  We propose a hydrodynamics theory of collective quantum Hall states, which
describes incompressible liquids, hexatic liquid crystals, a bubble solid and a
Wigner crystal states within a unified framework. The structure of the theory
is uniquely determined by the space-time symmetry, and a symmetry with respect
to static shear deformations. In agreement with recent experiments the theory
predicts two gapped collective modes for incompressible liquids. We argue that
the presence of the above two modes is a universal property of a magnetized
two-dimensional collective liquid.

Mesoscale and Nanoscale Physics;Strongly Correlated Electrons