TJ-II:Electron Bernstein Wave Heating: Difference between revisions
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i.e. at 28 GHz. | i.e. at 28 GHz. | ||
<ref>[http://www.new.ans.org/store/j_571 F. Castejón et al., ''Electron Bernstein wave heating calculations for TJII plasmas,'' Fusion Sci. Tech. '''46''', pp. 327-334 (2004)]</ref> | <ref>[http://www.new.ans.org/store/j_571 F. Castejón et al., ''Electron Bernstein wave heating calculations for TJII plasmas,'' Fusion Sci. Tech. '''46''', pp. 327-334 (2004)]</ref> | ||
The system is located in [[TJ-II:Sectors|sector]] D6. | |||
==References== | ==References== | ||
<references /> | <references /> | ||
Revision as of 11:41, 5 August 2009
In TJ-II, the possibility of achieving high-density plasmas using Electron Bernstein Wave Heating (EBWH), which has been used successfully in the W7-AS and H-J stellarators, is being explored. [1] It offers a way of overcoming the cut-off density limit associated with ECRH methods (1.7×1019 m-3 in TJ-II). Preliminary studies highlighted several promising EBWH first harmonic schemes, i.e. at 28 GHz. [2]
The system is located in sector D6.