STRUCTURE AT 200 AND 298 K AND X-RAY-INVESTIGATIONS OF THE PHASE-TRANSITION AT 242 K OF [NH2(CH3)(2)]3SB2CL9 (DMACA)

[NH2(CH3)(2)]3Sb2Cl9 (dimethylammonium nonachlorodiantimonate, DMACA) has, at 200 K, a monoclinic Pc space group, with a = 9.470(3), b = 9.0 34(3), c = 14.080(4) Angstrom, beta = 95.81(3)degrees, V = 1198.4(4) A ngstrom(3) Z = 2 [R = 0.024, wR = 0.025 for 4613 independent reflectio ns with F > 4 sigma(F)]. At 298 K DMACA has P2(1)/c space group with a = 9.686(3), b = 9.037(3), c = 14.066(4) Angstrom, beta = 95.57(3)degr ees, V = 1225.3(5) Angstrom(3), Z = 2 [R = 0.034, wR = 0.035 for 2736 reflections with F > 4 sigma(F)]. The anionic sublattice of DMACA cons ists of polyanionic (Sb2Cl93-)(n) layers. In the low-temperature phase there are three crystallographically non-equivalent dimethylammonium cations in the crystal structure. One of the cations is located inside the polyanionic layers, two others - one ordered and one disordered - between the polyanionic layers. In the room-temperature phase there a re two non-equivalent cations - both disordered - in the crystal struc ture. Temperature dependencies of lattice parameters between 200 and 3 00 K were determined. The occurrence of a second-order phase transitio n at T = 242 K was confirmed. The dependence of lengths of Sb-Cl conta cts on the presence and strength of N-H ... Cl hydrogen bonds was disc ussed. It was found that lengths of Sb-Cl bonds may differ from each o ther by as much as 0.3 Angstrom, because of the presence of N-H ... Cl hydrogen bonds. These differences were attributed to distortion of th e lone-electron pair on antimony(III).