DIII-D RESEARCH OPPORTUNITIES FORUM FOR THE 2017 EXPERIMENTAL CAMPAIGN

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

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Below is a public summary listing: