The metal organic framework material Ni 3 (2,3,6,7,10,11-hexaiminotriphenylene) 2 , (Ni 3 (HITP) 2 ) is composed of layers of extended conjugated planes analogous to graphene. We carried out density functional theory (DFT) calculations to model the electronic structure of monolayer, bilayer and bulk Ni 3 (HITP) 2 . These materials have intriguing electronic properties; for example, appreciable band dispersion is predicted not only in-plane but also perpendicular to the stacking planes. This suggests that, unlike graphene, the material may have appreciable conductivity in all crystallographic directions. Moreover, the bulk and bilayer structures are predicted to be metallic; in contrast, a 2D monolayer of the material exhibits a band gap. Insight obtained from studies of the transition of the material from semiconducting to metallic as the dimensionality increases from 2D to 3D suggests the possibility of producing a 3D semiconducting material by inserting spacer moieties between the layers. Our calculations suggest that it is not energetically favorable for Ni 3 (HITP) 2 to accept a spacer linker (i.e. pyridine); however, changing the coordinating metal to Cr makes spacer insertion energetically favorable. The proposed 3D material is predicted to possess a band gap of ~1 eV with electron/hole effective masses similar to that of silicon.
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IntroductionMany two-dimensional materials exhibit remarkable properties that suggest tantalizing possibilities for electronic applications. 1 Perhaps the most famous such material, graphene, is generating a great deal of excitement. Unfortunately, its metallic conductivity limits the potential for electronic device applications; a semiconducting material would be far more versatile. Moreover, graphene offers few straightforward routes to chemical modification and high-quality material has proved notoriously difficult to fabricate in useful shapes, sizes, and quantities on practical substrates. 2-4 Other known twodimensional materials, such as boron nitride (BN), silicene, germanene, and transition-metal dichalcogenides (TMDs), also suffer from production processing issues. Nevertheless, these materials have intriguing electronic properties with a breath of potential applications, such as field-effect transistors (FETs), thermoelectrics, spin-and valleytronics, and even topological insulators. 5-7 Molecular systems, such as pentacene, rubrene, and conjugated polymers, exhibit a wide diversity of electrical behaviors, including both metallic and semiconducting properties, and arguably offer the greatest potential for tunable properties. Molecular systems have the added benefit of being readily deposited as films and are conformable to traditional roll-to-roll processing techniques. However, the electrical properties of these materials are often inferior to inorganic conductors, having reduced charge carrier mobilities and inconsistent properties credited to molecular disorder. 8 Consequently, 2-D materials with tunable optoelectronic properties, high charge-carrier mobility, a...