Lisa Lopez, F. Druon, Patrick Georges, F. Balembois
{"title":"LED-pumped Er: Cr: YSGG","authors":"Lisa Lopez, F. Druon, Patrick Georges, F. Balembois","doi":"10.1109/CLEO/Europe-EQEC57999.2023.10232330","DOIUrl":null,"url":null,"abstract":"Er:Cr:YSGG is a well know crystal with laser emission at 2.79 μm [1] useful for medical applications and particularly for dentistry [2]. Energy transfer between Cr and Er allows to pump this crystal with flashlamps. In a search for new sources emitting in the SWIR, we propose to revisit this crystal with a new way of pumping: with LEDs. Er:Cr:YSGG generally operates on its ${ }^{4} \\mathrm{I}_{11 / 2}{ }^{-4} \\mathrm{I}_{13 / 2}$ transition for laser emission at 2.79 μm. Its ${ }^{4} \\mathrm{I}_{13 / 2}{ }^{-4} \\mathrm{I}_{15 / 2}$ transition around 1.6 $\\mu \\mathrm{m}$ can also be investigated for spontaneous emission. Indeed, this wavelength range is interesting for high-brightness, spectrally broadband and incoherent sources in the SWIR adapted for InGaAs cameras. In order to collect the spontaneous emission efficiently, a geometry of luminescent concentrator (LC) can be used [3]. The purpose of this work is to investigate the performance of Er:Cr:YSGG on both transitions.","PeriodicalId":19477,"journal":{"name":"Oceans","volume":"32 1","pages":"1-1"},"PeriodicalIF":0.0000,"publicationDate":"2023-06-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"LED-pumped Er:Cr:YSGG\",\"authors\":\"Lisa Lopez, F. Druon, Patrick Georges, F. Balembois\",\"doi\":\"10.1109/CLEO/Europe-EQEC57999.2023.10232330\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Er:Cr:YSGG is a well know crystal with laser emission at 2.79 μm [1] useful for medical applications and particularly for dentistry [2]. Energy transfer between Cr and Er allows to pump this crystal with flashlamps. In a search for new sources emitting in the SWIR, we propose to revisit this crystal with a new way of pumping: with LEDs. Er:Cr:YSGG generally operates on its ${ }^{4} \\\\mathrm{I}_{11 / 2}{ }^{-4} \\\\mathrm{I}_{13 / 2}$ transition for laser emission at 2.79 μm. Its ${ }^{4} \\\\mathrm{I}_{13 / 2}{ }^{-4} \\\\mathrm{I}_{15 / 2}$ transition around 1.6 $\\\\mu \\\\mathrm{m}$ can also be investigated for spontaneous emission. Indeed, this wavelength range is interesting for high-brightness, spectrally broadband and incoherent sources in the SWIR adapted for InGaAs cameras. In order to collect the spontaneous emission efficiently, a geometry of luminescent concentrator (LC) can be used [3]. The purpose of this work is to investigate the performance of Er:Cr:YSGG on both transitions.\",\"PeriodicalId\":19477,\"journal\":{\"name\":\"Oceans\",\"volume\":\"32 1\",\"pages\":\"1-1\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2023-06-26\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Oceans\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/CLEO/Europe-EQEC57999.2023.10232330\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Oceans","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/CLEO/Europe-EQEC57999.2023.10232330","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Er:Cr:YSGG is a well know crystal with laser emission at 2.79 μm [1] useful for medical applications and particularly for dentistry [2]. Energy transfer between Cr and Er allows to pump this crystal with flashlamps. In a search for new sources emitting in the SWIR, we propose to revisit this crystal with a new way of pumping: with LEDs. Er:Cr:YSGG generally operates on its ${ }^{4} \mathrm{I}_{11 / 2}{ }^{-4} \mathrm{I}_{13 / 2}$ transition for laser emission at 2.79 μm. Its ${ }^{4} \mathrm{I}_{13 / 2}{ }^{-4} \mathrm{I}_{15 / 2}$ transition around 1.6 $\mu \mathrm{m}$ can also be investigated for spontaneous emission. Indeed, this wavelength range is interesting for high-brightness, spectrally broadband and incoherent sources in the SWIR adapted for InGaAs cameras. In order to collect the spontaneous emission efficiently, a geometry of luminescent concentrator (LC) can be used [3]. The purpose of this work is to investigate the performance of Er:Cr:YSGG on both transitions.