DIII-D RESEARCH OPPORTUNITIES FORUM FOR THE 2013 EXPERIMENTAL CAMPAIGN
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| ID | Title | Research Area | Name | Affiliation |
Time Req'ed |
ITPA Joint Exp |
ITER IO Urgent Research Task |
| 1 details | C vs I Coil NTV | Plasma Rotation | GA | No | No | No | |
| 2 details | Hysteresis and Turbulence Spreading in the H-L Back Transition | L-H Transition | UCLA | No | No | No | |
| 3 details | The effect of LSN Shape on the q95 windows in RMP ELM Suppression | ELM Control | GA | No | No | Yes | |
| 4 details | Turbulence and Intrinsic Rotation | Plasma Rotation | GA | No | No | No | |
| 5 details | Measure Intrinsic Rotation Size scaling in DIII-D alone -II | Plasma Rotation | GA | No | No | No | |
| 6 details | Prompt torque and zonal flow damping | Plasma Rotation | GA | No | No | No | |
| 7 details | Investigate angular momentum diffusion and pinch using off-axis torque | Plasma Rotation | GA | No | No | No | |
| 8 details | Compare Mach probe and CER measurements of intrinsic rotation profile of main ions in helium plasma | Plasma Rotation | GA | No | No | No | |
| 9 details | Test of Neoclassical Toroidal Viscosity theory using modulated I-coil currents | Plasma Rotation | GA | No | No | No | |
| 10 details | Maintain low-rotation QH-mode with ECH only | Inductive Scenarios | GA | No | No | No | |
| 11 details | Investigate in-out density asymmetry at large toroidal rotation | Plasma Rotation | GA | No | No | No | |
| 12 details | Diagnostic spatial cross calibration using edge sweeps in QH-mode | Pedestal Structure | GA | No | No | No | |
| 13 details | Compare edge particle transport in ELMing H-mode and QH-mode with and without NRMF | Inductive Scenarios | GA | No | No | No | |
| 14 details | Control of toroidal mode number of EHO | Inductive Scenarios | GA | No | No | No | |
| 15 details | Edge rotation shear threshold for QH-mode access | Inductive Scenarios | GA | No | No | No | |
| 16 details | Further development of QH-mode with strong co-Ip NBI torque | Inductive Scenarios | GA | No | No | No | |
| 17 details | 3-D Fields and ECH Density Pumpout | Turbulence & Transport | GA | No | No | No | |
| 18 details | High Collisionless NBI Torque Drive for GAMs, aka the VH-mode path? | Turbulence & Transport | GA | No | No | No | |
| 19 details | Effect of n=1 applied and error fields on n=3 RMP ELM suppression | ELM Control | GA | No | No | No | |
| 20 details | L-H transition Trigger Physics/ Main Ion Momentum Balance | L-H Transition | UCLA | No | No | No | |
| 21 details | Magnitude of cross-field drifts in the Private Flux Region, divertor asymmetries and detachment | Divertor & SOL Physics | Aalto U | No | No | No | |
| 22 details | Assessment of main chamber carbon sources | Divertor & SOL Physics | Aalto U | No | No | No | |
| 23 details | RMP ELM Suppression at q95 above 4 | ELM Control | GA | No | No | No | |
| 25 details | Transport mechanisms induced by RMP | ELM Control | UCSD | No | No | Yes | |
| 26 details | Investigate the role of RS on inward momentum transport | Turbulence & Transport | UCSD | No | No | No | |
| 27 details | COupling between core and SOL parallel flow | Divertor & SOL Physics | UCSD | No | No | No | |
| 28 details | Role of profile evolution and energy transfer in L-H transition | L-H Transition | UCSD | No | No | No | |
| 29 details | Modulation of Bootstrap Current | ELM Control | GA | No | No | No | |
| 30 details | New Optimal Plasma Shape for AT Scenario? | Steady State Heating and Current Drive | GA | No | No | No | |
| 31 details | Test of Turbulence Spreading Using Turbulence Propagation | Turbulence & Transport | GA | No | No | No | |
| 32 details | High Beta Hybrids and Pressure Profile Broadening | Steady State Heating and Current Drive | GA | No | No | No | |
| 33 details | High Beta, Steady State Hybrids | Steady State Heating and Current Drive | GA | No | No | No | |
| 34 details | Electron Critical Gradient and Heat Pinch | Turbulence & Transport | GA | No | No | No | |
| 35 details | Non-Diffusive Heat Fluxes in the Edge "Shortfall" Region | Turbulence & Transport | GA | No | No | No | |
