研究目的
To investigate the regenerative property of nonlinearity-based UWB pulse generation techniques and compare them with the optical delay line-based technique, including dynamically controlling the width of UWB mono-cycle pulses and demonstrating noise resilience.
研究成果
The nonlinear medium-based technique allows dynamic width tuning of UWB mono-cycle pulses by adjusting optical signal power and exhibits high resilience to ASE noise, outperforming the optical delay line-based technique at low OSNRs. HNLF performs better than SOA due to its passive nature and lower noise induction. This regenerative property is attributed to XPM-induced phase shift isolating the CW signal from noise.
研究不足
The study is based on numerical simulations using OptSim, not experimental validation, which may not capture all real-world effects. The wireless channel is not considered, limiting the applicability to full UWB systems. The techniques are sensitive to specific parameters like filter characteristics and nonlinear medium properties, which could affect robustness in practical scenarios.
1:Experimental Design and Method Selection:
The study uses numerical simulations via the OptSim commercial tool to model UWB signal generation. Two techniques are compared: nonlinear medium-based (using HNLF or SOA) and optical delay line-based. The nonlinear technique involves cross-phase modulation (XPM) in the medium, followed by PM-to-IM conversion using an optical band-pass filter (OBPF). The delay line technique uses optical splitting, delaying, and subtraction to generate pulses.
2:Sample Selection and Data Sources:
Simulated optical signals are generated with specific parameters, including a pulsed laser source at 1549 nm modulated with 5 Gbps baseband data, a CW laser at 1548 nm, and a white light source to introduce ASE noise. No real-world samples are used; it is entirely simulation-based.
3:List of Experimental Equipment and Materials:
Key components include pulsed laser source, CW laser, optical couplers, Mach-Zehnder modulator, erbium-doped fiber amplifier (EDFA), highly nonlinear fiber (HNLF), semiconductor optical amplifier (SOA), optical band-pass filter (OBPF), single-mode fiber (SMF), photodetector, electrical amplifier, electrical splitter, low-pass filter, optical delay line, variable optical attenuator, and subtractor. Parameters for HNLF (length 0.4 km, dispersion -1.7 ps/nm/km, dispersion slope 0.023 ps/nm2/km, nonlinear coefficient 18/W·km) and SOA (cavity length 5e-4 m, injection current 0.3 A, differential gain 2.78e-20 m2, initial carrier density 3e24 m?3) are specified.
4:4 km, dispersion -7 ps/nm/km, dispersion slope 023 ps/nm2/km, nonlinear coefficient 18/W·km) and SOA (cavity length 5e-4 m, injection current 3 A, differential gain 78e-20 m2, initial carrier density 3e24 m?3) are specified. Experimental Procedures and Operational Workflow:
4. Experimental Procedures and Operational Workflow: For the nonlinear technique, the pulsed signal is coupled with CW probe and noise source, amplified by EDFA, passed through the nonlinear medium (HNLF or SOA) to induce chirp via XPM, filtered by OBPF for PM-to-IM conversion, transmitted over 20 km SMF, photodetected, and processed for BER analysis. For the delay line technique, the signal is split, delayed, attenuated, photodetected, subtracted, and similarly processed. BER is measured at different OSNR values.
5:Data Analysis Methods:
BER is calculated using the BER estimator in the simulation tool. Results are plotted against received optical power for various OSNRs to compare performance and noise resilience.
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OptSim
Commercial simulation tool used for numerical simulations of optical communication systems.
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Highly Nonlinear Fiber
Used as a nonlinear medium to induce cross-phase modulation (XPM) on the CW probe signal for UWB pulse generation.
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Semiconductor Optical Amplifier
Used as a nonlinear medium to induce cross-phase modulation (XPM) on the CW probe signal for UWB pulse generation.
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Erbium-Doped Fiber Amplifier
Amplifies the optical signal before input to the nonlinear medium or transmission.
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Optical Band-Pass Filter
Performs PM-to-IM conversion by filtering the chirped CW signal, acting as a shaping filter.
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Single-Mode Fiber
Transmits the optical signal over a distance of 20 km.
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Photodetector
PIN-PD
Converts the optical signal to an electrical signal for UWB pulse generation and analysis.
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Electrical Amplifier
Amplifies the electrical signal after photodetection.
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Optical Delay Line
Delays one path of the optical signal in the delay line-based technique for pulse generation.
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Variable Optical Attenuator
VOA
Attenuates the optical signal in one path to match power levels in the delay line technique.
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Subtractor
Sub
Subtracts the delayed and attenuated signals to generate UWB pulses in the electrical domain.
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Low-Pass Filter
LPF
Filters out high-frequency harmonics after self-mixing to extract baseband data.
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Electrical Splitter
ES
Splits the electrical signal for self-mixing in the mobile station.
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Mixer
Performs self-mixing of the UWB signal to extract baseband data.
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BER Estimator
Calculates the bit error rate to characterize system performance.
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