  We revisit the problem of baryons in the large N limit of Quantum
Chromodynamics. A special case in which the theory of Skyrmions is inapplicable
is one-flavor QCD, where there are no light pions to construct the baryon from.
More generally, the description of baryons made out of predominantly one flavor
within the Skyrmion model is unsatisfactory. We propose a model for such
baryons, where the baryons are interpreted as quantum Hall droplets. An
important element in our construction is an extended, 2+1 dimensional,
meta-stable configuration of the $\eta'$ particle. Baryon number is identified
with a magnetic symmetry on the 2+1 dimensional sheet. If the sheet has a
boundary, there are finite energy chiral excitations which carry baryon number.
These chiral excitations are analogous to the electron in the fractional
quantum Hall effect. Studying the chiral vertex operators we are able to
determine the spin, isospin, and certain excitations of the droplet. In
addition, balancing the tension of the droplet against the energy stored at the
boundary we estimate the size and mass of the baryons. The mass, size, spin,
isospin, and excitations that we find agree with phenomenological expectations.
