  We describe dynamical symmetry breaking in a system of massless Dirac
fermions with both electromagnetic and four-fermion interactions in (2+1)
dimensions. The former is described by the Pseudo Quantum Electrodynamics
(PQED) and the latter is given by the so-called Gross-Neveu action. We apply
the Hubbard-Stratonovich transformation and the large$-N_f$ expansion in our
model to obtain a Yukawa action. Thereafter, the presence of a symmetry broken
phase is inferred from the non-perturbative Schwinger-Dyson equation for the
electron propagator. This is the physical solution whenever the fine-structure
constant is larger than a critical value $\alpha_c(D N_f)$. In particular, we
obtain the critical coupling constant $\alpha_c\approx 0.36$ for $D N_f=8$.,
where $D=2,4$ corresponds to the SU(2) and SU(4) cases, respectively, and $N_f$
is the flavor number. Our results show a decreasing of the critical coupling
constant in comparison with the case of pure electromagnetic interaction, thus
yielding a more favorable scenario for the occurrence of dynamical symmetry
breaking. For two-dimensional materials,in application in condensed matter
systems, it implies an energy gap at the Dirac points or valleys of the
honeycomb lattice.
