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Partial Wigner transforms and the quantum--classical Liouville equation


SC 99-10 Christof Schuette.: Partial Wigner transforms and the quantum--classical Liouville equation


Abstract: In molecular dynamics applications there is a growing interest in mixed quantum-classical models. The article is concerned with the so-called quantum-classical Liouville equation (QCL). This model describes most atoms of the molecular system by the means of classical phase space density but an important, small portion of the system by the means of a wavefunction. The QCL results from the full quantum dynamical (QD) description via applying the Wigner transform to the ``classical part of the system only. We discuss the conditions under which the QCL model approximates the full QD 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 QCL model does include non-adiabatic processes, e.g., transitions between the energy levels of the quantum system. It is demonstrated that the QCL yields good approximations of such non-adiabatic effects in full quantum dynamics.
Keywords: QCMD, quantum-classical Liouville equation, surface hopping, Wigner transform, asymptotic expansion, nonadiabatic effects
MSC: 81Q15, 81Q20