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 |
1 | Welcome to the ROF for the 2019-20 DIII-D Run Campaign | General Physics | Fenstermacher | LLNL | No | Breakout | No | No |
2 | testing, please ignore! | Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization | Coviello | GA | No | Breakout | No | No |
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 |
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 |
6 | H vs. D Core Transport Model Validation at High Te/Ti | Isotope mass Thrust | Grierson | GA | Yes | General | Yes | Yes |
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 |
8 | ECH Beat Wave Generation of ICE | Torkil Jensen | Grierson | GA | No | General | No | No |
9 | Improved H-mode access in mixed H/He plasmas | Isotope mass Thrust | Schmitz | UCLA | Yes | 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 |
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 |
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 |
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 |
20 | Ignition mechanism of arc by ELMs | Surface Evolution | Rohde | Max Planck Institut fuer Plasmaphysiks, Garching, Germany | No | General | 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 |
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 |
24 | Tuning of Controller/Observer Gains for n=1 and n=2 Resistive Wall Mode Control | Control | Battey | Columbia U | Yes | Breakout | No | No |
25 | How fast can we go? | Torkil Jensen | Victor | LLNL | Yes | 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 |
27 | Dependence of Ohmic energy confinement in negative triangularity diverted plasmas | Turbulence and transport | Thome | GA | No | 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 |
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 |
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 |
31 | Optimization of hydrogen H-mode transition targeting ITER's Pre Fusion Plasma Operation Stage | Isotope mass Thrust | Rhodes | UCLA | 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 |
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 |
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 |
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 |
37 | Wide Pedestal QH-Mode Path to Super H-Mode | Inductive Scenarios | Ernst | Massachusetts Institute of Technology | 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 |
39 | Revisit pellet triggered L-H transition and understand underlying turbulence suppression mechanisms | L-H transition | Kumar Barada | UCLA | 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 |
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 |
42 | Determine accuracy of NUBEAM power and torque outside mid-radius | Energetic Particle Physics | Chrystal | GA | No | Breakout | No | No |
43 | Low and mid-Z impurity density asymmetry | Turbulence and transport | Chrystal | GA | No | Breakout | No | No |
44 | Real time measurements of impurity density | Control | Chrystal | 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 |
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 |
47 | Divertor configuration effects on the L-H power threshold | L-H transition | Yan | U of Wisconsin | Yes | 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 |
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 |
50 | D2 pellet pacing with tangential injection | ELM Control | Wilcox | ORNL | Yes | Breakout | No | No |
51 | Deuterium poloidal rotation measurements using main ion CER spectroscopy | Rotation physics | Haskey | PPPL | Yes | Breakout | No | No |
52 | Pellet pacing with with peeling-limited pedestal | ELM Control | Wilcox | ORNL | Yes | 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 |
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 |
55 | Soft-landing of a major disruption using 3D fields | Torkil Jensen | Du | GA | Yes | General | No | No |
56 | Hunt the instabilities responsible for the formation of phase space hole | Energetic Particle Physics | Du | GA | No | General | No | No |
57 | Assess robustness of ITER baseline plasma response control | Inductive Scenarios | Hanson | Columbia U | No | Breakout | No | No |
58 | Assess robustness of ITER baseline plasma response control | 3DSP | Hanson | 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 |
60 | Measure and control resistive kink mode stability | 3DSP | 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 |
62 | Disruption Avoidance via ECCD Stabilization of Locked Islands and the Impact of Current Condensation | 3DSP | Reiman | PPPL | Yes | 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 |
64 | Liquid Metal Dust Break-up Mechanisms | Materials Migration and Mitigation | Andrew | Imperial College London | Yes | 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 |
66 | Impact of RMP on the L-H threshold | L-H transition | Diallo | PPPL | No | Breakout | No | No |
67 | Unraveling the mechanism linking the pedestal structure and its dynamics to ELM energy densities in ITER relevant regimes | Pedestal Physics and Pedestal Structure & QH Thrust | Diallo | PPPL | No | Breakout | No | No |
68 | Isotope Mass Scaling of Turbulence, Transport and Confinement | Isotope mass Thrust | McKee | U of Wisconsin | Yes | Breakout | Yes | No |
69 | EHO dominated sustained wide-pedestal QH-mode | Pedestal Physics and Pedestal Structure & QH Thrust | Kumar Barada | 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 |
