DIII-D RESEARCH OPPORTUNITIES FORUM FOR THE 2015 EXPERIMENTAL CAMPAIGN
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ID | Title | Research Area | Name | Affiliation |
Time Req'ed |
ITPA Joint Exp |
ITER IO Urgent Research Task |
132 | A Study of Ablation for Tungsten-Alternative PFCs Due to ELMs and Hard Disruptions | PMI Physics | ORNL and NCSU | Yes | No | No | |
108 | Active Control of the LH power theshold via n=3 magnetic perturbations | LH Physics | UCLA | Yes | No | No | |
61 | Active Particle Exhaust of H-mode plasmas in the Snowflake Divertor Configuration | SOL and Divertor Physics | GA | No | No | No | |
269 | Active probing of tearing stability | 3D & Stability Physics | Consultant | No | No | No | |
403 | Active probing of tearing stability 2 | 3D & Stability Physics | Retired from GA | No | No | No | |
177 | Actuator Sharing and Integrated Control Demonstration for ITER | Control | ITER Organization | Yes | Yes | Yes | |
339 | Adaptive EFC | Control | PPPL | No | No | No | |
69 | Adaptive ELM Control | ELM Stability & Control | PPPL | No | No | No | |
338 | Adaptive ELM Control | Control | PPPL | No | No | No | |
151 | Adaptive ELM control | Control | GA | No | No | No | |
154 | Adaptive ELM Control with Advanced Divertors | ELM Stability & Control | GA | No | No | No | |
68 | Adaptive Error Field Correction | 3D & Stability Physics | PPPL | Yes | No | No | |
155 | Advanced Divertors with adapative ELM control | SOL and Divertor Physics | GA | No | No | No | |
448 | Advanced tokamak scenarios with metal tiles | Steady State | LLNL | Yes | No | No | |
358 | An attempt to Edge Electro-Magnetic torque injection with feedback | Control | PPPL | No | No | No | |
71 | Analysis of ECH Deposition Profile Broadening through use of MECH. | Heating & Current Drive | GA | No | No | No | |
307 | Analysis of ECH Deposition Profile Broadening through use of MECH. | Turbulence & Transport | U of Texas | No | No | No | |
205 | Another approach to super H-mode? | Pedestal Transport & Control | GA | No | No | No | |
356 | Anti-Miss NTM control | 3D & Stability Physics | EPFL | Yes | Yes | No | |
394 | Applying Phase Space Manipulation of the Beam Ion Distribution to Control MHD and Optimize Beam Heat | Torkil Jensen Award | GA | No | No | No | |
283 | Assess RE suppression in early CQ with less perturbative SPI | Disruption Mitigation | GA | No | No | Yes | |
171 | Assess the destabilization mechanism for the n = 1 tearing mode in steady-state scenario discharges | Steady State | GA | Yes | No | No | |
445 | Assessing Tungsten as a Possible Material for a Future Slot Divertor with High Power AT Plasmas | SOL and Divertor Physics | GA | No | No | No | |
17 | Attaining higher Betan with advanced feedback control and external control coils | 3D & Stability Physics | PPPL | Yes | No | No | |
75 | Automatic phase controller of slowly rotating 2/1 mode (f<200Hz) | 3D & Stability Physics | GA | Yes | No | No | |
253 | Avalanche-triggered LH Transitions | LH Physics | UCLA | No | No | No | |
425 | Beam modulation to measure fast-ion transport by 3D fields | Energetic Particles | UC, Irvine | No | No | No | |
424 | Beam modulation to measure fast-ion transport by tearing modes | Energetic Particles | UC, Irvine | No | No | No | |
168 | Beta limit and bootstrap current fraction in ITER steady-state scenario discharges | Steady State | GA | No | No | No | |
7 | Calibrate the Fast Ion Loss Detector System Using Neutral Beam Prompt Losses | General Physics | GA | No | No | No | |
148 | Calibration of tungsten erosion rate via W gas puffing in the divertor | PMI Physics | GA | No | No | No | |
63 | Can Flux Expansion Help Control Carbon Influx in AT Plasmas at Elevated Power Input in Long Pulse? | Steady State | GA | No | No | No | |
56 | Can Flux Expansion Significantly Lower Heat Flux and Control Carbon Influx in High Power AT Plasmas? | SOL and Divertor Physics | GA | Yes | No | No | |
62 | Can Radiating Divertor Be Effective for AT Plasmas at Elevated Power Input? | Steady State | GA | No | No | No | |
55 | Can Radiating Divertor Be Effective for AT Plasmas at Elevated power input? | SOL and Divertor Physics | GA | Yes | No | No | |
59 | Can the Non-Resonant RMP/Puff and Pump be Effective in Divertor Heat Flux Reduction? | Pedestal Transport & Control | GA | No | No | No | |
114 | Cascaded PID control for detachment | Control | GA | No | No | No | |
113 | Characterization of Detachment in Advanced Divertor Configurations | SOL and Divertor Physics | GA | No | No | No | |
111 | Characterization of detachment with MIMO detachment and radiation profile control | SOL and Divertor Physics | GA | No | No | No | |
153 | Characterization of detachment with variation of bias away from a double null shape | SOL and Divertor Physics | GA | No | No | No | |
196 | Characterization of edge plasma in the case of extinguishing ELMs | SOL and Divertor Physics | CompX | Yes | No | No | |
267 | Characterization of EHO for the improvement of its saturated kink-peeling mode physics basis | EHO Stability & Control | ITER Organization | Yes | No | Yes | |
246 | Characterization of final VDE during current quench following massive particle injection | Disruption Mitigation | ORNL | No | No | No | |
152 | Characterization of marginally suppressed plasmas using adaptive ELM control | ELM Stability & Control | GA | No | No | No | |
143 | Characterization of QCFs via parity | Pedestal Transport & Control | PPPL | No | No | No | |
8 | Characterize Energetic Ion Losses as Measured by the Rippled Tile Diagnostic | Energetic Particles | GA | No | No | No | |
302 | Characterize heat load at injection port for SPI | Disruption Mitigation | ORNL | No | No | Yes | |
30 | Clarify snowflake divertor physics | SOL and Divertor Physics | LLNL | No | No | No | |
320 | Closed-loop MHD spectroscopy combined with EF correction | Control | Consultant | No | No | No | |
126 | Co-injected Super H-Mode Physics Exploration | Pedestal Transport & Control | ORNL | Yes | No | No | |
413 | Collection of core W impurities at the OMP due to W shell pellets: A dry-run | PMI Physics | ORNL | Yes | No | No | |
40 | Collisionality-dependence of plasma response in low-torque ITER baseline | 3D & Stability Physics | Columbia U | Yes | No | No | |
311 | Collsionality scaling in AI plasmas at q95~5 | Turbulence & Transport | U of Wisconsin | No | No | No | |
357 | Combined sawtooth control and NTM preemption | Control | EPFL | Yes | Yes | No | |
88 | Comparing upper and lower divertors to measure the effect of closure on detachment | SOL and Divertor Physics | GA | Yes | No | No | |
