Abstract:The creation of electronic excitations during the reaction of atomic hydrogen on and with coinage and noble metals has been studied using metal-insulator-metal heterostructures. A characteristic current trace is observed when the outer metal surface of the structure is exposed to a 20 s pulse of H atoms. Comparison to the chemical kinetics allows to disentangle the contributions from the different chemical processes to this current. In the case of the coinage metals studied the observation is interpreted to su… Show more
“…First evidence of electronic excitations in H atom interactions with surfaces was provided by experiments using Schottky diodes and metal-insulator-metal devices to measure the chemicurrent produced by H atom adsorption or by the H-H recombination reaction on metal surfaces. [4][5][6][7] The experimental findings inspired several theoretical studies. [8][9][10][11][12] However, the only experimental observable here is the chemicurrent that is strongly dependent on the design of the sensor making comparison to theory difficult.…”
Efficient transfer of translational energy to electron-hole pair excitation involving multiple collisions dominates H atom collisions with metal surfaces. For this reason, H atom interaction with metal surfaces cannot be modeled within the commonly used Born-Oppenheimer approximation (BOA). This fact makes H atom scattering from metal surfaces an ideal model system for dynamics that go beyond the BOA. We chose the H/Au(111) system as a model system to obtain a detailed dataset that can serve as a benchmark for theoretical models developed for describing electronically nonadiabatic processes at metal surfaces. Therefore, we investigate the influence of various experimental parameters on the energy loss in detail including isotopic variant, incidence translational energy, incidence polar and azimuthal angles, and outgoing scattering angles.
“…First evidence of electronic excitations in H atom interactions with surfaces was provided by experiments using Schottky diodes and metal-insulator-metal devices to measure the chemicurrent produced by H atom adsorption or by the H-H recombination reaction on metal surfaces. [4][5][6][7] The experimental findings inspired several theoretical studies. [8][9][10][11][12] However, the only experimental observable here is the chemicurrent that is strongly dependent on the design of the sensor making comparison to theory difficult.…”
Efficient transfer of translational energy to electron-hole pair excitation involving multiple collisions dominates H atom collisions with metal surfaces. For this reason, H atom interaction with metal surfaces cannot be modeled within the commonly used Born-Oppenheimer approximation (BOA). This fact makes H atom scattering from metal surfaces an ideal model system for dynamics that go beyond the BOA. We chose the H/Au(111) system as a model system to obtain a detailed dataset that can serve as a benchmark for theoretical models developed for describing electronically nonadiabatic processes at metal surfaces. Therefore, we investigate the influence of various experimental parameters on the energy loss in detail including isotopic variant, incidence translational energy, incidence polar and azimuthal angles, and outgoing scattering angles.
“…Experiments on reaction of H with H adsorbed to Au observe ehp excitation, which has been attributed to the Langmuir-Hinshelwood recombination reaction. 30,31 However, by themselves these experiments give no information on the extent to which ehp excitation affects the reverse dissociative chemisorption probability, and ehp excitation is also observed in experiments on reaction of H with H adsorbed on Cu surfaces 31 although the dissociation of H 2 on Cu( 111) is described quite well with electronically adiabatic theory. 19,20,32 Calculations using ab initio molecular dynamics with electronic friction (AIMDEF) on H 2 + Pd(100) do show that the dissociation of H 2 on a metal surface can be accompanied by substantial energy dissipation to ehps, but this dissipation takes place at the product side of the barrier.…”
We have performed calculations on the dissociative chemisorption of H on un-reconstructed and reconstructed Au(111) with density functional theory, and dynamics calculations on this process on un-reconstructed Au(111). Due to a very late barrier for dissociation, H + Au(111) is a candidate H-metal system for which the dissociative chemisorption could be considerably affected by the energy transfer to electron-hole pairs. Minimum barrier geometries and potential energy surfaces were computed for six density functionals. The functionals tested yield minimum barrier heights in the range of 1.15-1.6 eV, and barriers that are even later than found for the similar H + Cu(111) system. The potential energy surfaces have been used in quasi-classical trajectory calculations of the initial (v,J) state resolved reaction probability for several vibrational states v and rotational states J of H and D. Our calculations may serve as predictions for state-resolved associative desorption experiments, from which initial state-resolved dissociative chemisorption probabilities can be extracted by invoking detailed balance. The vibrational efficacy η reported for D dissociating on un-reconstructed Au(111) (about 0.9) is similar to that found in earlier quantum dynamics calculations on H + Ag(111), but larger than found for D + Cu(111). With the two functionals tested most extensively, the reactivity of H and D exhibits an almost monotonic increase with increasing rotational quantum number J. Test calculations suggest that, for chemical accuracy (1 kcal/mol), the herringbone reconstruction of Au(111) should be modeled.
“…Part of this argument can be based on the findings of recent density functional theory (DFT) calculations, which suggest that the surface reconstruction only has a small influence on the interaction of surface adsorbed H-atoms with Au(111). 59 A further reason for studying H + Au(111) is that, like H + Cu(111), 60 H + Au(111) has been the subject of recent experiments that have measured ehp excitation in interactions of H-atoms with metal surfaces, and have made attempts to determine whether the observed ehp excitation could be attributed to ER or to associative desorption reactions. [60][61][62] Furthermore, experiments using a Schottky diode detector have detected ehp excitation in scattering of thermal H-atoms from Cu and Ag surfaces in the form of chemicurrents, 63 and such experiments have determined ehp excitation energy distributions for both thermal H-and D-atoms scattering from Ag surfaces.…”
Section: Introductionmentioning
confidence: 99%
“…59 A further reason for studying H + Au(111) is that, like H + Cu(111), 60 H + Au(111) has been the subject of recent experiments that have measured ehp excitation in interactions of H-atoms with metal surfaces, and have made attempts to determine whether the observed ehp excitation could be attributed to ER or to associative desorption reactions. [60][61][62] Furthermore, experiments using a Schottky diode detector have detected ehp excitation in scattering of thermal H-atoms from Cu and Ag surfaces in the form of chemicurrents, 63 and such experiments have determined ehp excitation energy distributions for both thermal H-and D-atoms scattering from Ag surfaces. 64,65 Electron emission from Cu, Ag, and Au surfaces induced by hyperthermal H-and D-atoms incident in plasma beams (with energies between 15 and 200 eV) has been studied by Kovacs et al 66 Much earlier, electron-hole pair excitation induced by hyperthermal Xe and Kr atoms incident on semi-conductor surfaces had been studied experimentally by Weiss et al 67 Scattering of H-atoms from copper surfaces has been investigated with electronically adiabatic models in a number of theoretical studies.…”
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