Theory of triangulene two-dimensional crystals
arXiv:2206.14907 · doi:10.1088/2053-1583/aca4e2
Abstract
Equilateral triangle-shaped graphene nanoislands with a lateral dimension of benzene rings are known as triangulenes. Individual triangulenes are open-shell molecules, with single-particle electronic spectra that host half-filled zero modes and a many-body ground state with spin . The on-surface synthesis of triangulenes has been demonstrated for and the observation of a Haldane symmetry-protected topological phase has been reported in chains of triangulenes. Here, we provide a unified theory for the electronic properties of a family of two-dimensional honeycomb lattices whose unit cell contains a pair of triangulenes with dimensions . Combining density functional theory and tight-binding calculations, we find a wealth of half-filled narrow bands, including a graphene-like spectrum (for ), spin-1 Dirac electrons (for ), -orbital physics (for ), as well as a gapped system with flat valence and conduction bands (for ). All these results are rationalized with a class of effective Hamiltonians acting on the subspace of the zero-energy states that generalize the graphene honeycomb model to the case of fermions with an internal pseudospin degree of freedom with symmetry.
12 pages, 7 figures
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Cited by in corpus (7)
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- Broken-symmetry magnetic phases in two-dimensional triangulene crystals
- Conformational tuning of magnetic interactions in coupled nanographenes
- Superexchange Mechanism in Coupled Triangulenes Forming Spin-1 Chains
- Magnetic frustration and fractionalization in oligo(indenoindenes)
- Quantum Monte Carlo study of artificial triangular graphene quantum dots
- Modulated Dirac bands and integer hopping ratios in a honeycomb lattice of phenalenyl-tessellation molecules