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中国科学院长春物理研究所
收稿日期:1988-03-14,
纸质出版日期:1989-02-28
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梁力恒, 钟国柱. ZnS:TbF<sub>3</sub>,ErF<sub>3</sub>,HoF<sub>3</sub>ACTFEL的亮度与跃迁几率的关系[J]. 发光学报, 1989,10(1): 30-36
Liang Liheng, Zhong Guozhu. THE RELATIONSHIP BETWEEN ACEL BRIGHTNESS AND TRANSITION PROBABILITIES IN ZnS:TbF<sub>3</sub>,ErF<sub>3</sub>,HoF<sub>3</sub> THIN FILMS[J]. Chinese Journal of Luminescence, 1989,10(1): 30-36
梁力恒, 钟国柱. ZnS:TbF<sub>3</sub>,ErF<sub>3</sub>,HoF<sub>3</sub>ACTFEL的亮度与跃迁几率的关系[J]. 发光学报, 1989,10(1): 30-36 DOI:
Liang Liheng, Zhong Guozhu. THE RELATIONSHIP BETWEEN ACEL BRIGHTNESS AND TRANSITION PROBABILITIES IN ZnS:TbF<sub>3</sub>,ErF<sub>3</sub>,HoF<sub>3</sub> THIN FILMS[J]. Chinese Journal of Luminescence, 1989,10(1): 30-36 DOI:
测量了低浓度下ZnS:TbF
3
ErF
3
和ZnS:TbF
3
HoF
3
交流电致发光薄膜(ACTFEL)中的Tb
3+
Er
3+
HO
3+
主要发射峰的相对积分强度
并与Tb
3+
Er
3+
Ho
3+
主要发射能级的辐射跃迁几率及高浓度时的发光特性进行了比较
发现稀土氟化物掺杂的ZnS薄膜电致发光(ACTFEL)的最大亮度
不完全取决于稀土离予本身的辐射跃迁几率
而主要取决于稀土离子主要发射能级激发态的运动。本文首次给出了Tb
3+
离子在ZnS中的强度参数Ω
2
=3.2×10
-19
cm
2
Ω
4
=1.6×10
-19
cm
2
Ω
6
=2.6×10
-19
cm
2
并应用这组Ω
λ
参数估算了Tb
3+
离子的交叉弛豫(cross-relaxation)几率。
We have measured the integrated intensities of main emission lines for Tb
3+
Er
3+
Ho
3+
ions in ZnS. TbF
3
ErF
3
and ZnS:TbF
3
HoF
3
ACEL thin films (TF) at low concentration
furthermore
compared them with their transition probabilities and their ACEL characteristics at high concentration.It is found that when the concentration is low(-10-4mol)
the concentration quenching process could be neglected and transition probabilities of the main emission energy levels
5
D
4
2
H
11/2
+
4
S
3/2
5
S
2
(
6
F
4
)for Tb
3+
Er
3+
Ho
3+
ions can be determined by decay time. The transition probabilities of
5
D
4
-
7
F
5
2
H
11
/2+
4
S
3
/2-
4
I
15
/2 and
5
S
2
(
5
F
4
)-
5
I
8
are about 5300s
-1
13000s
-1
and 7700s
-1
respectively. In this case
the integrated intensities of main emission lines for Tb
3+
Er
3+
and Ho
3+
in ZnS ACELTF are approximately proportional to the transition probabilities. But the maximum brightness of ACEL in ZnS:Tb
3+
ZnS:Er
3+
and ZnS:Ho
3+
thin films is about 2300cd/m
2
1100cd/m
2
and 500cd/m
2
respectively. Therefore
the maximum brightness of ACEL in ZnS thin films doped with rare earth fluorides is not determined completely by the transition probability of rare earth ions themselves
but mainly depends on the concentration quenching process dominated by the cross-relaxation process of main emission energy level of rare earth ions.In the present paper
the intensity parameters for Tb
3+
in ZnS thin film have been obtained for the first time. They are Ω
2
=3.2×10
-19
cm
2
Ω
4
=1.6×10
19
cm
2
. Ω
6
=2.6×10
19
cm
2
. They have been used to estimate the cross-relaxation probability between Tb
3+
ions. The calculated result is in agreement with the experimental observation.
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