Mode-locked lasers with nonlinear external cavities
A nonlinear element, when introduced into an external cavity, is shown to improve the mode locking of lasers. Mode locking is achieved by inducing coupling between the cavity modes, thus enabling more efficient transmission of phase information. We begin by discussing a phenomenological laser model...
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Veröffentlicht in: | J. Opt. Soc. Am. B: Opt. Phys.; (United States) 1988-03, Vol.5 (3), p.629-632 |
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container_title | J. Opt. Soc. Am. B: Opt. Phys.; (United States) |
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creator | BLOW, K. J WOOD, D |
description | A nonlinear element, when introduced into an external cavity, is shown to improve the mode locking of lasers. Mode locking is achieved by inducing coupling between the cavity modes, thus enabling more efficient transmission of phase information. We begin by discussing a phenomenological laser model for homogeneously broadened systems. The model laser is coupled to an external cavity and contains a nonlinear element. The returning pulse from this external cavity is then mixed with a circulating pulse in the laser at the output mirror. We have considered two nonlinear elements, a saturable absorber and a saturable amplifier. Although these elements have quite different pulse-shaping effects, they both cause considerable improvement in mode-locked performance. |
doi_str_mv | 10.1364/JOSAB.5.000629 |
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J ; WOOD, D</creator><creatorcontrib>BLOW, K. J ; WOOD, D ; British Telecom Research Laboratories, Martlesham Heath, Ipswich IP5 7RE, UK</creatorcontrib><description>A nonlinear element, when introduced into an external cavity, is shown to improve the mode locking of lasers. Mode locking is achieved by inducing coupling between the cavity modes, thus enabling more efficient transmission of phase information. We begin by discussing a phenomenological laser model for homogeneously broadened systems. The model laser is coupled to an external cavity and contains a nonlinear element. The returning pulse from this external cavity is then mixed with a circulating pulse in the laser at the output mirror. We have considered two nonlinear elements, a saturable absorber and a saturable amplifier. Although these elements have quite different pulse-shaping effects, they both cause considerable improvement in mode-locked performance.</description><identifier>ISSN: 0740-3224</identifier><identifier>EISSN: 1520-8540</identifier><identifier>DOI: 10.1364/JOSAB.5.000629</identifier><identifier>CODEN: JOBPDE</identifier><language>eng</language><publisher>Washington, DC: Optical Society of America</publisher><subject>420300 - Engineering- Lasers- (-1989) ; ENGINEERING ; Exact sciences and technology ; Fundamental areas of phenomenology (including applications) ; LASER CAVITIES ; LASER MIRRORS ; Laser optical systems: design and operation ; LASERS ; LINE BROADENING ; MATHEMATICAL MODELS ; MIRRORS ; MODE LOCKING ; Modulation, tuning, and mode locking ; NONLINEAR OPTICS ; OPTICS ; Physics ; PULSES ; QUASI PARTICLES ; SOLITONS</subject><ispartof>J. Opt. Soc. Am. B: Opt. 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J</creatorcontrib><creatorcontrib>WOOD, D</creatorcontrib><creatorcontrib>British Telecom Research Laboratories, Martlesham Heath, Ipswich IP5 7RE, UK</creatorcontrib><title>Mode-locked lasers with nonlinear external cavities</title><title>J. Opt. Soc. Am. B: Opt. Phys.; (United States)</title><description>A nonlinear element, when introduced into an external cavity, is shown to improve the mode locking of lasers. Mode locking is achieved by inducing coupling between the cavity modes, thus enabling more efficient transmission of phase information. We begin by discussing a phenomenological laser model for homogeneously broadened systems. The model laser is coupled to an external cavity and contains a nonlinear element. The returning pulse from this external cavity is then mixed with a circulating pulse in the laser at the output mirror. We have considered two nonlinear elements, a saturable absorber and a saturable amplifier. Although these elements have quite different pulse-shaping effects, they both cause considerable improvement in mode-locked performance.