The resolution of the measurement detection and sensitivity of a polarized low coherence interferometer (PLCI) can be pre-engineered by optimizing the key parameters of the birefringent wedge, which is rarely reported. In this work, we introduce a liquid crystal (LC) wedge in the PLCI and use it to demodulate Fabry–Perot (FP) cavity length. The birefringence property of the nematic LC is used to convert the optical path difference (OPD) of the sensor into a spatial distribution. This results in the production of localized interference fringe patterns. The formation of PLCI fringes and the related shift of the interferogram with a variation in the displacement of the FP displacement sensor is explained with reference to the OPD matching between an LC wedge and the FP cavity. The displacement value is demodulated from the obtained fringe pattern by tracking the centroid position of the fringe envelope and also considering the birefringence dispersion. An additional simulation study shows that the spatial position of the interferogram signal coupled with the dispersion coefficient is almost identical to the experimental data. The demodulated results from both the simulation and experimental investigations are found to be consistent with each other and closely agree with the actual cavity length. Further, the possibility to enhance the sensing resolution is examined by modulating the interferogram fringes using an electric field. Compared to birefringent crystals, the LC wedge presented here is found to be advantageous for high precision and tunability of the measurement range, which is useful for robust fiber optic sensing applications.
We report a new, to the best of our knowledge, approach to determine the refractive indices (RIs) of liquid crystal (LC) systems by considering a double transmission phenomenon of a light beam within the LC medium and the principle of the wedged-cell refractometer. This modified system delivers better spatial resolution of refracted beams in terms of well-resolved spots, compared to the single transmission of a beam in the conventional thin-prism method. The deviation angle obtained in this method is found to be comparatively greater than that of the thin-prism method. The higher values of deviation angle are described using a theoretical model and further experimentally demonstrated for the 5CB nematic LC compound. The variation of the principal RIs (
n
o
,
n
e
), and hence the birefringence (
Δ
n
) with temperature as well as electric field is investigated for both transmission methods. A relative comparison is carried out between the simulated and standard values obtained from literature. The present technique provides a higher spatial beam resolution to determine the RIs and birefringence of LC systems, which can be very advantageous for different modern photonic applications based on beam shaping and steering.
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