2009
DOI: 10.1063/1.3273780
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Non-Linear Effects on the LH Wave Coupling in Tore Supra and Impact on the LH Current Drive Efficiency

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Cited by 12 publications
(9 citation statements)
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“…L 0.5 ). Studies 19 have shown that LHW-plasma coupling was related to the connection length in front of the LHW antenna. Let us consider the 3 configurations of limiter, single null, and double null.…”
Section: Experiments and Resultsmentioning
confidence: 98%
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“…L 0.5 ). Studies 19 have shown that LHW-plasma coupling was related to the connection length in front of the LHW antenna. Let us consider the 3 configurations of limiter, single null, and double null.…”
Section: Experiments and Resultsmentioning
confidence: 98%
“…The reason for the different coupling characteristics in the different rows is not understood completely yet. Since magnetic connection is local and LHW-plasma coupling depends on connection length, 19 it is speculated that different sensitivity of coupling on distance may be ascribed to the different magnetic connection length. Unfortunately, no density measurement at different rows is available for the present.…”
Section: Experiments and Resultsmentioning
confidence: 99%
“…During October and November 2008, dedicated experiments were carried out in Tore Supra in order to compare the measured power RCs on the C2 and C3 antennas with the numerical results from the ALOHA code. In order to avoid possible non-linear effects [35,36], low power pulses were used, i.e. pulses for which the power density at the mouth of the antenna is lower than 2 MW m −2 (corresponding to a total requested input power of 100 kW for C2 and 75 kW for C3).…”
Section: Comparison With Experimental Resultsmentioning
confidence: 99%
“…A complete qualification of this new antenna at a low power (∼200 kW) has been made to test the coupling characteristics (power reflection coefficient, directivity, etc) and to compare them with predicted results from linear coupling theory. Low power experiments are required to avoid non-linear plasma-waves interactions, as previously observed [8]. After briefly mentioning the linear theory of LH coupling in section 2, this paper describes the design and the principle of the new launcher as well as the main differences with a FAM launcher in section 3.…”
Section: Introductionmentioning
confidence: 99%