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1. 长春科学技术大学, 吉林, 长春, 130026
2. 中国科学院长春应用化学研究所, 吉林, 长春, 130022
3. Division of Applied Science, Korea Institute of Science and Technology, P.O.Box 131, Seoul 130-650, Korea
收稿日期:1999-11-03,
修回日期:2000-01-21,
纸质出版日期:2000-05-30
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宋桂兰, 尤洪鹏, 洪广言, 曾小青, 甘树才, 金昌弘, 卞钟洪, 庾炳容, 裴贤淑, 权一亿, 朴哲熙. Y<sub>1.95-x</sub>Gd<sub>x</sub>SiO<sub>5</sub>:Eu<sub>0.05</sub>的真空紫外光谱[J]. 发光学报, 2000,21(2): 145-149
SONG Gui-lan, YOU Hong-peng, HONG Guang-yan, GAN Shu-cai, KIM Chang-Hong, PYUN Chong-Hong, YU Byung-yong, BAE Hyun-Sook, KWON Il-Eok, PARK Cheol-Hee. VUV Spectra of Y<sub>1.95-x</sub>Gd<sub>x</sub>SiO<sub>5</sub>: Eu<sub>0.05</sub>[J]. Chinese Journal of Luminescence, 2000,21(2): 145-149
宋桂兰, 尤洪鹏, 洪广言, 曾小青, 甘树才, 金昌弘, 卞钟洪, 庾炳容, 裴贤淑, 权一亿, 朴哲熙. Y<sub>1.95-x</sub>Gd<sub>x</sub>SiO<sub>5</sub>:Eu<sub>0.05</sub>的真空紫外光谱[J]. 发光学报, 2000,21(2): 145-149 DOI:
SONG Gui-lan, YOU Hong-peng, HONG Guang-yan, GAN Shu-cai, KIM Chang-Hong, PYUN Chong-Hong, YU Byung-yong, BAE Hyun-Sook, KWON Il-Eok, PARK Cheol-Hee. VUV Spectra of Y<sub>1.95-x</sub>Gd<sub>x</sub>SiO<sub>5</sub>: Eu<sub>0.05</sub>[J]. Chinese Journal of Luminescence, 2000,21(2): 145-149 DOI:
利用高温固相法合成了Y
1.95-x
Gd
x
SiO
5
:Eu
0.05
(
x
=0.6mol%)荧光体。结构测定表明所合成的荧光体为单斜晶系的X
2
型Y
2
SiO
5
相
空间群为B2/b。真空紫外光谱表明:随着Gd
3+
含量的增加
在192nm附近
出现了Gd
3+
的激发峰
且此峰的强度随着Gd
3+
含量的增加而增大;同时位于150~185nm之间的基质吸收带的强度也增大;而位于200~300nm之间的Eu的电荷迁移带的强度却随着Gd
3+
含量的增加而降低。
Color plasma display panel(PDP)is the most promising flat display for the large area display.Phosphors used in PDP are excited with vacuum-ultraviolet radiation.Naturally
the phosphors are required to have a good quantum efficiency in the region below 200um.Some silicates have stronger absorption in the VUV region.Therefore
it is important to investigate silicates.On the other hand
oxyorthosilicates have good thermal stability and chemistry stability
and also are good host for luminescent materials under UV excitation.However
optical properties of Y
2-x
Gd
x
SiO
5
: Eu in the VUV range have not been reported up to now.Y
1.95-x
Gd
x
SiO
5
:Eu
0.05
were prepared at 1200℃ for two hours with NH4F flux by solid-state reaction.Y
1.95-x
Gd
x
SiO
5
:Eu
0.05
are polymorphic and crytallizable in the monoclinic X
2
type with space group B2/b.The excitation spectra of Y
1.95-x
Gd
x
SiO
5
:Eu
0.05
monitored at 612um consists of a broad band at 220-300um corresponding to the charge transfer band of Eu
and a number of lines which could be assigned to the f-f transition of Eu
3+
for 300-540nm
and the strongest excited peak lies at 396nm.The emission spectrum of Y
1.95-x
Gd
x
SiO
5
:Eu
0.05
phosphors excited under 396mn irradiation consists of four groups of emission lines in the rang of 560-720nm.The maximum emission peak is located at 612urn.One luminescence line at 580nm
three lines at 590-596nm
five lines at 610-630nm and three lines at 685-705nm are assigned to the transitions 5D07F0
5DO7F1
5DO7F2
5D07F4
respectively.When a x(
x
= 0.2
0.4
0.6)mol faction of gadolinium is incorporated into the host lattice
the location of absorption peaks of Eu
3+
shown in VU-vis excitation specturm of Y1.95-xGdxSiO5: Eu0.05 are not changed
but the relative intensities of these peaks decrease with increasing Gd
3+
concentration.In the vacuum-ultraviolet region
the new absorption peak near 192nm appears.The intensity of the new peak assigned to the absorption of 6Gj configuration of Gd
3+
increases with increasing Gd
3+
concentration until 0.4 mol%
and then
the intensity decreases.The intensity of the host absorption band of the phosphors at 150-185nm is enhanced while the intensity of the charge transfer band of Eu decreases with increasing Gd
3+
concentration.Generally speaking
when a x mol fraction of gadolinium is incorporated into the host lattice
the luminescent intensity in vacuum-ultraviolet region increases in spite of the decreasing in VU-vis region.That is in favor of enhanching the luminescent intensity of phosphors used in PDP.
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