Dark matter, if represented by a ℤ2-symmetric scalar field, can manifest as
both particles and condensates. In this paper, we study the evolution of an oscillating
homogeneous condensate of a ℤ2-symmetric scalar field in a thermal plasma in an FLRW
universe. We focus on the perturbative regime where the oscillation amplitude is sufficiently
small so that parametric resonance is inefficient. This perturbative regime necessarily comprises
the late stage of the condensate decay and determines its fate. The coupled coarse-grained
equations of motion for the condensate, radiation, and spacetime are derived from first principles
using nonequilibrium quantum field theory. We obtain analytical expressions for the relevant
microscopic quantities that enter the equations of motion and solve the latter numerically. We
find that there is always a nonvanishing relic abundance for a condensate with a ℤ2
symmetry that is not spontaneously broken. This is because its decay rate decreases faster than
the Hubble parameter at late times due to either the amplitude dependence or the temperature
dependence in the condensate decay rate. Consequently, accounting for the condensate contribution
to the overall dark matter relic density is essential for ℤ2 scalar singlet
dark matter.