无机材料学报 ›› 2026, Vol. 41 ›› Issue (5): 673-680.DOI: 10.15541/jim20250442
• 研究快报 • 上一篇
董浪平1(
), 李施璇1, 杨少星1, 侯京山1, 林燕丹4, 周鹏程5, 孙雪娇3, 孙宜阳3(
), 陈大钦2, 房永征1(
)
收稿日期:2025-11-01
修回日期:2025-12-06
出版日期:2025-12-19
网络出版日期:2025-12-19
通讯作者:
孙宜阳, 研究员. E-mail: yysun@mail.sic.ac.cn;作者简介:董浪平(1993-), 女, 副教授. E-mail: lpdong@sit.edu.cn
DONG Langping1(
), LI Shixuan1, YANG Shaoxing1, HOU Jingshan1, LIN Yandan4, ZHOU Pengcheng5, SUN Xuejiao3, SUN Yiyang3(
), CHEN Daqin2, FANG Yongzheng1(
)
Received:2025-11-01
Revised:2025-12-06
Published:2025-12-19
Online:2025-12-19
Contact:
SUN Yiyang, professor. E-mail: yysun@mail.sic.ac.cn;About author:DONG Langping (1993-), female, associate professor. E-mail: lpdong@sit.edu.cn
Supported by:摘要:
热猝灭是荧光材料在固态照明器件中应用时面临的关键挑战。本研究报道了一种具有抗热猝灭行为的钙钛矿型荧光粉RbZnF3:Eu3+。在紫光激发下, 该荧光粉发出明亮的红光。随着温度升高, 其发光强度先增大(175 ℃, 即抗热猝灭), 随后下降; 当温度高于200 ℃时, 发光强度低于室温值。通过全面表征发现, 抗热猝灭行为主要源于缺陷能级的存在。第一性原理计算表明, Rb空位和F空位可能是形成这些缺陷能级的主要原因。本研究还利用RbZnF3:Eu3+荧光粉制备了白光发光二极管(LED), 验证了其潜在应用价值。
中图分类号:
董浪平, 李施璇, 杨少星, 侯京山, 林燕丹, 周鹏程, 孙雪娇, 孙宜阳, 陈大钦, 房永征. 一种可被紫光激发的红色荧光粉RbZnF3:Eu3+ 中的异常热猝灭现象[J]. 无机材料学报, 2026, 41(5): 673-680.
DONG Langping, LI Shixuan, YANG Shaoxing, HOU Jingshan, LIN Yandan, ZHOU Pengcheng, SUN Xuejiao, SUN Yiyang, CHEN Daqin, FANG Yongzheng. Anomalous Fluorescence Thermal Quenching in a Red-emitting RbZnF3:Eu3+ Phosphor under Violet Excitation[J]. Journal of Inorganic Materials, 2026, 41(5): 673-680.
Fig. 1 Synthesis, phase identification and crystal structure of the RbZnF3:0.13Eu3+ phosphor (a) Schematic diagram of the synthesis process; (b) XRD patterns and enlarged areas at 2θ=25°-35° of the synthesized RbZnF3:xEu3+; (c) Schematic diagram of crystal structure and cation coordination of RbZnF3 matrix
Fig. 2 Photoluminescence, concentration quenching and thermal quenching behavior of RbZnF3:0.13Eu3+ (a) Excitation and (b) emission spectra of RbZnF3:0.13Eu3+; (c) Emission spectra of RbZnF3:xEu3+ samples; (d) Relationship between concentration x and luminescence intensity; (e) Temperature-dependent emission spectra of RbZnF3:0.13Eu3+ sample; (f) Evolution trend of luminescence intensity with increasing temperature
Fig. 3 Investigation of the anti-thermal quenching performance and mechanism in RbZnF3:0.13Eu3+ phosphor (a) Temperature-dependent XRD patterns of RbZnF3:0.13Eu3+ sample; (b) Thermoluminescence curve of RbZnF3:0.13Eu3+ sample at different temperatures; (c-f) Defect forming energy of various defects when the chemical composition is (c) A, (b) B, (c) C, and (d) D points; (g) EPR spectra for RZF and RZF:Eu3+; (h) Schematic illustration of the mechanism for the anti-thermal quenching in RZF:0.13Eu3+ phosphor. Colorful figures are available on website
Fig. 4 Electroluminescence spectrum of WLED produced by 390 nm violet LED chip combining BAM:Eu2+ blue phosphor, (Ba, Sr)2SiO4:Eu2+ green phosphor and prepared RZF:0.13Eu3+ red phosphor Inset: a photo of the fabricated WLED when it is powered on
Fig. S3 Repeated testing of the thermal quenching process in RbZnF3:0.13Eu3+ (a) Thermal-dependent emission spectra of RbZnF3:0.13Eu3+; (b) Evolution of the luminescence intensity as a function of temperature during repeated testing
Fig. S5 Chemical potential and potential chemical composition distribution A and D are extreme composition points rich in Zn, while B and C are extreme composition points rich in F. RbZnF3 can only form within a closed area composed of points A, B, C, and D
Fig. S6 Evaluation of the thermal quenching behavior in RbZnF3:Tb3+ (a) Temperature-dependent emission spectra of RbZnF3:Tb3+ sample; (b) Evolution trend of luminescence intensity with increasing temperature
| Temperature | 25 ℃ | 75 ℃ | 125 ℃ | 175 ℃ |
|---|---|---|---|---|
| Space group | Pm3m(221)-Cubic | |||
| a/Å | 4.1329 | 4.1330 | 4.1369 | 4.1406 |
| α/(º) | 90 | 90 | 90 | 90 |
| V/Å3 | 70.5935 | 70.6140 | 70.7987 | 70.9880 |
| Rwp | 2.67% | 2.69% | 2.29% | 2.33% |
| Rp | 2.11% | 2.13% | 1.86% | 1.89% |
Table S1 Variation of cell parameter of RbZnF3:0.13Eu3+ sample with the increase of temperature
| Temperature | 25 ℃ | 75 ℃ | 125 ℃ | 175 ℃ |
|---|---|---|---|---|
| Space group | Pm3m(221)-Cubic | |||
| a/Å | 4.1329 | 4.1330 | 4.1369 | 4.1406 |
| α/(º) | 90 | 90 | 90 | 90 |
| V/Å3 | 70.5935 | 70.6140 | 70.7987 | 70.9880 |
| Rwp | 2.67% | 2.69% | 2.29% | 2.33% |
| Rp | 2.11% | 2.13% | 1.86% | 1.89% |
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