|
ID |
Title |
Research Area |
Name |
Affiliation |
Time Req'ed |
ITPA Joint Exp |
ITER IO Urgent Research Task |
| 1 | Welcome to 2017 DIII-D ROF | General Physics | Fenstermacher | LLNL | 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 |
| 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 |
| 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 |
| 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 |
| 14 | Characterization of the quasi-coherent fluctuations between ELMs | PE - Pedestal/SOL physics and Pedestal optimization | Diallo | PPPL | 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 |
| 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 |
| 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 |
| 27 | Effect of Fast Ion Loss on L-H Transition | BPP - L-H transition | deGrassie | GA | 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 |
| 31 | Negative Triangularity LSN Scenario | Integrated Core-Edge Steady State Solution | deGrassie | GA | 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 |
| 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 |
| 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 |
| 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 |
| 42 | Role of EP transport in rotation of tearing-unstable plasmas | BPP - Energetic Particle Physics | Tobias | Los Alamos National Laboratory | 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 |
| 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 |
| 56 | Divertor turbulence and detachment | Address Critical Detachment Physics Models | Boedo | UCSD | No | No | No |
| 61 | Long pulse, high pedestal pressure, ELM free discharges with Li injection | Scenarios and Transport | Osborne | GA | 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 |
| 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 |
| 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 |
| 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 |
| 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 |
| 77 | Is the Coriolis Pinch the Key to Intrinsic Rotation | Develop Basis to Predict and Control Rotation in ITER | deGrassie | GA | No | No | 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 |
| 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 |
| 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 |
| 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 |
| 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 |
| 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 |
| 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 |
| 106 | Fast-ion transport by NTMs | BPP - Energetic Particle Physics | Heidbrink | UC, Irvine | 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 |
| 108 | Fast-ion transport by NTMs in hybrid plasmas | Integrated Core-Edge Steady State Solution | Heidbrink | UC, Irvine | 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 |
| 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 |
| 111 | Understand and reduce fishbone activity in hybrid plasmas | Integrated Core-Edge Steady State Solution | Thome | GA | 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 |
| 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 |
| 125 | Wider negative shear for the confinement improvement at high Te/Ti | BPP - turbulence and transport | Yoshida | QST | No | No | No |
| 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 |
| 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 |
| 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 |
| 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 |
| 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 |
| 155 | Enhanced pedestal H-mode through low-Z impurity injection | PE - Pedestal/SOL physics and Pedestal optimization | Bortolon | PPPL | No | No | No |
| 156 | Pedestal optimization in stationary plasmas | PE - Pedestal/SOL physics and Pedestal optimization | Snyder | ORNL | No | No | No |
| 158 | Development of ECH TS-ECE Cross-Cal | General Physics | Brookman | GA | No | No | 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 |
| 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 |
| 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 |
| 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 |
| 164 | Differentiate L-mode turbulence regimes preceding the L-H transition | BPP - L-H transition | Schmitz | UCLA | No | No | No |
| 165 | Pedestal detachment with n = 4 and 6 RMP fields | Torkil Jensen Award | Evans | 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 |
| 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 |
| 181 | Demonstration of Divertor SPRED | Address Critical Detachment Physics Models | McLean | LLNL | 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 |
| 186 | Electron Critical Gradient in H-mode | BPP - turbulence and transport | Petty | GA | No | No | No |
| 187 | Systematic detachment characterization in high triangularity, high performance plasmas | Address Critical Detachment Physics Models | McLean | LLNL | No | No | No |
| 188 | Test of Turbulence Spreading Using Turbulence Propagation | BPP - turbulence and transport | Petty | GA | No | No | No |
| 190 | Probing the 2D flow evolution during the L/H transition | BPP - L-H transition | Staebler | GA | No | No | No |
| 191 | Hybrids with co-NBI QH-mode edge | Integrated Core-Edge Steady State Solution | Petty | GA | 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 |
| 193 | Probing X-point and inboard SOL plasma for fluctuations | Address Critical Detachment Physics Models | McLean | LLNL | 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 |
| 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 |
| 199 | multi-scale turbuelnce validation | Scenarios and Transport | Staebler | 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 |
| 201 | DiMES tests of novel Mo PMI materials | AMV: Erosion/migration | Thomas | 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 |
| 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 |
| 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 |
| 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 |
| 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 |
| 214 | Pellet ELM triggering as a function of injection location | PE - RMP and pellets (non ELM suppression thrust) | Baylor | ORNL | No | No | No |
| 215 | Experimental test of two-threshold-field theory of RE generation | Disruption Mitigation Physics | Lvovskiy | ORAU | No | No | No |
| 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 |
