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首页> 外文期刊>Journal of Applied Physics >Interface Structure And Anisotropic Strain Relaxation Of Nonpolar Wurtzite (1120) And (1010) Orientations: Zno Epilayers Grown On Sapphire
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Interface Structure And Anisotropic Strain Relaxation Of Nonpolar Wurtzite (1120) And (1010) Orientations: Zno Epilayers Grown On Sapphire

机译:非极性纤锌矿(1120)和(1010)取向的界面结构和各向异性应变弛豫:蓝宝石上生长的Zno外延层

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The interface properties between nonpolar ZnO and sapphire have been studied using high resolution transmission electron microscopy. Two nonpolar orientations are investigated: a- and m-orientations corresponding to [1120] and [1010] crystallographic directions. After the definition of the epitaxial relationships and the resulting initial lattice mismatch, we show that nonpolar ZnO can be grown on sapphire with perfectly flat interfaces. Geometrical misfit dislocations are observed at the interface ZnO/sapphire and their density gives the residual strain in the layer. A strong anisotropy in the strain relaxation is found along the two perpendicular in-plane directions. This anisotropy may be explained in terms of initial anisotropic mismatch yielding different relaxation processes. A domain matching epitaxy is observed in m- and a-oriented layers for mismatches larger than 9% while a lattice matching epitaxy, in which the relaxation is driven by nucleation and glide of dislocations, is observed in a-oriented ZnO along the [0001] in-plane direction. In order to explain the observed relaxation the activated slip systems are calculated for both nonpolar orientations as a function of the in-plane stress due to the anisotropic mismatch. There is a major difference from the polar orientations. Low energy prismatic slip systems can be effective for plastic relaxation in the nonpolar orientations because they are no longer parallel to the growth direction, which is the case of c-oriented layers, nor to the applied stress. Our results can be directly extended to other nonpolar wurtzite structures such as Ill-nitrides.
机译:已经使用高分辨率透射电子显微镜研究了非极性ZnO和蓝宝石之间的界面特性。研究了两种非极性取向:对应于[1120]和[1010]结晶方向的a和m取向。在定义了外延关系和由此产生的初始晶格失配之后,我们证明了非极性ZnO可以在具有完美平坦界面的蓝宝石上生长。在ZnO /蓝宝石界面观察到几何失配位错,其密度给出了层中的残余应变。沿着两个垂直的平面内方向发现了应变松弛中的强各向异性。可以用产生不同弛豫过程的初始各向异性失配来解释这种各向异性。在m取向和a取向的层中发现了大于9%的失配的域匹配外延,而在a取向的ZnO中沿着[0001]观察到晶格匹配的外延,其中弛豫是由成核和位错滑动驱动的。 ]面内方向。为了解释观察到的松弛,由于各向异性失配,针对两个非极性取向计算了激活的滑移系统,作为面内应力的函数。与极性方向有很大的不同。低能量棱柱滑动系统对于非极性取向的塑性松弛可能是有效的,因为它们不再平行于c取向层的情况,即与生长方向平行,也不与施加的应力平行。我们的结果可以直接扩展到其他非极性纤锌矿结构,例如III族氮化物。

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