  1) For the hard core interaction there is some freedom left in the choice of
the exact multiskyrmionic wave function's topology. The statistics of textured
quasiholes, analyzed by calculation of the Berry phase, depends on this choice
of topology.
  2) We find a class of textured two-hole eigenstates of the Coulomb
interaction. There is no definite quantum statistics but there is a definite
rule of how to construct Coulomb eigenstates out of the hard core wave
functions.
  3) A wave function for the 5/2 state is constructed according to this rule.
