研究目的
To perform phase noise characterization of a tunable laser source and investigate the impact of equalization-enhanced phase noise (EEPN) in a coherent transmission system.
研究成果
The low frequency region of the FM-noise PSD of the LO laser combined with the accumulated dispersion will introduce an OSNR penalty and BER floor limiting the performance of the system. The OSNR penalty and BER floor increase with the accumulated dispersion but they can be reduced by using a LO laser with flat FM-noise PSD profile or by using a LO laser with reduced linewidth.
研究不足
The study is limited to a 30 Gbaud channel with 16QAM modulation and pilot-based carrier phase estimation with 3% overhead. The impact of higher order modulation formats and higher baudrates, which are more sensitive to phase noise, is not investigated.
1:Experimental Design and Method Selection:
The phase noise characterization of a tunable laser source is performed using a delayed self-homodyne configuration. The measured FM-noise PSD is reproduced by simulations to investigate the impact of EEPN in a coherent transmission system.
2:Sample Selection and Data Sources:
The tunable laser source is capable of tuning to 103 channels in a 50 GHz grid between 1527.6-1568.36 nm. The phase noise characterization is performed for channels 13, 45, 95, and
3:6-36 nm. The phase noise characterization is performed for channels 13, 45, 95, and List of Experimental Equipment and Materials:
103.
3. List of Experimental Equipment and Materials: The measurement setup includes a tunable laser under test, a fiber optic isolator, a 3 dB power splitter, a polarization controller (PC), a coherent receiver, and a real-time scope.
4:Experimental Procedures and Operational Workflow:
The measurement consists of the tunable laser under test; a fiber optic isolator, to avoid reflections back into the laser; a 3 dB power splitter, with the first branch connected to a polarization controller (PC) and afterwards to the coherent receiver; and the second branch connected to a 27 km delay fiber, assuring that the coherence length of the laser is exceeded, then connected to a PC and finally to the coherent receiver. From the coherent receiver, the in-phase and quadrature signals are recovered and digitized by the real-time scope at 20 GS/s.
5:Data Analysis Methods:
The FM-noise PSD and the field spectrum are generated from the measured signal. The linewidth of each channel is calculated by averaging the FM-noise PSD values from the frequency region >1 MHz.
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