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机构地区:[1]西北工业大学凝固技术国家重点实验室
出 处:《航空学报》1998年第1期62-67,共6页Acta Aeronautica et Astronautica Sinica
摘 要:以A.Kobayashi等的半经验紧束缚模型和Hjalmarson-Vogh-Wolford-Dow深能级理论为基础,计算了Hg1-xCdxTe中阳离子位替代式杂质(包括N,O,C)与最近邻替代式杂质形成sp3键杂质对后阳离子位杂质A1对称性深能级的变化以及最近邻理想双空位(Vc,Va)的深能级。计算结果表明:阳离子位杂质A1能级的变化取决于与其配对杂质的电负性,杂质对a1能级组分依赖关系dE/dx小于阳离子位单杂质A1能级的dE/dx,大于阴离子位单杂质T2能级的dE/dx,不同杂质对的dE/dx基本相同;理想双空位(Vc,Va)在能隙或近能隙区域产生一个a1态深能级,该能级的dE/dx很小,对于CdTe,位置在0.5eV,对于x<0.37的Hg1-xCdxTe,该能级成为导带共振态。On the basis of the semiempirical tight binding model of A.Kobayashi et al and Hjalmarson Vogl Wolford Dow theory of deep levels, in Hg 1- x Cd x Te, the deep level of ideal vacancy pair ( V c, V a) as well as the variation of the A 1 symmetric deep level of cation site substitutional impurities (N,O,C) when they are paired with nearest neighbor sp 3 bonded substitutional impurities is calculated. The results of this calculation show that the variation of the A 1 level of a cation site impurity depends on the electronegativity of its paired impurity. The energy level composition dependence ( d E/ d x) of the a 1 level of an impurity pair is smaller than that of the A 1 level of isolated cation site impurity, but is larger than that of the T 2 level of an isolated anion site impurity. Different impurity pairs have almost the same d E/ d x. The ideal vacancy pair ( V c, V a) introduces an a 1 symmetric level with very small d E/ d x near or in the band gap. For CdTe, its magnitude is about 0.5eV in CdTe. In Hg 1- x Cd x Te ( x <0.37), the level becomes a resonant state in conduction band.
分 类 号:TN213[电子电信—物理电子学]
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