首页> 外文期刊>Crystal Research and Technology: Journal of Experimental and Industrial Crystallography >Defect structure of strained heteroepitaxial In(1-x)Al-(x)P layers deposited by MOVPE on (001)GaAs substrates
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Defect structure of strained heteroepitaxial In(1-x)Al-(x)P layers deposited by MOVPE on (001)GaAs substrates

机译:MOVPE在(001)GaAs衬底上沉积的应变异质外延In(1-x)Al-(x)P层的缺陷结构

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摘要

Weak-beam, large angle convergent beam electron diffraction and high resolution transmission electron microscope experiments have revealed, that after strain relaxation due to plastic deformation dislocation networks can be observed in In(1-x)Al-(x)P heteroepitaxial layers grown on (001) GaAs substrates under compressive stress. The 60 degrees slip dislocations are mostly dissociated into partials of Shockley type whereas in the particular case of layers grown under tension twins are predominantly formed by successive nucleation and slip of 90 degrees Shockley partials on adjacent {111} glide planes lying inclined to the (001) surface. When a few 90 degrees Shockley partials pile up during extension of twins, then planar incoherent twin boundaries with {112} coincidence planes have been formed during strain relaxation. Due to the space group symmetry ((InAl)P belongs to the space group F43m) there is a striking asymmetry in defect formation, i.e. defect nucleation and slip on the planes (111) and ((1) over bar (1) over bar 1) slip of the [(1) over bar 10] zone are preferred to nucleation and slip on the {111} planes of the [110] zone. Apparently. the occupacy of the atomic sites in the dislocation core with either group-III or group-V atoms is responsible for this behaviour. The nature of the defects implies that their spontaneous nucleation should have taken place at the growing surface. Under tensile strain the 90 degrees Shockley partial is nucleation first and the 30 degrees one trails. Under compressive strain this sequence is reversed. It is evident, for dissociated dislocations lying at the interface always the 30 degrees partial, i.e. the partial with less mobility or with higher friction force, is detained near or directly in the interface. Thus, in layers grown under tension the stacking fault associated with the dissociated 60 degrees dislocation lies inside the GaAs substrate. For layers grown under compression it is located inside the ternary laver. [References: 35]
机译:弱束,大角度会聚束电子衍射和高分辨率透射电子显微镜实验表明,在塑性变形引起的应变松弛之后,可以在生长在其上的In(1-x)Al-(x)P异质外延层中观察到(001)GaAs衬底在压缩应力下。 60度滑脱位错大多分解为Shockley型部分,而在特定情况下,在张力双生下生长的层主要是由相继于({001} )表面。当双胞胎延伸期间一些90度的Shockley分部堆积时,则在应变松弛过程中形成了具有{112}重合面的平面非相干双胞胎边界。由于空间群对称((InAl)P属于空间群F43m),缺陷形成中存在显着的不对称性,即在平面(111)和((1)在平面上(1)在平面上1)[(1)在棒10上的区域)的滑动比成核和在[110]区域的{111}平面上的滑动更可取。显然。该位错是由位错核中的原子位点与III族或V族原子占据引起的。缺陷的性质意味着它们的自发形核应该发生在生长表面。在拉伸应变下,90度的肖克利部分首先成核,而30度的部分则成核。在压缩应变下,该顺序相反。显然,对于位于界面处的解离的位错,总是将30度的部分,即,具有较小运动性或较高摩擦力的部分保留在界面附近或直接保留在界面中。因此,在张力下生长的层中,与解离的60度位错相关的堆叠缺陷位于GaAs衬底内部。对于受压生长的层,其位于三元紫菜内部。 [参考:35]

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