Abstract

Here we extend a recently introduced state-to-state kinetic model describing single- and multi-quantum vibrational excitation of molecular beams of NO scattering from a Au(111) metal surface. We derive an analytical expression for the rate of electronically non-adiabatic vibrational energy transfer, which is then employed in the analysis of the temperature dependence of the kinetics of direct overtone and two-step sequential energy transfer mechanisms. We show that the Arrhenius surface temperature dependence for vibrational excitation probability reported in many previous studies emerges as a low temperature limit of a more general solution that describes the approach to thermal equilibrium in the limit of infinite interaction time and that the pre-exponential term of the Arrhenius expression can be used not only to distinguish between the direct overtone and sequential mechanisms, but also to deduce their relative contributions. We also apply the analytical expression for the vibrational energy transfer rates introduced in this work to the full kinetic model and obtain an excellent fit to experimental data, the results of which show how to extract numerical values of the molecule-surface coupling strength and its fundamental properties.

Highlights

  • Chemical reactivity at metal surfaces plays an important role in the modern industrial world

  • metal surfaces introduced in ref

  • An analytical expression for the rate of electronically non-adiabatic vibrational energy transfer was derived within the first order perturbation theory

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Summary

Introduction

Chemical reactivity at metal surfaces plays an important role in the modern industrial world. P 1⁄4 AeÀDkbETviSb ð3Þ from the kinetic model, examine the Arrhenius pre-exponents as a function of the interaction time and the surface temperature, and to discover the departure from the Arrhenius behavior at high temperatures This analysis allows us to determine the relative importance of direct two-quantum and sequential single-quantum excitation pathways, where the latter proceeds via an intermediate NO(v = 1) state to NO(v = 2). This analysis makes it possible to relate the observed absolute vibrational excitation probabilities to the strength of electronically non-adiabatic coupling

Experimental
The rate of vibrational energy transfer
Kinetics and absolute excitation probabilities
Single-step excitation
À eÀavv0 Evv0 coth
Sequential two-step excitation
Full model and fit to experimental data
Discussion
Summary

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