  By means of the local, iterative Lie Schwinger block-diagonalization method,
in this paper we study the low-lying spectrum of the AKLT model perturbed by
small, finite-range potentials and with open boundary conditions imposed at the
edges of the chain. Our method allows us to control small interaction terms
localized near the boundary of the chain that are responsible for the possible
splitting of the ground-state energy of the AKLT Hamiltonian into energy levels
separated by small gaps. This improves earlier results restricted to the
persistence of the so called bulk gap.
