TJ-II:Electron Bernstein Wave Heating: Difference between revisions
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In TJ-II, the possibility of achieving high-density | In [[TJ-II]], the possibility of achieving high-density | ||
plasmas using Electron Bernstein Wave Heating (EBWH), | plasmas using Electron Bernstein Wave Heating (EBWH), | ||
which has been used successfully in the W7-AS and H-J | which has been used successfully in the W7-AS and H-J | ||
stellarators, is being explored. | stellarators, is being explored. | ||
<ref> | <ref>A. Fernández et al., ''The design of an electron Bernstein wave heating system for the TJ-II stellarator,'' [http://www.new.ans.org/store/j_572 Fusion Sci. Tech. '''46''', pp. 335-341 (2004)]</ref> | ||
<ref> | <ref>A. Fernández et al., ''Status of the TJ-II Electron Bernstein Waves heating project'', [[doi:10.1016/j.fusengdes.2005.06.309|Fusion Engineering and Design '''74''', Issues 1-4 (2005) 325-329]]</ref> | ||
It offers a way of | It offers a way of | ||
overcoming the cut-off density limit associated with ECRH | overcoming the cut-off density limit associated with ECRH | ||
Line 10: | Line 10: | ||
highlighted several promising EBWH first harmonic schemes, | highlighted several promising EBWH first harmonic schemes, | ||
i.e. at 28 GHz. | i.e. at 28 GHz. | ||
<ref>[http://www.new.ans.org/store/j_571 | <ref>F. Castejón et al., ''Electron Bernstein wave heating calculations for TJII plasmas,'' [http://www.new.ans.org/store/j_571 Fusion Sci. Tech. '''46''', pp. 327-334 (2004)]</ref> | ||
Results have also been reported. | |||
<ref>J.B.O. Caughman, Á. Fernández, Á. Cappa, et al., ''Initial Electron Bernstein Wave Emission Measurements on the TJ-II Stellarator'', [[doi:10.13182/FST10-A9267|Fusion Sc. Technol. '''57''' (2010) 41]]</ref> | |||
<ref>J.M. García-Regaña, Á. Cappa, F. Castejón, J.B.O. Caughman, M. Tereshchenko, A. Ros, D.A. Rasmussen and J.B. Wilgen, ''Electron Bernstein waves emission in the TJ-II stellarator'', [[doi:10.1088/0741-3335/53/6/065009|Plasma Phys. Control. Fusion '''53''' (2011) 065009]]</ref> | |||
The system is located in [[TJ-II:Sectors|sector]] D6. | The system is located in [[TJ-II:Sectors|sector]] D6. |
Latest revision as of 06:28, 13 October 2018
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] [2] 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. [3] Results have also been reported. [4] [5]
The system is located in sector D6.
References
- ↑ A. Fernández et al., The design of an electron Bernstein wave heating system for the TJ-II stellarator, Fusion Sci. Tech. 46, pp. 335-341 (2004)
- ↑ A. Fernández et al., Status of the TJ-II Electron Bernstein Waves heating project, Fusion Engineering and Design 74, Issues 1-4 (2005) 325-329
- ↑ F. Castejón et al., Electron Bernstein wave heating calculations for TJII plasmas, Fusion Sci. Tech. 46, pp. 327-334 (2004)
- ↑ J.B.O. Caughman, Á. Fernández, Á. Cappa, et al., Initial Electron Bernstein Wave Emission Measurements on the TJ-II Stellarator, Fusion Sc. Technol. 57 (2010) 41
- ↑ J.M. García-Regaña, Á. Cappa, F. Castejón, J.B.O. Caughman, M. Tereshchenko, A. Ros, D.A. Rasmussen and J.B. Wilgen, Electron Bernstein waves emission in the TJ-II stellarator, Plasma Phys. Control. Fusion 53 (2011) 065009