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STM / STS measurements of Mn atoms in Group III-V semiconductors

机译:STM / STS测量III-V族半导体中的锰原子

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Diluted magnetic semiconductor (DMSs) are semiconductors doped with magnetic atoms. For practicaluse, it is necessary to clarify the electronic states around the magnetic atoms. Recent scanning tunnelingmicroscopy (STM) measurements revealed the hole state bound to a Mn acceptor in III-V semiconductorssuch as GaAs[1], InAs[2] and InSb[3]. It was shown by STM that the hole state bound to a Mn acceptor inIII-V semiconductors has a strongly anisotropic shape which is even more pronounced at cleaved (110)surfaces. This anisotropy is caused by the strain field of the surface relaxation and the tip-induced electricfield[4]. Also, it is known that the appearance of the STM image changes depending on the depth of theacceptor level. At a fixed depth, the charge distribution of a deep acceptor, such as Mn in GaAs and InAs, ischaracterized by a bow-tie shape whereas the shape of the charge distribution of a shallow acceptor, such asZn in GaAs and Mn in InSb, is triangular.
机译:稀释磁性半导体(DMS)是掺杂有磁性原子的半导体。为了实际应用,有必要弄清楚磁性原子周围的电子状态。最近的扫描隧道显微镜(STM)测量揭示了在III-V型半导体(例如GaAs [1],InAs [2]和InSb [3])中与Mn受体结合的空穴状态。 STM显示,III-V族半导体中结合到Mn受体上的空穴状态具有强烈的各向异性形状,该形状在劈开的(110)表面上更加明显。这种各向异性是由表面弛豫的应变场和尖端感应电场引起的[4]。同样,已知STM图像的外观根据受体水平的深度而改变。在固定深度处,深接受体(如GaAs和InAs中的Mn)的电荷分布以蝴蝶结形为特征,而浅接受体(如GaAs中的Zn和InSb中的Mn)的电荷分布的形状为三角形。

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