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Photonic Microwave Up-Conversion Link With Compensation of Chromatic Dispersion-Induced Power Fading
An effective scheme of frequency doubling up-conversion is proposed and demonstrated, which achieves the generation of high-frequency microwave signal and the compensation of chromatic dispersion-induced power fading (CDIPF). The system structure is based on a cascading of a Sagnac loop and a Mach-Z...
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Published in: | IEEE photonics journal 2019-08, Vol.11 (4), p.1-10 |
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description | An effective scheme of frequency doubling up-conversion is proposed and demonstrated, which achieves the generation of high-frequency microwave signal and the compensation of chromatic dispersion-induced power fading (CDIPF). The system structure is based on a cascading of a Sagnac loop and a Mach-Zehnder modulator (MZM), where a phase modulator is used in the Sagnac loop. In the loop, only the clockwise propagating light wave is modulated by a small local oscillator signal, leaving the counter-clockwise propagating light wave unmodulated because of the velocity mismatch. The output signal is divided into two parts, one traveling into an MZM and the other entering an optical phase shifter. The intermediate frequency signal is supplied to the MZM, which is biased at its minimum point and then the carrier-suppressed double sideband is achieved. With the adjustment of the optical phase shift, the CDIPF can be compensated at any frequency. In the simulation, by comparing the frequency responses of the proposed link with and without dispersion compensation, we successfully demonstrate the performance of power fading compensation for 60- and 80-km link. Consequently, the spurious-free dynamic range is effectively improved by 13.54 dB at 22.6 GHz for 60-km link. |
doi_str_mv | 10.1109/JPHOT.2019.2928031 |
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The system structure is based on a cascading of a Sagnac loop and a Mach-Zehnder modulator (MZM), where a phase modulator is used in the Sagnac loop. In the loop, only the clockwise propagating light wave is modulated by a small local oscillator signal, leaving the counter-clockwise propagating light wave unmodulated because of the velocity mismatch. The output signal is divided into two parts, one traveling into an MZM and the other entering an optical phase shifter. The intermediate frequency signal is supplied to the MZM, which is biased at its minimum point and then the carrier-suppressed double sideband is achieved. With the adjustment of the optical phase shift, the CDIPF can be compensated at any frequency. In the simulation, by comparing the frequency responses of the proposed link with and without dispersion compensation, we successfully demonstrate the performance of power fading compensation for 60- and 80-km link. Consequently, the spurious-free dynamic range is effectively improved by 13.54 dB at 22.6 GHz for 60-km link.</description><identifier>ISSN: 1943-0655</identifier><identifier>EISSN: 1943-0655</identifier><identifier>EISSN: 1943-0647</identifier><identifier>DOI: 10.1109/JPHOT.2019.2928031</identifier><identifier>CODEN: PJHOC3</identifier><language>eng</language><publisher>Piscataway: IEEE</publisher><subject>Compensation ; Fading ; Fiber optic communications ; Frequency modulation ; Mach-Zehnder interferometers ; Microwave photonics ; Optical fibers ; Optical modulation ; Phase shifters ; power fading ; Radio over fiber (RoF) ; Sagnac interferometers ; Second harmonic generation ; Signal generation ; up-conversion ; Upconversion ; Wave propagation</subject><ispartof>IEEE photonics journal, 2019-08, Vol.11 (4), p.1-10</ispartof><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. (IEEE) 2019</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c405t-f5ae19dd4a4ac1be97f9869d12d68d3a5b033de4623d6c68cc1cd8107c338e83</citedby><cites>FETCH-LOGICAL-c405t-f5ae19dd4a4ac1be97f9869d12d68d3a5b033de4623d6c68cc1cd8107c338e83</cites><orcidid>0000-0002-5638-5988 ; 0000-0002-8647-6127 ; 0000-0003-4877-5975</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/8760364$$EHTML$$P50$$Gieee$$Hfree_for_read</linktohtml><link.rule.ids>314,780,784,27633,27924,27925,54933</link.rule.ids></links><search><creatorcontrib>Chen, Dan</creatorcontrib><creatorcontrib>Shang, Tao</creatorcontrib><creatorcontrib>Liu, Xiongchao</creatorcontrib><creatorcontrib>Li, Gufeng</creatorcontrib><creatorcontrib>Zhang, Yinling</creatorcontrib><title>Photonic Microwave Up-Conversion Link With Compensation of Chromatic Dispersion-Induced Power Fading</title><title>IEEE photonics journal</title><addtitle>JPHOT</addtitle><description>An effective scheme