# Synthesis and Luminescence Properties of SrGd2O4:Eu3+ Red Phosphors

Authors: Jun-Feng Wang; Hao Zu; Chuan-Wen Lin; Shou-Jun Ding; Peng-Yu Shao; Ye Xia
Journal: International Journal of Optics
 (2020)

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## Abstract

As one of the important raw materials for LED products, phosphors play an important role. At present, the spectrum of LED phosphors lacks red light, resulting in poor quality of white LED products and a low color rendering index (Ra <80), which affects lighting effects. To solve this problem, we synthesized the SrGd2O4:Eu3+ red phosphor by a high-temperature solid-phase method. The structure and luminescence properties of SrGd2O4:Eu3+ red phosphors were studied by means of X-ray diffraction (XRD) measurements of their emission and excitation spectra, and their spectra were analyzed. We also studied the Eu3+ doping concentration with the best luminous efficiency and the color coordinate of the SrGd2O4:Eu3+ phosphor. The experimental results show that SrGd2O4:Eu3+ is a new red phosphor material that can be used for near-ultraviolet or blue-light excitation and has good practicability.


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## Body

## 1. Introduction

With the global climate change and the background of energy crisis, the awareness of environmental protection and energy conservation is becoming more and more important. Because LED (light-emitting diode) has the advantages of durability, energy conservation, fast response, compactness, strong anti-interference ability, high brightness, no mercury pollution, and environmental protection, it is becoming a trend in lighting [1, 2].The way in which the LED realizes white light is mainly by mixing a light-emitting chip and phosphors that can be activated by the light-emitting chip. Since the phosphor degrades during use and affects the quality of light, the phosphor material is the key to ensuring the quality of LED products [3]. Commercially produced white LEDs require red phosphors to be added to compensate for the lacking of red light components [4, 5].The currently used red phosphors remain at the traditional level of rare earth ion-activated sulfide substrates, and their synthesis and application generally have the following problems: (1) The optimal excitation wavelength of the red phosphor cannot closely match with the emission wavelength of the blue chip, resulting in a low red light excitation rate [5, 6]. (2) The red phosphor itself has low luminous efficiency and poor application effect [7]. (3) When the red phosphor is effectively excited, its emission spectrum range is narrow, and the compensation effect on light is poor [8, 9]. (4) Whether the matching of the red phosphor matrix with the widely used yellow phosphor matrix affects the respective luminescence interaction remains to be studied. In addition, conventional red fluorescence based on sulfide substrates may produce toxic substances during the synthesis process [10–12].Recently, the investigation of red phosphor matrix is mainly divided into the following types: (1) nitride or nitrogen oxide matrix, which has excellent thermal stability, chemical stability, and good controllability; it has been widely studied, and Eu2+ is usually used as an activating ion. However, the requirements for the preparation conditions of the nitride red phosphor are very strict, generally high temperature up to 1400°C∼2000°C, long-term insulation, and need to be protected under nitrogen. This will inevitably increase the cost of the phosphor and consume a lot of resources, which is a disadvantage for commercial production [13, 14]. (2) Borate matrix, which is easy to synthesize and stable in physical and chemical properties. However, it has shortcomings such as short emission wavelength and serious aging phenomenon [15]. (3) Silicate matrix, which has good light permeability, high luminous efficiency, and low production cost, but the silicate itself has poor chemical stability, and it is necessary to study whether it can widely use white LED [16]. (4) Aluminate matrix, which has a high quantum conversion rate and the color of the light is stable [17]. However, there are few research reports on the red phosphor of the matrix.In summary, the traditional commercial phosphors CaS:Eu3+, Y2O2S:Eu3+ et al have shortcomings such as low luminous efficiency, poor stability and short life [18, 19]. Recently, researchers are exploring new red phosphor materials to study the effects of different matrices and different doping ions on the luminescence properties of fluorescent materials [20–22]. It can be foreseen that the luminescent properties of red phosphors will be making big progress. In this study, SrGd2O4 was chosen as the new luminescent matrix material. The SrGd2O4:Eu3+ phosphor was synthesized by a high-temperature solid-phase method, and the relationship between luminescence properties and concentration was explored.


## 2. Principle and Experiment

Fluorescence is a process that produces light with little heat compared to thermal radiation. A suitable material absorbs high-energy radiation, which in turn emits light, the energy of which is lower than the energy of the excitation radiation. When the luminescent material is a solid, the material is commonly referred to as a phosphor. The high-energy radiation that excites the phosphor may be electrons or ions with high velocity, or photons ranging from gamma rays to visible light.Figure1 shows the unit cell structure of SrGd2O4. It can be seen from the figure that strontium is equipped with six oxygen atoms in a unit cell to form a triangular prism, which is in the center of inversion symmetry. The gadolinium is equipped with six oxygens in one unit cell to form an octahedron in the center of noninversion symmetry.Figure 1
The cell structure of SrGd2O4.In this work, SrGd2O4:Eu3+ phosphors were synthesized by the high-temperature solid-phase method. The raw materials Eu2O3, Gd2O3, and SrCO3 were weighed accurately according to stoichiometric ratios. The doping concentrations of Eu3+ are 1%, 2%, 5%, 10%, and 15%, respectively. The agate mortar was wiped with alcohol cotton, and the raw materials were separately mixed in a mortar, and each group was thoroughly ground for 30 minutes. Then, the ground mixtures were loaded in a clean crucible and placed in a furnace. The reaction temperature and time were set as 1400°C and 48 hours, respectively. Lastly, the samples were cooled down to room temperature naturally and thoroughly ground.A Philips X' pert Pro X-ray powder diffractometer equipped with Cu Kα radiation was employed to determine the crystal structure. In the measured 2θ range (10° to 90°), the scan step was set as 0.033°. An Edinburgh FLSP-920 spectrometer was used to measure the excitation and emission spectra of the samples. The international CIE 1931 standard chromaticity system was used to draw the chromaticity coordinate diagram of the phosphor.