| 36 details | Natural ELM Pacing in High-Beta, Steady-State Plasmas | Steady State Heating and Current Drive | GA | No | No | No | |
| 38 details | Calibrated passive FIDA spectrum | Energetic Particles | UC, Irvine | No | No | No | |
| 39 details | Measure and understand energetic particle profiles in steady-state plasmas | Steady State Heating and Current Drive | UC, Irvine | No | No | No | |
| 40 details | MGI with applied n=1 RMP fields | Disruption Mitigation | Fiat Lux LLC | No | No | No | |
| 41 details | Investigation of the effects of the EHO toroidal mode number on the edge particle transport | Inductive Scenarios | PPPL | No | No | No | |
| 42 details | Compatibility of High Performance Plasmas With a Puff-and-Pump Radiating Divertor | Steady State Heating and Current Drive | GA | No | No | No | |
| 43 details | Density Control and Active Impurity Removal from Double-null H-mode Plasmas | Divertor & SOL Physics | GA | No | No | No | |
| 44 details | Can Nitrogen impurity Seeding Improve Radiating Divertor Performance? | Divertor & SOL Physics | GA | No | No | No | |
| 45 details | Differences in Impurity Accumulation Between Resonant and Non-resonant RMP Plasmas | ELM Control | GA | No | No | No | |
| 46 details | Does Added Baffling From Re-Configured Tiles on the Lower Divertor Shelf Facilitate Detachment? | Divertor & SOL Physics | GA | No | No | No | |
| 47 details | Quantifying the TBM torque, both in magnitude and radial location | Plasma Rotation | VTT Technical Research Centre | No | No | No | |
| 48 details | Dependence of momentum transport and intrinsic torque on rho* and beta | Plasma Rotation | VTT Technical Research Centre | No | Yes | No | |
| 49 details | Turbulent transport in detached divertor | Divertor & SOL Physics | UCSD | No | No | Yes | |
| 51 details | Study of chirping Alfvén eigenmodes in DIII-D | Energetic Particles | PPPL | No | Yes | No | |
| 52 details | Control of TAE/RSAE modes via external perturbations | Energetic Particles | PPPL | No | No | No | |
| 53 details | QH-mode with low torque start-up | Inductive Scenarios | GA | No | No | No | |
| 55 details | RMP Elm Suppression in DN Plasmas | ELM Control | ORNL | No | No | No | |
| 56 details | Sawtooth Control | Plasma Control | ORNL | No | No | No | |
| 59 details | Effect of Changing the Grad-B Drift Direction on Snowflake Divertor Behavior, Including Detachment | Divertor & SOL Physics | GA | No | No | No | |
| 60 details | Effective NTM control in low torque plasmas | Stability & Disruption Avoidance | GA | No | No | No | |
| 71 details | 4. ELM Characterization to Validate BOUT++ ELM Simulations | Pedestal Structure | LLNL | No | No | No | |
| 81 details | Active Particle Exhaust of H-mode Plasmas in the Snowflake-minus Divertor Configuration | Divertor & SOL Physics | GA | No | No | No | |
| 82 details | IR Imaging of I-coil Induced Fast Ion Losses | Energetic Particles | GA | No | Yes | No | |
| 86 details | Safety Factor Scaling of Turbulence and Transport in Hybrid Scenario Plasmas | Turbulence & Transport | U of Wisconsin | No | No | No | |
| 90 details | Carbon-13 in He Plasma erosion/deposition experiment to benchmark DIVIMP code being used by ITER | Plasma-material Interface | Commonwealth Fusion Systems | No | No | No | |
| 94 details | Turbulence Structure and Amplitude Variation with ExB Shear in H-mode Plasmas | Turbulence & Transport | U of Wisconsin | No | No | No | |
| 95 details | Experimental Validation of a Revised PCS Error Field Category | Plasma Control | Department of Energy | No | No | No | |
| 96 details | Effect of Error Field Control Currents on Strike Point Splitting | Stability & Disruption Avoidance | Department of Energy | No | No | No | |
| 115 details | QH-mode at low co-Ip torque using n=2 NRMF | Inductive Scenarios | GA | No | No | No | |
| 120 details | Optimizing non-resonant, nonaxisymmetric fields in QH-mode | Inductive Scenarios | GA | No | No | No | |
| 123 details | Bid farewell to locked modes - NTM-locking avoidance by feedback synchronization assisted with ECCD | Stability & Disruption Avoidance | PPPL | No | No | No | |
