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Beyond Ehrenfest: correlated non-adiabatic molecular dynamics

Andrew P Horsfield et al 2004 J. Phys.: Condens. Matter 16 8251-8266   doi: 10.1088/0953-8984/16/46/012  Help

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Andrew P Horsfield1, D R Bowler1,2, A J Fisher1,2, Tchavdar N Todorov3 and Cristián G Sánchez3
1 Department of Physics and Astronomy, University College London, Gower Street, London WC1E 6BT, UK
2 London Centre for Nanotechnology, University College London, Gower Street, London WC1E 6BT, UK
3 School of Mathematics and Physics, Queen's University of Belfast, Belfast BT7 1NN, UK
E-mail: a.horsfield@ucl.ac.uk, david.bowler@ucl.ac.uk and t.todorov@qub.ac.uk

Abstract. A method for introducing correlations between electrons and ions that is computationally affordable is described. The central assumption is that the ionic wavefunctions are narrow, which makes possible a moment expansion for the full density matrix. To make the problem tractable we reduce the remaining many-electron problem to a single-electron problem by performing a trace over all electronic degrees of freedom except one. This introduces both one- and two-electron quantities into the equations of motion. Quantities depending on more than one electron are removed by making a Hartree–Fock approximation. Using the first-moment approximation, we perform a number of tight binding simulations of the effect of an electric current on a mobile atom. The classical contribution to the ionic kinetic energy exhibits cooling and is independent of the bias. The quantum contribution exhibits strong heating, with the heating rate proportional to the bias. However, increased scattering of electrons with increasing ionic kinetic energy is not observed. This effect requires the introduction of the second moment.

Print publication: Issue 46 (24 November 2004)
Received 2 August 2004, in final form 11 October 2004
Published 5 November 2004

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