DIII-D RESEARCH OPPORTUNITIES FORUM FOR THE 2019 EXPERIMENTAL CAMPAIGN
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| ID | Title | Research Area | Name | Affiliation |
Time Req'ed |
Presentation |
ITPA Joint Exp |
ITER IO Urgent Research Task |
| 457 | m/n=2/1 NTM control by ECCD in steady state hybrid | 3DSP | Bardoczi | GA | No | Breakout | No | No |
| 459 | Use pellets to lower the ECCD requirement for 2/1 NTM stabilization | 3DSP | Bardoczi | GA | No | Breakout | No | No |
| 190 | Impact of Current Condensation in the ECCD Stabilization of Rotating 2/1 NTMs | 3DSP | Bardoczi | GA | No | Breakout | No | No |
| 192 | m/n=2/1 NTM control by ECCD in IBS | 3DSP | Bardoczi | GA | No | Breakout | No | No |
| 199 | Machine Learning based Instability Prediction & Avoidance | 3DSP | Kolemen | PPPL | No | Breakout | No | No |
| 205 | RT stability analysis to find/avoid the instabilities with mhd calc. and feedback 3D spectroscopy | 3DSP | Kolemen | PPPL | No | Breakout | No | No |
| 206 | ECCD and ECH for IBS with real-time modulation control | 3DSP | Kolemen | PPPL | No | Breakout | No | No |
| 82 | Clarify key snowflake divertor physics | Advanced Magnetic Configurations | Soukhanovskii | LLNL | No | Breakout | No | No |
| 83 | Particle exhaust in snowflake divertor | Advanced Magnetic Configurations | Soukhanovskii | LLNL | No | Breakout | No | No |
| 210 | Puff and Pump Flow measurement in DN as a function of drsep | Advanced Magnetic Configurations | Allen | LLNL | No | Breakout | No | No |
| 84 | Clarify snowflake divertor physics | Advanced Magnetic Configurations | Soukhanovskii | LLNL | No | Breakout | No | No |
| 325 | Profile control for high qmin steady state scenario | Control | Wehner | Lehigh | No | Breakout | No | No |
| 326 | Model-based rotation control development | Control | Wehner | Lehigh | No | Breakout | No | No |
| 288 | Exploration of IBS variation with direct gain metric regulation | Control | Olofsson | Consultant | No | Breakout | No | No |
| 289 | Shape control enabled study of IBS stability as function of edge features | Control | Olofsson | Consultant | No | Breakout | No | No |
| 458 | m/n=2/1 NTM control by ECCD in steady state hybrid | Control | Bardoczi | GA | No | Breakout | No | No |
| 419 | Commissioning of a proximity-to-stability-boundary control architecture for disruption prevention | Control | Barr | GA | No | Breakout | No | No |
| 420 | Commissioning of a Vertical Control proximity-to-stability-boundary algorithm for VDE prevention | Control | Barr | GA | No | Breakout | No | No |
| 346 | Developing low-disruptivity ramp-down techniques for the ITER Baseline Scenario | Control | Barr | GA | No | Breakout | No | No |
| 201 | m/n=2/1 NTM control by ECCD in IBS | Control | Bardoczi | GA | No | Breakout | No | No |
| 339 | Detachment control w/ Te request translated to ne estimate & direct ne feedback | Control | Eldon | GA | No | Breakout | No | No |
| 342 | Vertical stability control with simulated horizontal interferometer channels | Control | Eldon | GA | No | Breakout | No | No |
| 275 | Divertor radiated power control in non-ELMing plasmas | Control | Eldon | GA | No | Breakout | No | No |
| 506 | PCS supervisory algorithm for negotiating complex controller requests | Control | Eidietis | GA | No | Breakout | No | No |
| 44 | Real time measurements of impurity density | Control | Chrystal | GA | No | Breakout | No | No |
| 314 | Voltage controlled SuperSpas for plasma shape control | Control | Hyatt | GA | No | Breakout | No | No |
| 315 | VFI-less Plasma operations | Control | Hyatt | GA | No | Breakout | No | No |
| 347 | ITER plasma initiation and ECH assist | Control | Walker | GA | No | Breakout | Yes | Yes |
| 403 | Burn Condition Emulation for ITER-relevant Control Experiments | Control | Schuster | Lehigh U | No | Breakout | No | No |
| 429 | Real time neutron control | Control | Heidbrink | UC, Irvine | No | Breakout | No | No |
| 511 | Feedback control for divertor impurity seeding based on Surface Eroding Thermocouple | Control | Ren | U of Tennessee, Knoxville | No | Breakout | No | No |
| 323 | Tune RMP Controlled Phase of Locked Island and Radial Alignment of ECCD Deposition for Stabilization | Control | Reiman | PPPL | No | Breakout | No | No |
| 338 | Combining variable beam energy/perveance and NTV for rotation control | Control | Boyer | PPPL | No | Breakout | No | No |
| 521 | ECCD and ECH for IBS with real-time modulation control | Control | Kolemen | PPPL | No | Breakout | No | No |
| 522 | RT stability analysis to find/avoid the instabilities with mhd calc. and feedback 3D spectroscopy | Control | Kolemen | PPPL | No | Breakout | No | No |
