Orbital selectivity in Sn adatom adlayer on a Si(111) surface

Luis Craco, S. S. Carara
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Abstract

Unconventional quantum many-particle phenomena naturally emerges when approaching the Mott-Hubbard insulating state. Finding insulator-metal transition in correlated adatoms in semiconductor surfaces provide an ideal material platform to design electronic states which may host superconductivity in two-dimensional electron systems. To uncover the micro-scopics underlying by multi-orbital interactions, we perform density functional plus dynamical mean-field theory calculations for the all-electron 5p-band Hubbard model, unraveling a Mott assisted Kondo insulating state in the atomic Sn layer deposited onto a Si(111) surface, also referred to as α-Sn. We propose that α-Sn is an ideal testing ground to explore hidden orbital selectivity and pseudogap behavior all arising from Mottness and discuss the relevance of our results for pure and hole doped α-Sn in the context of spectroscopy and tunnelling experiments of adatom lattices.
Si(111)表面锡金刚原子层的轨道选择性
当接近莫特-哈伯德绝缘态时,自然会出现非常规的量子多粒子现象。在半导体表面的相关原子中发现绝缘体-金属转变,为设计二维电子系统中可能具有超导性的电子态提供了理想的材料平台。为了揭示多轨道相互作用的微观原理,我们对全电子 5p 带哈伯德模型进行了密度泛函加动力学均场理论计算,揭示了沉积在 Si(111) 表面的锡原子层(也称为 α-Sn)中的莫特辅助近藤绝缘态。我们提出,α-Sn 是探索隐藏轨道选择性和伪缺口行为的理想试验场,所有这些都源于莫特性,并结合金刚晶格的光谱学和隧道实验,讨论了我们的结果与纯掺杂和空穴掺杂 α-Sn 的相关性。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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