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Interstitial Carbon-Related Defects in Si_(1-x)Ge_x Alloys

机译:Si_(1-x)Ge_x合金中与碳有关的间隙缺陷

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The interstitial carbon impurity (C_1) vibrational modes in monocrystalline Si-rich SiGe were investigated by Fourier Transform Infra Red spectroscopy and density functional modelling. The two absorption bands of C_1 are found to be close to those in silicon, but show shifts in opposite directions with increasing Ge content. The transversal mode band at 932 cm~(-1) shifts slightly to the high frequency side, while the longitudinal mode at 922 cm~(-1) suffers a pronounced red-shift. Each C_1-related band is found to consist of two components. An annealing of C_1 in Si_(1-x)Ge_x occures in two stage. During the first stage (210-250 K) the main components of bands anneals and revealed components grow in intensity. At T>250 K all components disappear. Two component structure of bands is suppose most likely correspond to different combinations of Si and Ge atoms in the neighbourhood of the carbon atom. The interstitial carbon defect was modelled by a supercell density-functional pseudopotential method (AIMPRO) for alloys with 4.69% Ge concentration. From energetics, it has been found that each Ge-C bond costs at least 0.4 eV in excess of a Si-C bond. However, structures where Ge atoms are second neighbors to the C atom are marginally bound, and may explain the two-component band structure in the absorption measurements. The vibrational mode frequencies taken from several randomly generated SiGe cells produce the observed opposite shifts for the transverse and longitudinal modes.
机译:利用傅立叶变换红外光谱和密度泛函模型研究了单晶富硅SiGe中间隙碳杂质(C_1)的振动模式。发现C_1的两个吸收带与硅中的吸收带接近,但是随着Ge含量的增加,显示出在相反方向上的位移。横向模式带在932 cm〜(-1)处向高频侧稍有偏移,而纵向模式在922 cm〜(-1)处出现明显的红移。发现每个与C_1相关的频段都由两个部分组成。 Si_(1-x)Ge_x中C_1的退火过程分为两个阶段。在第一阶段(210-250 K)中,带退火的主要成分和显露成分的强度增加。在T> 250 K时,所有分量消失。推测带的两个组成结构最可能对应于碳原子附近的Si和Ge原子的不同组合。用Supercell密度函数pseudo势方法(AIMPRO)对间隙浓度为4.69%Ge的合金的碳缺陷进行了建模。从能量学上,已经发现每个Ge-C键的成本至少比Si-C键高0.4eV。然而,Ge原子是C原子的第二邻居的结构是有限边界的,并且可以解释吸收测量中的双组分带结构。从几个随机生成的SiGe单元获取的振动模式频率会产生横向模式和纵向模式的观察到的相反位移。

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