Optical pulse propagation in a heavily saturated laser amplifier: laser parameter analysis
An optical pulse propagating through a partially homogeneously broadened laser amplifier is analyzed theoretically and experimentally in the heavily saturated region as well as in the linear and slightly saturated regions. In the heavily saturated region pulse shortening takes place, whereas pulse l...
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Veröffentlicht in: | J. Opt. Soc. Am. B: Opt. Phys.; (United States) 1986-02, Vol.3 (2), p.183 |
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container_issue | 2 |
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container_title | J. Opt. Soc. Am. B: Opt. Phys.; (United States) |
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creator | Takahashi, Nobuaki Sato, Heihachi Gamo, Hideya |
description | An optical pulse propagating through a partially homogeneously broadened laser amplifier is analyzed theoretically and experimentally in the heavily saturated region as well as in the linear and slightly saturated regions. In the heavily saturated region pulse shortening takes place, whereas pulse lengthening is observed in the linear or slightly saturated region. Emphasis is especially placed on a laser parameter analysis by using the formulas for the pulse-peak irradiance, the pulse duration, and the pulse-delay time. A new method to determine the saturation irradiance I/sub s/ of the laser medium is proposed based on the condition for maximizing the pulse-delay time. By demonstrating the above method and the methods in the linear region to the 3.5-..mu..m line of a He-Xe laser, we have obtained the following laser parameters: The saturation irradiance I/sub s/ is 6.34 ..mu..W/mm/sup 2/, the gain parameter G is 0.063 cm/sup -1/, the Lorentzian linewidth ..delta nu../sub L/ is 11.7 MHz, and the Doppler linewidth ..delta nu../sub D/ is 104 MHz. |
doi_str_mv | 10.1364/JOSAB.3.000183 |
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In the heavily saturated region pulse shortening takes place, whereas pulse lengthening is observed in the linear or slightly saturated region. Emphasis is especially placed on a laser parameter analysis by using the formulas for the pulse-peak irradiance, the pulse duration, and the pulse-delay time. A new method to determine the saturation irradiance I/sub s/ of the laser medium is proposed based on the condition for maximizing the pulse-delay time. By demonstrating the above method and the methods in the linear region to the 3.5-..mu..m line of a He-Xe laser, we have obtained the following laser parameters: The saturation irradiance I/sub s/ is 6.34 ..mu..W/mm/sup 2/, the gain parameter G is 0.063 cm/sup -1/, the Lorentzian linewidth ..delta nu../sub L/ is 11.7 MHz, and the Doppler linewidth ..delta nu../sub D/ is 104 MHz.</description><identifier>ISSN: 0740-3224</identifier><identifier>EISSN: 1520-8540</identifier><identifier>DOI: 10.1364/JOSAB.3.000183</identifier><language>eng</language><publisher>United States</publisher><subject>420300 - Engineering- Lasers- (-1989) ; AMPLIFICATION ; ELECTROMAGNETIC RADIATION ; ENGINEERING ; GAIN ; GAS LASERS ; LASER RADIATION ; LASERS ; LINE BROADENING ; LINE WIDTHS ; NONLINEAR OPTICS ; OPTICS ; PULSES ; RADIATIONS ; SATURATION ; TIME DELAY</subject><ispartof>J. Opt. Soc. Am. B: Opt. 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Opt. Soc. Am. B: Opt. Phys.; (United States)</title><description>An optical pulse propagating through a partially homogeneously broadened laser amplifier is analyzed theoretically and experimentally in the heavily saturated region as well as in the linear and slightly saturated regions. In the heavily saturated region pulse shortening takes place, whereas pulse lengthening is observed in the linear or slightly saturated region. Emphasis is especially placed on a laser parameter analysis by using the formulas for the pulse-peak irradiance, the pulse duration, and the pulse-delay time. A new method to determine the saturation irradiance I/sub s/ of the laser medium is proposed based on the condition for maximizing the pulse-delay time. By demonstrating the above method and the methods in the linear region to the 3.5-..mu..m line of a He-Xe laser, we have obtained the following laser parameters: The saturation irradiance I/sub s/ is 6.34 ..mu..W/mm/sup 2/, the gain parameter G is 0.063 cm/sup -1/, the Lorentzian linewidth ..delta nu../sub L/ is 11.7 MHz, and the Doppler linewidth ..delta nu../sub D/ is 104 MHz.