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1. 中国科学技术大学物理系
2. 中国科学技术大学结构分析开放实验室
纸质出版:1991-08-30
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张吉林, 洪广言. K<sub>2</sub>NaAlF<sub>6</sub>:Ce<sup>3+</sup>和KAlF<sub>4</sub>:Ce<sup>3+</sup>磷光体的光谱特性[J]. 发光学报, 1991,12(3): 224-229
Znang Jilin, Hong Guangyan. SPECTRAL PROPERTIES OF K<sub>2</sub>NaA1F<sub>8</sub>:Ce<sup>3+</sup> AND KAlF:Ce<sup>3+</sup>[J]. Chinese Journal of Luminescence, 1991,12(3): 224-229
张吉林, 洪广言. K<sub>2</sub>NaAlF<sub>6</sub>:Ce<sup>3+</sup>和KAlF<sub>4</sub>:Ce<sup>3+</sup>磷光体的光谱特性[J]. 发光学报, 1991,12(3): 224-229 DOI:
Znang Jilin, Hong Guangyan. SPECTRAL PROPERTIES OF K<sub>2</sub>NaA1F<sub>8</sub>:Ce<sup>3+</sup> AND KAlF:Ce<sup>3+</sup>[J]. Chinese Journal of Luminescence, 1991,12(3): 224-229 DOI:
本文研究了基质发光材料Na
5
Eu(MoO
4
)
4
和NaEu(MoO
4
)
2
的喇曼光谱.用群论方法分析了它们的内、外振动模式
对实验振动模进行了指认.本文还将上述喇曼光谱与Na
5
Eu(WO
4
)
4
、CaWO
4
、SrWO
4
、CaMoO
4
和SrMoO
4
的喇曼光谱进行了比较
Na
5
Eu(MoO
4
)
4
和NaEu(MoO
4
)
2
的喇曼光谱结果表明(MoO
4
)
2-
离子团的高能量拉伸内振动是产生Eu
3+
的
5
D
2
→
5
D
1
5
D
1
→
5
D
0
-
多声子无辐射弛豫的原因
这导致了Eu
3+
在这类材料中主要产生
5
D
O
→
7
F
j
的发光跃迁.
Na
5
Eu(MoO
4
)
4
and NaEu(MoO
4
)
2
are stoichiorr.etric host luminescent materials having high concentration of luminescent Eu
3+
ions and no noticeable concentration quenching. Raman spectra of these two materials have been studied. The symmetry species of the lattice vibration modes of Na
5
Eu(MoO
4
)
4
have been analysed by means of the group theory.The structures of both materials belong to tetragonal
I
4
I
/a (C
4h
6
) space group. For Na
5
Eu(MoO
4
)
4
the free ion symmetries of (MoO
4
)
2-
Eu
3+
and Na
1+
correlate with factor group C
4h
through their site groups. A primitive cell includes two Na
5
Eu(MoO
4
)
4
molecules. It mears that 8 (MoO
4
)
4
2-
10 Na
1+
and 2 Eu
3+
are included in the cell. So the lattice vibration of Na
5
Eu(MoO
4
)
4
in the cell can be classified into 72 internal modes and 84 external modes. For crystal factor group C
4h
the
A
g
B
g
and
E
g
modes are Raman active and
A
u
and
E
u
modes are infrared active.
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