26 | Comparison of non-dimensionally similar ITER baseline plasmas | Inductive Scenarios | Columbia U | No | No | No | |
372 | Comparison of the effects of ELM pellet pacing and RMP ELM mitigation on divertor conditions | SOL and Divertor Physics | ORNL | No | No | No | |
238 | Comparison of transport & microturbulence levels in positive & negative triangularity discharges | Turbulence & Transport | U of Texas, Austin | No | No | No | |
443 | Comparison the main ion and impurity flow at high-field side | SOL and Divertor Physics | GA | Yes | No | No | |
260 | Compatibility of pellet fuelling with ELM suppression with I coils. | Pedestal Transport & Control | ITER Organization | Yes | No | Yes | |
239 | Competition between NBI unlocking and ECCD stabilization of locked modes | 3D & Stability Physics | Columbia U | No | No | No | |
377 | Confinement Impacts of Impurity-seeding of H-mode plasmas | Turbulence & Transport | U of Wisconsin | No | No | No | |
78 | Continuos High Pressure Pedestal with Lithium and Pedestal Control | Pedestal Transport & Control | PPPL | Yes | No | No | |
203 | Control EP transport in high qmin steady-state plasmas using central ECH | Steady State | GA | No | Yes | No | |
204 | Control EP transport in high qmin steady-state plasmas using central ECH | Energetic Particles | GA | No | Yes | No | |
398 | Control needs for the D3D divertor upgrade | Control | GA | No | No | No | |
197 | Control of (grad-T_e-driven) TEM in low collisionality QH-mode plasmas | Turbulence & Transport | UCLA | No | No | No | |
112 | Control of Detachment in Advanced Divertor Configurations | Control | GA | Yes | No | No | |
392 | Control of Major Disruptions in DIII-D / ITER | Control | Columbia U | No | No | No | |
94 | Control of n=1 Tearing Modes using Off-axis Broad ECCD in Steady State Discharges with qmin > 1.5 | Steady State | Retired | Yes | No | No | |
395 | Control of the radiation profile with multi-species puffing | Inductive Scenarios | GA | No | No | No | |
388 | Control of tungsten surface erosion by in-situ low-Z coatings | PMI Physics | UCSD | No | No | No | |
354 | Control/Ops Evening Development Time | Control | GA | No | No | No | |
376 | Controlled injection of high-Z impurities in DIII-D using DiMES | PMI Physics | UCSD | No | No | No | |
227 | Core and edge particle transport and sources | Turbulence & Transport | VTT Technical Research Centre | No | Yes | Yes | |
212 | Core momentum transport validation: Magnetic shear | Turbulence & Transport | GA | Yes | No | No | |
142 | Core Optimization of Advanced Inductive Scenario with Strong Electron Heating | Turbulence & Transport | Massachusetts Institute of Technology | Yes | No | No | |
401 | Core transport model validation in high-betaP, low-torque, steady-state plasmas | Steady State | UCSD | No | No | No | |
125 | Coupled High Performance DivSOL & Pedestal | Integrated Modeling | ORNL | Yes | No | No | |
359 | coupling of rotating magnetic islands | 3D & Stability Physics | Los Alamos National Laboratory | No | No | No | |
195 | Current Drive Measurements with 1 MW Helicon System (FY16) | Heating & Current Drive | GA | Yes | No | No | |
244 | D2 pellet pacing of ELMs in the low-torque ITER baseline | ELM Stability & Control | ORNL | No | No | No | |
370 | D3d/EAST Joint Exp. on Extending Noninductive Scenario to Higher Beta and Testing Lower NBI Torque | Steady State | ASIPP | No | No | No | |
102 | DELETED | 3D & Stability Physics | Department of Energy | No | No | No | |
262 | Demonstration of integrated ELM-paced pellet fuelled H-mode plasma in ITER-relevant range | Pedestal Transport & Control | ITER Organization | Yes | Yes | Yes | |
60 | Density Control and Active Impurity Removal from Double-null H-mode Plasmas | SOL and Divertor Physics | GA | No | No | No | |
165 | Dependence of confinement and stability on toroidal rotation in high li discharges | Steady State | GA | No | No | No | |
149 | Detached divertor with Super H-mode pedestal | SOL and Divertor Physics | GA | No | No | No | |
19 | Detachment Characteristics in H-mode Helium Plasmas | SOL and Divertor Physics | ORNL | Yes | No | No | |
446 | Detachment thresholds vs. divertor geometry | SOL and Divertor Physics | GA | No | No | No | |
407 | Detachment with strike point on metal tiles | SOL and Divertor Physics | GA | No | No | No | |
409 | Detachment with strike point on metal tiles | PMI Physics | GA | No | No | No | |
190 | Detection of magnetic islands and Coalescence Instability in RMP ELM suppression | ELM Stability & Control | GA | Yes | Yes | Yes | |
298 | Determination of Runaway Electron Parameters by Measurement of Synchrotron Emission Polarization | Disruption Mitigation | UCSD | No | No | No | |
345 | Determine density scaling of confinement in QH-mode | Inductive Scenarios | GA | No | No | No | |
290 | Develop and benchmark technique to measure ELM-induced peak heat flux in pumped LSN discharges | ELM Stability & Control | UCSD | No | No | No | |
130 | Develop and optimize ELM paced super H-mode | Pedestal Transport & Control | PPPL | No | No | No | |
360 | Develop feedback-controlled 3D equilibria | 3D & Stability Physics | Columbia U | No | No | No | |
110 | Develop MIMO algorithm for detachment and radiation profile control | Control | GA | Yes | No | No | |
84 | Developing ITER Locking avoidance by EM torque control by comparing NSTX/DIID(C-coil)/RFX-mod | 3D & Stability Physics | PPPL | Yes | No | No | |
133 | Development of Eroding Surface Thermocouples for In-Tile Measurements of Surface Heat Flux | PMI Physics | Sandia National Laboratories | No | No | No | |
48 | Development of Rotation Profile Feedback Control Capability | Control | Lehigh U | Yes | No | No | |
23 | Diagnosis of n=1 structures during n>1 RMP-ELM suppression | ELM Stability & Control | Columbia U | No | No | No | |
436 | Differential rotation driven by 3-wave coupling | 3D & Stability Physics | Los Alamos National Laboratory | No | Yes | No | |
371 | DIII-D/EAST joint experiment on extending qmin>2 inductive scenario to lower torque and higher Ip | Inductive Scenarios | GA | No | No | No | |
286 | DiMES and MiMES exposure of solute enforced tungsten | PMI Physics | U of Wisconsin | No | No | No | |
361 | DiMES tests of high-Z metal coatings for DIII-D tiles | PMI Physics | UCSD | No | No | No | |
27 | Direct measurement of C-coil n=1 sideband during n=3 NRMF | 3D & Stability Physics | Columbia U | No | No | No | |
35 | Direct measurement of multi-mode kinetic plasma response using Nyquist Analysis | 3D & Stability Physics | PPPL | Yes | Yes | No | |
36 | Direct measurement of multi-mode kinetic plasma response using Nyquist Analysis | 3D & Stability Physics | PPPL | Yes | Yes | No | |
