“…The geometry around Pt (3) is identical with that found for phosphanidoplatinum(I) complexes bonded to terminal phosphanes (or phosphinites) and bridged by diorganophosphanides of the general formula [(PR 1 2 R 2 )Pt(μ-PR 3 2 ) 2 Pt(PR 4 2 R 5 )](Pt−Pt) (R 1 = R 2 = R 4 = R 5 = Me, R 3 = t Bu; R 1 = R 2 = R 4 = R 5 = Ph, R 3 = t Bu; 34 R 1 = R 4 = Me, R 2 = R 5 = OMe, R 3 = cyclo-C 6 H 11 ; 5 R 1 = R 2 = R 3 = R 4 = R 5 = Ph). 35 Considering that the geometry of Pt(2) is reminiscent of that of the known phosphanido-bridged Pt III atoms, i.e., Pt 1/2 in [(C 6 F 5 ) 2 Pt 1 (μ-PPh 2 ) 2 Pt 2 (C 6 F 5 ) 2 ](Pt−Pt), 10 [(C 6 F 5 ) 2 Pt 1 (μ-PPh 2 ) 2 Pt 2 (μ-PPh 2 ) 2 Pt 3 (O,O-acac)](Pt 1 −Pt 2 ) + , 31 and [(C 6 F 5 ) 2 Pt 1 (μ-PPh 2 ) 2 Pt 2 (μ-PPh 2 ) 2 Pt 3 (C 6 F 5 ) 2 ](Pt 1 −Pt 2 ), 36 On the other hand, the Pt 2 and Pt 3 signals of 1 (δ −4720 and −5228, respectively) were obtained by recording a 1 H− 195 Pt HMQC NMR spectrum (Figure 3), which was set to exploit the scalar coupling between the o-H of the phenyl rings and Pt atoms. Once the chemical shifts of each of the three 195 Pt signals were located, their fine structures were obtained by recording a 1D 195 Pt{ 1 H} NMR spectrum ( Figure S1 in the Supporting Information), which showed inter alia a coupling constant between Pt 2 and Pt 3 of 515 Hz.…”