| 124 details | Electron Energy Transport during q0 control using modulated EC power | Inductive Scenarios | ORNL | No | No | No | |
| 125 details | Observation of non-linear interactions in fast-ion loss spectra | Energetic Particles | PPPL | No | No | No | |
| 128 details | Carbon-13 in He Plasma erosion/deposition experiment to benchmark DIVIMP code being used by ITER | Plasma-material Interface | Commonwealth Fusion Systems | No | No | No | |
| 130 details | Synergy between core-localized Alfven eigenmodes and edge localized TBM fields on fast ion losses. | Energetic Particles | PPPL | No | Yes | No | |
| 132 details | Dissipation & Control of RE from ITER-like LSN targets | Disruption Mitigation | GA | No | No | Yes | |
| 135 details | Measurement of RE diffusion to center post | Disruption Mitigation | UCSD | No | No | Yes | |
| 136 details | Disruption main chamber heat loads | Disruption Mitigation | UCSD | No | Yes | Yes | |
| 138 details | SSI target improvement by minimizing global low-n MHD activity in 1.5 | Steady State Heating and Current Drive | PPPL | No | No | No | | |
| 139 details | TQ radiation distribution from R-2 MGI | Disruption Mitigation | UCSD | No | No | Yes | |
| 140 details | q0 control with Counter-ECCD in ITER Baseline Discharges | Inductive Scenarios | Retired | No | No | No | |
| 141 details | Studies of RE final loss | Disruption Mitigation | UCSD | No | No | Yes | |
| 145 details | Explore RMP ELM suppression mechanism at moderate collisionality | ELM Control | UCSD | No | No | No | |
| 149 details | Measurement of ion temperatures in the divertor region of DIII-D using the DiMES platform | Divertor & SOL Physics | U of Tennessee, Knoxville | No | No | No | |
| 150 details | Sensitivity study of toroidally-asymmetric halo current to error field during VDE | Disruption Mitigation | PPPL | No | No | No | |
| 151 details | ITER SS Demo Discharge Documentations | Steady State Heating and Current Drive | Retired | No | No | No | |
| 152 details | Transport shortfall at high gyrobohm flux | Turbulence & Transport | GA | No | No | No | |
| 154 details | High frequency pellet ELM pacing | ELM Control | ORNL | No | Yes | Yes | |
| 155 details | Investigation of pellet induced ELM heat flux footprint variation with q95 | ELM Control | ORNL | No | No | Yes | |
| 157 details | Imaging of pellet induced ELM events from mulitple simultaneous views. | ELM Control | ORNL | No | No | Yes | |
| 158 details | Expand the high li, betaN >4 operating regime through instability avoidance and higher heating power | Steady State Heating and Current Drive | GA | No | No | No | |
| 160 details | Dependence of confinement and stability on toroidal rotation in high li discharges | Steady State Heating and Current Drive | GA | No | No | No | |
| 161 details | n=3 offset and ELM suppression with RMP | ELM Control | GA | No | No | Yes | |
| 162 details | 210RT MSE and low rotation, elevated q_min steady-state scenario discharges at high betaN | Steady State Heating and Current Drive | GA | No | No | No | |
| 164 details | Produce fNI = 1 discharges at q_min near 1.5 using off-axis injection and a model guided approach | Steady State Heating and Current Drive | GA | No | No | No | |
| 165 details | D2 + few % Ne shattered pellets for disruption mitigation | Disruption Mitigation | ORNL | No | No | Yes | |
| 166 details | Effect of q95 on SPI shutdown | Disruption Mitigation | ORNL | No | No | Yes | |
| 167 details | Control of radiation asymmetries by application of external field on SPI/MGI shutdown | Disruption Mitigation | ORNL | No | No | Yes | |
| 168 details | Influence of the delay time between multiple massive gas injections at different toroidal locations | Disruption Mitigation | ORNL | No | No | Yes | |
| 169 details | Runaway flattop mitigation by Neon shattered pellet injection | Disruption Mitigation | ORNL | No | No | Yes | |
| 170 details | Nature of Energy Released During H-L Back Transition | L-H Transition | GA | No | No | No | |
| 171 details | Test of the argon pellet injector | Disruption Mitigation | ORNL | No | No | Yes | |
