  The formations of the $K(\bar{K})$, $D(\bar{D})$, and $B(\bar{B})$
meson-nucleus bound states in $^{16}O$, $^{40}Ca$, $^{90}Zr$, $^{197}Au$, and
$^{208}Pb$ nucleus are investigated using the quark meson coupling model. The
model relies on a mean field description of non-overlapping nucleon bags bound
by the self-consistent interactions of scalar ($\sigma$, $\delta$) and vector
($\omega$, $\rho$) mesons with the (anti)quarks inside the bags, which is
further extended to explore the properties of nuclei. We estimate the
meson-nucleus bound state energies by solving the Klein-Gordon equations with
the real potentials calculated self-consistently within the model, using a
coordinate space approach. The calculations are carried out for different
nuclear interactions. The effects of Coulomb interaction are considered in the
present study for the charged mesons. Our study indicates the formation of
rather deeply bound $B$-mesic states at the very central region of the nuclei,
compared to the $D$ and $K$ mesons, offering a more promising probe to explore
subtle nuclear medium effects. The investigations of such bound states are of
particular interest for the upcoming $\rm{\bar{P}ANDA}$ at FAIR, J-PARC-E29 and
JLab experiments.
