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Abstract
Lieb lattice has been extensively studied to realize ferromagnetism due to its exotic flat band. However, its material realization has remained elusive; so far only artificial Lieb lattices have been made experimentally. Here, based on first-principles and tight-binding calculations, we discover that a recently synthesized two-dimensional sp2 carbon-conjugated covalent-organic framework (sp2c-COF) represents a material realization of a Lieb-like lattice. The observed ferromagnetism upon doping arises from a Dirac (valence) band in a non-ideal Lieb lattice with strong electronic inhomogeneity (EI) rather than the topological flat band in an ideal Lieb lattice. The EI, as characterized with a large on-site energy difference and a strong dimerization interaction between the corner and edge-center ligands, quenches the kinetic energy of the usual dispersive Dirac band, subjecting to an instability against spin polarization. We predict an even higher spin density for monolayer sp2c-COF to accommodate a higher doping concentration with reduced interlayer interaction.
While ferromagnetism has been observed in an sp2 covalent-organic framework, its origin remains unclear. Here, by first-principle and tight-binding calculations, the authors identify the Lieb-lattice-like feature of the two-dimensional covalent-organic material and the Stoner mechanism responsible for its magnetic behavior.
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1 University of Utah, Department of Materials Science and Engineering, Salt Lake City, USA (GRID:grid.223827.e) (ISNI:0000 0001 2193 0096); University of Minnesota, Department of Electrical and Computer Engineering, Minneapolis, USA (GRID:grid.17635.36) (ISNI:0000000419368657)
2 University of Utah, Department of Materials Science and Engineering, Salt Lake City, USA (GRID:grid.223827.e) (ISNI:0000 0001 2193 0096)
3 University of Utah, Department of Materials Science and Engineering, Salt Lake City, USA (GRID:grid.223827.e) (ISNI:0000 0001 2193 0096); Collaborative Innovation Center of Quantum Matter, Beijing, China (GRID:grid.495569.2)