Abstract

We improve Knabe's spectral gap bound for frustration-free translation-invariant local Hamiltonians in 1D. The bound is based on a relationship between global and local gaps. The global gap is the spectral gap of a size-mm chain with periodic boundary conditions, while the local gap is that of a subchain of size n<mn<m with open boundary conditions. Knabe proved that if the local gap is larger than the threshold value 1/(n−1)1/(n-1) for some n>2n>2, then the global gap is lower bounded by a positive constant in the thermodynamic limit m→∞m\rightarrow \infty. Here we improve the threshold to 6n(n+1)\frac{6}{n(n+1)}, which is better (smaller) for all n>3n>3 and which is asymptotically optimal. As a corollary we establish a surprising fact about 1D translation-invariant frustration-free systems that are gapless in the thermodynamic limit: for any such system the spectral gap of a size-nn chain with open boundary conditions is upper bounded as O(n−2)O(n^{-2}). This contrasts with gapless frustrated systems where the gap can be Θ(n−1)Θ(n^{-1}). It also limits the extent to which the area law is violated in these frustration-free systems, since it implies that the half-chain entanglement entropy is O(1/ε)O(1/\sqrtε) as a function of spectral gap εε. We extend our results to frustration-free systems on a 2D square lattice.

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