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The dynamics of the scanning tunneling microscope (STM)-induced desorption of hydrogen atoms from Si(100)−(2 × 1):H (D) surfaces in the “above electronic threshold limit”, which is believed to proceed via a short-lived σ → σ* resonance, is investigated theoretically. We use both time-dependent wave packet and density matrix methods and compare them to classical mechanics. Isotope effects in the desorption yields and desorbate translational energies, the role of coordinate-dependent electronic relaxation, and finally the dependence of the observables on the surface temperature T s are addressed. In agreement with experiment we find no significant dependence of the isotope effect in the desorption yield up to T s ≈ 300 K. However, for higher T s a substantial decrease of the ratio between H and D yield is predicted.
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Boendgen et al. (1998) studied this question.
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