G. Lesly Jimenez , Lijun Wang , C. Vazquez-Lopez , A.N. Meza-Rocha , Marcin Kochanowicz , B. Starzyk , Ciro Falcony , Dominik Dorosz
{"title":"808 纳米激发下氟茚酸盐玻璃中的蓝色和绿色上转换辐射","authors":"G. Lesly Jimenez , Lijun Wang , C. Vazquez-Lopez , A.N. Meza-Rocha , Marcin Kochanowicz , B. Starzyk , Ciro Falcony , Dominik Dorosz","doi":"10.1016/j.omx.2024.100289","DOIUrl":null,"url":null,"abstract":"<div><p>In this study, the upconversion (UC) luminescence of fluoroindate glasses (InF<sub>3</sub>G) co-doped with Yb-Nd-Er (Tm) ions excited in the NIR-I biological window was analyzed. In the first system, UC emission of singly Er<sup>3+</sup> doped InF<sub>3</sub>G under 808 nm excitation occurred to be more efficient than those observed in InF<sub>3</sub>G co-doped with Yb–Er and Yb-Nd-Er. The intensity of UC emission (InF<sub>3</sub>G-Er) was 22 % higher than InF<sub>3</sub>G-Yb-Er, and even more than two times higher than in the InF<sub>3</sub>G-Yb-Nd-Er sample. The effective energy transfer (η) between Nd<sup>3+</sup>- Yb<sup>3+</sup> (η = 45 %) and Yb<sup>3+</sup>-Er<sup>3+</sup> (η = 68 %), was reflected in the emission observed in the NIR region mainly, ascribed to Yb<sup>3+</sup>:<sup>2</sup>F<sub>5/2</sub> → <sup>2</sup>F<sub>7/2</sub> (978 and 999 nm) and Nd<sup>3+</sup>:<sup>4</sup>F<sub>3/2</sub> → <sup>4</sup>I<sub>9/2</sub> (1053 nm) transitions. Meanwhile, the samples co-doped with Tm<sup>3+</sup> exhibited a strong dependence on Yb-Nd-Tm co-doping. Samples without Yb and Nd did not exhibit any UC emission due to the absence of pumping channel. This contrasts with the downshifting NIR emission, which was at least two times higher than those exhibited in samples co-doped Yb-Nd-Er. These results suggest that Tm<sup>3+</sup> plays a crucial role in populating the lower-lying exited levels of Yb and Nd, influencing the overall emission behavior.</p></div>","PeriodicalId":52192,"journal":{"name":"Optical Materials: X","volume":"21 ","pages":"Article 100289"},"PeriodicalIF":0.0000,"publicationDate":"2024-01-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S2590147824000019/pdfft?md5=82c3f54a0d7074916a7246c876db2cee&pid=1-s2.0-S2590147824000019-main.pdf","citationCount":"0","resultStr":"{\"title\":\"Blue and green upconverted emission in fluoroindate glasses under 808 nm excitation\",\"authors\":\"G. Lesly Jimenez , Lijun Wang , C. Vazquez-Lopez , A.N. Meza-Rocha , Marcin Kochanowicz , B. Starzyk , Ciro Falcony , Dominik Dorosz\",\"doi\":\"10.1016/j.omx.2024.100289\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>In this study, the upconversion (UC) luminescence of fluoroindate glasses (InF<sub>3</sub>G) co-doped with Yb-Nd-Er (Tm) ions excited in the NIR-I biological window was analyzed. In the first system, UC emission of singly Er<sup>3+</sup> doped InF<sub>3</sub>G under 808 nm excitation occurred to be more efficient than those observed in InF<sub>3</sub>G co-doped with Yb–Er and Yb-Nd-Er. The intensity of UC emission (InF<sub>3</sub>G-Er) was 22 % higher than InF<sub>3</sub>G-Yb-Er, and even more than two times higher than in the InF<sub>3</sub>G-Yb-Nd-Er sample. The effective energy transfer (η) between Nd<sup>3+</sup>- Yb<sup>3+</sup> (η = 45 %) and Yb<sup>3+</sup>-Er<sup>3+</sup> (η = 68 %), was reflected in the emission observed in the NIR region mainly, ascribed to Yb<sup>3+</sup>:<sup>2</sup>F<sub>5/2</sub> → <sup>2</sup>F<sub>7/2</sub> (978 and 999 nm) and Nd<sup>3+</sup>:<sup>4</sup>F<sub>3/2</sub> → <sup>4</sup>I<sub>9/2</sub> (1053 nm) transitions. Meanwhile, the samples co-doped with Tm<sup>3+</sup> exhibited a strong dependence on Yb-Nd-Tm co-doping. Samples without Yb and Nd did not exhibit any UC emission due to the absence of pumping channel. This contrasts with the downshifting NIR emission, which was at least two times higher than those exhibited in samples co-doped Yb-Nd-Er. These results suggest that Tm<sup>3+</sup> plays a crucial role in populating the lower-lying exited levels of Yb and Nd, influencing the overall emission behavior.</p></div>\",\"PeriodicalId\":52192,\"journal\":{\"name\":\"Optical Materials: X\",\"volume\":\"21 \",\"pages\":\"Article 100289\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-01-02\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://www.sciencedirect.com/science/article/pii/S2590147824000019/pdfft?md5=82c3f54a0d7074916a7246c876db2cee&pid=1-s2.0-S2590147824000019-main.pdf\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Optical Materials: X\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S2590147824000019\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"Engineering\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Optical Materials: X","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S2590147824000019","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"Engineering","Score":null,"Total":0}
Blue and green upconverted emission in fluoroindate glasses under 808 nm excitation
In this study, the upconversion (UC) luminescence of fluoroindate glasses (InF3G) co-doped with Yb-Nd-Er (Tm) ions excited in the NIR-I biological window was analyzed. In the first system, UC emission of singly Er3+ doped InF3G under 808 nm excitation occurred to be more efficient than those observed in InF3G co-doped with Yb–Er and Yb-Nd-Er. The intensity of UC emission (InF3G-Er) was 22 % higher than InF3G-Yb-Er, and even more than two times higher than in the InF3G-Yb-Nd-Er sample. The effective energy transfer (η) between Nd3+- Yb3+ (η = 45 %) and Yb3+-Er3+ (η = 68 %), was reflected in the emission observed in the NIR region mainly, ascribed to Yb3+:2F5/2 → 2F7/2 (978 and 999 nm) and Nd3+:4F3/2 → 4I9/2 (1053 nm) transitions. Meanwhile, the samples co-doped with Tm3+ exhibited a strong dependence on Yb-Nd-Tm co-doping. Samples without Yb and Nd did not exhibit any UC emission due to the absence of pumping channel. This contrasts with the downshifting NIR emission, which was at least two times higher than those exhibited in samples co-doped Yb-Nd-Er. These results suggest that Tm3+ plays a crucial role in populating the lower-lying exited levels of Yb and Nd, influencing the overall emission behavior.