Theoretical Analyses of Different Nonlinear Compensation Methods Based on Perturbation Theories in the Unrepeatered System With Raman Amplification
In this paper, the pre- and post-nonlinear compensation (NLC) methods based on regular perturbation (RP) theory are contrastively investigated with the original NLC as a bridge for analyses. Firstly, the numerical error functions of pre-NLC and original NLC are derived, revealing that the numerical...
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description | In this paper, the pre- and post-nonlinear compensation (NLC) methods based on regular perturbation (RP) theory are contrastively investigated with the original NLC as a bridge for analyses. Firstly, the numerical error functions of pre-NLC and original NLC are derived, revealing that the numerical error of pre-NLC is more severe due to the error accumulation. Secondly, we deduce the relevance of post-NLC and original NLC, which uncovers the essential difference is that the input condition of post-NLC possesses certain additional information, making the signal's intensity distribution after post-NLC more beneficial for the hard-decision. Meanwhile, the pre-, post- and original NLC methods based on enhanced regular perturbation (ERP) theory have also been discussed. Finally, the simulation is carried out with signal modulation of 16/32/64 QAM and baud-rate of 32 GBaud in an unrepeartered system with Raman amplification. The results agree with the analyses, the post-NLC is the best while the original NLC surpasses the pre-NLC. Additionally, we demonstrate an experiment with signal modulation of 16 QAM and baud-rate of 10 GBaud. The improvements of the Q 2 -factor of the RP-based and ERP-based post-NLC are about 0.6 dB and 1 dB compared with the electronic dispersion compensation (EDC). |
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Firstly, the numerical error functions of pre-NLC and original NLC are derived, revealing that the numerical error of pre-NLC is more severe due to the error accumulation. Secondly, we deduce the relevance of post-NLC and original NLC, which uncovers the essential difference is that the input condition of post-NLC possesses certain additional information, making the signal's intensity distribution after post-NLC more beneficial for the hard-decision. Meanwhile, the pre-, post- and original NLC methods based on enhanced regular perturbation (ERP) theory have also been discussed. Finally, the simulation is carried out with signal modulation of 16/32/64 QAM and baud-rate of 32 GBaud in an unrepeartered system with Raman amplification. The results agree with the analyses, the post-NLC is the best while the original NLC surpasses the pre-NLC. Additionally, we demonstrate an experiment with signal modulation of 16 QAM and baud-rate of 10 GBaud. The improvements of the Q 2 -factor of the RP-based and ERP-based post-NLC are about 0.6 dB and 1 dB compared with the electronic dispersion compensation (EDC).</description><identifier>ISSN: 1943-0655</identifier><identifier>EISSN: 1943-0655</identifier><identifier>EISSN: 1943-0647</identifier><identifier>DOI: 10.1109/JPHOT.2020.3002655</identifier><identifier>CODEN: PJHOC3</identifier><language>eng</language><publisher>Piscataway: IEEE</publisher><subject>Amplification ; Compensation ; Computer simulation ; digital signal processing ; Error analysis ; Error functions ; Licenses ; Nonlinear analysis ; nonlinearity mitigation ; Optical fiber communication ; Optical fiber dispersion ; Optical fiber theory ; Perturbation methods ; Perturbation theory ; Quadrature amplitude modulation ; Raman amplification ; Stimulated emission</subject><ispartof>IEEE photonics journal, 2020-08, Vol.12 (4), p.1-11</ispartof><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. (IEEE) 2020</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c356t-a8e5baef6f24fb7cd6bcc1bf20549b7d7812c21059c86a1bf0df1f22f9fa7cc13</cites><orcidid>0000-0002-8183-8889 ; 0000-0003-2394-8745</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/9117167$$EHTML$$P50$$Gieee$$Hfree_for_read</linktohtml><link.rule.ids>314,776,780,860,2096,27610,27901,27902,54908</link.rule.ids></links><search><creatorcontrib>Wang, You</creatorcontrib><creatorcontrib>Li, Wei</creatorcontrib><creatorcontrib>Mei, Muyang</creatorcontrib><creatorcontrib>Feng, Zhongshuai</creatorcontrib><creatorcontrib>Zheng, Hao</creatorcontrib><creatorcontrib>Chen, YaoBing</creatorcontrib><title>Theoretical Analyses of Different Nonlinear Compensation Methods Based on Perturbation Theories in the Unrepeatered System With Raman Amplification</title><title>IEEE photonics journal</title><addtitle>JPHOT</addtitle><description>In this paper, the pre- and post-nonlinear compensation (NLC) methods based on regular perturbation (RP) theory are contrastively investigated with the original NLC as a