Ye Kuang, Junhao Xu, Guangli Shi, Tengbo Hu, Xian Wang, Bo Li, Yu Liang, Panpan Qin, Wen Zeng, Hao Wang, Longhai Shen, Yiwei Wang
{"title":"高掺杂核-多壳上转换纳米颗粒中Ho3+和Yb3+浓度分布对Ce3+微调上转换发光的影响","authors":"Ye Kuang, Junhao Xu, Guangli Shi, Tengbo Hu, Xian Wang, Bo Li, Yu Liang, Panpan Qin, Wen Zeng, Hao Wang, Longhai Shen, Yiwei Wang","doi":"10.1016/j.jallcom.2025.181927","DOIUrl":null,"url":null,"abstract":"Although widely used for Ho-based upconversion luminescence (UCL) fine-tuning of upconversion nanoparticles (UCNPs), Ce<ce:sup loc=\"post\">3+</ce:sup> doping has lacked comprehensive investigation in core–multi-shell and highly doped structures. Herein, a series of highly doped core–multi-shell UCNPs with Ce<ce:sup loc=\"post\">3+</ce:sup> doping were synthesised via oleate-based methods. The structures and morphologies were characterised by X-ray diffraction (XRD), transmission emission microscopy (TEM) and elemental mapping, while UCL properties were assessed using emission spectra, decay curves and pump power measurements. The distributions of Ho<ce:sup loc=\"post\">3+</ce:sup> and Yb<ce:sup loc=\"post\">3+</ce:sup> concentrations were systematically varied to explore, for the first time, their distinct effects on Ce<ce:sup loc=\"post\">3+</ce:sup>-mediated UCL fine-tuning. These effects arose from different energy mechanisms and varied with the number of shell layers. A deficiency in phonon energy was found to reduce the efficiency of both Yb<ce:sup loc=\"post\">3+</ce:sup>–Ho<ce:sup loc=\"post\">3+</ce:sup> energy transfer and Ho<ce:sup loc=\"post\">3+</ce:sup>–Ce<ce:sup loc=\"post\">3+</ce:sup> cross-relaxation while also exacerbating surface energy quenching. Beyond mitigating the phonon energy shortage and providing greater shielding for surrounding Ho<ce:sup loc=\"post\">3+</ce:sup> ions, a low Ho<ce:sup loc=\"post\">3+</ce:sup> concentration in the core and a high concentration in the first shell (S<ce:inf loc=\"post\">1</ce:inf>) were found to reduce the overall distance between Yb<ce:sup loc=\"post\">3+</ce:sup> and activated Ho<ce:sup loc=\"post\">3+</ce:sup> ions, enhancing energy transfer but increasing surface quenching. A high Yb<ce:sup loc=\"post\">3+</ce:sup> concentration in the second shell (S<ce:inf loc=\"post\">2</ce:inf>) and a low concentration in the third shell helped to promote inward sensitising energy transfer and suppress surface quenching, though this configuration partially intensified the phonon energy shortage. UCNPs with the composition NaHoF<ce:inf loc=\"post\">4</ce:inf>:10%Ce<ce:sup loc=\"post\">3+</ce:sup>,40%Gd<ce:sup loc=\"post\">3+</ce:sup>@NaHoF<ce:inf loc=\"post\">4</ce:inf>:10%Ce<ce:sup loc=\"post\">3+</ce:sup>@NaGdF<ce:inf loc=\"post\">4</ce:inf>:10%Ce<ce:sup loc=\"post\">3+</ce:sup>,60%Yb<ce:sup loc=\"post\">3+</ce:sup>@NaGdF<ce:inf loc=\"post\">4</ce:inf>:20%Yb<ce:sup loc=\"post\">3+</ce:sup> demonstrated optimal performance, exhibiting a red UCL decay time of 164.97 μs, a green-to-red intensity ratio of 0.43 and a quantum yield of 1.23%. Both metrics declined when Ce<ce:sup loc=\"post\">3+</ce:sup> dopants were confined only to S<ce:inf loc=\"post\">2</ce:inf>. Multi-layer Ce<ce:sup loc=\"post\">3+</ce:sup> doping outperformed configurations with doping limited to the core or S<ce:inf loc=\"post\">1</ce:inf>. Moreover, the emission colour of Ce<ce:sup loc=\"post\">3+</ce:sup>-doped UCNPs remained tunable with variations in pump power. These findings provided valuable theoretical guidance for the design of Ce<ce:sup loc=\"post\">3+</ce:sup>-doped and highly doped UCNPs and enhanced the multifunction potential of NaHoF<ce:inf loc=\"post\">4</ce:inf>-based materials.","PeriodicalId":344,"journal":{"name":"Journal of