| 172 details | High betaN with off-axis injection at reduced Bt (if 2011-level beam power is available) | Steady State Heating and Current Drive | GA | No | No | No | |
| 173 details | Confinement and fast ion diffusion in high betaN, steady-state scenario discharges | Steady State Heating and Current Drive | GA | No | No | No | |
| 174 details | Exploration of DEFC in the feedback stabilized plasma in low-q discharges | Stability & Disruption Avoidance | PPPL | No | No | No | |
| 175 details | Beta collapse avoidance in SSI discharges by de-synchronizing toroidal harmonics by using feedback | Steady State Heating and Current Drive | PPPL | No | No | No | |
| 176 details | Beta collapse avoidance in SSI discharges by de-synchronizing toroidal harmonics by using feedback | Steady State Heating and Current Drive | PPPL | No | No | No | |
| 178 details | Beta limit and bootstrap current fraction in ITER steady-state scenario discharges | Steady State Heating and Current Drive | GA | No | No | No | |
| 179 details | Snowflake in AT Plasma | Steady State Heating and Current Drive | LLNL | No | No | No | |
| 180 details | Establish the incremental confinement of EC power in high betaN steady-state scenario discharges | Steady State Heating and Current Drive | GA | No | No | No | |
| 181 details | Heat pulse propagation in a perturbed magnetic topology | ELM Control | GA | No | Yes | Yes | |
| 182 details | Systematic test of paleoclassical transport | Turbulence & Transport | GA | No | No | No | |
| 184 details | Comparision DIII-D and AUG high collisionality ELM response to 3D magnetic perturbations | ELM Control | GA | No | Yes | Yes | |
| 188 details | Extension of proxy error field experiments to H-mode plasmas | Stability & Disruption Avoidance | Columbia U | No | No | No | |
| 189 details | Measurement of optimal n=2 phasing for RMP & ELM suppression without q95 windows | ELM Control | Columbia U | No | No | No | |
| 190 details | Measurement of n=3 error field effects in RMP phase-flip experiments | ELM Control | Columbia U | No | No | No | |
| 192 details | Measurement of heat flux on the divertor using the embedded thermocouple array | Divertor & SOL Physics | U of Tennessee, Knoxville | No | No | No | |
| 194 details | Correlation of confinement and fluctuations with electron heating in ITER Baseline Scenario | Inductive Scenarios | GA | No | No | No | |
| 195 details | Correlation of confinement and fluctuations with electron heating in ITER Baseline Scenario | Turbulence & Transport | GA | No | No | No | |
| 204 details | Suppression of Density Limit Disruptions with RMP Fields | Torkil Jensen Award | GA | No | No | Yes | |
| 205 details | SOL width in top-limited discharges | Divertor & SOL Physics | UCSD | No | No | Yes | |
| 206 details | Studies of arcing on divertor PFC surfaces | Plasma-material Interface | UCSD | No | No | No | |
| 207 details | Dust generation from deposited layers and leading edges | Plasma-material Interface | UCSD | No | No | No | |
| 210 details | The Dependence of Poloidal Rotation on Turbulence | Plasma Rotation | GA | No | No | No | |
| 215 details | Control of tungsten PFC erosion by local gas injection | Plasma-material Interface | UCSD | No | No | No | |
| 219 details | Establishing an experimental basis for plasma effects on magnetic islands | ELM Control | GA | No | No | No | |
| 220 details | Comparison of n=2 RMP field effects on ELMs and pedestal properties in KSTAR and DIII-D | ELM Control | GA | No | Yes | Yes | |
| 231 details | Stabilization of NTMs with ECCD | Stability & Disruption Avoidance | QST | No | Yes | No | |
| 233 details | C erosion and D up-take at high surface temperature | Plasma-material Interface | GA | No | No | No | |
| 234 details | Study fishbone-like instability at the edge of QH-modes | Inductive Scenarios | Instituto Superior Tecnico, Lisboa, Portugal | No | No | No | |
| 235 details | High resolution Te pedestal measurements in RMP ELM suppression experiments | ELM Control | Sandia National Lab | No | No | No | |
