DIII-D RESEARCH OPPORTUNITIES FORUM FOR THE 2019 EXPERIMENTAL CAMPAIGN

DIII-D RESEARCH OPPORTUNITIES FORUM FOR THE 2019 EXPERIMENTAL CAMPAIGN
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ID	Title	Research Area	Name	Affiliation	Time Req'ed	Presentation	ITPA Joint Exp	ITER IO Urgent Research Task
142	Helical core in high performance scenario	Turbulence and transport	Knolker	GA	Yes	Breakout	No	No
27	Dependence of Ohmic energy confinement in negative triangularity diverted plasmas	Turbulence and transport	Thome	GA	No	Breakout	No	No
208	Investigation of high-Z impurity pump-out mechanism inside of saturated MHD modes	Turbulence and transport	Odstrcil	GA	Yes	Breakout	No	No
203	Fast particle effects on transport of high Z ions with HFS asymmetry	Turbulence and transport	Odstrcil	GA	Yes	Breakout	No	No
266	Test of Turbulence Spreading Using Turbulence Propagation	Turbulence and transport	Petty	GA	No	Breakout	No	No
43	Low and mid-Z impurity density asymmetry	Turbulence and transport	Chrystal	GA	No	Breakout	No	No
402	Nonlinear Effects of Impurity Dilution, Te/Ti, Safety Factor, and Magnetic Shear on Transport	Turbulence and transport	Ernst	Massachusetts Institute of Technology	Yes	Breakout	No	No
317	Role of edge neoclassical particle transport and grad(B) drift direction in I-mode transitions	Turbulence and transport	Sciortino	Max-Planck Institute for Plasma Physics	Yes	Breakout	No	No
263	Impurity temperature screening in ITBs	Turbulence and transport	Sciortino	Max-Planck Institute for Plasma Physics	No	Breakout	No	No
90	Impurity transport in diverted negative triangularity discharges	Turbulence and transport	Sciortino	Max-Planck Institute for Plasma Physics	Yes	Breakout	No	No
385	Effect of 3D fields on turbulence and transport in DIII-D plasmas	Turbulence and transport	Kumar Barada	UCLA	Yes	Breakout	No	No
38	Role of turbulence in "No man's land" in determining pedestal structure and core profiles of H-mode	Turbulence and transport	Kumar Barada	UCLA	Yes	Breakout	No	No
88	Exploring new reactor concepts: H-mode in negative triangularity diverted plasmas	Turbulence and transport	Marinoni	UCSD	No	Breakout	No	No
398	Parametric Dependence of Turbulence and Transport on rho-star in low-rotation H-mode plasmas	Turbulence and transport	McKee	U of Wisconsin	Yes	Breakout	No	No
399	Safety Factor Scaling of Turbulence and Transport in Hybrid Scenario Plasmas	Turbulence and transport	McKee	U of Wisconsin	No	Breakout	No	No
386	Complete plasma turbulence measurements of DIII-D L-mode plasmas	Turbulence and transport	Burke	LLNL	Yes	Breakout	No	No
194	Comparing the transport models experimentally	Turbulence and transport	Kolemen	PPPL	No	Breakout	No	No
179	Model validation of betaN > 3 in negative triangularity DIII-D discharges	Turbulence and transport	Austin	U of Texas, Austin	No	Breakout	No	No
180	Transport vs rotation in DIII-D negative triangularity discharges	Turbulence and transport	Austin	U of Texas, Austin	No	Breakout	No	No
401	Determine the critical gradient in negative triangularity discharges	Turbulence and transport	Austin	U of Texas, Austin	No	Breakout	No	No
256	Avalanche-like electron heat transport events in MHD-quiescent plasmas	Turbulence and transport	Choi	Korea Institute of Fusion Energy	Yes	General	No	No
111	Controlled ITB formation with narrow current channel	Torkil Jensen	Victor	LLNL	Yes	Breakout	No	No
25	How fast can we go?	Torkil Jensen	Victor	LLNL	Yes	Breakout	No	No
534	Doublet shape in DIII-D	Torkil Jensen	Austin	U of Texas, Austin	Yes	Breakout	No	No
139	ITER pedestal turbulence properties	Torkil Jensen	Boedo	UCSD	No	Breakout	No	No
542	LH power threshold, confinement scaling and CER calibration in carbon plasmas	Torkil Jensen	Marinoni	UCSD	No	Breakout	No	No
65	Negligible background carbon via boron dropper for a closer approach to fusion reactor conditions	Torkil Jensen	Rhodes	UCLA	Yes	Breakout	No	No
541	Soliton like Shock Front Dynamics during Pellet Deposition in H-mode	Torkil Jensen	Baylor	ORNL	Yes	Breakout	No	No
535	Demonstration of impurity control via an actively heated divertor in DIII-D	Torkil Jensen	Abrams	GA	Yes	Breakout	No	No
8	ECH Beat Wave Generation of ICE	Torkil Jensen	Grierson	GA	No	General	No	No
460	Use pellets to enable 2/1 NTM stabilization with very low gyrotron power	Torkil Jensen	Bardoczi	GA	No	Breakout	No	No
98	A new path to ELM mitigation	Torkil Jensen	Knolker	GA	Yes	Breakout	No	Yes
74	Modify RE distribution function with externally launched helicon (whistler) waves	Torkil Jensen	Paz-Soldan	Columbia U	Yes	Breakout	No	No
55	Soft-landing of a major disruption using 3D fields	Torkil Jensen	Du	GA	Yes	General	No	No
92	Decouple target inward/outward asymmetries due to ExB drift and due to finite ion gyro-radius	Surface Evolution	Bykov	GA	Yes	Breakout	No	No
20	Ignition mechanism of arc by ELMs	Surface Evolution	Rohde	Max Planck Institut fuer Plasmaphysiks, Garching, Germany	No	General	No	No
470	Measuring intra-ELM D recycling on pre-exposed W surfaces	Surface Evolution	Sinclair	Oak Ridge Associated Universities	Yes	Breakout	No	No
500	Tracking erosion and redeposition of crystalline SiC in the DIII-D divertor	Surface Evolution	Sinclair	GA	Yes	Breakout	No	No
491	Spectroscopic inference of tungsten re-deposition fractions	Surface Evolution	Abrams	GA	No	Breakout	No	No
242	Controlled low Z melting experiments using DiMES in support of ITER	Surface Evolution	Rudakov	UCSD	Yes	Breakout	Yes	Yes
373	Measuring net and gross erosion rates of SiC in DIII-D divertor at forward Bt	Surface Evolution	Rudakov	UCSD	Yes	Breakout	No	No
318	Exploring the role of nonlinear MHD in triggering tearing modes in high-qmin and steady-state hybrid	Steady State Scenarios & High qmin Thrust	Chapman	U of Wisconsin	Yes	Breakout	No	No
319	Exploring the role of fluctuation-based dynamos in magnetic flux pumping	Steady State Scenarios & High qmin Thrust	Chapman	U of Wisconsin	Yes	Breakout	No	No
447	Optimizing Transport Through Magnetic Shear	Steady State Scenarios & High qmin Thrust	McKee	U of Wisconsin	No	Breakout	No	No
13	Impact of broadened pressure profile on AE stability in qmin>2 reversed shear steady state scenario	Steady State Scenarios & High qmin Thrust	Collins	ORNL	Yes	Breakout	Yes	No
117	Validate theory-based integrated scenario modeling for high qmin	Steady State Scenarios & High qmin Thrust	Park	ORNL	Yes	Breakout	No	No
118	High density & high qmin	Steady State Scenarios & High qmin Thrust	Park	ORNL	Yes	Breakout	No	No
119	High qmin in ITER shape	Steady State Scenarios & High qmin Thrust	Park	ORNL	Yes	Breakout	No	No
121	High qmin in lower elongation, Z = +10 cm plasma with far off-axis NBCD	Steady State Scenarios & High qmin Thrust	Park	ORNL	Yes	Breakout	No	No
125	Optimize BT for high qmin	Steady State Scenarios & High qmin Thrust	Park	ORNL	Yes	Breakout	No	No
189	Mitigation of AEs in high performance discharges using high off-axis current drive	Steady State Scenarios & High qmin Thrust	Kramer	PPPL	No	Breakout	No	No
101	ELM suppression by n=1 Ex-Vessel Coil at high qmin	Steady State Scenarios & High qmin Thrust	Hu	PPPL	Yes	Breakout	No	No
221	Detection of marginally stable modes in high qmin scenarios using the MM MHD spectroscopy vs q95	Steady State Scenarios & High qmin Thrust	Munaretto	PPPL	Yes	Breakout	No	No
222	Apply MM MHD spectroscopy results from #219/#221 experiments to achieve ELM suppression in high qmin	Steady State Scenarios & High qmin Thrust	Munaretto	PPPL	Yes	Breakout	No	No
223	Use the multimode MHD spectroscopy in real time to control the NBI and modify the modes stability	Steady State Scenarios & High qmin Thrust	Munaretto	PPPL	Yes	Breakout	No	No
219	Detection of marginally stable modes in high qmin scenarios using the MM MHD spectroscopy vs shape	Steady State Scenarios & High qmin Thrust	Munaretto	PPPL	Yes	Breakout	No	No
3	High qmin with betaN > 4	Steady State Scenarios & High qmin Thrust	Victor	LLNL	Yes	Breakout	No	No
4	Effect of rotation on confinement and stability in the high qmin scenario	Steady State Scenarios & High qmin Thrust	Victor	LLNL	Yes	Breakout	No	No
110	Controlled ITB formation with narrow current channel	Steady State Scenarios & High qmin Thrust	Victor	LLNL	Yes	Breakout	No	No
200	Locking Avoidance in high q_min by Dynamic Error Field Correction Assisted by 3D Field Entrainment	Steady State Scenarios & High qmin Thrust	Okabayashi	PPPL	Yes	Breakout	No	No
298	Optimize fast ion confinement in high qmin plasmas at high beta !	Steady State Scenarios & High qmin Thrust	Nazikian	GA	Yes	Breakout	No	No
265	High Pedestal in Hybrid Scenario With Unfavorable Grad-B Drift Direction	Steady State Scenarios & High qmin Thrust	Petty	GA	No	Breakout	No	No
336	Pushing Steady-State Hybrid Scenario to Lower q95, Higher Beta and Higher Fusion Gain	Steady State Scenarios & High qmin Thrust	Petty	GA	No	Breakout	No	Yes
488	Steady-State Hybrids in Hydrogen With Higher Bootstrap Fraction	Steady State Scenarios & High qmin Thrust	Petty	GA	No	Breakout	No	No
21	High performance in the qmin~1.5 scenario	Steady State Scenarios & High qmin Thrust	Thome	GA	Yes	Breakout	No	No
22	Optimizing of q and fast-ion profiles in high-qmin scenario	Steady State Scenarios & High qmin Thrust	Thome	GA	No	Breakout	No	No
333	Validation of Predict First Simulations using CCOANB 210	Steady State Scenarios & High qmin Thrust	Grierson	GA	Yes	Breakout	No	No
228	Use new off-axis CD tools to improve noninductive sustainability of high beta AT plasma	Steady State Scenarios & High qmin Thrust	Garofalo	GA	Yes	Breakout	No	No
484	- Feasibility of plasma performance and stability of ITER steady-state operation with NB+EC CD	Steady State Scenarios & High qmin Thrust	Polevoi	ITER Organization	No	Breakout	No	Yes
431	Profile control for high qmin steady state scenario	Steady State Scenarios & High qmin Thrust	Wehner	Lehigh	No	Breakout	No	No