71 | Role of scrape-off layer electric field in L-H power threshold scaling | L-H transition | Schmitz | UCLA | No | Breakout | No | No |
72 | H-mode access in electron-heat dominated ITER PFPO hydrogen plasmas | Isotope Mass Thrust | Schmitz | UCLA | Yes | 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 |
74 | Modify RE distribution function with externally launched helicon (whistler) waves | Torkil Jensen | Paz-Soldan | Columbia U | Yes | Breakout | No | No |
75 | RMP-ELM Suppression and Mitigation in Hydrogen Plasmas | Isotope Mass Thrust | Paz-Soldan | Columbia U | 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 |
78 | RMP-ELM Control in Strongly Shaped Plasmas | ELM Control | Paz-Soldan | Columbia U | Yes | Breakout | Yes | 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 |
81 | Snowflake SAS divertor | Impurity Radiative Divertor Dependence on Divertor Closure | Soukhanovskii | 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 |
84 | Clarify snowflake divertor physics | Advanced Magnetic Configurations | 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 |
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 |
88 | Exploring new reactor concepts: H-mode in negative triangularity diverted plasmas | Turbulence and transport | Marinoni | UCSD | No | 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 |
90 | Impurity transport in diverted negative triangularity discharges | Turbulence and transport | Sciortino | Max-Planck Institute for Plasma Physics | 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 |
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 |
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 |
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 |
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 |
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 |
98 | A new path to ELM mitigation | Torkil Jensen | Knolker | GA | Yes | 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 |
101 | ELM suppression by n=1 Ex-Vessel Coil at high qmin | Steady State Scenarios & High qmin Thrust | Hu | 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 |
103 | Comparison of high density ELM suppression in H and He to D | Isotope Mass Thrust | Evans | GA | No | Breakout | No | Yes |
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 |
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 |
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 |
108 | Measure and control resistive kink mode stability | Pedestal Physics and Pedestal Structure & QH Thrust | Hanson | Columbia U | 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 |
110 | Controlled ITB formation with narrow current channel | Steady State Scenarios & High qmin Thrust | Victor | LLNL | Yes | Breakout | No | No |
111 | Controlled ITB formation with narrow current channel | Torkil Jensen | Victor | LLNL | Yes | Breakout | No | No |
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 |
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 |
115 | Role of fueling in determining the pedestal structure | Isotope Mass Thrust | Mordijck | The college of William and Mary | No | Breakout | Yes | Yes |
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 |
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 |
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 |
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 |
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 |
124 | Characterization of Fast-ion Diagnostic to Edge Neutral Populations | Energetic Particle Physics | Stagner | GA | No | Breakout | No | No |
125 | Optimize BT for high qmin | Steady State Scenarios & High qmin Thrust | Park | ORNL | 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 |
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 |
128 | Dependence of upstream low-Z impurity accumulation on ExB drift direction | Materials Migration and Mitigation | Nichols | 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 |
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 |
131 | Isotope identity pair in H and D type I ELMy H-modes | Isotope mass Thrust | Maggi | CCFE | Yes | Breakout | Yes | No |
132 | Disruption Prediction via Random Forests v2.0 and Interpretability | 3DSP | Rea | Massachusetts Institute of Technology | Yes | Breakout | No | 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 |
135 | Reducing the L-H power threshold in H plasmas with pellets | Isotope mass Thrust | Wilcox | ORNL | Yes | 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 |
138 | Physics of pedestal turbulence vs width | Div/SOL Turbulence and transport | Boedo | UCSD | No | Breakout | No | No |
139 | ITER pedestal turbulence properties | Torkil Jensen | Boedo | UCSD | No | Breakout | No | No |
140 | Electron density up-down assymetry | Pedestal Physics and Pedestal Structure & QH Thrust | Mordijck | The college of William and Mary | No | Breakout | No | No |
141 | Isotope effect and the role of divertor geometry | Isotope Mass Thrust | Casali | U of Tennessee, Knoxville | Yes | Breakout | Yes | Yes |
142 | Helical core in high performance scenario | Turbulence and transport | Knolker | GA | 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 |
144 | Transport and turbulence in Divertor and pedestal during detachment | Div/SOL Turbulence and transport | Boedo | UCSD | 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 |
