The Aryl Bromine−Halide Ion Synthon and Its Role in the Control of the Crystal Structures of Tetrahalocuprate(II) Ions

R.D. Willett, Firas F. Awwadi, Robert E. Butcher, Salim F. Haddad, Brendan Twamley

Crystal Growth & Design · 2003 · 122 citations · 61 references

Concepts

Abstract

The role of the arylbromine-halide ion (C−Br···X - ) synthons in the development of the supramolecular frameworks is explored in a set of six bromopyridinium tetrahalocuprate(II) salts. The compounds belong to the series ( n BP) 2 CuX 4, where n BP + denotes the n -bromopyridinium cation and n = 2, 3, or 4 and X = Cl - or Br - and include (2BP) 2 CuBr 4, (3BP) 2 CuBr 4, (4BP) 2 CuBr 4, (2BP) 2 CuCl 4, (3BP) 2 CuCl 4, and (4BP) 2 CuCl 4 . The structures all consist of isolated pyridinium cations and flattened tetrahedral CuX 4 2- anions. The supramolecular assembly of these ionic species is dominated by the novel C−Br···X - synthon and the more traditional N−H···X - synthon. The C−Br···X - synthon is invariably characterized by essentially linear C−Br···X - angles with Br···X - contacts 0.3−0.4 Å less than the sum of the van der Waals radii. In contrast, the N−H···X - synthons show a variety of geometries: linear, symmetric bifurcated, and asymmetric bifurcated. In all cases, low dimensional supramolecular networks are developed based on combinations of the C−Br···X - and N−H···X - synthons. These include chain networks in (3BP) 2 CuCl 4, (4BP) 2 CuBr 4, and the (4BP) 2 CuX 4 salts. A double chain network exists in (3BP) 2 CuBr 4, while the structure of (4BP) 2 CuCl 4 contains a two-dimensional network. A common feature in all six networks is the existence of bibridged [CuX 4 2- − ( n BP + ) 2 − CuX 4 2- ] units, while the more complex double chain and layer networks also contain monobridged [CuX 4 2- − ( n BP + ) − CuX 4 2- ] units. These units then aggregate into the final crystal structures generally with coplanar stacking of the substituted pyridinium cations. The stacking interactions between cations include both π−π and π−Br interactions. In general, the π−π stacking is not optimal and, in some cases, it is nonexistent. Comparison with other previous studies show the competitive nature of the C−Br···X - and N−H···X - synthons in halocuprate(II) structures.

References

61