9 | Directed Phase Space Manipulation to Control Alfv Ì?en Eigenmode Chirping | Energetic Particles | GA | No | Yes | No | |
145 | Disruption avoidance control using DCON real time stability analysis | Control | GA | No | No | No | |
90 | Disruption mitigation via Real-time LGI control | Disruption Mitigation | PPPL | Yes | No | No | |
340 | Disruption mitigation via Real-time LGI control | Control | PPPL | No | No | No | |
273 | Disruption mitigation with large shell pellet | Disruption Mitigation | UCSD | No | No | Yes | |
285 | Disruption mitigation with Li shell pellet | Disruption Mitigation | UCSD | No | No | No | |
317 | Disruption mitigation with x-point pre-puff | Disruption Mitigation | UCSD | No | No | Yes | |
353 | Disruptions, Exponentially Growing Islands and the Radiative Island Growth | 3D & Stability Physics | PPPL | No | No | No | |
121 | Disruptive 2/1 island width vs. q95 | 3D & Stability Physics | Massachusetts Institute of Technology | Yes | No | No | |
442 | Divertor closure on impurity seeding detachment | SOL and Divertor Physics | GA | Yes | No | No | |
418 | Divertor Detachment Dynamics | SOL and Divertor Physics | VTT Technical Research Centre | No | No | No | |
175 | Divertor ExB mapping attached./detached | SOL and Divertor Physics | UCSD | No | No | No | |
431 | Divertor heat flux modulation during RMP ELM suppression | ELM Stability & Control | GA | No | Yes | Yes | |
387 | Dust re-mobilization studies using DiMES | PMI Physics | UCSD | No | No | No | |
80 | EC Current Drive Physics | Heating & Current Drive | PPPL | No | No | No | |
352 | EC Current Drive Physics | 3D & Stability Physics | PPPL | No | No | No | |
347 | EC Current Drive Physics | 3D & Stability Physics | PPPL | No | No | No | |
51 | ECCD control of 3/2 NTM in low rotation IBS to avoid locking | 3D & Stability Physics | Retired from GA | No | No | No | |
393 | Edge neutral density through spectroscopy | General Physics | UC, Irvine | No | No | No | |
327 | Edge particle transport and turbulence investigations in different phases of n=3 RMP | ELM Stability & Control | UCLA | No | No | No | |
174 | Edge poloidal rotation physics | Pedestal Transport & Control | ORAU | No | No | No | |
362 | Effect of biasing on high-Z material erosion | PMI Physics | UCSD | No | No | No | |
385 | Effect of electric biasing on arcing | PMI Physics | UCSD | No | No | No | |
319 | Effect of external torque variations on the turbulence-GAM interaction, and gyrokinetic analysis | Turbulence & Transport | KAIST | No | No | No | |
170 | Effect of Fast Ion Loss on L-H Transition | LH Physics | GA | No | No | No | |
363 | Effect of gas pressure on RE plateau mitigation | Disruption Mitigation | GA | No | No | Yes | |
216 | Effect of impurities and wall conditioning on NTMs | 3D & Stability Physics | Columbia U | No | No | No | |
180 | Effect of Impurities on momentum transport in IBS plasmas | Inductive Scenarios | Columbia U | No | No | No | |
306 | Effect of impurity species on runaway dissipation | Disruption Mitigation | ORNL | No | No | Yes | |
247 | Effect of low order rational surfaces on MHD activity during SPI shutdown | Disruption Mitigation | ORNL | No | No | No | |
178 | Effect of low-Z impurity on pedestal and global confinement | Pedestal Transport & Control | U of York | Yes | Yes | No | |
404 | Effect of metal test tiles on confinement and turbulence | Integrated Modeling | UCLA | No | No | No | |
405 | Effect of metal test tiles on confinement and turbulence - duplicate of one submitted to BPMIC | Turbulence & Transport | UCLA | No | No | No | |
303 | Effect of MHD on radiation asymmetries during SPI injection | Disruption Mitigation | ORNL | No | No | Yes | |
14 | Effect of pre-existing MHD activity on shattered pellet injection | Disruption Mitigation | ORNL | No | No | Yes | |
245 | Effect of the ablation path length on SPI shutdown | Disruption Mitigation | ORNL | No | No | Yes | |
375 | Effect on SEE on Langmuir probe measurements in the SOL | PMI Physics | UCSD | No | No | No | |
201 | Effects of magnetic islands on ECCD | Heating & Current Drive | GA | No | No | No | |
206 | Effects of magnetic islands on ECCD | 3D & Stability Physics | GA | No | No | No | |
33 | Electromagnetic turbulence effects at high beta | Turbulence & Transport | CCFE | Yes | No | No | |
81 | Electromagnetic fluctuations and transport during ELM cycles and comparison to theory and simulation | Pedestal Transport & Control | UCLA | Yes | No | No | |
73 | Electron Critical Gradient in H-mode | Turbulence & Transport | GA | No | No | No | |
183 | ELM control by impurity injection | SOL and Divertor Physics | UCSD | No | No | No | |
176 | ELM D and C backflow | PMI Physics | UCSD | No | No | No | |
210 | ELM pacing by modulating RMPs at optimal q95, or modulating q95 with RMPs on | ELM Stability & Control | Columbia U | No | No | No | |
198 | ELM suppressed steady state hybrid plasmas | Steady State | GA | Yes | No | No | |
85 | ELM suppression exploration with n=1 RMP | ELM Stability & Control | PPPL | Yes | No | No | |
428 | ELM Suppression for Investigating Flux Pumping in hybrids | ELM Stability & Control | Oak Ridge Associated Universities | No | No | No | |
199 | ELM Suppression in Low rotation Deuterium Plasmas | ELM Stability & Control | GA | No | No | Yes | |
228 | ELM Suppression with Advanced Divertors | ELM Stability & Control | GA | No | No | No | |
6 | Energetic Ion Interactions with Microturbulence | Energetic Particles | GA | No | No | No | |
292 | Error field correction at rational surface by measurement of shielding currents â?? ECCD actuator | 3D & Stability Physics | Massachusetts Institute of Technology | No | No | No | |
374 | Error field correction by measurement of shielding currents â?? rigid body vertical oscillations | 3D & Stability Physics | Massachusetts Institute of Technology | No | No | No | |
106 | Error field correction through alignment of drift precession profile with omega_E | 3D & Stability Physics | Department of Energy | No | No | No | |
169 | Establish the incremental confinement of EC power in high betaN steady-state scenario discharges | Steady State | GA | No | No | No | |
92 | Evaluate Prospect for ITB in high q-min Steady Scenarios for FNSF | Steady State | Retired | Yes | No | No | |
129 | Explore Impurity Pellet Induced L-H transitions | LH Physics | PPPL | No | No | No | |
200 | Exploring Fast-Ion Critical Gradient Threshold Using ECH | Energetic Particles | ORNL | Yes | No | No | |
128 | Exploring new materials for impurity pellet pacing of ELMs in reactor relevant environment | ELM Stability & Control | PPPL | Yes | No | No | |