147 | Pellet Fueled High Density Operation of RMP ELM Mitigated Plasmas | ELM Control | Baylor | ORNL | 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 |
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 |
150 | Competition Between Intrinsic Torque and NTV for ITER | Rotation physics | Grierson | GA | No | 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 |
152 | Assessment of Ly-alpha opacity in fully detached divertor plasmas | Dissipative Divertor Physics | Groth | Aalto U | 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 |
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 |
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 |
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 |
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 |
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 |
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 |
168 | Extend Zero Torque Wide Pedestal QH-Mode Operation to IBS Parameters | Inductive Scenarios | Ernst | Massachusetts Institute of Technology | 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 |
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 |
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 |
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 |
177 | Evaluate the effect of penetration theory on RMP ELM suppression | ELM Control | WANG | ASIPP | Yes | Breakout | Yes | Yes |
178 | Use NBI to evaluate n=2 RMP penetration position | 3DSP | WANG | ASIPP | Yes | Breakout | Yes | Yes |
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 |
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 |
183 | Evaluate the effect of penetration theory on RMP ELM suppression | ELM Control | WANG | ASIPP | Yes | Breakout | Yes | Yes |
184 | Use NBI to evaluate n=2 RMP penetration position | 3DSP | WANG | ASIPP | Yes | Yes | Yes | |
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 |
187 | Scaling of 2D structure of detachment front | Dissipative Divertor Physics | Jarvinen | VTT Technical Research Centre | Yes | Breakout | No | No |
188 | Electron- and ion-heat dominated L-H transition regimes | L-H transition | Schmitz | UCLA | 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 |
190 | Impact of Current Condensation in the ECCD Stabilization of Rotating 2/1 NTMs | 3DSP | Bardoczi | GA | No | Breakout | No | No |
191 | What can lost fast-ions tell us about the H-mode pedestal? | Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization | Kramer | PPPL | No | Breakout | No | No |
192 | m/n=2/1 NTM control by ECCD in IBS | 3DSP | Bardoczi | GA | No | Breakout | No | No |
193 | Impact of molecular processes on divertor detachment and validation of UEDGE fluid molecular model | Dissipative Divertor Physics | Holm | PPPL | No | Breakout | No | No |
194 | Comparing the transport models experimentally | Turbulence and transport | Kolemen | PPPL | 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 |
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 |
197 | Test the new method for finding the 3D perturbation needed to avoid tearing | 3DSP | Kolemen | PPPL | Yes | Breakout | No | No |
198 | Radial structure and identification of intermediate frequency Alfven eignemodes | Energetic Particle Physics | Crocker | UCLA | No | Breakout | No | No |
199 | Machine Learning based Instability Prediction & Avoidance | 3DSP | Kolemen | PPPL | No | 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 |
201 | m/n=2/1 NTM control by ECCD in IBS | Control | Bardoczi | GA | No | 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 |
203 | Fast particle effects on transport of high Z ions with HFS asymmetry | Turbulence and transport | Odstrcil | GA | 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 |
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 |
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 |
208 | Investigation of high-Z impurity pump-out mechanism inside of saturated MHD modes | Turbulence and transport | Odstrcil | GA | Yes | Breakout | No | No |
209 | Isotope mass dependence of multichannel transport | Isotope Mass Thrust | Odstrcil | GA | Yes | 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 |
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 |
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 |
213 | Search for SOL impurity stagnation region | SOL Flows | Allen | LLNL | No | 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 |
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 |
216 | Test ExB shear importance in QH using co-Ip approach | Pedestal Physics and Pedestal Structure & QH Thrust | Chen | GA | Yes | 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 |
218 | The Disruption Free Protocol | Control | Barr | GA | 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 |
220 | Metastable multiphase tungsten compounds: toward new fusion friendly material?* | Innovative Materials Evaluation | Guterl | GA | 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 |
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 |
225 | Detachment onset with X-point height | Dissipative Divertor Physics | McLean | LLNL | Yes | Breakout | No | No |
226 | Controlling ITB formation via impurity puffing | DIII-D/EAST Task Force/Thrust | McClenaghan | GA | No | Breakout | No | No |
227 | Impact of plasma opacity on divertor detachment | Dissipative Divertor Physics | McLean | LLNL | 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 |
