DIII-D RESEARCH OPPORTUNITIES FORUM FOR THE 2018 EXPERIMENTAL CAMPAIGN
You are not logged in. Click here to log in for more options. 2017 ROF Ideas: Click here for ROF2017 submissions |
ID | Title | Research Area | Name | Affiliation |
Time Req'ed |
ITPA Joint Exp |
ITER IO Urgent Research Task |
385 | Low energy NBI for efficient angular momentum injection | Torkil Jensen Award | Eidietis | GA | Yes | No | No |
387 | Can Pellets Completely Stabilize the deleterious 2/1 NTMs? | Torkil Jensen Award | Bardoczi | GA | Yes | No | No |
502 | Exploring new reactor concepts: H-mode at negative triangularity | Torkil Jensen Award | Marinoni | UCSD | Yes | No | No |
375 | Advanced tokamak core with Super-H pedestal | Torkil Jensen Award | Victor | LLNL | Yes | No | No |
655 | World first deuterium poloidal rotation measurements using main ion CER spectroscopy | Torkil Jensen Award | Haskey | PPPL | Yes | No | No |
660 | Poloidal rotation measurements using main ion CER spectroscopy | Thrust 4 - Rotation Physics | Haskey | PPPL | No | No | No |
403 | Investigate impact of energetic particles on neoclassical toroidal viscosity | Thrust 4 - Rotation Physics | Wang | PPPL | Yes | No | No |
510 | Turbulence and core intrinsic rotation hollowing | Thrust 4 - Rotation Physics | Stoltzfus-Dueck | PPPL | No | No | No |
359 | Effect of beam tangency on locking threshold | Thrust 4 - Rotation Physics | Ferraro | PPPL | No | No | No |
369 | Role of micro-turbulence in intrinsic rotation reversals through JET DIII-D similarity experiments | Thrust 4 - Rotation Physics | Nave | Instituto Superior Tecnico, Lisboa, Portugal | Yes | No | No |
340 | Improved stability of counter rotating plasmas | Thrust 4 - Rotation Physics | Victor | LLNL | Yes | No | No |
366 | Using up/down asymmetry to Increase the intrinsic rotation | Thrust 4 - Rotation Physics | Victor | LLNL | Yes | No | No |
623 | Intrinsic rotation drive and RS asymmetries with geometry. USN/LSN and poloidal variation | Thrust 4 - Rotation Physics | Boedo | UCSD | No | No | No |
551 | Intrinsic Rotation in a Negative Triangularity Plasma | Thrust 4 - Rotation Physics | Ashourvan | GA | No | No | No |
530 | Intrinsic Rotation and Core Transport in Wide Pedestal QH-Mode with Electron Heating | Thrust 4 - Rotation Physics | Ernst | Massachusetts Institute of Technology | Yes | No | No |
520 | Intrinsic rotation in detached divertor | Thrust 4 - Rotation Physics | Grierson | GA | No | No | No |
348 | Intrinsic Rotation Dependence on Plasma Shape | Thrust 4 - Rotation Physics | deGrassie | GA | No | No | No |
469 | Effect of neutrals on edge momentum transport | Thrust 4 - Rotation Physics | Chrystal | GA | No | No | No |
585 | Er dependency of NTV | Thrust 4 - Rotation Physics | Lee | National Fusion Research Institute | No | No | No |
621 | QH-mode similarity experiment between DIII-D and AUG with co-current beams | Thrust 3 - ELM Control | Viezzer | U of Seville | Yes | No | No |
523 | ELM suppression in a matched KSTAR shape with n=2 fields | Thrust 3 - ELM Control | Evans | GA | No | No | No |
524 | ELM suppression in a matched KSTAR shape with n=2 fields | Thrust 3 - ELM Control | Evans | GA | No | No | No |
571 | Imaging of the ELM suppression mechanism using MIR and ECEI | Thrust 3 - ELM Control | Zhu | UC Davis | Yes | No | No |
427 | Super H-mode Access by Counter Beam Injection with n=3 RMP. | Thrust 3 - ELM Control | Nazikian | GA | Yes | No | No |
430 | Extend broad pedestal QH regime to high power and high density | Thrust 3 - ELM Control | Nazikian | GA | Yes | No | No |
420 | Low n, Low Field ELM-suppression with edge ECCD | Thrust 3 - ELM Control | Logan | Columbia U | No | No | No |
352 | Direct comparison of ITER similar shape (ISS) and ITER baseline scenario (IBS) plasmas for RMP-ELM | Thrust 3 - ELM Control | Paz-Soldan | Columbia U | No | No | No |
526 | Explore rotation thresholds with variable upper triangularity | Thrust 3 - ELM Control | Paz-Soldan | Columbia U | No | No | No |
417 | QH-mode with zero torque throughout | Thrust 3 - ELM Control | Burrell | GA | No | No | No |
480 | Magnetic topology identification by dual soft X-ray camera system during non-rotating n=2 RMP | Thrust 3 - ELM Control | Du | GA | No | No | No |
518 | Further investigation of the saturation & underlying transport mechanism of EHO to allow ELM stable | Thrust 3 - ELM Control | Chen | GA | Yes | No | No |
351 | Development of the low-torque wide-pedestal QH-mode with EHO | Thrust 3 - ELM Control | Chen | GA | Yes | No | No |
371 | plasma response to n=2 rotating RMP with q95 scan between 4 and 6 | Thrust 3 - ELM Control | Liu | GA | No | No | No |
583 | Effect of prompt and delayed fuel re-emission on apparent SP footprint during ELMs | Thrust 3 - ELM Control | Bykov | GA | Yes | No | No |
592 | Toroidally-resolved lobe dynamics in ELM-mitigated and ELM-suppressed scenarios | Thrust 3 - ELM Control | Bykov | GA | Yes | No | No |
579 | Wide Pedestal QH-Mode Core and Pedestal Compatibility with Electron Heating | Thrust 3 - ELM Control | Ernst | Massachusetts Institute of Technology | Yes | No | No |
501 | Pellet ELM pacing with field aligned tangential injection | Thrust 3 - ELM Control | Baylor | ORNL | No | No | Yes |
355 | Rotating n=2 fields with edge ECCD to reduce ELM suppression threshold amplitude | Thrust 3 - ELM Control | Wilcox | ORNL | Yes | No | No |
487 | RMP ELM mitigation and suppression in the Super H-Mode regime | Thrust 3 - ELM Control | Snyder | ORNL | Yes | No | No |
541 | Plasma Response and ELM Supssion Dependence on SN v DN | Thrust 3 - ELM Control | Shafer | ORNL | No | No | No |
572 | Imaging of the ELM suppression mechanism using MIR and ECEI | Thrust 3 - ELM Control | Zhu | UC, Davis | Yes | No | No |
586 | Improve pedestal of wide-pedestal QH-mode with ECH and RMP and study the effect on LCOs | Thrust 3 - ELM Control | Kumar Barada | UCLA | Yes | No | No |
620 | QH-mode without NBI | Thrust 3 - ELM Control | Bortolon | PPPL | No | No | No |