| 523 | Test the new method for finding the 3D perturbation needed to avoid tearing | Control | Kolemen | PPPL | No | Breakout | No | No |
| 524 | Control of pressure/current profile transport models experimentally | Control | Kolemen | PPPL | No | Breakout | No | No |
| 278 | A Boron-Nitrogen radiative divertor for AT scenarios | Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization | Bortolon | PPPL | No | Breakout | No | No |
| 316 | A Boron-Nitrogen radiative divertor for AT scenarios | Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization | Bortolon | PPPL | No | Breakout | No | No |
| 191 | What can lost fast-ions tell us about the H-mode pedestal? | Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization | Kramer | PPPL | No | Breakout | No | No |
| 212 | Minimize carbon in DIII-D AT plasmas | Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization | Allen | LLNL | No | Breakout | No | No |
| 207 | Measure and Influence Flow with Pump and Pump | Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization | Allen | LLNL | No | Breakout | No | No |
| 448 | Optimizing core-pedestal performance in Super H-Mode | Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization | Snyder | ORNL | No | Breakout | No | No |
| 253 | Investigation and optimization of core and pedestal performance | Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization | Solomon | GA | No | Breakout | No | No |
| 565 | Measure lambda-q during rotation scans at constant heating power in super H mode plasmas | Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization | Garofalo | GA | No | Breakout | No | No |
| 462 | Pedestal pressure enhancement at high density through decoupling of ped peeling and ballooning modes | Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization | Osborne | GA | No | Breakout | No | No |
| 217 | co-Ip QH-mode approach to super H-mode | Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization | Chen | GA | No | Breakout | No | No |
| 344 | Detachment onset density vs. 3D field strength | Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization | Eldon | GA | No | Breakout | No | No |
| 269 | Pushing Steady-State Hybrid Scenario to Lower q95, Higher Beta and Higher Fusion Gain | Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization | Petty | GA | No | Breakout | No | No |
| 272 | High Density Electron Heating With O-Mode | Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization | Petty | GA | No | Breakout | No | Yes |
| 277 | Divertor radiated power control vs. ELM frequency | Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization | Eldon | GA | No | Breakout | No | No |
| 409 | Detachment/T_e cliff onset density vs. I_p using control to stay on the edge of the cliff | Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization | Eldon | GA | No | Breakout | No | No |
| 340 | Burn through of paced ELMs in detachment | Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization | Eldon | GA | No | Breakout | No | No |
| 153 | Balancing the Tradeoffs Between High Performance and Core Purity & Stability in High Power Hybrid | Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization | Grierson | GA | No | Breakout | No | No |
| 2 | testing, please ignore! | Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization | Coviello | GA | No | Breakout | No | No |
| 226 | Controlling ITB formation via impurity puffing | DIII-D/EAST Task Force/Thrust | McClenaghan | GA | No | Breakout | No | No |
| 442 | Access to small ELM regime in DIII-D high �²P scenario | DIII-D/EAST Task Force/Thrust | Qian | ASIPP | No | Breakout | Yes | Yes |
| 505 | Assessing Helicon wave current drive in high betap experiments | DIII-D/EAST Task Force/Thrust | Zhang | ASIPP | No | Breakout | No | No |
| 473 | Evaluating the internal MHD response to shell pellet injection | Disruption Mitigation Thrust | Pandya | U of Wisconsin | No | Breakout | No | No |
| 474 | Evaluating the internal MHD response to SPI | Disruption Mitigation Thrust | Pandya | U of Wisconsin | No | Breakout | No | No |
| 475 | Measuring internal MHD during the formation and evolution of a runaway electron beam | Disruption Mitigation Thrust | Pandya | U of Wisconsin | No | Breakout | No | No |
| 517 | Penetration characterization of small pellet injection into D3D plasmas | Disruption Mitigation Thrust | Raman | U of Washington | No | Breakout | No | No |
| 372 | whistler polarization | Disruption Mitigation Thrust | Heidbrink | UC, Irvine | No | Breakout | No | No |
| 14 | Comparison of dispersive vs non-dispersive shell pellet payload | Disruption Mitigation Thrust | Hollmann | UCSD | No | Breakout | No | No |
| 15 | Suppression of RE seeds with W grains in shell pellet | Disruption Mitigation Thrust | Hollmann | UCSD | No | Breakout | No | No |
