A systematic theoretical and computational investigation of the microscopic
factors which determine the phase of the signal field in time-resolved qua
sidegenerate three-pulse scattering experiments is presented. The third-ord
er phase-matched response is obtained by density-matrix perturbation theory
using a Green-function formalism for a system composed of two well-separat
ed sets of closely spaced energy levels. Equations for calculating the elec
tric field of four-wave mixing signals generated by path-length delayed pul
ses are given. It is found that the phase of the signal field is determined
by the excitation pulse phases, the dynamics of the nonlinear polarization
decay, the product of four transition dipole matrix elements, and by a pul
se-delay-dependent phase modulation at the frequency of the first dipole os
cillation in the four-wave-mixing process. Analytic results for a two-level
Bloch model show the phase shift from rapid nonlinear polarization decoy.
The product of dipole matrix elements is real and positive for three-level
processes (bleached ground-state absorption and excited-state emission), bu
t can be real and negative for some four-level Raman processes. The pulse-d
elay-dependent phase modulation treated here is closely related to the inte
rferometric pulse-delay-dependent amplitude modulation observed in some col
linear experiments, and plays a role in producing photon echos in inhomogen
eously broadened samples. Numerical calculations of phase-resolved electric
fields for finite duration pulses using a Brownian oscillator model approp
riate for condensed-phase dynamics ore presented. The ability of pulse-dela
y-dependent phase modulation to encode the frequency of the initially excit
ed dipole onto the phase of the signal field can be exploited to examine en
ergy-level connectivity, reveal correlations hidden under the inhomogeneous
lineshape, and probe relaxation pathways in multilevel systems.