Locality at the boundary implies gap in the bulk for 2D PEPS
arXiv:1709.07691 · doi:10.1007/s00220-019-03404-9
Abstract
Proving that the parent Hamiltonian of a Projected Entangled Pair State (PEPS) is gapped remains an important open problem. We take a step forward in solving this problem by showing two results: first, we identify an approximate factorization condition on the boundary state of rectangular subregions that is sufficient to prove that the parent Hamiltonian of the bulk 2D PEPS has a constant gap in the thermodynamic limit; second, we then show that Gibbs state of a local, finite-range Hamiltonian satisfy such condition. The proof applies to the case of injective and MPO-injective PEPS, employs the martingale method of nearly commuting projectors, and exploits a result of Araki on the robustness of one dimensional Gibbs states. Our result provides one of the first rigorous connections between boundary theories and dynamical properties in an interacting many body system.
31 pages, 9 figures. Revised version
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- The minimal canonical form of a tensor network
- Thermalization in Kitaev's quantum double models via Tensor Network techniques
- Projector Matrix Product Operators, Anyons and Higher Relative Commutants of Subfactors
- Local topological order and boundary algebras
- Classical restrictions of generic matrix product states are quasi-locally Gibbsian
- Deformations of the Boundary Theory of the Square Lattice AKLT Model
- On a bulk gap strategy for quantum lattice models