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Constructing locally indistinguishable orthogonal product bases in an $m \otimes n$ system

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arxiv 1512.06485 v2 pith:HQXJ2LU6 submitted 2015-12-21 quant-ph

classification quant-ph
keywords locallyotimesproductorthogonalindistinguishablebasiscompletablemembers
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abstract

Recently, Zhang et al [Phys. Rev. A 92, 012332 (2015)] presented $4d-4$ orthogonal product states that are locally indistinguishable and completable in a $d\otimes d$ quantum system. Later, Zhang et al. [arXiv: 1509.01814v2 (2015)] constructed $2n-1$ orthogonal product states that are locally indistinguishable in $m\otimes n$ ($3\leq m \leq n$). In this paper, we construct a locally indistinguishable and completable orthogonal product basis with $4p-4$ members in a general $m\otimes n$ ($3\leq m \leq n$) quantum system, where $p$ is an arbitrary integer from $3$ to $m$, and give a very simple but quite effective proof for its local indistinguishability. Specially, we get a completable orthogonal product basis with $8$ members that cannot be locally distinguished in $m\otimes n$ ($3\leq m \leq n$) when $p=3$. It is so far the smallest completable orthogonal product basis that cannot be locally distinguished in a $m\otimes n$ quantum system. On the other hand, we construct a small locally indistinguishable orthogonal product basis with $2p-1$ members, which is maybe uncompletable, in $m\otimes n$ ($3\leq m \leq n$ and $p$ is an arbitrary integer from $3$ to $m$). We also prove its local indistinguishability. As a corollary, we give an uncompletable orthogonal product basis with $5$ members that are locally indistinguishable in $m\otimes n$ ($3\leq m \leq n$). All the results can lead us to a better understanding of the structure of a locally indistinguishable product basis in $m \otimes n$.

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  1. LOCC distinguishable orthogonal product states with least entanglement resource

    quant-ph 2019-08 conditional novelty 5.0 of 10

    New explicit families of LOCC-indistinguishable orthogonal product states in bipartite systems with dimensions n and m become perfectly distinguishable by LOCC when the parties share a C^2⊗C^2 maximally entangled state.

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