  Phase separation plays an role in determining the self-assembly of biological
and soft-matter systems. In biological systems, liquid-liquid phase separation
inside a cell leads to the formation of various macromolecular aggregates. The
interaction among these aggregates is soft, i.e., these can significantly
overlap at a small energy cost. From the computer simulation point of view,
these complex macromolecular aggregates are generally modeled by the so-called
soft particles. The effective interaction between two particles is defined via
the generalized exponential potential (GEM-n) with n = 4. Here, using molecular
dynamics simulations, we study the phase separation dynamics of a
size-symmetric binary mixture of ultrasoft particles. We find that when the
mixture is quenched to a lower temperature below the critical temperature, the
two components spontaneously start to separate. Domains of the two components
form, and the equal-time order parameter reveals that the domains grow in a
power-law manner with exponent 1/3, which is consistent with the
Lifshitz-Slyozov law for conserved systems. Further, the static structure
factor shows a power-law decay with exponent 4 consistent with the Porod law.
