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复旦大学材料科学研究所
收稿日期:1989-04-12,
纸质出版日期:1990-02-28
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黄京根, 余兴海, 胡建国, 王惠琴, 徐燕. Ce<sup>3+</sup>,Pb<sup>2+</sup>和Sn<sup>2+</sup>离子在β′-Al<sub>2</sub>O<sub>3</sub>型六角铝酸盐1.30BaO&#183;6Al<sub>2</sub>O<sub>3</sub>中的发光性质[J]. 发光学报, 1990,11(1): 8-13
Huang Jinggen, Yu Xinghai, Hu Jianguo, Wang Huiqin, Xu Yian. LUMINESCENCE OF Ce<sup>3+</sup>, Pb<sup>2+</sup> AND Sn<sup>2+</sup> IN THE β'-ALUMINA TYPE Ba-RICH HEXAALUMINATE 1.30BaO&#183;6Al<sub>2</sub>O<sub>3</sub>[J]. Chinese Journal of Luminescence, 1990,11(1): 8-13
黄京根, 余兴海, 胡建国, 王惠琴, 徐燕. Ce<sup>3+</sup>,Pb<sup>2+</sup>和Sn<sup>2+</sup>离子在β′-Al<sub>2</sub>O<sub>3</sub>型六角铝酸盐1.30BaO&#183;6Al<sub>2</sub>O<sub>3</sub>中的发光性质[J]. 发光学报, 1990,11(1): 8-13 DOI:
Huang Jinggen, Yu Xinghai, Hu Jianguo, Wang Huiqin, Xu Yian. LUMINESCENCE OF Ce<sup>3+</sup>, Pb<sup>2+</sup> AND Sn<sup>2+</sup> IN THE β'-ALUMINA TYPE Ba-RICH HEXAALUMINATE 1.30BaO&#183;6Al<sub>2</sub>O<sub>3</sub>[J]. Chinese Journal of Luminescence, 1990,11(1): 8-13 DOI:
本文研究稀土离子Ce
3+
和S
2
型离子(Pb
2+
和Sn
2+
)在β′-Al
2
O
3
型富钡相六角铝酸盐1.30BaO·6Al
2
O
3
中的发光性质。发射光谱和激发光谱表明
在富钡相中激活离子占据两个不等当的晶体学格位。Ce
3+
激活的样品
发射光谱由四个带组成
其相对强度不依赖于激活离子的浓度
不同Ce
3+
发光中心间没有能量传递。对于Pb
2+
和Sn
2+
在紫外激发下
荧光光谱包含三个带
Pb
2+
的带峰值为390nm
425nm和485nm;Sn
2+
为388nm
418nm和457nm。425nm和418nm发射分别归于占据晶体学BR格位的Pb
2+
和Sn
2+
;390nm和388nm发射归于反BR格位上的Pb
2+
和Sn
2+
;而485nm和457nm的带分别是Pb
2+
和Sn
2+
的离子对的发射。离子对是由占据(Ba)
n
O镜面层上的BR和反BR格位的Pb
2+
(或Sn
2+
)所形成。Pb
2+
和Sn
2+
离子的发光按照S
x
型离子能级作了讨论。
The luminescecnee of the Al
2
O
3
type Ba-rich hexaaluminale 1.30BaO·6Al
2
O
3
activated with Ce
3+
Pb
2+
and Sn
2+
is investigated. Emission and excitation spectra show the existence of two different activator centers for all these ions in the Ba-rich compound. For 1.30 BaO·6Al
2
O
3
:Ce
3+
the emission spectrum of Ce
3+
ions is consisted of four bands
the relative intensities of which are independent on the activator concentration
indicating that no energy transfer takes place between two different Ce
3+
centers. For the Pb
2+
- or Sn
2+
-activated compounds
fluorescence spectra contain three bands
390nm
425nm and 485nm for Pb
2+
and 388nm
418nm and 457nm for Sn
2+
lespectively. The bands of 425nm and 390nm (or 418nm and 388nm) are attributed to Pb
2+
(or Sn
2+
) ions
situated in the crystallographic BR and anti-BR sites
lespectively
whereas the bands of 485nm and 457nm are ascribed to pairs of Pb
2+
and Sn
2+
ions
respectively
whereas to their increasing intensities relative to the other two bands with increasing Pb
2+
and Sn
2+
concent. The formation of the ion pair is compared with data reported in the literature for SrAl
12
O
19
:Pb
2+
and is shown to be due to the interaction between the activator ions occupying the BR and anti-BR sites in the same mirror plane. Besides
the luminescence properties of Pb
2+
and Sn
2+
are dhcussed in the light of the energy scheme of Sn
2+
ions.
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