543 | ELMs and ELM mitigation during ITER relevant Ip ramp-up/down | Thrust 3 - ELM Control | Bortolon | PPPL | No | No | No |
517 | n=1 RMP ELM suppression with full I+C coil optimization | Thrust 3 - ELM Control | Park | PPPL | Yes | No | No |
445 | Effect of plasma rotation on ELM suppression threshold and density pump-out by RMPs | Thrust 3 - ELM Control | Hu | PPPL | No | No | No |
563 | ELM suppression with rotation control with NBI voltage | Thrust 3 - ELM Control | Kolemen | PPPL | No | No | No |
466 | Control with new real-time Pedestal CER system | Thrust 3 - ELM Control | Kolemen | PPPL | No | No | No |
478 | ELM pacing using impurity pellet injection | Thrust 3 - ELM Control | Laggner | North Carolina State | No | No | No |
479 | The hysteresis between the access of ELM suppression and its exit | Thrust 3 - ELM Control | Laggner | North Carolina State | Yes | No | No |
663 | Role of the turbulent transport due to a broadband MHD in association with a change in Er structure | Thrust 3 - ELM Control | Ono | QST | No | No | No |
488 | n=1 RMP ELM suppression (in conjunction with intrinsic error fields, phasing and shape dependence) | Thrust 3 - ELM Control | In | Ulsan National Institute of Science and Technolog | Yes | No | No |
560 | Understanding divertor closure's effect on power dissipation and radiation by impurity seeding | Thrust 2 - Divertor Development | Casali | U of Tennessee, Knoxville | No | No | No |
561 | Understanding divertor closure's effect on SOL impurity transport | Thrust 2 - Divertor Development | Casali | U of Tennessee, Knoxville | No | No | No |
644 | Impact of main ion dilution on core and edge turbulence and transport in high performance IBSs | Thrust 2 - Divertor Development | Marinoni | UCSD | No | No | No |
527 | Comparison of pumping with private flux and shared flux pumping in attached and detached plasmas | Thrust 2 - Divertor Development | Luce | ITER Organization | No | No | No |
544 | Detachment dependence on neutral pressure in the SAS divertor | Thrust 2 - Divertor Development | Shafer | ORNL | No | No | No |
678 | Characterizing misalignment between SAS and magnetic field | Thrust 2 - Divertor Development | Moser | GA | No | No | No |
569 | Effect of SAS divertor on pedestal | Thrust 2 - Divertor Development | Moser | GA | No | No | No |
635 | Convex mirror on DiMES to view upper SAS | Thrust 2 - Divertor Development | Bykov | GA | No | No | No |
627 | Impact of siliconization on SAS divertor performance | Thrust 2 - Divertor Development | Abrams | GA | Yes | No | No |
398 | Magnetic Balance Combined with Divertor Closure and Its Effect on Radiating Diverter Performance | Thrust 2 - Divertor Development | Petrie | GA | No | No | No |
401 | The Most Effective Radiating Divertor That DIII-D Can Presently Make in the DN Shape | Thrust 2 - Divertor Development | Petrie | GA | No | No | No |
677 | Effect of RMP application on the dissipative divertor regime | Thrust 2 - Divertor Development | Schmitz | UW Madison | No | Yes | Yes |
630 | ELM suppression in the SAS | Thrust 2 - Divertor Development | Nazikian | GA | Yes | No | No |
587 | SAS meets DN | Thrust 2 - Divertor Development | Thomas | GA | No | No | No |
464 | Assessing the importance of intrinsic carbon radiation and D2 molecules in SAS 1 power dissipation | Thrust 2 - Divertor Development | Covele | GA | Yes | No | No |
460 | Detachment facilitation with flux expansion in the SAS 1 slot | Thrust 2 - Divertor Development | Covele | GA | Yes | No | No |
426 | Extend robust ELM suppression to the Q=10 ITER baseline scenario. | Thrust 1 - ITER Q=10 (Inductive Scenarios) | Nazikian | GA | Yes | Yes | No |
626 | RMP ELM suppression in the IBS with radiating divertor by Ar injection | Thrust 1 - ITER Q=10 (Inductive Scenarios) | Turco | Columbia U | Yes | Yes | No |
512 | Effect of EC location and heat/CD on the confinement and stability of the IBS | Thrust 1 - ITER Q=10 (Inductive Scenarios) | Turco | Columbia U | Yes | No | No |
449 | Exploit and explore the new stable zero torque ITER Baseline Scenario | Thrust 1 - ITER Q=10 (Inductive Scenarios) | Turco | Columbia U | Yes | No | No |
450 | Stable zero torque IBS with dominant e- heating and low collisionality | Thrust 1 - ITER Q=10 (Inductive Scenarios) | Turco | Columbia U | Yes | No | No |
451 | ITER Baseline Scenario with zero and negative rotation | Thrust 1 - ITER Q=10 (Inductive Scenarios) | Turco | Columbia U | Yes | No | No |
353 | Increase normalized beta of torque-free 3rd harmonic EC heated ITER baseline scenario plasmas | Thrust 1 - ITER Q=10 (Inductive Scenarios) | Paz-Soldan | Columbia U | No | No | No |
368 | Get Advance Inductive QH Mode to Zero Torque | Thrust 1 - ITER Q=10 (Inductive Scenarios) | Buttery | GA | Yes | No | No |
399 | Access and control of QH-mode in IBS at low NBI torque | Thrust 1 - ITER Q=10 (Inductive Scenarios) | Garofalo | GA | Yes | No | Yes |
553 | Test compatibility of radiative divertor with QH-mode | Thrust 1 - ITER Q=10 (Inductive Scenarios) | Garofalo | GA | Yes | No | No |
528 | ECCD-induced ELM suppression in low-torque ITER-baseline scenario | Thrust 1 - ITER Q=10 (Inductive Scenarios) | Lyons | GA | Yes | No | No |
636 | Safety Factor Profile Optimization of Wide Pedestal QH-Mode for Electron Heating | Thrust 1 - ITER Q=10 (Inductive Scenarios) | Ernst | Massachusetts Institute of Technology | Yes | No | No |
648 | Extend Zero Torque Wide Pedestal QH-Mode Operation to IBS Parameters | Thrust 1 - ITER Q=10 (Inductive Scenarios) | Ernst | Massachusetts Institute of Technology | Yes | No | No |
419 | Search for path towards zero torque QH-mode for IBS and scaling of critical ExB shear requirements | Thrust 1 - ITER Q=10 (Inductive Scenarios) | Wilks | Massachusetts Institute of Technology | Yes | No | No |
625 | Measuring the effect of edge Z effective on RMP ELM suppression via impurity injection | Thrust 1 - ITER Q=10 (Inductive Scenarios) | Weisberg | GA | No | No | No |
452 | ITER Baseline Scenario at Zero and Negative Rotation | Thrust 1 - ITER Q=10 (Inductive Scenarios) | Luce | ITER Organization | No | Yes | No |
