path to Q=10 | D&C - inductive (apart from core stability in low torque ITER thrust) | Buttery | GA | No | Yes | Yes |
77 | Is the Coriolis Pinch the Key to Intrinsic Rotation | Develop Basis to Predict and Control Rotation in ITER | deGrassie | GA | No | No | No |
27 | Effect of Fast Ion Loss on L-H Transition | BPP - L-H transition | deGrassie | GA | No | No | No |
31 | Negative Triangularity LSN Scenario | Integrated Core-Edge Steady State Solution | deGrassie | GA | No | No | No |
5 | Transformative Torque-less ITER similarity discharges in DIII-D with the present gyrotron set. | Control and Understand Core Stability in low Torque ITER Baseline | deGrassie | GA | No | No | No |
6 | ECCD and Core Intrinsic Rotation | Develop Basis to Predict and Control Rotation in ITER | deGrassie | GA | No | No | No |
279 | Negative Triangularity LSN Scenario | Torkil Jensen Award | deGrassie | GA | No | No | No |
251 | Joint KSTAR/DIII-D n=2 Transport and Stability Experiment | Understand Limits and Means to Extend ELM suppression for future | Evans | GA | No | No | No |
165 | Pedestal detachment with n = 4 and 6 RMP fields | Torkil Jensen Award | Evans | GA | No | No | No |
105 | Developing new RMP physics insights based on rotating n=3 perturbation fields | PE - RMP and pellets (non ELM suppression thrust) | Evans | GA | No | Yes | Yes |
188 | Test of Turbulence Spreading Using Turbulence Propagation | BPP - turbulence and transport | Petty | GA | No | No | No |
186 | Electron Critical Gradient in H-mode | BPP - turbulence and transport | Petty | GA | No | No | No |
191 | Hybrids with co-NBI QH-mode edge | Integrated Core-Edge Steady State Solution | Petty | GA | No | No | No |
286 | Off-Axis ECCD in Steady-State Hybrids | Integrated Core-Edge Steady State Solution | Petty | GA | No | No | No |
336 | Test of improved 2/1 stability with reduced pedestal height | Control and Understand Core Stability in low Torque ITER Baseline | Petty | GA | No | No | No |
287 | Plasma Response in DN versus SN | Understand Limits and Means to Extend ELM suppression for future | Turnbull | GA | No | No | No |
222 | AE Drive Due to Ions Lost on Their First Orbit | BPP - Energetic Particle Physics | Van Zeeland | GA | No | No | No |
220 | AEs in Negative Triangularity Plasmas | BPP - Energetic Particle Physics | Van Zeeland | GA | No | No | No |
244 | Suppression of plasma current after plasma initialization | D&C - control (apart from core stability in low torque ITER thrust) | Walker | GA | No | No | Yes |
61 | Long pulse, high pedestal pressure, ELM free discharges with Li injection | Scenarios and Transport | Osborne | GA | No | No | No |
202 | Effect of divertor geometry, closure, and SOL plasma on fueling and impurity effects on pedestal | Understand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL Dynamics | Osborne | GA | No | Yes | No |
159 | Loss of Effective Heat Flux Reduction by Puff-and-Pump Under High Power AT Conditions | Understand the Impact of Geometry and Fueling on Divertor, Pedestal and SOL Dynamics | Petrie | GA | No | No | No |
160 | ITER Baseline Scenario in a Radiating Divertor Environment with near-Zero Applied Torque | Control and Understand Core Stability in low Torque ITER Baseline | Petrie | GA | No | No | No |
162 | Density Control and Active Middle-Z Impurity Removal from Double-null H-mode Plasmas | Integrated Core-Edge Steady State Solution | Petrie | GA | No | No | No |
259 | Midplane Impurity Density Asymmetry | BPP - turbulence and transport | Chrystal | GA | No | No | No |
288 | All Carbon Plasma Density Measurement | PE - RMP and pellets (non ELM suppression thrust) | Chrystal | GA | No | No | No |
290 | Improve radial control during rampup | D&C - control (apart from core stability in low torque ITER thrust) | Eidietis | GA | No | No | No |
291 | Default ONFR on all D3D shots | D&C - control (apart from core stability in low torque ITER thrust) | Eidietis | GA | No | No | No |
280 | Placeholder: Dedicated camrea time to get SPI solid fraction estimate | Disruption Mitigation Physics | Eidietis | GA | No | No | No |
272 | D3D/JET comparison of pure Ne SPI size scaling | Disruption Mitigation Physics | Eidietis | GA | No | No | Yes |
282 | Placeholder: Spatially resolved measurement of RE pleateau f(E) with GRI | Disruption Mitigation Physics | Eidietis | GA | No | No | No |
210 | Improving impurity injection into RE by avoiding high energy shfited RE orbits | Disruption Mitigation Physics | Eidietis | GA | No | No | No |