| 16 | Dynamic measurement of impurity transport into RE plateau using carbon deposition | Disruption Mitigation Thrust | Hollmann | UCSD | No | Breakout | No | No |
| 17 | Change in RE plateau vertical loss rate with low-Z injection | Disruption Mitigation Thrust | Hollmann | UCSD | No | Breakout | No | No |
| 18 | Scan of RE plateau final loss footprint with I-coil perturbation | Disruption Mitigation Thrust | Hollmann | UCSD | No | Breakout | No | No |
| 19 | Scan of RE plateau impurity assimilation with auxiliary heating | Disruption Mitigation Thrust | Hollmann | UCSD | No | Breakout | No | No |
| 26 | Determine the cause of RE beam final loss in post disruption vertical displacement events | Disruption Mitigation Thrust | Bardoczi | GA | No | Breakout | No | Yes |
| 507 | ITER DMS design validation | Disruption Mitigation Thrust | Lehnen | ITER Organization | No | Breakout | No | No |
| 73 | Role of pre-disruption electron temperature in runaway electron seed formation | Disruption Mitigation Thrust | Paz-Soldan | Columbia U | No | Breakout | No | No |
| 11 | Identification of Alfven instabilities driven by REs at negative Uloop during RE plateau stage | Disruption Mitigation Thrust | Lvovskiy | GA | No | Breakout | No | No |
| 525 | Mass scaling of shell pellet assimilation | Disruption Mitigation Thrust | Eidietis | GA | No | Breakout | No | No |
| 526 | Full profile measurement of shell Te profile | Disruption Mitigation Thrust | Eidietis | GA | No | Breakout | No | No |
| 527 | Test Li coating for "ideal" shell pellet | Disruption Mitigation Thrust | Eidietis | GA | No | Breakout | No | No |
| 528 | Ablation measurments of single snall Ne pellet | Disruption Mitigation Thrust | Eidietis | GA | No | Breakout | No | No |
| 529 | Effect of D admixture in SPI | Disruption Mitigation Thrust | Eidietis | GA | No | Breakout | No | No |
| 530 | dilution cooling in SPI superposition | Disruption Mitigation Thrust | Eidietis | GA | No | Breakout | No | No |
| 531 | Scaling of fragment penetration depth with energy: | Disruption Mitigation Thrust | Eidietis | GA | No | Breakout | No | No |
| 532 | JET SPI similarity experiments | Disruption Mitigation Thrust | Eidietis | GA | No | Breakout | No | No |
| 539 | Effect of underlying non-axisymmetric (NA) fields on disruption mitigation process | Disruption Mitigation Thrust | Eidietis | GA | No | Breakout | No | No |
| 510 | Superposition of identical dual SPIs | Disruption Mitigation Thrust | Herfindal | ORNL | No | Breakout | No | No |
| 533 | Ballistic transport and energy/size scaling for SPI | Disruption Mitigation Thrust | Shiraki | ORNL | No | Breakout | No | No |
| 343 | Check for Te cliff at inner strike point in reverse Bt | Dissipative Divertor Physics | Eldon | GA | No | Breakout | No | No |
| 252 | Effect of divertor radiation front on drifts and parallel flow | Dissipative Divertor Physics | Boedo | UCSD | No | Breakout | No | No |
| 193 | Impact of molecular processes on divertor detachment and validation of UEDGE fluid molecular model | Dissipative Divertor Physics | Holm | PPPL | No | Breakout | No | No |
| 152 | Assessment of Ly-alpha opacity in fully detached divertor plasmas | Dissipative Divertor Physics | Groth | Aalto U | No | Breakout | No | No |
| 259 | Divertor to pedestal trace impurity transport | Div/SOL Turbulence and transport | Bortolon | PPPL | No | Breakout | No | No |
| 273 | Scaling of blobby transport with divertor conditions and pedestal/SOL widening | Div/SOL Turbulence and transport | Boedo | UCSD | No | Breakout | No | No |
| 248 | Poloidal asymmetries of radial transport in the edge/SOL | Div/SOL Turbulence and transport | Boedo | UCSD | No | Breakout | No | No |
| 374 | Effect on SEE on Langmuir probe measurements in the SOL | Div/SOL Turbulence and transport | Rudakov | UCSD | No | Breakout | No | No |
| 358 | Parallel correlation of turbulence/blobs between mid-plane and divertor SOL | Div/SOL Turbulence and transport | Rudakov | UCSD | No | Breakout | No | No |
| 354 | Study of impurity ion entrainment in divertor cross-field transport | Div/SOL Turbulence and transport | Hollmann | UCSD | No | Breakout | No | No |
| 421 | Magnetic shear at X-point and radial turbulence transport | Div/SOL Turbulence and transport | Boedo | UCSD | No | Breakout | No | No |
| 144 | Transport and turbulence in Divertor and pedestal during detachment | Div/SOL Turbulence and transport | Boedo | UCSD | No | Breakout | No | No |
| 138 | Physics of pedestal turbulence vs width | Div/SOL Turbulence and transport | Boedo | UCSD | No | Breakout | No | No |