| 236 details | Wavenumber dependence of turbulence suppression in the L-H transition | L-H Transition | UCLA | No | No | No | |
| 241 details | C-13 and background carbon | Plasma-material Interface | GA | No | No | No | |
| 242 details | q95 < 2 Tokamak Operation Via Dynamic Error Field Correction | Stability & Disruption Avoidance | GA | No | No | No | |
| 243 details | 256: SOL width and divertor peak heat flux in QH-mode plasmas with/without n=3 fields | Inductive Scenarios | GA | No | No | No | |
| 244 details | Study NRMF driven torque in ECH-only heated plasma (ELMing H-modes) | Plasma Rotation | GA | No | No | No | |
| 245 details | Investigate the physics of NTM suppression by large externally applied helical fields | Torkil Jensen Award | GA | No | No | No | |
| 246 details | Develop low-torque, high normalized fusion performance QH-mode for ITER baseline scenario | Inductive Scenarios | GA | No | No | No | |
| 247 details | Develop low-torque, high normalized fusion performance QH-mode for FNSF-AT scenario | Inductive Scenarios | GA | No | No | No | |
| 248 details | Investigate elongation limit in low li discharges with/without applied 3D magnetic fields | Torkil Jensen Award | GA | No | No | No | |
| 249 details | Steady-state high beta with NCS and qmin>2 | Steady State Heating and Current Drive | GA | No | No | No | |
| 250 details | Plateau Ecrit with MGI | Disruption Mitigation | GA | No | Yes | Yes | |
| 251 details | New Study of Alfven Eigenmodes Induced Fast Ion Transport/Loss | Energetic Particles | GA | No | No | No | |
| 252 details | Implement finite-state Off Normal Fault Response system | Plasma Control | GA | No | No | No | |
| 253 details | Study QH-mode with advanced fast ion diagnostics and codes | Inductive Scenarios | GA | No | No | No | |
| 254 details | Neon SPI injection into early CQ to stunt RE formation | Disruption Mitigation | GA | No | No | No | |
| 256 details | Fine scale stepwise q-scan: role of low-order rationales and resonance condition for ELM suppression | ELM Control | U of Wisconsin | No | No | No | |
| 257 details | Transport Investigation During Slow Current Ramp-Up and Ramp-Down [for ITER] | Inductive Scenarios | U of Wisconsin | No | Yes | No | |
| 258 details | Main-ion and impurity rotation in helium plasmas | Plasma Rotation | GA | No | No | No | |
| 259 details | Helium Campaign (D beams) | General Physics | GA | No | No | No | |
| 260 details | ITER Baseline Scenario Demonstration | Inductive Scenarios | ITER Organization | No | Yes | No | |
| 261 details | Demonstration of stationary inductive solutions at low and moderate q95 | Inductive Scenarios | ITER Organization | No | No | No | |
| 262 details | Test Pedestal Structure Model Where Paleoclassical Transport Is Dominant | Pedestal Structure | U of Wisconsin | No | No | No | |
| 263 details | Radiative divertor solutions in the ITER baseline scenario | Inductive Scenarios | ITER Organization | No | Yes | Yes | |
| 264 details | Radiative divertor solutions in the ITER baseline scenario | Divertor & SOL Physics | ITER Organization | No | Yes | Yes | |
| 265 details | o Experiments using the centerpost Swing-probes | Divertor & SOL Physics | UCSD | No | No | No | |
| 266 details | Understand resistive wall mode control physics in low-q95 plasmas | Inductive Scenarios | Columbia U | No | No | No | |
| 267 details | Understand and control resistive wall mode stability in high-qmin plasmas | Steady State Heating and Current Drive | Columbia U | No | No | No | |
| 268 details | nu* dimensionless scaling | Turbulence & Transport | CEA | No | Yes | No | |
| 278 details | Possibility of â??Off-axis-Fishbone Mode and ELM Pacingâ?? due to Direct Energetic Particle Coupling | ELM Control | JAEA | No | No | No | |
| 280 details | : Trigger-less onset of NTMs with PEC and NTV effects on rotation regime | Plasma Rotation | Istituto di Fisica del Plasma, Euratom-ENEA-CNR | No | No | No | |
| 283 details | ITER Baseline Scenario Operation near the LH Threshold | Inductive Scenarios | ITER Organization | No | Yes | No | |
