DIII-D RESEARCH OPPORTUNITIES FORUM FOR THE 2014 EXPERIMENTAL CAMPAIGN
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(Proposal numbers 1-382 are from 2013) | |||||||||
ID | Title | Research Area | Name | Affiliation |
Time Req'ed |
ITPA Joint Exp |
ITER IO Urgent Research Task |
||
40 | MGI with applied n=1 RMP fields | Disruption Mitigation | Fiat Lux LLC | No | No | No | |||
58 | Progressing Towards a Staged Approach to Disruption Mitigation | Disruption Mitigation | GA | Yes | No | Yes | |||
113 | Heat Load during slow current quench phase of disruptions/VDEs and its relation with poloidal halo c | Disruption Mitigation | ITER Organization | Yes | No | Yes | |||
114 | Toroidal peaking of radiation, response time for triggering TQ and mitigation efficiency during mass | Disruption Mitigation | ITER Organization | Yes | No | Yes | |||
129 | Optimization and Control of ITER-like MGI | Disruption Mitigation | GA | Yes | Yes | Yes | |||
131 | Understanding runaway equilibrium to minimize damage hazard | Disruption Mitigation | Yes | Yes | Yes | ||||
132 | Dissipation & Control of RE from ITER-like LSN targets | Disruption Mitigation | GA | No | No | Yes | |||
133 | Fast Runaway Shutdowns by MGI | Disruption Mitigation | GA | Yes | Yes | Yes | |||
135 | Measurement of RE diffusion to center post | Disruption Mitigation | UCSD | No | No | Yes | |||
136 | Disruption main chamber heat loads | Disruption Mitigation | UCSD | No | Yes | Yes | |||
139 | TQ radiation distribution from R-2 MGI | Disruption Mitigation | UCSD | No | No | Yes | |||
141 | Studies of RE final loss | Disruption Mitigation | UCSD | No | No | Yes | |||
150 | Sensitivity study of toroidally-asymmetric halo current to error field during VDE | Disruption Mitigation | PPPL | No | No | No | |||
165 | D2 + few % Ne shattered pellets for disruption mitigation | Disruption Mitigation | ORNL | No | No | Yes | |||
166 | Effect of q95 on SPI shutdown | Disruption Mitigation | ORNL | No | No | Yes | |||
167 | Control of radiation asymmetries by application of external field on SPI/MGI shutdown | Disruption Mitigation | ORNL | No | No | Yes | |||
168 | Influence of the delay time between multiple massive gas injections at different toroidal locations | Disruption Mitigation | ORNL | No | No | Yes | |||
169 | Runaway flattop mitigation by Neon shattered pellet injection | Disruption Mitigation | ORNL | No | No | Yes | |||
171 | Test of the argon pellet injector | Disruption Mitigation | ORNL | No | No | Yes | |||
191 | Critical electric field for runaway electron growth and decay under quiescent conditions | Disruption Mitigation | Columbia U | Yes | Yes | No | |||
227 | Mechanisms leading to termination of the runaway discharges and effects on PFC energy deposition | Disruption Mitigation | ITER Organization | Yes | No | Yes | |||
229 | CQ de-confinement of REs using pulsed impurity injection | Disruption Mitigation | ITER Organization | Yes | No | Yes | |||
237 | Critical electric field for runaway electron growth and decay under quiescent conditions | Disruption Mitigation | Massachusetts Institute of Technology | Yes | Yes | No | |||
250 | Plateau Ecrit with MGI | Disruption Mitigation | GA | No | Yes | Yes | |||
254 | Neon SPI injection into early CQ to stunt RE formation | Disruption Mitigation | GA | No | No | No | |||
377 | NTM locking disruption avoidance by the EM torque with toroidal-phase forward magnetic feed | Disruption Mitigation | PPPL | No | No | No | |||
396 | Measurement of RE diffusion to center post | Disruption Mitigation | UCSD | No | No | No | |||
397 | Disruption main chamber heat loads | Disruption Mitigation | UCSD | No | Yes | Yes | |||
398 | TQ radiation distribution from R-2 MGI | Disruption Mitigation | UCSD | No | No | Yes | |||
399 | TQ radiation distribution from R-2 MGI | Disruption Mitigation | UCSD | No | No | Yes | |||
400 | Studies of RE final loss | Disruption Mitigation | UCSD | No | No | No | |||
437 | TQ radiation distribution from R-2 MGI | Disruption Mitigation | Massachusetts Institute of Technology | No | No | No | |||
506 | Understanding the synchrotron emission patterns in QRE discharges | Disruption Mitigation | UCSD | Yes | No | No | |||
517 | Physics of Crescent-shaped synchrotron emission patterns in runaway plateau dischar | Disruption Mitigation | UCSD | Yes | No | No | |||
583 | Dissipation of runaway energy by high-Z impurity injection | Disruption Mitigation | ITER Organization | Yes | Yes | Yes | |||
608 | Quiescent runaway electron studies for 2014 | Disruption Mitigation | Columbia U | No | No | No | |||
609 | MHD spectroscopy and poloidal coupling of plateau RE plasmas | Disruption Mitigation | Columbia U | No | No | No | |||
625 | Disruption Precursor Identification | Disruption Mitigation | U of Colorado, Boulder | No | No | No | |||
634 | Mitigation: Reduction of toroidal-asymmetry of radiation loss by 3D-magnetic mode rotation control | Disruption Mitigation | PPPL | No | No | Yes | |||
635 | Mitigation: pellet and massive gas injections in helically favorable ways for reducing asymmetry | Disruption Mitigation | PPPL | No | No | Yes | |||
661 | Massive gas injection into an unstable plasma | Disruption Mitigation | GA | No | No | No | |||
712 | D2 + few % Ne shattered pellets for disruption mitigation | Disruption Mitigation | ORNL | No | No | Yes | |||
713 | Control of radiation asymmetries by application of external field on SPI/MGI shutdown | Disruption Mitigation | ORNL | No | No | Yes | |||
714 | Runaway flattop mitigation by Neon shattered pellet injection | Disruption Mitigation | ORNL | No | No | Yes | |||
715 | Test of the upgraded SPI | Disruption Mitigation | ORNL | No | No | No | |||
747 | Dissipation & Control of RE from ITER-like LSN targets | Disruption Mitigation | GA | No | No | No | |||
749 | Neon SPI injection into early CQ to stunt RE formation | Disruption Mitigation | GA | No | No | No | |||
767 | Radiation asymmetry measurements in opposite-handed plasmas | Disruption Mitigation | ORNL | No | No | No |