| 270 | Evolution of edge turbulence and turbulence flow near midplane during divertor detachment | Div/SOL Turbulence and transport | Wang | UCLA | No | Breakout | No | No |
| 262 | Divertor-localized turbulence and characterization of 2D profiles of divertor turbulence | Div/SOL Turbulence and transport | Scotti | LLNL | No | Breakout | No | No |
| 414 | Quasi-coherent fluctuations near the divertor plate | Div/SOL Turbulence and transport | Wang | GA | No | Breakout | No | No |
| 397 | Establish ELM suppression in DND plasma | ELM Control | Lyons | GA | No | Breakout | No | No |
| 147 | Pellet Fueled High Density Operation of RMP ELM Mitigated Plasmas | ELM Control | Baylor | ORNL | No | Breakout | No | No |
| 407 | Divertor radiated power control vs. ELM frequency | ELM Control | Eldon | GA | No | Breakout | No | No |
| 408 | Burn through of paced ELMs in detachment | ELM Control | Eldon | GA | No | Breakout | No | No |
| 356 | ELM pacing by pellet injection in low-collisionality ITER relevant scenarios | ELM Control | Bortolon | PPPL | No | Breakout | No | No |
| 554 | ELM pacing during ITER-like current ramp-up/down | ELM Control | Bortolon | PPPL | No | Breakout | No | Yes |
| 537 | ELM pacing during ITER-like current ramp-up/down | ELM Control | Bortolon | PPPL | No | Breakout | No | Yes |
| 393 | ELM pacing by pellet injection in low-collisionality ITER relevant scenarios | ELM Control | Bortolon | PPPL | No | Breakout | No | No |
| 394 | ELM pacing during ITER-like current ramp-up/down | ELM Control | Bortolon | PPPL | No | Breakout | No | Yes |
| 395 | ELM pacing during ITER-like current ramp-up/down | ELM Control | Bortolon | PPPL | No | Breakout | No | Yes |
| 181 | ICE internal amplitude and radial structure | Energetic Particle Physics | Crocker | UCLA | No | Breakout | No | No |
| 182 | CAE suppression by more parallel injection | Energetic Particle Physics | Crocker | UCLA | No | Breakout | No | No |
| 198 | Radial structure and identification of intermediate frequency Alfven eignemodes | Energetic Particle Physics | Crocker | UCLA | No | Breakout | No | No |
| 299 | Transient ExB flows caused by bursting fast-ion modes and secondary transport-related impacts | Energetic Particle Physics | Crocker | UCLA | No | Breakout | No | No |
| 42 | Determine accuracy of NUBEAM power and torque outside mid-radius | Energetic Particle Physics | Chrystal | GA | No | Breakout | No | No |
| 490 | BAAE and BAE validation | Energetic Particle Physics | Heidbrink | UC, Irvine | No | Breakout | Yes | No |
| 496 | Orbit Tomography (OT) | Energetic Particle Physics | Garcia | UC, Irvine | No | Breakout | Yes | No |
| 515 | Parameter scan of fast-ion critical gradient threshold | Energetic Particle Physics | Collins | ORNL | No | Breakout | No | No |
| 501 | Modification of AE Drive and Nonlinear Saturation Through Variation of Beam Modulation | Energetic Particle Physics | Van Zeeland | GA | No | Breakout | Yes | No |
| 56 | Hunt the instabilities responsible for the formation of phase space hole | Energetic Particle Physics | Du | GA | No | General | No | No |
| 546 | Direct measurement of the wave-particle interactions and associated phase space flow | Energetic Particle Physics | Du | GA | No | Breakout | No | No |
| 547 | Direct measurement of the wave-particle interactions and associated phase space flow | Energetic Particle Physics | du | General Atomic | No | Breakout | No | No |
| 456 | Stabilization of TAEs by Localized Electron Cyclotron Current Drive | Energetic Particle Physics | Sharapov | CCFE | No | Breakout | Yes | No |
| 124 | Characterization of Fast-ion Diagnostic to Edge Neutral Populations | Energetic Particle Physics | Stagner | GA | No | Breakout | No | No |
| 561 | Experimental Validation of Heteroclitic magnetic Island Bifurcations in DIII-D | General Physics | Evans | GA | No | Breakout | No | No |
| 1 | Welcome to the ROF for the 2019-20 DIII-D Run Campaign | General Physics | Fenstermacher | LLNL | No | Breakout | No | No |
| 504 | Helicon Launcher Checkout and Conditioning | Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools) | Zhang | ASIPP | No | Breakout | No | No |
| 324 | Measurement of helicon wave internal amplitude and validation of simulation | Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools) | Crocker | UCLA | No | Breakout | No | No |
| 370 | Checkout 210 beams | Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools) | Heidbrink | UC, Irvine | No | Breakout | No | No |
| 552 | Parametric instabilities during Helicon wave Iinjection in DIII-D | Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools) | Porkolab | Massachusetts Institute of Technology | No | Breakout | No | No |