</description><subject>420300 - Engineering- Lasers- (-1989)</subject><subject>ENGINEERING</subject><subject>Exact sciences and technology</subject><subject>Fundamental areas of phenomenology (including applications)</subject><subject>LASER CAVITIES</subject><subject>LASER MIRRORS</subject><subject>Laser optical systems: design and operation</subject><subject>LASERS</subject><subject>LINE BROADENING</subject><subject>MATHEMATICAL MODELS</subject><subject>MIRRORS</subject><subject>MODE LOCKING</subject><subject>Modulation, tuning, and mode locking</subject><subject>NONLINEAR OPTICS</subject><subject>OPTICS</subject><subject>Physics</subject><subject>PULSES</subject><subject>QUASI PARTICLES</subject><subject>SOLITONS</subject><issn>0740-3224</issn><issn>1520-8540</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1988</creationdate><recordtype>article</recordtype><recordid>eNo9kElPwzAQRi0EEqVw5RwhrgnOeEuOpWJVUQ_A2ZpOHNUQksq2WP49gSBOc3nv0-gxdlryohRaXtyvHxeXhSo45xrqPTYrFfC8UpLvsxk3kucCQB6yoxhfRkZygBkTD0Pj8m6gV9dkHUYXYvbh0zbrh77zvcOQuc_kQo9dRvjuk3fxmB202EV38nfn7Pn66ml5m6_WN3fLxSonqFXKm40jAwCtdo5QcaRNZWpCwIZrwTe1rqjl0FRajo-CBtK6McrI1iCBUGLOzqbdISZvI_nkaEtD3ztKVkGlQJoRKiaIwhBjcK3dBf-G4cuW3P50sb9drLJTl1E4n4QdRsKuDdiTj_-WKQWYSolvQhNhtQ</recordid><startdate>19880301</startdate><enddate>19880301</enddate><creator>BLOW, K. J</creator><creator>WOOD, D</creator><general>Optical Society of America</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>OTOTI</scope></search><sort><creationdate>19880301</creationdate><title>Mode-locked lasers with nonlinear external cavities</title><author>BLOW, K. J ; WOOD, D</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c295t-dbec7222f6eeca50acb879ca2ad0630b968cf02d864520262c66d7574f7ac2353</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1988</creationdate><topic>420300 - Engineering- Lasers- (-1989)</topic><topic>ENGINEERING</topic><topic>Exact sciences and technology</topic><topic>Fundamental areas of phenomenology (including applications)</topic><topic>LASER CAVITIES</topic><topic>LASER MIRRORS</topic><topic>Laser optical systems: design and operation</topic><topic>LASERS</topic><topic>LINE BROADENING</topic><topic>MATHEMATICAL MODELS</topic><topic>MIRRORS</topic><topic>MODE LOCKING</topic><topic>Modulation, tuning, and mode locking</topic><topic>NONLINEAR OPTICS</topic><topic>OPTICS</topic><topic>Physics</topic><topic>PULSES</topic><topic>QUASI PARTICLES</topic><topic>SOLITONS</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>BLOW, K. J</creatorcontrib><creatorcontrib>WOOD, D</creatorcontrib><creatorcontrib>British Telecom Research Laboratories, Martlesham Heath, Ipswich IP5 7RE, UK</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>OSTI.GOV</collection><jtitle>J. Opt. Soc. Am. B: Opt. Phys.; (United States)</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>BLOW, K. J</au><au>WOOD, D</au><aucorp>British Telecom Research Laboratories, Martlesham Heath, Ipswich IP5 7RE, UK</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Mode-locked lasers with nonlinear external cavities</atitle><jtitle>J. Opt. Soc. Am. B: Opt. Phys.; (United States)</jtitle><date>1988-03-01</date><risdate>1988</risdate><volume>5</volume><issue>3</issue><spage>629</spage><epage>632</epage><pages>629-632</pages><issn>0740-3224</issn><eissn>1520-8540</eissn><coden>JOBPDE</coden><abstract>A nonlinear element, when introduced into an external cavity, is shown to improve the mode locking of lasers. Mode locking is achieved by inducing coupling between the cavity modes, thus enabling more efficient transmission of phase information. We begin by discussing a phenomenological laser model for homogeneously broadened systems. The model laser is coupled to an external cavity and contains a nonlinear element. The returning pulse from this external cavity is then mixed with a circulating pulse in the laser at the output mirror. We have considered two nonlinear elements, a saturable absorber and a saturable amplifier. Although these elements have quite different pulse-shaping effects, they both cause considerable improvement in mode-locked performance.</abstract><cop>Washington, DC</cop><pub>Optical Society of America</pub><doi>10.1364/JOSAB.5.000629</doi><tpages>4</tpages></addata></record> |
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source | OSA_美国光学学会数据库1 |
subjects | 420300 - Engineering- Lasers- (-1989) ENGINEERING Exact sciences and technology Fundamental areas of phenomenology (including applications) LASER CAVITIES LASER MIRRORS Laser optical systems: design and operation LASERS LINE BROADENING MATHEMATICAL MODELS MIRRORS MODE LOCKING Modulation, tuning, and mode locking NONLINEAR OPTICS OPTICS Physics PULSES QUASI PARTICLES SOLITONS |
title | Mode-locked lasers with nonlinear external cavities |
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