211 | Effect of global MHD stability on RE plateau dissipation in D3D & JET | Disruption Mitigation Physics | Eidietis | GA | No | No | Yes |
70 | Optimized lower torque hybrids | D&C - steady state (apart from core-edge SS thrust) | Turco | Columbia U | No | No | No |
71 | Study and eliminate fishbones, high frequency modes and ELMs in high betaN hybrids | Integrated Core-Edge Steady State Solution | Turco | Columbia U | No | No | No |
161 | Finish exploring the higher q95 IBS alternative, with RMP ELM suppression | Control and Understand Core Stability in low Torque ITER Baseline | Turco | Columbia U | No | No | No |
217 | Develop a no-ECH high betaN hybrid for radiative divertor studies | Integrated Core-Edge Steady State Solution | Turco | Columbia U | No | No | No |
265 | Increase the stability limits of high-betaN hybrids by optimising the plasma shape | Integrated Core-Edge Steady State Solution | Turco | Columbia U | No | No | No |
17 | Scaling of intrinsic rotation in ECH H-mode | Develop Basis to Predict and Control Rotation in ITER | Chrystal | GA | No | No | No |
18 | Charge Exchange Cross Section Study with Co/counter beams | General Physics | Chrystal | GA | No | No | No |
246 | Develop low q95 post-disruption runaway electron scenario | Disruption Mitigation Physics | Paz-Soldan | Columbia U | No | Yes | No |
281 | Develop counter-rotating analog to co-rotating ITER baseline plasma for stability study | Control and Understand Core Stability in low Torque ITER Baseline | Paz-Soldan | Columbia U | No | No | No |
20 | Quiescent runaway electron studies with refurbished gamma-ray-imaging detectors | Disruption Mitigation Physics | Paz-Soldan | Columbia U | No | Yes | No |
21 | Revisit rotating n=2 fields at higher amplitude for 3D structure diagnosis during ELM suppression | Understand Limits and Means to Extend ELM suppression for future | Paz-Soldan | Columbia U | No | No | No |
22 | Effect of shaping on pedestal and 3D response for ELM control: aspect ratio, triangularity, X-point | Understand Limits and Means to Extend ELM suppression for future | Paz-Soldan | Columbia U | No | No | No |
23 | High current phase flips during rotation scans in RMP-ELM suppression in ITER baseline | Understand Limits and Means to Extend ELM suppression for future | Paz-Soldan | Columbia U | No | No | No |
24 | Apply n=1,2,3 error field control to low torque IBS plasma | Control and Understand Core Stability in low Torque ITER Baseline | Paz-Soldan | Columbia U | No | No | No |
25 | Create different yet non-dimensionally similar low torque ITER baseline plasmas | Control and Understand Core Stability in low Torque ITER Baseline | Paz-Soldan | Columbia U | No | No | No |
26 | Non-resonant braking for tearing mode onset studies | Control and Understand Core Stability in low Torque ITER Baseline | Paz-Soldan | Columbia U | No | No | No |
267 | Mixed spectrum of n=2 and 3 RMP for ELM suppression | Understand Limits and Means to Extend ELM suppression for future | Sun | ASIPP | No | No | No |
268 | Rotating n=2 RMP for ELM suppression | Understand Limits and Means to Extend ELM suppression for future | Sun | ASIPP | No | No | No |
297 | Understanding I-mode access and I-mode physics through identity experiments DIII-D / ASDEX Upgrade | PE - Pedestal/SOL physics and Pedestal optimization | Happel | Max-Planck-Institut für Plasmaphysik | No | Yes | No |
319 | Skin Current Tokamak at higher Current | Scenarios and Transport | Staebler | GA | No | No | No |
168 | H-mode detachment data in deuterium plasma to compliment existing helium detachment data | Address Critical Detachment Physics Models | Briesemeister | ORNL | No | No | No |
169 | Feedback control of 2/1 locked mode phase and rotation with RMP | Control and Understand Core Stability in low Torque ITER Baseline | Choi | Columbia U | No | No | No |
173 | Effect of intrinsic and applied MP on error field tolerance in low torque high beta plasmas | Control and Stability | Wang | ASIPP | No | No | No |
174 | Mixed spectrum of n=2 and 3 RMP for ELM suppression | Boundary | Sun | ASIPP | No | No | No |
175 | Rotating n=2 RMP for ELM suppression | Boundary | Sun | ASIPP | No | No | No |
201 | DiMES tests of novel Mo PMI materials | AMV: Erosion/migration | Thomas | GA | No | No | No |
215 | Experimental test of two-threshold-field theory of RE generation | Disruption Mitigation Physics | Lvovskiy | ORAU | No | No | No |
223 | AEs in Negative Triangularity Plasmas | BPP - Energetic Particle Physics | Van Zeeland | GA | No | No | No |