bridge for analyses. Firstly, the numerical error functions of pre-NLC and original NLC are derived, revealing that the numerical error of pre-NLC is more severe due to the error accumulation. Secondly, we deduce the relevance of post-NLC and original NLC, which uncovers the essential difference is that the input condition of post-NLC possesses certain additional information, making the signal's intensity distribution after post-NLC more beneficial for the hard-decision. Meanwhile, the pre-, post- and original NLC methods based on enhanced regular perturbation (ERP) theory have also been discussed. Finally, the simulation is carried out with signal modulation of 16/32/64 QAM and baud-rate of 32 GBaud in an unrepeartered system with Raman amplification. The results agree with the analyses, the post-NLC is the best while the original NLC surpasses the pre-NLC. Additionally, we demonstrate an experiment with signal modulation of 16 QAM and baud-rate of 10 GBaud. The improvements of the Q 2 -factor of the RP-based and ERP-based post-NLC are about 0.6 dB and 1 dB compared with the electronic dispersion compensation (EDC).</description><subject>Amplification</subject><subject>Compensation</subject><subject>Computer simulation</subject><subject>digital signal processing</subject><subject>Error analysis</subject><subject>Error functions</subject><subject>Licenses</subject><subject>Nonlinear analysis</subject><subject>nonlinearity mitigation</subject><subject>Optical fiber communication</subject><subject>Optical fiber dispersion</subject><subject>Optical fiber theory</subject><subject>Perturbation methods</subject><subject>Perturbation theory</subject><subject>Quadrature amplitude modulation</subject><subject>Raman amplification</subject><subject>Stimulated emission</subject><issn>1943-0655</issn><issn>1943-0655</issn><issn>1943-0647</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2020</creationdate><recordtype>article</recordtype><sourceid>ESBDL</sourceid><sourceid>RIE</sourceid><sourceid>DOA</sourceid><recordid>eNpNkc9uGyEQxldVIzVN8wLtBalnu8Au7HJ03T9JlSZR6qhHBOxQY-3CBvDBz9EXLvZGUU-MZr7vN2i-qnpP8JIQLD79uL-62ywppnhZY0w5Y6-qcyKaeoFL_fq_-k31NqUdxlwQJs6rv5sthAjZGTWglVfDIUFCwaIvzlqI4DO6DX5wHlRE6zBO4JPKLnj0E_I29Al9Vgl6VBr3EPM-6nl6wrqCch7lLaBHH2EClQuyR78OKcOIfru8RQ9qVB6txmlwtnziaH5XnVk1JLh8fi-qx29fN-urxc3d9-v16mZhasbzQnXAtALLLW2sbk3PtTFEW4pZI3Tbtx2hhhLMhOm4KgPcW2IptcKqtijri-p65vZB7eQU3ajiQQbl5KkR4h-pYrnMALLrDMaad4z0pBEt77imuOlJqwkljPPC-jizphie9pCy3IV9LPdMkjbl-KLpxFFFZ5WJIaUI9mUrwfIYpDwFKY9Byucgi-nDbHIA8GIQhLSEt_U_crucVw</recordid><startdate>20200801</startdate><enddate>20200801</enddate><creator>Wang, You</creator><creator>Li, Wei</creator><creator>Mei, Muyang</creator><creator>Feng, Zhongshuai</creator><creator>Zheng, Hao</creator><creator>Chen, YaoBing</creator><general>IEEE</general><general>The Institute of Electrical and Electronics Engineers, Inc. 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Firstly, the numerical error functions of pre-NLC and original NLC are derived, revealing that the numerical error of pre-NLC is more severe due to the error accumulation. Secondly, we deduce the relevance of post-NLC and original NLC, which uncovers the essential difference is that the input condition of post-NLC possesses certain additional information, making the signal's intensity distribution after post-NLC more beneficial for the hard-decision. Meanwhile, the pre-, post- and original NLC methods based on enhanced regular perturbation (ERP) theory have also been discussed. Finally, the simulation is carried out with signal modulation of 16/32/64 QAM and baud-rate of 32 GBaud in an unrepeartered system with Raman amplification. The results agree with the analyses, the post-NLC is the best while the original NLC surpasses the pre-NLC. Additionally, we demonstrate an experiment with signal modulation of 16 QAM and baud-rate of 10 GBaud. The improvements of the Q 2 -factor of the RP-based and ERP-based post-NLC are about 0.6 dB and 1 dB compared with the electronic dispersion compensation (EDC).</abstract><cop>Piscataway</cop><pub>IEEE</pub><doi>10.1109/JPHOT.2020.3002655</doi><tpages>11</tpages><orcidid>https://orcid.org/0000-0002-8183-8889</orcidid><orcidid>https://orcid.org/0000-0003-2394-8745</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | Amplification Compensation Computer simulation digital signal processing Error analysis Error functions Licenses Nonlinear analysis nonlinearity mitigation Optical fiber communication Optical fiber dispersion Optical fiber theory Perturbation methods Perturbation theory Quadrature amplitude modulation Raman amplification Stimulated emission |
title | Theoretical Analyses of Different Nonlinear Compensation Methods Based on Perturbation Theories in the Unrepeatered System With Raman Amplification |
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