Topological and nematic ordered phases in many-body cluster-Ising models
arXiv:1503.08598 · doi:10.1103/PhysRevA.92.012306
Abstract
We present a fully analytically solvable family of models with many-body cluster interaction and Ising interaction. This family exhibits two phases, dubbed cluster and Ising phases, respectively. The critical point turns out to be independent of the cluster size and is reached exactly when both interactions are equally weighted. For even we prove that the cluster phase corresponds to a nematic ordered phase and in the case of odd to a symmetry protected topological ordered phase. Though complex, we are able to quantify the multi-particle entanglement content of neighboring spins. We prove that there exists no bipartite or, in more detail, no -partite entanglement. This is possible since the non-trivial symmetries of the Hamiltonian restrict the state space. Indeed, only if the Ising interaction is strong enough (local) genuine -partite entanglement is built up. Due to their analytically solvableness the -cluster-Ising models serve as a prototype for studying non trivial-spin orderings and due to their peculiar entanglement properties they serve as a potential reference system for the performance of quantum information tasks.
arXiv comment10 pages, 9 figures
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