611 | Radiative divertor solutions in the ITER baseline scenario | Thrust 1 - ITER Q=10 (Inductive Scenarios) | Luce | ITER Organization | No | Yes | No |
500 | Test advanced inductive performance vs q95 at fixed B | Thrust 1 - ITER Q=10 (Inductive Scenarios) | Luce | ITER Organization | No | No | No |
505 | Revisit zero torque advanced inductive scenario | Thrust 1 - ITER Q=10 (Inductive Scenarios) | Luce | ITER Organization | No | No | No |
557 | Controlling the plasma edge rotation for QH-mode access | Thrust 1 - ITER Q=10 (Inductive Scenarios) | Kolemen | PPPL | No | No | No |
442 | Stability of Plasma with Derivative of Current Profile Equal to zero | Thrust 1 - ITER Q=10 (Inductive Scenarios) | Kolemen | PPPL | No | No | No |
647 | ELMs and ELM pacing in an ITER-baseline without NBI | Thrust 1 - ITER Q=10 (Inductive Scenarios) | Bortolon | PPPL | No | No | No |
519 | ELM suppression in the low torque IBS using rotating n=2 fields | Thrust 1 - ITER Q=10 (Inductive Scenarios) | Wang | PPPL | Yes | No | No |
410 | Characterize the pedestal particle transport induced by RMP | PE - Pedestal/SOL Physics and Pedestal Optimization | Diallo | PPPL | No | No | No |
605 | Validate EPED and Eich's ELM model in He plasmas | PE - Pedestal/SOL Physics and Pedestal Optimization | Bortolon | PPPL | No | No | No |
672 | Understanding the physics of RMP density pump-out | PE - Pedestal/SOL Physics and Pedestal Optimization | Sung | KAIST | No | No | No |
582 | Sustain and investigate EDA H-mode regime at near zero torque | PE - Pedestal/SOL Physics and Pedestal Optimization | Kumar Barada | UCLA | Yes | No | No |
506 | Reproduce past IBS He plasmas in D to compare H-mode characteristics for ITER | PE - Pedestal/SOL Physics and Pedestal Optimization | Marinoni | UCSD | No | No | No |
619 | Study of ELM Dynamics using Fast Main-Ion CER | PE - Pedestal/SOL Physics and Pedestal Optimization | Ashourvan | GA | No | No | No |
421 | Impact of shape and q95 on QH-mode EHO behavior | PE - Pedestal/SOL Physics and Pedestal Optimization | Wilks | Massachusetts Institute of Technology | Yes | No | No |
486 | Super H-Mode Pedestal Optimization: Effect of fuelling source, density and current | PE - Pedestal/SOL Physics and Pedestal Optimization | Snyder | ORNL | Yes | No | No |
631 | Further investigation of the saturation & underlying transport mechanism of EHO to allow ELM stable | PE - Pedestal/SOL Physics and Pedestal Optimization | Chen | GA | No | No | No |
367 | ELM studies close to LH boundary | PE - Pedestal/SOL Physics and Pedestal Optimization | Knolker | GA | Yes | Yes | No |
467 | The effects of divertor detachment on pedestal width scaling | PE - Pedestal/SOL Physics and Pedestal Optimization | Wang | GA | Yes | No | No |
444 | Displacement between the density and temperature pedestal | PE - Pedestal/SOL Physics and Pedestal Optimization | Wang | GA | Yes | No | No |
492 | Does the edge localized pedestal particle source directly effect pedestal structure | PE - Pedestal/SOL Physics and Pedestal Optimization | Osborne | GA | No | No | No |
354 | Pedestal Stability in ELM free ECH H-mode | PE - Pedestal/SOL Physics and Pedestal Optimization | Chrystal | GA | No | No | No |
370 | Control of the inter-ELM pedestal fluctuations | PE - Pedestal/SOL Physics and Pedestal Optimization | Laggner | Princeton Universtiy | Yes | No | No |
411 | Characterize the pedestal particle transport induced by RMP | PE - Pedestal/SOL Physics and Pedestal Optimization | Diallo | PPPL | No | No | No |
493 | I-mode identity experiment on DIII-D and ASDEX Upgrade: access, performance and transport | PE - Pedestal/SOL Physics and Pedestal Optimization | Happel | Max-Planck-Institut f�¼r Plasmaphysik | Yes | Yes | No |
494 | I-mode identity experiment on DIII-D and ASDEX Upgrade: access, performance and transport | PE - Pedestal/SOL Physics and Pedestal Optimization | Happel | Max-Planck-Institut f�¼r Plasmaphysik | Yes | Yes | No |
409 | Isotope scaling at fixed grad-te | General Physics | scott | PPPL | Yes | No | No |
640 | Aimed visible/NIR spectroscopy for measurement of impurity flux from natural hot spots | General Physics | Bykov | GA | Yes | No | No |
614 | Non thermal contribution to MWIR during ELMs, disruptions and in detachment (ROF2017 #177) | General Physics | Bykov | GA | No | No | No |
670 | Validation of high-Z dust ablation models in edge plasma | General Physics | Guterl | GA | Yes | No | No |
675 | Compare Er measured by DBS and CER in important DIII-D plasmas | General Physics | Kumar Barada | UCLA | Yes | No | No |
338 | Welcome to the 2018 ROF - note you don't need to re-enter last year's proposals | General Physics | Fenstermacher | LLNL | No | No | No |
549 | Helium Campain 2018 | General Physics | Samuell | LLNL | Yes | No | No |
491 | Boron and Boron Carbide granule injection for real time wall conditioning | General Physics | Lunsford | PPPL | No | No | No |
578 | Establish in-shot boronization for low collisionality operation | General Physics | Bortolon | PPPL | No | No | No |
535 | Extend fully non-inductive high betap scenario to Ip~1MA towards Q=5 mission of ITER | EAST - Scenarios and Transport | Huang | ASIPP | Yes | No | No |
436 | Development of high betaP scenario with active pedestal control | EAST - Scenarios and Transport | Qian | ASIPP | No | No | No |
437 | Exploration of Fully Non-inductive High �²p Scenarios with QH-mode Edge | EAST - Scenarios and Transport | Qian | ASIPP | No | No | No |
628 | Understanding the limits of confinement from internal transport barriers | EAST - Scenarios and Transport | McClenaghan | GA | No | No | No |
485 | Investigate the Turbulence Suppression in High Betap Plasmas when Te is Close to Ti | EAST - Scenarios and Transport | Ding | GA | Yes | No | No |
361 | RMP ELM suppression in the high betaP scenario at lower q95 | EAST - Control and Stability | Weisberg | GA | No | No | No |
