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引用次数: 0
摘要
综上所述,PAS给出了浓度范围为10 15 -10 19 cm -3的半导体空位缺陷的微观信息。正电子寿命是与缺陷相关的开放体积的指纹,它可以用来识别单位和空位以及更大的空位团簇。另一方面,湮灭辐射的多普勒展宽可以用来确定空位周围原子的性质。因此,可以区分化合物半导体的不同子晶格上的空位,并且可以识别与空位相关的杂质。空位缺陷的电荷状态可以通过正电子捕获系数的温度依赖性来确定,正电子在负中心周围的里德伯态定位可以得到关于没有开放体积的离子受体的信息。重要的是,正如本章所示,基于正电子湮灭的方法不受半导体的性质或物理尺寸的限制。可以在任何电导率的样品中研究窄带隙和宽带隙半导体材料中的缺陷。块状晶体和薄膜可以经受实验和缺陷识别。
Positron annihilation spectroscopy, experimental and theoretical aspects
In summary, PAS gives microscopic information about vacancy defects in semiconductors in the concentration range 10 15 -10 19 cm -3 . The positron lifetime is the fingerprint of the open volume associated with a defect, and it can be used to identify mono- and divacancies and larger vacancy clusters. Doppler broadening of the annihilation radiation, on the other hand, can be used to identify the nature of the atoms surrounding the vacancy. Consequently, vacancies on different sub lattices of a compound semiconductor can be distinguished, and impurities associated with the vacancies can be identified. The charge state of a vacancy defect can be determined by the temperature dependence of the positron -trapping coefficient, and positron localization into Rydberg states around negative centers yields information about ionic acceptors that have no open volume. Importantly, as shown in this chapter, the methods based on positron annihilation are not restricted by the nature or physical dimensions of the semiconductor. Defects can be studied in narrow- and wide-bandgap semiconductor materials in samples of any conductivity. Bulk crystals as well as thin films can be subjected to the experiments and defects identified.