📝 SummarXiv

Abstract

In this work, surface diffusion is studied with a different perspective by showing how the corresponding open dynamics is transformed when passing, in a continuous and smooth way, from a pure quantum regime to a full classical regime; the so-called quantum-to-classical transition. This continuous process is carried out from the Liouville-von Neumann equation by scaling Planck's constant. For this goal, the Brownian motion of an adsorbate on a flat surface is analyzed in order to show how this transition takes place. In particular, this open dynamics is studied from the master equation for the reduced density matrix within the Caldeira-Leggett formalism; in particular, the two extreme time behaviors, the ballistic and diffusive motions. It is also shown that the origin of the ballistic motion is different for the quantum and classical regimes. In this scenario, the corresponding Gaussian function for the intermediate scattering function is governed by the thermal velocity in the classical regime versus the initial spreading velocity of the wave packet for the quantum regime, leading to speak of classical and quantum ideal gas, respectively. Finally, in the diffusive regime, and starting from the Chudley-Elliott model, the quantum-to-classical transition is also discussed in terms of the well-known H-function for three surface temperatures in the diffusion of H and D on a Pt(111) surface. The main goal in this analysis is if one can discriminate the irreversibility coming from tunneling and thermal activation diffusion.