Chapter Raman Fiber Laser–Based Amplification in Telecommunications
The chapter demonstrates a detailed study of Raman fiber laser (RFL)-based amplification techniques and their applications in long-haul/unrepeatered coherent transmission systems. RFL-based amplification techniques are investigated from signal/noise power distributions, relative intensity noise (RIN...
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| Fformat: | Online |
| Iaith: | Saesneg |
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InTechOpen
2021
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| Mynediad Ar-lein: | ONIX_20210602_10.5772/intechopen.73632_381 |
| Tagiau: |
Dim Tagiau, Byddwch y cyntaf i dagio'r cofnod hwn!
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| _version_ | 1869514257752653824 |
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| author | Tan, Mingming |
| author_browse | Tan, Mingming |
| author_facet | Tan, Mingming |
| author_sort | Tan, Mingming |
| collection | Directory of Open Access Books |
| description | The chapter demonstrates a detailed study of Raman fiber laser (RFL)-based amplification techniques and their applications in long-haul/unrepeatered coherent transmission systems. RFL-based amplification techniques are investigated from signal/noise power distributions, relative intensity noise (RIN), and fiber laser mode structures. RFL-based amplification techniques can be divided into two categories according to the fiber laser generation mechanism: cavity Raman fiber laser with two fiber Bragg gratings (FBGs) and random distributed feedback (DFB) Raman fiber laser using one FBG. In addition, in cavity fiber laser–based amplification, reducing the reflectivity near the input helps mitigate the signal RIN, thanks to the reduced efficiency of the Stokes shift from the second-order pump. To evaluate the transmission performance, different RFL-based amplifiers were optimized in long-haul coherent transmission systems. Cavity fiber laser–based amplifier introduces >4.15 dB Q factor penalty, because the signal RIN is transferred from the second-order pump. However, random DFB fiber laser–based amplifier prevents the RIN transfer and therefore enables bidirectional second-order pumping, which gives the longest transmission distance up to 7915 km. In addition, using random DFB laser-based amplification achieves the distance of >350 km single mode fiber in unrepeatered DP-QPSK transmission. |
| format | Online |
| id | doab-20.500.12854ir-70425 |
| institution | Directory of Open Access Books |
| language | eng |
| publishDate | 2021 |
| publishDateRange | 2021 |
| publishDateSort | 2021 |
| publisher | InTechOpen |
| publisherStr | InTechOpen |
| record_format | ojs |
| spelling | doab-20.500.12854ir-704252025-08-13T14:11:56Z Chapter Raman Fiber Laser–Based Amplification in Telecommunications Tan, Mingming Raman amplification, Raman fiber laser, coherent transmission, random fiber laser, cavity fiber laser thema EDItEUR::P Mathematics and Science::PH Physics::PHJ Optical physics::PHJL Laser physics thema EDItEUR::P Mathematics and Science::PH Physics::PHJ Optical physics::PHJL Laser physics The chapter demonstrates a detailed study of Raman fiber laser (RFL)-based amplification techniques and their applications in long-haul/unrepeatered coherent transmission systems. RFL-based amplification techniques are investigated from signal/noise power distributions, relative intensity noise (RIN), and fiber laser mode structures. RFL-based amplification techniques can be divided into two categories according to the fiber laser generation mechanism: cavity Raman fiber laser with two fiber Bragg gratings (FBGs) and random distributed feedback (DFB) Raman fiber laser using one FBG. In addition, in cavity fiber laser–based amplification, reducing the reflectivity near the input helps mitigate the signal RIN, thanks to the reduced efficiency of the Stokes shift from the second-order pump. To evaluate the transmission performance, different RFL-based amplifiers were optimized in long-haul coherent transmission systems. Cavity fiber laser–based amplifier introduces >4.15 dB Q factor penalty, because the signal RIN is transferred from the second-order pump. However, random DFB fiber laser–based amplifier prevents the RIN transfer and therefore enables bidirectional second-order pumping, which gives the longest transmission distance up to 7915 km. In addition, using random DFB laser-based amplification achieves the distance of >350 km single mode fiber in unrepeatered DP-QPSK transmission. 2021-02-10T12:58:18Z 2021-06-02T10:10:57Z 2018 chapter ONIX_20210602_10.5772/intechopen.73632_381 https://library.oapen.org/handle/20.500.12657/49267 https://directory.doabooks.org/handle/20.500.12854/70425 eng open access image/jpeg image/jpeg image/jpeg n/a n/a n/a https://library.oapen.org/bitstream/20.500.12657/49267/1/59240.pdf https://library.oapen.org/bitstream/20.500.12657/49267/1/59240.pdf https://library.oapen.org/bitstream/20.500.12657/49267/1/59240.pdf InTechOpen 10.5772/intechopen.73632 10.5772/intechopen.73632 035ecc65-6737-43cf-a13a-6bdf67ce01f4 H2020 Science with and for Society open access |
| spellingShingle | Raman amplification, Raman fiber laser, coherent transmission, random fiber laser, cavity fiber laser thema EDItEUR::P Mathematics and Science::PH Physics::PHJ Optical physics::PHJL Laser physics thema EDItEUR::P Mathematics and Science::PH Physics::PHJ Optical physics::PHJL Laser physics Tan, Mingming Chapter Raman Fiber Laser–Based Amplification in Telecommunications |
| title | Chapter Raman Fiber Laser–Based Amplification in Telecommunications |
| title_full | Chapter Raman Fiber Laser–Based Amplification in Telecommunications |
| title_fullStr | Chapter Raman Fiber Laser–Based Amplification in Telecommunications |
| title_full_unstemmed | Chapter Raman Fiber Laser–Based Amplification in Telecommunications |
| title_short | Chapter Raman Fiber Laser–Based Amplification in Telecommunications |
| title_sort | chapter raman fiber laser based amplification in telecommunications |
| topic | Raman amplification, Raman fiber laser, coherent transmission, random fiber laser, cavity fiber laser thema EDItEUR::P Mathematics and Science::PH Physics::PHJ Optical physics::PHJL Laser physics thema EDItEUR::P Mathematics and Science::PH Physics::PHJ Optical physics::PHJL Laser physics |
| topic_facet | Raman amplification, Raman fiber laser, coherent transmission, random fiber laser, cavity fiber laser thema EDItEUR::P Mathematics and Science::PH Physics::PHJ Optical physics::PHJL Laser physics thema EDItEUR::P Mathematics and Science::PH Physics::PHJ Optical physics::PHJL Laser physics |
| url | ONIX_20210602_10.5772/intechopen.73632_381 |
| work_keys_str_mv | AT tanmingming chapterramanfiberlaserbasedamplificationintelecommunications |