2001
DOI: 10.1063/1.1321744
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Multichannel far-infrared polarimeter-interferometer system on the MST reversed field pinch

Abstract: The multichannel far-infrared ͑FIR͒ heterodyne polarimeter-interferometer system on the Madison Symmetric Torus ͑MST͒ is now operational. The combined system consists of 11 channels with variable radial and toroidal spacing. Poloidal magnetic field is determined by measuring the Faraday rotation of the FIR laser beam after propagation through the plasma by use of a phase technique. The polarimeter has 3 mrad rms noise level and 1 ms temporal resolution while the interferometer resolution is n e dlϭ1ϫ10 12 cm Ϫ… Show more

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Cited by 43 publications
(27 citation statements)
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“…In order to obtain the correct Faraday rotation angle, this response must be measured and used to calibrate the measured data. 24 The measured Faraday rotation angle is equal to the line integral of the product of the electron density and the poloidal magnetic field. Therefore, changes or fluctuations in the Faraday rotation can be caused by either density or magnetic field fluctuations.…”
Section: Methodsmentioning
confidence: 99%
“…In order to obtain the correct Faraday rotation angle, this response must be measured and used to calibrate the measured data. 24 The measured Faraday rotation angle is equal to the line integral of the product of the electron density and the poloidal magnetic field. Therefore, changes or fluctuations in the Faraday rotation can be caused by either density or magnetic field fluctuations.…”
Section: Methodsmentioning
confidence: 99%
“…Details of this procedure have been described elsewhere. 17 Typical polarimeter system rms noise levels are 1 mrad ͑Ϸ0.1°͒ at 100 kHz bandwidth ͓0.4 mrad ͑0.04°͒ at 20 kHz bandwidth͔. The data can be ensemble averaged over similar time windows ͑e.g., sawtooth cycle͒ for further noise reduction.…”
Section: Polarimeter-interferometer Systemmentioning
confidence: 99%
“…A practical method to examine the polarization of counter-rotating circularly polarized probe beams is polarization modulation. 13 To accomplish this, we add a rotating (few Hz) half-wave plate in the optical path to replace the plasma and modulate the polarization. If the probe beams' polarizations are counter-rotating circularly polarized, phase difference between the R beam and L beam will change linearly and equal four times the rotation angle of the half wave plate; any distortion of polarization will lead to a nonlinear response.…”
Section: Systematic Errorsmentioning
confidence: 99%