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Absence of a Band Gap at Interface of a Metal and Highly Doped Monolayer $MoS_2$

机译:在金属界面和高度掺杂的单层膜上没有带隙   $二硫化钼$

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摘要

High quality electrical contact to semiconducting transition metaldichalcogenides (TMDCs) such as $MoS_2$ is key to unlocking their uniqueelectronic and optoelectronic properties for fundamental research and deviceapplications. Despite extensive experimental and theoretical efforts reliableohmic contact to doped TMDCs remains elusive and would benefit from a betterunderstanding of the underlying physics of the metal-TMDC interface. Here wepresent measurements of the atomic-scale energy band diagram of junctionsbetween various metals and heavily doped monolayer $MoS_2$ using ultra-highvacuum scanning tunneling microscopy (UHV-STM). Our measurements reveal thatthe electronic properties of these junctions are dominated by 2D metal inducedgap states (MIGS). These MIGS are characterized by a spatially growing measuredgap in the local density of states (L-DOS) of the $MoS_2$ within 2 nm of themetal-semiconductor interface. Their decay lengths extend from a minimum of~0.55 nm near mid gap to as long as 2 nm near the band edges and are nearlyidentical for Au, Pd and graphite contacts, indicating that it is a universalproperty of the monolayer semiconductor. Our findings indicate that even inheavily doped semiconductors, the presence of MIGS sets the ultimate limit forelectrical contact.
机译:与诸如MoS_2 $之类的半导体过渡金属卤化物(TMDC)的高质量电接触是为基础研究和设备应用解锁其独特的电子和光电特性的关键。尽管进行了大量的实验和理论上的努力,但与掺杂TMDC的可靠欧姆接触仍然难以捉摸,并且将从对金属-TMDC接口的基本物理原理的更好理解中受益。在这里,我们介绍了使用超高真空扫描隧道显微镜(UHV-STM)对各种金属与重掺杂单层$ MoS_2 $之间的结进行原子级能带图的测量。我们的测量结果表明,这些结的电子特性主要由2D金属诱导间隙态(MIGS)决定。这些MIGS的特征在于,在金属-半导体界面的2 nm范围内,$ MoS_2 $的局部态密度(L-DOS)在空间上不断增大,并且在测量间隙中。它们的衰减长度从中间隙附近的最小〜0.55 nm延伸到能带边缘附近的2 nm,对于Au,Pd和石墨接触几乎相同,这表明它是单层半导体的通用属性。我们的发现表明,即使掺杂很低的半导体,MIGS的存在也为电接触设置了极限。

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