44 | Extend performance of qmin > 2 AT scenario by optimizing MHD stability | 3D & Stability Physics | Columbia U | Yes | No | No | |
45 | Extend performance of qmin > 2 AT scenario by optimizing MHD stability | Steady State | Columbia U | No | No | No | |
373 | Extend the ELM free phase with Li on DIIID while linking to the similar phenomenon on EAST | Pedestal Transport & Control | GA | No | No | No | |
382 | Extending DIII-Dâ??s operating window to achieve divertor conditions predicted for burning AT tokamaks | SOL and Divertor Physics | U of Toronto | No | No | No | |
344 | Extension of Super H-mode pedestal into co-injected plasma | Pedestal Transport & Control | GA | No | No | No | |
366 | Far SOL fluxes and link to detachment | SOL and Divertor Physics | UCSD | No | No | Yes | |
280 | Fast entrainment by sub-harmonic kicks | 3D & Stability Physics | Columbia U | No | No | No | |
232 | Fast Er profile changes at the onset of ELM suppression | ELM Stability & Control | GA | No | No | Yes | |
300 | Fast Imaging of Visible Brehmsstrahlung for impurity transport and Zeff | Pedestal Transport & Control | UCSD | No | No | No | |
123 | Fast partial Ip ramp-down to avoid locked mode disruption | 3D & Stability Physics | Massachusetts Institute of Technology | Yes | No | No | |
122 | Feedback control of detachment using bolometry inversion | Control | GA | No | No | No | |
420 | Find a better parameter space for the ITER Baseline Scenario | Inductive Scenarios | Columbia U | No | No | No | |
421 | Find a better parameter space for the ITER Baseline Scenario | 3D & Stability Physics | Columbia U | No | No | No | |
378 | Fine scale stepwise q-scan: role of low-order rationales and resonance condition for ELM suppression | ELM Stability & Control | U of Wisconsin | No | No | No | |
18 | Flow or flow shear for m/n=3/2 tearing mode stability? | 3D & Stability Physics | Retired from GA | Yes | No | No | |
193 | Fluctuation measurements in MECH limiter H-modes with RMP fields | ELM Stability & Control | GA | No | No | Yes | |
109 | Fuel Ion Mass (Isotope) Scaling of Turbulence and Transport | Turbulence & Transport | U of Wisconsin | Yes | No | No | |
189 | Fully non-inductive current overdrive prospects for ST | Integrated Modeling | PPPL | Yes | No | No | |
297 | Further development of Catch & Subdue | Control | GA | No | No | No | |
235 | Further development of QH-mode with strong co-Ip NBI torque | Inductive Scenarios | GA | No | No | No | |
449 | Further investigation of the QH with high&wide pedestal and how EHO behaves in this new regime | Pedestal Transport & Control | GA | No | No | No | |
450 | Further investigation of the QH with high&wide pedestal and how EHO behaves in this new regime | EHO Stability & Control | GA | No | No | No | |
219 | Further XD investigations on DIIID | SOL and Divertor Physics | university of texas | Yes | No | No | |
412 | FY2016 ROF Proposals Update Test | General Physics | LLNL | No | No | No | |
160 | GPU based RWM feedback control algorithm development(Thursday evening control development) | 3D & Stability Physics | PPPL | No | No | No | |
325 | GPU based RWM feedback control algorithm development(Thursday evening control development) | Control | UCSD | No | No | No | |
429 | H-mode spectroscopic studies of the erosion of W coatings in forward BT | PMI Physics | GA | No | No | No | |
301 | Hardware test of second SPI | Disruption Mitigation | ORNL | No | No | No | |
79 | Helicon stabilization of 2/1 rotating or locked modes | 3D & Stability Physics | GA | Yes | No | No | |
444 | Helium scenarios for ITER | Inductive Scenarios | ITER Organization | No | Yes | Yes | |
252 | HFS shaping for ELM suppression | ELM Stability & Control | PPPL | Yes | No | No | |
400 | High beta_pol plasmas with enhanced pedestal temperature | Steady State | UCLA | No | No | No | |
136 | High fusion yield QH-Mode core based on validated predictive simulations | Turbulence & Transport | Massachusetts Institute of Technology | Yes | No | No | |
164 | High li, maximum betaN at reduced q95 (< 7) | Steady State | GA | No | No | No | |
131 | High Z impurity transport during ELM pacing by impurity pellet injection | Turbulence & Transport | PPPL | No | No | No | |
185 | High-power helicon antenna characterization (FY16) | Heating & Current Drive | GA | Yes | No | No | |
137 | High-power modulated ECRH during QH mode to Assess Transport and ECCD Efficiency | Turbulence & Transport | U of Texas | Yes | No | No | |
147 | High-temperature W morphology changes in the divertor during intense He plasma bombardment | PMI Physics | GA | Yes | No | No | |
38 | Higher betaN, lower torque SS-hybrids | Steady State | Columbia U | Yes | No | No | |
256 | How NTMs affect edge turbulence and transport | Turbulence & Transport | The college of William and Mary | No | No | No | |
76 | Hybrids with co-NBI QH-mode edge | Inductive Scenarios | GA | No | No | No | |
118 | I-mode plasmas as a tool to study basic turbulence and the H-mode transition | LH Physics | UCSD | Yes | No | No | |
255 | IBS low torque disruption avoidance through modified sawtooth stability | 3D & Stability Physics | Department of Energy | No | No | Yes | |
390 | Ideal wall betaN stability dependency on edge pedestal | Steady State | ORNL | No | No | No | |
120 | Identification of culprits behind core/pedestal degradation associated with divertor detachment | SOL and Divertor Physics | GA | No | No | No | |
214 | Impact of 3D field perturbations on main-ion rotation | Pedestal Transport & Control | GA | Yes | No | No | |
323 | Impact of Edge Harmonic Oscillations (EHO) on turbulence | EHO Stability & Control | National Institute for Fusion Science, Japan | No | No | No | |
432 | Impact of impurities and detachment on AT plasmas | Steady State | GA | No | No | No | |
312 | Impact of plasma parameter on SPI performance | Disruption Mitigation | ITER Organization | No | No | Yes | |
284 | Implement finite-state Off Normal Fault Response system | Control | GA | No | No | No | |
336 | Implement finite-state Off Normal Fault Response system | Control | GA | No | No | No | |
96 | improved ITER performance due to fueling | Turbulence & Transport | GA | No | Yes | Yes | |
34 | Influence of plasma shape on ELM suppression at low collisionality | ELM Stability & Control | CCFE | No | Yes | No | |
437 | Informed pre-emptive RF to maintain sheared flow and suppress tearing | 3D & Stability Physics | Los Alamos National Laboratory | No | Yes | No | |
438 | Informed pre-emptive RF to maintain sheared flow and suppress tearing | 3D & Stability Physics | Los Alamos National Laboratory | No | Yes | No | |