| 284 details | Access conditions for steady-state operation in ITER | Steady State Heating and Current Drive | ITER Organization | No | Yes | No | |
| 285 details | Access to advanced inductive operation in ITER | Inductive Scenarios | ITER Organization | No | Yes | No | |
| 286 details | Collisionality scaling of confinement in advanced inductive regimes | Inductive Scenarios | ITER Organization | No | Yes | No | |
| 287 details | High li steady-state scenario development | Steady State Heating and Current Drive | ITER Organization | No | No | No | |
| 288 details | Amplifying the Geodesic Acoustic Mode via Resonant Radial Field Amplification: New Methods | Turbulence & Transport | U of Wisconsin | No | No | No | |
| 289 details | Demonstrate access to beta_N=5 with min(q)>2 | Steady State Heating and Current Drive | ITER Organization | No | No | No | |
| 290 details | Effect of n=2 Poloidal Spectrum on NTV Torque | Plasma Rotation | Department of Energy | No | No | No | |
| 291 details | Trigger-less onset of NTMs with P_EC and NTV effects on rotation regime | Stability & Disruption Avoidance | Instituto Superior Tecnico, Lisboa, Portugal | No | No | No | |
| 292 details | Optimize electron pedestal pressure in low-torque ITER baseline plasmas | Inductive Scenarios | UCLA | No | No | No | |
| 293 details | Test of ETG zeff supression | Turbulence & Transport | GA | No | No | No | |
| 294 details | Simulated Alpha particle dillution | Turbulence & Transport | GA | No | No | No | |
| 295 details | preliminary simulated burn control | Turbulence & Transport | GA | No | No | No | |
| 297 details | ITER baseline scenario with low NBI torque | Inductive Scenarios | GA | No | No | No | |
| 298 details | Soft landing with 2/1 TM in the ITER shape | Stability & Disruption Avoidance | GA | No | No | No | |
| 299 details | Aspect ratio scaling of turbulence and transport: DIII-D and NSTX-U comparison | Turbulence & Transport | Univ. Wisconsin (at PPPL) | No | No | No | |
| 300 details | Effect of triangularity in ITER shape and improved shaping | Inductive Scenarios | GA | No | No | No | |
| 302 details | RMP ELM Suppression at the NTV Offset Rotation | ELM Control | GA | No | No | No | |
| 303 details | Effect on lithium wall conditioning for Co-QH-mode and edge pedestal characteristics | Inductive Scenarios | GA | No | No | No | |
| 304 details | Birth of ITER: the world's largest resistor | General Physics | GA | No | No | No | |
| 305 details | Scaling Of Pedestal Plasma Transport With RMP I-coil Current | ELM Control | U of Wisconsin | No | No | No | |
| 306 details | Edge turbulence and blob generation | Divertor & SOL Physics | Univ. Wisconsin | No | No | No | |
| 307 details | Role of turbulent-driven and Ion pressure gradient-sustained ExB flows in Triggering H-mode | L-H Transition | UCSD | No | No | No | |
| 308 details | RMP (Resonant Magnetic Perturbation) code validation via UCLA 288 GHz polarimeter | ELM Control | UCLA | No | No | No | |
| 309 details | Full 3D Rotation optimization of H mode | Stability & Disruption Avoidance | GA | No | Yes | Yes | |
| 310 details | Energy Transport During Electron-Dominated Heating of ITER-Relevant H-Mode Discharges | Steady State Heating and Current Drive | PPPL | No | No | No | |
| 311 details | Transport with qmin>2 | Steady State Heating and Current Drive | LLNL | No | No | No | |
| 312 details | Limits to pedestal radiation high beta discharges | Steady State Heating and Current Drive | GA | No | No | No | |
| 313 details | Hybrids with co-NBI QH-mode edge | Inductive Scenarios | GA | No | No | No | |
| 314 details | Optimization of castellation for a new W-divertor of ITER: studies of shaped castellation in DIII-D | Plasma-material Interface | UCSD | No | Yes | Yes | |
| 315 details | Current profile control model requirements | Plasma Control | GA | No | No | No | |
| 316 details | Model-based control of the current profile and βN for steady state scenarios | Plasma Control | Cadarache | No | No | No | |
| 317 details | Study on sawteeth in the neutral beam (NB) heated plasmas | Stability & Disruption Avoidance | Korea National Fusion Research Center | No | No | No | |
