The pseudopotentials describing interaction of Laughlin quasielectrons (QE)
and quasiholes (QH) in an infinite fractional quantum Hall system are stud
ied. The QE and QH pseudopotentials are similar, which suggests the (approx
imate) particle-hole symmetry recovered in the thermodynamical limit. The p
roblem of the hypothetical symmetry-breaking QE hard-core repulsion is reso
lved by the estimate that the "forbidden'' QE pair state has too high an en
ergy and is unstable. Strong oscillations of the QE and QH pseudopotentials
persist in an infinite system, and the analogous QE and QH pair states wit
h small relative angular momentum and nearly vanishing interaction energy a
re predicted.