I am studying the Chern-Simons approach to fractional quantum Hall effect, which a special focus on the topological order in the context of Abelian fractional quantum Hall effect. To me, the logic to adopt (Maxwell-) Chern-Simons theory as an effective theory is pretty bottom up (says, Wen's book): We can write down a current with fractional Hall conductivity, from which we can introduce the statistical gauge fields as auxiliary fields for the effective action and it turns out to be the Chern-Simons theory. However, it seems to me that the concept of topological order is mainly based on ground state degeneracy and gapped bulk systems.
My questions are:
- Consider systems satisfy (my prototype example is Laughlin's state at filling 1/m): (i) gapped bulk; (ii) degenerate ground state; (iii) $U(1)$ charge conservation; (iv) only one kind of fractional excitation. What are the extra minimal ingredients needed to derive the corresponding effective (topological) action? Is it possible to derive the Chern-Simons theory directly, only based on these constraints?
- Also, can the fractional Hall conductivity be derived solely from these constraints?