331 | Inner/Outer ELM Divertor Energy Deposition Comparison | SOL and Divertor Physics | AKIMA Infrastructure Services | No | No | Yes | |
342 | Integrate QH-mode edge into low torque AI scenario with NRMF | Inductive Scenarios | GA | No | No | No | |
47 | Integrated Current Profile and Beta Control for Development and Sustainment of Advanced Scenarios | Control | Lehigh U | Yes | No | No | |
215 | Integrated Disruption Control | 3D & Stability Physics | Columbia U | No | No | No | |
15 | Interaction of neon shattered pellets with post-disruption runaway electron plateaus | Disruption Mitigation | ORNL | No | No | Yes | |
134 | Interaction of NTM and broadband turbulence: experiment and comparison to theory | Turbulence & Transport | UCLA | Yes | No | No | |
42 | Intrinsic pedestal rotation in hydrogen plasmas | Pedestal Transport & Control | PPPL | Yes | No | No | |
66 | Investigate and optimize spontaneous pedestal improvement in low rotation QH-mode | EHO Stability & Control | GA | Yes | No | No | |
236 | Investigate angular momentum diffusion and pinch using off-axis torque | Turbulence & Transport | GA | No | No | No | |
234 | Investigate in-out density asymmetry at large toroidal rotation | Turbulence & Transport | GA | No | No | No | |
427 | Investigating Flux Pumping with ELM Suppression in hybrids | Steady State | Oak Ridge Associated Universities | No | No | No | |
97 | Investigating Magnetic Flux Pumping in Hybrid Scenarios | Inductive Scenarios | Oak Ridge Associated Universities | Yes | No | No | |
3 | Investigation of AE Critical Gradient Energetic Ion Transport through Adjustment of Phase Space Grad | Energetic Particles | GA | No | No | No | |
11 | Inward pinch vs neutral fueling | Turbulence & Transport | The college of William and Mary | No | Yes | Yes | |
268 | Ion Cyclotron Driven Pedestal Relaxation | Torkil Jensen Award | GA | Yes | No | No | |
229 | Is the plasma response to external 3D fields large in the core of SS hybrids? | Steady State | Consorzio RFX | No | No | No | |
230 | Is the plasma response to external 3D fields large in the core of SS hybrids? | 3D & Stability Physics | Consorzio RFX | No | No | No | |
95 | Island seeding with saw teeth pacing: New method to control tearing modes | 3D & Stability Physics | PPPL | No | No | No | |
57 | ITER Baseline Scenario in a Radiating Divertor Environment with near-Zero Applied Torque | Inductive Scenarios | GA | No | No | No | |
441 | ITER Baseline Scenario Radiative Divertor Demonstration | Inductive Scenarios | ITER Organization | No | Yes | No | |
364 | ITER NTM Control Under Radiative Island Growth | 3D & Stability Physics | PPPL | No | No | No | |
389 | ITER steady-state scenario in USN, +BT | Steady State | ORNL | No | No | No | |
50 | Kink and tearing stability in low rotation qmin~1.5 scenario using n=2 NTV | Steady State | Department of Energy | Yes | No | No | |
217 | LIBP to probe plasma response to 3D field | Energetic Particles | GA | No | No | No | |
224 | Locked mode "catch & subdue" for recovery of pre-locking performance | 3D & Stability Physics | Columbia U | Yes | No | No | |
25 | Long-pulse stability of low torque ITER baseline plasmas | Inductive Scenarios | Columbia U | No | No | No | |
192 | Low torque Li-induced enhanced pedestal for ITER | Pedestal Transport & Control | GA | No | No | No | |
221 | Low-tech "controlled locking" (and automatic locked mode suppression by automated NTM control) | 3D & Stability Physics | Columbia U | Yes | No | No | |
220 | Low-tech locking avoidance by rotating fields, and measure of their impact on confinement and Q | 3D & Stability Physics | Columbia U | Yes | No | No | |
49 | m/n=2/1 NTM Control by ECCD in IBS | 3D & Stability Physics | Retired from GA | Yes | No | No | |
324 | Magnetic & density turbulence of EHO-broadband transitions, comparison to EPED and gyrokinetics | EHO Stability & Control | UCLA | No | No | No | |
293 | Magnetic measurement of error field induced shielding currents by plasma geometry oscillations | 3D & Stability Physics | Columbia U | No | No | No | |
365 | Magnetic ripple effects on particle transport from the comparison between tokamak and helical device | Turbulence & Transport | National Institute for Fusion Science, Japan | No | No | No | |
213 | Main-ion particle transport in the H-mode pedestal | Pedestal Transport & Control | GA | Yes | No | No | |
379 | Map the maximum performance of the low-torque ITER-similar discharges as a function of stability | 3D & Stability Physics | Columbia U | No | No | No | |
380 | Map the maximum performance of the low-torque ITER-similar discharges as a function of stability | Inductive Scenarios | Columbia U | No | No | No | |
435 | Maximizing NBI torque shear | 3D & Stability Physics | Los Alamos National Laboratory | No | Yes | No | |
10 | Measure counter streaming 3D flows | SOL and Divertor Physics | U of Wisconsin | Yes | No | No | |
29 | Measure edge/core turbulence and model transport in Helium plasmas | Turbulence & Transport | Massachusetts Institute of Technology | No | No | No | |
161 | Measure Intrinsic Rotation Size scaling in DIII-D alone -III | Turbulence & Transport | GA | No | No | No | |
222 | Measure island moment of inertia | 3D & Stability Physics | Columbia U | Yes | No | No | |
241 | Measure NTV torque profile | 3D & Stability Physics | Columbia U | No | No | No | |
242 | Measure NTV torque profile | General Physics | Columbia U | No | No | No | |
282 | Measure poloidal asymmetry of SPI injection | Disruption Mitigation | GA | No | No | Yes | |
72 | Measurement of Inductive Poloidal Current | 3D & Stability Physics | GA | No | No | No | |
383 | Measurements of TQ impurity transport during mitigated disruptions | Disruption Mitigation | ORNL | No | No | Yes | |
20 | Measuring Divertor Impurity Ion Temperature as a Function of Density and Heating Power | SOL and Divertor Physics | ORNL | Yes | No | No | |
434 | Measuring net W erosion and transport via disruptions on DiMES | PMI Physics | GA | No | No | No | |
410 | Metallic impurity accumulation (due to tiles) differences in ELMing / ELM suppressed plasmas | Turbulence & Transport | GA | No | No | No | |
411 | Metallic impurity accumulation (due to tiles) differences in ELMing / ELM suppressed plasmas | PMI Physics | GA | No | No | No | |
158 | Midplane Impurity Density Asymmetry | Turbulence & Transport | ORAU | Yes | No | No | |
191 | Mitigate the VH-mode X-event | Steady State | GA | No | No | No | |
426 | Mitigation of AEs in high performance discharges | Steady State | PPPL | No | No | No | |