432	Profile control for high qmin steady state scenario	Steady State Scenarios & High qmin Thrust	Wehner	Lehigh	No	Breakout	No	No
433	Profile control for high qmin steady state scenario	Steady State Scenarios & High qmin Thrust	Wehner	Lehigh	No	Breakout	No	No
268	Map and optimize the fully non-inductive operational space for the steady-state hybrid scenario	Steady State Scenarios & High qmin Thrust	Turco	Columbia U	Yes	Breakout	No	No
286	Assess the benefits of the hybrid vs the high-qmin AT scenarios	Steady State Scenarios & High qmin Thrust	Turco	Columbia U	Yes	Breakout	No	No
169	Study the access to the hybrid regime, the conditions for its sustainment and its consequences	Steady State Scenarios & High qmin Thrust	Turco	Columbia U	Yes	Breakout	No	No
165	Increase the ideal MHD limits, and the passively stable operational space, of steady-state plasmas	Steady State Scenarios & High qmin Thrust	Turco	Columbia U	Yes	Breakout	No	No
166	Impact of EC location and CD on current evolution, confinement and stability of steady-state plasmas	Steady State Scenarios & High qmin Thrust	Turco	Columbia U	Yes	Breakout	No	No
167	Proximity of tearing mode onset to ideal limits in high-beta plasmas	Steady State Scenarios & High qmin Thrust	Turco	Columbia U	Yes	Breakout	No	No
59	Assess kinetic RWM stability of ITER steady-state scenario	Steady State Scenarios & High qmin Thrust	Hanson	Columbia U	Yes	Breakout	No	No
61	Measure the influence of profile broadness on global stability	Steady State Scenarios & High qmin Thrust	Hanson	Columbia U	Yes	Breakout	No	No
563	Probe RWM stability using off-axis NBI	Steady State Scenarios & High qmin Thrust	Hanson	Columbia U	No	Breakout	No	No
23	Simultaneous Control of n=1 and n=2 Resistive Wall Modes and Stability Measurements	Steady State Scenarios & High qmin Thrust	Battey	Columbia U	Yes	Breakout	No	No
449	m/n=2/1 NTM control by ECCD in steady state hybrid	Steady State Scenarios & High qmin Thrust	Bardoczi	GA	No	Breakout	No	No
413	Redistribute plasma momentum and particles in divertor due to the coupling of drift and sheath	SOL Flows	Wang	GA	Yes	Breakout	No	No
213	Search for SOL impurity stagnation region	SOL Flows	Allen	LLNL	No	Breakout	No	No
233	Carbon flow in plasma crown	SOL Flows	Allen	LLNL	No	Breakout	No	No
244	Are kinetics the missing piece in our ability to predict impurity velocities in the SOL?	SOL Flows	Samuell	LLNL	Yes	Breakout	No	No
251	Methane Injection Changing D+ flows in SOL	SOL Flows	Boedo	UCSD	No	Breakout	No	No
247	ExB drifts and paralel flows in divertor and SOL before/during detachment	SOL Flows	Boedo	UCSD	No	Breakout	No	No
249	ExB drifts and paralel flows in divertor and SOL before/during detachment	SOL Flows	Boedo	UCSD	No	Breakout	No	No
422	Increase "intrinsic" edge rotation via control of edge stochasticity	Rotation physics	Schmitz	UCLA	No	Breakout	No	No
479	ITG and TEM's impacts on toroidal rotation profile and intrinsic rotation	Rotation physics	Qin	U of Wisconsin	No	Breakout	No	No
51	Deuterium poloidal rotation measurements using main ion CER spectroscopy	Rotation physics	Haskey	PPPL	Yes	Breakout	No	No
150	Competition Between Intrinsic Torque and NTV for ITER	Rotation physics	Grierson	GA	No	Breakout	No	No
54	NTV Electron Root as Cause of Core Velocity Hollowing with On-Axis ECH in Very High Te H-Mode Core	Rotation physics	Ernst	Massachusetts Institute of Technology	Yes	Breakout	No	No
12	Toward Initiation of Wide Pedestal QH-Mode without NBI	Pedestal Physics and Pedestal Structure & QH Thrust	Ernst	Massachusetts Institute of Technology	Yes	Breakout	No	No
291	Elucidate the Physics Setting the I-mode Pedestal	Pedestal Physics and Pedestal Structure & QH Thrust	Hughes	Massachusetts Institute of Technology	Yes	Breakout	Yes	No
295	Pedestal Structure and Neutral Source Measurement	Pedestal Physics and Pedestal Structure & QH Thrust	Rosenthal	Massachusetts Institute of Technology	Yes	Breakout	No	No
556	168: Extend Zero Torque Wide Pedestal QH-Mode Operation to IBS Parameters	Pedestal Physics and Pedestal Structure & QH Thrust	Ernst	Massachusetts Institute of Technology	No	Breakout	No	No
29	Parametric Variation of Pedestal Turbulence and Transport in Wide Pedestal QH-Mode	Pedestal Physics and Pedestal Structure & QH Thrust	Ernst	Massachusetts Institute of Technology	Yes	Breakout	No	No
367	Wide pedestal access at high power in QH-mode and RMP Hybrid plasmas.	Pedestal Physics and Pedestal Structure & QH Thrust	Nazikian	GA	Yes	Breakout	No	No
280	Physics requirements for high pressure staircase pedestal formation	Pedestal Physics and Pedestal Structure & QH Thrust	Nazikian	GA	Yes	Breakout	No	No
151	Test hypothesis for the cause of improved energy confinement at lower NBI torque	Pedestal Physics and Pedestal Structure & QH Thrust	Garofalo	GA	Yes	Breakout	No	Yes
548	Effect of outer gap on wide-pedestal QH-mode	Pedestal Physics and Pedestal Structure & QH Thrust	Garofalo	GA	No	Breakout	No	No
464	Effect of impurities on pedestal structure in Peeling and Ballooning dominate discharges.	Pedestal Physics and Pedestal Structure & QH Thrust	Osborne	GA	No	Breakout	No	No
216	Test ExB shear importance in QH using co-Ip approach	Pedestal Physics and Pedestal Structure & QH Thrust	Chen	GA	Yes	Breakout	No	No
353	Wide pedestal QH-mode operation at lower Zeff	Pedestal Physics and Pedestal Structure & QH Thrust	Burrell	GA	No	Breakout	No	No
116	Measuring Te-fluctuations within the pedestal of wide pedestal Quiescent H-mode plasmas	Pedestal Physics and Pedestal Structure & QH Thrust	Houshmandyar	GA	No	Breakout	No	No
79	what are those modes observed in the wide-pedestal QH edge?	Pedestal Physics and Pedestal Structure & QH Thrust	Chen	GA	No	Breakout	No	No
80	B x gradB drift, divertor config, Carbon effects on QH-mode	Pedestal Physics and Pedestal Structure & QH Thrust	Chen	GA	Yes	Breakout	No	No
549	Further investigation of the saturation & underlying transport mechanism of EHO to allow ELM stable	Pedestal Physics and Pedestal Structure & QH Thrust	Chen	GA	No	Breakout	No	No
550	What's the physics leads to std QH, Wide Pedestal QH,or ELMing IBS from L-mode at low torque?	Pedestal Physics and Pedestal Structure & QH Thrust	Chen	GA	No	Breakout	No	No
120	Disentangling impacts of heating scheme and neutral sourcing on pedestal structure	Pedestal Physics and Pedestal Structure & QH Thrust	Nelson	Columbia U	Yes	Breakout	No	No
290	Collisionality Dependence of Quasi-Coherent Fluctuations	Pedestal Physics and Pedestal Structure & QH Thrust	Ashourvan	GA	Yes	Breakout	No	No
292	Dependence of staircase pedestal formation on input power in the RMP grassy-ELM regime	Pedestal Physics and Pedestal Structure & QH Thrust	Ashourvan	GA	Yes	Breakout	No	No
108	Measure and control resistive kink mode stability	Pedestal Physics and Pedestal Structure & QH Thrust	Hanson	Columbia U	No	Breakout	No	No
283	Exploring Access Conditions to Standard QH and WPQH Pedestals	Pedestal Physics and Pedestal Structure & QH Thrust	Wilks	MIT	Yes	Breakout	No	No
49	When Is Ion Thermal Transport Neoclassical in the H-mode Pedestal?	Pedestal Physics and Pedestal Structure & QH Thrust	Haskey	PPPL	Yes	Breakout	No	No
467	Main-ion, impurity and electron profile evolution throughout the ELM cycle	Pedestal Physics and Pedestal Structure & QH Thrust	Haskey	PPPL	Yes	Breakout	No	No
67	Unraveling the mechanism linking the pedestal structure and its dynamics to ELM energy densities in ITER relevant regimes	Pedestal Physics and Pedestal Structure & QH Thrust	Diallo	PPPL	No	Breakout	No	No
109	Effects of the IPD on pedestal structure and edge fluctuations leading to ELM suppressed phases	Pedestal Physics and Pedestal Structure & QH Thrust	Diallo	PPPL	No	Breakout	No	No
387	Local Magnetic Field Measurements of QH-mode EHO	Pedestal Physics and Pedestal Structure & QH Thrust	Burke	LLNL	No	Breakout	No	No
383	Active MHD Spectroscopy of Edge Harmonic Oscillation (EHO) Mode Control for QH-mode	Pedestal Physics and Pedestal Structure & QH Thrust	WANG	ASIPP	Yes	Breakout	Yes	Yes
140	Electron density up-down assymetry	Pedestal Physics and Pedestal Structure & QH Thrust	Mordijck	The college of William and Mary	No	Breakout	No	No
301	QH-mode similarity experiment between DIII-D and AUG with co-current beams	Pedestal Physics and Pedestal Structure & QH Thrust	Viezzer	U of Seville	Yes	Breakout	No	No
518	Dimensionless scaling of pedestal height, width and stability - a turbulence & transport perspective	Pedestal Physics and Pedestal Structure & QH Thrust	Banerjee	PPPL	No	Breakout	No	No
287	Validation of the NIMROD results	Pedestal Physics and Pedestal Structure & QH Thrust	Pankin	PPPL	No	Breakout	No	No
519	Role of poloidal rotation on pedestal instabilities	Pedestal Physics and Pedestal Structure & QH Thrust	Pankin	PPPL	Yes	Breakout	No	No
102	Density pump-in by RMP in H-mode plasma	Pedestal Physics and Pedestal Structure & QH Thrust	Hu	PPPL	Yes	Breakout	No	No
196	ELM cycle: induce at will and find the effect of edge current variation using burst CER/Thomson	Pedestal Physics and Pedestal Structure & QH Thrust	Kolemen	PPPL	No	Breakout	No	No
239	Pedestal structure and stability as a function of Te/Ti and momentum injection	Pedestal Physics and Pedestal Structure & QH Thrust	Banerjee	PPPL	Yes	Breakout	No	No
258	Deuterium lifecycle during ELM pacing with pellet injection	Pedestal Physics and Pedestal Structure & QH Thrust	Bortolon	PPPL	No	Breakout	No	No
281	Perturbative study of inter-ELM pedestal localized instabilities	Pedestal Physics and Pedestal Structure & QH Thrust	Laggner	North Carolina State	Yes	Breakout	No	No
302	Measurement of EHO particle vs energy transport and phase angles with fluctuation diagnostics	Pedestal Physics and Pedestal Structure & QH Thrust	Morton	U of Wisconsin	No	Breakout	No	No