Alloys and Compounds","volume":"39 1","pages":""},"PeriodicalIF":6.3000,"publicationDate":"2025-06-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Influence of Ho3+ and Yb3+ Concentration Distributions on Ce3+-Fine-Tuned Upconversion Luminescence in Highly Doped Core–Multi-Shell Upconversion Nanoparticles\",\"authors\":\"Ye Kuang, Junhao Xu, Guangli Shi, Tengbo Hu, Xian Wang, Bo Li, Yu Liang, Panpan Qin, Wen Zeng, Hao Wang, Longhai Shen, Yiwei Wang\",\"doi\":\"10.1016/j.jallcom.2025.181927\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Although widely used for Ho-based upconversion luminescence (UCL) fine-tuning of upconversion nanoparticles (UCNPs), Ce<ce:sup loc=\\\"post\\\">3+</ce:sup> doping has lacked comprehensive investigation in core–multi-shell and highly doped structures. Herein, a series of highly doped core–multi-shell UCNPs with Ce<ce:sup loc=\\\"post\\\">3+</ce:sup> doping were synthesised via oleate-based methods. The structures and morphologies were characterised by X-ray diffraction (XRD), transmission emission microscopy (TEM) and elemental mapping, while UCL properties were assessed using emission spectra, decay curves and pump power measurements. The distributions of Ho<ce:sup loc=\\\"post\\\">3+</ce:sup> and Yb<ce:sup loc=\\\"post\\\">3+</ce:sup> concentrations were systematically varied to explore, for the first time, their distinct effects on Ce<ce:sup loc=\\\"post\\\">3+</ce:sup>-mediated UCL fine-tuning. These effects arose from different energy mechanisms and varied with the number of shell layers. A deficiency in phonon energy was found to reduce the efficiency of both Yb<ce:sup loc=\\\"post\\\">3+</ce:sup>–Ho<ce:sup loc=\\\"post\\\">3+</ce:sup> energy transfer and Ho<ce:sup loc=\\\"post\\\">3+</ce:sup>–Ce<ce:sup loc=\\\"post\\\">3+</ce:sup> cross-relaxation while also exacerbating surface energy quenching. Beyond mitigating the phonon energy shortage and providing greater shielding for surrounding Ho<ce:sup loc=\\\"post\\\">3+</ce:sup> ions, a low Ho<ce:sup loc=\\\"post\\\">3+</ce:sup> concentration in the core and a high concentration in the first shell (S<ce:inf loc=\\\"post\\\">1</ce:inf>) were found to reduce the overall distance between Yb<ce:sup loc=\\\"post\\\">3+</ce:sup> and activated Ho<ce:sup loc=\\\"post\\\">3+</ce:sup> ions, enhancing energy transfer but increasing surface quenching. A high Yb<ce:sup loc=\\\"post\\\">3+</ce:sup> concentration in the second shell (S<ce:inf loc=\\\"post\\\">2</ce:inf>) and a low concentration in the third shell helped to promote inward sensitising energy transfer and suppress surface quenching, though this configuration partially intensified the phonon energy shortage. UCNPs with the composition NaHoF<ce:inf loc=\\\"post\\\">4</ce:inf>:10%Ce<ce:sup loc=\\\"post\\\">3+</ce:sup>,40%Gd<ce:sup loc=\\\"post\\\">3+</ce:sup>@NaHoF<ce:inf loc=\\\"post\\\">4</ce:inf>:10%Ce<ce:sup loc=\\\"post\\\">3+</ce:sup>@NaGdF<ce:inf loc=\\\"post\\\">4</ce:inf>:10%Ce<ce:sup loc=\\\"post\\\">3+</ce:sup>,60%Yb<ce:sup loc=\\\"post\\\">3+</ce:sup>@NaGdF<ce:inf loc=\\\"post\\\">4</ce:inf>:20%Yb<ce:sup loc=\\\"post\\\">3+</ce:sup> demonstrated optimal performance, exhibiting a red UCL decay time of 164.97 μs, a green-to-red intensity ratio of 0.43 and a quantum yield of 1.23%. Both metrics declined when Ce<ce:sup loc=\\\"post\\\">3+</ce:sup> dopants were confined only to S<ce:inf loc=\\\"post\\\">2</ce:inf>. Multi-layer Ce<ce:sup loc=\\\"post\\\">3+</ce:sup> doping outperformed configurations with doping limited to the core or S<ce:inf loc=\\\"post\\\">1</ce:inf>. Moreover, the emission colour of Ce<ce:sup loc=\\\"post\\\">3+</ce:sup>-doped UCNPs remained tunable with variations in pump power. These findings provided valuable theoretical guidance for the design of Ce<ce:sup loc=\\\"post\\\">3+</ce:sup>-doped and highly doped UCNPs and enhanced the multifunction potential of NaHoF<ce:inf loc=\\\"post\\\">4</ce:inf>-based materials.