| 318 details | Current profile control for stable ITER baseline scenario plasmas | Inductive Scenarios | Columbia U | No | No | No | |
| 319 details | Impact of fast-ions on the RWM stability boundary | General Physics | Columbia U | No | No | No | |
| 320 details | RWM excitation in the SSI target by reducing triangularity" | Stability & Disruption Avoidance | PPPL | No | No | No | |
| 321 details | Access to low torque QH-mode using high beta low torque AI target with NRMF | Inductive Scenarios | GA | No | No | No | |
| 322 details | ELM pacing in low torque, electron heated ITER baseline | Inductive Scenarios | GA | No | No | No | |
| 323 details | Access to QH-mode with low NBI torque | Inductive Scenarios | GA | No | No | No | |
| 324 details | Document turbulence change with rotation in AI, and compare with theory | Inductive Scenarios | GA | No | No | No | |
| 325 details | Document turbulence change with rotation in AI, and compare with theory | Turbulence & Transport | GA | No | No | No | |
| 326 details | Understand mechanisms by which ECH influences NTM stablility | Stability & Disruption Avoidance | GA | No | No | No | |
| 327 details | rho* scaling of intrinsic torque between DIII-D and JET | Plasma Rotation | GA | No | Yes | No | |
| 328 details | Error field correction at low rotation | Stability & Disruption Avoidance | GA | No | No | No | |
| 329 details | Discussion of plasma rotation transient process during OFM/ELM-driven RWM w/wo feedback usin | Stability & Disruption Avoidance | PPPL | No | No | No | |
| 330 details | QH-mode with TBM | Inductive Scenarios | GA | No | No | No | |
| 331 details | QH-mode with TBM (dup 330) | Stability & Disruption Avoidance | GA | No | No | No | |
| 332 details | Demonstration of noninductive Q=5 scenario in ITER shape using off-axis NBI | Steady State Heating and Current Drive | ORNL | No | No | No | |
| 333 details | Far off-axis NBCD | Steady State Heating and Current Drive | ORNL | No | No | No | |
| 334 details | Measurement of neoclassical response of off-axis beam ions | Steady State Heating and Current Drive | ORNL | No | No | No | |
| 335 details | Off-axis NBCD measurement in steady state scenario | Steady State Heating and Current Drive | ORNL | No | No | No | |
| 336 details | Routine current profile control in operation | Steady State Heating and Current Drive | GA | No | No | No | |
| 337 details | Routine current profile control in operation | Inductive Scenarios | GA | No | No | No | |
| 338 details | Local correction of the TBM error field | Stability & Disruption Avoidance | Columbia U | No | No | Yes | |
| 339 details | Combined effect of TBM and NTM fields on fast-ion confinement | Stability & Disruption Avoidance | UC, Irvine | No | Yes | No | |
| 340 details | Combined effect of TBM and Sawtooth fields on fast-ion confinement | Stability & Disruption Avoidance | UC, Irvine | No | Yes | No | |
| 342 details | Investigation of Core Poloidal Rotation Anomaly Change at ITG -> TEM transition | Plasma Rotation | National Fusion Research Institute (NFRI) | No | Yes | Yes | |
| 343 details | Evaluating Physics of RMP Stationary Enhanced Confinement Regime Without ELMs for the 2013 JRT | ELM Control | LLNL | No | No | Yes | |
| 344 details | Evaluating Physics of QH-mode Stationary Enhanced Confinement Regime Without ELMs for the 2013 J | Inductive Scenarios | LLNL | No | No | No | |
| 345 details | Evaluating Physics of I-mode Stationary Enhanced Confinement Regime Without ELMs for the 2013 JR | ELM Control | LLNL | No | No | No | |
| 346 details | Control of H-L back transition via applied RMP fields | L-H Transition | UCLA | No | No | No | |
| 347 details | Do differences in co/cnter GAM/ZF behavior affect deficit in gyrokinetic predicted Lmode transport? | Turbulence & Transport | UCLA | No | No | No | |
| 348 details | Can we obtain ELM suppression without substantial loss of density? | ELM Control | UCLA | No | No | No | |
| 349 details | Density/current Scaling of Intrinsic Rotation and ITG/TEM Transition | Turbulence & Transport | UCLA | No | No | No | |