297	Identifying and Detecting Microtearing Modes within the Pedestal of an H-mode Plasma	Pedestal Physics and Pedestal Structure & QH Thrust	Major	U of Wisconsin	No	Breakout	No	No
48	Identify and control pedestal turbulence modes in ELMing H-mode plasmas	Pedestal Physics and Pedestal Structure & QH Thrust	Yan	U of Wisconsin	No	Breakout	No	No
145	HFS Pellet Fueling Deposition Dynamics in H-mode Plasmas	Pedestal Physics and Pedestal Structure & QH Thrust	Baylor	ORNL	No	Breakout	No	No
146	Pellet Fueling of Wide Pedestal QH-mode Plasmas	Pedestal Physics and Pedestal Structure & QH Thrust	Baylor	ORNL	No	Breakout	No	No
69	EHO dominated sustained wide-pedestal QH-mode	Pedestal Physics and Pedestal Structure & QH Thrust	Kumar Barada	UCLA	Yes	Breakout	No	No
104	Radially inward propagation of pedestal after L-H transition until the first ELM	Pedestal Physics and Pedestal Structure & QH Thrust	Kumar Barada	UCLA	Yes	Breakout	No	No
97	Inter-ELM pedestal turbulence and transport when ELMs appear in wide-pedestal QH-mode	Pedestal Physics and Pedestal Structure & QH Thrust	Kumar Barada	UCLA	Yes	Breakout	No	No
127	Identify and assess pedestal magnetic fluctuations in H-mode plasmas in DIII-D	Pedestal Physics and Pedestal Structure & QH Thrust	Chen	UCLA	Yes	Breakout	No	No
30	Multi-scale/field pedestal turbulence, transport, drive, damping just prior to ELM and inter-ELM	Pedestal Physics and Pedestal Structure & QH Thrust	Rhodes	UCLA	Yes	Breakout	No	No
34	Physics of density pump-out with application of resonant magnetic perturbations (RMP)	Pedestal Physics and Pedestal Structure & QH Thrust	Rhodes	UCLA	Yes	Breakout	No	No
363	Assessing impact of SAS alignment on divertor particle content and transition to detachment	Particle Balance and Impact of Divertor Closure Including SAS on Detachment Thrust	Lore	ORNL	Yes	Breakout	No	No
364	Dependence of divertor conditions on SOL width in SAS configuration	Particle Balance and Impact of Divertor Closure Including SAS on Detachment Thrust	Lore	ORNL	Yes	Breakout	No	No
430	How does closure impact the path to complete detachment?	Particle Balance and Impact of Divertor Closure Including SAS on Detachment Thrust	Canik	ORNL	Yes	Breakout	No	No
437	Optimizing the pumping geometry for SAS2	Particle Balance and Impact of Divertor Closure Including SAS on Detachment Thrust	Canik	ORNL	No	Breakout	No	No
428	Interplay of particle control and drifts in detached divertors	Particle Balance and Impact of Divertor Closure Including SAS on Detachment Thrust	Shafer	ORNL	Yes	Breakout	No	No
155	Characterize the impact of 3D fields on divertor closure and detachment in SAS	Particle Balance and Impact of Divertor Closure Including SAS on Detachment Thrust	Hinson	ORNL	Yes	Breakout	No	No
427	Characterization of the impact of baffling on SOL profiles at varying plasma decay lengths	Particle Balance and Impact of Divertor Closure Including SAS on Detachment Thrust	Jarvinen	VTT Technical Research Centre	Yes	Breakout	No	No
404	Experimentally test edge code predictions of strong correlation between T_e_target and n_D2_target	Particle Balance and Impact of Divertor Closure Including SAS on Detachment Thrust	Stangeby	U of Toronto	Yes	Breakout	No	No
423	Characterizing the widths of heat flux footprint in closed diverotr	Particle Balance and Impact of Divertor Closure Including SAS on Detachment Thrust	Ren	U of Tennessee, Knoxville	Yes	Breakout	No	No
436	Probing the drift effect by actively biased SAS divertor	Particle Balance and Impact of Divertor Closure Including SAS on Detachment Thrust	Ren	U of Tennessee, Knoxville	Yes	Breakout	No	No
359	Neutrals: How fast are they going and where are they headed?	Particle Balance and Impact of Divertor Closure Including SAS on Detachment Thrust	Samuell	LLNL	Yes	Breakout	No	No
257	Detachment onset in SAS: The mysterious case of shot 173537 with a fully attached divertor	Particle Balance and Impact of Divertor Closure Including SAS on Detachment Thrust	McLean	LLNL	Yes	Breakout	No	No
267	Detachment onset in SAS: The curious case of missing neutral pressure at cold plasma onset in 175816	Particle Balance and Impact of Divertor Closure Including SAS on Detachment Thrust	McLean	LLNL	Yes	Breakout	No	No
271	Detachment onset in SAS: The peculiar case of a Te cliff in 175816 with BxgradB out of the divertor	Particle Balance and Impact of Divertor Closure Including SAS on Detachment Thrust	McLean	LLNL	Yes	Breakout	No	No
425	Characterizing the widths of heat flux footprint in closed diverotr	Particle Balance and Impact of Divertor Closure Including SAS on Detachment Thrust	Ren	UTK	Yes	Breakout	No	No
426	Characterizing the widths of heat flux footprint in closed diverotr	Particle Balance and Impact of Divertor Closure Including SAS on Detachment Thrust	Ren	UTK	Yes	Breakout	No	No
440	Optimizing SOL width in closed divertor for particle control and detachment	Particle Balance and Impact of Divertor Closure Including SAS on Detachment Thrust	Moser	GA	No	Breakout	No	No
438	Effect of in-divertor gas puff location in SAS	Particle Balance and Impact of Divertor Closure Including SAS on Detachment Thrust	Moser	GA	No	Breakout	No	No
45	Coupling of drift-closure v.s. good performance pedestal assisted with dissipative divertor	Particle Balance and Impact of Divertor Closure Including SAS on Detachment Thrust	Wang	GA	Yes	Breakout	No	No
40	characterize divertor detachment in closed divertor	Particle Balance and Impact of Divertor Closure Including SAS on Detachment Thrust	Wang	GA	Yes	Breakout	No	No
441	How does SAS performance depend on enclosed poloidal flux?	Particle Balance and Impact of Divertor Closure Including SAS on Detachment Thrust	Thomas	GA	No	Breakout	No	No
466	Plasma flow in a closed divertor	Particle Balance and Impact of Divertor Closure Including SAS on Detachment Thrust	Leonard	GA	Yes	Breakout	No	No
461	Pedestal and core transport comparison of SAS , upper closed, and lower open divertor	Particle Balance and Impact of Divertor Closure Including SAS on Detachment Thrust	Osborne	GA	No	Breakout	No	No
463	QH-mode with detached divertor	Particle Balance and Impact of Divertor Closure Including SAS on Detachment Thrust	Osborne	GA	No	Breakout	No	No
540	SAS 2 precursor experiments	Particle Balance and Detachment Characterization in Closed Divertors Thrust	Watkins	Sandia National Lab	Yes	Breakout	No	No
508	Understand divertor leakage & SOL accumulation using isotopic methane & main ion puff/pump methods	Materials Migration and Mitigation	Unterberg	ORNL	Yes	Breakout	No	No
128	Dependence of upstream low-Z impurity accumulation on ExB drift direction	Materials Migration and Mitigation	Nichols	ORNL	Yes	Breakout	No	No
406	W-pellet injection to calibrate the DIII-D Collector Probe	Materials Migration and Mitigation	Stangeby	U of Toronto	No	Breakout	No	No
148	Impurity particle balance model in order to characterize near-SOL accumulation of carbon using 13CH4	Materials Migration and Mitigation	Duran	U of Tennessee, Knoxville	Yes	Breakout	No	No
64	Liquid Metal Dust Break-up Mechanisms	Materials Migration and Mitigation	Andrew	Imperial College London	Yes	Breakout	No	No
235	Physics of real-time wall conditioning by B dust injection	Materials Migration and Mitigation	Bortolon	PPPL	No	Breakout	No	No
465	Test free-streaming+recycling model (FSRM) for W sputtering during ELMs at low collisionality	Materials Migration and Mitigation	Abrams	GA	Yes	Breakout	No	No
93	Characterize arc ignition threshold due to ELM deposition	Materials Migration and Mitigation	Bykov	GA	Yes	Breakout	No	No
94	Core impurity contamination by unipolar arcing on high-Z PFCs and on SiC	Materials Migration and Mitigation	Bykov	GA	Yes	Breakout	No	No
96	High-resolved ELM filament properties: spatial frequency, q_perp, j_sat, profiles of n_e and T_e	Materials Migration and Mitigation	Bykov	GA	Yes	Breakout	No	No
130	Time resoved measurements of CX D energy and flux density at the midplane with MiMES	Materials Migration and Mitigation	Bykov	GA	Yes	Breakout	No	No
91	Effect of ionization in the sheath on prompt redeposition of high-Z impurities	Materials Migration and Mitigation	Bykov	GA	Yes	Breakout	No	No
337	ECRH plasma production on DIII-D	Materials Migration and Mitigation	Wauters	LPP-ERM-KMS â�?�? Brussels â�?�? Belgium (EUROfusion member)	No	Breakout	Yes	Yes
112	Measurement of surface incident ion direction using engineered targets on DiMES at DIII-D	Materials Migration and Mitigation	Skinner	PPPL	Yes	Breakout	No	No
246	Interpret W I & W II emission to benchmark S/XB coefficients & infer prompt redeposition fractions	Materials Migration and Mitigation	Ennis	Auburn U	Yes	Breakout	No	No
520	Impact of Nonresonant Magnetic Perturbations on L-H and H-L Transitions	L-H transition	Logan	Columbia U	Yes	Breakout	No	No
352	Stationary Zonal Flows	L-H transition	Burrell	GA	No	Breakout	No	No
551	What's the physics leads to std QH, Wide Pedestal QH,or ELMing IBS from L-mode at low torque?	L-H transition	Chen	GA	No	Breakout	No	No
105	L-H Transitions dynamics: Impact of the beam voltage and its effects on the edge rotation shear	L-H transition	Banerjee	PPPL	Yes	Breakout	No	No
86	H-mode Access Dependence on Divertor Magnetic Configuration	L-H transition	Andrew	Imperial College London	Yes	Breakout	No	No
87	Density Dependence of L-H Transition	L-H transition	Andrew	Imperial College London	Yes	Breakout	No	No
66	Impact of RMP on the L-H threshold	L-H transition	Diallo	PPPL	No	Breakout	No	No
47	Divertor configuration effects on the L-H power threshold	L-H transition	Yan	U of Wisconsin	Yes	Breakout	No	No
71	Role of scrape-off layer electric field in L-H power threshold scaling	L-H transition	Schmitz	UCLA	No	Breakout	No	No
360	LH power threshold, confinement scaling and CER calibration in carbon plasmas	L-H transition	Marinoni	UCSD	No	Breakout	No	No