229 | Measure and control resistive kink mode stability | 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 |
231 | Study the high density branch of RMP ELM suppression in the IBS | ELM Control | Turco | Columbia U | Yes | Breakout | No | No |
232 | Impact of spectral contamination of the MWIR region | Dissipative Divertor Physics | McLean | LLNL | Yes | Breakout | No | No |
233 | Carbon flow in plasma crown | SOL Flows | Allen | 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 |
235 | Physics of real-time wall conditioning by B dust injection | Materials Migration and Mitigation | Bortolon | PPPL | No | Breakout | No | No |
236 | wide-pedestal QH in dominant electron-heated ITER PFPO hydrogen plasmas | Isotope Mass Thrust | Chen | GA | No | Breakout | No | No |
237 | Influence of isotope on H-mode density limit | Isotope Mass Thrust | Hong | UCLA | Yes | 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 |
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 |
240 | How much protection does detachment give us from ELMs? | Dissipative Divertor Physics | Samuell | LLNL | Yes | Breakout | Yes | 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 |
242 | Controlled low Z melting experiments using DiMES in support of ITER | Surface Evolution | Rudakov | UCSD | Yes | Breakout | Yes | Yes |
243 | Optimizing the process for developing 2D reconstructions of divertor conditions | Dissipative Divertor Physics | Samuell | LLNL | Yes | 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 |
245 | Characterizing Detachment in H-mode Helium Plasmas | Isotope mass Thrust | Samuell | LLNL | No | 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 |
247 | ExB drifts and paralel flows in divertor and SOL before/during detachment | SOL Flows | 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 |
249 | ExB drifts and paralel flows in divertor and SOL before/during detachment | SOL Flows | Boedo | UCSD | No | 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 |
251 | Methane Injection Changing D+ flows in SOL | SOL Flows | Boedo | UCSD | No | Breakout | No | No |
252 | Effect of divertor radiation front on drifts and parallel flow | Dissipative Divertor Physics | Boedo | UCSD | No | Breakout | No | No |
253 | Investigation and optimization of core and pedestal performance | Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization | Solomon | GA | No | Breakout | No | No |
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 |
255 | Contribution of molecules to radiated power | Dissipative Divertor Physics | McLean | LLNL | Yes | 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 |
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 |
258 | Deuterium lifecycle during ELM pacing with pellet injection | Pedestal Physics and Pedestal Structure & QH Thrust | Bortolon | PPPL | No | Breakout | No | No |
259 | Divertor to pedestal trace impurity transport | Div/SOL Turbulence and transport | Bortolon | PPPL | No | Breakout | No | 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 |
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 |
262 | Divertor-localized turbulence and characterization of 2D profiles of divertor turbulence | Div/SOL Turbulence and transport | Scotti | LLNL | No | Breakout | No | No |
263 | Impurity temperature screening in ITBs | Turbulence and transport | Sciortino | Max-Planck Institute for Plasma Physics | No | 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 |
265 | High Pedestal in Hybrid Scenario With Unfavorable Grad-B Drift Direction | Steady State Scenarios & High qmin Thrust | Petty | GA | No | Breakout | No | No |
266 | Test of Turbulence Spreading Using Turbulence Propagation | Turbulence and transport | Petty | GA | No | 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 |
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 |
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 |
270 | Evolution of edge turbulence and turbulence flow near midplane during divertor detachment | Div/SOL Turbulence and transport | Wang | UCLA | No | 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 |
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 |
273 | Scaling of blobby transport with divertor conditions and pedestal/SOL widening | Div/SOL Turbulence and transport | Boedo | UCSD | No | Breakout | No | No |
274 | edge/SOL turbulence with plasma isotopic mass scaling. | Isotope mass Thrust | Boedo | UCSD | No | Breakout | No | No |
275 | Divertor radiated power control in non-ELMing plasmas | Control | Eldon | GA | No | 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 |
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 |
279 | Isotope effect on the detachment rollover density | Isotope Mass Thrust | Solokha | Aalto U | No | No | No | |
280 | Physics requirements for high pressure staircase pedestal formation | Pedestal Physics and Pedestal Structure & QH Thrust | Nazikian | GA | Yes | 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 |
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 |
283 | Exploring Access Conditions to Standard QH and WPQH Pedestals | Pedestal Physics and Pedestal Structure & QH Thrust | 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 |
285 | Understanding the connection between ELM suppression and magnetic footprint size. | ELM Control | Munaretto | PPPL | 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 |
