Ye Zhang, Siyuan Liu, Jianwei Yang, Yufei Chen, Hongsen He, Jun Dong
{"title":"拉曼微芯片激光器中二维可调指数结构光场","authors":"Ye Zhang, Siyuan Liu, Jianwei Yang, Yufei Chen, Hongsen He, Jun Dong","doi":"10.1002/apxr.202400167","DOIUrl":null,"url":null,"abstract":"<p>Structured light fields in the form of Hermite-Gaussian modes with 2D tunable indices of <i>m</i> and <i>n</i> (HG<i><sub>m</sub></i><sub>,</sub><i><sub>n</sub></i>), and optical vortices in the form of Laguerre-Gaussian modes with radial index <i>p</i> and azimuthal index <i>l</i> (LG<sub>p,</sub><i><sub>l</sub></i>) are extremely needed for applications on optical communications, optical trapping, and quantum information processing. Here, high-order HG<i><sub>m</sub></i><sub>,</sub><i><sub>n</sub></i> modes and LG<i><sub>p</sub></i><sub>,</sub><i><sub>l</sub></i> optical vortices with 2D tunable indices are generated in a gain-manipulated Yb:YAG/YVO<sub>4</sub> Raman microchip laser (RML). The gain distribution is manipulated by controlling the separation between Yb:YAG crystal and the focus spot of the <i>y</i>-axis of the laser diode (Δz). HG<i><sub>m</sub></i><sub>,</sub><i><sub>n</sub></i> modes with 2D tunable indices of <i>m</i> up to 14 and <i>n</i> up to 2 are generated in Yb:YAG/YVO<sub>4</sub> RML by setting Δz = −0.5, −4.1, and −6.6 mm. The power of HG<sub>14,0</sub>, HG<sub>7,1</sub>, and HG<sub>6,2</sub> mode lasers are 0.49, 0.31, and 0.34 W under pump power of 3.1 W, and corresponding optical efficiencies are 11%, 7%, and 7.7%. LG<i><sub>p</sub></i><sub>,</sub><i><sub>l</sub></i> optical vortices with <i>p</i> = 0, 1, 2, and <i>l</i> up to 14 are converted from HG<i><sub>m</sub></i><sub>,</sub><i><sub>n</sub></i> mode lasers with a conversion efficiency of over 90%. High beam quality HG<i><sub>m</sub></i><sub>,</sub><i><sub>n</sub></i> modes, and LG<i><sub>p</sub></i><sub>,</sub><i><sub>l</sub></i> optical vortices with 2D tunable indices oscillating at Stokes wavelengths dramatically extend their applications.</p>","PeriodicalId":100035,"journal":{"name":"Advanced Physics Research","volume":"4 5","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2025-02-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1002/apxr.202400167","citationCount":"0","resultStr":"{\"title\":\"Structured Light Fields with 2D Tunable Indices Generated in a Raman Microchip Laser\",\"authors\":\"Ye Zhang, Siyuan Liu, Jianwei Yang, Yufei Chen, Hongsen He, Jun Dong\",\"doi\":\"10.1002/apxr.202400167\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>Structured light fields in the form of Hermite-Gaussian modes with 2D tunable indices of <i>m</i> and <i>n</i> (HG<i><sub>m</sub></i><sub>,</sub><i><sub>n</sub></i>), and optical vortices in the form of Laguerre-Gaussian modes with radial index <i>p</i> and azimuthal index <i>l</i> (LG<sub>p,</sub><i><sub>l</sub></i>) are extremely needed for applications on optical communications, optical trapping, and quantum information processing. Here, high-order HG<i><sub>m</sub></i><sub>,</sub><i><sub>n</sub></i> modes and LG<i><sub>p</sub></i><sub>,</sub><i><sub>l</sub></i> optical vortices with 2D tunable indices are generated in a gain-manipulated Yb:YAG/YVO<sub>4</sub> Raman microchip laser (RML). The gain distribution is manipulated by controlling the separation between Yb:YAG crystal and the focus spot of the <i>y</i>-axis of the laser diode (Δz). HG<i><sub>m</sub></i><sub>,</sub><i><sub>n</sub></i> modes with 2D tunable indices of <i>m</i> up to 14 and <i>n</i> up to 2 are generated in Yb:YAG/YVO<sub>4</sub> RML by setting Δz = −0.5, −4.1, and −6.6 mm. The power of HG<sub>14,0</sub>, HG<sub>7,1</sub>, and HG<sub>6,2</sub> mode lasers are 0.49, 0.31, and 0.34 W under pump power of 3.1 W, and corresponding optical efficiencies are 11%, 7%, and 7.7%. LG<i><sub>p</sub></i><sub>,</sub><i><sub>l</sub></i> optical vortices with <i>p</i> = 0, 1, 2, and <i>l</i> up to 14 are converted from HG<i><sub>m</sub></i><sub>,</sub><i><sub>n</sub></i> mode lasers with a conversion efficiency of over 90%. High beam quality HG<i><sub>m</sub></i><sub>,</sub><i><sub>n</sub></i> modes, and LG<i><sub>p</sub></i><sub>,</sub><i><sub>l</sub></i> optical vortices with 2D tunable indices oscillating at Stokes wavelengths dramatically extend their applications.</p>\",\"PeriodicalId\":100035,\"journal\":{\"name\":\"Advanced Physics Research\",\"volume\":\"4 5\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2025-02-25\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://onlinelibrary.wiley.com/doi/epdf/10.1002/apxr.202400167\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Advanced Physics Research\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://onlinelibrary.wiley.com/doi/10.1002/apxr.202400167\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Advanced Physics Research","FirstCategoryId":"1085","ListUrlMain":"https://onlinelibrary.wiley.com/doi/10.1002/apxr.202400167","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Structured Light Fields with 2D Tunable Indices Generated in a Raman Microchip Laser
Structured light fields in the form of Hermite-Gaussian modes with 2D tunable indices of m and n (HGm,n), and optical vortices in the form of Laguerre-Gaussian modes with radial index p and azimuthal index l (LGp,l) are extremely needed for applications on optical communications, optical trapping, and quantum information processing. Here, high-order HGm,n modes and LGp,l optical vortices with 2D tunable indices are generated in a gain-manipulated Yb:YAG/YVO4 Raman microchip laser (RML). The gain distribution is manipulated by controlling the separation between Yb:YAG crystal and the focus spot of the y-axis of the laser diode (Δz). HGm,n modes with 2D tunable indices of m up to 14 and n up to 2 are generated in Yb:YAG/YVO4 RML by setting Δz = −0.5, −4.1, and −6.6 mm. The power of HG14,0, HG7,1, and HG6,2 mode lasers are 0.49, 0.31, and 0.34 W under pump power of 3.1 W, and corresponding optical efficiencies are 11%, 7%, and 7.7%. LGp,l optical vortices with p = 0, 1, 2, and l up to 14 are converted from HGm,n mode lasers with a conversion efficiency of over 90%. High beam quality HGm,n modes, and LGp,l optical vortices with 2D tunable indices oscillating at Stokes wavelengths dramatically extend their applications.