Dual synchronously pumped and synchronously amplified dye lasers
A dual synchronously pumped and synchronously amplified dye-laser system has been constructed and tested. A regenerative amplifier is used as the amplification source. An amplification factor of 6 x 10/sup 4/ is reached in each of two synchronously pumped dye-laser output beams. Thus, the total inci...
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Veröffentlicht in: | Opt. Lett.; (United States) 1988-07, Vol.13 (7), p.577-579 |
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container_title | Opt. Lett.; (United States) |
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creator | JUHASZ, T KUHL, J BRON, W. E |
description | A dual synchronously pumped and synchronously amplified dye-laser system has been constructed and tested. A regenerative amplifier is used as the amplification source. An amplification factor of 6 x 10/sup 4/ is reached in each of two synchronously pumped dye-laser output beams. Thus, the total incident beam intensity available for two-photon nonlinear excitations reaches an amplification of the order of 4 x 10/sup 9/ times that available from unamplified laser beams. |
doi_str_mv | 10.1364/OL.13.000577 |
format | Article |
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Thus, the total incident beam intensity available for two-photon nonlinear excitations reaches an amplification of the order of 4 x 10/sup 9/ times that available from unamplified laser beams.</description><subject>420300 - Engineering- Lasers- (-1989)</subject><subject>DESIGN</subject><subject>DYE LASERS</subject><subject>ENGINEERING</subject><subject>Exact sciences and technology</subject><subject>Fundamental areas of phenomenology (including applications)</subject><subject>LASER SPECTROSCOPY</subject><subject>LASERS</subject><subject>LIQUID LASERS</subject><subject>Optics</subject><subject>Physics</subject><subject>PUMPING</subject><subject>RADIATION SOURCES</subject><subject>RAMAN SPECTROSCOPY</subject><subject>SPECTROSCOPY</subject><subject>TESTING</subject><issn>0146-9592</issn><issn>1539-4794</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1988</creationdate><recordtype>article</recordtype><recordid>eNpd0EtLxDAUBeAgio6jO9dSRHBjx6RJk2anjE8ozEbXIb1JmUpfJu2i_95Ii4Krs7gfB-5B6ILgDaGc3e3ykBuMcSrEAVqRlMqYCckO0QoTxmOZyuQEnXr_GQwXlB6jEyIFSyWXK3T_OOo68lMLe9e13ejrKerHprcm0q35d9BNX1dlFW5mslGtvXX-DB2Vuvb2fMk1-nh-et--xvnu5W37kMdAGR9iWRCpAVhCCyNLU3ArEgKmlAKAcqtLAGI4oTjLpJYUhMkIplmBSWnTDBu6Rldzb-eHSnmoBgt76NrWwqAECU9iGdDNjHrXfY3WD6qpPNi61q0NLyhBGWYJYzjI21mC67x3tlS9qxrtJkWw-tlV7fKQat418MuleCwaa_7wMmQA1wvQHnRdOt1C5X-dCC1ScPoNhTh_1g</recordid><startdate>19880701</startdate><enddate>19880701</enddate><creator>JUHASZ, T</creator><creator>KUHL, J</creator><creator>BRON, W. 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E</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c346t-9b19acc423bd9fdb6e721cdf97cc36eafcc1d6130889a93c7d81038b01fe580d3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1988</creationdate><topic>420300 - Engineering- Lasers- (-1989)</topic><topic>DESIGN</topic><topic>DYE LASERS</topic><topic>ENGINEERING</topic><topic>Exact sciences and technology</topic><topic>Fundamental areas of phenomenology (including applications)</topic><topic>LASER SPECTROSCOPY</topic><topic>LASERS</topic><topic>LIQUID LASERS</topic><topic>Optics</topic><topic>Physics</topic><topic>PUMPING</topic><topic>RADIATION SOURCES</topic><topic>RAMAN SPECTROSCOPY</topic><topic>SPECTROSCOPY</topic><topic>TESTING</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>JUHASZ, T</creatorcontrib><creatorcontrib>KUHL, J</creatorcontrib><creatorcontrib>BRON, W. 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Lett.; (United States)</jtitle><addtitle>Opt Lett</addtitle><date>1988-07-01</date><risdate>1988</risdate><volume>13</volume><issue>7</issue><spage>577</spage><epage>579</epage><pages>577-579</pages><issn>0146-9592</issn><eissn>1539-4794</eissn><coden>OPLEDP</coden><abstract>A dual synchronously pumped and synchronously amplified dye-laser system has been constructed and tested. A regenerative amplifier is used as the amplification source. An amplification factor of 6 x 10/sup 4/ is reached in each of two synchronously pumped dye-laser output beams. Thus, the total incident beam intensity available for two-photon nonlinear excitations reaches an amplification of the order of 4 x 10/sup 9/ times that available from unamplified laser beams.</abstract><cop>Washington, DC</cop><pub>Optical Society of America</pub><pmid>19745969</pmid><doi>10.1364/OL.13.000577</doi><tpages>3</tpages></addata></record> |
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subjects | 420300 - Engineering- Lasers- (-1989) DESIGN DYE LASERS ENGINEERING Exact sciences and technology Fundamental areas of phenomenology (including applications) LASER SPECTROSCOPY LASERS LIQUID LASERS Optics Physics PUMPING RADIATION SOURCES RAMAN SPECTROSCOPY SPECTROSCOPY TESTING |
title | Dual synchronously pumped and synchronously amplified dye lasers |
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