AVS 60th International Symposium and Exhibition | |
Surface Science | Thursday Sessions |
Session SS2-ThA |
Session: | Surface Dynamics and Non-adiabatic Processes |
Presenter: | S.B. Donald, University of Virginia |
Authors: | S.B. Donald, University of Virginia I.A. Harrison, University of Virginia |
Correspondent: | Click to Email |
The effects of dynamics, surface temperature, and tunneling on the dissociative chemisorption of hydrogen on Cu(111) are explored using a dynamically-biased precursor mediated microcanonical trapping (d-PMMT) model. Transition state vibrational frequencies were taken from recent GGA-DFT electronic structure calculations and the model’s few remaining parameters were fixed by optimizing simulations to a limited number of quantum-state-resolved associative desorption experiments. The d-PMMT model reproduces a diverse variety of dissociative chemisorption and associative desorption experimental results, and, importantly, largely captures the surface temperature dependence of quantum-state-resolved dissociative sticking coefficients. Molecular translational energy parallel to the surface was treated as a spectator degree of freedom. The efficacy of molecular rotational energy to promote dissociation, relative to normal translational energy, varied monotonically from -45% to 33% as the rotational energy increased. The molecular vibrational and surface phonon efficacies were 60%. Efficacies did not vary with isotope change from H2 to D2. The thermal dissociative sticking coefficient for H2/Cu(111) is predicted to vary as S(T) = S0 exp(-Ea/RT) where S0 = 0.075 and Ea = 49.2 kJ/mol over the 300 K ≤ T ≤ 1000 K temperature range. Dynamical effects are significant and suppress S(T) by ~2 orders of magnitude as compared to statistical expectations. For thermal dissociative chemisorption of H2/Cu(111) at 1000 K, a temperature of catalytic interest, normal translational energy is calculated to provide 74% of the energy necessary to react, surface phonons 17%, molecular rotation 5%, and vibration 4%. Tunneling is calculated to account for 13% of S(T) at 1000 K, but more than 50% at temperatures below 400 K.