</description><subject>420300 - Engineering- Lasers- (-1989)</subject><subject>AMPLIFICATION</subject><subject>ELECTROMAGNETIC RADIATION</subject><subject>ENGINEERING</subject><subject>GAIN</subject><subject>GAS LASERS</subject><subject>LASER RADIATION</subject><subject>LASERS</subject><subject>LINE BROADENING</subject><subject>LINE WIDTHS</subject><subject>NONLINEAR OPTICS</subject><subject>OPTICS</subject><subject>PULSES</subject><subject>RADIATIONS</subject><subject>SATURATION</subject><subject>TIME DELAY</subject><issn>0740-3224</issn><issn>1520-8540</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1986</creationdate><recordtype>article</recordtype><recordid>eNotkDtPwzAYRS0EEqWwMlvsCX7FsdlKxVOVOgALi_Xh2NQoTSzbReq_p6WdrnTv0R0OQteU1JRLcfu6fJvd17wmhFDFT9CENoxUqhHkFE1IK0jFGRPn6CLnnx0jCGMT9LmMJVjocdz02eGYxgjfUMI44DBgwCsHv6Hf4gxlk6C4DveQXcKwjn3wwaW7YxEhwdqV_TRAv80hX6IzD7vTq2NO0cfjw_v8uVosn17ms0VlmZSlYkRpC7q1SjglNOssEAvUdrrxkui2o8JLAAUaLANoOLNfXknPJGUtaz2fopvD75hLMNmG4uzKjsPgbDGNbpiWfAfVB8imMefkvIkprCFtDSVmr8_86zPcHPTxPy5VZDY</recordid><startdate>19860201</startdate><enddate>19860201</enddate><creator>Takahashi, Nobuaki</creator><creator>Sato, Heihachi</creator><creator>Gamo, Hideya</creator><scope>AAYXX</scope><scope>CITATION</scope><scope>OTOTI</scope></search><sort><creationdate>19860201</creationdate><title>Optical pulse propagation in a heavily saturated laser amplifier: laser parameter analysis</title><author>Takahashi, Nobuaki ; Sato, Heihachi ; Gamo, Hideya</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c266t-2089ca97c84e8492dca0ca1cd95f6097d14f6aa8a9ac2aa532cbf86f2612727f3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1986</creationdate><topic>420300 - Engineering- Lasers- (-1989)</topic><topic>AMPLIFICATION</topic><topic>ELECTROMAGNETIC RADIATION</topic><topic>ENGINEERING</topic><topic>GAIN</topic><topic>GAS LASERS</topic><topic>LASER RADIATION</topic><topic>LASERS</topic><topic>LINE BROADENING</topic><topic>LINE WIDTHS</topic><topic>NONLINEAR OPTICS</topic><topic>OPTICS</topic><topic>PULSES</topic><topic>RADIATIONS</topic><topic>SATURATION</topic><topic>TIME DELAY</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Takahashi, Nobuaki</creatorcontrib><creatorcontrib>Sato, Heihachi</creatorcontrib><creatorcontrib>Gamo, Hideya</creatorcontrib><creatorcontrib>Department of Applied Physics, The National Defense Academy, Yokosuka 239, Japan</creatorcontrib><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>Takahashi, Nobuaki</au><au>Sato, Heihachi</au><au>Gamo, Hideya</au><aucorp>Department of Applied Physics, The National Defense Academy, Yokosuka 239, Japan</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Optical pulse propagation in a heavily saturated laser amplifier: laser parameter analysis</atitle><jtitle>J. Opt. Soc. Am. B: Opt. Phys.; (United States)</jtitle><date>1986-02-01</date><risdate>1986</risdate><volume>3</volume><issue>2</issue><spage>183</spage><pages>183-</pages><issn>0740-3224</issn><eissn>1520-8540</eissn><abstract>An optical pulse propagating through a partially homogeneously broadened laser amplifier is analyzed theoretically and experimentally in the heavily saturated region as well as in the linear and slightly saturated regions. In the heavily saturated region pulse shortening takes place, whereas pulse lengthening is observed in the linear or slightly saturated region. Emphasis is especially placed on a laser parameter analysis by using the formulas for the pulse-peak irradiance, the pulse duration, and the pulse-delay time. A new method to determine the saturation irradiance I/sub s/ of the laser medium is proposed based on the condition for maximizing the pulse-delay time. By demonstrating the above method and the methods in the linear region to the 3.5-..mu..m line of a He-Xe laser, we have obtained the following laser parameters: The saturation irradiance I/sub s/ is 6.34 ..mu..W/mm/sup 2/, the gain parameter G is 0.063 cm/sup -1/, the Lorentzian linewidth ..delta nu../sub L/ is 11.7 MHz, and the Doppler linewidth ..delta nu../sub D/ is 104 MHz.</abstract><cop>United States</cop><doi>10.1364/JOSAB.3.000183</doi></addata></record> |
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source | Optica Publishing Group Journals |
subjects | 420300 - Engineering- Lasers- (-1989) AMPLIFICATION ELECTROMAGNETIC RADIATION ENGINEERING GAIN GAS LASERS LASER RADIATION LASERS LINE BROADENING LINE WIDTHS NONLINEAR OPTICS OPTICS PULSES RADIATIONS SATURATION TIME DELAY |
title | Optical pulse propagation in a heavily saturated laser amplifier: laser parameter analysis |
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