Solid state structures of group 13 metal halide complexes with pyrazine ( pyz) of 2 : 1 and 1 : 1 composition have been established by X-ray structural analysis. Complexes of 2 : 1 composition adopt molecular structures MX 3 ·pyz·MX 3 with tetrahedral geometry of group 13 metals. Complexes of AlBr 3 and GaCl 3 of 1 : 1 composition are 1D polymers (MX 3 ·pyz) ∞ with trigonal bipyramidal geometry of the group 13 metal, while the weaker Lewis acid GaI 3 forms the monomeric molecular complex GaI 3 ·pyz, which is isostructural to its pyridine analog GaI 3 ·py. Tensimetry studies of vaporization and thermal dissociation of AlBr 3 ·pyz and AlBr 3 ·pyz·AlBr 3 complexes have been carried out using the static method with a glass membrane null-manometer. Thermodynamic characteristics of vaporization and equilibrium gas phase dissociation of the AlBr 3 ·pyz complex have been determined. Comprehensive theoretical studies of (MX 3 ) n ·( pyz) m complexes (M = Al, Ga; X = Cl, Br, I; n = 1, 2; m = 1-3) have been carried out at the B3LYP/ TZVP level of theory. Donor-acceptor bond energies were obtained taking into account reorganization energies of the fragments. Computational data indicate that the formation of (MX 3 ·pyz) ∞ polymers with coordination number 5 is only slightly more energetically favorable than the formation of molecular complexes of type MX 3 ·pyz for X = Cl, Br. It is expected that on melting (MX 3 ·pyz) ∞ polymers dissociate into individual MX 3 ·pyz molecules. This dovetails with low melting enthalpies of the (MX 3 ·pyz) ∞ complexes.Polymer stability decreases in the order AlCl 3 > AlBr 3 > GaCl 3 > AlI 3 > GaBr 3 > GaI 3 . For MI 3 ·pyz complexes computations predict that the monomeric structure motif is more energetically favorable compared to the catena polymer. These theoretical predictions agree well with the experimentally observed monomeric complex GaI 3 ·pyz in the solid state. Thus, the Lewis acidity of the group 13 halides may play a decisive role in the formation of 1D polymeric networks.