Fractional quantum Hall effect is a strongly interacting topological phase of matter that has been experimentally observed and exists beyond the reasonable doubt. It naturally occurs in clean two-dimensional heterostructures at low temperatures and in strong magnetic fields. Groundstate physics of a fractional quantum Hall phase is traditionally described using topological quantum field theory, which encodes information about transport properties as well as statistics of topologically non-trivial quasiparticles aka anyons.