381 | Model-Predictive Control of Magnetic/Kinetic Profiles using fast data-driven models and observers. | Control | Cadarache | No | Yes | No | |
257 | Modify ITER baseline scenario shape to increase outer gap | Inductive Scenarios | Columbia U | No | No | No | |
275 | Modulate NBI for NTM probing | 3D & Stability Physics | Columbia U | No | No | No | |
77 | Modulated ECCD stabilization of rotating 2/1 islands with phase control by RMP | 3D & Stability Physics | GA | Yes | No | No | |
417 | Modulated ECH For Transport Analysis in the He Campaign | Turbulence & Transport | GA | No | No | No | |
32 | Momentum transport and intrinsic torque under electron heating; Te/Ti~1 | Turbulence & Transport | JAEA | Yes | No | No | |
65 | Multi-machine studies of the L-H power threshold dependence on aspect ratio | LH Physics | U of Wisconsin | Yes | No | No | |
330 | Multi-Mode n=3 Response | 3D & Stability Physics | PPPL | No | No | No | |
281 | Multi-n EFC by rotating fields and modes | 3D & Stability Physics | Columbia U | No | No | No | |
211 | Multi-Z Impurity Transport in Regimes without ELMs | Pedestal Transport & Control | GA | Yes | No | No | |
146 | Multiple mode phasing shifts with rotating n=1,2,3 fields to access low q95 | 3D & Stability Physics | Department of Energy | No | No | No | |
67 | Multiple periods of NTM suppression | 3D & Stability Physics | PPPL | Yes | No | No | |
351 | Multiple periods of NTM suppression | Control | PPPL | No | No | No | |
208 | Mutual alignment of gyrotrons by mirror-steering and anti-phase modulation | Heating & Current Drive | Columbia U | No | No | No | |
101 | n = 1 ELM suppression access through n=2 RMP | 3D & Stability Physics | Department of Energy | No | No | No | |
64 | n=2 error field correction of TBM-like error fields | 3D & Stability Physics | Department of Energy | No | No | No | |
369 | n>1 Island Formation | 3D & Stability Physics | ORNL | No | No | No | |
124 | NBI torque assisted unlocking and spinup experiments | 3D & Stability Physics | Massachusetts Institute of Technology | No | No | No | |
24 | Neoclassical origin of density pumpout | Pedestal Transport & Control | Columbia U | No | No | No | |
187 | Net wall pumping in Helium vs. Deuterium H-mode discharges | PMI Physics | CompX | Yes | No | No | |
225 | Neutral Beam Model Validation | Heating & Current Drive | GA | No | No | No | |
194 | Neutral Effects on Turbulence in Edge & Pedestal Region | Turbulence & Transport | U of Wisconsin | No | No | No | |
334 | Nonlinear Burn Control Demonstration in ITER-relevant Conditions | Control | Lehigh U | No | No | No | |
82 | NTM locking avoidance, magnetic island removal and H-mode recovery by spinig-up assisted by ECCD | 3D & Stability Physics | PPPL | Yes | No | No | |
259 | NTMs â??on demandâ?? | 3D & Stability Physics | Columbia U | No | No | No | |
447 | Observation of Kinetic Ballooning Modes in H-Mode Inner Core | Turbulence & Transport | Massachusetts Institute of Technology | No | No | No | |
251 | Off-Axis ECCD in Steady-State Hybrids | Steady State | GA | No | No | No | |
157 | Off-axis NBCD study based on similarity experiments in DIII-D and ASDEX Upgrade | Heating & Current Drive | U of Wisconsin | No | No | No | |
83 | Optimal Plasma Shape for High-Beta, Steady-State Hybrid Scenario | Steady State | GA | No | No | No | |
5 | Optimization of Counter-current Beam Heating in Steady State Scenarios | Steady State | GA | Yes | No | No | |
309 | Optimization of runaway electron diagnostic coverage | Disruption Mitigation | Columbia U | No | No | No | |
13 | Optimize & test robustness of qmin>1.5, fNI=1 scenario | Steady State | LLNL | No | No | No | |
289 | Optimize RMP ELM control in low torque ITER Baseline at high collisionality | Inductive Scenarios | UCSD | No | No | Yes | |
93 | Optimizing ITER Steady State Scenarios with High-qmin (qmin > 1.5) | Steady State | Retired | No | Yes | No | |
31 | Optimizing magnetic and rotation shears to mitigate confinement degradation with increasing Te/Ti | Turbulence & Transport | JAEA | No | No | No | |
261 | Optimum pellet injection geometry for pellet triggering with minimum throughput/PFC power fluxes | Pedestal Transport & Control | ITER Organization | Yes | No | Yes | |
315 | Origin of runaway electron cutoff energy | Disruption Mitigation | UCSD | No | No | No | |
22 | Orthogonal plasma response from ex-vessel coil in ITER baseline scenario | 3D & Stability Physics | Columbia U | No | No | No | |
343 | Pedestal Control | Control | PPPL | No | No | No | |
264 | Pedestal particle transport in ELM suppressed H-modes on medium/high Z impurities and optimization | Pedestal Transport & Control | ITER Organization | Yes | No | Yes | |
266 | Pedestal particle transport mechanisms for high density plasmas with low core neutral source | Pedestal Transport & Control | ITER Organization | Yes | Yes | Yes | |
89 | Pedestal Pressure Adjustment and ELM Regularization via Real-time LGI control | ELM Stability & Control | PPPL | Yes | No | No | |
104 | Pedestal stability at low collisionality | Pedestal Transport & Control | UCLA | No | No | No | |
41 | Pedestal transport studies in matched hydrogen and deuterium discharges | Pedestal Transport & Control | PPPL | Yes | No | No | |
271 | Pellet ELM Pacing in the Low-Torque ITER Scenario | ELM Stability & Control | ORNL | No | No | Yes | |
248 | Pellet pacing with true 0.9mmx1.9mm D2 pellets | ELM Stability & Control | ORNL | No | No | Yes | |
316 | Penetration of electric field into runaway plateau | Disruption Mitigation | UCSD | No | No | No | |
99 | Performance Enhancement via qmin control | Steady State | PPPL | No | No | No | |
91 | Physics behind the low density branch of the LH power threshold scaling | LH Physics | UCLA | Yes | No | No | |
329 | Physics of 3D field perturbation on EHO and edge density profile flattening | EHO Stability & Control | UCLA | No | No | No | |
384 | Physics of leading edge power loading in support of ITER divertor design | PMI Physics | UCSD | No | Yes | Yes | |
159 | Piggy-back measurements of helicon antenna loading | Heating & Current Drive | GA | Yes | No | No | |
209 | Poloidal rotation of plasma column to simulate rotating wall | 3D & Stability Physics | Columbia U | No | No | No | |
279 | Poloidal torque injection by off-axis NBI, and its effect on tearing mode physics | 3D & Stability Physics | Columbia U | No | No | No | |
226 | Power Dependence of the Near Edge Transport Shortfall During the L- and H-mode Phases | Turbulence & Transport | CompX | No | No | No | |
21 | Probability of soft landing success in ITER baseline | 3D & Stability Physics | Columbia U | No | No | No | |