552 | Understanding W edge transport via introducing a well-defined W source | EAST - Boundary | Ding | ASIPP | Yes | No | No |
642 | Testing and control of radiation divertor with neon and argon seeding in high beta_p scenario | EAST - Boundary | Wang | ASIPP | Yes | No | No |
622 | Effect of divertor turbulence on upstream pedestal/SOL | DDS - Turbulence | Boedo | UCSD | No | No | No |
390 | Study properties of the singularity that is the X-point | DDS - Turbulence | Boedo | UCSD | No | No | No |
391 | Turbulnce in detaching and detached divertor | DDS - Turbulence | Boedo | UCSD | No | No | No |
607 | Effect on SEE on Langmuir probe measurements in the SOL | DDS - Turbulence | Rudakov | UCSD | No | No | No |
468 | Enhanced quasi-coherent fluctuations and associated transport in detached plasmas | DDS - Turbulence | Wang | GA | No | No | No |
472 | Effects of radiative fluctuations and current convective instability on detachment | DDS - Turbulence | Guterl | GA | Yes | No | No |
343 | Mapping the Te cliff using detachment control | DDS - Drifts and Flows | Eldon | GA | No | No | No |
344 | Search for Te cliff at inner strike point in reverse Bt | DDS - Drifts and Flows | Eldon | GA | No | No | No |
661 | Effect of pumping on secondary strike point | DDS - Drifts and Flows | Eldon | GA | No | No | No |
584 | Divertor detachment in closed divertor with unfavorable Bt | DDS - Drifts and Flows | Wang | GA | No | No | No |
392 | DIvertor and pedestal flows in attached and detached plasmas | DDS - Drifts and Flows | Boedo | UCSD | No | No | No |
393 | ExB drifts in detached divertor and X-point | DDS - Drifts and Flows | Boedo | UCSD | No | No | No |
577 | Characterize upstream SOL impurity transport in attached/detached divertor | DDS - Drifts and Flows | Bortolon | PPPL | No | No | No |
547 | Long range impurity transport in the H-mode scrape off layer | DDS - Drifts and Flows | Samuell | LLNL | Yes | No | No |
548 | Characterizing Detachment in H-mode Helium Plasmas | DDS - Dissipation | Samuell | LLNL | Yes | No | No |
633 | Scaling of Detachment and Radiative Divertor with SOL heat flux | DDS - Dissipation | Jarvinen | VTT Technical Research Centre | No | No | No |
463 | Impurity Assisted Detachment in Moderate to High Density Conditions | DDS - Dissipation | Jarvinen | VTT Technical Research Centre | Yes | No | No |
454 | Scaling of Detachment Front Structure with IP, BT, Heating Power, and X-point Height | DDS - Dissipation | Jarvinen | VTT Technical Research Centre | Yes | No | No |
539 | Detachment physics of Helium H-modes | DDS - Dissipation | Canik | ORNL | No | No | No |
339 | Detachment onset density vs. 3D field strength | DDS - Dissipation | Eldon | GA | No | No | No |
341 | Detachment control with neon | DDS - Dissipation | Eldon | GA | No | No | No |
381 | Combined detachment + radiated power control | DDS - Dissipation | Eldon | GA | No | No | No |
634 | Measuring poloidal variations of cross-field transport in the DIII-D SOL | DDS - Dissipation | Covele | GA | No | No | No |
588 | Detachment Study using the Progressive Angle Divertor | DDS - Dissipation | Thomas | GA | No | No | No |
555 | Helium plasma detachment behavior in closed divertor | DDS - Dissipation | Meier | Zap Energy Inc. | No | No | No |
416 | ramp-up optimization for access to high qmin SS | D&C - Steady State Scenarios | Maria Poli | PPPL | No | No | No |
425 | Extend ELM suppression to DN Hybrid Fully Non-Inductive plasmas | D&C - Steady State Scenarios | Nazikian | GA | Yes | No | No |
580 | Steady-state hybrids with higher ideal MHD limits | D&C - Steady State Scenarios | Turco | Columbia U | Yes | No | No |
522 | Optimum EC and CD location in high betaN hybrids | D&C - Steady State Scenarios | Turco | Columbia U | Yes | No | No |
484 | High Pedestal in Hybrid Scenario With Unfavorable Grad-B Drift Direction | D&C - Steady State Scenarios | Petty | GA | No | No | No |
503 | Avoidance of TM during target formation of high beta, high qmin scenarios | D&C - Steady State Scenarios | Park | ORNL | Yes | No | No |
498 | High qmin, high beta in smaller shape | D&C - Steady State Scenarios | Park | ORNL | Yes | No | No |
509 | Optimum current profile for the integrated core/pedestal performance | D&C - Steady State Scenarios | Park | ORNL | No | No | No |
521 | Reduce AE induced EP transport in high q-min steady state scenarios with AE control tools | D&C - Steady State Scenarios | Collins | ORNL | Yes | Yes | No |
499 | Document and reduce fast-ion transport in steady-state scenarios | D&C - Steady State Scenarios | Thome | GA | Yes | No | No |
376 | Super H-mode with broader current density profile | D&C - Steady State Scenarios | Victor | LLNL | Yes | No | No |
379 | Test stability and confinement of qmin>2, q95<7 steady-state scenario | D&C - Steady State Scenarios | Holcomb | LLNL | Yes | No | No |
378 | Increase beta_n in high qmin plasmas with variable voltage beams | D&C - Steady State Scenarios | Victor | LLNL | Yes | No | No |
380 | Improved stability of high qmin plasmas through feedback control of the loop voltage profile | D&C - Steady State Scenarios | Victor | LLNL | Yes | No | No |
497 | Test of effect of wall stabilization | D&C - Steady State Scenarios | Luce | ITER Organization | No | No | No |
632 | AE control by ECH and NB voltage variation | D&C - Plasma Control | Hu | ASIPP | No | No | No |
513 | Develop Safe Rampdown for Plasmas with High Radiative Fraction | D&C - Plasma Control | Luce | ITER Organization | No | Yes | No |
413 | Ramp-down (dedicated+piggyback) survey for disruption avoidance | D&C - Plasma Control | Barr | GA | No | No | No |
595 | Integrated Current Profile Control and NTM Stabilization Demonstration | D&C - Plasma Control | Schuster | Lehigh U | No | No | No |
596 | Further Development of Real-time Optimization for MHD-free Steady-state Operation | D&C - Plasma Control | Schuster | Lehigh U | No | No | No |
597 | Development of Model-based qmin Control Capability in DIII-D | D&C - Plasma Control | Schuster | Lehigh U | No | No | No |