| 498 | Measurement of NBCD profile | Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools) | Petty | GA | No | Breakout | No | No |
| 7 | Checkout of 210 CCOANB Using Visible Imaging | Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools) | Van Zeeland | GA | No | Breakout | No | No |
| 471 | experimental demonstration both down-shift and up-shift top launch ECCD schemes | Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools) | Chen | GA | No | Breakout | No | No |
| 472 | polarization study of top launch | Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools) | Chen | GA | No | Breakout | No | No |
| 485 | Third harmonic ECH experiments | Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools) | Schneider | ITER Organization | No | Breakout | No | No |
| 345 | ECRH plasma production on DIII-D | Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools) | Wauters | LPP-ERM-KMS � Brussels � Belgium (EUROfusion member) | No | Breakout | Yes | Yes |
| 486 | Helicon Modulation and Shutdown Checkout | Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools) | Brookman | GA | No | Breakout | No | No |
| 5 | 210 CCOANB Counter-direction Checkout - Including Power and Ability to Balance Torque | Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools) | Grierson | GA | No | Breakout | No | No |
| 555 | Toroidal symmetry of SAS tiles | Impact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential Thrust | Bykov | GA | No | Breakout | No | No |
| 558 | High-Z impurity pump-out mechanism inside of MHD modes in plasma with divertor W source | Impact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential Thrust | Odstrcil | GA | No | Breakout | No | No |
| 560 | Using the SAS to control impurity pinch | Impact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential Thrust | Nelson | Columbia U | No | General | No | No |
| 557 | RMP ELM suppression in the SAS shape | Impact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential Thrust | Evans | GA | No | Breakout | No | No |
| 562 | Minimizing W divertor leakage in the SAS | Impact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential Thrust | Unterberg | ORNL | No | Breakout | No | No |
| 434 | Effect of main ion SOL flows on W impurity transport | Impact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential Thrust | Rudakov | UCSD | No | Breakout | No | No |
| 234 | Search for Tungsten Accumulation in Upper divertor | Impact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential Thrust | Allen | LLNL | No | Breakout | No | No |
| 564 | Impact of high-Z PFCs on impurity seeding experiments in SAS | Impact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential Thrust | Casali | U of Tennessee, Knoxville | No | Breakout | No | No |
| 503 | Impact of large area electrical biasing on material erosion and divertor leakage in SAS1-W | Impact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential Thrust | Ren | U of Tennessee, Knoxville | No | Breakout | No | No |
| 81 | Snowflake SAS divertor | Impurity Radiative Divertor Dependence on Divertor Closure | Soukhanovskii | LLNL | No | Breakout | No | No |
| 85 | Can open horizontal plate divertor act as baffled vertical plate divertor | Impurity Radiative Divertor Dependence on Divertor Closure | Soukhanovskii | LLNL | No | Breakout | No | No |
| 306 | Is krypton better than argon as a mantle seed in high power, high performance hybrid plasmas? | Impurity Radiative Divertor Dependence on Divertor Closuree | Petrie | GA | No | Breakout | No | No |
| 307 | Two-impurity approach as an optimal radiating divertor solution for DIII-D | Impurity Radiative Divertor Dependence on Divertor Closuree | Petrie | GA | No | Breakout | No | No |
| 310 | Two-impurity approach as an optimal radiating divertor solution for DIII-D | Impurity Radiative Divertor Dependence on Divertor Closuree | Petrie | GA | No | Breakout | No | No |
| 538 | Expanding the Wide Pedestal QH to IBS Parameters | Inductive Scenarios | Chen | GA | No | Breakout | No | No |
| 77 | Direct comparison of ITER similar shape (ISS) and ITER baseline scenario (IBS) plasmas for RMP-ELM | Inductive Scenarios | Paz-Soldan | Columbia U | No | Breakout | No | No |
| 355 | High fusion gain in the advanced inductive | Inductive Scenarios | Thome | GA | No | Breakout | No | No |
| 489 | Developing low-disruptivity ramp-down techniques for the ITER Baseline Scenario | Inductive Scenarios | Barr | GA | No | Breakout | No | No |
| 229 | Measure and control resistive kink mode stability | Inductive Scenarios | Hanson | Columbia U | No | Breakout | No | No |
| 57 | Assess robustness of ITER baseline plasma response control | Inductive Scenarios | Hanson | Columbia U | No | Breakout | No | No |
