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Broadband BiOCl Nonlinear Saturable Absorber for Watt‐Level Passively Q‐Switched Yb:LuAG Single Crystal Fiber Laser
The development of nonlinear optical (NLO) devices is limited to the mid‐infrared range due to the lack of broadband NLO response. As an indirect band gap semiconductor, BiOCl has a band gap of ≈3.3 eV. The special anisotropic lamellar structure makes it exhibit excellent electrical and optical prop...
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Published in: | Advanced optical materials 2022-11, Vol.10 (22), p.n/a |
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creator | Ma, Xiaofei Wang, Ci Zhang, Jian Wang, Tao Wang, Anye Wang, Siyuan Jia, Zhitai Zhang, Baitao He, Jingliang Smaalen, Sander Tao, Xutang |
description | The development of nonlinear optical (NLO) devices is limited to the mid‐infrared range due to the lack of broadband NLO response. As an indirect band gap semiconductor, BiOCl has a band gap of ≈3.3 eV. The special anisotropic lamellar structure makes it exhibit excellent electrical and optical properties; however, its NLO saturable absorption effect is rarely reported. In this study, the NLO response, optical properties, and applications of BiOCl crystals grown by chemical vapor phase transport method are studied in detail. The transmission spectrum indicates the BiOCl crystal has a broadband transparent region (0.4–11 µm). The saturable absorption of BiOCl is characterized by the Z‐scan method with 532 and 1030 nm pulsed lasers. With BiOCl as the saturable absorber (SA), watt‐level passively Q‐switched pulsed laser based on Yb:LuAG single crystal fiber (SCF) is realized. This is the first report of BiOCl as SA for passively Q‐switched all‐solid‐state pulsed laser, and the obtained average power is the highest value of passively Q‐switched SCF pulsed lasers reported so far. The high transmittance, high laser damage threshold, wideband NLO response, and environmental stability of BiOCl indicate that BiOCl crystal is a potential candidate for NLO applications.
The nonlinear optical properties of BiOCl crystal, which has a broadband (visible–infrared) nonlinear saturable absorption and a high laser damage threshold to be a saturable absorber of broadband high‐power laser, are studied. Combining BiOCl with single‐crystal fiber for the first time, a watt‐level passively Q‐switched Yb:LuAG single‐crystal fiber laser is realized. |
doi_str_mv | 10.1002/adom.202201087 |
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The nonlinear optical properties of BiOCl crystal, which has a broadband (visible–infrared) nonlinear saturable absorption and a high laser damage threshold to be a saturable absorber of broadband high‐power laser, are studied. Combining BiOCl with single‐crystal fiber for the first time, a watt‐level passively Q‐switched Yb:LuAG single‐crystal fiber laser is realized.</description><identifier>ISSN: 2195-1071</identifier><identifier>EISSN: 2195-1071</identifier><identifier>DOI: 10.1002/adom.202201087</identifier><language>eng</language><publisher>Weinheim: Wiley Subscription Services, Inc</publisher><subject>Absorbers ; Absorption ; BiOCl crystal ; Broadband ; Crystal fibers ; Crystal growth ; Energy gap ; Fiber lasers ; Lamellar structure ; Laser applications ; Laser damage ; Lasers ; Materials science ; nonlinear optical materials ; Nonlinear optics ; Optical properties ; Optics ; passively Q‐switched laser ; Pulsed lasers ; saturable absorption ; Single crystals ; single‐crystal fibers ; Vapor phases ; Yield point</subject><ispartof>Advanced optical materials, 2022-11, Vol.10 (22), p.n/a</ispartof><rights>2022 Wiley‐VCH GmbH</rights><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c3177-1cb48e2fe9a3bc815f01a91cf58fb4ef310292b01a2c7d2b767fdd6b41f6feec3</citedby><cites>FETCH-LOGICAL-c3177-1cb48e2fe9a3bc815f01a91cf58fb4ef310292b01a2c7d2b767fdd6b41f6feec3</cites><orcidid>0000-0002-1725-0466</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27922,27923</link.rule.ids></links><search><creatorcontrib>Ma, Xiaofei</creatorcontrib><creatorcontrib>Wang, Ci</creatorcontrib><creatorcontrib>Zhang, Jian</creatorcontrib><creatorcontrib>Wang, Tao</creatorcontrib><creatorcontrib>Wang, Anye</creatorcontrib><creatorcontrib>Wang, Siyuan</creatorcontrib><creatorcontrib>Jia, Zhitai</creatorcontrib><creatorcontrib>Zhang, Baitao</creatorcontrib><creatorcontrib>He, Jingliang</creatorcontrib><creatorcontrib>Smaalen, Sander</creatorcontrib><creatorcontrib>Tao, Xutang</creatorcontrib><title>Broadband BiOCl Nonlinear Saturable Absorber for Watt‐Level Passively Q‐Switched Yb:LuAG Single Crystal Fiber Laser</title><title>Advanced optical materials</title><description>The development of nonlinear optical (NLO) devices is limited to the mid‐infrared range due to the lack of broadband NLO response. As an indirect band gap semiconductor, BiOCl has a band gap of ≈3.3 eV. The special anisotropic lamellar structure makes it exhibit excellent electrical and optical properties; however, its NLO saturable absorption effect is rarely reported. In this study, the NLO response, optical properties, and applications of BiOCl crystals grown by chemical vapor phase transport method are studied in detail. The transmission spectrum indicates the BiOCl crystal has a broadband transparent region (0.4–11 µm). The saturable absorption of BiOCl is characterized by the Z‐scan method with 532 and 1030 nm pulsed lasers. With BiOCl as the saturable absorber (SA), watt‐level passively Q‐switched pulsed laser based on Yb:LuAG single crystal fiber (SCF) is realized. This is the first report of BiOCl as SA for passively Q‐switched all‐solid‐state pulsed laser, and the obtained average power is the highest value of passively Q‐switched SCF pulsed lasers reported so far. The high transmittance, high laser damage threshold, wideband NLO response, and environmental stability of BiOCl indicate that BiOCl crystal is a potential candidate for NLO applications.
