High-spectral-flatness mid-infrared supercontinuum generated from a Tm-doped fiber amplifier
Broadband mid-infrared supercontinuum pulses were generated directly from a short piece of active fiber in a single-mode Tm-doped fiber amplifier. The broadband mid-infrared pulses have an extremely high spectral flatness with ~600 nm FWHM bandwidth (from 1.9 μm to 2.5 μm), >15 kW peak power, and...
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Veröffentlicht in: | Applied optics (2004) 2012-03, Vol.51 (7), p.834-840 |
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creator | Geng, Jihong Wang, Qing Jiang, Shibin |
description | Broadband mid-infrared supercontinuum pulses were generated directly from a short piece of active fiber in a single-mode Tm-doped fiber amplifier. The broadband mid-infrared pulses have an extremely high spectral flatness with ~600 nm FWHM bandwidth (from 1.9 μm to 2.5 μm), >15 kW peak power, and >20 GW/cm(2) laser peak intensity. This new approach exhibits a significantly different physical mechanism from other supercontinuum generation demonstrations in the literature, in which usually a piece of passive fiber was used for nonlinear spectral broadening. The physical mechanism for the broadband mid-infrared supercontinuum generation in this approach has been attributed to a combined effect of two superradiative processes of Tm(3+) ions (i.e., the (3)F(4)-(3)H(6) transition covering the 1.8~2.1 μm spectral region and the (3)H(4)-(3)H(5) transition covering the 2.2~2.5 μm spectral region), and also nonlinear optical processes as well in the Tm-doped gain fiber. The spectra of the mid-infrared supercontinuum pulses were further broadened in a 2 m chalcogenide fiber with 20 dB bandwidth ~1100 nm and a 3 m fluoride fiber with 20 dB bandwidth ~2600 nm. |
doi_str_mv | 10.1364/AO.51.000834 |
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The broadband mid-infrared pulses have an extremely high spectral flatness with ~600 nm FWHM bandwidth (from 1.9 μm to 2.5 μm), >15 kW peak power, and >20 GW/cm(2) laser peak intensity. This new approach exhibits a significantly different physical mechanism from other supercontinuum generation demonstrations in the literature, in which usually a piece of passive fiber was used for nonlinear spectral broadening. The physical mechanism for the broadband mid-infrared supercontinuum generation in this approach has been attributed to a combined effect of two superradiative processes of Tm(3+) ions (i.e., the (3)F(4)-(3)H(6) transition covering the 1.8~2.1 μm spectral region and the (3)H(4)-(3)H(5) transition covering the 2.2~2.5 μm spectral region), and also nonlinear optical processes as well in the Tm-doped gain fiber. 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The broadband mid-infrared pulses have an extremely high spectral flatness with ~600 nm FWHM bandwidth (from 1.9 μm to 2.5 μm), >15 kW peak power, and >20 GW/cm(2) laser peak intensity. This new approach exhibits a significantly different physical mechanism from other supercontinuum generation demonstrations in the literature, in which usually a piece of passive fiber was used for nonlinear spectral broadening. The physical mechanism for the broadband mid-infrared supercontinuum generation in this approach has been attributed to a combined effect of two superradiative processes of Tm(3+) ions (i.e., the (3)F(4)-(3)H(6) transition covering the 1.8~2.1 μm spectral region and the (3)H(4)-(3)H(5) transition covering the 2.2~2.5 μm spectral region), and also nonlinear optical processes as well in the Tm-doped gain fiber. The spectra of the mid-infrared supercontinuum pulses were further broadened in a 2 m chalcogenide fiber with 20 dB bandwidth ~1100 nm and a 3 m fluoride fiber with 20 dB bandwidth ~2600 nm.