Abstract
The present contribution reports experimental and computational investigations of the interaction between [Cp*Fe(dppe)H] and different proton donors (HA). The focus is on the structure of the proton transfer intermediates and on the potential energy surface of the proton transfer leading to the dihydrogen complex [Cp*Fe(dppe)(H~2~)]^+^. With p‐nitrophenol (PNP) a UV/Visible study provides evidence of the formation of the ion‐pair stabilized by a hydrogen bond between the nonclassical cation [Cp*Fe(dppe)(H~2~)]^+^ and the homoconjugated anion ([AHA]^−^). With trifluoroacetic acid (TFA), the hydrogen‐bonded ion pair containing the simple conjugate base (A^−^) in equilibrium with the free ions is observed by IR spectroscopy when using a deficit of the proton donor. An excess leads to the formation of the homoconjugated anion. The interaction with hexafluoroisopropanol (HFIP) was investigated quantitatively by IR spectroscopy and by ^1^H and ^31^P NMR spectroscopy at low temperatures (200–260 K) and by stopped‐flow kinetics at about room temperature (288–308 K). The hydrogen bond formation to give [Cp*Fe(dppe)H]⋅⋅⋅HA is characterized by Δ__H°=−6.5±0.4 kcal mol^−1^ and Δ__S°=−18.6±1.7 cal mol^−1^ K^−1^. The activation barrier for the proton transfer step, which occurs only upon intervention of a second HFIP molecule, is Δ__H__^≠^=2.6±0.3 kcal mol^−1^ and Δ__S__^≠^=−44.5±1.1 cal mol^−1^ K^−1^. The computational investigation (at the DFT/B3 LYP level with inclusion of solvent effects by the polarizable continuum model) reproduces all the qualitative findings, provided the correct number of proton donor molecules are used in the model. The proton transfer process is, however, computed to be less exothermic than observed in the experiment.