| 217 | Develop a no-ECH high betaN hybrid for radiative divertor studies | Integrated Core-Edge Steady State Solution | Turco | Columbia U | No | No | No |
| 220 | AEs in Negative Triangularity Plasmas | BPP - Energetic Particle Physics | Van Zeeland | 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 |
| 223 | AEs in Negative Triangularity Plasmas | BPP - Energetic Particle Physics | Van Zeeland | GA | 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 |
| 228 | Establishing an experimental cyclone base case scenario for the LH transition | BPP - L-H transition | Marinoni | UCSD | No | No | No |
| 233 | Joint SPI experiment with JET | Disruption Mitigation Physics | Greenfield | ORNL | No | No | Yes |
| 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 |
| 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 |
| 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 |
| 241 | Fuel Ion Mass Scaling of Transport | BPP - turbulence and transport | McKee | U of Wisconsin | 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 |
| 245 | Inward particle transport of HFS pellet fueled plasmas | BPP - turbulence and transport | Baylor | ORNL | No | No | Yes |
| 246 | Develop low q95 post-disruption runaway electron scenario | Disruption Mitigation Physics | Paz-Soldan | Columbia U | 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 |
| 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 |
| 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 |
| 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 |
| 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 |
| 256 | Detachment Control with Nitrogen (or Carbon) | Address Critical Detachment Physics Models | Kolemen | PPPL | No | No | No |
| 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 |
| 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 |
| 259 | Midplane Impurity Density Asymmetry | BPP - turbulence and transport | Chrystal | GA | 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 |
| 264 | Unique Code Validation through Comparison of High and Low-field-side Turbulence Measurements | BPP - turbulence and transport | Sung | KAIST | 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 |
| 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 |
| 272 | D3D/JET comparison of pure Ne SPI size scaling | Disruption Mitigation Physics | Eidietis | GA | No | No | Yes |
| 277 | Comparison of hybrids with open and closed divertor | Integrated Core-Edge Steady State Solution | Thome | GA | No | No | No |
| 278 | Wall deposition of refracted ECH power | BPP - Heating & Current Drive Physicse | Chen | GA | No | No | No |
| 279 | Negative Triangularity LSN Scenario | Torkil Jensen Award | deGrassie | GA | No | No | No |
| 280 | Placeholder: Dedicated camrea time to get SPI solid fraction estimate | Disruption Mitigation Physics | Eidietis | GA | No | No | 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 |
| 282 | Placeholder: Spatially resolved measurement of RE pleateau f(E) with GRI | Disruption Mitigation Physics | Eidietis | GA | No | No | No |
| 285 | NTM Stabilization for IBS | Control and Understand Core Stability in low Torque ITER Baseline | Kolemen | PPPL | No | Yes | Yes |
| 286 | Off-Axis ECCD in Steady-State Hybrids | Integrated Core-Edge Steady State Solution | 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 |
| 288 | All Carbon Plasma Density Measurement | PE - RMP and pellets (non ELM suppression thrust) | Chrystal | GA | 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 |
| 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 |
| 292 | Plasma Control with SuperSpas | D&C - control (apart from core stability in low torque ITER thrust) | Hyatt | GA | 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 |
| 295 | Control EP transport in high qmin steady-state plasmas using central ECH | Integrated Core-Edge Steady State Solution | Chen | GA | No | Yes | No |
| 296 | Establishing H-mode at negative triangularity | Torkil Jensen Award | Marinoni | UCSD | 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 |
| 298 | Do Surface Patterns on the Tiles Matter? | AMV: Erosion/migration | Lasa Esquisabel | U of Tennessee, Knoxville | No | No | No |
| 300 | Studies of Arcing on Tungsten and Molybdenum PFC Surfaces | AMV: Erosion/migration | Rudakov | UCSD | 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 |
| 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 |
| 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 |
| 310 | H-mode impurity transport dependence on beam fueling | BPP - turbulence and transport | Thome | GA | No | No | Yes |
| 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 |
| 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 |
| 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 |
| 315 | Measurements of intrinsic torque using main ion rotation measurements | Develop Basis to Predict and Control Rotation in ITER | Haskey | PPPL | 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 |
| 319 | Skin Current Tokamak at higher Current | Scenarios and Transport | Staebler | GA | 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 |
| 321 | Greenwald limit: is radiative island the cause? | Torkil Jensen Award | Kolemen | PPPL | No | No | No |
| 322 | Dust re-mobilization studies using DiMES | AMV: Erosion/migration | Rudakov | UCSD | No | No | 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 |
| 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 |
| 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 |
| 329 | Use of thin poloidal gaps to inhibit surface migration of PFC material | AMV: Erosion/migration | Stangeby | U of Toronto | No | No | No |
| 330 | Control of high-Z material erosion by biasing in H mode plasma | AMV: Erosion/migration | Ding | ASIPP | No | No | No |
| 331 | Use of isotopic tracer elements to understand material migration properties | AMV: Erosion/migration | Unterberg | 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 |
| 334 | Use deposition on 3D material structures to understand material migration on the divertor target | AMV: 3D effects | Hinson | ORNL | No | No | No |
| 335 | Deposition Probe Background and Pellet Injection Exposures | AMV: Erosion/migration | Donovan | U of Tennessee-Knoxville | 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 |
| 337 | Detachment control in X-divertor | D&C - control (apart from core stability in low torque ITER thrust) | Eldon | GA | No | No | No |