The centroid effective
frequency representation of path integrals
as developed by Feynman and Kleinert was originally aimed at calculating
partition functions and related quantities in the canonical ensemble.
In its path integral formulation, only
closed
paths
were relevant. This formulation has been used by the present authors
in order to calculate the many-body Wigner function of the Boltzmann
operator, which includes also open paths. This usage of the theory
outside of the original intention can lead to mathematical divergence
issues for potentials with barriers, particularly at low temperature.
In the present paper, we modify the effective frequency theory of
Feynman and Kleinert by also including open paths in its variational
equations. In this way, a divergence-free approximation to the Boltzmann
operator matrix elements is derived. This generalized version of Feynman
and Kleinert’s formulation is thus more robust and can be applied
to all types of barriers at all temperatures. This new version is
used to calculate the Wigner functions of the Boltzmann operator for
a quartic oscillator and for a double well potential and both static
and dynamic properties are studied at several temperatures. The new
theory is found to be essentially as precise as the original one.
Its advantage is that it will always deliver a well-defined, even
if approximate, Wigner function, which can, for instance, be used
for sampling initial conditions for molecular dynamics simulations.
As will be discussed, the theory can be systematically improved by
including higher-order Fourier modes into the nonquadratic part of
the trial action.