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Physical Review A

Subspaces without locally distinguishable orthonormal bases

Wei Jiang, Xi-Jun Ren, Xingxiang Zhou, Zheng-Wei Zhou, Guang‐Can Guo

Published Mar 24, 2009• 6 citations
Publisher

Abstract

In this paper, we find subspaces that have no locally distinguishable orthonormal bases. For a ${C}^{m}\ensuremath{\bigotimes}{C}^{n}$ $(m,n\ensuremath{\ge}3)$ bipartite tensor system, we show that the orthogonal complement of the space spanned by a Schmidt rank-3 maximally entangled state is such a subspace. We further demonstrate that, when both parties' dimensions are greater than three, the orthogonal complement of the space spanned by any entangled state whose Schmidt rank is greater than three has no locally distinguishable orthonormal bases. Although derived using a scheme simpler than previous methods, our results are much more general than known before.

DOI
10.1103/physreva.79.032330

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In this paper, we find subspaces that have no locally distinguishable orthonormal bases. For a Cm\ensuremath⨂Cn{C}^{m}\ensuremath{\bigotimes}{C}^{n}Cm\ensuremath⨂Cn (m,n\ensuremath≥3)(m,n\ensuremath{\ge}3)(m,n\ensuremath≥3) bipartite tensor system, we show that the orthogonal complement of the space spanned by a Schmidt rank-3 maximally entangled state is such a subspace. We further demonstrate that, when both parties' dimensions are greater than three, the orthogonal complement of the space spanned by any entangled state whose Schmidt rank is greater than three has no locally distinguishable orthonormal bases. Although derived using a scheme simpler than previous methods, our results are much more general than known before.
In this paper, we study the distinguishability of multipartite quantum states by separable operations. We first present a necessary and sufficient condition for a finite set of orthogonal quantum states to be distinguishable by separable operations. An analytical version of this condition is derived for the case of(D-1) pure states, whereDis the total dimension of the state space under consideration. A number of interesting consequences of this result are then carefully investigated. Remarkably, we show there exists a large class of 2 otimes 2 separable operations not being realizable by local operations and classical communication. Before our work, only a class of 3 otimes 3 nonlocal separable operations was known [Bennett , Phys. Rev. A 59, 1070 (1999)]. We also show that any basis of the orthogonal complement of a multipartite pure state is indistinguishable by separable operations if and only if this state cannot be a superposition of one or two orthogonal product states, i.e., has an orthogonal Schmidt number not less than three, thus generalize the recent work about indistinguishable bipartite subspaces [Watrous, Phys. Rev. Lett. 95, 080505 (2005)]. Notably, we obtain an explicit construction of indistinguishable subspaces of dimension 7 (or 6) by considering a composite quantum system consisting of two qutrits (resp., three qubits), which is slightly better than the previously known indistinguishable bipartite subspace with dimension 8.
We study the local distinguishability of general multi-qubit states and show that local projective measurements and classical communication are as powerful as the most general local measurements and classical communication. Remarkably, this indicates that the local distinguishability of multi-qubit states can be decided efficiently. Another useful consequence is that a set of orthogonal nnn-qubit states is locally distinguishable only if the summation of their orthogonal Schmidt numbers is less than the total dimension 2n2^n2n. When n=2n=2n=2 such a condition is also sufficient. Employing these results, we show that any orthonormal basis of a subspace spanned by arbitrary three-qubit orthogonal unextendible product bases (UPB) cannot be exactly distinguishable by local operations and classical communication. This not only reveals another intrinsic property of three-qubit orthogonal UPB, but also provides a class of locally indistinguishable subspaces with dimension 4. We also explicitly construct locally indistinguishable subspaces with dimensions 3 and 5, respectively. In particular, 3 is the minimal possible dimension of locally indistinguishable subspaces. Combining with the previous results, we conclude that any positive integer between 3 and 7 is the possible dimension of some three-qubit locally indistinguishable subspace.
We study the local distinguishability of general multiqubit states and show that local projective measurements and classical communication are as powerful as the most general local measurements and classical communication. Remarkably, this indicates that the local distinguishability of multiqubit states can be decided efficiently. Another useful consequence is that a set of orthogonal nnn-qubit states is locally distinguishable only if the summation of their orthogonal Schmidt numbers is less than the total dimension 2n{2}^{n}2n. Employing these results, we show that any orthonormal basis of a subspace spanned by arbitrary three-qubit orthogonal unextendible product bases (UPB) cannot be exactly distinguishable by local operations and classical communication. This not only reveals another intrinsic property of three-qubit orthogonal UPB but also provides a class of locally indistinguishable subspaces with dimension 444. We also explicitly construct locally indistinguishable subspaces with dimensions 333 and 555, respectively. Similar to the bipartite case, these results on multipartite locally indistinguishable subspaces can be used to estimate the one-shot environment-assisted classical capacity of a class of quantum broadcast channels.
We study Schmidt rank for a vector (i.e., a pure state) and Schmidt number for a mixed state which are entanglement measures. We show that if a subspace of a certain bipartite system contains no vector of Schmidt rank ⩽k\leqslant k⩽k, then any state supported on that space has Schmidt number at least k+1k+1k+1. A construction of subspace of Cm⊗Cn\mathbb{C}^m \otimes \mathbb{C}^nCm⊗Cn of maximal dimension, which does not contain any vector of Schmidt rank less than 333, is given here.
We consider the question of how large a subspace of a given bipartite quantum system can be when the subspace contains only highly entangled states. This is motivated in part by results of Hayden et al. [e-print arXiv:quant-ph∕0407049; Commun. Math. Phys., 265, 95 (2006)], which show that in large d×d-dimensional systems there exist random subspaces of dimension almost d2, all of whose states have entropy of entanglement at least logd−O(1). It is also a generalization of results on the dimension of completely entangled subspaces, which have connections with the construction of unextendible product bases. Here we take as entanglement measure the Schmidt rank, and determine, for every pair of local dimensions dA and dB, and every r, the largest dimension of a subspace consisting only of entangled states of Schmidt rank r or larger. This exact answer is a significant improvement on the best bounds that can be obtained using the random subspace techniques in Hayden et al. We also determine the converse: the largest dimension of a subspace with an upper bound on the Schmidt rank. Finally, we discuss the question of subspaces containing only states with Schmidt equal to r.