593 | Development of Rotation Profile Feedback Control Capability in DIII-D | D&C - Plasma Control | Schuster | Lehigh U | No | No | No |
599 | Actuator Sharing and Integrated Control of Magnetic and Kinetic Plasma Parameters | D&C - Plasma Control | Schuster | Lehigh U | No | No | No |
534 | PCS implementation of Machine Learning algorithm for disruption prediction | D&C - Plasma Control | Rea | Massachusetts Institute of Technology | No | No | No |
342 | Detachment control with raw TS signals instead of analyzed Te | D&C - Plasma Control | Eldon | GA | No | No | No |
575 | Control/Ops Evening Test Sessions | D&C - Plasma Control | Humphreys | GA | No | No | No |
408 | Voltage controlled SuperSpas for plasma shape control | D&C - Plasma Control | Hyatt | GA | No | No | No |
448 | VFI-less Plasma operations | D&C - Plasma Control | Hyatt | GA | No | No | No |
676 | Shot-shot reproducibility against wall loading of impurities | D&C - Plasma Control | Eldon | GA | No | No | No |
443 | Langmuir probe based detachment control | D&C - Plasma Control | Eldon | GA | No | No | No |
345 | Detachment control performance vs. puff location | D&C - Plasma Control | Eldon | GA | No | No | No |
346 | Detachment control performance vs. power scans & impurity accumulation | D&C - Plasma Control | Eldon | GA | No | No | No |
347 | Divertor radiation control | D&C - Plasma Control | Eldon | GA | No | No | No |
495 | Evaluation of ITER startup scenario | D&C - Plasma Control | Walker | GA | No | No | Yes |
567 | Actuator sharing via control supervisor | D&C - Plasma Control | Walker | GA | No | No | Yes |
373 | helium startup characterization | D&C - Plasma Control | Walker | GA | No | No | Yes |
459 | Advanced Divertor Control Development | D&C - Plasma Control | Vail | Princeton U | No | No | No |
656 | Real-time Stability Analysis for Stability Control | D&C - Plasma Control | Kolemen | PPPL | No | No | No |
447 | Control based on Machine Learning | D&C - Plasma Control | Kolemen | PPPL | No | No | No |
457 | Real-time Stability Analysis for Stability Control | D&C - Plasma Control | Kolemen | PPPL | No | No | No |
456 | EPED-NN-based feedback control of pedestal parameters | D&C - Plasma Control | Boyer | PPPL | No | No | No |
446 | Feedback control of the edge rotation shear using variable beam voltage and perveance | D&C - Plasma Control | Boyer | PPPL | No | No | No |
629 | Feedback control of current and stored energy in non-inductive scenarios on DIII-D | D&C - Plasma Control | Boyer | PPPL | No | No | No |
481 | PCS setup for proposal #370 | D&C - Plasma Control | Laggner | North Carolina State | No | No | No |
482 | PCS setup for proposal #477 | D&C - Plasma Control | Laggner | North Carolina State | No | No | No |
435 | Disruption prediction and avoidance based on Machine Learning | D&C - Disruption Mitigation Physics | Kolemen | PPPL | No | No | No |
363 | Integration of Deep Learning Disruption Predictor with Plasma Control System | D&C - Disruption Mitigation Physics | Tang | PPPL | No | No | No |
438 | Shallow injection with shards only | D&C - Disruption Mitigation Physics | Michael | ITER Organization | No | No | Yes |
439 | Optimisation of multiple SPI | D&C - Disruption Mitigation Physics | Lehnen | ITER Organization | No | No | Yes |
440 | SPI injection into the early current quench | D&C - Disruption Mitigation Physics | Lehnen | ITER Organization | No | No | Yes |
441 | SPI penetration depth / assimilation efficiency | D&C - Disruption Mitigation Physics | Lehnen | ITER Organization | No | No | Yes |
382 | Inside-out mitigation with B & B+W shell pellets | D&C - Disruption Mitigation Physics | Eidietis | GA | Yes | No | Yes |
383 | Measure halo & core temperatures during type I & II VDE's | D&C - Disruption Mitigation Physics | Eidietis | GA | Yes | No | Yes |
362 | Effect of RMP on RE spatial gradients (in QRE) | D&C - Disruption Mitigation Physics | Paz-Soldan | Columbia U | No | No | No |
372 | Radiation saturation at reduced Ne quantity by order of magnitude increase in D2 inventory | D&C - Disruption Mitigation Physics | Sweeney | Massachusetts Institute of Technology | Yes | No | Yes |
529 | Low-current runaway electron plateau dissipation by injected impurities | D&C - Disruption Mitigation Physics | Lvovskiy | GA | No | No | No |
377 | ITPA Joint Experiment on gamma-ray measurements of runaway electrons | D&C - Disruption Mitigation Physics | Lvovskiy | GA | No | Yes | No |
465 | Superposition of dual SPIs for TQ mitigation � part 2 | D&C - Disruption Mitigation Physics | Herfindal | ORNL | No | No | Yes |
531 | Impurity spreading physics and impact on fast shutdown properties | D&C - Disruption Mitigation Physics | Shiraki | ORNL | No | No | Yes |
532 | Fast shutdown with argon shattered pellet | D&C - Disruption Mitigation Physics | Shiraki | ORNL | No | No | No |
404 | RE plateau vertical loss rate during high-Z dissipation | D&C - Disruption Mitigation Physics | Hollmann | UCSD | No | No | No |
374 | Aspect ratio scaling of tearing stability | D&C - 3D and Stability Physics | Morton | U of Wisconsin | Yes | No | No |
476 | Onset and scaling of helical cores in hybrid plasmas | D&C - 3D and Stability Physics | Wingen | ORNL | Yes | No | No |
415 | n=2 Locking Threshold Scaling for ITER | D&C - 3D and Stability Physics | Logan | Columbia U | No | Yes | No |
418 | Quantify contribution of resistivity to external kink mode stability | D&C - 3D and Stability Physics | Hanson | Columbia U | Yes | No | No |
455 | PCS Optimization of DIII-D Disruptivity Reduction via Deep Learning Guidance | D&C - 3D and Stability Physics | Tang | PPPL | Yes | No | No |
458 | �Integration of Deep Learning Disruption Predictor with Plasma Control System� | D&C - 3D and Stability Physics | Tang | PPPL | No | No | No |
462 | PCS Optimization of DIII-D Disruptivity Reduction via Deep Learning Guidance | D&C - 3D and Stability Physics | Kates-Harbeck | PPPL/Harvard U | Yes | No | No |
