Two tris(triphenylphosphinegold)oxonium dimer salts [{{Au(PPh 3 )} 3 (m 3 ÀO)} 2 ] 2+ (X À ) 2 (X ¼ BF À 4 , MnO À 4 ) were investigated via synchrotron-based far-infrared vibrational spectroscopy and density functional theory modelled at the M06/LANL2DZ level of theory. The 50-800 cm À1 region of both oxonium salts is presented, with the spectrum for [{{Au(PPh 3 )} 3 (m 3 ÀO)} 2 ] 2+ (BF À 4 ) 2 found to possess a large feature at 330.3 cm À1 , attributable to counter-ion vibrational modes, which is only predicted upon explicit inclusion of counter-ions in the calculation. A feature around 107 cm À1 observed for the [{{Au(PPh 3 )} 3 (m 3 ÀO)} 2 ] 2+ (BF À 4 ) 2 infrared spectrum is assigned to 21 distinct vibrational modes arising from Au-Au bond stretching and other motions of the Au core. The same feature is predicted to be present within the [{{Au(PPh 3 )} 3 (m 3 ÀO)} 2 ] 2+ (MnO À 4 ) 2 spectrum but is masked by experimental noise. In the 50-400 cm À1 region, the relative intensities of predicted vibrational modes is found to depend heavily on the presence and nature of the counter-ions, while within the 400-800 cm À1 region, little dependence of the theoretical spectra on the type of counter-ion is predicted. Finally, the dimerization energies of both [{{Au(PPh 3 )} 3 (m 3 ÀO)} 2 ] 2+ (BF À 4 ) 2 and [{{Au(PPh 3 )} 3 (m 3 ÀO)} 2 ] 2+ (MnO À 4 ) 2 are calculated to be 3.06 eV and 3.20 eV, respectively, when the counter-ions are explicitly included within the calculation, and just 1.10 eV in their absence.