Abstract

Halogen bonds are prevalent in many areas of chemistry, physics, and biology. We present a statistical model for the interaction energies of halogen-bonded systems at equilibrium based on high-accuracy ab initio benchmark calculations for a range of complexes. Remarkably, the resulting model requires only two fitted parameters, X and B—one for each molecule—and optionally the equilibrium separation, R e , between them, taking the simple form E = X B / R e n . For n = 4 , it gives negligible root-mean-squared deviations of 0.14 and 0.28 kcal mol − 1 over separate fitting and validation data sets of 60 and 74 systems, respectively. The simple model is shown to outperform some of the best density functionals for non-covalent interactions, once parameters are available, at essentially zero computational cost. Additionally, we demonstrate how it can be transferred to completely new, much larger complexes and still achieve accuracy within 0.5 kcal mol − 1 . Using a principal component analysis and symmetry-adapted perturbation theory, we further show how the model can be used to predict the physical nature of a halogen bond, providing an efficient way to gain insight into the behavior of halogen-bonded systems. This means that the model can be used to highlight cases where induction or dispersion significantly affect the underlying nature of the interaction.

Highlights

  • Halogen bonds are an important class of non-covalent interaction where a halogen-containing donor, AX, interacts with a Lewis base as acceptor, B

  • The criteria for which systems are to be considered are that they be tractable by the high-accuracy computational methods to be employed, and that they be representative of known halogen-bonded complexes

  • We have presented a statistical model for the interaction energy of halogen-bonded systems at equilibrium that takes the simple form Xi Bj /R4e,ij, where Xi and Bj are parameters for the halogen-bond donor and acceptor, while Re,ij is the equilibrium separation between the two molecules

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Summary

Introduction

Halogen bonds are an important class of non-covalent interaction where a halogen-containing donor, AX, interacts with a Lewis base as acceptor, B. Spectroscopic [7,8,9] studies that they were found to be prevalent in both the gas and condensed phases [10,11] These investigations discovered several striking properties, in particular the strong preference for linear geometries [12,13], where the AX···B angle is close to 180◦ , and interaction energies similar to those of hydrogen bonds [8,14]. The most popular recent explanation is that of a σ-hole, first suggested in 2005 by Clark et al [24] They posit that the attachment of a suitably electronwithdrawing group to a halogen atom results in withdrawal of electron density from the halogen along the σ-bond. A simple electrostatic argument can be made for how

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