of frequency doubling up-conversion is proposed and demonstrated, which achieves the generation of high-frequency microwave signal and the compensation of chromatic dispersion-induced power fading (CDIPF). The system structure is based on a cascading of a Sagnac loop and a Mach-Zehnder modulator (MZM), where a phase modulator is used in the Sagnac loop. In the loop, only the clockwise propagating light wave is modulated by a small local oscillator signal, leaving the counter-clockwise propagating light wave unmodulated because of the velocity mismatch. The output signal is divided into two parts, one traveling into an MZM and the other entering an optical phase shifter. The intermediate frequency signal is supplied to the MZM, which is biased at its minimum point and then the carrier-suppressed double sideband is achieved. With the adjustment of the optical phase shift, the CDIPF can be compensated at any frequency. In the simulation, by comparing the frequency responses of the proposed link with and without dispersion compensation, we successfully demonstrate the performance of power fading compensation for 60- and 80-km link. Consequently, the spurious-free dynamic range is effectively improved by 13.54 dB at 22.6 GHz for 60-km link.</description><subject>Compensation</subject><subject>Fading</subject><subject>Fiber optic communications</subject><subject>Frequency modulation</subject><subject>Mach-Zehnder interferometers</subject><subject>Microwave photonics</subject><subject>Optical fibers</subject><subject>Optical modulation</subject><subject>Phase shifters</subject><subject>power fading</subject><subject>Radio over fiber (RoF)</subject><subject>Sagnac interferometers</subject><subject>Second harmonic generation</subject><subject>Signal generation</subject><subject>up-conversion</subject><subject>Upconversion</subject><subject>Wave propagation</subject><issn>1943-0655</issn><issn>1943-0655</issn><issn>1943-0647</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2019</creationdate><recordtype>article</recordtype><sourceid>ESBDL</sourceid><sourceid>DOA</sourceid><recordid>eNpNUU1vEzEQXVUgUQp_gF4scd7U46-1j2ihNCioOQRxtBx7tnFo1ou9acW_76ZbVZxm5um9N6N5VfUJ6AKAmqsf65vbzYJRMAtmmKYczqpzMILXVEn55r_-XfW-lD2lyoA051VY79KY-ujJz-hzenQPSH4NdZv6B8wlpp6sYv-H_I7jjrTpMGBf3HiCU0faXU6HafLkayzDTK-XfTh6DGSdHjGTaxdif_ehetu5-4IfX-pFtbn-tmlv6tXt92X7ZVV7QeVYd9IhmBCEE87DFk3TGa1MABaUDtzJLeU8oFCMB-WV9h580EAbz7lGzS-q5WwbktvbIceDy_9sctE-AynfWZenc-_RKvRcqo41SoDQcuvMtlFSgNEaXNPA5PV59hpy-nvEMtp9OuZ-ut4yphopjGZiYrGZNb2ulIzd61ag9hSMfQ7GnoKxL8FMostZFBHxVaAbRbkS_AllGYmn</recordid><startdate>20190801</startdate><enddate>20190801</enddate><creator>Chen, Dan</creator><creator>Shang, Tao</creator><creator>Liu, Xiongchao</creator><creator>Li, Gufeng</creator><creator>Zhang, Yinling</creator><general>IEEE</general><general>The Institute of Electrical and Electronics Engineers, Inc. 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The system structure is based on a cascading of a Sagnac loop and a Mach-Zehnder modulator (MZM), where a phase modulator is used in the Sagnac loop. In the loop, only the clockwise propagating light wave is modulated by a small local oscillator signal, leaving the counter-clockwise propagating light wave unmodulated because of the velocity mismatch. The output signal is divided into two parts, one traveling into an MZM and the other entering an optical phase shifter. The intermediate frequency signal is supplied to the MZM, which is biased at its minimum point and then the carrier-suppressed double sideband is achieved. With the adjustment of the optical phase shift, the CDIPF can be compensated at any frequency. In the simulation, by comparing the frequency responses of the proposed link with and without dispersion compensation, we successfully demonstrate the performance of power fading compensation for 60- and 80-km link. Consequently, the spurious-free dynamic range is effectively improved by 13.54 dB at 22.6 GHz for 60-km link.</abstract><cop>Piscataway</cop><pub>IEEE</pub><doi>10.1109/JPHOT.2019.2928031</doi><tpages>10</tpages><orcidid>https://orcid.org/0000-0002-5638-5988</orcidid><orcidid>https://orcid.org/0000-0002-8647-6127</orcidid><orcidid>https://orcid.org/0000-0003-4877-5975</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | Compensation Fading Fiber optic communications Frequency modulation Mach-Zehnder interferometers Microwave photonics Optical fibers Optical modulation Phase shifters power fading Radio over fiber (RoF) Sagnac interferometers Second harmonic generation Signal generation up-conversion Upconversion Wave propagation |
title | Photonic Microwave Up-Conversion Link With Compensation of Chromatic Dispersion-Induced Power Fading |
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