We consider the charged excitations in the quantum Hall effect with a large
Zeeman splitting at filling factor v=2, When the Zeeman splitting is incre
ased over a critical value the ground state undergoes a first order phase t
ransition from a paramagnetic to a ferromagnetic phase. We have studied the
possibility of forming charged spin-textured excitations, "inter-Landau-le
vel skyrmions," close to this transition; and find that these are never the
lowest lying charged excitations but can under certain conditions provide
an effective driving mechanism for the paramagnetic to ferromagnetic phase
transition. We show that the charged excitations inevitably present in the
system can act as nucleation centers even at T = 0 and hence set a specific
limit for the maximal hysteresis attainable in this case. Calculations of
how the finite width of the two-dimensional electron gas affects the v = 2
phase transition ans of the olarization at higher filling factors are also
presented.