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arxiv: 1412.3780 · v2 · pith:2JBQV2JWnew · submitted 2014-12-11 · 🪐 quant-ph

Families of pure PEPS with efficiently simulatable local hidden variable models for most measurements

classification 🪐 quant-ph
keywords measurementsconstructefficientlyquantumentangledlocalpurestates
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An important problem in quantum information theory is to understand what makes entangled quantum systems non-local or hard to simulate efficiently. In this work we consider situations in which various parties have access to a restricted set of measurements on their particles, and construct entangled quantum states that are essentially classical for those measurements. In particular, given any set of local measurements on a large enough Hilbert space whose dual strictly contains (i.e. contains an open neighborhood of) a pure state, we use the PEPS formalism and ideas from generalized probabilistic theories to construct pure multiparty entangled states that have (a) local hidden variable models, and (b) can be efficiently simulated classically. We believe that the examples we construct cannot be efficiently classically simulated using previous techniques. Without the restriction on the measurements, the states that we construct are non-local, and in some proof-of-principle cases are universal for measurement based quantum computation.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Cylindrical Matter: A beyond-quantum many-body system for efficient classical simulation of quantum pure-Ising like systems

    quant-ph 2026-04 unverdicted novelty 7.0

    Cylindrical matter is a new beyond-quantum model that faithfully reproduces measurement statistics of some quantum pure-Ising systems with interactions decaying faster than 1/r^{3D/2}, allowing classical simulation.

  2. Classically efficient regimes in measurement based quantum computation performed using diagonal two qubit gates and cluster measurements

    quant-ph 2023-07 unverdicted novelty 6.0

    Explicit computation of the classical simulation threshold λ for arbitrary diagonal two-qubit gates, identifying families of states with simulable phases on finite-degree graphs.