DIII-D RESEARCH OPPORTUNITIES FORUM FOR THE 2017 EXPERIMENTAL CAMPAIGN
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| ID | Title | Research Area | Name | Affiliation |
Time Req'ed |
ITPA Joint Exp |
ITER IO Urgent Research Task |
| 20 | Quiescent runaway electron studies with refurbished gamma-ray-imaging detectors | Disruption Mitigation Physics | Paz-Soldan | Columbia U | No | Yes | No |
| 29 | Runaway plateau impurity assimilation | Disruption Mitigation Physics | Hollmann | UCSD | No | No | Yes |
| 30 | Vary runaway electron plateau wall strike phase | Disruption Mitigation Physics | Hollmann | UCSD | No | No | No |
| 32 | Asymmetry effects during SPI fast shutdown | Disruption Mitigation Physics | Shiraki | ORNL | No | No | No |
| 33 | Multiple shattered pellet injections for TQ/CQ mitigation | Disruption Mitigation Physics | Shiraki | ORNL | No | No | No |
| 34 | Ballistic transport and MHD mixing in SPI impurity assimilation | Disruption Mitigation Physics | Shiraki | ORNL | No | No | No |
| 36 | Alternative injection schemes for high-Z shattered pellets for dissipation of runaway electrons | Disruption Mitigation Physics | Shiraki | ORNL | No | No | No |
| 37 | Pellet ablation as a diagnostic for quiescent runaway electron growth | Disruption Mitigation Physics | Shiraki | ORNL | No | No | No |
| 85 | Effect of the post-TQ density on runaway beam mitigation with MGI and SPI | Disruption Mitigation Physics | Fil | PPPL | No | No | No |
| 95 | Use of shape driven vertical motion to probe non-axisymmetric VDE SOL currents | Disruption Mitigation Physics | Cabrera | Columbia U | Yes | No | No |
| 210 | Improving impurity injection into RE by avoiding high energy shfited RE orbits | Disruption Mitigation Physics | Eidietis | GA | No | No | No |
| 211 | Effect of global MHD stability on RE plateau dissipation in D3D & JET | Disruption Mitigation Physics | Eidietis | GA | No | No | Yes |
| 215 | Experimental test of two-threshold-field theory of RE generation | Disruption Mitigation Physics | Lvovskiy | ORAU | No | No | No |
| 233 | Joint SPI experiment with JET | Disruption Mitigation Physics | Greenfield | ORNL | No | No | Yes |
| 246 | Develop low q95 post-disruption runaway electron scenario | Disruption Mitigation Physics | Paz-Soldan | Columbia U | No | Yes | No |
| 248 | Prompt conversion of a full current into sub-MeV RE current | Disruption Mitigation Physics | Aleynikov | Max-Planck Institute for Plasma Physics | No | Yes | No |
| 272 | D3D/JET comparison of pure Ne SPI size scaling | Disruption Mitigation Physics | Eidietis | GA | No | No | Yes |
| 280 | Placeholder: Dedicated camrea time to get SPI solid fraction estimate | Disruption Mitigation Physics | Eidietis | GA | No | No | No |
| 282 | Placeholder: Spatially resolved measurement of RE pleateau f(E) with GRI | Disruption Mitigation Physics | Eidietis | GA | No | No | No |
| 311 | Runaway mitigation with solid pellets | Disruption Mitigation Physics | Lehnen | ITER Organization | No | Yes | Yes |
| 312 | SPI with varying target plasma parameters | Disruption Mitigation Physics | Lehnen | ITER Organization | No | No | Yes |