| 350 details | Current/Density Scaling of Intrinsic Rotation and ITG/TEM Transition | Plasma Rotation | UCLA | No | No | No | |
| 351 details | Confinement enhancement via impurity-seeding of H-mode plasmas | Turbulence & Transport | U of Wisconsin | No | No | No | |
| 352 details | Does increased turbulence in H-mode degrade agreement of GK transport/turbulence simulations? | Turbulence & Transport | UCLA | No | No | No | |
| 353 details | Correlation length of electron temperature turbulence measurement and comparison with simulations | Turbulence & Transport | UCLA | No | No | No | |
| 354 details | Control of Major Disruptions in DIII-D | Stability & Disruption Avoidance | Columbia U | No | No | No | |
| 355 details | q dependence of L-H transition power threshold | L-H Transition | UCLA | No | No | No | |
| 356 details | GAM eigenmode excitation mechanism | Turbulence & Transport | UCLA | No | No | No | |
| 357 details | GAM eigenmode 2D structure | Turbulence & Transport | UCLA | No | No | No | |
| 359 details | q95 scaling of the coupled turbulence/zonal flow during LH transition | L-H Transition | U of Wisconsin | No | No | No | |
| 360 details | density scaling and X-point position scan of LH transition power threshold | L-H Transition | U of Wisconsin | No | No | No | |
| 361 details | Dither injection for closed-loop system identification of vacuum and plasma response | Stability & Disruption Avoidance | Consultant | No | No | No | |
| 362 details | Investigation of GAMs during I-mode on D3D | Turbulence & Transport | Massachusetts Institute of Technology | No | Yes | No | |
| 363 details | TBM mockup simulating ITER GDC with ferritic materials | General Physics | GA | No | No | No | |
| 364 details | Absolute plasma response null measurement by multiple betaN steps | Stability & Disruption Avoidance | Columbia U | No | No | No | |
| 365 details | Lithium dropper commissioning and ELM modification | General Physics | GA | No | No | No | |
| 366 details | Up/down Asymmetric EFC | Stability & Disruption Avoidance | Department of Energy | No | No | No | |
| 367 details | JET/DIII-D similarity experiment on rotation in plasmas with low momentum input | Plasma Rotation | Instituto Superior Tecnico, Lisboa, Portugal | No | Yes | No | |
| 368 details | Investigation of extreme outer wall heating caused by the DIII-D TBM | Plasma-material Interface | LLNL | No | Yes | Yes | |
| 369 details | First-principles-driven Model-based Current-profile Control in H-mode Discharges | Plasma Control | Lehigh U | No | No | No | |
| 370 details | Particle pinch in pedestal | Pedestal Structure | GA | No | No | No | |
| 371 details | Effect of icoil current on energy confinement in RMP ELM-suppressed discharges | ELM Control | GA | No | No | No | |
| 372 details | Pedestal optimization via impurity injection | Pedestal Structure | ORNL | No | No | No | |
| 373 details | Pedestal optimization in VH mode | Pedestal Structure | ORNL | No | No | No | |
| 374 details | Pedestal optimization with RMP ELM Control | Pedestal Structure | ORNL | No | No | No | |
| 375 details | QH-mode pedestal optimization | Inductive Scenarios | ORNL | No | No | No | |
| 376 details | Role of q and magnetic shear of pedestal formation time and turbulent transport | Pedestal Structure | PPPL | No | No | No | |
| 377 details | NTM locking disruption avoidance by the EM torque with toroidal-phase forward magnetic feed | Disruption Mitigation | PPPL | No | No | No | |
| 378 details | Study of the connection between I-mode and low density Type III ELMs and optimization of I-mode | ELM Control | GA | No | No | No | |
| 379 details | Pedestal optimization of ITER baseline scenario discharges. | Pedestal Structure | GA | No | No | No | |
| 380 details | ELM Suppression at Lower Collisionality with Non-Resonant n=3 I-coil | ELM Control | GA | No | No | No | |
| 381 details | Search for turbulence at ion-cyclotron frequencies | Turbulence & Transport | UCLA | No | No | No | |
| 382 details | Transport and turbulence characterization experiment | Steady State Heating and Current Drive | UCLA | No | No | No |