研究目的
To achieve a single bandpass microwave photonic filter with wide tunability based on stimulated Brillouin scattering using a dual-fiber structure.
研究成果
The proposed dual-fiber structure successfully achieves a widely tunable single bandpass microwave photonic filter with a central frequency of 21.4 GHz, bandwidth of 38 MHz, and out-of-band rejection over 30 dB. Tunability up to 40 GHz is demonstrated using a CS-SSB modulation scheme, showing improved performance over single-fiber approaches.
研究不足
The tuning range is limited by the SBS frequency shifts in the fibers, and variations in bandwidth occur due to changes in pump power and non-ideal components like the intensity modulator and bandpass filter. Pump depletion in the fibers can affect linearity and gain spectrum broadening.
1:Experimental Design and Method Selection:
The experiment uses a dual-fiber structure to cascade Brillouin frequency shifter and amplification, employing stimulated Brillouin scattering (SBS) effects in two fibers to shift the filter center frequency higher and achieve wide tunability. The theoretical model includes Lorentzian gain profiles and equations for gain and filter response.
2:Sample Selection and Data Sources:
Optical fibers include a 6.2-km single mode fiber (SMF) with Brillouin frequency shift of 10.8 GHz and a 25-km non-zero dispersion shifted fiber (NZDSF) with Brillouin frequency shift of 10.6 GHz. Data is collected using a vector network analyzer (VNA).
3:2-km single mode fiber (SMF) with Brillouin frequency shift of 8 GHz and a 25-km non-zero dispersion shifted fiber (NZDSF) with Brillouin frequency shift of 6 GHz. Data is collected using a vector network analyzer (VNA). List of Experimental Equipment and Materials:
3. List of Experimental Equipment and Materials: Tunable laser (Keysight 81950A), VNA (Keysight N5234A), phase modulator (Thorlabs LN65S), erbium-doped fiber amplifiers (EDFA, Amonics), optical circulators, polarization controllers (PC1, PC2, PC3), optical isolator (ISO), dispersion compensator (DC, TeraXion), photodetector (PD), intensity modulator (Sumitomo), optical bandpass filter (Finisar Waveshaper 4000s), and various fibers (SMF, NZDSF).
4:Experimental Procedures and Operational Workflow:
Light from the tunable laser is split into two branches. The upper branch modulates the signal with RF from VNA using a phase modulator. The lower branch amplifies the carrier, injects it into SMF for first-stage SBS, amplifies the Stokes light, and injects it into NZDSF for second-stage SBS. The phase-modulated signal passes through NZDSF, dispersion is compensated, and detected by PD. Frequency response is measured with VNA. Tunability is tested by inserting a CS-SSB frequency shifter.
5:Data Analysis Methods:
Frequency response is analyzed using the VNA to measure central frequency, bandwidth, and rejection ratio. Bandwidth and peak power are plotted against pump power variations.
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Tunable Laser
81950A
Keysight
Provides the optical carrier at 1550.92 nm with narrow linewidth for the experiment.
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Vector Network Analyzer
N5234A
Keysight
Generates and measures RF signals to characterize the frequency response of the microwave photonic filter.
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Phase Modulator
LN65S
Thorlabs
Modulates the optical carrier with the RF signal from the VNA.
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Optical Bandpass Filter
Waveshaper 4000s
Finisar
Eliminates undesired sidebands in the CS-SSB modulation to achieve single sideband output.
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Non-Zero Dispersion Shifted Fiber
MetroCor
Corning
Used as Fiber2 for the second-stage SBS with a Brillouin frequency shift of 10.6 GHz.
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Erbium-Doped Fiber Amplifier
Amonics
Amplifies the optical signals in the pump and signal branches to achieve sufficient power for SBS.
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Dispersion Compensator
TeraXion
Compensates for dispersion in the NZDSF to minimize PM-IM conversion.
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Intensity Modulator
Sumitomo
Used in the CS-SSB modulation scheme to shift the optical frequency for tunability.
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Single Mode Fiber
Used as Fiber1 for the first-stage SBS with a Brillouin frequency shift of 10.8 GHz.
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