This feels a little trivial, but I don't see why it isn't an example of what you want: Seiberg duality typically relates an SU(Nc) gauge theory with Nf flavors to an SU(Nf−Nc) gauge theory. There are degenerate cases when Nf−Nc=1 or 0, which don't correspond to any dynamical gauge group in the infrared. These are usually described in terms of quantum moduli spaces (s-confining when Nf=Nc+1 and chiral symmetry breaking when Nf=Nc), with the low energy fields given by mesons and baryons, but you can equally well describe these as the "dual" quarks and mesons of the usual Seiberg duality, in a degenerate limit without gauge fields coupling to them.
Of course, in the same sense, nonsupersymmetric QCD is dual to a theory of massless pions and no gauge symmetry.
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