Kan Lu, Qifan Zhang, Juan Kong, Yan Hao, Wenxia Wu, Yazhao Wang, Haibo Lin, Shoulei Xu and Wen Deng
{"title":"由 980 纳米激光激发的 Ho/Tm/Yb 共掺杂鲁特西亚稳定氧化锆单晶上转换产生的高效紫外线和可见光发射","authors":"Kan Lu, Qifan Zhang, Juan Kong, Yan Hao, Wenxia Wu, Yazhao Wang, Haibo Lin, Shoulei Xu and Wen Deng","doi":"10.1039/D4CE00844H","DOIUrl":null,"url":null,"abstract":"<p >High-quality transparent cubic lutecia-stabilized zirconia (LSZ) and LSZ:Yb<small><sub>0.25</sub></small>Tm<small><sub>0.5</sub></small>Ho<small><sub>0.03</sub></small> single crystals were fabricated by the OFZ (optical floating zone) method for the first time. For comparison, YSZ and YSZ:Yb<small><sub>0.25</sub></small>Tm<small><sub>0.5</sub></small>Ho<small><sub>0.03</sub></small> single crystals were also fabricated. The transmittance of the LSZ single crystal (80.7%) is slightly lower than that of the YSZ single crystal (86.3%) in the visible light region, which is attributed to the LSZ single crystal with a higher density (6.604 g cm<small><sup>−3</sup></small>) in comparison with that of the YSZ single crystal (5.973 g cm<small><sup>−3</sup></small>). No absorption peaks were observed in the transmission and absorption spectra of LSZ and YSZ within 200–1100 nm, indicating that both crystals are excellent host crystals. The density of LSZ:Yb<small><sub>0.25</sub></small>Tm<small><sub>0.5</sub></small>Ho<small><sub>0.03</sub></small> single crystals (6.596 g cm<small><sup>−3</sup></small>) is also higher than that of YSZ:Yb<small><sub>0.25</sub></small>Tm<small><sub>0.5</sub></small>Ho<small><sub>0.03</sub></small> single crystals (6.005 g cm<small><sup>−3</sup></small>). The absorption spectra of LSZ:Yb<small><sub>0.25</sub></small>Tm<small><sub>0.5</sub></small>Ho<small><sub>0.03</sub></small> and YSZ:Yb<small><sub>0.25</sub></small>Tm<small><sub>0.5</sub></small>Ho<small><sub>0.03</sub></small> single crystals exhibited several absorption peaks at 363, 453, 678, and 785 nm and a strong broad absorption band within 850–1000 nm. The upconversion photoluminescence (UCPL) spectrum of the LSZ:Yb<small><sub>0.25</sub></small>Tm<small><sub>0.5</sub></small>Ho<small><sub>0.03</sub></small> single crystal excited at 980 nm exhibited several emission peaks at 308, 373, 488, 540, 550, 655 and 794 nm; similar emission peaks were observed in the UCPL spectrum of the YSZ:Yb<small><sub>0.25</sub></small>Tm<small><sub>0.5</sub></small>Ho<small><sub>0.03</sub></small> single crystal. The intensities of the emission peaks of the former are higher than those of the corresponding peaks of the latter, which is due to the former having a higher density and lower phonon energy in comparison with the latter. Power curves indicated that the 308 and 373 nm emissions are 4-photon upconversion processes, the 488 nm emission is a 3-photon process, and the 540 nm and 655 nm emissions are 2-photon processes. These results indicate that under the excitation at 980 nm, the LSZ:Yb<small><sub>0.25</sub></small>Tm<small><sub>0.5</sub></small>Ho<small><sub>0.03</sub></small> single crystal has high efficiency over the YSZ:Yb<small><sub>0.25</sub></small>Tm<small><sub>0.5</sub></small>Ho<small><sub>0.03</sub></small> single crystal in ultraviolet and visible light emissions.</p>","PeriodicalId":70,"journal":{"name":"CrystEngComm","volume":" 41","pages":" 5907-5915"},"PeriodicalIF":2.6000,"publicationDate":"2024-10-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Highly efficient ultraviolet and visible light emissions from upconversion transitions in Ho/Tm/Yb co-doped lutecia-stabilized zirconia single crystals excited by a 980 nm laser\",\"authors\":\"Kan Lu, Qifan Zhang, Juan Kong, Yan Hao, Wenxia Wu, Yazhao Wang, Haibo Lin, Shoulei Xu and Wen Deng\",\"doi\":\"10.1039/D4CE00844H\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p >High-quality transparent cubic lutecia-stabilized zirconia (LSZ) and LSZ:Yb<small><sub>0.25</sub></small>Tm<small><sub>0.5</sub></small>Ho<small><sub>0.03</sub></small> single crystals were fabricated by the OFZ (optical floating zone) method for the first time. For comparison, YSZ and YSZ:Yb<small><sub>0.25</sub></small>Tm<small><sub>0.5</sub></small>Ho<small><sub>0.03</sub></small> single crystals were also fabricated. The transmittance of the LSZ single crystal (80.7%) is slightly lower than that of the YSZ single crystal (86.3%) in the visible light region, which is attributed to the LSZ single crystal with a higher density (6.604 g cm<small><sup>−3</sup></small>) in comparison with that of the YSZ single crystal (5.973 g cm<small><sup>−3</sup></small>). No absorption peaks were observed in the transmission and absorption spectra of LSZ and YSZ within 200–1100 nm, indicating that both crystals are excellent host crystals. The density of