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TJ-II:Electron Cyclotron Resonant Heating: Difference between revisions
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TJ-II:Electron Cyclotron Resonant Heating (view source)
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The gyrotrons can be modulated for perturbative transport experiments <ref>S. Eguilior et al, ''Heat wave experiments on TJ-II flexible heliac'', [[doi:10.1088/0741-3335/45/2/303|Plasma Phys. Control. Fusion '''45''' (2003) 105–120]]</ref> and can be used to drive current. | The gyrotrons can be modulated for perturbative transport experiments <ref>S. Eguilior et al, ''Heat wave experiments on TJ-II flexible heliac'', [[doi:10.1088/0741-3335/45/2/303|Plasma Phys. Control. Fusion '''45''' (2003) 105–120]]</ref> and can be used to drive current. | ||
<ref>V. Tribaldos et al, ''Electron cyclotron heating and current drive in the TJ-II stellarator'', [[doi:10.1088/0741-3335/40/12/010|Plasma Phys. Control. Fusion '''40''' (1998) 2113]]</ref> | <ref>V. Tribaldos et al, ''Electron cyclotron heating and current drive in the TJ-II stellarator'', [[doi:10.1088/0741-3335/40/12/010|Plasma Phys. Control. Fusion '''40''' (1998) 2113]]</ref> | ||
== Signals in the TJ-II database == | |||
* GR, GR2: gyrotrons 1 and 2 | |||
* ECA1...4: sniffer probes | |||
== References == | == References == | ||
<references /> | <references /> | ||