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中国科学院长春物理研究所
收稿:1986-06-05,
纸质出版:1987-02-28
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陈一民, 徐叙瑢. Y<sub>3</sub>Al<sub>5</sub>O<sub>12</sub>中晶场造成的Er<sup>3+</sup>多重态重心的移动[J]. 发光学报, 1987,8(1): 1-6
Chen Yimin, Xu Xurong. SHIFTS IN THE CENTERS OF GRAVITY OF MULTIPLETS FOR Er<sup>3+</sup>:Y<sub>3</sub>Al<sub>5</sub>O<sub>12</sub> DUE TO CRYSTAL FIELD[J]. Chinese Journal of Luminescence, 1987,8(1): 1-6
陈一民, 徐叙瑢. Y<sub>3</sub>Al<sub>5</sub>O<sub>12</sub>中晶场造成的Er<sup>3+</sup>多重态重心的移动[J]. 发光学报, 1987,8(1): 1-6 DOI:
Chen Yimin, Xu Xurong. SHIFTS IN THE CENTERS OF GRAVITY OF MULTIPLETS FOR Er<sup>3+</sup>:Y<sub>3</sub>Al<sub>5</sub>O<sub>12</sub> DUE TO CRYSTAL FIELD[J]. Chinese Journal of Luminescence, 1987,8(1): 1-6 DOI:
计算了由晶场造成的Er
3+
:Y
3
Al
5
O
12
多重态重心的移动。比较了计入和不计入这种移动
用拉卡参数
E
1
、
E
2
、
E
3
和自旋与轨道相互作用参数ξ拟合Er
3+
能级的结果。
The Hamiltonian describing a rare-earth impurity ion is assumed to be composed of the free ion Hamiltonian
H
F
and the one-electron crystal-field Hamiltonian
H
CF
·We write
H
CF
=
V
0
+
H
’
CF
with
<
img style="vertical-align:middle" alt="" order="0" src="http://www.rhhz.net/qikantupian/fgxb-19870101-1.gif" /
>
here
V
0
is the part of
H
CF
that is independent of angular variables.Thus the Hamiltionian of the system can be written as
H
=
H
F
+
V
0
+
H
’
CF
(3)The eigenvalues of
H
F
+
V
0
are usually called free ion levels. Because of the existence of
H
’
CF
each free ion level will split into Stark levels
and the center of gravity of the Stark levels will be shifted from correspondent free ion level. It is not concluded whether these shifts are comparable with the contributions of configuration interaction
spin-spin interaction and other interactions. The systematical calculation on these shifts has not been reported so far as we know. In this paper we present the results for Er
3+
in Y
3
Al
5
O
12
.
0
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