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      Binding Properties of Small Electrophilic Anions [B 6X 5] and [B 10X 9] (X=Cl, Br, I): Activation of Small Molecules Based on π‐Backbonding

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          Abstract

          Superelectrophilic anions constitute a special class of molecular anions that show strong binding of weak nucleophiles despite their negative charge. In this study, the binding characteristics of smaller gaseous electrophilic anions of the types [B 6X 5] and [B 10X 9] (with X=Cl, Br, I) were computationally and experimentally investigated and compared to those of the larger analogues [B 12X 11] . The positive charge of vacant boron increases from [B 6X 5] via [B 10X 9] to [B 12X 11] , as evidenced by increasing attachment enthalpies towards typical σ‐donor molecules (noble gases, H 2O). However, this behavior is reversed for σ‐donor–π‐acceptor molecules. [B 6Cl 5] binds most strongly to N 2 and CO, even more strongly than to H 2O. Energy decomposition analysis confirms that the orbital interaction is responsible for this opposite trend. The extended transition state natural orbitals for chemical valence method shows that the π‐backdonation order is [B 6X 5] >[B 10X 9] >[B 12X 11] . This predicted order explains the experimentally observed red shifts of the CO and N 2 stretching fundamentals compared to those of the unbound molecules, as measured by infrared photodissociation spectroscopy. The strongest red shift is observed for [B 6Cl 5N 2] : 222 cm −1. Therefore, strong activation of unreactive σ‐donor–π‐acceptor molecules (commonly observed for cationic transition metal complexes) is achieved with metal‐free molecular anions.

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          The method of dispersion correction as an add-on to standard Kohn-Sham density functional theory (DFT-D) has been refined regarding higher accuracy, broader range of applicability, and less empiricism. The main new ingredients are atom-pairwise specific dispersion coefficients and cutoff radii that are both computed from first principles. The coefficients for new eighth-order dispersion terms are computed using established recursion relations. System (geometry) dependent information is used for the first time in a DFT-D type approach by employing the new concept of fractional coordination numbers (CN). They are used to interpolate between dispersion coefficients of atoms in different chemical environments. The method only requires adjustment of two global parameters for each density functional, is asymptotically exact for a gas of weakly interacting neutral atoms, and easily allows the computation of atomic forces. Three-body nonadditivity terms are considered. The method has been assessed on standard benchmark sets for inter- and intramolecular noncovalent interactions with a particular emphasis on a consistent description of light and heavy element systems. The mean absolute deviations for the S22 benchmark set of noncovalent interactions for 11 standard density functionals decrease by 15%-40% compared to the previous (already accurate) DFT-D version. Spectacular improvements are found for a tripeptide-folding model and all tested metallic systems. The rectification of the long-range behavior and the use of more accurate C(6) coefficients also lead to a much better description of large (infinite) systems as shown for graphene sheets and the adsorption of benzene on an Ag(111) surface. For graphene it is found that the inclusion of three-body terms substantially (by about 10%) weakens the interlayer binding. We propose the revised DFT-D method as a general tool for the computation of the dispersion energy in molecules and solids of any kind with DFT and related (low-cost) electronic structure methods for large systems.
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                Author and article information

                Contributors
                Journal
                Chemistry – A European Journal
                Chemistry A European J
                Wiley
                0947-6539
                1521-3765
                December 22 2023
                November 14 2023
                December 22 2023
                : 29
                : 72
                Affiliations
                [1 ] Wilhelm-Ostwald-Institut für Physikalische und Theoretische Chemie Universität Leipzig Linnéstr. 2 04103 Leipzig Germany
                [2 ] Anorganische Chemie Fakultät für Mathematik und Naturwissenschaften Bergische Universität Wuppertal Gaußstr. 20 42119 Wuppertal Germany
                [3 ] Institut für Anorganische Chemie Institut für Nachhaltige Chemie & Katalyse mit Bor (ICB) Julius-Maximilians-Universität Würzburg Am Hubland 97074 Würzburg Germany
                [4 ] Leibniz Institute of Surface Engineering (IOM) Permoserstr. 15 04318 Leipzig Germany
                Article
                10.1002/chem.202302247
                9c636e89-ceba-4b15-91c3-df4238d88463
                © 2023

                http://creativecommons.org/licenses/by-nc/4.0/

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