\",\"PeriodicalId\":344,\"journal\":{\"name\":\"Journal of Alloys and Compounds\",\"volume\":\"39 1\",\"pages\":\"\"},\"PeriodicalIF\":6.3000,\"publicationDate\":\"2025-06-29\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Alloys and Compounds\",\"FirstCategoryId\":\"88\",\"ListUrlMain\":\"https://doi.org/10.1016/j.jallcom.2025.181927\",\"RegionNum\":2,\"RegionCategory\":\"材料科学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"CHEMISTRY, PHYSICAL\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Alloys and Compounds","FirstCategoryId":"88","ListUrlMain":"https://doi.org/10.1016/j.jallcom.2025.181927","RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"CHEMISTRY, PHYSICAL","Score":null,"Total":0}
Influence of Ho3+ and Yb3+ Concentration Distributions on Ce3+-Fine-Tuned Upconversion Luminescence in Highly Doped Core–Multi-Shell Upconversion Nanoparticles
Although widely used for Ho-based upconversion luminescence (UCL) fine-tuning of upconversion nanoparticles (UCNPs), Ce3+ doping has lacked comprehensive investigation in core–multi-shell and highly doped structures. Herein, a series of highly doped core–multi-shell UCNPs with Ce3+ doping were synthesised via oleate-based methods. The structures and morphologies were characterised by X-ray diffraction (XRD), transmission emission microscopy (TEM) and elemental mapping, while UCL properties were assessed using emission spectra, decay curves and pump power measurements. The distributions of Ho3+ and Yb3+ concentrations were systematically varied to explore, for the first time, their distinct effects on Ce3+-mediated UCL fine-tuning. These effects arose from different energy mechanisms and varied with the number of shell layers. A deficiency in phonon energy was found to reduce the efficiency of both Yb3+–Ho3+ energy transfer and Ho3+–Ce3+ cross-relaxation while also exacerbating surface energy quenching. Beyond mitigating the phonon energy shortage and providing greater shielding for surrounding Ho3+ ions, a low Ho3+ concentration in the core and a high concentration in the first shell (S1) were found to reduce the overall distance between Yb3+ and activated Ho3+ ions, enhancing energy transfer but increasing surface quenching. A high Yb3+ concentration in the second shell (S2) and a low concentration in the third shell helped to promote inward sensitising energy transfer and suppress surface quenching, though this configuration partially intensified the phonon energy shortage. UCNPs with the composition NaHoF4:10%Ce3+,40%Gd3+@NaHoF4:10%Ce3+@NaGdF4:10%Ce3+,60%Yb3+@NaGdF4:20%Yb3+ demonstrated optimal performance, exhibiting a red UCL decay time of 164.97 μs, a green-to-red intensity ratio of 0.43 and a quantum yield of 1.23%. Both metrics declined when Ce3+ dopants were confined only to S2. Multi-layer Ce3+ doping outperformed configurations with doping limited to the core or S1. Moreover, the emission colour of Ce3+-doped UCNPs remained tunable with variations in pump power. These findings provided valuable theoretical guidance for the design of Ce3+-doped and highly doped UCNPs and enhanced the multifunction potential of NaHoF4-based materials.
期刊介绍:
The Journal of Alloys and Compounds is intended to serve as an international medium for the publication of work on solid materials comprising compounds as well as alloys. Its great strength lies in the diversity of discipline which it encompasses, drawing together results from materials science, solid-state chemistry and physics.