| 95 | ELM-resolved D and D2 re-emission from C,W,and SiC: characterization by ro-vibrational spectroscopy | Innovative Materials Evaluation | Bykov | GA | No | Breakout | No | No |
| 509 | Exposure of Graphitic foam at DiMES and Tile | Innovative Materials Evaluation | Unterberg | ORNL | No | Breakout | No | No |
| 476 | Pedestal dimensionless parameter match DIII-D to JET for H,D,He | Isotope Mass Thrust | Osborne | GA | No | Breakout | No | No |
| 103 | Comparison of high density ELM suppression in H and He to D | Isotope Mass Thrust | Evans | GA | No | Breakout | No | Yes |
| 334 | Negative Triangularity in H Plasma | Isotope Mass Thrust | Smith | GA | No | Breakout | No | No |
| 335 | High performance QH-mode in H plasma with pellet fueling | Isotope Mass Thrust | Smith | GA | No | Breakout | No | No |
| 236 | wide-pedestal QH in dominant electron-heated ITER PFPO hydrogen plasmas | Isotope Mass Thrust | Chen | GA | No | Breakout | No | No |
| 75 | RMP-ELM Suppression and Mitigation in Hydrogen Plasmas | Isotope Mass Thrust | Paz-Soldan | Columbia U | No | Breakout | No | No |
| 341 | Energy Confinement dependence on mass | Isotope mass Thrust | Thome | GA | No | Breakout | No | No |
| 350 | isotope scaling with matched kinetic profiles | Isotope Mass Thrust | scott | PPPL | No | Breakout | No | No |
| 279 | Isotope effect on the detachment rollover density | Isotope Mass Thrust | Solokha | Aalto U | No | No | No | |
| 245 | Characterizing Detachment in H-mode Helium Plasmas | Isotope mass Thrust | Samuell | LLNL | No | Breakout | No | No |
| 46 | Isotope mix effects (puffing He into H plasmas) on the L-H power threshold | Isotope mass Thrust | Yan | U of Wisconsin | No | Breakout | No | No |
| 348 | Divertor configuration effects on the L-H power threshold in H plasmas | Isotope mass Thrust | Yan | U of Wisconsin | No | Breakout | No | No |
| 115 | Role of fueling in determining the pedestal structure | Isotope Mass Thrust | Mordijck | The college of William and Mary | No | Breakout | Yes | Yes |
| 250 | Mitigate increased L-H transition threshold power in ITER PFPO hydrogen plasmas w/wo applied RMP | Isotope mass Thrust | Schmitz | UCLA | No | Breakout | No | No |
| 357 | Power loading at toroidal PFC gaps | Isotope Mass Thrust | Rudakov | UCSD | No | Breakout | Yes | Yes |
| 536 | Helium scenarios for ITER | Isotope mass Thrust | Marinoni | UCSD | No | Breakout | Yes | No |
| 274 | edge/SOL turbulence with plasma isotopic mass scaling. | Isotope mass Thrust | Boedo | UCSD | No | Breakout | No | No |
| 446 | Pedestal structure in hydrogen-1 plasmas relevant for non-nuclear Iter and access to ELM suppression | Isotope mass Thrust | Laggner | North Carolina State | No | Breakout | No | No |
| 66 | Impact of RMP on the L-H threshold | L-H transition | Diallo | PPPL | No | Breakout | No | No |
| 360 | LH power threshold, confinement scaling and CER calibration in carbon plasmas | L-H transition | Marinoni | UCSD | No | Breakout | No | No |
| 71 | Role of scrape-off layer electric field in L-H power threshold scaling | L-H transition | Schmitz | UCLA | No | Breakout | No | No |
| 551 | What's the physics leads to std QH, Wide Pedestal QH,or ELMing IBS from L-mode at low torque? | L-H transition | Chen | GA | No | Breakout | No | No |
| 352 | Stationary Zonal Flows | L-H transition | Burrell | GA | No | Breakout | No | No |
| 337 | ECRH plasma production on DIII-D | Materials Migration and Mitigation | Wauters | LPP-ERM-KMS � Brussels � Belgium (EUROfusion member) | No | Breakout | Yes | Yes |
| 406 | W-pellet injection to calibrate the DIII-D Collector Probe | Materials Migration and Mitigation | Stangeby | U of Toronto | No | Breakout | No | No |
| 235 | Physics of real-time wall conditioning by B dust injection | Materials Migration and Mitigation | Bortolon | PPPL | No | Breakout | No | No |
| 438 | Effect of in-divertor gas puff location in SAS | Particle Balance and Impact of Divertor Closure Including SAS on Detachment Thrust | Moser | GA | No | Breakout | No | No |
| 440 | Optimizing SOL width in closed divertor for particle control and detachment | Particle Balance and Impact of Divertor Closure Including SAS on Detachment Thrust | Moser | GA | No | Breakout | No | No |
| 463 | QH-mode with detached divertor | Particle Balance and Impact of Divertor Closure Including SAS on Detachment Thrust | Osborne | GA | No | Breakout | No | No |
| 437 | Optimizing the pumping geometry for SAS2 | Particle Balance and Impact of Divertor Closure Including SAS on Detachment Thrust | Canik | ORNL | No | Breakout | No | No |
| 441 | How does SAS performance depend on enclosed poloidal flux? | Particle Balance and Impact of Divertor Closure Including SAS on Detachment Thrust | Thomas | GA | No | Breakout | No | No |