LSZ:Yb<small><sub>0.25</sub></small>Tm<small><sub>0.5</sub></small>Ho<small><sub>0.03</sub></small> single crystals (6.596 g cm<small><sup>−3</sup></small>) is also higher than that of YSZ:Yb<small><sub>0.25</sub></small>Tm<small><sub>0.5</sub></small>Ho<small><sub>0.03</sub></small> single crystals (6.005 g cm<small><sup>−3</sup></small>). The absorption spectra of LSZ:Yb<small><sub>0.25</sub></small>Tm<small><sub>0.5</sub></small>Ho<small><sub>0.03</sub></small> and YSZ:Yb<small><sub>0.25</sub></small>Tm<small><sub>0.5</sub></small>Ho<small><sub>0.03</sub></small> single crystals exhibited several absorption peaks at 363, 453, 678, and 785 nm and a strong broad absorption band within 850–1000 nm. The upconversion photoluminescence (UCPL) spectrum of the LSZ:Yb<small><sub>0.25</sub></small>Tm<small><sub>0.5</sub></small>Ho<small><sub>0.03</sub></small> single crystal excited at 980 nm exhibited several emission peaks at 308, 373, 488, 540, 550, 655 and 794 nm; similar emission peaks were observed in the UCPL spectrum of the YSZ:Yb<small><sub>0.25</sub></small>Tm<small><sub>0.5</sub></small>Ho<small><sub>0.03</sub></small> single crystal. The intensities of the emission peaks of the former are higher than those of the corresponding peaks of the latter, which is due to the former having a higher density and lower phonon energy in comparison with the latter. Power curves indicated that the 308 and 373 nm emissions are 4-photon upconversion processes, the 488 nm emission is a 3-photon process, and the 540 nm and 655 nm emissions are 2-photon processes. These results indicate that under the excitation at 980 nm, the LSZ:Yb<small><sub>0.25</sub></small>Tm<small><sub>0.5</sub></small>Ho<small><sub>0.03</sub></small> single crystal has high efficiency over the YSZ:Yb<small><sub>0.25</sub></small>Tm<small><sub>0.5</sub></small>Ho<small><sub>0.03</sub></small> single crystal in ultraviolet and visible light emissions.</p>\",\"PeriodicalId\":70,\"journal\":{\"name\":\"CrystEngComm\",\"volume\":\" 41\",\"pages\":\" 5907-5915\"},\"PeriodicalIF\":2.6000,\"publicationDate\":\"2024-10-03\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"CrystEngComm\",\"FirstCategoryId\":\"92\",\"ListUrlMain\":\"https://pubs.rsc.org/en/content/articlelanding/2024/ce/d4ce00844h\",\"RegionNum\":3,\"RegionCategory\":\"化学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"CHEMISTRY, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"CrystEngComm","FirstCategoryId":"92","ListUrlMain":"https://pubs.rsc.org/en/content/articlelanding/2024/ce/d4ce00844h","RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"CHEMISTRY, MULTIDISCIPLINARY","Score":null,"Total":0}
Highly efficient ultraviolet and visible light emissions from upconversion transitions in Ho/Tm/Yb co-doped lutecia-stabilized zirconia single crystals excited by a 980 nm laser
High-quality transparent cubic lutecia-stabilized zirconia (LSZ) and LSZ:Yb0.25Tm0.5Ho0.03 single crystals were fabricated by the OFZ (optical floating zone) method for the first time. For comparison, YSZ and YSZ:Yb0.25Tm0.5Ho0.03 single crystals were also fabricated. The transmittance of the LSZ single crystal (80.7%) is slightly lower than that of the YSZ single crystal (86.3%) in the visible light region, which is attributed to the LSZ single crystal with a higher density (6.604 g cm−3) in comparison with that of the YSZ single crystal (5.973 g cm−3). No absorption peaks were observed in the transmission and absorption spectra of LSZ and YSZ within 200–1100 nm, indicating that both crystals are excellent host crystals. The density of LSZ:Yb0.25Tm0.5Ho0.03 single crystals (6.596 g cm−3) is also higher than that of YSZ:Yb0.25Tm0.5Ho0.03 single crystals (6.005 g cm−3). The absorption spectra of LSZ:Yb0.25Tm0.5Ho0.03 and YSZ:Yb0.25Tm0.5Ho0.03 single crystals exhibited several absorption peaks at 363, 453, 678, and 785 nm and a strong broad absorption band within 850–1000 nm. The upconversion photoluminescence (UCPL) spectrum of the LSZ:Yb0.25Tm0.5Ho0.03 single crystal excited at 980 nm exhibited several emission peaks at 308, 373, 488, 540, 550, 655 and 794 nm; similar emission peaks were observed in the UCPL spectrum of the YSZ:Yb0.25Tm0.5Ho0.03 single crystal. The intensities of the emission peaks of the former are higher than those of the corresponding peaks of the latter, which is due to the former having a higher density and lower phonon energy in comparison with the latter. Power curves indicated that the 308 and 373 nm emissions are 4-photon upconversion processes, the 488 nm emission is a 3-photon process, and the 540 nm and 655 nm emissions are 2-photon processes. These results indicate that under the excitation at 980 nm, the LSZ:Yb0.25Tm0.5Ho0.03 single crystal has high efficiency over the YSZ:Yb0.25Tm0.5Ho0.03 single crystal in ultraviolet and visible light emissions.