The halogen bond occurs when there is evidence of a net attractive interaction between an electrophilic region associated with a halogen atom in a molecular entity and a nucleophilic region in another, or the same, molecular entity. In this fairly extensive review, after a brief history of the interaction, we will provide the reader with a snapshot of where the research on the halogen bond is now, and, perhaps, where it is going. The specific advantages brought up by a design based on the use of the halogen bond will be demonstrated in quite different fields spanning from material sciences to biomolecular recognition and drug design.

The Halogen Bond

Halogen bonding refers to the non-covalent interactions of halogen atoms X in some molecules, RX, with negative sites on others. It can be explained by the presence of a region of positive electrostatic potential, the sigma-hole, on the outermost portion of the halogen's surface, centered on the R-X axis. We have carried out a natural bond order B3LYP analysis of the molecules CF(3)X, with X = F, Cl, Br and I. It shows that the Cl, Br and I atoms in these molecules closely approximate the [Formula: see text] configuration, where the z-axis is along the R-X bond. The three unshared pairs of electrons produce a belt of negative electrostatic potential around the central part of X, leaving the outermost region positive, the sigma-hole. This is not found in the case of fluorine, for which the combination of its high electronegativity plus significant sp-hybridization causes an influx of electronic charge that neutralizes the sigma-hole. These factors become progressively less important in proceeding to Cl, Br and I, and their effects are also counteracted by the presence of electron-withdrawing substituents in the remainder of the molecule. Thus a sigma-hole is observed for the Cl in CF(3)Cl, but not in CH(3)Cl.

Halogen bonding: the σ-hole

A halogen bond is a highly directional, electrostatically-driven noncovalent interaction between a region of positive electrostatic potential on the outer side of the halogen X in a molecule R–X and a negative site B, such as a lone pair of a Lewis base or the π-electrons of an unsaturated system. The positive region on X corresponds to the electronically-depleted outer lobe of the half-filled p-type orbital of X that is involved in forming the covalent bond to R. This depletion is labeled a σ-hole. The resulting positive electrostatic potential is along the extension of the R–X bond, which accounts for the directionality of halogen bonding. Positive σ-holes can also be found on covalently-bonded Group IV–VI atoms, which can similarly interact electrostatically with negative sites. Since positive σ-holes often exist in conjunction with negative potentials on other portions of the atom's surface, such atoms can interact electrostatically with both nucleophiles and electrophiles, as has been observed in surveys of crystallographic structures. Experimental as well as computational studies indicate that halogen and other σ-hole interactions can be competitive with hydrogen bonding, which itself can be viewed as a subset of σ-hole bonding.

Halogen bonding: an electrostatically-driven highly directional noncovalent interaction

A σ-hole bond is a noncovalent interaction between a covalently-bonded atom of Groups IV–VII and a negative site, e.g. a lone pair of a Lewis base or an anion. It involves a region of positive electrostatic potential, labeled a σ-hole, on the extension of one of the covalent bonds to the atom. The σ-hole is due to the anisotropy of the atom's charge distribution. Halogen bonding is a subset of σ-hole interactions. Their features and properties can be fully explained in terms of electrostatics and polarization plus dispersion. The strengths of the interactions generally correlate well with the magnitudes of the positive and negative electrostatic potentials of the σ-hole and the negative site. In certain instances, however, polarizabilities must be taken into account explicitly, as the polarization of the negative site reaches a level that can be viewed as a degree of dative sharing (coordinate covalence). In the gas phase, σ-hole interactions with neutral bases are often thermodynamically unfavorable due to the relatively large entropy loss upon complex formation.

Halogen bonding and other σ-hole interactions: a perspective

Halogen bonding (XB) is a type of noncovalent interaction between a halogen atom X in one molecule and a negative site in another. X can be chlorine, bromine or iodine. The strength of the interaction increases in the order Cl<Br<I. After a brief review of experimental evidence relating to halogen bonding, we present an explanation for its occurrence in terms of a region of positive electrostatic potential that is present on the outermost portions of some covalently-bonded halogen atoms. The existence and magnitude of this positive region, which we call the σ-hole, depends upon the relative electron-attracting powers of X and the remainder of its molecule, as well as the degree of sp hybridization of the s unshared electrons of X. The high electronegativity of fluorine and its tendency to undergo significant sp hybridization account for its failure to halogen bond. Some computed XB interaction energies are presented and discussed. Mention is also made of the importance of halogen bonding in biological systems and processes, and in crystal engineering.

An overview of halogen bonding

Intermolecular interactions of the carbon-fluorine bond: the crystallographic environment of fluorinated carboxylic acids and related structures

Absolute configuration of the isomer of fluorocitrate that inhibits aconitase

Three-point attachment of citrate to a cobalt(III) tetraamine complex

Magnitude of the equilibrium isotope effect on carbontritium bond synthesis

The enzyme 2-keto-3-deoxy-6-phosphogalactonate aldolase of Pseudomonas saccharophila is inactivated by the substrate analog beta-bromopyruvate, which satisfies several criteria of being an active site directed reagent. The inactivation exhibits saturation kinetics, and both bromopyruvate and pyruvate (substrate) compete for free enzyme. Upon prolonged incubation, inactivation is virtually complete. The Kinact for bromopyruvate is 12 mM and the minimum inactivation half-time is 16 min with a k of 0.0433 min minus 1. Bromopyruvate is also a substrate for the enzyme in that 3(R,S)-[3-3H2]bromopyruvate is asymmetrically detritiated by the enzyme yielding 3(S)-[3-3H,H]bromopyruvate concomitant with inactivation. At various concentrations of bromopyruvate which affect the inactivation rate, the ratio of nanomoles of bromopyruvate turned over/unit of enzyme inactivated remains constant averaging 12:1, consistent with both inactivation and catalysis occurring at a single protein site, the catalytic site. The above value does not take into account a possible hydrogen isotope effect and is not thus an absolute value. The stereochemistry of bromopyruvate turnover catalyzed by this enzyme is the same as that for 2-keto-3-deoxy-6-phosphogluconate aldolase of P. putida. This fact provides the first evidence that the pyruvate-specific portions of the two active sites may have evolved from a common precursor.

Claire T. Monti

Papers

Intermolecular interactions of the carbon-fluorine bond: the crystallographic environment of fluorinated carboxylic acids and related structures

Absolute configuration of the isomer of fluorocitrate that inhibits aconitase

Three-point attachment of citrate to a cobalt(III) tetraamine complex

Magnitude of the equilibrium isotope effect on carbontritium bond synthesis

Bromopyruvate inactivation of 2-keto-3-deoxy-6-phosphogalactonate aldolase of Pseudomonas saccharophila. Kinetics and stereochemistry