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arXiv 1301.7339cond-mat.mtrl-sci
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锌钛矿和纤锌矿GaAs纳米线中As空位、Ga反位和Au杂质的第一性原理研究

As vacancies, Ga antisites and Au impurities in Zincblende and Wurtzite GaAs nanowire segments from first principles

Yaojun A. Du, Sung Sakong, Peter Kratzer

摘要:

本文利用密度泛函理论计算了GaAs纳米线中的点缺陷。这些问题主要来自于纳米线在不同于用于薄膜或块状GaAs的条件下的生长,例如锌钛矿和纤锌矿多型体的共存、金颗粒作为催化剂的使用以及砷限制的生长制度。因此,我们对ZB和WZ GaAs晶体中As空位、Ga_As反位和Au杂质进行了密度泛函计算。我们的研究结果表明,砷空位可以扩散的ZB GaAs晶体内的迁移势垒为~1.9 eV。在WZ GaAs中,发现As空位扩散是各向异性的,在ab平面中具有1.60至1.79 eV的低势垒(取决于掺杂条件),而沿着c轴扩散具有2.07至2.44 eV的较高势垒。Au杂质的形成能一般比As空位或Ga_As反位的形成能低得多。因此,Au杂质将是Au催化纳米线生长中形成的主要缺陷。此外,我们发现,它是积极更有利的1至2 eV的Au杂质取代晶格Ga原子比晶格As原子在GaAs中。发现在ZB GaAs中的晶格Ga原子的Au替代缺陷在带隙的下半部分中产生电荷转移能级。当我们计算的能级为E_v + 0.22eV时,考虑到密度泛函的不精确性,我们的计算结果与实验结果(E_v + 0.4eV)符合得很好。

英文摘要:

In this paper some specific issues related to point defects in GaAs nanowires are addressed with the help of density functional theory calculations. These issues mainly arise from the growth of nanowires under conditions different from those used for thin films or bulk GaAs, such as the co-existence of zincblende and wurtzite polytypes, the use of gold particles as catalyst, and the arsenic-limited growth regime. Hence, we carry out density-functional calculations for As vacancies, Ga_As antisites, and Au impurities in ZB and WZ GaAs crystals. Our results show that As vacancies can diffuse within in a ZB GaAs crystal with migration barriers of ~1.9 eV. Within WZ GaAs, As vacancy diffusion is found to be anisotropic, with low barriers of 1.60 up to 1.79 eV (depending on doping conditions) in the ab-plane, while there are higher barriers of 2.07 to 2.44 eV to diffuse along the c-axis. The formation energy of Au impurities is found to be generally much lower than those of arsenic vacancies or Ga_As antisites. Thus, Au impurities will be the dominant defects formed in Au-catalyzed nanowire growth. Moreover, we find that it is energetically more favorable by 1 to 2 eV for an Au impurity to replace a lattice Ga atom than a lattice As atom in GaAs. An Au substitutional defect for a lattice Ga atom in ZB GaAs is found to create a charge transfer level in the lower half of the band gap. While our calculations locate this level at E_v + 0.22eV, taking into account the inaccuracy of the density functional that ought to be corrected by a downshift of E_v by about 0.2eV results in good agreement with the experimental result of E_v + 0.4eV.

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