Synthesis and Structural Features of Tunable Emitting Single-Phased Eu3+/Tb3+ Co-Doped LaAlO3 Nanophosphors

IF 1.2 4区 化学 Q4 CHEMISTRY, INORGANIC & NUCLEAR Journal of Structural Chemistry Pub Date : 2024-09-04 DOI:10.1134/S0022476624080080
D. Dhaterwal, M. Matoria, A. Dalal, S. Kumar, S. Singh
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Abstract

In the prevailing study, single-phased color-tunable La1–x–yEuxTbyAlO3 co-doped nanocrystalline phosphors have been synthesized via the most simplistic and low-cost urea-aided solution combustion synthetic route. This was done by adjusting the doping concentration of Eu3+ (x = 0.01 mol, 0.03 mol, 0.05 mol, 0.07 mol) and Tb3+ (y = 0.03 mol) ions in the LaAlO3 host lattice. The X-ray powder diffraction (XRD) and Rietveld refinement analysis confirmed the formation of single-phased La0.97–xAlO3:xEu3+/0.03Tb3+ (x = 0.07), co-doped nanophosphor at 800 °C. The synthesized nanophosphors were crystallized in cubic crystal system having \(Pm\overline{3}m\) space group with 221 space group number. The morphological studies, i.e. field emission scanning electron microscopy (FE-SEM), and transmission electron microscope (TEM) images depicted the agglomerated clusters of distinct spherical shaped particles of La0.97–xAlO3:xEu3+/0.03Tb3+ in nano-regime. Energy dispersive X-ray analysis (EDAX) was employed to ascertain the real elemental mapping of the fabricated phosphors. Through diffuse reflectance (DR) spectroscopy measurements, the optical band gap value for La0.92Eu0.05Tb0.03AlO3 nanocrystalline phosphor was determined to be 5.26 eV. The photoluminescent excitation (PLE) and photoluminescent emission (PL) spectra were studied in detail as a function of Eu3+ ion contents and La1–x–0.03AlO3:xEu3+/0.03Tb3+ (x = 0.05 mol) co-doped sample exhibits strongest emission and over the 0.05 Eu3+ ions doping concentration, the emission intensity falls as a consequence of the quenching phenomenon. The concentration quenching in directed co-doped nanophosphors was attributed to the dipole-dipole interactions. With the exploitation of photoluminescent data, Commission International de I′Eclairage 1931 (CIE) color coordinates (x, y) of co-doped samples have been calculated from the emission spectra, which revealed the color could be tuned i.e., from orange to red region in La0.97–xAlO3:xEu3+/0.03Tb3+ samples with divergences in the Eu3+ and other significant photometric assets viz. correlated color temperature (CCT), color purity (CP) of the synthesized La1–x–yAlO3:xEu3+, yTb3+ co-doped nanocrystalline photoluminescent materials were also determined. The studies outcomes suggested that Eu3+/Tb3+ co-doped LaAlO3 phosphors have great potential as color-tunable luminescent material in solid-state lighting and display technologies.

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可调谐发射单相 Eu3+/Tb3+ 共掺 LaAlO3 纳米荧光粉的合成与结构特征
摘要 在当前的研究中,通过最简单和低成本的尿素辅助溶液燃烧合成路线,合成了单相颜色可调的 La1-x-yEuxTbyAlO3 共掺杂纳米晶荧光粉。这是通过调整 Eu3+(x = 0.01 mol、0.03 mol、0.05 mol、0.07 mol)和 Tb3+(y = 0.03 mol)离子在 LaAlO3 主晶格中的掺杂浓度实现的。X 射线粉末衍射 (XRD) 和里特维尔德细化分析证实,在 800 °C 下形成了单相 La0.97-xAlO3:xEu3+/0.03Tb3+ (x = 0.07) 共掺杂纳米磷。合成的纳米磷在立方晶系中结晶,具有221空间群数的\(Pm\overline{3}m\)空间群。形态学研究,即场发射扫描电子显微镜(FE-SEM)和透射电子显微镜(TEM)图像显示,La0.97-xAlO3:xEu3+/0.03Tb3+在纳米状态下由明显的球形颗粒团聚而成。能量色散 X 射线分析(EDAX)被用来确定所制造荧光粉的真实元素图谱。通过漫反射(DR)光谱测量,确定了 La0.92Eu0.05Tb0.03AlO3 纳米晶荧光粉的光带隙值为 5.26 eV。详细研究了光致发光激发(PLE)和光致发光发射(PL)光谱与 Eu3+ 离子含量的函数关系,共掺杂 La1-x-0.03AlO3:xEu3+/0.03Tb3+ (x = 0.05 mol) 的样品表现出最强的发射,当 Eu3+ 离子掺杂浓度超过 0.05 时,由于淬火现象,发射强度下降。定向共掺杂纳米磷酸盐中的浓度淬灭归因于偶极-偶极相互作用。利用光致发光数据,从发射光谱中计算出了共掺杂样品的国际照明委员会(CIE)色坐标(x, y)、此外,还测定了合成的 La1-x-yAlO3:xEu3+, yTb3+ 共掺杂纳米晶体光致发光材料的其他重要光度资产,即相关色温(CCT)、色纯度(CP)。研究结果表明,Eu3+/Tb3+共掺杂LaAlO3荧光粉在固态照明和显示技术中作为颜色可调的发光材料具有巨大的潜力。
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来源期刊
Journal of Structural Chemistry
Journal of Structural Chemistry 化学-无机化学与核化学
CiteScore
1.60
自引率
12.50%
发文量
142
审稿时长
8.3 months
期刊介绍: Journal is an interdisciplinary publication covering all aspects of structural chemistry, including the theory of molecular structure and chemical bond; the use of physical methods to study the electronic and spatial structure of chemical species; structural features of liquids, solutions, surfaces, supramolecular systems, nano- and solid materials; and the crystal structure of solids.
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