The nonlinear optical properties of BiOCl crystal, which has a broadband (visible–infrared) nonlinear saturable absorption and a high laser damage threshold to be a saturable absorber of broadband high‐power laser, are studied. Combining BiOCl with single‐crystal fiber for the first time, a watt‐level passively Q‐switched Yb:LuAG single‐crystal fiber laser is realized.</description><subject>Absorbers</subject><subject>Absorption</subject><subject>BiOCl crystal</subject><subject>Broadband</subject><subject>Crystal fibers</subject><subject>Crystal growth</subject><subject>Energy gap</subject><subject>Fiber lasers</subject><subject>Lamellar structure</subject><subject>Laser applications</subject><subject>Laser damage</subject><subject>Lasers</subject><subject>Materials science</subject><subject>nonlinear optical materials</subject><subject>Nonlinear optics</subject><subject>Optical properties</subject><subject>Optics</subject><subject>passively Q‐switched laser</subject><subject>Pulsed lasers</subject><subject>saturable absorption</subject><subject>Single crystals</subject><subject>single‐crystal fibers</subject><subject>Vapor phases</subject><subject>Yield point</subject><issn>2195-1071</issn><issn>2195-1071</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><recordid>eNqFkEFLwzAcxYsoOOaungOeO5N0XVpvXXVTqE6ZIp5Ckiaa0TUzaR29-RH8jH4SMybqzdP_8Xi_94cXBMcIDhGE-JSVZjXEEGOIYEL2gh5GaRwiSND-H30YDJxbQuhDJEpHpBdsJtawkrO6BBM9zytwY-pK15JZsGBNaxmvJMi4M5ZLC5Sx4JE1zef7RyHfZAVumXPaiw7ceW-x0Y14kSV44mdFm83AQtfPns9t5xpWganelhTMSXsUHChWOTn4vv3gYXpxn1-GxXx2lWdFKCJESIgEHyUSK5myiIsExQoiliKh4kTxkVQRgjjF3JtYkBJzMiaqLMd8hNRYSSmifnCy611b89pK19ClaW3tX1JMIhIncZxgnxruUsIa56xUdG31itmOIki3-9LtvvRnXw-kO2CjK9n9k6bZ-fz6l_0CYW6BZA</recordid><startdate>20221118</startdate><enddate>20221118</enddate><creator>Ma, Xiaofei</creator><creator>Wang, Ci</creator><creator>Zhang, Jian</creator><creator>Wang, Tao</creator><creator>Wang, Anye</creator><creator>Wang, Siyuan</creator><creator>Jia, Zhitai</creator><creator>Zhang, Baitao</creator><creator>He, Jingliang</creator><creator>Smaalen, Sander</creator><creator>Tao, Xutang</creator><general>Wiley Subscription Services, Inc</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>7U5</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0002-1725-0466</orcidid></search><sort><creationdate>20221118</creationdate><title>Broadband BiOCl Nonlinear Saturable Absorber for Watt‐Level Passively Q‐Switched Yb:LuAG Single Crystal Fiber Laser</title><author>Ma, Xiaofei ; Wang, Ci ; Zhang, Jian ; Wang, Tao ; Wang, Anye ; Wang, Siyuan ; Jia, Zhitai ; Zhang, Baitao ; He, Jingliang ; Smaalen, Sander ; Tao, Xutang</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c3177-1cb48e2fe9a3bc815f01a91cf58fb4ef310292b01a2c7d2b767fdd6b41f6feec3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><topic>Absorbers</topic><topic>Absorption</topic><topic>BiOCl crystal</topic><topic>Broadband</topic><topic>Crystal fibers</topic><topic>Crystal growth</topic><topic>Energy gap</topic><topic>Fiber lasers</topic><topic>Lamellar structure</topic><topic>Laser applications</topic><topic>Laser damage</topic><topic>Lasers</topic><topic>Materials science</topic><topic>nonlinear optical materials</topic><topic>Nonlinear optics</topic><topic>Optical properties</topic><topic>Optics</topic><topic>passively Q‐switched laser</topic><topic>Pulsed lasers</topic><topic>saturable absorption</topic><topic>Single crystals</topic><topic>single‐crystal fibers</topic><topic>Vapor phases</topic><topic>Yield