287 | Validation of the NIMROD results | Pedestal Physics and Pedestal Structure & QH Thrust | Pankin | PPPL | No | Breakout | No | No |
288 | Exploration of IBS variation with direct gain metric regulation | Control | Olofsson | Consultant | No | Breakout | No | No |
289 | Shape control enabled study of IBS stability as function of edge features | Control | Olofsson | Consultant | No | Breakout | No | No |
290 | Collisionality Dependence of Quasi-Coherent Fluctuations | Pedestal Physics and Pedestal Structure & QH Thrust | Ashourvan | GA | 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 |
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 |
293 | Divertor detachment control based on Langmuir Probes measurement | Control | Wang | GA | Yes | 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 |
295 | Pedestal Structure and Neutral Source Measurement | Pedestal Physics and Pedestal Structure & QH Thrust | Rosenthal | Massachusetts Institute of Technology | Yes | 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 |
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 |
298 | Optimize fast ion confinement in high qmin plasmas at high beta ! | Steady State Scenarios & High qmin Thrust | Nazikian | GA | Yes | 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 |
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 |
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 |
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 |
303 | ECEI and MIR contribution | ELM Control | Zhu | UC Davis | Yes | 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 |
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 |
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 |
311 | Proximity of tearing mode onset to ideal limits in high-beta plasmas | 3DSP | Turco | Columbia U | 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 |
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 |
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 |
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 |
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 |
320 | Access super H-mode in ITER Q=10 baseline target | Inductive Scenarios | Nazikian | GA | 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 |
323 | Tune RMP Controlled Phase of Locked Island and Radial Alignment of ECCD Deposition for Stabilization | Control | Reiman | PPPL | 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 |
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 |
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 |
329 | Magnetic geometry as an actuator for detachment stability and control | Advanced Magnetic Configurations | Samuell | LLNL | Yes | Breakout | No | 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 |
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 |
332 | Detachment at horizontal and vertical targets | Advanced Magnetic Configurations | Wang | GA | Yes | Breakout | No | No |
333 | Validation of Predict First Simulations using CCOANB 210 | Steady State Scenarios & High qmin Thrust | Grierson | GA | Yes | 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 |
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 |
337 | ECRH plasma production on DIII-D | Materials Migration and Mitigation | Wauters | LPP-ERM-KMS � Brussels � Belgium (EUROfusion member) | No | Breakout | Yes | Yes |
338 | Combining variable beam energy/perveance and NTV for rotation control | Control | Boyer | PPPL | No | Breakout | No | No |
339 | Detachment control w/ Te request translated to ne estimate & direct ne feedback | Control | 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 |
341 | Energy Confinement dependence on mass | Isotope mass Thrust | Thome | GA | No | Breakout | No | No |
342 | Vertical stability control with simulated horizontal interferometer channels | Control | Eldon | GA | No | Breakout | No | No |
343 | Check for Te cliff at inner strike point in reverse Bt | Dissipative Divertor Physics | Eldon | GA | No | Breakout | No | No |
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 |
345 | ECRH plasma production on DIII-D | Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools) | Wauters | LPP-ERM-KMS � Brussels � Belgium (EUROfusion member) | No | Breakout | Yes | Yes |
346 | Developing low-disruptivity ramp-down techniques for the ITER Baseline Scenario | Control | Barr | GA | No | Breakout | No | No |
347 | ITER plasma initiation and ECH assist | Control | Walker | GA | No | Breakout | Yes | Yes |
348 | Divertor configuration effects on the L-H power threshold in H plasmas | Isotope mass Thrust | Yan | U of Wisconsin | No | Breakout | 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 |
351 | Machine Learning based Instability Prediction & Avoidance | Control | Kolemen | PPPL | Yes | Breakout | No | No |
352 | Stationary Zonal Flows | L-H transition | Burrell | GA | No | Breakout | No | No |
353 | Wide pedestal QH-mode operation at lower Zeff | Pedestal Physics and Pedestal Structure & QH Thrust | Burrell | GA | No | Breakout | No | No |
354 | Study of impurity ion entrainment in divertor cross-field transport | Div/SOL Turbulence and transport | Hollmann | UCSD | No | Breakout | No | No |
355 | High fusion gain in the advanced inductive | Inductive Scenarios | Thome | GA | No | Breakout | No | No |