431 | Exploring the avoidance of NTM-locking-induced disruption in High-beta n & low-q discharges | D&C - 3D and Stability Physics | Inoue | QST | Yes | No | No |
432 | Double Tearing Mode Exploration in Reversed Shear Plasmas with 3D Fields. | D&C - 3D and Stability Physics | Takechi | National Institutes for Quantum and Radiological Science and Technology (QST) | Yes | No | No |
473 | Double Tearing Mode Exploration in Reversed Shear Plasmas with 3D Fields. | D&C - 3D and Stability Physics | Takechi | QST | No | No | No |
428 | Feedback control of 2/1 locked mode phase with RMP and synchronized ECCD | D&C - 3D and Stability Physics | Choi | GA | No | No | No |
384 | Can Pellets Stabilize NTMs? | D&C - 3D and Stability Physics | Bardoczi | GA | Yes | No | No |
624 | Revisiting preemptive NTM locking avoidance with improved feedback logic in high ���²N plasma | D&C - 3D and Stability Physics | Okabayashi | PPPL | No | No | No |
638 | Machine Learning based Disruption Prediction & Avoidance | D&C - 3D and Stability Physics | Kolemen | PPPL | No | No | No |
508 | Island suppression using real-time Thomson Scattering enhanced EFIT | D&C - 3D and Stability Physics | Roelofs | PPPL | No | No | No |
388 | Study of the thermal quench during minor disruption triggered by RMPs | D&C - 3D and Stability Physics | Hu | PPPL | Yes | No | No |
386 | Control of rotating NTM by ECCD + RMP | D&C - 3D and Stability Physics | Hu | PPPL | No | No | No |
422 | Low Torque n=1 Locking Threshold Scaling with Rotation | D&C - 3D and Stability Physics | Park | PPPL | Yes | Yes | Yes |
402 | Direct measurement of n=2 Multimode Stability | D&C - 3D and Stability Physics | Wang | PPPL | Yes | No | No |
618 | Better Physics Understanding of NTM Seeding | D&C - 3D and Stability Physics | La Haye | Retired from GA | Yes | No | No |
474 | Particle source location and its impact on the pedestal | Core-Edge Integration Task Force | Laggner | North Carolina State | Yes | No | No |
477 | Active control of enhanced confinement regimes with Low Z impurity Powder Dropping | Core-Edge Integration Task Force | Laggner | North Carolina State | Yes | No | No |
609 | Compatibility of advanced scenarios with silicon coated PCF | Core-Edge Integration Task Force | Bortolon | PPPL | No | No | No |
550 | Transport in the no man's land: how pedestal performance propagates to the core | Core-Edge Integration Task Force | Bortolon | PPPL | No | No | No |
396 | The Interplay of Magnetic Balance With Divertor Closure and Its Effect on Radiating Div Performance | Core-Edge Integration Task Force | Petrie | GA | Yes | No | No |
525 | Global confinement and edge rotation for private, strike, and common flux pumping | Core-Edge Integration Task Force | Grierson | GA | No | No | No |
414 | Prospects for Suppressing Impurity Buildup at the Plasma Center During ECH Heating of AT Plasmas | Core-Edge Integration Task Force | Petrie | GA | Yes | No | No |
400 | The Most Effective Radiating Divertor That DIII-D Can Presently Make in the DN Shape | Core-Edge Integration Task Force | Petrie | GA | No | No | No |
574 | Compare DN/SN vertical and shape controllability | Core-Edge Integration Task Force | Humphreys | GA | No | Yes | No |
397 | Stable Super H-mode with optimized pedestal density | Core-Edge Integration Task Force | Knolker | GA | Yes | No | No |
581 | Effect of Divertor Geometry on High-Performance Core | Core-Edge Integration Task Force | Thome | GA | Yes | No | No |
594 | Physics of Puff and Pump | Core-Edge Integration Task Force | Allen | LLNL | No | No | No |
412 | Prospects for Suppressing Impurity Buildup at the Plasma Center During ECH Heating of AT Plasmas | Core-Edge Integration Task Force | Petrie | GA | No | No | No |
433 | RMP ELM Suppression with Lithium Enhanced Pedestal | Core-Edge Integration Task Force | Nazikian | GA | Yes | No | No |
475 | Onset and scaling of helical cores in hybrid plasmas | Core-Edge Integration Task Force | Wingen | ORNL | Yes | No | No |
658 | RMP effects on heavy non-recycling impurity confinement and exhaust | Core-Edge Integration Task Force | Hinson | ORNL | No | No | No |
358 | 3D boundary effects on heavy impurity removal | Core-Edge Integration Task Force | Hinson | ORNL | Yes | No | No |
564 | RMP effects on He confinement and exhaust | Core-Edge Integration Task Force | Hinson | ORNL | No | No | No |
515 | Core-Edge Investigations in the Super H and Near Super H Regime | Core-Edge Integration Task Force | Snyder | ORNL | Yes | No | No |
545 | Dependence of neutral pressure on detachment | Core-Edge Integration Task Force | Shafer | ORNL | No | No | No |
559 | Effects of divertor closure on pedestal fueling and non-diffusive transport with pellet fueling | Core-Edge Integration Task Force | Shafer | ORNL | No | No | No |
516 | Effect of differing edge relaxation mechanisms on global impurity confinement times | Core-Edge Integration Task Force | Hughes | Massachusetts Institute of Technology | No | Yes | No |
568 | Impact of medium Zi dilution of deuterium pasma on core and edge turbulence and transport | Core-Edge Integration Task Force | Porkolab | Massachusetts Institute of Technology | No | No | No |
566 | Impact of Divertor Conditions on Radial Electric Field at the Pedestal-SOL Boundary | Core-Edge Integration Task Force | Jarvinen | VTT Technical Research Centre | No | No | No |
389 | Poloidal asymmetry of RS inward momentum pinch and USN/LSN dependence | Core-Edge Integration Task Force | Boedo | UCSD | No | No | No |
558 | Transport alteration and confinement improvement via radiative impurity-seeding | Core-Edge Integration Task Force | McKee | U of Wisconsin | No | No | No |
645 | H-mode at negative triangularity as a feasibility study for future machines | Core-Edge Integration Task Force | Marinoni | UCSD | No | No | No |
643 | Steady-state, high beta_pol plasma utilizing the SAS divertor | Core-Edge Integration Task Force | Victor | LLNL | Yes | No | No |
364 | Role of divertor geometry on confinement | Core-Edge Integration Task Force | Mordijck | The college of William and Mary | No | No | No |
