A Channel Model to Deal with Distributed Noises and Nonlinear Effects in a Fiber System with Distributed Raman Amplifiers
Source abstract
Abstract
Nowadays, the distributed fiber Raman amplifier (FRA) has become more and more popular in long-haul fiber systems, owing to its lower noise figures and weaker nonlinear effects in the link. The critical issue in distributed FRAs is the presence of various kinds of noises and their interactions with the signal. However, the existing Raman channel models and their numerical solving methods can only partially describe how the randomly distributed noises interact with the signal. This causes the difficulties in analyzing the distributed FRA precisely and the inconveniences for the applications and the maintenance of FRA systems. In this paper, we propose a modified Raman channel model to describe more comprehensively the interactions between the distributed noises and the signal under the influence of loss, distributed gain, dispersion, and nonlinear effects in the distributed FRA systems. With the comparisons of the error–vector magnitude (EVM) curves, our model can get lower errors in the experimental results regarding bidirectional pumped FRA single-span fiber systems and multi-span systems with backward-pumped FRAs.
Source: crossref · Quality: baseline
Research context
OpenAlex topics: Optical Network Technologies · Random lasers and scattering media · Advanced Photonic Communication Systems
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Wuhan National Laboratory for Optoelectronics, Huazhong University of Science and Technology, Wuhan 430074, China
China Southern Power Grid, Guangzhou 510530, China
Funding
National Key Research and Development Program of China
References (19)
Show source-provided references
1. Raman Amplification for fiber communications systems10.1109/JLT.2003.822828 ↗
2. Pelouch, W.S. (2015, January 22–26). Raman amplification: An enabling technology for high capacity, long-haul transmission. Proceedings of the Optical Fiber Communication Conference, Los Angeles, CA, USA.10.1364/OFC.2015.W1C.1 ↗
3. Operational issues facing commercial raman amplifier system: Safety measures and system designs10.1109/JLT.2015.2471841 ↗
4. Power consumption analysis of hybrid EDFA/Raman amplifiers in long-haul transmission systems10.1109/JLT.2017.2668768 ↗
5. Spectrally efficient single carrier 400G optical signal transmission10.1007/s12200-018-0833-x ↗
6. Unrepeatered 100G transmission over 520.6 km of G.652 fiber and 556.7 km of G.654 fiber with commercial raman DWDM system and enhanced ROPA10.1109/JLT.2014.2356498 ↗
7. Random distributed feedback fibre laser10.1038/nphoton.2010.4 ↗
8. Distributed vibration sensor based on coherent detection of phase-OTDR
9. Achievable information rates for high-speed long-haul optical transmission10.1109/JLT.2005.857751 ↗
10. Creating single collective atomic excitations via spontaneous Raman emission in inhomogeneously broadened systems: Beyond the adiabatic approximation10.1103/PhysRevA.79.063828 ↗
11. Combined effect of ASE and DRBS on noise in pulse-pumped fiber Raman amplifiers10.1109/JLT.2012.2209630 ↗
12. Double rayleigh scattering noise in lumped and distributed raman amplifiers10.1109/JLT.2003.817705 ↗
13. Pump to signal RIN transfer in Raman fiber amplifiers10.1109/50.939794 ↗
14. Agrawal, G.P. (2013). Pulse Propagation in Fibers. Nonlinear Fiber Optics, Elsevier. [5th ed.]. Chapter 2.10.1016/B978-0-12-397023-7.00002-4 ↗
15. Agrawal, G.P. (2013). Stimulated Raman Scattering. Nonlinear Fiber Optics, Elsevier. [5th ed.]. Chapter 8.10.1016/B978-0-12-397023-7.00008-5 ↗
16. Statistical properties of partially coherent CW fiber lasers10.1364/OL.35.003288 ↗
17. Influence of polarization on pump-signal RIN transfer and cross-phase modulation in copumped Raman amplifiers10.1109/JLT.2006.879218 ↗
18. Quasi-lossless transmission using second-order Raman amplification and fibre Bragg gratings10.1364/OPEX.12.004372 ↗
19. Noise induced in optical fibers by double Rayleigh scattering of a laser with a 1/(f^ν) frequency noise10.1364/OL.41.001265 ↗