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Selective-area growth and magnetic characterization of MnAs/AlGaAs nanoclusters on insulating Al2O3 layers crystallized on Si(111) substrates

机译:Si(111)衬底上结晶的绝缘Al2O3层上MnAs / AlGaAs纳米团簇的选择性区域生长和磁性表征

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摘要

We report on selective-area metal-organic vapor phase epitaxy and magnetic characterization of coupled MnAs/AlGaAs nanoclusters formed on thin Al2O3 insulating layers crystallized on Si(111) substrates. Cross-sectional transmission electron microscopy reveals that poly-crystalline c-Al2O3 grains are formed after an annealing treatment of the amorphous Al2O3 layers deposited by atomic layer deposition on Si(111) substrates. The h111i direction of the c-Al2O3 grains tends to be oriented approximately parallel to the h111i direction of the Si substrate. We observe that hexagonal MnAs nanoclusters on AlGaAs buffer layers grown by selective-area metal-organic vapor phase epitaxy on partially SiO2-masked Al2O3 insulator crystallized on Si(111) substrates are oriented with the c-axis along the h111i direction of the substrates, but exhibit a random in-plane orientation. A likely reason is the random orientation of the poly-crystalline c-Al2O3 grains in the Al2O3 layer plane. Magnetic force microscopy studies at room temperature reveal that arrangements of coupled MnAs nanoclusters exhibit a complex magnetic domain structure. Such arrangements of coupled MnAs nanoclusters may also show magnetic random telegraph noise, i.e., jumps between two discrete resistance levels, in a certain temperature range, which can be explained by thermally activated changes of the complex magnetic structure of the nanocluster arrangements.
机译:我们报告选择性区域金属有机气相外延和耦合的MnAs / AlGaAs纳米团簇形成在Si(111)衬底上结晶的薄Al2O3绝缘层上的磁性表征。横截面透射电子显微镜显示,在对通过原子层沉积在Si(111)衬底上沉积的非晶Al2O3层进行退火处理之后,形成了多晶c-Al2O3晶粒。 c-Al2O3晶粒的h111i方向倾向于近似平行于Si衬底的h111i方向。我们观察到,在选择性沉积在Si(111)衬底上的部分SiO2掩膜的Al2O3绝缘体上,通过选择性区域金属有机气相外延生长的AlGaAs缓冲层上的六角形MnAs纳米团簇,其c轴沿衬底的h111i方向取向,但呈现出随机的面内方向。一个可能的原因是多晶c-Al2O3晶粒在Al2O3层平面中的无规取向。室温下的磁力显微镜研究表明,耦合的MnAs纳米簇的排列表现出复杂的磁畴结构。偶联的MnAs纳米团簇的这种布置还可能显示出磁性随机电报噪声,即在一定温度范围内在两个离散的电阻水平之间跳跃,这可以通过纳米团簇布置的复杂磁性结构的热激活变化来解释。

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