## 3. Results and Discussion

Figure2 shows the XRD pattern of the as-synthesized SrGd2O4:Eu3+ phosphors with different Eu3+ doping concentrations (1%–15%). Compared with the data from the standard card of SrGd2O4 (card number: ICSD#150876), the as-synthesized samples are coincident well with them, indicating that the structure of SrGd2O4 is unaffected by the doping of Eu3+. In addition, the diffraction peaks of the synthesized samples with different concentrations are symmetrical and sharp, indicating that the as-synthesized samples are well crystalline.Figure 2
The XRD patterns of (1 at%, 5 at%, and 15 at%) SrLa2O4:Eu3+.Figure3 shows the excitation spectrum of the 2 at% Eu3+ doped SrGd2O4 phosphor at room temperature. The excitation spectrum of the sample consists of a series of peaks. In the wavelength range of 240 nm to 330 nm, charge transfer of O2-⟶Eu3+ is generated, and the charge migrates from the 2p orbital of O2− to the 4f orbital of the central metal ion Eu3+. The Eu3+ samples also have strong excitation peaks at 370 nm, 380 nm, and 400 nm, respectively. 7D0⟶5D4 transitions occur around 370 nm, 7D0⟶5G2 transitions occur around 380 nm, and 7D0⟶5L6 transitions occur around 400 nm. It shows that the phosphor can be effectively excited by near-ultraviolet light and blue light, so it can be used as a red phosphor component excited by the near-ultraviolet LED chip and blue LED chip.Figure 3
The excitation spectra of (1 at%) SrGd2O4:Eu3+ phosphor.Figure4 shows the emission spectra of SrGd2O4 : Eu3+ phosphors with different doping concentrations at room temperature. A series of emission peaks are observed in the wavelength range of 580 nm to 720 nm, which are corresponding to the transitions of 5D0⟶7F1 (orange emission), 7F2 (orange emission), 7F3 (red emission), and 7F4 (red emission), respectively, as denoted in the figure. According to the unit cell structure SrGd2O4 (Figure 2), the gadolinium is in the noninversion symmetry center plus considering the charge balance and radius similarity. It can be concluded that Eu3+ is most likely to replace Gd3+, which coincides with the XRD characterization structure.Figure 4
The emission spectra of SrGd2O4 : Eu3+ phosphors with different doping concentrations.Figure5 shows the emission peak intensity at different doping concentrations of the SrGd2O4:Eu3+ phosphor at room temperature. It can be seen that with the increase of Eu3+ doping concentration, the luminescence intensity of the samples firstly increases and then weakens. When the doping concentration is between 1% and 5%, the luminescence effect of the phosphor can be greatly improved by incorporating Eu3+. This is because when the concentration of Eu3+ is low, it is not possible to form a sufficient luminescent center and the luminescence intensity is not high. When the doping concentration is 5%, the luminescence intensity reaches a peak, and then as the doping concentration increases (5% to 15%), the luminescence intensity decreases and concentration quenching occurs. This is because when the Eu3+ concentration exceeds a certain range, the interaction force between Eu3+ and Eu3+ is enhanced, which leads to energy transfer efficiency exceeding the energy emission probability, and energy loss is caused by lattice migration.Figure 5
The emission peak intensity value of the SrGd2O4 : Eu3+ phosphor with different doping concentrations.The international CIE 1931 standard chromaticity system is a two-dimensional planar CIE chromaticity diagram represented by a nominal value (X, Y), where X represents the red component and Y represents the green component. Figure 6 represents a color coordinate diagram of the SrGd2O4:Eu3+ phosphor. It can be seen from the figure that a strong red light is emitted at 611 nm under the excitation of 396 nm excitation light, and the color coordinates at this time are (0.62 and 0.3791).Figure 6
The CIE coordinate diagram of the SrGd2O4:Eu3+ phosphor.


## 4. Conclusion

In this work, SrGd2O4:Eu3+ phosphors were successfully prepared by the high-temperature solid-phase method. By studying its spectral analysis and luminescence properties, the following conclusions can be drawn: (1) the XRD pattern analysis showed that the SrGd2O4:Eu3+ crystal synthesized in the laboratory has good structure, and the Eu3+ doping has little effect on the lattice parameter of SrGd2O4. (2) When the Eu3+ doping concentration is 5%, the SrGd2O4:Eu3+ phosphor has the highest luminescence intensity. (3) The SrGd2O4:Eu3+ phosphor emits intense red light at 611 nm under the excitation of 267 nm excitation light, and the color coordinates are (0.62 and 0.3791). (4) By analyzing the excitation and emission spectroscopy of the SrGd2O4:Eu3+ phosphor, the phosphor can be used together with near-ultraviolet LED chip and blue LED chip to realize white light illumination. In summary, it can be determined that SrGd2O4:Eu3+ is a new red phosphor material that can be used for near-ultraviolet or blue-light excitation and has a good effect.



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