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
10The role of RE-driven kinetic instabilities on formation of post-disruption RE beamDisruption Mitigation ThrustLvovskiyGAYesBreakoutNoNo
11Identification of Alfven instabilities driven by REs at negative Uloop during RE plateau stageDisruption Mitigation ThrustLvovskiyGANoBreakoutNoNo
14Comparison of dispersive vs non-dispersive shell pellet payloadDisruption Mitigation ThrustHollmannUCSDNoBreakoutNoNo
15Suppression of RE seeds with W grains in shell pelletDisruption Mitigation ThrustHollmannUCSDNoBreakoutNoNo
16Dynamic measurement of impurity transport into RE plateau using carbon depositionDisruption Mitigation ThrustHollmannUCSDNoBreakoutNoNo
17Change in RE plateau vertical loss rate with low-Z injectionDisruption Mitigation ThrustHollmannUCSDNoBreakoutNoNo
18Scan of RE plateau final loss footprint with I-coil perturbationDisruption Mitigation ThrustHollmannUCSDNoBreakoutNoNo
19Scan of RE plateau impurity assimilation with auxiliary heatingDisruption Mitigation ThrustHollmannUCSDNoBreakoutNoNo
26Determine the cause of RE beam final loss in post disruption vertical displacement eventsDisruption Mitigation ThrustBardocziGANoBreakoutNoYes
73Role of pre-disruption electron temperature in runaway electron seed formationDisruption Mitigation ThrustPaz-SoldanColumbia UNoBreakoutNoNo
372whistler polarizationDisruption Mitigation ThrustHeidbrinkUC, IrvineNoBreakoutNoNo
473Evaluating the internal MHD response to shell pellet injectionDisruption Mitigation ThrustPandyaU of WisconsinNoBreakoutNoNo
474Evaluating the internal MHD response to SPIDisruption Mitigation ThrustPandyaU of WisconsinNoBreakoutNoNo
475Measuring internal MHD during the formation and evolution of a runaway electron beamDisruption Mitigation ThrustPandyaU of WisconsinNoBreakoutNoNo
507ITER DMS design validationDisruption Mitigation ThrustLehnenITER OrganizationNoBreakoutNoNo
510Superposition of identical dual SPIsDisruption Mitigation ThrustHerfindalORNLNoBreakoutNoNo
514MGI-assisted-SPI for decreased radiation asymmetries and increased penetration depthDisruption Mitigation ThrustSweeneyMassachusetts Institute of TechnologyYesBreakoutNoNo
517Penetration characterization of small pellet injection into D3D plasmasDisruption Mitigation ThrustRamanU of WashingtonNoBreakoutNoNo
525Mass scaling of shell pellet assimilationDisruption Mitigation ThrustEidietisGANoBreakoutNoNo
526Full profile measurement of shell Te profileDisruption Mitigation ThrustEidietisGANoBreakoutNoNo
527Test Li coating for "ideal" shell pelletDisruption Mitigation ThrustEidietisGANoBreakoutNoNo
528Ablation measurments of single snall Ne pelletDisruption Mitigation ThrustEidietisGANoBreakoutNoNo
529Effect of D admixture in SPIDisruption Mitigation ThrustEidietisGANoBreakoutNoNo
530dilution cooling in SPI superpositionDisruption Mitigation ThrustEidietisGANoBreakoutNoNo
531Scaling of fragment penetration depth with energy:Disruption Mitigation ThrustEidietisGANoBreakoutNoNo
532JET SPI similarity experimentsDisruption Mitigation ThrustEidietisGANoBreakoutNoNo
533Ballistic transport and energy/size scaling for SPIDisruption Mitigation ThrustShirakiORNLNoBreakoutNoNo
539Effect of underlying non-axisymmetric (NA) fields on disruption mitigation processDisruption Mitigation ThrustEidietisGANoBreakoutNoNo