188	Electron- and ion-heat dominated L-H transition regimes	L-H transition	Schmitz	UCLA	Yes	Breakout	No	No
497	Reducing the L-H power threshold in D plasmas with pellets	L-H transition	Wilcox	ORNL	Yes	Breakout	No	No
39	Revisit pellet triggered L-H transition and understand underlying turbulence suppression mechanisms	L-H transition	Kumar Barada	UCLA	Yes	Breakout	No	No
31	Optimization of hydrogen H-mode transition targeting ITER's Pre Fusion Plasma Operation Stage	Isotope mass Thrust	Rhodes	UCLA	Yes	Breakout	No	No
502	Scaling of turbulence properties with ion mix	Isotope mass Thrust	Carter	UCLA	Yes	Breakout	No	No
237	Influence of isotope on H-mode density limit	Isotope Mass Thrust	Hong	UCLA	Yes	Breakout	No	No
250	Mitigate increased L-H transition threshold power in ITER PFPO hydrogen plasmas w/wo applied RMP	Isotope mass Thrust	Schmitz	UCLA	No	Breakout	No	No
536	Helium scenarios for ITER	Isotope mass Thrust	Marinoni	UCSD	No	Breakout	Yes	No
357	Power loading at toroidal PFC gaps	Isotope Mass Thrust	Rudakov	UCSD	No	Breakout	Yes	Yes
72	H-mode access in electron-heat dominated ITER PFPO hydrogen plasmas	Isotope Mass Thrust	Schmitz	UCLA	Yes	Breakout	No	No
9	Improved H-mode access in mixed H/He plasmas	Isotope mass Thrust	Schmitz	UCLA	Yes	Breakout	No	No
70	Constrain first principles L-H transition models: Favorable/unfavorable grad-B in Helium plasmas	Isotope Mass Thrust	Schmitz	UCLA	Yes	Breakout	No	No
135	Reducing the L-H power threshold in H plasmas with pellets	Isotope mass Thrust	Wilcox	ORNL	Yes	Breakout	No	No
362	Fuel Ion Particle Transport using H/D Isotopes	Isotope Mass Thrust	McKee	U of Wisconsin	Yes	Breakout	No	No
68	Isotope Mass Scaling of Turbulence, Transport and Confinement	Isotope mass Thrust	McKee	U of Wisconsin	Yes	Breakout	Yes	No
348	Divertor configuration effects on the L-H power threshold in H plasmas	Isotope mass Thrust	Yan	U of Wisconsin	No	Breakout	No	No
46	Isotope mix effects (puffing He into H plasmas) on the L-H power threshold	Isotope mass Thrust	Yan	U of Wisconsin	No	Breakout	No	No
361	Simultaneous measurement of electron and ion particle transport from ITG up to TEM dominated plasma	Isotope Mass Thrust	Tala	VTT Technical Research Centre	Yes	Breakout	Yes	No
274	edge/SOL turbulence with plasma isotopic mass scaling.	Isotope mass Thrust	Boedo	UCSD	No	Breakout	No	No
53	Power Flow Through the Ion Channel for Hydrogen and He-doped L-H transition at ITER relevant Qe/Qi	Isotope mass Thrust	Haskey	PPPL	Yes	Breakout	No	No
245	Characterizing Detachment in H-mode Helium Plasmas	Isotope mass Thrust	Samuell	LLNL	No	Breakout	No	No
115	Role of fueling in determining the pedestal structure	Isotope Mass Thrust	Mordijck	The college of William and Mary	No	Breakout	Yes	Yes
446	Pedestal structure in hydrogen-1 plasmas relevant for non-nuclear Iter and access to ELM suppression	Isotope mass Thrust	Laggner	North Carolina State	No	Breakout	No	No
141	Isotope effect and the role of divertor geometry	Isotope Mass Thrust	Casali	U of Tennessee, Knoxville	Yes	Breakout	Yes	Yes
236	wide-pedestal QH in dominant electron-heated ITER PFPO hydrogen plasmas	Isotope Mass Thrust	Chen	GA	No	Breakout	No	No
334	Negative Triangularity in H Plasma	Isotope Mass Thrust	Smith	GA	No	Breakout	No	No
335	High performance QH-mode in H plasma with pellet fueling	Isotope Mass Thrust	Smith	GA	No	Breakout	No	No
209	Isotope mass dependence of multichannel transport	Isotope Mass Thrust	Odstrcil	GA	Yes	Breakout	No	No
341	Energy Confinement dependence on mass	Isotope mass Thrust	Thome	GA	No	Breakout	No	No
6	H vs. D Core Transport Model Validation at High Te/Ti	Isotope mass Thrust	Grierson	GA	Yes	General	Yes	Yes
122	Alfven Eigenmode Stability and Fast Ion Transport with Hydrogen and Deuterium Beams	Isotope Mass Thrust	Van Zeeland	GA	Yes	Breakout	No	No
123	Alfven Eigenmode Stability and Fast Ion Transport with Helium and Deuterium Beams	Isotope Mass Thrust	Van Zeeland	GA	Yes	Breakout	No	No
28	Effect of Isotopic Mass on Wide Pedestal QH-Mode Core and Pedestal Turbulence and Intrinsic Rotation	Isotope mass Thrust	Ernst	Massachusetts Institute of Technology	Yes	Breakout	No	No
126	Effect of Isotope Mass on Intrinsic Rotation and Momentum Transport in H-Mode Plasmas	Isotope Mass Thrust	Ernst	Massachusetts Institute of Technology	Yes	Breakout	No	Yes
103	Comparison of high density ELM suppression in H and He to D	Isotope Mass Thrust	Evans	GA	No	Breakout	No	Yes
476	Pedestal dimensionless parameter match DIII-D to JET for H,D,He	Isotope Mass Thrust	Osborne	GA	No	Breakout	No	No
300	Study of MHD modes near L-H transition in H, H+D and H+He plasmas	Isotope Mass Thrust	Solano	Ciemat	Yes	Breakout	No	No
131	Isotope identity pair in H and D type I ELMy H-modes	Isotope mass Thrust	Maggi	CCFE	Yes	Breakout	Yes	No
133	Rho* scaling in Hydrogen type I ELMy H-modes	Isotope mass Thrust	Maggi	CCFE	Yes	Breakout	Yes	No
134	Validation of core and edge transport models in Hydrogen L-mode	Isotope mass Thrust	Maggi	CCFE	Yes	Breakout	Yes	No
279	Isotope effect on the detachment rollover density	Isotope Mass Thrust	Solokha	Aalto U	No	No	No
349	isotope scaling at constant rhostar	Isotope Mass Thrust	scott	PPPL	Yes	Breakout	No	No
350	isotope scaling with matched kinetic profiles	Isotope Mass Thrust	scott	PPPL	No	Breakout	No	No
365	Power Threshold Studies in Mixed Ion Species Plasmas	Isotope Mass Thrust	Plank	IPP Garching	Yes	Breakout	Yes	Yes
378	Impact of isotope and first wall on plasma (Te, Zeff, q) during IP ramp-up	Isotope mass Thrust	Mailloux	UKAEA	Yes	Breakout	Yes	Yes
379	Compare H-mode plasmas with controlled ELMs in H, He, D	Isotope mass Thrust	Mailloux	UKAEA	Yes	Breakout	Yes	Yes
380	Investigate impact of isotope on plasmas at low and high beta/power and at low and high torque	Isotope mass Thrust	Mailloux	UKAEA	Yes	Breakout	Yes	Yes
75	RMP-ELM Suppression and Mitigation in Hydrogen Plasmas	Isotope Mass Thrust	Paz-Soldan	Columbia U	No	Breakout	No	No
95	ELM-resolved D and D2 re-emission from C,W,and SiC: characterization by ro-vibrational spectroscopy	Innovative Materials Evaluation	Bykov	GA	No	Breakout	No	No
220	Metastable multiphase tungsten compounds: toward new fusion friendly material?*	Innovative Materials Evaluation	Guterl	GA	Yes	Breakout	No	No
553	Studying the PMI properties of advanced tungsten alloys with DiMES	Innovative Materials Evaluation	Allain	U of Illinois at Urbana-Champaign	Yes	Breakout	No	No
509	Exposure of Graphitic foam at DiMES and Tile	Innovative Materials Evaluation	Unterberg	ORNL	No	Breakout	No	No
482	Pyroid HT Material Assessment using DiMES	Innovative Materials Evaluation	Wukitch	Massachusetts Institute of Technology	Yes	Breakout	No	No
312	Exploring the role of nonlinear MHD in triggering tearing modes in IBS and adv. ind. hybrid scenario	Inductive Scenarios	Chapman	U of Wisconsin	Yes	Breakout	No	No
313	Exploring the role of fluctuation-based dynamos in magnetic flux pumping	Inductive Scenarios	Chapman	U of Wisconsin	Yes	Breakout	No	No
229	Measure and control resistive kink mode stability	Inductive Scenarios	Hanson	Columbia U	No	Breakout	No	No
57	Assess robustness of ITER baseline plasma response control	Inductive Scenarios	Hanson	Columbia U	No	Breakout	No	No
230	Study the high density branch of RMP ELM suppression in the IBS	Inductive Scenarios	Turco	Columbia U	Yes	Breakout	No	No
170	Tailor the T=0 IBS to achieve the fusion power and gain mission	Inductive Scenarios	Turco	Columbia U	Yes	Breakout	No	No
171	Assess the impact of EC power location on the performance and the stability of the T=0 IBS	Inductive Scenarios	Turco	Columbia U	Yes	Breakout	No	No
172	Integrate ITER relevant perturbations to the IBS, assess options to maintain stability & performance	Inductive Scenarios	Turco	Columbia U	Yes	Breakout	No	No
173	Asses the benefits and impact of ohmic or heated L-mode phase in the IBS ramp-up	Inductive Scenarios	Turco	Columbia U	Yes	Breakout	No	No
174	Make DIII-D a W or no W machine	Inductive Scenarios	Turco	Columbia U	Yes	Breakout	No	No
489	Developing low-disruptivity ramp-down techniques for the ITER Baseline Scenario	Inductive Scenarios	Barr	GA	No	Breakout	No	No
76	RMP-ELM Suppression Access Conditions with the actual ITER shape	Inductive Scenarios	Paz-Soldan	Columbia U	Yes	Breakout	No	No
77	Direct comparison of ITER similar shape (ISS) and ITER baseline scenario (IBS) plasmas for RMP-ELM	Inductive Scenarios	Paz-Soldan	Columbia U	No	Breakout	No	No
37	Wide Pedestal QH-Mode Path to Super H-Mode	Inductive Scenarios	Ernst	Massachusetts Institute of Technology	Yes	Breakout	No	No
168	Extend Zero Torque Wide Pedestal QH-Mode Operation to IBS Parameters	Inductive Scenarios	Ernst	Massachusetts Institute of Technology	Yes	Breakout	No	No
377	RMP ELM suppression for inductive Hybrid plasmas relevant to the ITER Q=10 mission	Inductive Scenarios	Nazikian	GA	Yes	Breakout	No	No
320	Access super H-mode in ITER Q=10 baseline target	Inductive Scenarios	Nazikian	GA	Yes	Breakout	No	No
149	QH-mode for Q=10 IBS at Zero NBI torque by reducing the pressure profile peaking	Inductive Scenarios	Garofalo	GA	Yes	Breakout	No	Yes
355	High fusion gain in the advanced inductive	Inductive Scenarios	Thome	GA	No	Breakout	No	No
538	Expanding the Wide Pedestal QH to IBS Parameters	Inductive Scenarios	Chen	GA	No	Breakout	No	No
304	How changes in ROSP, fueling location, and dRsep during D2 injection affect hybrid performance	Impurity Radiative Divertor Dependence on Divertor Closuree	Petrie	GA	Yes	Breakout	No	No
305	Effect of seed selection, ROSP, and magnetic balance on successful radiating divertor operation	Impurity Radiative Divertor Dependence on Divertor Closuree	Petrie	GA	Yes	Breakout	No	No
306	Is krypton better than argon as a mantle seed in high power, high performance hybrid plasmas?	Impurity Radiative Divertor Dependence on Divertor Closuree	Petrie	GA	No	Breakout	No	No
