• Advanced Photonics Nexus
  • Vol. 4, Issue 2, 025001 (2025)
Guang-Yao Wang, Han Cao, Zheng-Hao Guo, Chun-Ting Xu*..., Quan-Ming Chen and Wei Hu*|Show fewer author(s)
Author Affiliations
  • Nanjing University, College of Engineering and Applied Sciences, National Laboratory of Solid State Microstructures, Key Laboratory of Intelligent Optical Sensing and Manipulation, Nanjing, China
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    DOI: 10.1117/1.APN.4.2.025001 Cite this Article Set citation alerts
    Guang-Yao Wang, Han Cao, Zheng-Hao Guo, Chun-Ting Xu, Quan-Ming Chen, Wei Hu, "All-liquid-crystal and full-visible-band tunable polarimetry," Adv. Photon. Nexus 4, 025001 (2025) Copy Citation Text show less

    Abstract

    Polarization, the vector nature of electromagnetic waves, plays a vital role in optics. Polarization is characterized by the amplitude contrast and phase difference between two orthogonal polarization states. The present polarimeters usually perform a series of intensity measurements to carry out the polarization detection, making the process bulky and time-consuming. Thereby, compact and broadband-available polarimetry within a single snapshot is urgently demanded. We propose an all-liquid-crystal polarimeter for broadband polarization detection. It is cascaded by a q-plate and a polarization grating. The former is electrically tuned to meet the half-wave condition, whereas the latter is driven to deviate from this condition. After a polarized light passes through this device followed by a polarizer, its amplitude contrast and phase difference between orthogonal spins are read directly from the diffraction pattern. The intensity contrast between ±1st orders depicts the amplitude contrast, whereas the rotating angle of the dark split reveals the phase difference. The Stokes parameters can be calculated accordingly. The polarimeter works in a broad spectral range of 470 to 1100 nm. Through presetting a q-plate array, polarization imaging is demonstrated. It supplies an all-liquid-crystal and full-visible-band tunable Stokes polarimeter that significantly promotes advances in polarization optics.
    E=aLeiφL|L+aReiφR|R=aReiφR(reiΔφ|L+|R),

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    {S1=2r1+r2cosΔφS2=2r1+r2sinΔφS3=1r21+r2.

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    E=Tq-plate·E=i(aLeiφLei2α|R+aReiφRei2α|L),

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    E=TLCPG·E=icos(Γ2)Esin(Γ2)aLeiφLe2i(αβ)|Lsin(Γ2)aReiφRe2i(αβ)|R,

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    Iy=p2cos2(Γ2)[aL2+aR22aLaRcos(Δφ2θ)],

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    Guang-Yao Wang, Han Cao, Zheng-Hao Guo, Chun-Ting Xu, Quan-Ming Chen, Wei Hu, "All-liquid-crystal and full-visible-band tunable polarimetry," Adv. Photon. Nexus 4, 025001 (2025)
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