研究目的
To analyze the effect of phase mask alignment on the Bragg grating reflection spectra in polymer optical fibers, specifically investigating the splitting of the reflection peak at λB = 1560 nm due to tilt angle φ.
研究成果
The experimental analysis confirmed that tilting the phase mask relative to the fiber causes the Bragg reflection peak to split into five peaks, with separation increasing linearly with tilt angle. The peaks were identified as first- and second-order reflections from index periodicities close to Λ and Λ/2, associated with interference of specific diffraction orders. There was good agreement between experimental and theoretical data for inner peaks but slight divergence for outer peaks, likely due to measurement quality. This work provides insights into grating formation mechanisms and has implications for sensing applications where peak distortion must be minimized.
研究不足
The study is limited to a specific type of polymer optical fiber and phase mask, with potential inaccuracies in peak position measurements due to low signal-to-noise ratio for outer side-peaks. The theoretical model neglects wavelength dependence of the effective refractive index, which could introduce minor errors. The setup had constraints in angle control and verification, and the peak heights were low (about 10 dB) due to fiber attenuation.
1:Experimental Design and Method Selection:
The study involved fabricating fiber Bragg gratings (FBGs) in polymer optical fibers (POFs) using a phase mask technique with a multiple order phase mask. The experimental setup allowed for precise control of the tilt angle φ between the phase mask and the fiber. Reflection spectra were monitored during UV irradiation to observe peak splitting and evolution.
2:Sample Selection and Data Sources:
A step-index POF made of PMMA cladding and PMMA/PS copolymer core was used, fabricated at Maria Curie-Sklodowska University. The fiber was annealed at 85°C for 10 hours before inscription to improve spectrum quality.
3:List of Experimental Equipment and Materials:
Equipment included a CW 30 mW He-Cd laser (λUV = 325 nm), a phase mask from Ibsen Photonics (Λ = 1052 nm), plano-convex lenses (focal lengths 75 mm and 25 mm), a silica fiber coupler, a supercontinuum source (SuperK Versa, NKT Photonics), an optical spectrum analyzer (AQ6370C, Yokogawa Electric Corporation), index matching gel, goniometer stage (OptoSigma), rotational stage (OptoSigma), and camera with DLTCamViewer software for angle measurement.
4:Experimental Procedures and Operational Workflow:
The UV beam was focused on the fiber core using lenses. The phase mask was tilted at various angles φ, and reflection spectra were recorded during irradiation. Angles were adjusted and measured with high precision. The inscription process involved monitoring peak positions and separations over time.
5:Data Analysis Methods:
Data were analyzed by comparing experimental peak positions and separations with theoretical predictions based on a model considering interference of diffraction orders. Linear fits were applied to peak separation data, and statistical analysis included fitting errors.
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Phase mask
Λ = 1052 nm
Ibsen Photonics
Used to diffract the UV beam and create interference patterns for grating inscription.
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Supercontinuum source
SuperK Versa
NKT Photonics
Used as a light source for monitoring reflection spectra.
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Optical spectrum analyzer
AQ6370C
Yokogawa Electric Corporation
Used to measure and analyze the reflection spectra of the Bragg gratings.
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He-Cd laser
CW 30 mW
Used for UV irradiation to inscribe Bragg gratings in the polymer optical fiber.
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Plano-convex lenses
Focal lengths 75 mm and 25 mm
Used to focus the UV beam onto the fiber core.
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Goniometer stage
OptoSigma
Used for precise adjustment of the angle θ between the phase mask and fiber.
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Rotational stage
OptoSigma
Used for precise adjustment of the tilt angle φ between the phase mask and fiber.
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Camera with software
DLTCamViewer
Used to observe and measure angles between the fiber and phase mask.
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