A recent development on the working of effective field theories in nuc
lei and in dense hadronic matter is discussed. We consider two extreme
regimes: One, dilute regime for which fluctuations are made on top of
the matter-free vacuum; two, dense systems for which fluctuations are
treated on top of the ''vacuum'' defined at a given density, with mas
ses and coupling constants varying as function of matter density (''Br
own-Rho scaling''). Based on an intricate - as yet mostly conjectural
- connection between the in-medium structure of chiral Lagrangian fiel
d theory which is a beautiful effective theory of QCD and that of Land
au Fermi liquid theory which is an equally beautiful and highly succes
sful effective theory of many-body systems, it is suggested that a chi
ral Lagrangian with Brown-Rho scaling in the mean field is equivalent
to Fermi-liquid fixed point theory. I make this connection using elect
roweak and strong responses of nuclear matter up to nuclear matter den
sity and then extrapolating to higher densities encountered in heavy-i
on collisions and compact stars.