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中国科学技术大学物理系
纸质出版:1981-08-30
移动端阅览
夏上达. Ⅱ-Ⅵ化合物中钒中心的光致发光[J]. 发光学报, 1981,2(3): 1-11
Xia Shang-da. PHOTOLUMINESCENSE OF VANADIUM IN Ⅱ-Ⅵ COMPOUNDS[J]. Chinese Journal of Luminescence, 1981,2(3): 1-11
通过对T
d
对称群中V
++
(d
8
)所有能量矩阵的完全对角化计算
发现B≈0.4B.、C≈5.0B、D
q
≈1.7B时的晶场跃迁
4
T
2
(drde
2
)→
4
T
1
(dr
2
de)能较好的拟合ZnS、CdS、CdSe等化合物中V中心在5000cm
-1
附近的辐射.其整个光激发谱的基本面貌也能在此模型中得到解释;进一步
还用Y.Tanabe和H.Kaminura的不可约张量法考虑了对称性降低到C
3
和旋轨耦合S·L的一级修正
结果和实验符合较好.
The characteristic luminescence near 5000cm
-1
in vanadium-activated Ⅱ-Ⅵ compounds is ascribed to the transition
4
T
2
(drde
2
)→
4
T
1
(dr
2
dε)within the V
2+
ion which is in a crystal field of T
d
symmetry. According to the complete dia-gonalization calculation of energy matrix
the appropriate crystal-field parameters are derived as follows:B=0.4B
0
C=5.0Band D
q
=1.7B. This avoids the difficulty of "T
d
forbidden"which occurs in other models
and qualitatively exp-lains the main charaters of positions
intensities and shapes of excitation spectra of ZnS:V
CdS:V
CdSe:V and CdS:V(Cu)
Furthermore
the first step correction fo-mulas of energy are derived by using the irreducible tensor method of Y.Tanabe and H.Kaminura when the symmetry is lowered from T
d
to C
3
t and the spin-orbit coupling is considered. As an example
the first step correction of CdS:V (Cu)is carried out and it is shown that the broad split of the first excitation band(8820cm
-1
~9500cm
-1
)can also be explained in this model.
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