We have experimentally observed the pattern instabilities of an Ising wall
formed in a nematic or cholesteric liquid crystal layer. We have deduced an
envelope equation, relevant close to the Freedericksz transition, from whi
ch we derived an equation for the dynamics of the interface in the vicinity
of itu bifurcation. In the case of the zig-zag instability, this model is
characterized by a conservative and variational order parameter whose gradi
ent satisfies a Cahn-Hilliard equation. We have also investigated the influ
ence of slightly broken symmetries on the dynamical behaviour of the system
. The disappearance of the interface translational invariance or of the ref
lection symmetry along the wall axis may induce new interfacial patterns wh
ich have been both experimentally and theoretically pointed out.