</description><subject>Amplifiers</subject><subject>Bandwidth</subject><subject>Broadband</subject><subject>Covering</subject><subject>Fibers</subject><subject>Noise levels</subject><subject>Nonlinearity</subject><subject>Spectra</subject><issn>1559-128X</issn><issn>2155-3165</issn><issn>1539-4522</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2012</creationdate><recordtype>article</recordtype><recordid>eNp90M9LwzAUB_AgipvTm2fpTQ9m5meTHMdQJwx2meBBKGmTzEjT1qQ9-N_bsenR03uP9-E9-AJwjdEc05w9LDZzjucIIUnZCZgSzDmkOOenYDq2CmIi3ybgIqVPhChnSpyDCSEMIynpFLyv_O4Dps5WfdQ1dLXuG5tSFryBvnFRR2uyNHQ2Vm3T-2YYQrazjY26HxcutiHT2TZA03b72Zc2Zjp0tXfexktw5nSd7NWxzsDr0-N2uYLrzfPLcrGGFZWqhwYLiYwipTY5qoTVjitOBTaMYyqEU9Row8tyNIaYSgqKWGkYw4zgXCNGZ-D2cLeL7ddgU18Enypb17qx7ZAKRYSSIqdilHf_SowIUUio8fEM3B9oFduUonVFF33Q8XtExT75YrEpOC4OyY_85nh5KIM1f_g3avoDOLV-Qw</recordid><startdate>20120301</startdate><enddate>20120301</enddate><creator>Geng, Jihong</creator><creator>Wang, Qing</creator><creator>Jiang, Shibin</creator><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>7U5</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><scope>7X8</scope></search><sort><creationdate>20120301</creationdate><title>High-spectral-flatness mid-infrared supercontinuum generated from a Tm-doped fiber amplifier</title><author>Geng, Jihong ; Wang, Qing ; Jiang, Shibin</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c389t-d1780d92bad60c7eaf595371d451377f93dad5bb0d9d2dc87304bd4414216a043</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2012</creationdate><topic>Amplifiers</topic><topic>Bandwidth</topic><topic>Broadband</topic><topic>Covering</topic><topic>Fibers</topic><topic>Noise levels</topic><topic>Nonlinearity</topic><topic>Spectra</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Geng, Jihong</creatorcontrib><creatorcontrib>Wang, Qing</creatorcontrib><creatorcontrib>Jiang, Shibin</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>Electronics & Communications Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>MEDLINE - Academic</collection><jtitle>Applied optics (2004)</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Geng, Jihong</au><au>Wang, Qing</au><au>Jiang, Shibin</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>High-spectral-flatness mid-infrared supercontinuum generated from a Tm-doped fiber amplifier</atitle><jtitle>Applied optics (2004)</jtitle><addtitle>Appl Opt</addtitle><date>2012-03-01</date><risdate>2012</risdate><volume>51</volume><issue>7</issue><spage>834</spage><epage>840</epage><pages>834-840</pages><issn>1559-128X</issn><eissn>2155-3165</eissn><eissn>1539-4522</eissn><abstract>Broadband mid-infrared supercontinuum pulses were generated directly from a short piece of active fiber in a single-mode Tm-doped fiber amplifier. The broadband mid-infrared pulses have an extremely high spectral flatness with ~600 nm FWHM bandwidth (from 1.9 μm to 2.5 μm), >15 kW peak power, and >20 GW/cm(2) laser peak intensity. This new approach exhibits a significantly different physical mechanism from other supercontinuum generation demonstrations in the literature, in which usually a piece of passive fiber was used for nonlinear spectral broadening. The physical mechanism for the broadband mid-infrared supercontinuum generation in this approach has been attributed to a combined effect of two superradiative processes of Tm(3+) ions (i.e., the (3)F(4)-(3)H(6) transition covering the 1.8~2.1 μm spectral region and the (3)H(4)-(3)H(5) transition covering the 2.2~2.5 μm spectral region), and also nonlinear optical processes as well in the Tm-doped gain fiber. The spectra of the mid-infrared supercontinuum pulses were further broadened in a 2 m chalcogenide fiber with 20 dB bandwidth ~1100 nm and a 3 m fluoride fiber with 20 dB bandwidth ~2600 nm.</abstract><cop>United States</cop><pmid>22410883</pmid><doi>10.1364/AO.51.000834</doi><tpages>7</tpages></addata></record> |
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source | OSA_美国光学学会数据库1; Alma/SFX Local Collection |
subjects | Amplifiers Bandwidth Broadband Covering Fibers Noise levels Nonlinearity Spectra |
title | High-spectral-flatness mid-infrared supercontinuum generated from a Tm-doped fiber amplifier |
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