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We consider the fractional quantum Hall effect at the filling $\nu=6/17$,where experiments have observed features of incompressibility in the form of aminimum in the longitudinal resistance. We propose a parton state denoted as"$3\bar{2}1^{3}$" and show it to be a feasible candidate to capture the groundstate at $\nu=6/17$. We work out the low-energy effective theory of the$3\bar{2}1^{3}$ edge and make several predictions for experimentally measurableproperties of the state which can help detect its underlying topological order.Intriguingly, we find that the $3\bar{2}1^{3}$ state likely lies in the sameuniversality class as the state obtained from composite-fermionizing the 1+1/5Laughlin state.

Parton wave function for the fractional quantum Hall effect at $\nu=6/17$