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Power and energy scaling of an acousto-optically Q switched Raman deep-red laser
An efficient high-power nanosecond pulsed deep-red laser at 745 nm is produced by intracavity frequency-doubling an acousto-optically Q switched Nd:YLF/KGW Raman laser using a lithium triborate (LBO) crystal. The critically phase-matched type-I LBO crystal with an optimized length of 25 mm is adopte...
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Published in: | Optics letters 2022-09, Vol.47 (18), p.4754-4757 |
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container_title | Optics letters |
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creator | Zhao, Hui Jiang, Cong Li, Keyin Zhou, Haiqiong Zhu, Siqi Yin, Hao Li, Zhen Chen, Zhenqiang Dai, Shibo |
description | An efficient high-power nanosecond pulsed deep-red laser at 745 nm is produced by intracavity frequency-doubling an acousto-optically Q switched Nd:YLF/KGW Raman laser using a lithium triborate (LBO) crystal. The critically phase-matched type-I LBO crystal with an optimized length of 25 mm is adopted to enable efficient second-harmonic generation and to suppress unwanted cascaded Stokes fields. Under a repetition rate of 4 kHz, the maximum average output power of 4.1 W is obtained with the launched pump power of 50 W, resulting in an overall optical power conversion efficiency of 8.2%. The average beam quality factor is determined to be M 2 = 1.46. The pulse energy is scaled up to 3.3 mJ at the repetition rate of 1 kHz, corresponding to a pulse width of 4.2 ns and a peak power of up to 0.8 MW. Moreover, we theoretically investigate the dependence of the conversion efficiency on the walk-off angle as well as the fundamental and first-Stokes losses, which will guide further optimization of experimental devices. |
doi_str_mv | 10.1364/OL.468820 |
format | article |
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The critically phase-matched type-I LBO crystal with an optimized length of 25 mm is adopted to enable efficient second-harmonic generation and to suppress unwanted cascaded Stokes fields. Under a repetition rate of 4 kHz, the maximum average output power of 4.1 W is obtained with the launched pump power of 50 W, resulting in an overall optical power conversion efficiency of 8.2%. The average beam quality factor is determined to be M 2 = 1.46. The pulse energy is scaled up to 3.3 mJ at the repetition rate of 1 kHz, corresponding to a pulse width of 4.2 ns and a peak power of up to 0.8 MW. 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The critically phase-matched type-I LBO crystal with an optimized length of 25 mm is adopted to enable efficient second-harmonic generation and to suppress unwanted cascaded Stokes fields. Under a repetition rate of 4 kHz, the maximum average output power of 4.1 W is obtained with the launched pump power of 50 W, resulting in an overall optical power conversion efficiency of 8.2%. The average beam quality factor is determined to be M 2 = 1.46. The pulse energy is scaled up to 3.3 mJ at the repetition rate of 1 kHz, corresponding to a pulse width of 4.2 ns and a peak power of up to 0.8 MW. Moreover, we theoretically investigate the dependence of the conversion efficiency on the walk-off angle as well as the fundamental and first-Stokes losses, which will guide further optimization of experimental devices.</description><subject>Energy conversion efficiency</subject><subject>Lasers</subject><subject>Lithium</subject><subject>Nanosecond pulses</subject><subject>Neodymium lasers</subject><subject>Optimization</subject><subject>Phase matching</subject><subject>Pulse duration</subject><subject>Raman lasers</subject><subject>Repetition</subject><subject>Second harmonic generation</subject><issn>0146-9592</issn><issn>1539-4794</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><recordid>eNpdkE1LAzEQhoMoWKsH_0HAix5W87nZHKX4BQutoueQJrN1y3azJltK_70p9eRpmJmH4Z0HoWtK7ikvxcO8vhdlVTFygiZUcl0IpcUpmhAqykJLzc7RRUprQkipOJ-gxSLsIGLbeww9xNUeJ2e7tl_h0OQpti5s0xiKMIxtXnR7_I7Trh3dN3j8YTcZ8QBDEXPb2QTxEp01tktw9Ven6Ov56XP2WtTzl7fZY104pslYCGicYgy8dq4SFWdLVipnKWGcaSe4pNJLrz3VQoJfEiuBLBkj1FqglbZ8im6Pd4cYfraQRrNpk4Ousz3kyIap_LFUklUZvfmHrsM29jndgZKiUllYpu6OlIshpQiNGWK7sXFvKDEHt2Zem6Nb_guVhWpB</recordid><startdate>20220915</startdate><enddate>20220915</enddate><creator>Zhao, Hui</creator><creator>Jiang, Cong</creator><creator>Li, Keyin</creator><creator>Zhou, Haiqiong</creator><creator>Zhu, Siqi</creator><creator>Yin, Hao</creator><creator>Li, Zhen</creator><creator>Chen, Zhenqiang</creator><creator>Dai, Shibo</creator><general>Optical