  We show the low-lying excitations at filling factor $\nu=n+1/3$ with
realistic interactions are contained completely within the well-defined Hilbert
space of "Gaffnian quasiholes". Each Laughlin quasihole can thus be understood
as a bound state of two Gaffnian quasiholes, which in the lowest Landau level
(LLL) behaves like "partons" with "asymptotic freedom" mediated by neutral
excitations acting as "gluons". Near the experimentally observed nematic FQH
phase in higher LLs, quasiholes become weakly bounded and fractionalise with
rich dynamical properties. By studying the effective interactions between
quasiholes, we predict a finite temperature phase transition of the Laughlin
quasiholes even when the Laughlin ground state remains incompressible, and
derive relevant experimental conditions for its possible observations.