28 | Probe role of ETG turbulence, TEM turbulence, and non-local transport in LOC/SOC transition | Turbulence & Transport | Massachusetts Institute of Technology | No | No | No | |
231 | Probing flux pumping mechanisms in SS hybrids using the plasma response to external 3D fields | Steady State | Consorzio RFX | No | No | No | |
167 | Produce fNI = 1 discharges at q_min near 1.5 using off-axis injection with varying toroidal rotation | Steady State | GA | Yes | No | No | |
233 | Prompt torque and zonal flow damping | Turbulence & Transport | GA | No | No | No | |
287 | Prong 3 approach to ELM Control in ITER Baseline Scenario (low torque) | ELM Stability & Control | UCSD | No | No | Yes | |
2 | Propensity for Detrimental Modes Driven by Energetic Electrons as ECH Power Increases | Heating & Current Drive | GA | No | No | No | |
310 | q95 scaling of the coupled turbulence/zonal flow during LH transition | LH Physics | U of Wisconsin | No | No | No | |
265 | QH-mode compatibility with pellet fuelling, radiative divertor and beta Pinput/PL-H | EHO Stability & Control | ITER Organization | Yes | No | Yes | |
341 | qmin control | Control | PPPL | No | No | No | |
321 | Quantification of model predictive control of flux diffusion | Control | Consultant | No | No | No | |
422 | Quantifying deuterium retention in W-coated regions of the divertor after the metal tile experiment | PMI Physics | GA | No | No | No | |
240 | Quasi-stationary Modes (QSMs) | 3D & Stability Physics | Columbia U | No | No | No | |
414 | Quiescent runaway electron experiments for model validation in ITER-like parameter regimes | Disruption Mitigation | Columbia U | No | No | No | |
308 | Quiescent runaway electron studies for 2015 | Disruption Mitigation | Columbia U | No | No | No | |
181 | Radiating mantle + radiating divertor | PMI Physics | UCSD | No | No | No | |
156 | Radiation profile control | Control | GA | No | No | No | |
419 | Radiative Plasmas for Power Exhaust Predictions | SOL and Divertor Physics | VTT Technical Research Centre | No | No | No | |
144 | Real time stability analysis and disruption avoidance control using DCON | 3D & Stability Physics | GA | No | No | No | |
39 | Real-time error field control using extremum seeking | Control | Department of Energy | Yes | Yes | No | |
348 | Real-time Reduced Kinetic EFIT | Control | PPPL | No | No | No | |
349 | Real-time Stability Control | Control | PPPL | No | No | No | |
386 | Reduced heat flux in highly powered AT plasmas using either carbon or metallic-based divertors | Steady State | GA | No | No | No | |
249 | Return of ELMs during RMP and low torque operation | ELM Stability & Control | UCLA | No | No | No | |
172 | Rho* Scaling of momentum transport in DIII-D | Turbulence & Transport | GA | No | No | No | |
313 | RMP ELM suppression in low torque ITER Baselines | Inductive Scenarios | UCSD | No | No | Yes | |
254 | Role of collisionality and density on rotation | Turbulence & Transport | The college of William and Mary | No | No | No | |
243 | Role of emission from deuterium molecules on the radiation shortfall | SOL and Divertor Physics | Aalto U | No | No | No | |
250 | Role of magnetic, n_e, and Te fluctuations in core H-mode confinement & comparison to simulation | Turbulence & Transport | UCLA | No | No | No | |
274 | Rotating fields should spin plasma even in absence of mode (NTV in a moving frame) | 3D & Stability Physics | Columbia U | No | No | No | |
276 | Rotating n=3 fields by out-of-phase I-coils and C-coils | 3D & Stability Physics | Columbia U | No | No | No | |
337 | Rotation Profile Control | Control | PPPL | No | No | No | |
179 | Rotation Profile Manipulation using 3D Fields | 3D & Stability Physics | Columbia U | Yes | No | No | |
332 | Rotation scaling for penetration of low n error fields | 3D & Stability Physics | Department of Energy | No | Yes | No | |
333 | Rotation scaling for penetration of low n error fields | 3D & Stability Physics | Department of Energy | No | Yes | No | |
294 | Rotational Stabilization on NTM, and effect on pedestal and H-mode | 3D & Stability Physics | GA | No | No | No | |
223 | Rutherford equation at fixed beta & rotation | 3D & Stability Physics | Columbia U | Yes | No | No | |
52 | Safety Factor Scaling of Turbulence and Transport in Hybrid Scenario Plasmas | Turbulence & Transport | U of Wisconsin | No | No | No | |
335 | Sawtooth control and predictions for ITER | Control | EPFL | Yes | Yes | No | |
258 | Sawtooth control in low collisionality + low safety factor plasmas | 3D & Stability Physics | Columbia U | No | No | No | |
103 | Sawtooth stabilization with n=1 applied fields | 3D & Stability Physics | Department of Energy | No | No | No | |
173 | Scaling of core poloidal rotation | Turbulence & Transport | ORAU | No | No | No | |
150 | Scenario integration: developing a detached, radiating divertor to support an AT core | SOL and Divertor Physics | GA | Yes | No | No | |
117 | Scenario integration: developing a detached, radiating divertor to support an AT core | Steady State | GA | No | No | No | |
291 | Search for Plasma Response Bifurcation to ELM Suppression in ISS discharges with n = 3 RMP | ELM Stability & Control | UCSD | No | No | No | |
182 | Search for Positive NTV Offset Rotation | 3D & Stability Physics | Columbia U | No | No | No | |
105 | Separating multiple kink mode responses using I and C-coil for studying nonlinear coupling to n=1 | 3D & Stability Physics | Department of Energy | No | No | No | |
305 | Sequential SPI injections in runaway plateau | Disruption Mitigation | ORNL | No | No | No | |
328 | SOL density and helicon coupling | Heating & Current Drive | UCLA | No | No | No | |
70 | Spectroscopic studies of W erosion/re-deposition with wide scans of divertor plasma parameters | PMI Physics | GA | Yes | No | No | |
218 | Stabilization of radiatively induced tearing modes (RiTMs) using off-axis-heating | 3D & Stability Physics | PPPL | Yes | No | No | |
270 | Stabilization of radiatively induced tearing modes (RiTMs) using off-axis-heating | Torkil Jensen Award | PPPL | Yes | No | No | |
115 | Stabilization of the detachment front at the secondary X point in advanced divertor configurations | Control | GA | No | No | No | |
116 | Stabilization of the detachment front at the secondary X point in advanced divertor configurations | SOL and Divertor Physics | GA | Yes | No | No | |
188 | Steady state ELM free lithium induced enhanced pedestal | Pedestal Transport & Control | GA | No | No | No | |
391 | Steady-state hybrid in scaled ITER shape | Steady State | ORNL | No | No | No | |
439 | Studies of arcing on W coatings in support of W Tile Ring experiment | PMI Physics | UCSD | No | No | No | |
