Effects of Li+, Na+, and K+ doping on the microstructure, fluorescence thermometry, and thermochromism of Ho3+,Yb3+:Bi2WO6 materials†

IF 5.1 2区 材料科学 Q2 MATERIALS SCIENCE, MULTIDISCIPLINARY
Mengliang Jiang, Linxiang Wang, Munire Maimaiti, Xin Feng, Yan Zhang and Jiachen Shi
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引用次数: 0

Abstract

Luminescent materials with 1% M, 3% Ho3+, and 10% Yb3+:Bi2WO6 (M = Li+, Na+, K+) upconversion ability were prepared by a high-temperature solid-phase method. The band structure and density of states of the synthesized material were calculated using density functional theory, and the UV visible absorption spectrum of the synthesized material was measured experimentally. Theoretical calculations and experimental results both indicated that, compared with the Bi2WO6 substrate, doping with Ho3+/Yb3+ or continuing to be doped with M+ (M = Li+, Na+, K+) gradually reduced the bandgap of the material. The bandgap was reduced, and the material could absorb photons with lower energy, which was beneficial for the absorption of infrared photons. X-ray diffraction experiments revealed that Li+, Na+, K+, Ho3+ and Yb3+ doping had no effect on the orthorhombic crystal structure of the Bi2WO6 matrix. For 1% M, 3% Ho3+, and 10% Yb3+:Bi2WO6 (M = Na+, K+), scanning electron micrographs revealed that the powder sample particle size ranged from 1–3 μm, and energy-dispersive spectroscopy (EDS) maps revealed that all the elements were relatively uniformly distributed in the samples. The fluorescence intensity ratio of the Ho3+ emission peaks (I756nm/I538nm) was used for temperature characterization. The maximum relative thermometric sensitivities of 3% Ho3+, 10% Yb3+:Bi2WO6 doped with Li+, Na+, or K+ in the 298–573 K temperature range were 1.69% K−1 (348 K), 2.54% K−1 (298 K), and 2.65% K−1 (298 K), and the minimum temperature resolutions were 0.14 K (323 K), 0.05 K (298 K), and 0.04 K (298 K), respectively. Under 980 nm excitation from 298 K to 573 K, the luminescence of the samples not doped with Li+, Na+, or K+ changed from yellow–green to yellow and then red, whereas the Li+, Na+, or K+-doped sample luminescence colors all changed from green to yellow, orange, and finally red, with the K+-doped samples having the slowest rate of change to red. The luminescent colors of all the samples were reversible during the cooling process within the same temperature range, indicating that the synthesized samples have potential applications in thermochromism and optical anticounterfeiting.

Abstract Image

Li+, Na+和K+掺杂对Ho3+,Yb3+:Bi2WO6材料微观结构、荧光测温和热致变色的影响
采用高温固相法制备了具有1% M、3% Ho3+和10% Yb3+:Bi2WO6 (M = Li+, Na+, K+)上转换能力的发光材料。利用密度泛函理论计算了合成材料的能带结构和态密度,实验测量了合成材料的紫外可见吸收光谱。理论计算和实验结果均表明,与Bi2WO6衬底相比,掺杂Ho3+/Yb3+或继续掺杂M+ (M = Li+, Na+, K+)会逐渐减小材料的带隙。带隙减小,材料能吸收较低能量的光子,有利于红外光子的吸收。x射线衍射实验表明,Li+、Na+、K+、Ho3+和Yb3+的掺杂对Bi2WO6基体的正交晶型结构没有影响。对于1% M、3% Ho3+和10% Yb3+:Bi2WO6 (M = Na+, K+),扫描电镜显示粉末样品的粒径范围在1 ~ 3 μm之间,能谱图显示所有元素在样品中的分布相对均匀。用Ho3+发射峰的荧光强度比(I756nm/I538nm)进行温度表征。在298 ~ 573 K温度范围内,掺Li+、Na+或K+的3% Ho3+、10% Yb3+:Bi2WO6的最大相对温度灵敏度分别为1.69% K−1 (348 K)、2.54% K−1 (298 K)和2.65% K−1 (298 K),最小温度分辨率分别为0.14 K (323 K)、0.05 K (298 K)和0.04 K (298 K)。在298 ~ 573 K的980 nm激发下,未掺杂Li+、Na+、K+的样品的发光颜色由黄绿色变为黄色再变为红色,而掺杂Li+、Na+、K+的样品的发光颜色均由绿色变为黄色、橙色,最后变为红色,其中掺杂K+的样品的变红速度最慢。在相同的温度范围内,所有样品的发光颜色在冷却过程中都是可逆的,这表明合成的样品在热变色和光学防伪方面具有潜在的应用前景。
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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来源期刊
Journal of Materials Chemistry C
Journal of Materials Chemistry C MATERIALS SCIENCE, MULTIDISCIPLINARY-PHYSICS, APPLIED
CiteScore
10.80
自引率
6.20%
发文量
1468
期刊介绍: The Journal of Materials Chemistry is divided into three distinct sections, A, B, and C, each catering to specific applications of the materials under study: Journal of Materials Chemistry A focuses primarily on materials intended for applications in energy and sustainability. Journal of Materials Chemistry B specializes in materials designed for applications in biology and medicine. Journal of Materials Chemistry C is dedicated to materials suitable for applications in optical, magnetic, and electronic devices. Example topic areas within the scope of Journal of Materials Chemistry C are listed below. This list is neither exhaustive nor exclusive. Bioelectronics Conductors Detectors Dielectrics Displays Ferroelectrics Lasers LEDs Lighting Liquid crystals Memory Metamaterials Multiferroics Photonics Photovoltaics Semiconductors Sensors Single molecule conductors Spintronics Superconductors Thermoelectrics Topological insulators Transistors
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