356 | ELM pacing by pellet injection in low-collisionality ITER relevant scenarios | ELM Control | Bortolon | PPPL | No | Breakout | No | No |
357 | Power loading at toroidal PFC gaps | Isotope Mass Thrust | Rudakov | UCSD | No | Breakout | Yes | Yes |
358 | Parallel correlation of turbulence/blobs between mid-plane and divertor SOL | Div/SOL Turbulence and transport | Rudakov | UCSD | No | 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 |
360 | LH power threshold, confinement scaling and CER calibration in carbon plasmas | L-H transition | Marinoni | UCSD | 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 |
362 | Fuel Ion Particle Transport using H/D Isotopes | Isotope Mass Thrust | McKee | U of Wisconsin | 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 |
365 | Power Threshold Studies in Mixed Ion Species Plasmas | Isotope Mass Thrust | Plank | IPP Garching | Yes | Breakout | Yes | Yes |
366 | DIII-D Experiments in Support of ITPA DSOL Detachment Research | Dissipative Divertor Physics | Reinke | ORNL | Yes | Breakout | Yes | 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 |
368 | Limits of RMP ELM Suppression Toward Double Null | ELM Control | Shafer | ORNL | Yes | Breakout | No | No |
369 | Limits of RMP ELM Suppression Toward Double Null | ELM Control | Shafer | ORNL | Yes | 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 |
371 | ICE Mode Structure | Energetic Particle Physics | DeGrandchamp | UC, Irvine | Yes | Breakout | Yes | No |
372 | whistler polarization | Disruption Mitigation Thrust | Heidbrink | UC, Irvine | No | Breakout | No | No |
373 | Measuring net and gross erosion rates of SiC in DIII-D divertor at forward Bt | Surface Evolution | Rudakov | UCSD | Yes | 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 |
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 |
377 | RMP ELM suppression for inductive Hybrid plasmas relevant to the ITER Q=10 mission | Inductive Scenarios | Nazikian | GA | Yes | Breakout | No | No |
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 |
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 |
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 |
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 |
385 | Effect of 3D fields on turbulence and transport in DIII-D plasmas | Turbulence and transport | Kumar Barada | UCLA | Yes | Breakout | No | No |
386 | Complete plasma turbulence measurements of DIII-D L-mode plasmas | Turbulence and transport | Burke | LLNL | Yes | 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 |
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 |
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 |
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 |
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 |
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 |
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 |
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 |
400 | Verification of Imaging Fast Ion D-Alpha and application to EP model validation | Energetic Particle Physics | Marini | ORAU | Yes | Breakout | No | No |
401 | Determine the critical gradient in negative triangularity discharges | Turbulence and transport | Austin | U of Texas, Austin | 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 |
403 | Burn Condition Emulation for ITER-relevant Control Experiments | Control | Schuster | Lehigh U | No | 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 |
405 | Max-Planck-Institut f�¼r Plasmaphysik | ELM Control | Willensdorfer | Max-Planck-Institut f�¼r Plasmaphysik | 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 |
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 |
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 |
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 |
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 |
413 | Redistribute plasma momentum and particles in divertor due to the coupling of drift and sheath | SOL Flows | Wang | GA | Yes | Breakout | No | No |
414 | Quasi-coherent fluctuations near the divertor plate | Div/SOL Turbulence and transport | Wang | GA | No | 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 |
416 | Characterization of pedestal/SOL coupling at X-point in detached conditions | Dissipative Divertor Physics | Jarvinen | VTT Technical Research Centre | Yes | Breakout | No | No |
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 |
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 |
421 | Magnetic shear at X-point and radial turbulence transport | Div/SOL Turbulence and transport | Boedo | UCSD | No | Breakout | No | No |
422 | Increase "intrinsic" edge rotation via control of edge stochasticity | Rotation physics | Schmitz | UCLA | No | 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 |
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 |
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 |
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 |
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 |
429 | Real time neutron control | Control | Heidbrink | UC, Irvine | No | 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 |
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 |
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 |
435 | Fully non-inductive high betap scenario at q95~6-7 | DIII-D/EAST Task Force/Thrust | Huang | ASIPP | 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 |
