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1. 中国科学院激发态物理开放实验室, 吉林长春 130021
2. 中国科学院长春光学精密机械与物理研究所, 吉林长春130021
3. 中国科学院高能物理研究所同步辐射实验室 北京,100039
收稿日期:2000-12-27,
修回日期:2001-04-03,
纸质出版日期:2001-08-30
移动端阅览
初本莉, 刘行仁, 王晓君, 金伟华, 陶冶, 王渭, 侯雪颖. Ln<sub>7</sub>O<sub>6</sub>(BO<sub>3</sub>)(PO<sub>4</sub>)<sub>2</sub>Eu(<em>Ln</em>=La, Gd, Y)的VUV-UV激发和辐射发光[J]. 发光学报, 2001,22(3): 263-267
CHU Ben-li, LIU Xing-ren, WANG Xiao-jun, JIN Wei-hua, TAO Ye, WANG Wei, HOU Xue-ying. VUV Spectra Characteristics of Eu<sup>3+</sup>-activated Ln<sub>7</sub>O<sub>6</sub>(BO<sub>3</sub>)(PO<sub>4</sub>)<sub>2</sub> (<em>Ln</em>=La,Gd,Y)[J]. Chinese Journal of Luminescence, 2001,22(3): 263-267
初本莉, 刘行仁, 王晓君, 金伟华, 陶冶, 王渭, 侯雪颖. Ln<sub>7</sub>O<sub>6</sub>(BO<sub>3</sub>)(PO<sub>4</sub>)<sub>2</sub>Eu(<em>Ln</em>=La, Gd, Y)的VUV-UV激发和辐射发光[J]. 发光学报, 2001,22(3): 263-267 DOI:
CHU Ben-li, LIU Xing-ren, WANG Xiao-jun, JIN Wei-hua, TAO Ye, WANG Wei, HOU Xue-ying. VUV Spectra Characteristics of Eu<sup>3+</sup>-activated Ln<sub>7</sub>O<sub>6</sub>(BO<sub>3</sub>)(PO<sub>4</sub>)<sub>2</sub> (<em>Ln</em>=La,Gd,Y)[J]. Chinese Journal of Luminescence, 2001,22(3): 263-267 DOI:
本文报道了Ln
7
O
6
(BO
3
)(PO
4
)
2
:Eu(
Ln
=La
Gd
Y)在VUVUV区的激发光谱及Eu
3+
在可见区的发射光谱。其激发光谱包括基质在真空紫外区的激发带和激活剂离子在紫外区的Eu
3+
-O
2-
电荷迁移带
随La
3+
Gd
3+
Y
3+
离子半径逐渐减小
Eu
3+
-O
2-
电荷迁移带的重心位置逐渐向高能量方向移动
Gd
7
O
6
(BO
3
)(PO
4
)
2
:Eu和Y
7
O
6
(BO
3
)(PO
4
)
2
:Eu在真空紫外区的吸收与Eu
3+
-O
2-
电荷迁移带位于紫外区的吸收的比值要高于在La
7
O
6
(BO
3
)(PO
4
)
2
:Eu中的这个比值。激发能可被基质吸收
传递给激活剂离子
得到Eu
3+
的红光发射。在Gd
7
O
6
(BO
3
)(PO
4
)
2
:Eu中
5
D
0
7
F
1
的发射强度较强
在Y
7
O
6
(BO
3
)(PO
4
)
2
:Eu中
5
D
0
7
F
2
和
5
D
0
7
F
3
的跃迁较强。
Eu
3+
doped materials has made an important role in the PDP
but the color purity and fluorescent efficiency of the materials now available can not be satisfactory. To look for better materials
the fluorescent properties of Ln
7
O
6
(BO
3
)(PO
4
)
2
:Eu(
Ln
=La
Gd
Y) have been studied. The samples were synthesized by high temperature solid phase technique. The structures of the samples were complicated
it was showed by the infrared absorption spectra that the basic structure unit are [BO
3
]
3-
and [PO
4
]
3-
but because there are interaction between of [BO
3
]
3-
and [PO
4
]
3-
the radius of Eu
3+
ions is different from the La
3+
Gd
3+
Y
3+
ions
and there exists other anion group
etc.
the absorption spectra of Ln
7
O
6
(BO
3
)(PO
4
)
2
:Eu are not entirely the same as that of
Ln
BO
3
and
Ln
PO
4
doped with Eu. The excitation spectra in the region of VUV UV and the emission spectra in the visible region were studied. The excitation spectra are consisted of the Eu
3+
-O
2
charge transfer band and the host absorption band. The location of the Eu
3+
-O
2
charge transfer band shifted to the high energy with the radius of the La
3+
Gd
3+
Y
3+
decreasing; in the excitation spectra of the Gd
7
O
6
(BO
3
)(PO
4
)
2
:Eu and Y
7
O
6
(BO
3
)(PO
4
)
2
:Eu
the ratio between the absorption in the VUV region and in the Eu
3+
-O
2
charge transfer band is higher than that in the La
7
O
6
(BO
3
)(PO
4
)
2
:Eu; there is high absorption at 147nm in the Y
7
O
6
(BO
3
)(PO
4
)
2
:Eu.
0
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