High-efficiency cascaded Raman fiber laser with random distributed feedback
Cascaded lasing provided by Raman gain (at 1115-nm pumping) and random distributed feedback (via Rayleigh backscattering) in a 1.65-km phosphosilicate fiber is studied. Output power for the second Stokes component (1398 nm) exceeds 5 W at pump power of 11 W. In contrast to conventional cascaded Rama...
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Veröffentlicht in: | Optics express 2014-10, Vol.22 (21), p.24929-24934 |
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creator | Babin, S A Vatnik, I D Laptev, A Yu Bubnov, M M Dianov, E M |
description | Cascaded lasing provided by Raman gain (at 1115-nm pumping) and random distributed feedback (via Rayleigh backscattering) in a 1.65-km phosphosilicate fiber is studied. Output power for the second Stokes component (1398 nm) exceeds 5 W at pump power of 11 W. In contrast to conventional cascaded Raman laser with high-Q cavity for the intermediate first Stokes component, there is no cavity here and no cavity losses, correspondingly. Longitudinal power distribution is shown to be quite different also. As a result, the efficiency of pump to 2nd Stokes wave conversion is not influenced by the intermediate stage and depends only on the integral attenuation in the fiber. Herewith, the number of generated 2nd Stokes photons at the output may even exceed the absorbed pump photons due to the lower attenuation of Stokes waves. |
doi_str_mv | 10.1364/OE.22.024929 |
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Output power for the second Stokes component (1398 nm) exceeds 5 W at pump power of 11 W. In contrast to conventional cascaded Raman laser with high-Q cavity for the intermediate first Stokes component, there is no cavity here and no cavity losses, correspondingly. Longitudinal power distribution is shown to be quite different also. As a result, the efficiency of pump to 2nd Stokes wave conversion is not influenced by the intermediate stage and depends only on the integral attenuation in the fiber. Herewith, the number of generated 2nd Stokes photons at the output may even exceed the absorbed pump photons due to the lower attenuation of Stokes waves.</description><identifier>ISSN: 1094-4087</identifier><identifier>EISSN: 1094-4087</identifier><identifier>DOI: 10.1364/OE.22.024929</identifier><identifier>PMID: 25401526</identifier><language>eng</language><publisher>United States</publisher><subject>Electricity ; Feedback ; Lasers ; Optical Fibers ; Photons ; Spectrum Analysis, Raman</subject><ispartof>Optics express, 2014-10, Vol.22 (21), p.24929-24934</ispartof><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c329t-e1e22a181a7ba1909636c358d301c5a9b85afa03c8acb5358b6ce1b9043f53253</citedby><cites>FETCH-LOGICAL-c329t-e1e22a181a7ba1909636c358d301c5a9b85afa03c8acb5358b6ce1b9043f53253</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,860,27901,27902</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/25401526$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Babin, S A</creatorcontrib><creatorcontrib>Vatnik, I D</creatorcontrib><creatorcontrib>Laptev, A Yu</creatorcontrib><creatorcontrib>Bubnov, M M</creatorcontrib><creatorcontrib>Dianov, E M</creatorcontrib><title>High-efficiency cascaded Raman fiber laser with random distributed feedback</title><title>Optics express</title><addtitle>Opt Express</addtitle><description>Cascaded lasing provided by Raman gain (at 1115-nm pumping) and random distributed feedback (via Rayleigh backscattering) in a 1.65-km phosphosilicate fiber is studied. Output power for the second Stokes component (1398 nm) exceeds 5 W at pump power of 11 W. In contrast to conventional cascaded Raman laser with high-Q cavity for the intermediate first Stokes component, there is no cavity here and no cavity losses, correspondingly. Longitudinal power distribution is shown to be quite different also. As a result, the efficiency of pump to 2nd Stokes wave conversion is not influenced by the intermediate stage and depends only on the integral attenuation in the fiber. Herewith, the number of generated 2nd Stokes photons at the output may even exceed the absorbed pump photons due to the lower attenuation of Stokes waves.