| 461 | Pedestal and core transport comparison of SAS , upper closed, and lower open divertor | Particle Balance and Impact of Divertor Closure Including SAS on Detachment Thrust | Osborne | GA | No | Breakout | No | No |
| 79 | what are those modes observed in the wide-pedestal QH edge? | Pedestal Physics and Pedestal Structure & QH Thrust | Chen | GA | No | Breakout | No | No |
| 549 | Further investigation of the saturation & underlying transport mechanism of EHO to allow ELM stable | Pedestal Physics and Pedestal Structure & QH Thrust | Chen | GA | No | Breakout | No | No |
| 550 | What's the physics leads to std QH, Wide Pedestal QH,or ELMing IBS from L-mode at low torque? | Pedestal Physics and Pedestal Structure & QH Thrust | Chen | GA | No | Breakout | No | No |
| 145 | HFS Pellet Fueling Deposition Dynamics in H-mode Plasmas | Pedestal Physics and Pedestal Structure & QH Thrust | Baylor | ORNL | No | Breakout | No | No |
| 146 | Pellet Fueling of Wide Pedestal QH-mode Plasmas | Pedestal Physics and Pedestal Structure & QH Thrust | Baylor | ORNL | No | Breakout | No | No |
| 556 | 168: Extend Zero Torque Wide Pedestal QH-Mode Operation to IBS Parameters | Pedestal Physics and Pedestal Structure & QH Thrust | Ernst | Massachusetts Institute of Technology | No | Breakout | No | No |
| 464 | Effect of impurities on pedestal structure in Peeling and Ballooning dominate discharges. | Pedestal Physics and Pedestal Structure & QH Thrust | Osborne | GA | No | Breakout | No | No |
| 353 | Wide pedestal QH-mode operation at lower Zeff | Pedestal Physics and Pedestal Structure & QH Thrust | Burrell | GA | No | Breakout | No | No |
| 548 | Effect of outer gap on wide-pedestal QH-mode | Pedestal Physics and Pedestal Structure & QH Thrust | Garofalo | GA | No | Breakout | No | No |
| 108 | Measure and control resistive kink mode stability | Pedestal Physics and Pedestal Structure & QH Thrust | Hanson | Columbia U | No | Breakout | No | No |
| 116 | Measuring Te-fluctuations within the pedestal of wide pedestal Quiescent H-mode plasmas | Pedestal Physics and Pedestal Structure & QH Thrust | Houshmandyar | GA | No | Breakout | No | No |
| 518 | Dimensionless scaling of pedestal height, width and stability - a turbulence & transport perspective | Pedestal Physics and Pedestal Structure & QH Thrust | Banerjee | PPPL | No | Breakout | No | No |
| 67 | Unraveling the mechanism linking the pedestal structure and its dynamics to ELM energy densities in ITER relevant regimes | Pedestal Physics and Pedestal Structure & QH Thrust | Diallo | PPPL | No | Breakout | No | No |
| 109 | Effects of the IPD on pedestal structure and edge fluctuations leading to ELM suppressed phases | Pedestal Physics and Pedestal Structure & QH Thrust | Diallo | PPPL | No | Breakout | No | No |
| 196 | ELM cycle: induce at will and find the effect of edge current variation using burst CER/Thomson | Pedestal Physics and Pedestal Structure & QH Thrust | Kolemen | PPPL | No | Breakout | No | No |
| 287 | Validation of the NIMROD results | Pedestal Physics and Pedestal Structure & QH Thrust | Pankin | PPPL | No | Breakout | No | No |
| 140 | Electron density up-down assymetry | Pedestal Physics and Pedestal Structure & QH Thrust | Mordijck | The college of William and Mary | No | Breakout | No | No |
| 48 | Identify and control pedestal turbulence modes in ELMing H-mode plasmas | Pedestal Physics and Pedestal Structure & QH Thrust | Yan | U of Wisconsin | No | Breakout | No | No |
| 302 | Measurement of EHO particle vs energy transport and phase angles with fluctuation diagnostics | Pedestal Physics and Pedestal Structure & QH Thrust | Morton | U of Wisconsin | No | Breakout | No | No |
| 297 | Identifying and Detecting Microtearing Modes within the Pedestal of an H-mode Plasma | Pedestal Physics and Pedestal Structure & QH Thrust | Major | U of Wisconsin | No | Breakout | No | No |
| 387 | Local Magnetic Field Measurements of QH-mode EHO | Pedestal Physics and Pedestal Structure & QH Thrust | Burke | LLNL | No | Breakout | No | No |
| 258 | Deuterium lifecycle during ELM pacing with pellet injection | Pedestal Physics and Pedestal Structure & QH Thrust | Bortolon | PPPL | No | Breakout | No | No |
| 479 | ITG and TEM's impacts on toroidal rotation profile and intrinsic rotation | Rotation physics | Qin | U of Wisconsin | No | Breakout | No | No |
| 150 | Competition Between Intrinsic Torque and NTV for ITER | Rotation physics | Grierson | GA | No | Breakout | No | No |
| 422 | Increase "intrinsic" edge rotation via control of edge stochasticity | Rotation physics | Schmitz | UCLA | No | Breakout | No | No |
| 233 | Carbon flow in plasma crown | SOL Flows | Allen | LLNL | No | Breakout | No | No |
