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1. 复旦大学材料科学研究所
2. 复旦大学测试中心
收稿日期:1986-06-10,
纸质出版日期:1986-11-30
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黄京根, 胡建国, 王惠琴, 余兴海, 马礼敦, 何志强. CeMgAl<sub>11</sub>O<sub>19</sub>-SrAl<sub>12</sub>O<sub>19</sub>固溶体和CeMgAl<sub>11</sub>O<sub>19</sub>-SrMgAl<sub>10</sub>O<sub>17</sub>固溶体在稀土和碱土复合六角铝酸盐体系中的光谱学性质研究[J]. 发光学报, 1986,7(4): 357-366
Huang Jinggen(J. Huang), Hu Jianguo, Wang Huiqin, Yu Xinghai, Ma Lidun, He Zhiqiang. SPECTROSCOPIC PROPERTIES OF CeMgAl<sub>11</sub>O<sub>19</sub>-SrAl<sub>12</sub>O<sub>19</sub> and CeMgAl<sub>11</sub>O<sub>19</sub>-SrMgAl<sub>10</sub>O<sub>17</sub> SOLID SOLUTIONS IN RARE EARTHS AND ALKALINE EARTHS DOUBLE HEXALUMINATES SYSTEMS[J]. Chinese Journal of Luminescence, 1986,7(4): 357-366
黄京根, 胡建国, 王惠琴, 余兴海, 马礼敦, 何志强. CeMgAl<sub>11</sub>O<sub>19</sub>-SrAl<sub>12</sub>O<sub>19</sub>固溶体和CeMgAl<sub>11</sub>O<sub>19</sub>-SrMgAl<sub>10</sub>O<sub>17</sub>固溶体在稀土和碱土复合六角铝酸盐体系中的光谱学性质研究[J]. 发光学报, 1986,7(4): 357-366 DOI:
Huang Jinggen(J. Huang), Hu Jianguo, Wang Huiqin, Yu Xinghai, Ma Lidun, He Zhiqiang. SPECTROSCOPIC PROPERTIES OF CeMgAl<sub>11</sub>O<sub>19</sub>-SrAl<sub>12</sub>O<sub>19</sub> and CeMgAl<sub>11</sub>O<sub>19</sub>-SrMgAl<sub>10</sub>O<sub>17</sub> SOLID SOLUTIONS IN RARE EARTHS AND ALKALINE EARTHS DOUBLE HEXALUMINATES SYSTEMS[J]. Chinese Journal of Luminescence, 1986,7(4): 357-366 DOI:
本文研究CeMSAl
11
O
19
-SrAl
12
O
19
和CeMeAl
11
O
19
-SrMgAl
10
O
17
体系固溶体的发光性质。发现在CeMgAl
11
O
19
-SrAl
12
O
19
体系中
能形成完全的固溶体
随着SrAl
12
O
19
含量的增加
晶胞常数a线性地减小
c保持不变
Ce
3+
的Nephelauxetic效应和晶场强度减弱
Ce
3+
最低5d激发带边能量呈指数形式变化
Ce
3+
的发射能量线性地高移。在CeMgAl
11
O
19
-SrMgAl
10
O
17
体系中
不能形成完全的固溶体。固溶体终端组成大约为0.3CeMgAl
11
O
19-0.1
SrMgAl
10
O
17
。在这种固溶体中
晶胞常数α和c则随SrMgAl
10
O
17
含量分别线性地减小和增大。样品制备中添加H
3
BO
3
引起固溶体晶僻特性改变
大大提高Ce
3+
的发光强度。但当H
3
BO
3
量超过0.4(摩尔比)时
硼将进入晶格
反而减弱Ce
3+
的发光。
The systems of CeMgAl
11
O
19
-SrAl
12
O
19
and CeMgAl
12
O
19
-SrMgAl
10
O
17
were studied. In CeMgAl
12
O
19
-SrAl
12
O
19
complete solid solutions were observed and the positions of the lower d-band edge and emission peak of Ce
3+
shifted to higher energy while the cell of the solid solutions contracted as a result of decrease of the parameter a as the concentration of SrAl
12
O
19
increased. Furthermore
both the Nephelauxetic effect and the crystal field intensity of Ce
3+
decreased with increasing SrAl
12
O
19
concentration. Except for 0.9 CeMgAl
12
O
19
-0.1 SrAl
12
O
19
the emission position of Ce
3+
in energy increased linearly with increasing SrAl
12
O
19
content
which could be accounted for by power development fashion of the relation
E
=Q [1-(z/4)
l/z
10
-ar
] (see ref. [6]
). For 0.1 CeMgAl
12
O
19
-0.9 SrAl
12
O
19
the deviation of the emission peak of Ce
3+
from the straight line position could be due to a small Stokes shift for the compound. For CeMgAl
12
O
19
-SrMgAl
10
O
17
solid solutions were observed only when SrMgAl
10
O
17
content was within 70%.In the solid solutions
the emission peak energy of Ce
3+
increased linearly
and the cell parameters a and c decreased and increased respectively with increasing SrMgAl
10
O
17
concentration. For 0.1 CeMgAl
12
O
19
-0.9 SrMgAl
10
O
17
two phases were found with SrMgAl
10
O
17
as the primary phase and a magnetoplumbite-type Ce-and Si-double hexaluminate as the second phase
The emission of Ce
3+
in the mixed phases originated probably from the latter compound.The intensity of Ce
3+
emission in solid solutions was considerably enhanced by adding H
3
BO
3
to starting materials. But the Ce
3+
emission would reversely decrease if the quantity of H
3
BO
3
was too high. It was found that the change of crystal habit of solid solutions by H
3
BO
3
and the substitution of B for Al in the compounds were responsible for the observations.
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