We derive and analyse a normal form governing dynamics of Hopf bifurca
tions of partial differential evolution equations on a square domain.
We assume that the differential operator for the linearized problem de
composes into two one-dimensional self-adjoint operators and a local '
reaction' operator; this gives a basis of i.e. of the form u(x(1),x(2)
) = f(1)(x(1))f(2)(x(2)). The normal form reduces to that investigated
by Swift [23] for bifurcation of modes with odd parity but is new for
modes with even parity where the centre eigenspace carries a reducibl
e action of D-4 x S-1. We consider the Brusselator equations as an exa
mple and discover that a separable linearization introduces a degenera
cy which causes the three` new third order terms in the normal form to
be related in an unexpected but simple way.