{"title":"用庞德-德雷弗-霍尔方案稳定腔内双连续波光学参量振荡器的kHz电平","authors":"O. Mhibik, D. Paboeuf, C. Drag, F. Bretenaker","doi":"10.1109/CLEOE.2011.5942757","DOIUrl":null,"url":null,"abstract":"Quantum manipulation using the optical transition (3H4→1D2) of Pr3+ embedded in solid state host materials requires a visible source emitting at 606 nm with a linewidth at the kHz level [1]. In a previous work, we have reported the stabilization of a continuous wave intracavity frequency doubled singly resonant optical parametric oscillator (cw-SHG-SRO) by locking it onto the side of the transmission fringe of a medium finesse Fabry-Perot (FP) cavity [2]. In this scheme, the signal transmitted by the FP cavity was not only sensitive to any frequency fluctuation but also to any change in the source power, which can be misinterpreted as a frequency fluctuation.","PeriodicalId":6331,"journal":{"name":"2011 Conference on Lasers and Electro-Optics Europe and 12th European Quantum Electronics Conference (CLEO EUROPE/EQEC)","volume":"25 1","pages":"1-1"},"PeriodicalIF":0.0000,"publicationDate":"2011-05-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"The kHz level stabilization of an intracavity doubled continuous wave optical parametric oscillator using Pound-Drever-Hall scheme\",\"authors\":\"O. Mhibik, D. Paboeuf, C. Drag, F. Bretenaker\",\"doi\":\"10.1109/CLEOE.2011.5942757\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Quantum manipulation using the optical transition (3H4→1D2) of Pr3+ embedded in solid state host materials requires a visible source emitting at 606 nm with a linewidth at the kHz level [1]. In a previous work, we have reported the stabilization of a continuous wave intracavity frequency doubled singly resonant optical parametric oscillator (cw-SHG-SRO) by locking it onto the side of the transmission fringe of a medium finesse Fabry-Perot (FP) cavity [2]. In this scheme, the signal transmitted by the FP cavity was not only sensitive to any frequency fluctuation but also to any change in the source power, which can be misinterpreted as a frequency fluctuation.\",\"PeriodicalId\":6331,\"journal\":{\"name\":\"2011 Conference on Lasers and Electro-Optics Europe and 12th European Quantum Electronics Conference (CLEO EUROPE/EQEC)\",\"volume\":\"25 1\",\"pages\":\"1-1\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2011-05-22\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2011 Conference on Lasers and Electro-Optics Europe and 12th European Quantum Electronics Conference (CLEO EUROPE/EQEC)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/CLEOE.2011.5942757\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2011 Conference on Lasers and Electro-Optics Europe and 12th European Quantum Electronics Conference (CLEO EUROPE/EQEC)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/CLEOE.2011.5942757","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
The kHz level stabilization of an intracavity doubled continuous wave optical parametric oscillator using Pound-Drever-Hall scheme
Quantum manipulation using the optical transition (3H4→1D2) of Pr3+ embedded in solid state host materials requires a visible source emitting at 606 nm with a linewidth at the kHz level [1]. In a previous work, we have reported the stabilization of a continuous wave intracavity frequency doubled singly resonant optical parametric oscillator (cw-SHG-SRO) by locking it onto the side of the transmission fringe of a medium finesse Fabry-Perot (FP) cavity [2]. In this scheme, the signal transmitted by the FP cavity was not only sensitive to any frequency fluctuation but also to any change in the source power, which can be misinterpreted as a frequency fluctuation.