2022
DOI: 10.1039/d2ta02993f
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Band gap opening from displacive instabilities in layered covalent-organic frameworks

Abstract: Symmetry breaking in covalent organic frameworks (COFs) lowers the energy and increases the valence to conduction band separation of the material.

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Cited by 10 publications
(14 citation statements)
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“…The optimised structures agree with prior experiments in terms of similar intralayer metal‐to‐metal distances (7.77 for Ti and 7.67 for V) and interlayer distance (8.67 for Ti and a slightly deviating 8.01 Å for V). The Ti‐based structure however differs strongly from the reported layer stacking: instead of being eclipsed, subsequent layers are displaced ( α115 ${\alpha \approx {115}^{\circ }}$ , β78 ${\beta \approx {78}^{\circ }}$ ) by d2.9 ${d\approx 2.9}$ Å), as seems to be common in other layered frameworks [36] . For [Fe III 2 (Cl 2 dhbq 2− )(Cl 2 dhbq 3− ) 2 ] 2− , no combination of spin initialization or variation of the atomic relaxation parameters led to the reported hexagonal structure.…”
Section: Resultsmentioning
confidence: 70%
See 1 more Smart Citation
“…The optimised structures agree with prior experiments in terms of similar intralayer metal‐to‐metal distances (7.77 for Ti and 7.67 for V) and interlayer distance (8.67 for Ti and a slightly deviating 8.01 Å for V). The Ti‐based structure however differs strongly from the reported layer stacking: instead of being eclipsed, subsequent layers are displaced ( α115 ${\alpha \approx {115}^{\circ }}$ , β78 ${\beta \approx {78}^{\circ }}$ ) by d2.9 ${d\approx 2.9}$ Å), as seems to be common in other layered frameworks [36] . For [Fe III 2 (Cl 2 dhbq 2− )(Cl 2 dhbq 3− ) 2 ] 2− , no combination of spin initialization or variation of the atomic relaxation parameters led to the reported hexagonal structure.…”
Section: Resultsmentioning
confidence: 70%
“…The Ti-based structure however differs strongly from the reported layer stacking: instead of being eclipsed, subsequent layers are displaced (a � 115 � , b � 78 � ) by d � 2:9 Å), as seems to be common in other layered frameworks. [36] For [Fe III 2 (Cl 2 dhbq 2À )(Cl 2 dhbq 3À ) 2 ] 2À , no combination of spin initialization or variation of the atomic relaxation parameters led to the reported hexagonal structure. Instead, the trifold symmetry around the metal node is found to be broken, leading to angles deviating from their quasi-hexagonal values of around 122°to 107 and 154°, respectively (Figure 2).…”
Section: Implicit Electrostatic Charge Compensationmentioning
confidence: 96%
“…The optimised structures agree with prior experiments in terms of similar intralayer metal-to-metal distances (7.77 Å for Ti and 7.67 Å for V) and interlayer distance (8.67 Å for Ti and a slightly deviating 8.01 Å for V). The Ti-based structure however differs strongly from the reported layer stacking: instead of being eclipsed, subsequent layers are displaced (α ≈ 115 • , β ≈ 78 • ) by d ≈ 2.9 Å), as seems to be common in other layered frameworks [36] . For [Fe III 2(Cl2dhbq 2− )(Cl2dhbq 3− )2] 2− , no combination of spin initialization or variation of the atomic relaxation parameters led to the reported hexagonal structure.…”
Section: Implicit Electrostatic Charge Compensationmentioning
confidence: 63%
“…The calculated chemical potentials for all elements are listed in Table S2. Interlayer binding energies were calculated as follows, E normalb = ( E M 1 n E B ) / A where E M is the calculated energy of the monolayer, n is the number of layers in the bulk structure, E B is the calculated energy of the bulk structure, and A is the surface area of the monolayer. All the needed energetic data are extracted and calculated by our in-house codes.…”
Section: Computational Developmentsmentioning
confidence: 99%