2018
DOI: 10.1088/1741-4326/aae7e9
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High field side lower hybrid wave launch for steady state plasma sustainment

Abstract: This paper explores how the use of waves in the lower hybrid range of frequencies (LHRF) alleviates many unresolved current drive issues when launched from the high field side (HFS) of a tokamak. Efficient, robust, reliable, steady-state current drive is a requirement for a viable tokamak fusion reactor. Launching LHRF waves from the HFS opens the ‘accessibility window’, allowing for use of a lower parallel refractive index, , for a given plasma density and on-axis magnetic field. The lower waves damp in a re… Show more

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Cited by 20 publications
(15 citation statements)
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“…Fluctuations may therefore be important in understanding the observed SOL absorption of LH waves, particularly at high line averaged densities. Launching at a region with significantly lower density fluctuation amplitudes such as the high field side of a tokamak [59] may therefore be beneficial for increased LHCD efficiency at high densities.…”
Section: Discussionmentioning
confidence: 99%
“…Fluctuations may therefore be important in understanding the observed SOL absorption of LH waves, particularly at high line averaged densities. Launching at a region with significantly lower density fluctuation amplitudes such as the high field side of a tokamak [59] may therefore be beneficial for increased LHCD efficiency at high densities.…”
Section: Discussionmentioning
confidence: 99%
“…The potential benefits of the HFS location are detailed in Ref. 16. The empirical scaling laws for LHRF antenna net power density predict 20 to 40 MW/m 2 at 4.6 GHz (Refs.…”
Section: Radiofrequency Designmentioning
confidence: 99%
“…One feasible approach, which opens up * Author to whom any correspondence should be addressed. the accessibility window in high density plasmas, is that the LHW is launched from the high field side (HFS) [9]; however, the CD efficiency is still limited although the accessibility is improved. High harmonic fast waves (HHFW), also called 'helicon waves', with a frequency between ion cyclotron waves and the LHW can propagate into the center of the plasma without a density limit [10][11][12][13] because the HHFW's main absorption mechanism-electron Landau damping-is weaker than that of the LHW, such that the HHFW can provide an on-axis CD in low electron beta β e (= n e κT e /B 2 /2μ 0 ) [1] operation.…”
Section: Introductionmentioning
confidence: 99%