</description><subject>Electricity</subject><subject>Feedback</subject><subject>Lasers</subject><subject>Optical Fibers</subject><subject>Photons</subject><subject>Spectrum Analysis, Raman</subject><issn>1094-4087</issn><issn>1094-4087</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2014</creationdate><recordtype>article</recordtype><sourceid>EIF</sourceid><recordid>eNpNkE1Lw0AQhhdRbK3ePEuOHkzdj2ySPYpUKxYKoudldjNrV5O07iZI_70preJhZl6Yh_fwEHLJ6JSJPLtdzqacTynPFFdHZMyoytKMlsXxvzwiZzF-UMqyQhWnZMRlRpnk-Zg8z_37KkXnvPXY2m1iIVqosEpeoIE2cd5gSGqIw_723SoJ0FbrJql87II3fTeQDrEyYD_PyYmDOuLF4U7I28Ps9X6eLpaPT_d3i9QKrroUGXIOrGRQGGCKqlzkVsiyEpRZCcqUEhxQYUuwRg4Pk1tkRtFMOCm4FBNyve_dhPVXj7HTjY8W6xpaXPdRs5znw3C5Q2_2qA3rGAM6vQm-gbDVjOqdPr2cac71Xt-AXx2ae9Ng9Qf_-hI_uvRpmw</recordid><startdate>20141020</startdate><enddate>20141020</enddate><creator>Babin, S A</creator><creator>Vatnik, I D</creator><creator>Laptev, A Yu</creator><creator>Bubnov, M M</creator><creator>Dianov, E M</creator><scope>CGR</scope><scope>CUY</scope><scope>CVF</scope><scope>ECM</scope><scope>EIF</scope><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope></search><sort><creationdate>20141020</creationdate><title>High-efficiency cascaded Raman fiber laser with random distributed feedback</title><author>Babin, S A ; Vatnik, I D ; Laptev, A Yu ; Bubnov, M M ; Dianov, E M</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c329t-e1e22a181a7ba1909636c358d301c5a9b85afa03c8acb5358b6ce1b9043f53253</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2014</creationdate><topic>Electricity</topic><topic>Feedback</topic><topic>Lasers</topic><topic>Optical Fibers</topic><topic>Photons</topic><topic>Spectrum Analysis, Raman</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Babin, S A</creatorcontrib><creatorcontrib>Vatnik, I D</creatorcontrib><creatorcontrib>Laptev, A Yu</creatorcontrib><creatorcontrib>Bubnov, M M</creatorcontrib><creatorcontrib>Dianov, E M</creatorcontrib><collection>Medline</collection><collection>MEDLINE</collection><collection>MEDLINE (Ovid)</collection><collection>MEDLINE</collection><collection>MEDLINE</collection><collection>PubMed</collection><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><jtitle>Optics express</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Babin, S A</au><au>Vatnik, I D</au><au>Laptev, A Yu</au><au>Bubnov, M M</au><au>Dianov, E M</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>High-efficiency cascaded Raman fiber laser with random distributed feedback</atitle><jtitle>Optics express</jtitle><addtitle>Opt Express</addtitle><date>2014-10-20</date><risdate>2014</risdate><volume>22</volume><issue>21</issue><spage>24929</spage><epage>24934</epage><pages>24929-24934</pages><issn>1094-4087</issn><eissn>1094-4087</eissn><abstract>Cascaded lasing provided by Raman gain (at 1115-nm pumping) and random distributed feedback (via Rayleigh backscattering) in a 1.65-km phosphosilicate fiber is studied. Output power for the second Stokes component (1398 nm) exceeds 5 W at pump power of 11 W. In contrast to conventional cascaded Raman laser with high-Q cavity for the intermediate first Stokes component, there is no cavity here and no cavity losses, correspondingly. Longitudinal power distribution is shown to be quite different also. As a result, the efficiency of pump to 2nd Stokes wave conversion is not influenced by the intermediate stage and depends only on the integral attenuation in the fiber. Herewith, the number of generated 2nd Stokes photons at the output may even exceed the absorbed pump photons due to the lower attenuation of Stokes waves.</abstract><cop>United States</cop><pmid>25401526</pmid><doi>10.1364/OE.22.024929</doi><tpages>6</tpages><oa>free_for_read</oa></addata></record> |
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source | MEDLINE; DOAJ Directory of Open Access Journals; EZB-FREE-00999 freely available EZB journals; Alma/SFX Local Collection |
subjects | Electricity Feedback Lasers Optical Fibers Photons Spectrum Analysis, Raman |
title | High-efficiency cascaded Raman fiber laser with random distributed feedback |
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