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1. 中国科学院长春应用化学研究所, 稀土化学与物理开放实验室,吉林 长春,130022
2. 中山大学超快速激光国家重点实验室, 中山大学, 化学与化学工程学院,广东 广州,510275
收稿日期:2001-09-20,
修回日期:2002-03-11,
纸质出版日期:2002-05-20
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李成宇, 王淑彬, 于英宁, 苏锵. Eu<sup>2+</sup>,Dy<sup>3+</sup>共掺杂硼铝锶长余辉玻璃陶瓷[J]. 发光学报, 2002,23(3): 233-237
LI Cheng-yu, WANG Shu-bin, YU Ying-ning, SU Qiang. Long-lasting Phosphorescence in Eu<sup>2+</sup>,Dy<sup>3+</sup> Co-doped Strontium Aluminoborate Glass-ceramic[J]. Chinese Journal of Luminescence, 2002,23(3): 233-237
李成宇, 王淑彬, 于英宁, 苏锵. Eu<sup>2+</sup>,Dy<sup>3+</sup>共掺杂硼铝锶长余辉玻璃陶瓷[J]. 发光学报, 2002,23(3): 233-237 DOI:
LI Cheng-yu, WANG Shu-bin, YU Ying-ning, SU Qiang. Long-lasting Phosphorescence in Eu<sup>2+</sup>,Dy<sup>3+</sup> Co-doped Strontium Aluminoborate Glass-ceramic[J]. Chinese Journal of Luminescence, 2002,23(3): 233-237 DOI:
首次介绍了一种新型长余辉材料:Eu
2+
Dy
3+
共掺杂硼铝锶长余辉玻璃陶瓷
该玻璃陶瓷用紫外灯、日光、荧光灯均可激发
发射黄绿色余辉
余辉的发射峰位于516nm
来自于Eu
2+
的5d
→
8
S
7/2
跃迁。用12000lx的荧光灯激发样品20分钟
停止激发后10秒时
该玻璃陶瓷的余辉亮度为353cd/m
2
色坐标为:
x
=02842
y
=05772;停止激发后5小时55分钟
该玻璃陶瓷的余辉亮度为001cd/m
2
;停止激发30小时后
余辉在黑暗中仍肉眼可见。文中对该玻璃陶瓷的相关性质进行了表征
并提出了可能的长余辉机理。
Because glasses have particular properties
for example it is easy to be fabricated into products with various shape in the range from bulk plate to fine fiber
and many key optoelectronic components
e.g.
amplifier
display and storage devices etc.are made of glass with special optical properties
therefore we think the studies on long lasting phosphorescent (LLP) glasses and glass ceramics are important in views of not only the traditional application of LLP materials
but researching of new optoelectronic materials and devices.This article introduces the study on a new kind of LLP material:Eu
2+
Dy
3+
co-doped strontium aluminoborate glass-ceramic with a composition of 29% B
2
O
3
28% Al
2
O
3
43% SrCO
3
0.1% Eu
2
O
3
and 0.1% Dy
2
O
3
(mol%).TransparentEu
2+
Dy
3+
co-doped strontium aluminoborate glass with the same composition was synthesized under a CO atmosphere at 1550℃ which didn’temit LLP
however
opaque glass-ceramic with LLP phenomenon was formed by appropriate heat-treatment to glass.The XRD and infrared analysis show that the main microcrystalline phase in the sample is SrAl
2
O
4
.The excitation spectrum of the sample shows a broad band peaking at about 366nm which is due to the f→d transition of divalent europium; the emission spectrum is alike with the long lasting phosphrescent spectrum
showing a band which peaks at 516nm attributed to 5d→
8
S
7/2
transition of divalent europium.Thus the LLP of the sample is due to the characteristic emission of Eu
2+
ion.The thermoluminescence spectrum consists of three Gaussian fitted components
which may indicate there exist three kinds of traps.When the glass ceramic is irradiated with fluorescent lamp with a power density of 1.2×10
4
lx for 20 minutes
the luminance of the sample is 3.53cd/m
2
10 seconds after stopping the irradiation
the chromaticity coordinates are
x
=0.2842
y
=0.5772.After 5 hours of the irradiation
the sample still has a luminance of 0.01cd/m
2
.The phosphorescence can be seen in dark even 30 hours after the irradiation.The decay of the luminescence is a complex process that consists of three parts: a fast decay
a intermidate and a long decay process.We considered that the formation of SrAl
2
O
4
micro crystal was essential for the LLP of glass ceramic
it was very possible that Eu
2+
and Dy
3+
ions were incorporated in the SrAl
2
O
4
micro crystal
thus the LLP of glass ceramic was emitted by Eu
2+
Dy
3+
co-doped SrAl
2
O
4
micro crystal.However
directly proof showing the formation of SrAl
2
O
4
:Eu
2+
Dy
3+
was absent.We suggest the LLP is due to the recombination of trapped holes and electrons which
c
an be thermally released from trapping centers at room temperature.However
further studied should be carried on the mechanism of the LLP of Eu
2+
Dy
3+
co-doped strontium aluminoborate glass ceramic
as well as the relationship between the treatment processing of glass ceramic and its phosphorescent properties.
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