Chapter Raman Fiber Laser–Based Amplification in Telecommunications (Record no. 43414)

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001 - CONTROL NUMBER
control field https://directory.doabooks.org/handle/20.500.12854/70425
020 ## - INTERNATIONAL STANDARD BOOK NUMBER
International Standard Book Number intechopen.73632
024 7# - OTHER STANDARD IDENTIFIER
Standard number or code 10.5772/intechopen.73632
Terms of availability doi
041 0# - LANGUAGE CODE
Language code of text/sound track or separate title English
042 ## - AUTHENTICATION CODE
Authentication code dc
072 #7 - SUBJECT CATEGORY CODE
Subject category code PHJL
Source bicssc
100 1# - MAIN ENTRY--PERSONAL NAME
Personal name Tan, Mingming
Relationship auth
245 10 - TITLE STATEMENT
Title Chapter Raman Fiber Laser–Based Amplification in Telecommunications
260 ## - PUBLICATION, DISTRIBUTION, ETC.
Name of publisher, distributor, etc. InTechOpen
Date of publication, distribution, etc. 2018
506 0# - RESTRICTIONS ON ACCESS NOTE
Terms governing access Open Access
Source of term star
Standardized terminology for access restriction Unrestricted online access
520 ## - SUMMARY, ETC.
Summary, etc. 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.
540 ## - TERMS GOVERNING USE AND REPRODUCTION NOTE
Terms governing use and reproduction Creative Commons
Use and reproduction rights https://creativecommons.org/licenses/by/3.0/
Source of term cc
-- https://creativecommons.org/licenses/by/3.0/
546 ## - LANGUAGE NOTE
Language note English
650 #7 - SUBJECT ADDED ENTRY--TOPICAL TERM
Topical term or geographic name entry element Laser physics
Source of heading or term bicssc
653 ## - INDEX TERM--UNCONTROLLED
Uncontrolled term Raman amplification, Raman fiber laser, coherent transmission, random fiber laser, cavity fiber laser
773 10 - HOST ITEM ENTRY
Host Biblionumber OAPEN Library ID: ONIX_20210602_10.5772/intechopen.73632_381
Control subfield nnaa
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Uniform Resource Identifier <a href="https://library.oapen.org/bitstream/20.500.12657/49267/1/59240.pdf">https://library.oapen.org/bitstream/20.500.12657/49267/1/59240.pdf</a>
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Public note DOAB: download the publication
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Host name www.oapen.org
Uniform Resource Identifier <a href="https://library.oapen.org/bitstream/20.500.12657/49267/1/59240.pdf">https://library.oapen.org/bitstream/20.500.12657/49267/1/59240.pdf</a>
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Public note DOAB: download the publication
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Host name www.oapen.org
Uniform Resource Identifier <a href="https://directory.doabooks.org/handle/20.500.12854/70425">https://directory.doabooks.org/handle/20.500.12854/70425</a>
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