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1. 中国科学技术大学物理系稀土发光实验室,安徽 合肥,230026
2. 福建师范大学物光学院,福建 福州,350007
收稿日期:2007-08-25,
修回日期:2007-11-24,
纸质出版日期:2008-01-20
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秦丽芳, 侯延冰, 师全民, 蒋婧思, 高瑞, 王琰. 电场诱导空穴注入缓冲层PEDOT:PSS取向对OLED发光性能的影响[J]. 发光学报, 2008,29(1): 41-45
QIN Li-fang, HOU Yan-Bing, SHI Quan-min, JIANG Jing-si, GAO Rui, WANG Yan. High-electric-field Treated PEDOT:PSS as Hole Injecting Buffer Layer for Polymer Light-emitting Diodes[J]. Chinese Journal of Luminescence, 2008,29(1): 41-45
秦丽芳, 侯延冰, 师全民, 蒋婧思, 高瑞, 王琰. 电场诱导空穴注入缓冲层PEDOT:PSS取向对OLED发光性能的影响[J]. 发光学报, 2008,29(1): 41-45 DOI:
QIN Li-fang, HOU Yan-Bing, SHI Quan-min, JIANG Jing-si, GAO Rui, WANG Yan. High-electric-field Treated PEDOT:PSS as Hole Injecting Buffer Layer for Polymer Light-emitting Diodes[J]. Chinese Journal of Luminescence, 2008,29(1): 41-45 DOI:
用高温固相法合成了红色长余辉发光材料LiAl
5
O
8
:Mn
4+
Li
5
AlO
4
:Mn
4+
LiAlO
2
:Mn
4+
发现前两种材料有红色余辉
这方面并没有报道过
并对这两种材料的发光性能作了研究
指明了不同基质中发光强弱不同原因。对不同Mn
4+
掺杂浓度的材料做了浓度依赖关系研究
确认Mn
4+
的发光是
2
E→
4
A
2
的跃迁。Mn
4+
的发光是个宽带谱
材料在紫外区有强的吸收
发射谱范围可达620~770nm
峰值在675nm。对长余辉机制进行了探讨。
As a new generation of long afterglow phosphors
rare earth doped aluminates are drawing more and more attention. However
though the blue and the green phosphors with excellent afterglow performance are put into commercial use
the red afterglow phosphor doped with Dy
3+
or Tb
3+
suitable for illuminating is still dissatisfied with the white afterglow phosphor. We developed a new way to meet the conditions of red afterglow phosphor: aluminates doped with Mn
4+
.Following this new method
we synthesize LiAl
5
O
8
:Mn
4+
Li
5
AlO
4
:Mn
4+
LiAlO
2
:Mn
4+
and find that the former two have red long afterglow
this have not been reported before
then the luminescent properties of the two kinds of materials were studied
the reason of different intensity in different hosts was pointed out. We also test the intensity-concentration curve
notate that the radiation of Mn
4+
is due to transition of
2
E→
4
A
2
its emission spectrum is a broad band
peaked at 675 nm. It absorb ultraviolet strongly
the excitation spectrum extends from 620 nm to 770 nm
At last we research the mechanism of long afterglow of these materials
discuss why the long afterglow properties are different between these kinds of materials.
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