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中国科学院长春物理研究所
收稿日期:1986-09-01,
纸质出版日期:1987-08-30
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刘宪平, 鲍庆成, 田乃良, 李多录, 徐叙瑢, 戴仁崧. 高密度激发下CdS中束缚激子与激子的散射发光[J]. 发光学报, 1987,8(3): 192-198
Liu Xianping, Bao Qingcheng, Tian Nailiang, Li Duolu, Xu Xurong, Dai Rensong. THE LUMINESCENCE OF BOUND EXCITON-EXCITON SC<sub>A</sub> TTERING IN HIGHLY EXCITED CdS[J]. Chinese Journal of Luminescence, 1987,8(3): 192-198
刘宪平, 鲍庆成, 田乃良, 李多录, 徐叙瑢, 戴仁崧. 高密度激发下CdS中束缚激子与激子的散射发光[J]. 发光学报, 1987,8(3): 192-198 DOI:
Liu Xianping, Bao Qingcheng, Tian Nailiang, Li Duolu, Xu Xurong, Dai Rensong. THE LUMINESCENCE OF BOUND EXCITON-EXCITON SC<sub>A</sub> TTERING IN HIGHLY EXCITED CdS[J]. Chinese Journal of Luminescence, 1987,8(3): 192-198 DOI:
本文在液氦温度下在CdS中观测到一个新的发光峰
并提出束缚激子与激子非弹性散射发光模型对该峰的产生和特性进行了解释。
We have studied the emission spectrum of CdS single crystal in the excitation range from 10
6
to 10
7
W/cm
2
at temperature 4.2K.When the excitation density is low (106 W/cm
2
)
the emission spectrum is characterized by two peaks 4869Å (named I
2
) and 4888Å (named I
1
) which are the luminescence lines of neutral-donor-bound eXciton and of neutral-acceptor-bound exciton. As the excitation density goes up
the intensity of I
2
-peak decreases relatively and a luminescence band structure appears in the red side of I
1
-peak. When the excitation density up to 1.7×10
7
W/cm
2
a new peak (named U) is found. The new peak is characterized by narrow line width (about 3Å half width) and great luminescence intensity (Fig.1)We studied the polarization of I
1
-peak
I
2
-peak and U-peak as the excitation density changed. We found that the polarization v.s. excitation density for I
1
and U is the same. And we also studied the U-peak luminescence intensity by changing temperature in a fixed excitation. And the result is the same with that of I
2
-peak.Finally we concluded that the U-peak is the inelastic scattering luminescence of neutral-donor-bound exciton.We also caculated the intensity and energy of U-peak theoretically
the results are in correspondence with experimental results.We suggested the model of luminescence of inelastic bound exciton-exciton scattering.The causation and features of the peak were clearly explained using the model.
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