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Polarization-independent tilted fiber Bragg grating surface plasmon resonance sensor based on spectrum optimization

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Abstract

We experimentally demonstrated polarization multiplexing schemes in a tilted fiber grating (TFBG) to achieve polarization-independent fiber-optic surface plasmon resonance (SPR) sensors. The first used two orthogonal polarized lights separated by a polarization beam splitter (PBS) that are p-polarized in polarization-maintaining fiber (PMF) and precisely aligned with the tilted grating plane, so as to achieve the transmission of p-polarized light in two opposite directions of the Au-coated TFBG to excite SPR. Alternatively, polarization multiplexing was also achieved by exploring two polarization components to achieve the SPR effect through a Faraday rotator mirror (FRM). The SPR reflection spectra are polarization-independent of the light source and any perturbations to fibers, which are explained by the superposition of p- and s-polarized transmission spectra in equal proportions. The spectrum optimization is presented to reduce the proportion of the s-polarization component. A polarization-independent TFBG-based SPR refractive index (RI) sensor with a wavelength sensitivity of 555.14 nm/RIU and an amplitude sensitivity of 1724.92 dB/RIU for small changes is obtained, exhibiting unique advantages of minimizing the polarization alterations by mechanical perturbations.

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Supplementary Material (6)

NameDescription
Visualization 1       The setup of monitoring the SOP reflecting from a FRM by a polarization analyzer as PCs are adjusted
Visualization 2       The setup of monitoring the SOP reflecting from a FRM by a polarization analyzer as PCs are adjusted
Visualization 3       The setup of proposed polarization-independent TFBG-SPR sensor with a FRM; PCs are not necessary only for the proof of stable SPR spectrum verified by any SOP perpetuation to TFBG and light source.
Visualization 4       The setup of proposed polarization-independent TFBG-SPR sensor with a FRM; PCs are not necessary only for the proof of stable SPR spectrum verified by any SOP perpetuation to TFBG and light source.
Visualization 5       The conventional polarization-dependent TFBG-SPR sensor spectrum changes when adjusting the PC (Visualization 3)
Visualization 6       The conventional polarization-dependent TFBG-SPR sensor spectrum changes when adjusting the PC (Visualization 3)`

Data availability

Data underlying the results presented in this paper are not publicly available at this time but may be obtained from the authors upon reasonable request.

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Figures (6)

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Equations (5)

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