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1. 中国科学技术大学物理系, 安徽合肥 230026
2. 中国科学技术大学国家同步辐射实验室,安徽 合肥,230029
收稿日期:2000-03-22,
修回日期:2000-12-05,
纸质出版日期:2001-05-30
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刘波, 施朝淑, 张庆礼. GdVO<sub>4</sub>:Eu<sup>3+</sup>发光的温度效应[J]. 发光学报, 2001,22(2): 111-114
LIU Bo, SHI Chao-shu, ZHANG Qing-li. Temperature Effect of GdVO<sub>4</sub>:Eu<sup>3+</sup> Luminescence[J]. Chinese Journal of Luminescence, 2001,22(2): 111-114
研究了GdVO
4
:Eu
3+
在高压汞灯的313和365nm激发下室温以上(300~600K)发光的温度依赖关系。发现来自
5
D
0
的发射强度随温度的升高而显著增强
直到600K也未见饱和。其中
5
D
0
7
f
2
的619nm发射在600K温度时的强度是室温下的20多倍。我们认为Eu
3+
的电荷迁移态作为中间态是造成其发光增强的根本原因。激发过程中
先激发到Eu
3+
本身的
5
D
J
(J=1
2
3)激发态
然后在温度的作用下上升到电荷迁移态(CTS)
温度升高时传递几率显著增强
并按
5
D
3
5
D
2
5
D
1
依次使被激发的电子转入CTS态
从电荷迁移态直接弛豫传递给
5
D
0
态
由于
5
D
0
态电子数不断增多
致使来自5D0的发射随温度升高而增强。
The temperature dependence of GdVO
4
:Eu
3+
luminescence from Eu
3+
5
D
0
7
F
J
transition excited by 313 and 365nm of high pressure mercury lamp above room temperature has been studied including the emission spectra at different temperature and the emission intensity of Eu
3+
as function of temperature.In addition
the excitation spectrum of GdVO
4
:Eu
3+
with emission wavelength 619nm at RT was measured. The characteristic emissions of Eu
3+
were observed
including 608
616
619nm of
5
D
0
7
F
2
transition
594
598nm of
5
D
0
7
F
1
transition and 538nm of
5
D
1
7
F
1
transition.Each of them increases with rising temperature.And the relative intensity of the emission lines maintains constant each other.In the range of 300~600K
each emission line increases as temperature rises
especially above 400K
and there is a rapid increase without intensity saturation up to 600K.The emission intensity at 600K is twenties time stronger than that at 300K.We observed that the excitation spectrum of 619nm emission contains two main excitation bands peaked at about 250 and 310nm
beside the intrinsic excitation of Eu
3+
.But the intensity of intrinsic excitation is weaker than that of the excitation bands at 250
310nm. When Eu
3+
is excited by 365nm which is Eu
3+
intrinsic excitation
there are two ways to deplete its energy.One is cascade down to
5
D
J
states according to the order of
5
D
3
5
D
2
5
D
1
5
D
0
.The other is to be promoted thermally to charge transfer state and sequentially to feed
5
D
0
without passing by cascade from higher
5
D state by which
5
D
0
can be excited more effectively.The possibility of the latter process depends on temperature intensively.Therefore
when temperature rises
more Eu
3+
can be excited into
5
D
0
.Using this model the experimental result can be explained reasonably.If Eu
3+
is excited by 313nm which can be the sorption by VO
4
3-
it can also be promoted thermally into charge transfer state. In conclusion
the intensity of the luminescence excited by 313
365nm increases rapidly as temperature rises up to 600K.The CTS of Eu
3+
as a middle state plays an important role which can make the excitation energy transfer to
5
D
0
effectively.Such process is more remarkable when the temperature rises.With high temperature property
GdVO
4
:Eu can be used in high temperature environment.
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