Society of America</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>7U5</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><scope>7X8</scope><orcidid>https://orcid.org/0000-0001-8880-3171</orcidid><orcidid>https://orcid.org/0000-0003-4441-710X</orcidid></search><sort><creationdate>20220915</creationdate><title>Power and energy scaling of an acousto-optically Q switched Raman deep-red laser</title><author>Zhao, Hui ; Jiang, Cong ; Li, Keyin ; Zhou, Haiqiong ; Zhu, Siqi ; Yin, Hao ; Li, Zhen ; Chen, Zhenqiang ; Dai, Shibo</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c290t-4efc722ed9cc84832b267ca102329c43515d5d9d1945edb0a5e0b2201aae189a3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><topic>Energy conversion efficiency</topic><topic>Lasers</topic><topic>Lithium</topic><topic>Nanosecond pulses</topic><topic>Neodymium lasers</topic><topic>Optimization</topic><topic>Phase matching</topic><topic>Pulse duration</topic><topic>Raman lasers</topic><topic>Repetition</topic><topic>Second harmonic generation</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Zhao, Hui</creatorcontrib><creatorcontrib>Jiang, Cong</creatorcontrib><creatorcontrib>Li, Keyin</creatorcontrib><creatorcontrib>Zhou, Haiqiong</creatorcontrib><creatorcontrib>Zhu, Siqi</creatorcontrib><creatorcontrib>Yin, Hao</creatorcontrib><creatorcontrib>Li, Zhen</creatorcontrib><creatorcontrib>Chen, Zhenqiang</creatorcontrib><creatorcontrib>Dai, Shibo</creatorcontrib><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>Optics letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Zhao, Hui</au><au>Jiang, Cong</au><au>Li, Keyin</au><au>Zhou, Haiqiong</au><au>Zhu, Siqi</au><au>Yin, Hao</au><au>Li, Zhen</au><au>Chen, Zhenqiang</au><au>Dai, Shibo</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Power and energy scaling of an acousto-optically Q switched Raman deep-red laser</atitle><jtitle>Optics letters</jtitle><date>2022-09-15</date><risdate>2022</risdate><volume>47</volume><issue>18</issue><spage>4754</spage><epage>4757</epage><pages>4754-4757</pages><issn>0146-9592</issn><eissn>1539-4794</eissn><abstract>An efficient high-power nanosecond pulsed deep-red laser at 745 nm is produced by intracavity frequency-doubling an acousto-optically Q switched Nd:YLF/KGW Raman laser using a lithium triborate (LBO) crystal. The critically phase-matched type-I LBO crystal with an optimized length of 25 mm is adopted to enable efficient second-harmonic generation and to suppress unwanted cascaded Stokes fields. Under a repetition rate of 4 kHz, the maximum average output power of 4.1 W is obtained with the launched pump power of 50 W, resulting in an overall optical power conversion efficiency of 8.2%. The average beam quality factor is determined to be M 2 = 1.46. The pulse energy is scaled up to 3.3 mJ at the repetition rate of 1 kHz, corresponding to a pulse width of 4.2 ns and a peak power of up to 0.8 MW. Moreover, we theoretically investigate the dependence of the conversion efficiency on the walk-off angle as well as the fundamental and first-Stokes losses, which will guide further optimization of experimental devices.</abstract><cop>Washington</cop><pub>Optical Society of America</pub><doi>10.1364/OL.468820</doi><tpages>4</tpages><orcidid>https://orcid.org/0000-0001-8880-3171</orcidid><orcidid>https://orcid.org/0000-0003-4441-710X</orcidid></addata></record> |
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source | Optica Publishing Group Journals |
subjects | Energy conversion efficiency Lasers Lithium Nanosecond pulses Neodymium lasers Optimization Phase matching Pulse duration Raman lasers Repetition Second harmonic generation |
title | Power and energy scaling of an acousto-optically Q switched Raman deep-red laser |
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