307	Two-impurity approach as an optimal radiating divertor solution for DIII-D	Impurity Radiative Divertor Dependence on Divertor Closuree	Petrie	GA	No	Breakout	No	No
308	Effect of reversing the grad-B drift on high betaN plasmas under radiating divertor conditions	Impurity Radiative Divertor Dependence on Divertor Closuree	Petrie	GA	Yes	Breakout	No	No
310	Two-impurity approach as an optimal radiating divertor solution for DIII-D	Impurity Radiative Divertor Dependence on Divertor Closuree	Petrie	GA	No	Breakout	No	No
331	Minimize upstream density for divertor detachment and test radiation detachment model	Impurity Radiative Divertor Dependence on Divertor Closuree	Wang	GA	Yes	Breakout	No	No
327	Effect of drifts in Ne/N2 seeded SAS divertor	Impurity Radiative Divertor Dependence on Divertor Closuree	Casali	U of Tennessee, Knoxville	Yes	Breakout	Yes	No
328	Impurity screening in closed divertors	Impurity Radiative Divertor Dependence on Divertor Closuree	Casali	U of Tennessee, Knoxville	Yes	Breakout	Yes	No
330	Development of high radiation scenario with dual seeding in open and closed divertors	Impurity Radiative Divertor Dependence on Divertor Closuree	Casali	U of Tennessee, Knoxville	Yes	Breakout	Yes	No
81	Snowflake SAS divertor	Impurity Radiative Divertor Dependence on Divertor Closure	Soukhanovskii	LLNL	No	Breakout	No	No
85	Can open horizontal plate divertor act as baffled vertical plate divertor	Impurity Radiative Divertor Dependence on Divertor Closure	Soukhanovskii	LLNL	No	Breakout	No	No
234	Search for Tungsten Accumulation in Upper divertor	Impact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential Thrust	Allen	LLNL	No	Breakout	No	No
503	Impact of large area electrical biasing on material erosion and divertor leakage in SAS1-W	Impact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential Thrust	Ren	U of Tennessee, Knoxville	No	Breakout	No	No
63	Effect of Divertor Closure on Dust Transport	Impact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential Thrust	Andrew	Imperial College London	Yes	Breakout	No	No
564	Impact of high-Z PFCs on impurity seeding experiments in SAS	Impact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential Thrust	Casali	U of Tennessee, Knoxville	No	Breakout	No	No
434	Effect of main ion SOL flows on W impurity transport	Impact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential Thrust	Rudakov	UCSD	No	Breakout	No	No
559	Impurity leakage from a closed divertor during RMP application	Impact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential Thrust	Hinson	ORNL	Yes	Breakout	No	No
129	Dependence of upstream high-Z impurity accumulation on ExB drift direction	Impact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential Thrust	Nichols	ORNL	Yes	Breakout	No	No
562	Minimizing W divertor leakage in the SAS	Impact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential Thrust	Unterberg	ORNL	No	Breakout	No	No
560	Using the SAS to control impurity pinch	Impact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential Thrust	Nelson	Columbia U	No	General	No	No
555	Toroidal symmetry of SAS tiles	Impact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential Thrust	Bykov	GA	No	Breakout	No	No
424	Fueling effects of metal Rings in the divertor	Impact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential Thrust	Bykov	GA	Yes	Breakout	No	No
390	Characterization of tungsten transport and leakage in the SAS divertor	Impact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential Thrust	Ma	ORAU	Yes	Breakout	No	No
264	Impact of ELM size and footprint on W sputtering and W leakage from open & closed divertors	Impact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential Thrust	Abrams	GA	Yes	Breakout	No	Yes
558	High-Z impurity pump-out mechanism inside of MHD modes in plasma with divertor W source	Impact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential Thrust	Odstrcil	GA	No	Breakout	No	No
113	Characterization of SOL impurity accumulation using 13CH4 injection and collector probes	Impact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential Thrust	Zamperini	GA	Yes	Breakout	No	No
114	Characterizing the radial/poloidal structure of SOL impurity accumulation with collector probes	Impact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential Thrust	Zamperini	GA	Yes	Breakout	No	No
388	Characterization of tungsten transport and leakage in the SAS divertor	Impact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential Thrust	Ma	GA	Yes	Breakout	No	No
557	RMP ELM suppression in the SAS shape	Impact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential Thrust	Evans	GA	No	Breakout	No	No
5	210 CCOANB Counter-direction Checkout - Including Power and Ability to Balance Torque	Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)	Grierson	GA	No	Breakout	No	No
486	Helicon Modulation and Shutdown Checkout	Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)	Brookman	GA	No	Breakout	No	No
487	Measure Peak Current Drive Efficiency in Non-Inductive Scenerio	Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)	Brookman	GA	Yes	Breakout	No	No
157	Perturbative Measurements of Helicon Power Deposition and Transport	Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)	Brookman	GA	Yes	Breakout	No	No
468	absorption study of top launch ECCD scheme	Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)	Chen	GA	Yes	Breakout	No	No
469	compare the off-axis ECCD efficiency between top and outside launch	Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)	Chen	GA	Yes	Breakout	No	No
471	experimental demonstration both down-shift and up-shift top launch ECCD schemes	Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)	Chen	GA	No	Breakout	No	No
472	polarization study of top launch	Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)	Chen	GA	No	Breakout	No	No
7	Checkout of 210 CCOANB Using Visible Imaging	Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)	Van Zeeland	GA	No	Breakout	No	No
552	Parametric instabilities during Helicon wave Iinjection in DIII-D	Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)	Porkolab	Massachusetts Institute of Technology	No	Breakout	No	No
481	Develop QH Mode for HFS LHCD Experiments	Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)	Wukitch	Massachusetts Institute of Technology	Yes	Breakout	No	No
309	Validate beta_e dependence of helicon CD	Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)	Garofalo	GA	Yes	Breakout	No	No
478	O-mode absorption and refraction for top launch ECH	Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)	Petty	GA	Yes	Breakout	No	No
498	Measurement of NBCD profile	Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)	Petty	GA	No	Breakout	No	No
499	Helicon Current Drive Measurements	Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)	Petty	GA	Yes	Breakout	No	No
493	Establishment of High Power Operation of Comb-line Antenna Operation with Plasma	Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)	Pinsker	GA	Yes	Breakout	No	No
494	Measurement of high-efficiency central current drive with helicon system	Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)	Pinsker	GA	Yes	Breakout	No	No
512	Parametric decay study with helicon launch	Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)	Pinsker	GA	Yes	Breakout	No	No
345	ECRH plasma production on DIII-D	Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)	Wauters	LPP-ERM-KMS â�?�? Brussels â�?�? Belgium (EUROfusion member)	No	Breakout	Yes	Yes
485	Third harmonic ECH experiments	Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)	Schneider	ITER Organization	No	Breakout	No	No
370	Checkout 210 beams	Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)	Heidbrink	UC, Irvine	No	Breakout	No	No
324	Measurement of helicon wave internal amplitude and validation of simulation	Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)	Crocker	UCLA	No	Breakout	No	No
483	Off-axis NBCD measurement with 210 CCOANB	Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)	Park	ORNL	Yes	Breakout	No	No
504	Helicon Launcher Checkout and Conditioning	Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools)	Zhang	ASIPP	No	Breakout	No	No
1	Welcome to the ROF for the 2019-20 DIII-D Run Campaign	General Physics	Fenstermacher	LLNL	No	Breakout	No	No
561	Experimental Validation of Heteroclitic magnetic Island Bifurcations in DIII-D	General Physics	Evans	GA	No	Breakout	No	No
42	Determine accuracy of NUBEAM power and torque outside mid-radius	Energetic Particle Physics	Chrystal	GA	No	Breakout	No	No
501	Modification of AE Drive and Nonlinear Saturation Through Variation of Beam Modulation	Energetic Particle Physics	Van Zeeland	GA	No	Breakout	Yes	No
56	Hunt the instabilities responsible for the formation of phase space hole	Energetic Particle Physics	Du	GA	No	General	No	No
546	Direct measurement of the wave-particle interactions and associated phase space flow	Energetic Particle Physics	Du	GA	No	Breakout	No	No
124	Characterization of Fast-ion Diagnostic to Edge Neutral Populations	Energetic Particle Physics	Stagner	GA	No	Breakout	No	No
456	Stabilization of TAEs by Localized Electron Cyclotron Current Drive	Energetic Particle Physics	Sharapov	CCFE	No	Breakout	Yes	No
547	Direct measurement of the wave-particle interactions and associated phase space flow	Energetic Particle Physics	du	General Atomic	No	Breakout	No	No
400	Verification of Imaging Fast Ion D-Alpha and application to EP model validation	Energetic Particle Physics	Marini	ORAU	Yes	Breakout	No	No
515	Parameter scan of fast-ion critical gradient threshold	Energetic Particle Physics	Collins	ORNL	No	Breakout	No	No
299	Transient ExB flows caused by bursting fast-ion modes and secondary transport-related impacts	Energetic Particle Physics	Crocker	UCLA	No	Breakout	No	No
