Please use this identifier to cite or link to this item: http://hdl.handle.net/2248/6956
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dc.contributor.authorNagaraju, K-
dc.contributor.authorPhanindra, D. V. S-
dc.contributor.authorKrishna Prasad, S-
dc.contributor.authorShankar Rao, D. S-
dc.contributor.authorSreekumar, P-
dc.date.accessioned2020-11-12T15:07:52Z-
dc.date.available2020-11-12T15:07:52Z-
dc.date.issued2018-07-06-
dc.identifier.citationProceedings of the SPIE, Vol. 10702, pp. 107024X-1-107024X-7en_US
dc.identifier.issn1996-756X-
dc.identifier.urihttp://prints.iiap.res.in/handle/2248/6956-
dc.descriptionRestricted Access © SPIE--The International Society for Optical Engineering https://doi.org/10.1117/12.2312503en_US
dc.description.abstractIn a dual-frequency liquid crystal (DFLC), when the frequency of the applied voltage is more than a critical value (fc), the dielectric anisotropy of the material changes from positive to negative. This causes the director to switch its orientation from parallel to the field (for f < fc), to perpendicular to it (f > fc). Hence DFLC can be used in modulating the light by switching the frequency of an externally applied voltage. We present in this work about application of DFLCs in full Stokes polarimetery. A polarization modulator has been worked out based on two DFLCs and two static retarders. The combination of DFLCs’ switching and static retarders are chosen such that more or less equal weightage is given to all the Stokes parameters. Initial results on the optimization of position angles of the modulators are presented towards the goal of achieving polychromatic modulator in the wavelength range 600-900 nm.en_US
dc.language.isoenen_US
dc.publisherSPIE-The International Society for Optical Engineeringen_US
dc.subjectLiquid crystalsen_US
dc.subjectPolarization modulatorsen_US
dc.subjectPolarimetric efficiencyen_US
dc.subjectPolychromatic modulatoren_US
dc.titleFull Stokes polarimetry using dual-frequency liquid crystalsen_US
dc.typeArticleen_US
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