| 213 | Search for SOL impurity stagnation region | SOL Flows | Allen | LLNL | No | Breakout | No | No |
| 249 | ExB drifts and paralel flows in divertor and SOL before/during detachment | SOL Flows | Boedo | UCSD | No | Breakout | No | No |
| 251 | Methane Injection Changing D+ flows in SOL | SOL Flows | Boedo | UCSD | No | Breakout | No | No |
| 247 | ExB drifts and paralel flows in divertor and SOL before/during detachment | SOL Flows | Boedo | UCSD | No | Breakout | No | No |
| 447 | Optimizing Transport Through Magnetic Shear | Steady State Scenarios & High qmin Thrust | McKee | U of Wisconsin | No | Breakout | No | No |
| 189 | Mitigation of AEs in high performance discharges using high off-axis current drive | Steady State Scenarios & High qmin Thrust | Kramer | PPPL | No | Breakout | No | No |
| 265 | High Pedestal in Hybrid Scenario With Unfavorable Grad-B Drift Direction | Steady State Scenarios & High qmin Thrust | Petty | GA | No | Breakout | No | No |
| 336 | Pushing Steady-State Hybrid Scenario to Lower q95, Higher Beta and Higher Fusion Gain | Steady State Scenarios & High qmin Thrust | Petty | GA | No | Breakout | No | Yes |
| 488 | Steady-State Hybrids in Hydrogen With Higher Bootstrap Fraction | Steady State Scenarios & High qmin Thrust | Petty | GA | No | Breakout | No | No |
| 449 | m/n=2/1 NTM control by ECCD in steady state hybrid | Steady State Scenarios & High qmin Thrust | Bardoczi | GA | No | Breakout | No | No |
| 22 | Optimizing of q and fast-ion profiles in high-qmin scenario | Steady State Scenarios & High qmin Thrust | Thome | GA | No | Breakout | No | No |
| 484 | - Feasibility of plasma performance and stability of ITER steady-state operation with NB+EC CD | Steady State Scenarios & High qmin Thrust | Polevoi | ITER Organization | No | Breakout | No | Yes |
| 563 | Probe RWM stability using off-axis NBI | Steady State Scenarios & High qmin Thrust | Hanson | Columbia U | No | Breakout | No | No |
| 431 | Profile control for high qmin steady state scenario | Steady State Scenarios & High qmin Thrust | Wehner | Lehigh | No | Breakout | No | No |
| 432 | Profile control for high qmin steady state scenario | Steady State Scenarios & High qmin Thrust | Wehner | Lehigh | No | Breakout | No | No |
| 433 | Profile control for high qmin steady state scenario | Steady State Scenarios & High qmin Thrust | Wehner | Lehigh | No | Breakout | No | No |
| 20 | Ignition mechanism of arc by ELMs | Surface Evolution | Rohde | Max Planck Institut fuer Plasmaphysiks, Garching, Germany | No | General | No | No |
| 491 | Spectroscopic inference of tungsten re-deposition fractions | Surface Evolution | Abrams | GA | No | Breakout | No | No |
| 460 | Use pellets to enable 2/1 NTM stabilization with very low gyrotron power | Torkil Jensen | Bardoczi | GA | No | Breakout | No | No |
| 8 | ECH Beat Wave Generation of ICE | Torkil Jensen | Grierson | GA | No | General | No | No |
| 542 | LH power threshold, confinement scaling and CER calibration in carbon plasmas | Torkil Jensen | Marinoni | UCSD | No | Breakout | No | No |
| 139 | ITER pedestal turbulence properties | Torkil Jensen | Boedo | UCSD | No | Breakout | No | No |
| 88 | Exploring new reactor concepts: H-mode in negative triangularity diverted plasmas | Turbulence and transport | Marinoni | UCSD | No | Breakout | No | No |
| 399 | Safety Factor Scaling of Turbulence and Transport in Hybrid Scenario Plasmas | Turbulence and transport | McKee | U of Wisconsin | No | Breakout | No | No |
| 194 | Comparing the transport models experimentally | Turbulence and transport | Kolemen | PPPL | No | Breakout | No | No |
| 179 | Model validation of betaN > 3 in negative triangularity DIII-D discharges | Turbulence and transport | Austin | U of Texas, Austin | No | Breakout | No | No |
| 180 | Transport vs rotation in DIII-D negative triangularity discharges | Turbulence and transport | Austin | U of Texas, Austin | No | Breakout | No | No |
| 401 | Determine the critical gradient in negative triangularity discharges | Turbulence and transport | Austin | U of Texas, Austin | No | Breakout | No | No |
| 27 | Dependence of Ohmic energy confinement in negative triangularity diverted plasmas | Turbulence and transport | Thome | GA | No | Breakout | No | No |
| 263 | Impurity temperature screening in ITBs | Turbulence and transport | Sciortino | Max-Planck Institute for Plasma Physics | No | Breakout | No | No |
| 266 | Test of Turbulence Spreading Using Turbulence Propagation | Turbulence and transport | Petty | GA | No | Breakout | No | No |
| 43 | Low and mid-Z impurity density asymmetry | Turbulence and transport | Chrystal | GA | No | Breakout | No | No |