2016
DOI: 10.7149/opa.49.4.49501
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Design of polarimeters based on liquid crystals and biaxial crystals for polarization metrology

Abstract: ABSTRACT:This paper reviews three polarimeters based on different types of liquid crystal cells (parallel and twisted nematic, and ferroelectric), as well as a polarimeter based on the conical refraction phenomenon (occurring in biaxial crystals). A comparative analysis between them is included in order to summarize their main features and to point out their strengths and limitations. Then, the best candidate for imaging polarimetry is selected and implemented. Several polarization images are analyzed in order… Show more

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Cited by 6 publications
(6 citation statements)
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“…So that our measurement closely aligns with the operating paradigms used for imaging short-lived phenomena, the measurements shown in this paper were achieved using a gate width of 1 µs and a gain of 4095. There has been much research into optimizing many different types of polarimeters [3,[27][28][29][30]. Our decision to mount LCVRs at 0 • and 45 • for both the PSA and PSG was due to the ease of use and flexibility afforded by this setup.…”
Section: Methodsmentioning
confidence: 99%
“…So that our measurement closely aligns with the operating paradigms used for imaging short-lived phenomena, the measurements shown in this paper were achieved using a gate width of 1 µs and a gain of 4095. There has been much research into optimizing many different types of polarimeters [3,[27][28][29][30]. Our decision to mount LCVRs at 0 • and 45 • for both the PSA and PSG was due to the ease of use and flexibility afforded by this setup.…”
Section: Methodsmentioning
confidence: 99%
“…Each row of the matrix M then corresponds to the Stokes vector of a polarization component that is sampled by the polarimeter. The polarization state is determined from the power measurements by inverting the device matrix, via S M −1 P. The accuracy and extent to which polarization can be deduced depends on the properties of the device matrix with respect to inversion, and the left inverse of the device matrix,M −1 M T M −1 M T , can be used instead of M −1 when the dimensions of M are not 4 × 4 [24]. The optimization of the device matrix is a problem that is generally applicable to polarimeter design, not just the architecture discussed here, and is discussed in greater detail in Supplement 1, Section 4, which discusses device matrix design.…”
Section: Conceptmentioning
confidence: 99%
“…This may in part be explained by the difficulty associated with capturing its inherently vectorial nature: polarization measurements require several measurements of the same signal, each targeting one of its vector components. This issue is addressed by current polarimeters by dividing the signal up either in space or in time [7,24]. Typically, the signal is either split into several beam paths (amplitude division), spread over an array of analyzers (wavefront division), or measured multiple times with a time-varying analyzer (time division).…”
Section: Introductionmentioning
confidence: 99%
“…Therefore, tunable linear retarders were required. Liquid-crystal retarders (LCR) [27] are one very useful option. They have been used in a number of spectral birefringent filters, including tunable Lyot filters [25], or dynamic colour filters that combine cholesteric liquid crystal layers [26].…”
Section: Tunable Solc Filter With Liquid-crystal Retardersmentioning
confidence: 99%