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Non-Adiabatic Effects in Quantum-Classical Molecular Dynamics


SC 98-38 Christof Schütte, Peter Nettesheim: Non-Adiabatic Effects in Quantum-Classical Molecular Dynamics Appeared in: F. Keil, W. Mackens et al. Scientific Computing in Chemical Engineering II, Computational Fluid Dynamics, Reaction Engineering and Molecular Properties. Springer (1999) pp. 42-56


Abstract: In molecular dynamics applications there is a growing interest in mixed quantum-classical models. The article is concerned with the so-called QCMD model. This model describes most atoms of the molecular system by the means of classical mechanics but an important, small portion of the system by the means of a wavefunction. We review the conditions under which the QCMD model is known to approximate the full quantum dynamical evolution of the system.
In most quantum-classical simulations the Born-Oppenheimer model (BO) is used. In this model, the wavefunction is adiabatically coupled to the classical motion which leads to serious approximation deficiencies with respect to non-adiabatic effects in the fully quantum dynamical description of the system. In contrast to the BO model, the QCMD model does include non-adiabatic processes, e.g., transitions between the energy levels of the quantum system. It is demonstrated that, in mildly non-adiabatic scenarios, so-called surface hopping extensions of QCMD simulations yield good approximations of the non-adiabatic effects in full quantum dynamics. The algorithmic strategy of such extensions of QCMD is explained and the crucial steps of its realization are discussed with special emphasis on the numerical problems caused by highly oscillatory phase effects.
Keywords: quantum-classical molecular dynamics, non-adiabatic processes, Schrödinger equation, highly oscillatory phase, adiabatic limit, quantum adiabatic theorem, Born-Oppenheimer model, energy level crossings, transition zone, QCMD-based surface hopping, QCMD trajectory bundle, long-stepsize integration schemes, averaging
MSC: 81Q20, 81Q15, 81S25, 81V55, 92E10