超导电性
配对
位置和动量空间
马约拉纳
物理
拓扑(电路)
凝聚态物理
望远镜
拓扑绝缘体
齐次空间
平移对称性
理论物理学
量子力学
几何学
数学
组合数学
作者
Sourav Manna,Sanjib Kumar Das,Bitan Roy
出处
期刊:Physical review
[American Physical Society]
日期:2024-05-06
卷期号:109 (17)
被引量:20
标识
DOI:10.1103/physrevb.109.174512
摘要
Topological insulators, featuring bulk-boundary correspondence, have been realized on a large number of noncrystalline materials, among which amorphous network, quasicrystals, and fractal lattices are the most prominent ones. By contrast, topological superconductors beyond the realm of quantum crystals are yet to be harnessed, as their nucleation takes place around a well-defined Fermi surface with a Fermi momentum, the existence of which rests on the underlying translational symmetry. Here we identify a family of noncrystalline Dirac materials, devoid of time-reversal ($\mathcal{T}$) and translational symmetries, on which a suitable local or on-site pairing yields topological superconductors. We showcase this outcome on all the abovementioned noncrystalline platforms embedded in a two-dimensional flat space. The resulting noncrystalline topological superconductors possess quantized topological invariants (Bott index and local Chern marker) and harbor robust one-dimensional Majorana edge modes, analogs of $\mathcal{T}$-odd $p+ip$ pairing in noncrystalline materials.
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