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中国科学院长春物理研究所
收稿日期:1990-08-01,
纸质出版日期:1991-08-30
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江风益, 范广涵, 范希武, 马英忠. 在CaF<sub>2</sub>衬底上常压MOCVD法生长ZnSe-ZnTe应变超晶格[J]. 发光学报, 1991,12(3): 183-189
Jiang Fengyi, Fan Guanghan, Fan Xiwu(X. W. Fan), Ma Yingzhong. GROWTH OF ZnSe-ZnTe STRAINED-LAYER SUPERLATTICES ON CaF<sub>2</sub> (111) SUBSTRATE BY ATMOSPHERIC PRESSURE METAL ORGANIC CHEMICAL VAPOR DEPOSITION[J]. Chinese Journal of Luminescence, 1991,12(3): 183-189
江风益, 范广涵, 范希武, 马英忠. 在CaF<sub>2</sub>衬底上常压MOCVD法生长ZnSe-ZnTe应变超晶格[J]. 发光学报, 1991,12(3): 183-189 DOI:
Jiang Fengyi, Fan Guanghan, Fan Xiwu(X. W. Fan), Ma Yingzhong. GROWTH OF ZnSe-ZnTe STRAINED-LAYER SUPERLATTICES ON CaF<sub>2</sub> (111) SUBSTRATE BY ATMOSPHERIC PRESSURE METAL ORGANIC CHEMICAL VAPOR DEPOSITION[J]. Chinese Journal of Luminescence, 1991,12(3): 183-189 DOI:
我们首次在透明衬底CaF
2
上生长了ZnSe-ZnTe应变超晶格。通过X射线衍射测量
观测到多级卫星峰
表明超晶格周期结构的形成.光致发光光谱峰值的蓝移
表征ZnSe-ZnTe超晶格中应变与量子尺寸效应的存在.吸收光谱中几个明显的拐点
表明了发生在超晶格导带与价带子能级之间的多级跃迁的形成。
The growth of ZnSe-ZnTe strained-layer superlattices on CaF
2
(111) substrate by atmospheric pressure metal organic chemical vapor deposition is reported for the first time. The typical growth conditions are shown in Table 1. The critical thickness of ZnTe/CaF
2
heterojuncticn is appraised as 2nm. With X-ray diffraction measurement
we observe many satellites of ZnSe-ZnTe SLS around(333) reflection
which confirms the formation of the period structure of superlattices
and shown in. Fig.1.The lattice parameters of ZnTe
Zr.Se and CaF
2
are 0.6101 nm
0.56686 nm
0.54626 nm
corresponding to the Bragg diffraction angles 29 around (333) reflection 82.00
89.837 and 94.231 degree
respectively. We found that the satellites around the ZnSe Bragg angle are very strong
while the satellites around ZnTe Brafg argle are too weak to observe them in Fig.1. So the thickness of ZnSe layers is much larger than that of ZnTe layers.Using the zero-order peak corresponding to the average perpendicular lattice parameter and the superlattice periodicity calculation
we obtain the data of ZnSe and ZnTe layers a.s 6nm
0.6nm
respectively.For ZnSe (6nm)-ZnTe(0.6nm) SLS/CaF
2
(111)
the first ZnTe layer on substrate CaF
2
can not be accommodated by elastic deformation
and the lattice constant of the SLS parallel to the surface determined by Eq.1 does not equal the lattice constant of the substrate.Fig.2 is the photoluminescence emission spectrum of ZnSe (6nm)-ZnTe(0.6nm) SLS/CaF
2
with the excitation of the line 337.1nm of N
2
-laser at 77K. The peak value is 630nm which shows the existence of strain and quantum confinement effects. Fig.3 is the optical absorption spectrum of ZnSe(6nm)-ZnTe(0.6nm) SLS on CaF
2
transparent substrate with the measurement of UV-3000 Double Wave-length/Dual Beam Recording Spectrophotometer at room temperature. The first absorption peak at 640nm is thought to be the optical absorption due to the transition Between the
n
=1 electronic subband in ZnSe layers and the
n
=1 heavy hole subband in ZnTe layers.
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