1990
DOI: 10.1088/0029-5515/30/3/005
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Measurement of suprathermal electrons in tokamaks via electron cyclotron transmission

Abstract: The momentum distribution of the current carrying suprathermal electrons is determined from the measurement of X mode transmission near the fundamental of the cyclotron frequency during inductive and radio frequency current drive in the Versator II tokamak. The measurement of the differential attenuation of radiation of two beams with finite and opposite N allows the separation of the wave attenuation due to cyclotron absorption from that due to non-resonant mechanisms. It is shown that such transmission measu… Show more

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Cited by 37 publications
(32 citation statements)
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“…This technique was first implemented by Kirkwood. 23 Previous electron cyclotron absorption measurements have used X-mode waves on MIT's Versator II to determine the fraction of the parallel current drive carried by suprathermal electrons. 24,25 Since the electron plasma frequency f pe ¼ 9.0 GHz is greater than the electron cyclotron frequency jf ce j ¼ 5:0 GHz, the LAPD plasma is overdense f pe > jf ce j.…”
Section: A Overview Of the Wwadmentioning
confidence: 99%
“…This technique was first implemented by Kirkwood. 23 Previous electron cyclotron absorption measurements have used X-mode waves on MIT's Versator II to determine the fraction of the parallel current drive carried by suprathermal electrons. 24,25 Since the electron plasma frequency f pe ¼ 9.0 GHz is greater than the electron cyclotron frequency jf ce j ¼ 5:0 GHz, the LAPD plasma is overdense f pe > jf ce j.…”
Section: A Overview Of the Wwadmentioning
confidence: 99%
“…Figure 1 also shows two whistler probes that are a part of the Whistler Wave Absorption Diagnostic (WWAD) [Thuecks et al, 2012]. This diagnostic measures the suprathermal (v z > v te ) portion of g e (v z ) and is based on a principle that was first implemented by Kirkwood et al [1990]. A whistler mode wave is transmitted between the two whistler probes (1 ′′ dipole antennas immersed in the plasma), and the attenuation of the received signal is used to determine the damping of the wave.…”
Section: 1002/2016gl068865mentioning
confidence: 99%
“…98 With an appropriate choice of parameters, a nearly one-to-one correspondence between major radius ͑or frequency͒ and parallel velocity can be achieved, surrendering spatial resolution. 99 In particular, information on the average skewness of the parallel distribution can be obtained readily by comparing similar measurements with opposite k ʈ , in which all effects attributable to the bulk plasma, such as refraction and scattering, are equal. This type of setup, illustrated by Fig.…”
Section: F501-5mentioning
confidence: 99%
“…7, is naturally attractive for the investigation of LHCD plasmas, and most of the implementations have accordingly been in conjunction with LHCD experiments. [99][100][101][102][103][104][105][106] A variant of this approach consists of launching the waves from the LFS in an oblique, approximately horizontal direction, and measuring the power reflected back from a cutoff layer. The relative attenuation is then attributed to ECA by resonant electrons situated on the LFS of the cutoff, which for appropriate choices of parameters can be selected to be suprathermal within a particular range of velocities.…”
Section: F501-5mentioning
confidence: 99%