Relative Abundance of <math xmlns="http://www.w3.org/1998/Math/MathML"> <msub> <mrow class="MJX-TeXAtom-ORD"> <mi mathvariant="double-struck">Z</mi> </mrow> <mn>2</mn> </msub> </math> Topological Order in Exfoliable Two-Dimensional Insulators.
basic_science · Level V
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- Record sourced from PubMed, PMID 31658415.
- Also identified by DOI 10.1021/acs.nanolett.9b02689.
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Abstract
Quantum spin Hall insulators make up a class of two-dimensional materials with a finite electronic band gap in the bulk and gapless helical edge states. In the presence of time-reversal symmetry, <math xmlns="http://www.w3.org/1998/Math/MathML"> <msub> <mrow class="MJX-TeXAtom-ORD"> <mi mathvariant="double-struck">Z</mi> </mrow> <mn>2</mn> </msub> </math> topological order distinguishes the topological phase from the ordinary insulating one. Some of the phenomena that can be hosted in these materials, from one-dimensional low-dissipation electronic transport to spin filtering, could be promising for many technological applications in the fields of electronics, spintronics, and topological quantum computing. Nevertheless, the rarity of two-dimensional materials that can exhibit nontrivial [Formula: see text] topological order at room temperature hinders development. Here, we screen a comprehensive database we recently identified of 1825 monolayers that can be exfoliated from experimentally known compounds to search for novel quantum spin Hall insulators. Using density-functional and many-body perturbation theory simulations, we identify 13 monolayers that are candidates for quantum spin Hall insulators including high-performing materials such as AsCuLi<sub>2</sub> and (platinum) jacutingaite (Pt<sub>2</sub>HgSe<sub>3</sub>). We also identify monolayer Pd<sub>2</sub>HgSe<sub>3</sub> (palladium jacutingaite) as a novel Kane-Mele quantum spin Hall insulator and compare it with platinum jacutingaite. A handful of promising materials are mechanically stable and exhibit <math xmlns="http://www.w3.org/1998/Math/MathML"> <msub> <mrow class="MJX-TeXAtom-ORD"> <mi mathvariant="double-struck">Z</mi> </mrow> <mn>2</mn> </msub> </math> topological order, either unperturbed or driven by small amounts of strain. Such screening highlights a relative abundance of <math xmlns="http://www.w3.org/1998/Math/MathML"> <msub> <mrow class="MJX-TeXAtom-ORD"> <mi mathvariant="double-struck">Z</mi> </mrow> <mn>2</mn> </msub> </math> topological order of around 1% and provides an optimal set of candidates for experimental efforts.