English

Grassmannian and Flag sigma models on interval: phase structure and L-dependence

High Energy Physics - Theory 2019-12-17 v3

Abstract

We discuss the two-dimensional Grassmannian SU(N)/S(U(N2)×U(2))SU(N)/S(U(N-2)\times U(2)) and the flag SU(N)/S(U(N2)×U(1)×U(1))SU(N)/S(U(N-2)\times U(1)\times U(1)) 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 LL and undergoes a phase transition from the phase of partly broken gauge symmetry (U(1)U(1)) to the symmetric phase (U(1)×U(1)U(1)\times U(1)) for large LL. On the other hand, the Grassmannian model has a detached phase with one massive and one massless non-zero condensates that completely break U(2)U(2) gauge symmetry. This phase lives on a region of LL 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.

Cite

@article{arxiv.1905.02416,
  title  = {Grassmannian and Flag sigma models on interval: phase structure and L-dependence},
  author = {D. Pavshinkin},
  journal= {arXiv preprint arXiv:1905.02416},
  year   = {2019}
}

Comments

13 pages, 1 figure. The generalization of the previous results to periodic, periodic twisted and unmixed DD, NN boundaries is discussed in Conclusion

R2 v1 2026-06-23T08:58:56.388Z