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 |
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 |
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 |
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 |
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 |
442 | Access to small ELM regime in DIII-D high �²P scenario | DIII-D/EAST Task Force/Thrust | Qian | ASIPP | No | Breakout | Yes | Yes |
443 | Compatibility of highly radiative divertor with high beta_p scenario | DIII-D/EAST Task Force/Thrust | Wang | ASIPP | Yes | Breakout | No | 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 |
447 | Optimizing Transport Through Magnetic Shear | Steady State Scenarios & High qmin Thrust | McKee | U of Wisconsin | No | Breakout | No | No |
448 | Optimizing core-pedestal performance in Super H-Mode | Core-Edge Integration Task Force incorporating Thrust: Core-Edge Scenario Optimization | Snyder | ORNL | No | Breakout | No | No |
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 |
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 |
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 |
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 |
454 | Validating Dominant Micro-Turbulence Instabilities in DIII-D high BetaP Scenarios | DIII-D/EAST Task Force/Thrust | Jian | GA | 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 |
456 | Stabilization of TAEs by Localized Electron Cyclotron Current Drive | Energetic Particle Physics | Sharapov | CCFE | No | Breakout | Yes | No |
457 | m/n=2/1 NTM control by ECCD in steady state hybrid | 3DSP | Bardoczi | GA | No | Breakout | No | No |
458 | m/n=2/1 NTM control by ECCD in steady state hybrid | Control | 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 |
460 | Use pellets to enable 2/1 NTM stabilization with very low gyrotron power | Torkil Jensen | Bardoczi | GA | No | Breakout | No | No |
461 | Pedestal and core transport comparison of SAS , upper closed, and lower open divertor | Particle Balance and Impact of Divertor Closure Including SAS on Detachment Thrust | Osborne | GA | No | Breakout | No | No |
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 |
463 | QH-mode with detached divertor | Particle Balance and Impact of Divertor Closure Including SAS on Detachment Thrust | Osborne | 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 |
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 |
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 |
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 |
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 |
470 | Measuring intra-ELM D recycling on pre-exposed W surfaces | Surface Evolution | Sinclair | Oak Ridge Associated Universities | 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 |
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 |
476 | Pedestal dimensionless parameter match DIII-D to JET for H,D,He | Isotope Mass Thrust | Osborne | GA | No | Breakout | No | No |
477 | Optimizing NTV torque profiles with multi-modal 3D control | 3DSP | Weisberg | 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 |
479 | ITG and TEM's impacts on toroidal rotation profile and intrinsic rotation | Rotation physics | Qin | U of Wisconsin | No | 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 |
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 |
482 | Pyroid HT Material Assessment using DiMES | Innovative Materials Evaluation | Wukitch | Massachusetts Institute of Technology | Yes | 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 |
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 |
485 | Third harmonic ECH experiments | Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools) | Schneider | ITER Organization | 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 |
488 | Steady-State Hybrids in Hydrogen With Higher Bootstrap Fraction | Steady State Scenarios & High qmin Thrust | Petty | GA | No | Breakout | No | No |
489 | Developing low-disruptivity ramp-down techniques for the ITER Baseline Scenario | Inductive Scenarios | Barr | GA | No | Breakout | No | No |
490 | BAAE and BAE validation | Energetic Particle Physics | Heidbrink | UC, Irvine | No | Breakout | Yes | No |
491 | Spectroscopic inference of tungsten re-deposition fractions | Surface Evolution | Abrams | GA | No | Breakout | No | No |
492 | Understanding outliers of ITER error field correction criteria | 3DSP | Park | PPPL | Yes | Breakout | Yes | Yes |
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 |
495 | SAS, meet DN | Advanced Magnetic Configurations | Thomas | GA | Yes | Breakout | No | No |
496 | Orbit Tomography (OT) | Energetic Particle Physics | Garcia | UC, Irvine | No | Breakout | Yes | No |
497 | Reducing the L-H power threshold in D plasmas with pellets | L-H transition | Wilcox | ORNL | 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 |
500 | Tracking erosion and redeposition of crystalline SiC in the DIII-D divertor | Surface Evolution | Sinclair | GA | Yes | 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 |
502 | Scaling of turbulence properties with ion mix | Isotope mass Thrust | Carter | UCLA | Yes | 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 |
504 | Helicon Launcher Checkout and Conditioning | Heating & Current Drive Physics (including Thrust: Validation of New Current Drive Tools) | Zhang | ASIPP | No | Breakout | No | No |
