Treatment of triphenylgallium with 3,5-dimethylpyrazole, 3,5-diphenylpyrazole, or 3,5-di-tert-butylpyrazole in a 2:1 stoichiometry afforded the phenyl-bridged complexes (C6H5)2Ga(μ-Me2pz)(μ-C6H5)Ga(C6H5)2 (62%), (C6H5)2Ga(μ-Ph2pz)(μ-C6H5)Ga(C6H5)2·C7H8 (62%), and (C6H5)2Ga(μ-tBu2pz)(μ-C6H5)Ga(C6H5)2 (40%), respectively, as colorless or off-white crystalline solids. Treatment of triphenylindium with 3,5-di-tert-butylpyrazole in a 2:1 stoichiometry afforded the phenyl-bridged complex (C6H5)2In(μ-tBu2pz)(μ-C6H5)In(C6H5)2·(C6H14)0.5 (40%). The molecular structures of (C6H5)2Ga(μ-Ph2pz)(μ-C6H5)Ga(C6H5)2·C7H8, (C6H5)2Ga(μ-tBu2pz)(μ-C6H5)Ga(C6H5)2·(C6H14)0.5, and (C6H5)2In(μ-tBu2pz)(μ-C6H5)In(C6H5)2·(C6H14)0.5 consist of a 3,5-disubstituted pyrazolato ligand with a diphenylgallio or diphenylindio group bonded to each nitrogen atom. A phenyl group acts as a bridge between the two metal atoms. By contrast, treatment of triphenylgallium with 3,5-di-tert-butylpyrazole in a 1:1 stoichiometry or triphenylindium with 3,5-diphenylpyrazole or 3,5-dimethylpyrazole in 2:1 or 1:1 stoichiometry afforded the dimeric complexes [(C6H5)2Ga(μ-tBu2pz)]2 (63%), [(C6H5)2In(μ-Ph2pz)]2 (40%), and [(C6H5)2In(μ-Me2pz)]2 (92%), respectively, as colorless crystalline solids. The dimeric nature of these complexes was determined by X-ray crystallography. Treatment of 3,5-di-tert-butylpyrazole with excess trimethylgallium afforded the dimeric complex [Me2Ga(μ-tBu2pz)]2 (82%) as the major product and Me2Ga(μ-tBu2pz)(μ-OCH3)GaMe2 (2.6%) as a minor product. There was no evidence for the formation of the methyl-bridged complex Me2Ga(μ-tBu2pz)(μ-CH3)GaMe2. The kinetics of bridge-terminal phenyl exchange in (C6H5)2Ga(μ-Me2pz)(μ-C6H5)Ga(C6H5)2, (C6H5)2Ga(μ-Ph2pz)(μ-C6H5)Ga(C6H5)2·C7H8, (C6H5)2Ga(μ-tBu2pz)(μ-C6H5)Ga(C6H5)2, and (C6H5)2In(μ-tBu2pz)(μ-C6H5)In(C6H5)2·(C6H14)0.5 was determined by 13C NMR spectroscopy and afforded the following range of activation parameters: ΔH⧧ = 6.0−8.9 kcal/mol, ΔS⧧ = −23.1 to −32.0 eu, and ΔG⧧(298 K) = 15.5−15.8 kcal/mol. The large, negative values of ΔS⧧ imply ordered transition states relative to the ground state and rotation along the N−GaPh3 or N−InPh3 vector without metal−nitrogen bond cleavage. The combined results suggest that the close proximity of the metal atoms is the principal determinant of the bridging phenyl interactions and that complexes of the heavier group 13 elements with bridging hydrocarbon ligands are likely to be more accessible than the current state of literature would suggest.