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dc.contributor.authorRice, John E.en_US
dc.contributor.authorLin, Y.en_US
dc.contributor.authorPerks, C.J.en_US
dc.contributor.authorReinke, M.L.en_US
dc.contributor.authorMarmar, E.S.en_US
dc.contributor.authorCao, N.en_US
dc.contributor.authorGao, C.en_US
dc.contributor.authorSciortino, Francescoen_US
dc.contributor.authorWukitch, S.J.en_US
dc.contributor.authorWright, John C.en_US
dc.date.accessioned2025-03-21T20:16:09Z
dc.date.available2025-03-21T20:16:09Z
dc.date.issued2022-02
dc.identifier22ja011
dc.identifier.urihttps://hdl.handle.net/1721.1/158633
dc.descriptionSubmitted for publication in Nuclear Fusion
dc.description.abstractPumpout of argon ions by ICRF waves has been observed in C-Mod deuterium L- and I-mode plasmas that had a substantial hydrogen fraction. The effect is manifested by a reduction of core argon x-ray brightness up to a factor of 90% on time scales of tens of milliseconds following injection of ICRF power. For Ar^16+, the pumpout is strongest for hydrogen minority concentrations between 0.25 and 0.4, when the ICRF waves are not expected to result in minority heating. Modeling with the TORIC code suggests that the pumpout process occurs when the H/D mode conversion layer overlaps with the 2nd harmonic impurity resonance layer. The magnitude of the argon pumpout is independent of ICRF power above an apparent threshold of ~500 kW, independent of electron density and appears to decrease as the plasma current is increased. Potential application as a heavy impurity control tool in reactors is discussed.
dc.publisherIOPen_US
dc.relation.isversionofdoi.org/10.1088/1741-4326/ac6ef0
dc.sourcePlasma Science and Fusion Centeren_US
dc.titleArgon Pumpout by ICRF Waves in C-Mod L- and I-mode Plasmasen_US
dc.typeArticleen_US
dc.contributor.departmentMassachusetts Institute of Technology. Plasma Science and Fusion Center
dc.relation.journalNuclear Fusion


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