198	Radial structure and identification of intermediate frequency Alfven eignemodes	Energetic Particle Physics	Crocker	UCLA	No	Breakout	No	No
181	ICE internal amplitude and radial structure	Energetic Particle Physics	Crocker	UCLA	No	Breakout	No	No
182	CAE suppression by more parallel injection	Energetic Particle Physics	Crocker	UCLA	No	Breakout	No	No
490	BAAE and BAE validation	Energetic Particle Physics	Heidbrink	UC, Irvine	No	Breakout	Yes	No
496	Orbit Tomography (OT)	Energetic Particle Physics	Garcia	UC, Irvine	No	Breakout	Yes	No
371	ICE Mode Structure	Energetic Particle Physics	DeGrandchamp	UC, Irvine	Yes	Breakout	Yes	No
147	Pellet Fueled High Density Operation of RMP ELM Mitigated Plasmas	ELM Control	Baylor	ORNL	No	Breakout	No	No
52	Pellet pacing with with peeling-limited pedestal	ELM Control	Wilcox	ORNL	Yes	Breakout	No	No
50	D2 pellet pacing with tangential injection	ELM Control	Wilcox	ORNL	Yes	Breakout	No	No
389	Rotating MPs to study the change of ELMs in AUG similar shapes	ELM Control	Willensdorfer	Max-Planck Institute for Plasma Physics	Yes	Breakout	No	No
368	Limits of RMP ELM Suppression Toward Double Null	ELM Control	Shafer	ORNL	Yes	Breakout	No	No
177	Evaluate the effect of penetration theory on RMP ELM suppression	ELM Control	WANG	ASIPP	Yes	Breakout	Yes	Yes
543	Strategy for ELM control	ELM Control	Loarte-Prieto	ITER Organization	Yes	General	No	Yes
544	3-D ELM suppressed regime access/exit	ELM Control	Loarte-Prieto	ITER Organization	Yes	General	No	Yes
545	3-D ELM suppressed H-mode and pellet fuelling	ELM Control	Loarte-Prieto	ITER Organization	Yes	General	No	Yes
285	Understanding the connection between ELM suppression and magnetic footprint size.	ELM Control	Munaretto	PPPL	Yes	Breakout	No	No
356	ELM pacing by pellet injection in low-collisionality ITER relevant scenarios	ELM Control	Bortolon	PPPL	No	Breakout	No	No
537	ELM pacing during ITER-like current ramp-up/down	ELM Control	Bortolon	PPPL	No	Breakout	No	Yes
554	ELM pacing during ITER-like current ramp-up/down	ELM Control	Bortolon	PPPL	No	Breakout	No	Yes
393	ELM pacing by pellet injection in low-collisionality ITER relevant scenarios	ELM Control	Bortolon	PPPL	No	Breakout	No	No
394	ELM pacing during ITER-like current ramp-up/down	ELM Control	Bortolon	PPPL	No	Breakout	No	Yes
395	ELM pacing during ITER-like current ramp-up/down	ELM Control	Bortolon	PPPL	No	Breakout	No	Yes
99	Scaling of ELM suppression threshold	ELM Control	Hu	PPPL	Yes	Breakout	No	No
100	Understanding density pump-out in ELM control experiment	ELM Control	Hu	PPPL	Yes	Breakout	No	No
405	Max-Planck-Institut f�?¼r Plasmaphysik	ELM Control	Willensdorfer	Max-Planck-Institut f�?¼r Plasmaphysik	Yes	Breakout	No	No
391	Max-Planck-Institut f�?¼r Plasmaphysik	ELM Control	Willensdorfer	Max-Planck-Institut f�?¼r Plasmaphysik	Yes	Breakout	No	No
392	Rotating MPs to study helically edge localized modes in AUG similar shapes	ELM Control	Willensdorfer	Max-Planck-Institut f�?¼r Plasmaphysik	Yes	Breakout	No	No
369	Limits of RMP ELM Suppression Toward Double Null	ELM Control	Shafer	ORNL	Yes	Breakout	No	No
183	Evaluate the effect of penetration theory on RMP ELM suppression	ELM Control	WANG	ASIPP	Yes	Breakout	Yes	Yes
303	ECEI and MIR contribution	ELM Control	Zhu	UC Davis	Yes	Breakout	No	No
231	Study the high density branch of RMP ELM suppression in the IBS	ELM Control	Turco	Columbia U	Yes	Breakout	No	No
396	Overdriven ELM Suppression	ELM Control	Lyons	GA	Yes	Breakout	No	No
397	Establish ELM suppression in DND plasma	ELM Control	Lyons	GA	No	Breakout	No	No
78	RMP-ELM Control in Strongly Shaped Plasmas	ELM Control	Paz-Soldan	Columbia U	Yes	Breakout	Yes	No
375	direct detection of islands with rotating n=1 RMP	ELM Control	Nazikian	GA	Yes	Breakout	No	No
376	Main ion rotation in ELM suppression	ELM Control	Nazikian	GA	Yes	Breakout	No	No
407	Divertor radiated power control vs. ELM frequency	ELM Control	Eldon	GA	No	Breakout	No	No
408	Burn through of paced ELMs in detachment	ELM Control	Eldon	GA	No	Breakout	No	No
513	Boundary Ion temperature measurement based on retarding field analyzer	Divertor Closure	Ren	U of Tennessee, Knoxville	Yes	Breakout	No	No
259	Divertor to pedestal trace impurity transport	Div/SOL Turbulence and transport	Bortolon	PPPL	No	Breakout	No	No
262	Divertor-localized turbulence and characterization of 2D profiles of divertor turbulence	Div/SOL Turbulence and transport	Scotti	LLNL	No	Breakout	No	No
270	Evolution of edge turbulence and turbulence flow near midplane during divertor detachment	Div/SOL Turbulence and transport	Wang	UCLA	No	Breakout	No	No
36	Turbulence spreading from pedestal into SOL and testing models/scalings of lambda_q	Div/SOL Turbulence and transport	Rhodes	UCLA	Yes	Breakout	No	No
358	Parallel correlation of turbulence/blobs between mid-plane and divertor SOL	Div/SOL Turbulence and transport	Rudakov	UCSD	No	Breakout	No	No
294	Characterization of Te fluctuations in the divertor and main SOL	Div/SOL Turbulence and transport	Rudakov	UCSD	Yes	Breakout	No	No
354	Study of impurity ion entrainment in divertor cross-field transport	Div/SOL Turbulence and transport	Hollmann	UCSD	No	Breakout	No	No
273	Scaling of blobby transport with divertor conditions and pedestal/SOL widening	Div/SOL Turbulence and transport	Boedo	UCSD	No	Breakout	No	No
248	Poloidal asymmetries of radial transport in the edge/SOL	Div/SOL Turbulence and transport	Boedo	UCSD	No	Breakout	No	No
374	Effect on SEE on Langmuir probe measurements in the SOL	Div/SOL Turbulence and transport	Rudakov	UCSD	No	Breakout	No	No
421	Magnetic shear at X-point and radial turbulence transport	Div/SOL Turbulence and transport	Boedo	UCSD	No	Breakout	No	No
144	Transport and turbulence in Divertor and pedestal during detachment	Div/SOL Turbulence and transport	Boedo	UCSD	No	Breakout	No	No
138	Physics of pedestal turbulence vs width	Div/SOL Turbulence and transport	Boedo	UCSD	No	Breakout	No	No
414	Quasi-coherent fluctuations near the divertor plate	Div/SOL Turbulence and transport	Wang	GA	No	Breakout	No	No
296	Imaging of turbulence in the divertor and SOL and poloidal asymmetries	Div/SOL Turbulence and transport	Bykov	GA	Yes	Breakout	No	No
415	Power and momentum detachment in impurity seeded plasmas and test radiation detachment model	Dissipative Divertor Physics	Wang	GA	Yes	Breakout	No	No
225	Detachment onset with X-point height	Dissipative Divertor Physics	McLean	LLNL	Yes	Breakout	No	No
366	DIII-D Experiments in Support of ITPA DSOL Detachment Research	Dissipative Divertor Physics	Reinke	ORNL	Yes	Breakout	Yes	No
343	Check for Te cliff at inner strike point in reverse Bt	Dissipative Divertor Physics	Eldon	GA	No	Breakout	No	No
252	Effect of divertor radiation front on drifts and parallel flow	Dissipative Divertor Physics	Boedo	UCSD	No	Breakout	No	No
410	Radiative divertor with impurity seeding at moderate density	Dissipative Divertor Physics	Jarvinen	VTT Technical Research Centre	Yes	Breakout	No	No
411	Impurity seeded radiative divertor in L-mode	Dissipative Divertor Physics	Jarvinen	VTT Technical Research Centre	Yes	Breakout	No	No
416	Characterization of pedestal/SOL coupling at X-point in detached conditions	Dissipative Divertor Physics	Jarvinen	VTT Technical Research Centre	Yes	Breakout	No	No
187	Scaling of 2D structure of detachment front	Dissipative Divertor Physics	Jarvinen	VTT Technical Research Centre	Yes	Breakout	No	No
240	How much protection does detachment give us from ELMs?	Dissipative Divertor Physics	Samuell	LLNL	Yes	Breakout	Yes	No
243	Optimizing the process for developing 2D reconstructions of divertor conditions	Dissipative Divertor Physics	Samuell	LLNL	Yes	Breakout	No	No
227	Impact of plasma opacity on divertor detachment	Dissipative Divertor Physics	McLean	LLNL	Yes	Breakout	No	No
232	Impact of spectral contamination of the MWIR region	Dissipative Divertor Physics	McLean	LLNL	Yes	Breakout	No	No
255	Contribution of molecules to radiated power	Dissipative Divertor Physics	McLean	LLNL	Yes	Breakout	No	No
193	Impact of molecular processes on divertor detachment and validation of UEDGE fluid molecular model	Dissipative Divertor Physics	Holm	PPPL	No	Breakout	No	No
152	Assessment of Ly-alpha opacity in fully detached divertor plasmas	Dissipative Divertor Physics	Groth	Aalto U	No	Breakout	No	No
517	Penetration characterization of small pellet injection into D3D plasmas	Disruption Mitigation Thrust	Raman	U of Washington	No	Breakout	No	No
473	Evaluating the internal MHD response to shell pellet injection	Disruption Mitigation Thrust	Pandya	U of Wisconsin	No	Breakout	No	No
474	Evaluating the internal MHD response to SPI	Disruption Mitigation Thrust	Pandya	U of Wisconsin	No	Breakout	No	No
475	Measuring internal MHD during the formation and evolution of a runaway electron beam	Disruption Mitigation Thrust	Pandya	U of Wisconsin	No	Breakout	No	No
14	Comparison of dispersive vs non-dispersive shell pellet payload	Disruption Mitigation Thrust	Hollmann	UCSD	No	Breakout	No	No
15	Suppression of RE seeds with W grains in shell pellet	Disruption Mitigation Thrust	Hollmann	UCSD	No	Breakout	No	No
16	Dynamic measurement of impurity transport into RE plateau using carbon deposition	Disruption Mitigation Thrust	Hollmann	UCSD	No	Breakout	No	No
17	Change in RE plateau vertical loss rate with low-Z injection	Disruption Mitigation Thrust	Hollmann	UCSD	No	Breakout	No	No
18	Scan of RE plateau final loss footprint with I-coil perturbation	Disruption Mitigation Thrust	Hollmann	UCSD	No	Breakout	No	No
19	Scan of RE plateau impurity assimilation with auxiliary heating	Disruption Mitigation Thrust	Hollmann	UCSD	No	Breakout	No	No
510	Superposition of identical dual SPIs	Disruption Mitigation Thrust	Herfindal	ORNL	No	Breakout	No	No
514	MGI-assisted-SPI for decreased radiation asymmetries and increased penetration depth	Disruption Mitigation Thrust	Sweeney	Massachusetts Institute of Technology	Yes	Breakout	No	No