505 | Assessing Helicon wave current drive in high betap experiments | DIII-D/EAST Task Force/Thrust | Zhang | ASIPP | No | Breakout | No | No |
506 | PCS supervisory algorithm for negotiating complex controller requests | Control | Eidietis | GA | No | Breakout | No | No |
507 | ITER DMS design validation | Disruption Mitigation Thrust | Lehnen | ITER Organization | No | 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 |
509 | Exposure of Graphitic foam at DiMES and Tile | Innovative Materials Evaluation | Unterberg | ORNL | No | Breakout | No | No |
510 | Superposition of identical dual SPIs | Disruption Mitigation Thrust | Herfindal | ORNL | 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 |
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 |
513 | Boundary Ion temperature measurement based on retarding field analyzer | Divertor Closure | Ren | U of Tennessee, Knoxville | Yes | 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 |
515 | Parameter scan of fast-ion critical gradient threshold | Energetic Particle Physics | Collins | ORNL | No | Breakout | No | No |
516 | Role of Quasi-symmetric Magnetic Perturbations on LH-transition and pedestal transport | 3DSP | Zarnstorff | Princeton U | Yes | Breakout | No | No |
517 | Penetration characterization of small pellet injection into D3D plasmas | Disruption Mitigation Thrust | Raman | U of Washington | No | Breakout | No | No |
518 | Dimensionless scaling of pedestal height, width and stability - a turbulence & transport perspective | Pedestal Physics and Pedestal Structure & QH Thrust | Banerjee | PPPL | No | Breakout | No | No |
519 | Role of poloidal rotation on pedestal instabilities | Pedestal Physics and Pedestal Structure & QH Thrust | Pankin | PPPL | 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 |
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 |
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 |
533 | Ballistic transport and energy/size scaling for SPI | Disruption Mitigation Thrust | Shiraki | ORNL | No | Breakout | No | No |
534 | Doublet shape in DIII-D | Torkil Jensen | Austin | U of Texas, Austin | 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 |
536 | Helium scenarios for ITER | Isotope mass Thrust | Marinoni | UCSD | No | Breakout | Yes | No |
537 | ELM pacing during ITER-like current ramp-up/down | ELM Control | Bortolon | PPPL | No | Breakout | No | Yes |
538 | Expanding the Wide Pedestal QH to IBS Parameters | Inductive Scenarios | Chen | GA | No | Breakout | No | No |
539 | Effect of underlying non-axisymmetric (NA) fields on disruption mitigation process | Disruption Mitigation Thrust | Eidietis | GA | No | Breakout | No | No |
540 | SAS 2 precursor experiments | Particle Balance and Detachment Characterization in Closed Divertors Thrust | Watkins | Sandia National Lab | Yes | Breakout | No | No |
541 | Soliton like Shock Front Dynamics during Pellet Deposition in H-mode | Torkil Jensen | Baylor | ORNL | Yes | Breakout | No | No |
542 | LH power threshold, confinement scaling and CER calibration in carbon plasmas | Torkil Jensen | Marinoni | UCSD | No | Breakout | No | No |
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 |
546 | Direct measurement of the wave-particle interactions and associated phase space flow | Energetic Particle Physics | Du | GA | No | Breakout | No | No |
547 | Direct measurement of the wave-particle interactions and associated phase space flow | Energetic Particle Physics | du | General Atomic | No | Breakout | No | No |
548 | Effect of outer gap on wide-pedestal QH-mode | Pedestal Physics and Pedestal Structure & QH Thrust | Garofalo | GA | No | Breakout | No | No |
549 | Further investigation of the saturation & underlying transport mechanism of EHO to allow ELM stable | Pedestal Physics and Pedestal Structure & QH Thrust | Chen | GA | No | Breakout | No | No |
550 | What's the physics leads to std QH, Wide Pedestal QH,or ELMing IBS from L-mode at low torque? | Pedestal Physics and Pedestal Structure & QH Thrust | Chen | GA | No | Breakout | No | No |
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 |
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 |
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 |
554 | ELM pacing during ITER-like current ramp-up/down | ELM Control | Bortolon | PPPL | No | Breakout | No | Yes |
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 |
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 |
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 |
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 |
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 |
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 |
561 | Experimental Validation of Heteroclitic magnetic Island Bifurcations in DIII-D | General Physics | Evans | GA | No | Breakout | No | No |
562 | Minimizing W divertor leakage in the SAS | Impact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential Thrust | Unterberg | ORNL | No | Breakout | No | No |
563 | Probe RWM stability using off-axis NBI | Steady State Scenarios & High qmin Thrust | Hanson | Columbia U | No | Breakout | No | No |
564 | Impact of high-Z PFCs on impurity seeding experiments in SAS | Impact of Divertor Geometry on Divertor Leakage and SOL Impurity Transport - SAS-1W Potential Thrust | Casali | U of Tennessee, Knoxville | No | Breakout | No | No |
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 |