We discuss the two-dimensional Grassmannian and the flag sigma models on a finite interval and construct analytical solutions of gap equations in the large N limit. We show that the flag model admits a homogeneous solution for `mixed’ Dirichlet-Neumann (DN) boundary conditions only for sufficiently large length and undergoes a phase transition from the phase of partly broken gauge symmetry () to the symmetric phase () for large . On the other hand, the Grassmannian model has a detached phase with one massive and one massless non-zero condensates that completely break gauge symmetry. This phase lives on a region of bounded from above and has to use the Robin boundary conditions. We also examine the L-dependence of the total energy and detect the linear growth inherent to confining string in all phases.

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