2007
DOI: 10.1364/ao.46.001040
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Polarization-holographic gratings for analysis of light 1 Analysis of completely polarized light

Abstract: We consider the possibility of a complete real-time analysis of the polarization state of light using two types of polarization-holographic grating that decompose the light analyzed into orthogonal circular and orthogonal linear bases. It is shown that it is possible to determine the ellipticity, the direction of rotation, and the azimuth of the polarization ellipse of light by the measurement of the intensity of the diffraction orders by the obtained formulas. The possibility of creating gratings that give an… Show more

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Cited by 35 publications
(11 citation statements)
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“…describe the local polarization ellipse, we used the same formalism as Kilosanidze and Kakauridze [18]. To create a rotational pattern, we chose a four-beams configuration.…”
Section: Polarization Holography With Four Beamsmentioning
confidence: 99%
“…describe the local polarization ellipse, we used the same formalism as Kilosanidze and Kakauridze [18]. To create a rotational pattern, we chose a four-beams configuration.…”
Section: Polarization Holography With Four Beamsmentioning
confidence: 99%
“…Such an element was created by means of polarization-holographic method 15 , when several polarization-holographic gratings with different profile of the anisotropy and gyrotropy in the band (gratings C , 90 L , 45 L ) are recorded on one and the same area of polarization-sensitive material, so that the diffracted beams have been spatially separated. [10][11][12] We use polarization-sensitive materials for recording polarization-holographic gratings and elements on their basis. In such materials under the action of polarized light a photoanisotropy and photogyrotropy of optical parameters are induced.…”
Section: Theoretical Modelmentioning
confidence: 99%
“…[12][13][14][15] In the process of diffraction, the element decomposes light incoming on them onto orthogonal circular and linear basis. As a result the element forms 3 beams in +1-st and 3 beams in -1-st orders of diffraction: two orthogonal circularly polarized beams with intensities C I + , C I − , two linearly polarized beam 45 I with an azimuth +45 0 with equal intensities and two linearly polarized beams 90 I with an azimuth +90 0 with equal intensities, and also nondiffracted beam with a state of polarization identical to incoming beam by a state of polarization.…”
Section: Theoretical Modelmentioning
confidence: 99%