Abstract

We investigate the von Neumann entanglement entropy as function of the size of a subsystem for permutation invariant ground states in models with finite number of states per site, e.g., in quantum spin models. We demonstrate that the entanglement entropy of nn sites in a system of length LL generically grows as σlog⁡2[2πen(L−n)/L]+Cσ\log_{2}[2πen(L-n)/L]+C, where σσ is the on-site spin and CC is a function depending only on magnetization.

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