By directly diagonalizing the many-body interacting Hamiltonian for tw
o-model confinement potentials, we calculate the dipole-allowed optica
l-transition Spectra for a few electrons confined in a small quantum d
ot subjected to a strong external magnetic field. We find substantial
and qualitative many-body corrections to the optical-transition energi
es for quartic and flat-bottomed parabolic confinement in contrast to
the well-studied purely parabolic confinement where optical transition
s are known to be unaffected by interaction effects by virtue of the g
eneralized Kohn's theorem. We predict strong non-monotonic structures
as a function of the magnetic field in the magneto-optical excitation
energy spectrum.