The recently formulated mixed quantum classical rate theory (MQCLT) is impl
emented for a model system with two degrees of freedom. In MQCLT, one must
compute the Wigner representation of the symmetrized thermal flux operator.
This phase space flux distribution is then multiplied by the classical rea
ction probability to obtain the rate. The major computational difficulty is
the multidimensional Fourier transform necessary for obtaining the Wigner
distribution. The Fourier transform reintroduces a sign problem when attemp
ting to estimate the MQCLT rate using Monte Carlo methods. Two different me
thods for overcoming the sign problem are explored in this paper. Numerical
results are presented for a model problem of an Eckart barrier coupled bil
inearly to a slow oscillator and compared with numerically exact results. (
C) 1999 American Institute of Physics. [S0021-9606(99)02740-3].