  Charm and bottom transport coefficients in a medium constituted of light
mesons, such as is formed in the hadronic phase of Heavy Ion Collisions, are
obtained within an effective field theory approach implementing heavy quark
symmetry and chiral symmetry breaking. Heavy flavor propagates in the medium as
$D/B$ and $D^*/B^*$ degrees of freedom, and unitarization of the lowest order
heavy-light meson amplitudes is used in order to reach high temperatures. The
latter accounts for dynamically generated resonances in isospin 1/2 channels, a
feature that leads to a more efficient heavy flavor diffussion. We discuss the
temperature and momentum dependence of the friction and diffusion coefficients
in a transport approach up to temperatures of about $T\simeq 150$ MeV, and
provide estimates of the charm/bottom relaxation lengths and momentum loss.
Implications for heavy meson spectrum observables in Heavy Ion Collisions are
discussed.
