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We study the phase diagram of interacting electrons in a dispersionless Chern band as a function of their filling. We find hierarchy multiplets of incompressible states at fillings ν = 1/3, 2/5, 3/7, 4/9, 5/9, 4/7, 3/5 as well as ν = 1/5, 2/7. These are accounted for by an analogy to Haldane pseudopotentials extracted from an analysis of the two-particle problem. Important distinctions to standard fractional quantum Hall physics are striking: in the absence of particle-hole symmetry in a single band, an interaction-induced single-hole dispersion appears, which perturbs and eventually destabilizes incompressible states as ν increases. For this reason, the nature of the state at ν = 2/3 is hard to pin down, while ν = 5/7, 4/5 do not seem to be incompressible in our system.
Läuchli et al. (Tue,) studied this question.