point</topic><toplevel>online_resources</toplevel><creatorcontrib>Ma, Xiaofei</creatorcontrib><creatorcontrib>Wang, Ci</creatorcontrib><creatorcontrib>Zhang, Jian</creatorcontrib><creatorcontrib>Wang, Tao</creatorcontrib><creatorcontrib>Wang, Anye</creatorcontrib><creatorcontrib>Wang, Siyuan</creatorcontrib><creatorcontrib>Jia, Zhitai</creatorcontrib><creatorcontrib>Zhang, Baitao</creatorcontrib><creatorcontrib>He, Jingliang</creatorcontrib><creatorcontrib>Smaalen, Sander</creatorcontrib><creatorcontrib>Tao, Xutang</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><jtitle>Advanced optical materials</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Ma, Xiaofei</au><au>Wang, Ci</au><au>Zhang, Jian</au><au>Wang, Tao</au><au>Wang, Anye</au><au>Wang, Siyuan</au><au>Jia, Zhitai</au><au>Zhang, Baitao</au><au>He, Jingliang</au><au>Smaalen, Sander</au><au>Tao, Xutang</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Broadband BiOCl Nonlinear Saturable Absorber for Watt‐Level Passively Q‐Switched Yb:LuAG Single Crystal Fiber Laser</atitle><jtitle>Advanced optical materials</jtitle><date>2022-11-18</date><risdate>2022</risdate><volume>10</volume><issue>22</issue><epage>n/a</epage><issn>2195-1071</issn><eissn>2195-1071</eissn><abstract>The development of nonlinear optical (NLO) devices is limited to the mid‐infrared range due to the lack of broadband NLO response. As an indirect band gap semiconductor, BiOCl has a band gap of ≈3.3 eV. The special anisotropic lamellar structure makes it exhibit excellent electrical and optical properties; however, its NLO saturable absorption effect is rarely reported. In this study, the NLO response, optical properties, and applications of BiOCl crystals grown by chemical vapor phase transport method are studied in detail. The transmission spectrum indicates the BiOCl crystal has a broadband transparent region (0.4–11 µm). The saturable absorption of BiOCl is characterized by the Z‐scan method with 532 and 1030 nm pulsed lasers. With BiOCl as the saturable absorber (SA), watt‐level passively Q‐switched pulsed laser based on Yb:LuAG single crystal fiber (SCF) is realized. This is the first report of BiOCl as SA for passively Q‐switched all‐solid‐state pulsed laser, and the obtained average power is the highest value of passively Q‐switched SCF pulsed lasers reported so far. The high transmittance, high laser damage threshold, wideband NLO response, and environmental stability of BiOCl indicate that BiOCl crystal is a potential candidate for NLO applications.
The nonlinear optical properties of BiOCl crystal, which has a broadband (visible–infrared) nonlinear saturable absorption and a high laser damage threshold to be a saturable absorber of broadband high‐power laser, are studied. Combining BiOCl with single‐crystal fiber for the first time, a watt‐level passively Q‐switched Yb:LuAG single‐crystal fiber laser is realized.</abstract><cop>Weinheim</cop><pub>Wiley Subscription Services, Inc</pub><doi>10.1002/adom.202201087</doi><tpages>10</tpages><orcidid>https://orcid.org/0000-0002-1725-0466</orcidid></addata></record> |
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subjects | Absorbers Absorption BiOCl crystal Broadband Crystal fibers Crystal growth Energy gap Fiber lasers Lamellar structure Laser applications Laser damage Lasers Materials science nonlinear optical materials Nonlinear optics Optical properties Optics passively Q‐switched laser Pulsed lasers saturable absorption Single crystals single‐crystal fibers Vapor phases Yield point |
title | Broadband BiOCl Nonlinear Saturable Absorber for Watt‐Level Passively Q‐Switched Yb:LuAG Single Crystal Fiber Laser |
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