2165Bulk Susceptibility Mmurements. The raw data (XRT = 3.58x 10-4 emu/mol) were corrected for temperature-independent diamagnetism (xd = -4.90 X lo4 emu/mo1)22 to afford the paramagnetic susceptibility xiT = 8.54 X lo-' emu/mol. This value is significantly larger than that of [Ni(tmp)12[Re04] (xi, Pt-spine conductors. The rhenium(VI1) complex [ H B ( p~)~l R e 0~ (1) is readily reduced by triphenylphosphine in the presence of excess (CH,)$iX (X = Br, Cl) to give the corresponding rhenium(V) complexes [HB(pz),]ReOX, (2, X = CI; 3, X = Br, pz = pyrazolyl (ClH1N2)).[HB(pz),]ReOCI2 (2), which seems to exist as two bond stretch isomers, reacts with 1 equiv of thiophenol in refluxing THF In the presence of a base [DBU or N(C,H,)J to give [HB(pz),]ReO(CI)(SC,H,) (4). Two equivalents of thiophenol reacts with 2 in refluxing THF, also in the presence of base, to give [ H B (~Z ) , ] R~O ( S C~H~)~ (5). 2 will react with 1.2-ethanedithiol or 1,2-benzenedithiol under similar conditions to give [HB(pz)l]ReO(S2C,H4) (6) and [HB(pz),]ReO(S2C2H4) (7), respectively. The solid-state structures of 4 and 5 have been determined by X-ray crystallography. Both were found to be monomeric with an approximately octahedral arrangement of ligands around the rhenium atoms. 4 crystallizes in the orthorhombic space group Pbcu (No. 61) with cell parameters a = 13.159 ( I ) A, b = 18.656 ( I ) A, c = 15.902 ( I ) A, V = 3904 ( I ) AI, Z = 8, R = 0.043, and R, = 0.031 for 271 3 reflections with I > 244). 5 crystallizes in the monoclinic space group P2Jc (No. 14) with cell parameters a = 15.594 (3) A, b = 21.624 (1) A, c = 15.931 (1) A, @ = 107.00 (I)', V = 5137 (1) AI, Z = 4, R = 0.050, and R, = 0.036 for 6683 reflections with I > 2 4 .