365 | High opacity SOL effect on pedestal | Core-Edge Integration Task Force | Mordijck | The college of William and Mary | No | Yes | Yes |
667 | Measurement of poloidal flow structures | BPP - Turbulence and Transport | Bortolon | PPPL | Yes | No | No |
669 | Study of Electro-Magnetic quasi-coherent fluctuation under various plasma conditions | BPP - Turbulence and Transport | Chen | UCLA | Yes | No | No |
576 | Understanding improved confinement in negative triangularity discharges | BPP - Turbulence and Transport | Austin | U. Texas | No | No | No |
511 | Investigation of loss of linear current scaling at low q95 | BPP - Turbulence and Transport | Luce | ITER Organization | No | No | No |
673 | LH power threshold, confinement scaling and CER calibration in C plasmas | BPP - Turbulence and Transport | Marinoni | UCSD | No | No | No |
674 | Investigating the link between electron scale fluctuations and the ECH density pump-out | BPP - Turbulence and Transport | Marinoni | UCSD | No | No | No |
507 | Optimization of ELMfree high-performance plasmas at negative triangularity | BPP - Turbulence and Transport | Marinoni | UCSD | Yes | No | No |
504 | Exploring new reactor concepts: H-mode at negative triangularity | BPP - Turbulence and Transport | Marinoni | UCSD | Yes | No | No |
657 | Investigation of turbulence changes with ELM suppression by RMPs | BPP - Turbulence and Transport | Sung | KAIST | No | No | No |
664 | Unique Code Validation via Comparison of HFS/LFS and exploring up/down asymmetry in turbulence | BPP - Turbulence and Transport | Sung | KAIST | Yes | No | No |
570 | Impact of medium Zi dilution of deuterium pasma on core and edge turbulence and transport | BPP - Turbulence and Transport | Porkolab | Massachusetts Institute of Technology | No | No | No |
538 | Electron Temperature Profile Stiffness in Wide Pedestal QH-Mode | BPP - Turbulence and Transport | Ernst | Massachusetts Institute of Technology | Yes | No | No |
429 | Study of cold-pulse dynamics and 'nonlocal transport effects' using perturbative LBO injections | BPP - Turbulence and Transport | Rodriguez Fernandez | Massachusetts Institute of Technology | Yes | No | No |
423 | Commissioning of Laser Blow-Off (LBO) and Piggyback Studies of Impurity Transport on DIII-D | BPP - Turbulence and Transport | Howard | Massachusetts Institute of Technology | Yes | No | No |
424 | Studying the Ability of External Heating to Modify Impurity Transport in Reactor Scenarios | BPP - Turbulence and Transport | Howard | Massachusetts Institute of Technology | Yes | No | No |
405 | Investigation on core impurity transport in ITER-relevant ELM-y and QH-mode plasmas | BPP - Turbulence and Transport | Sciortino | Max-Planck Institute for Plasma Physics | Yes | No | No |
406 | Investigation on impurity transport and turbulence in internal transport barriers | BPP - Turbulence and Transport | Sciortino | Max-Planck Institute for Plasma Physics | No | No | No |
407 | Effect of Injected Torque and Current Drive on Impurity Transport | BPP - Turbulence and Transport | Sciortino | Max-Planck Institute for Plasma Physics | No | No | No |
496 | 2D Isotope Scan for Energy Confinement | BPP - Turbulence and Transport | Thome | GA | Yes | No | No |
665 | H-mode impurity transport dependence on beam fueling | BPP - Turbulence and Transport | Thome | GA | No | No | Yes |
668 | Measurement of poloidal flow structures | BPP - Turbulence and Transport | Bortolon | PPPL | Yes | No | No |
666 | Validate low-k magnetic turbulence predictions relevant to the burning plasma core | BPP - Turbulence and Transport | Guttenfelder | PPPL | No | No | No |
573 | Understanding improved confinement in negative triangularity discharges | BPP - Turbulence and Transport | Austin | U of Texas, Austin | No | No | No |
360 | L-H Transitions dynamics: Impact of the beam voltage and its effects on the edge rotation shear | BPP - L-H transition | Diallo | PPPL | No | No | No |
671 | Pellet induced H-mode with Tangential D2 Pellet Injection | BPP - L-H transition | Baylor | ORNL | No | No | No |
565 | Understand effect of resonant vs non-resonant magnetic perturbations on L-H transition dynamics | BPP - L-H transition | Kriete | U of Wisconsin | Yes | No | No |
434 | RMP Spectrum Control to Improve H-mode Access | BPP - L-H transition | Schmitz | UCLA | No | No | No |
546 | Dependence of L-H power threshold on X-point height | BPP - L-H transition | Samuell | LLNL | Yes | No | No |
615 | 3D spectrum dependence on L-H transition in DIII-D | BPP - L-H transition | Ko | National Fusion Research Institute | Yes | No | No |
616 | 3D spectrum dependence on L-H transition in DIII-D | BPP - L-H transition | Ko | National Fusion Research Institute | Yes | No | No |
395 | Prospects for Suppressing Impurity Buildup at the Plasma Center During ECH Heating of AT Plasmas | BPP - Heating & Current Drive | Petrie | GA | No | No | No |
514 | Test DIII-D NB operation to 93 kV | BPP - Heating & Current Drive | Luce | ITER Organization | No | No | No |
662 | HFS LHCD Passive High Z Metallic Structure Test | BPP - Heating & Current Drive | Wukitch | Massachusetts Institute of Technology | No | No | No |
533 | Reduce AE induced EP transport in high q-min steady state scenarios with AE control tools | BPP - Energetic Particle Physics | Collins | ORNL | Yes | Yes | No |
490 | Triton Burn-up Study in DIII-D Tokamak | BPP - Energetic Particle Physics | Zhu | UC, Irvine | No | No | No |
600 | BAE/BAAE validation | BPP - Energetic Particle Physics | Heidbrink | UC, Irvine | No | Yes | No |
601 | Fast-ion transport by BAAEs | BPP - Energetic Particle Physics | Heidbrink | UC, Irvine | No | No | No |
604 | Resonant fast-ion transport by applied 3D fields | BPP - Energetic Particle Physics | Heidbrink | UC, Irvine | No | No | No |
654 | Fast-ion and AE control via externally applied 3D fields | BPP - Energetic Particle Physics | Garcia Munoz | U of Seville | No | Yes | No |
