Abstract

In this paper, we describe a new and fully coherent stochastic surface hopping method for simulating mixed quantum-classical systems. We illustrate the approach on the simple but unforgiving problem of quantum evolution of a two-state quantum system in the limit of unperturbed pure state dynamics and for dissipative evolution in the presence of both stationary and nonstationary random environments. We formulate our approach in the Liouville representation and describe the density matrix elements by ensembles of trajectories. Population dynamics are represented by stochastic surface hops for trajectories representing diagonal density matrix elements. These are combined with an unconventional coherent stochastic hopping algorithm for trajectories representing off-diagonal quantum coherences. The latter generalizes the binary (0,1) "probability" of a trajectory to be associated with a given state to allow integers that can be negative or greater than unity in magnitude. Unlike existing surface hopping methods, the dynamics of the ensembles are fully entangled, correctly capturing the coherent and nonlocal structure of quantum mechanics.

Highlights

  • We describe a new and fully coherent stochastic surface hopping method for simulating mixed quantum-classical systems

  • We formulate our approach in the Liouville representation and describe the density matrix elements by ensembles of trajectories

  • Population dynamics are represented by stochastic surface hops for trajectories representing diagonal density matrix elements

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Summary

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We describe a new and fully coherent stochastic surface hopping method for simulating mixed quantum-classical systems. Population dynamics are represented by stochastic surface hops for trajectories representing diagonal density matrix elements These are combined with an unconventional coherent stochastic hopping algorithm for trajectories representing off-diagonal quantum coherences. A range of theoretical quantumclassical methods have been proposed to treat such systems These include trajectory surface hopping, semiclassical initial value representation, and quantum-classical Wigner function-based approaches, to cite just a few. The most popular method for combining classical dynamics with quantum transitions is trajectory surface hopping, and, in particular, variants of Tully’s fewest switches surface hopping (FSSH).. The most popular method for combining classical dynamics with quantum transitions is trajectory surface hopping, and, in particular, variants of Tully’s fewest switches surface hopping (FSSH).2 Together, these methods are well-known for their mistreatment of coherence. We formulate our approach in the Liouville representation and describe the quantum evolution by a density matrix. The

Hamiltonian of the system is given by
The real and imaginary parts give the relations
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