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

IF 2.4 3区 化学 Q2 CHEMISTRY, MULTIDISCIPLINARY CrystEngComm Pub Date : 2024-10-03 DOI:10.1039/D4CE00844H
Kan Lu, Qifan Zhang, Juan Kong, Yan Hao, Wenxia Wu, Yazhao Wang, Haibo Lin, Shoulei Xu and Wen Deng
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引用次数: 0

摘要

首次采用 OFZ(光学浮区)方法制备了高质量的透明立方镥稳定氧化锆(LSZ)和 LSZ:Yb0.25Tm0.5Ho0.03 单晶体。为了进行比较,还制作了 YSZ 和 YSZ:Yb0.25Tm0.5Ho0.03 单晶。在可见光区域,LSZ 单晶的透射率(80.7%)略低于 YSZ 单晶的透射率(86.3%),这是因为 LSZ 单晶的密度(6.604 g cm-3)高于 YSZ 单晶的密度(5.973 g cm-3)。在 LSZ 和 YSZ 的透射和吸收光谱中,200-1100 纳米范围内均未观察到吸收峰,这表明这两种晶体都是优良的主晶。LSZ:Yb0.25Tm0.5Ho0.03 单晶的密度(6.596 g cm-3)也高于 YSZ:Yb0.25Tm0.5Ho0.03 单晶的密度(6.005 g cm-3)。LSZ:Yb0.25Tm0.5Ho0.03 和 YSZ:Yb0.25Tm0.5Ho0.03 单晶的吸收光谱在 363、453、678 和 785 纳米波长处有几个吸收峰,在 850-1000 纳米波长处有一个很宽的吸收带。在 980 纳米波长下激发的 LSZ:Yb0.25Tm0.5Ho0.03 单晶的上转换光致发光(UCPL)光谱在 308、373、488、540、550、655 和 794 纳米波长处显示出几个发射峰;在 YSZ:Yb0.25Tm0.5Ho0.03 单晶的 UCPL 光谱中也观察到类似的发射峰。前者的发射峰强度高于后者的相应峰强度,这是由于前者与后者相比具有更高的密度和更低的声子能量。功率曲线表明,308 和 373 nm 发射属于 4 光子上转换过程,488 nm 发射属于 3 光子过程,540 nm 和 655 nm 发射属于 2 光子过程。这些结果表明,在 980 纳米波长的激发下,LSZ:Yb0.25Tm0.5Ho0.03 单晶的紫外线和可见光发射效率高于 YSZ:Yb0.25Tm0.5Ho0.03 单晶。
本文章由计算机程序翻译,如有差异,请以英文原文为准。

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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.

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来源期刊
CrystEngComm
CrystEngComm 化学-化学综合
CiteScore
5.50
自引率
9.70%
发文量
747
审稿时长
1.7 months
期刊介绍: Design and understanding of solid-state and crystalline materials
期刊最新文献
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