471 | Parametric Study of Mode Stability, Frequency, and Wave Number Dependence in Mixed Species Plasmas | BPP - Energetic Particle Physics | Tang | Oak Ridge Associated Universities | Yes | Yes | No |
453 | Verification of Imaging Neutral Particle Analyzer and its application to the phase-space flow study | BPP - Energetic Particle Physics | Du | GA | No | No | No |
461 | Investigation of runaway electron-driven magnetized plasma wave and whistler in tokamak | BPP - Energetic Particle Physics | Du | GA | No | No | No |
470 | Investigation of fuel recycling on tungsten in fusion-relevant conditions | AMV - Surface Evolution Science | Guterl | GA | Yes | No | No |
637 | ELM filament footprint in j, q_perp, Da etc. (#583 for AMV) | AMV - Surface Evolution Science | Bykov | GA | Yes | No | No |
556 | High-Z and textured surface arcing susceptibility | AMV - Surface Evolution Science | Jaworski | PPPL | No | No | No |
602 | Performance of irradiated W, SiC, and SiC/W composites as a PFC material | AMV - Surface Evolution Science | Abrams | GA | Yes | No | No |
646 | Density Dependence of W I & W II SXB Ratios for Improved Erosion and Redeposition Diagnosis | AMV - Surface Evolution Science | Ennis | Auburn U | No | No | No |
608 | Dust re-mobilization studies using DiMES | AMV - Surface Evolution Science | Rudakov | UCSD | No | No | No |
349 | In-situ formation of Si-C coatings on DiMES | AMV - Surface Evolution Science | Rudakov | UCSD | Yes | No | No |
350 | Measuring net and gross erosion rates of SiC in DIII-D divertor and main chamber | AMV - Surface Evolution Science | Rudakov | UCSD | No | No | No |
606 | Studies of Arcing on high-Z PFC Surfaces | AMV - Surface Evolution Science | Rudakov | UCSD | No | No | No |
653 | Preferential sputtering of Si or C from SiC versus temperature | AMV - Surface Evolution Science | Unterberg | ORNL | Yes | No | No |
562 | Measurement of local erosion/redeposition impulse function | AMV - Surface Evolution Science | Hinson | ORNL | Yes | No | No |
489 | Arcing threshold due to ELM deposition at the strike point and in the scrape-off layer | AMV - Surface Evolution Science | Bykov | GA | Yes | No | No |
679 | SiC Sputtering and Near-surface Characterization Under He Bombardment | AMV - Surface Evolution Science | Bringuier | GA | Yes | No | No |
650 | Influence of thin in-situ Si coatings on SOL carbon content | AMV - Material Migration and Mitigation | Unterberg | ORNL | Yes | No | No |
651 | Impact of gaps/trenches on high-Z material migration | AMV - Material Migration and Mitigation | Unterberg | ORNL | Yes | No | No |
652 | W deposition from a complete core source with shell pellets and collector probe | AMV - Material Migration and Mitigation | Unterberg | ORNL | Yes | No | No |
536 | Testing of a new neutral H sensor for C-X H fluxes on the wall and divertor | AMV - Material Migration and Mitigation | Barton | Sandia National Lab | No | No | No |
394 | Comparison of silicon and carbon erosion and migration by exposure of isotope SiC coating | AMV - Material Migration and Mitigation | Ding | ASIPP | No | No | No |
610 | Power loading at toroidal PFC gaps | AMV - Material Migration and Mitigation | Rudakov | UCSD | No | Yes | Yes |
483 | Core impurity contamination by unipolar arcing on PFCs | AMV - Material Migration and Mitigation | Bykov | GA | Yes | No | No |
641 | Visible spectroscopy for impurity flux from and temperature of leading edges on DiMES (#640 for AMV) | AMV - Material Migration and Mitigation | Bykov | GA | Yes | No | No |
639 | Measurement of 3D ion impact geometry by erosion of med-Z spherical micro particles | AMV - Material Migration and Mitigation | Bykov | GA | Yes | No | No |
356 | Spectroscopic analysis of SiC preferential sputtering | AMV - Material Migration and Mitigation | Abrams | GA | Yes | No | No |
357 | ELM-resolved measurements of high-Z re-deposition fractions | AMV - Material Migration and Mitigation | Abrams | GA | Yes | No | No |
554 | Boundary Ion temperature measurement based on retarding field analyzer | AMV - Material Migration and Mitigation | Ren | U of Tennessee, Knoxville | No | No | No |
617 | D2 re-emission from prospective materials: characterization by ro-vibrational sp. in H-mode | AMV - Innovative Materials Development | Bykov | GA | Yes | No | No |
659 | testing the transparent materials with DIMES | AMV - Innovative Materials Development | Pigarov | CompX | No | No | No |
603 | Measure D retention/recycling properties of bulk SiC versus fibrous SiC/SiC in DIII-D divertor | AMV - Innovative Materials Development | Abrams | GA | Yes | No | No |
589 | SiC versus SiC Composite Dimes Tests | AMV - Innovative Materials Development | Thomas | GA | No | No | No |
590 | Heated SiC Dimes Tests | AMV - Innovative Materials Development | Thomas | GA | No | No | No |
591 | Test of micrograin Mo mirror concept | AMV - Innovative Materials Development | Thomas | GA | No | No | No |
613 | Assessment of property changes in W, SiC and their composites exposed to D3D environments | AMV - Innovative Materials Development | Vasudevamurthy | GA | No | No | No |
537 | Expose UFG W to DIII-D discharges to demonstrate improved properties useful in future PFCs | AMV - Innovative Materials Development | Barton | Sandia National Lab | No | No | No |
542 | Effect of heated DiMES on erosion of W-alternative PFMs | AMV - Innovative Materials Development | Coburn | Sandia National Lab | No | No | No |
540 | Erosion Characterization of W-alternative PFMs under L-mode & H-mode using Micro-Trench Technique | AMV - Innovative Materials Development | Coburn | Sandia National Lab | Yes | No | No |
649 | Exposure of graphitic foam with CVI SiC coatings | AMV - Innovative Materials Development | Unterberg | ORNL | Yes | No | No |
612 | Variations in Thermomechanical Stability between Amorphous and Polycrystalline SiC | AMV - Innovative Materials Development | Bringuier | GA | No | No | No |
598 | Influence of SiC Microstructure and Texture on Sputtering | AMV - Innovative Materials Development | Bringuier | GA | No | No | No |