533	Ballistic transport and energy/size scaling for SPI	Disruption Mitigation Thrust	Shiraki	ORNL	No	Breakout	No	No
372	whistler polarization	Disruption Mitigation Thrust	Heidbrink	UC, Irvine	No	Breakout	No	No
539	Effect of underlying non-axisymmetric (NA) fields on disruption mitigation process	Disruption Mitigation Thrust	Eidietis	GA	No	Breakout	No	No
525	Mass scaling of shell pellet assimilation	Disruption Mitigation Thrust	Eidietis	GA	No	Breakout	No	No
526	Full profile measurement of shell Te profile	Disruption Mitigation Thrust	Eidietis	GA	No	Breakout	No	No
527	Test Li coating for "ideal" shell pellet	Disruption Mitigation Thrust	Eidietis	GA	No	Breakout	No	No
528	Ablation measurments of single snall Ne pellet	Disruption Mitigation Thrust	Eidietis	GA	No	Breakout	No	No
529	Effect of D admixture in SPI	Disruption Mitigation Thrust	Eidietis	GA	No	Breakout	No	No
530	dilution cooling in SPI superposition	Disruption Mitigation Thrust	Eidietis	GA	No	Breakout	No	No
531	Scaling of fragment penetration depth with energy:	Disruption Mitigation Thrust	Eidietis	GA	No	Breakout	No	No
532	JET SPI similarity experiments	Disruption Mitigation Thrust	Eidietis	GA	No	Breakout	No	No
10	The role of RE-driven kinetic instabilities on formation of post-disruption RE beam	Disruption Mitigation Thrust	Lvovskiy	GA	Yes	Breakout	No	No
11	Identification of Alfven instabilities driven by REs at negative Uloop during RE plateau stage	Disruption Mitigation Thrust	Lvovskiy	GA	No	Breakout	No	No
73	Role of pre-disruption electron temperature in runaway electron seed formation	Disruption Mitigation Thrust	Paz-Soldan	Columbia U	No	Breakout	No	No
507	ITER DMS design validation	Disruption Mitigation Thrust	Lehnen	ITER Organization	No	Breakout	No	No
26	Determine the cause of RE beam final loss in post disruption vertical displacement events	Disruption Mitigation Thrust	Bardoczi	GA	No	Breakout	No	Yes
417	Collisionality effects on ELM dynamics in the high-betaP scenario	DIII-D/EAST Task Force/Thrust	Weisberg	GA	Yes	Breakout	No	No
418	Investigating RWM stability in the high-betaP scenario	DIII-D/EAST Task Force/Thrust	Weisberg	GA	Yes	Breakout	No	No
226	Controlling ITB formation via impurity puffing	DIII-D/EAST Task Force/Thrust	McClenaghan	GA	No	Breakout	No	No
450	Explore the Basis of Realizing ITER Q=10 at Ip<=9MA on DIII-D	DIII-D/EAST Task Force/Thrust	Ding	GA	Yes	Breakout	No	No
452	Develop High Betap Scenario toward High Non-Inductive Current Fraction at q95~6 on DIII-D	DIII-D/EAST Task Force/Thrust	Ding	GA	Yes	Breakout	No	No
453	Investigate the Turbulence Suppression in High Betap Plasmas when Te is Close to Ti	DIII-D/EAST Task Force/Thrust	Ding	GA	Yes	Breakout	No	No
480	Radiative divertor in high-betap plasma by utilizing SAS and local impurity injection	DIII-D/EAST Task Force/Thrust	Wang	GA	Yes	Breakout	No	No
454	Validating Dominant Micro-Turbulence Instabilities in DIII-D high BetaP Scenarios	DIII-D/EAST Task Force/Thrust	Jian	GA	Yes	Breakout	No	No
32	Testing and validating low pedestal height with high core confinement plasmas	DIII-D/EAST Task Force/Thrust	Rhodes	UCLA	Yes	Breakout	No	No
33	Is core ITB in high-betap plasmas due to ExB velocity shear or magnetic shear?	DIII-D/EAST Task Force/Thrust	Rhodes	UCLA	Yes	Breakout	No	No
443	Compatibility of highly radiative divertor with high beta_p scenario	DIII-D/EAST Task Force/Thrust	Wang	ASIPP	Yes	Breakout	No	Yes
439	Exploring high-frequency small-ELM regime in hybrid scenario on DIII-D	DIII-D/EAST Task Force/Thrust	Wang	ASIPP	Yes	Breakout	No	No
455	Detection of marginally stable modes in high betaP scenarios using the MM MHD spectroscopy	DIII-D/EAST Task Force/Thrust	Munaretto	PPPL	Yes	Breakout	No	No
282	Explore the use of the RMP to control the heat flux peak in high BetaP plasmas.	DIII-D/EAST Task Force/Thrust	Munaretto	PPPL	Yes	Breakout	No	No
384	Active MHD Spectroscopy of Edge Harmonic Oscillation (EHO) Mode Control for QH-mode	DIII-D/EAST Task Force/Thrust	WANG	ASIPP	Yes	Breakout	Yes	Yes
381	Evaluate the effect of penetration theory on RMP ELM suppression	DIII-D/EAST Task Force/Thrust	WANG	ASIPP	Yes	Breakout	Yes	Yes
382	Use NBI to evaluate n=2 RMP penetration position	DIII-D/EAST Task Force/Thrust	WANG	ASIPP	Yes	Breakout	Yes	Yes
505	Assessing Helicon wave current drive in high betap experiments	DIII-D/EAST Task Force/Thrust	Zhang	ASIPP	No	Breakout	No	No
435	Fully non-inductive high betap scenario at q95~6-7	DIII-D/EAST Task Force/Thrust	Huang	ASIPP	Yes	Breakout	No	No
442	Access to small ELM regime in DIII-D high �?²P scenario	DIII-D/EAST Task Force/Thrust	Qian	ASIPP	No	Breakout	Yes	Yes
207	Measure and Influence Flow with Pump and Pump	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Allen	LLNL	No	Breakout	No	No
212	Minimize carbon in DIII-D AT plasmas	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Allen	LLNL	No	Breakout	No	No
195	Obtaining High Core Confinement with High Edge Confinement using Pedestal Control	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Kolemen	PPPL	Yes	Breakout	No	No
143	Development of high radiation scenario with dual seeding in open and closed divertors	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Casali	U of Tennessee, Knoxville	Yes	Breakout	Yes	No
260	Wide pedestal QH-mode at low Zeff through real-time boronization	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Bortolon	PPPL	Yes	Breakout	No	No
278	A Boron-Nitrogen radiative divertor for AT scenarios	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Bortolon	PPPL	No	Breakout	No	No
238	Mapping the Super H-mode Boundary and Bifurcation	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Bortolon	PPPL	Yes	Breakout	No	No
316	A Boron-Nitrogen radiative divertor for AT scenarios	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Bortolon	PPPL	No	Breakout	No	No
241	High performance core at high radiative fraction with real-time impurity feedback control	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Abbate	PPPL	Yes	General	No	No
191	What can lost fast-ions tell us about the H-mode pedestal?	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Kramer	PPPL	No	Breakout	No	No
261	Exploring the role of nonlinear MHD in triggering tearing modes in Core-Edge Scenario Optimization	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Chapman	U of Wisconsin	Yes	Breakout	No	No
35	Reduction of background carbon via boron dropper for a closer approach to fusion reactor conditions	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Rhodes	UCLA	Yes	Breakout	No	No
156	Impact of magnetic perturbations on SOL force balance	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Hinson	ORNL	Yes	Breakout	No	No
106	Dependence of core-edge impurity transport on plasma shaping in Ti~Te and Ti>>Te regimes	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Sciortino	Max-Planck Institute for Plasma Physics	Yes	Breakout	No	No
107	Optimization of impurity transport in RMP ELM-suppressed discharges with variable ECH location	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Sciortino	Max-Planck Institute for Plasma Physics	Yes	Breakout	No	No
448	Optimizing core-pedestal performance in Super H-Mode	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Snyder	ORNL	No	Breakout	No	No
211	Shape Thresholds for Super H Access and Application to JET DT Campaign	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Snyder	ORNL	Yes	Breakout	No	No
215	Core-Edge Compatibility of Super H Mode with Closed Divertor	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Snyder	ORNL	Yes	Breakout	No	No
204	Understanding the Impact of the Tokamak Edge on Rf Propagation	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Brookman	GA	Yes	Breakout	No	No
202	Pedestal and core impurity transport in super H-mode discharges	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Odstrcil	GA	Yes	Breakout	No	No
276	Super QH-mode with feedback controlled radiation	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Eldon	GA	Yes	Breakout	No	No
277	Divertor radiated power control vs. ELM frequency	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Eldon	GA	No	Breakout	No	No
344	Detachment onset density vs. 3D field strength	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Eldon	GA	No	Breakout	No	No
340	Burn through of paced ELMs in detachment	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Eldon	GA	No	Breakout	No	No
409	Detachment/T_e cliff onset density vs. I_p using control to stay on the edge of the cliff	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Eldon	GA	No	Breakout	No	No
217	co-Ip QH-mode approach to super H-mode	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Chen	GA	No	Breakout	No	No
153	Balancing the Tradeoffs Between High Performance and Core Purity & Stability in High Power Hybrid	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Grierson	GA	No	Breakout	No	No
412	Test H-L back transition transient mitigation strategies in detachment	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Eldon	GA	Yes	Breakout	No	No
253	Investigation and optimization of core and pedestal performance	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Solomon	GA	No	Breakout	No	No
136	Impurity Transport from Core to Edge in IBS-like Conditions	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Howard	Massachusetts Institute of Technology	Yes	Breakout	No	No
137	Impurity Transport from Core to Edge in Steady State Hybrid Conditions	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Howard	Massachusetts Institute of Technology	Yes	Breakout	No	No
41	Impurity Transport and Carbon Reduction in Wide Pedestal QH-Mode	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Ernst	Massachusetts Institute of Technology	Yes	Breakout	No	No