367 | Study of high energy (> 700 keV) electrons generated during disruptions and low density QREs | Disruption Mitigation | Oak Ridge Associated Universities | No | No | No | |
272 | Study of runaway plateau impurity assimilation and final loss | Disruption Mitigation | UCSD | No | No | Yes | |
98 | subcritical beta limit in high-betap regime | Turbulence & Transport | GA | No | No | No | |
119 | Super H-mode pedestal with detached divertor | Steady State | GA | No | No | No | |
296 | Target Lock for more robust NTM suppression | Control | GA | No | No | No | |
163 | Tearing mode avoidance using EC in very high betaN, high li discharges | Steady State | GA | No | No | No | |
416 | Tearing Mode Magnetic Spectroscopy using ECH | 3D & Stability Physics | PPPL | No | No | No | |
304 | Test of dual SPI injection for disruption mitigation | Disruption Mitigation | ORNL | No | No | Yes | |
46 | Test of helicon coupling | Heating & Current Drive | GA | Yes | No | No | |
74 | Test of Turbulence Spreading Using Turbulence Propagation | Turbulence & Transport | GA | No | No | No | |
12 | Test ZF model with RMPs | LH Physics | The college of William and Mary | No | No | Yes | |
355 | The balance of C erosion and deposition on high-Z divertor substrates | PMI Physics | GA | No | No | No | |
433 | The balance of C erosion and deposition on tungsten in the divertor | PMI Physics | GA | No | No | No | |
162 | The effect of LSN Shape on the q95 windows in RMP ELM Suppression | ELM Stability & Control | GA | No | No | No | |
87 | The exploration of EM torque injection unlocking approach in various locking conditions | ELM Stability & Control | PPPL | Yes | No | No | |
166 | The impact of increased pressure gradient on scenarios for fully noninductive operation | Steady State | GA | Yes | No | No | |
86 | The improving the ELM suppression with n=2 | 3D & Stability Physics | PPPL | Yes | No | No | |
16 | Thermal quench MHD activity driven by shattered pellet injection | Disruption Mitigation | ORNL | No | No | Yes | |
43 | Time-resolved measurement of plasma response damping rate | 3D & Stability Physics | Columbia U | Yes | No | No | |
207 | Tomographic Reconstruction of the Full Fast-ion Distribution Function via FIDA Measurements | Energetic Particles | GA | No | No | No | |
423 | Toroidally dependent turbulence with applied 3D fields | Pedestal Transport & Control | ORNL | Yes | No | No | |
37 | Transformative Torque-less ITER similarity discharges in DIII-D with the present gyrotron set. | Turbulence & Transport | GA | No | No | No | |
314 | Transient Plasma Interaction, Recycling, and Pedestal Recovery following Type I ELMs | SOL and Divertor Physics | UCSD | No | No | No | |
186 | Transport evolution at the onset of RMP ELM suppression | ELM Stability & Control | GA | Yes | Yes | Yes | |
440 | Transport in ITER baseline plasmas | Inductive Scenarios | ITER Organization | No | No | No | |
430 | Tungsten thermal shock behavior during helium plasma exposure | PMI Physics | GA | No | No | No | |
368 | Turbulence behavior in high qmin steady state scenario | Steady State | UW-Madison | No | No | No | |
322 | Turbulence penetration into magnetic island | ELM Stability & Control | National Institute for Fusion Science, Japan | No | No | No | |
54 | Turbulence Response Across Applied low-n Magnetic Islands | Turbulence & Transport | UW-Madison | Yes | No | No | |
184 | Turbulent Ion Thermal Response to Electron Heat Flux and Te/Ti Variation | Turbulence & Transport | Sandia National Lab | Yes | No | No | |
277 | Two transients with one stone: ELM and locked-mode-disruption avoidance by n=2 or 3 fields | 3D & Stability Physics | Columbia U | No | No | No | |
278 | Two transients with one stone: ELM and locked-mode-disruption avoidance by n=2 or 3 fields | ELM Stability & Control | Columbia U | No | No | No | |
263 | Type I ELMy H-modes and ELM suppression at low Pinp/PL-H with low torque and extension to high beta | ELM Stability & Control | ITER Organization | Yes | No | Yes | |
346 | Understand mechanisms by which ECH influences NTM stablility | 3D & Stability Physics | GA | No | No | No | |
138 | Understand return of ELMs in low torque QH-mode at low q95 | Inductive Scenarios | GA | Yes | No | Yes | |
402 | Understanding the Heat Flux modification during RPM ELM Suppression | ELM Stability & Control | PPPL | No | No | No | |
396 | Understanding the radiating divertor in ITER low torque scenarios | Inductive Scenarios | GA | No | No | No | |
397 | Understanding the radiating divertor in QH mode | Inductive Scenarios | GA | No | No | No | |
399 | Understanding upgrade requirements for successful radiative divertor operation | Integrated Modeling | GA | No | No | No | |
350 | Upgraded Snowflake Divertor Control | Control | PPPL | No | No | No | |
406 | Upper divertor snowflake studies | SOL and Divertor Physics | GA | No | No | No | |
107 | Use of amplitude and phase of fast rotating tearing modes to identify intrinsic error-fields | 3D & Stability Physics | Massachusetts Institute of Technology | Yes | No | No | |
127 | Using Impurity Granule Injection to assist H-mode operation in close-to-threshold scenarios | ELM Stability & Control | PPPL | No | No | No | |
237 | Using intrinsic rotation to lower H-mode power threshold | LH Physics | ORAU | No | No | No | |
4 | Using Runaway Electron Beams to Commission the Gamma Ray Imager | General Physics | GA | No | No | No | |
295 | Validate entrainment limit of 2/1 slowly rotating modes | 3D & Stability Physics | GA | No | No | No | |
318 | VDE upper vs lower heat load study | Disruption Mitigation | UCSD | No | No | Yes | |
53 | VFI bus voltage control and the True scaled ITER shape at DIII-D | Control | GA | No | No | No | |
288 | Viability of ELM Control by Pellet Pacing in the ITER Baseline Scenario | ELM Stability & Control | UCSD | No | No | Yes | |
299 | Visualization of Island and Kink Response to RMPs | ELM Stability & Control | UCSD | No | No | No | |
202 | Wall deposition of refraccted ECH power | Heating & Current Drive | GA | No | No | No | |
1 | Welcome to 2015 DIII-D Research Opportunities Forum | General Physics | LLNL | No | No | No | |
58 | Why Does the Heat Flux Increase in the Secondary Divertor Under the BetaN = constant Constraint? | Steady State | GA | No | No | No | |
415 | Wind Tunnel Validation of ITER Steady-State Using ELM-Suppressed Hybrid Scenario | Steady State | GA | No | No | No | |
100 | wither counter dithers | LH Physics | GA | No | No | No | |
408 | X divertor in the upper divertor | SOL and Divertor Physics | GA | No | No | No |