We examine the competition between the charge-density wave (CDW) instability
and the excitonic condensate (EC) in spatially separated layers of electrons
and holes. The CDW and the EC order parameters (OPs), described by two
different mechanisms and hence two different transition temperatures
$T^{CDW}_c$ and $T^{EC}_c$, are self-consistently coupled by a microscopic mean
field theory. We discuss the results in our model specifically focusing on the
transition-metal dichalcogenides which are considered as the most typical
examples of strongly coupled CDW/EC systems with atomic layer separations where
the electronic energy scales are large with the critical temperatures in the
range $T^{EC}_c \sim T^{CDW}_c \sim 100-200 K$. An important consequence of
this is that the excitonic energy gap, hence the condensed free energy, vary
with the layer separation resulting in a new type of force ${\cal F}_{EC}$. We
discuss the possibility of this force as the possible driver of the structural
lattice deformation observed in some TMDCs with a particular attention on the $
1 {\it T}$-$TiSe_2$ below $200 K$.Comment: 8 pages, 5 figure