214	Hybrid approac to Super H-mode	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Nazikian	GA	Yes	Breakout	No	No
565	Measure lambda-q during rotation scans at constant heating power in super H mode plasmas	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Garofalo	GA	No	Breakout	No	No
462	Pedestal pressure enhancement at high density through decoupling of ped peeling and ballooning modes	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Osborne	GA	No	Breakout	No	No
158	Effect of O-mode deposition radius on tearing mode onset and impurity profiles in high betaN plasmas	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Petrie	GA	Yes	Breakout	No	No
159	Low level RMP feedback to control deuterium/impurity buildup in high power, high performance plasmas	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Petrie	GA	Yes	Breakout	No	No
160	How changes in ROSP, fueling location, and dRsep during D2 injection affect hybrid performance	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Petrie	GA	Yes	Breakout	No	No
161	Effect of seed selection, ROSP, and magnetic balance on successful radiating divertor operation	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Petrie	GA	Yes	Breakout	No	No
162	Is krypton better than argon as a mantle seed in high power, high performance hybrid plasmas?	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Petrie	GA	Yes	Breakout	No	No
163	Two-impurity approach as an optimal radiating divertor solution for DIII-D	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Petrie	GA	Yes	Breakout	No	No
164	Effect of reversing the grad-B drift on high betaN plasmas under radiating divertor conditions	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Petrie	GA	Yes	Breakout	No	No
272	High Density Electron Heating With O-Mode	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Petty	GA	No	Breakout	No	Yes
269	Pushing Steady-State Hybrid Scenario to Lower q95, Higher Beta and Higher Fusion Gain	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Petty	GA	No	Breakout	No	No
176	Reversing the direction of the impurity pinch at ITER-relevant edge conditions	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Nelson	Columbia U	Yes	Breakout	No	No
154	How does divertor drift affect upstream profiles?	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Wang	GA	Yes	Breakout	No	No
224	Integrate a divertor solution in the T=0 IBS	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Turco	Columbia U	Yes	Breakout	No	No
89	Sustainment of high Super H core confinement	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Knolker	GA	Yes	Breakout	No	No
2	testing, please ignore!	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Coviello	GA	No	Breakout	No	No
175	Make DIII-D a W or no W machine	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Turco	Columbia U	Yes	Breakout	No	No
254	Compatibility of QH-mode with Radiative Divertpr	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Wilks	MIT	Yes	Breakout	No	No
284	ELM-phase dependence on transport for different experimental conditions	Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization	Izacard	Princeton U	Yes	Breakout	No	No
321	Further PCS Development on q-profile Control and NTM Suppression	Control	Pajares	Lehigh U	Yes	Breakout	No	No
322	Integrated Control of Individual Scalars	Control	Pajares	Lehigh U	Yes	Breakout	No	No
325	Profile control for high qmin steady state scenario	Control	Wehner	Lehigh	No	Breakout	No	No
326	Model-based rotation control development	Control	Wehner	Lehigh	No	Breakout	No	No
458	m/n=2/1 NTM control by ECCD in steady state hybrid	Control	Bardoczi	GA	No	Breakout	No	No
346	Developing low-disruptivity ramp-down techniques for the ITER Baseline Scenario	Control	Barr	GA	No	Breakout	No	No
419	Commissioning of a proximity-to-stability-boundary control architecture for disruption prevention	Control	Barr	GA	No	Breakout	No	No
420	Commissioning of a Vertical Control proximity-to-stability-boundary algorithm for VDE prevention	Control	Barr	GA	No	Breakout	No	No
218	The Disruption Free Protocol	Control	Barr	GA	Yes	Breakout	No	No
288	Exploration of IBS variation with direct gain metric regulation	Control	Olofsson	Consultant	No	Breakout	No	No
289	Shape control enabled study of IBS stability as function of edge features	Control	Olofsson	Consultant	No	Breakout	No	No
293	Divertor detachment control based on Langmuir Probes measurement	Control	Wang	GA	Yes	Breakout	No	No
24	Tuning of Controller/Observer Gains for n=1 and n=2 Resistive Wall Mode Control	Control	Battey	Columbia U	Yes	Breakout	No	No
314	Voltage controlled SuperSpas for plasma shape control	Control	Hyatt	GA	No	Breakout	No	No
315	VFI-less Plasma operations	Control	Hyatt	GA	No	Breakout	No	No
44	Real time measurements of impurity density	Control	Chrystal	GA	No	Breakout	No	No
403	Burn Condition Emulation for ITER-relevant Control Experiments	Control	Schuster	Lehigh U	No	Breakout	No	No
347	ITER plasma initiation and ECH assist	Control	Walker	GA	No	Breakout	Yes	Yes
342	Vertical stability control with simulated horizontal interferometer channels	Control	Eldon	GA	No	Breakout	No	No
275	Divertor radiated power control in non-ELMing plasmas	Control	Eldon	GA	No	Breakout	No	No
339	Detachment control w/ Te request translated to ne estimate & direct ne feedback	Control	Eldon	GA	No	Breakout	No	No
506	PCS supervisory algorithm for negotiating complex controller requests	Control	Eidietis	GA	No	Breakout	No	No
201	m/n=2/1 NTM control by ECCD in IBS	Control	Bardoczi	GA	No	Breakout	No	No
429	Real time neutron control	Control	Heidbrink	UC, Irvine	No	Breakout	No	No
511	Feedback control for divertor impurity seeding based on Surface Eroding Thermocouple	Control	Ren	U of Tennessee, Knoxville	No	Breakout	No	No
351	Machine Learning based Instability Prediction & Avoidance	Control	Kolemen	PPPL	Yes	Breakout	No	No
521	ECCD and ECH for IBS with real-time modulation control	Control	Kolemen	PPPL	No	Breakout	No	No
522	RT stability analysis to find/avoid the instabilities with mhd calc. and feedback 3D spectroscopy	Control	Kolemen	PPPL	No	Breakout	No	No
523	Test the new method for finding the 3D perturbation needed to avoid tearing	Control	Kolemen	PPPL	No	Breakout	No	No
524	Control of pressure/current profile transport models experimentally	Control	Kolemen	PPPL	No	Breakout	No	No
338	Combining variable beam energy/perveance and NTV for rotation control	Control	Boyer	PPPL	No	Breakout	No	No
323	Tune RMP Controlled Phase of Locked Island and Radial Alignment of ECCD Deposition for Stabilization	Control	Reiman	PPPL	No	Breakout	No	No
210	Puff and Pump Flow measurement in DN as a function of drsep	Advanced Magnetic Configurations	Allen	LLNL	No	Breakout	No	No
82	Clarify key snowflake divertor physics	Advanced Magnetic Configurations	Soukhanovskii	LLNL	No	Breakout	No	No
83	Particle exhaust in snowflake divertor	Advanced Magnetic Configurations	Soukhanovskii	LLNL	No	Breakout	No	No
329	Magnetic geometry as an actuator for detachment stability and control	Advanced Magnetic Configurations	Samuell	LLNL	Yes	Breakout	No	No
495	SAS, meet DN	Advanced Magnetic Configurations	Thomas	GA	Yes	Breakout	No	No
332	Detachment at horizontal and vertical targets	Advanced Magnetic Configurations	Wang	GA	Yes	Breakout	No	No
84	Clarify snowflake divertor physics	Advanced Magnetic Configurations	Soukhanovskii	LLNL	No	Breakout	No	No
184	Use NBI to evaluate n=2 RMP penetration position	3DSP	WANG	ASIPP	Yes	Yes	Yes
60	Measure and control resistive kink mode stability	3DSP	Hanson	Columbia U	Yes	Breakout	No	No
311	Proximity of tearing mode onset to ideal limits in high-beta plasmas	3DSP	Turco	Columbia U	Yes	Breakout	No	No
58	Assess robustness of ITER baseline plasma response control	3DSP	Hanson	Columbia U	Yes	Breakout	No	No
457	m/n=2/1 NTM control by ECCD in steady state hybrid	3DSP	Bardoczi	GA	No	Breakout	No	No
192	m/n=2/1 NTM control by ECCD in IBS	3DSP	Bardoczi	GA	No	Breakout	No	No
190	Impact of Current Condensation in the ECCD Stabilization of Rotating 2/1 NTMs	3DSP	Bardoczi	GA	No	Breakout	No	No
459	Use pellets to lower the ECCD requirement for 2/1 NTM stabilization	3DSP	Bardoczi	GA	No	Breakout	No	No
477	Optimizing NTV torque profiles with multi-modal 3D control	3DSP	Weisberg	GA	Yes	Breakout	No	No
178	Use NBI to evaluate n=2 RMP penetration position	3DSP	WANG	ASIPP	Yes	Breakout	Yes	Yes
62	Disruption Avoidance via ECCD Stabilization of Locked Islands and the Impact of Current Condensation	3DSP	Reiman	PPPL	Yes	Breakout	No	No
199	Machine Learning based Instability Prediction & Avoidance	3DSP	Kolemen	PPPL	No	Breakout	No	No
205	RT stability analysis to find/avoid the instabilities with mhd calc. and feedback 3D spectroscopy	3DSP	Kolemen	PPPL	No	Breakout	No	No
206	ECCD and ECH for IBS with real-time modulation control	3DSP	Kolemen	PPPL	No	Breakout	No	No
492	Understanding outliers of ITER error field correction criteria	3DSP	Park	PPPL	Yes	Breakout	Yes	Yes
197	Test the new method for finding the 3D perturbation needed to avoid tearing	3DSP	Kolemen	PPPL	Yes	Breakout	No	No
451	Combine the MM MHD spectroscopy, ML, RT DCON to control q95 and beta and modify the modes stability	3DSP	Munaretto	PPPL	Yes	Breakout	No	No
516	Role of Quasi-symmetric Magnetic Perturbations on LH-transition and pedestal transport	3DSP	Zarnstorff	Princeton U	Yes	Breakout	No	No
132	Disruption Prediction via Random Forests v2.0 and Interpretability	3DSP	Rea	Massachusetts Institute of Technology	Yes	Breakout	No	No
185	Exploring the role of nonlinear MHD in triggering tearing modes	3DSP	Chapman	U of Wisconsin	Yes	Breakout	No	No
186	Exploring the role of fluctuation-based dynamos in magnetic flux pumping	3DSP	Chapman	U of Wisconsin	Yes	Breakout	No	No

Click here for internal detailed listing Below is a public summary listing:

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Below is a public summary listing: