There are few general physical principles that protect the low energy
excitations of a quantum phase. Of these, Goldstone's theorem and Landau Fermi
liquid theory are the most relevant to solids. We investigate the stability of
the resulting gapless excitations - Nambu Goldstone bosons (NGBs) and Landau
quasiparticles - when coupled to one another, which is of direct relevance to
metals with a broken continuous symmetry. Typically, the coupling between NGBs
and Landau quasiparticles vanishes at low energies leaving the gapless modes
unaffected. If however the low energy coupling is non-vanishing, non-Fermi
liquid behavior and overdamped bosons are expected. Here we prove a general
criterion which specifies when the coupling is non-vanishing. It is satisfied
by the case of a nematic Fermi fluid, consistent with earlier microscopic
calculations. In addition, the criterion identifies a new kind of symmetry
breaking - of magnetic translations - where non-vanishing couplings should
arise, opening a new route to realizing non-Fermi liquid phases.Comment: 6 pages + 10 pages (Supplemental Material), 3 + 2 figures; v2:revised
for clarit