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Journal of Physics A Mathematical and Theoretical

The distillability of entanglement of bipartite reduced density matrices of a tripartite state

Yize Sun, Lin Chen

Published Jun 1, 2020• 4 citations
Publisher

Abstract

Abstract The relation between the distillability of entanglement of three bipartite reduced density matrices from a tripartite pure state has been studied in Hayashi and Chen [2011 Phys. Rev. A 84 012325]. We extend this result to the tripartite mixed state of rank at most three. In particular we show that if the state has two bipartite reduced density operators with rank two, then the third bipartite reduced density operator additionally having non positive partial transpose (non-PPT) is distillable. In contrast, we show that the tripartite PPT state with two reduced density operators of rank two is a three-qubit fully separable state. We obtain these facts by proving a conjectured matrix inequality for the bipartite matrix M with Schmidt rank at most three. This is one of the main results of this paper. We also prove it for some M with arbitrary Schmidt rank.

DOI
10.1088/1751-8121/ab985b

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Abstract The relation between the distillability of entanglement of three bipartite reduced density matrices from a tripartite pure state has been studied in Hayashi and Chen [2011 Phys. Rev. A 84 012325]. We extend this result to the tripartite mixed state of rank at most three. In particular we show that if the state has two bipartite reduced density operators with rank two, then the third bipartite reduced density operator additionally having non positive partial transpose (non-PPT) is distillable. In contrast, we show that the tripartite PPT state with two reduced density operators of rank two is a three-qubit fully separable state. We obtain these facts by proving a conjectured matrix inequality for the bipartite matrix M with Schmidt rank at most three. This is one of the main results of this paper. We also prove it for some M with arbitrary Schmidt rank.
Entanglement distillation is a basic task in quantum information, and the distillable entanglement of three bipartite reduced density matrices from a tripartite pure state has been studied in [Phys. Rev. A 84, 012325 (2011)]. We extend this result to tripartite mixed states by studying a conjectured matrix inequality, namely rank(∑iRi⊗Si)≤Krank(∑iRiT⊗Si)\mathop{\rm rank}(\sum_i R_i \otimes S_i)\leq K \mathop{\rm rank}(\sum_i R_i^T \otimes S_i)rank(∑i​Ri​⊗Si​)≤Krank(∑i​RiT​⊗Si​) holds for any bipartite matrix M=∑iRi⊗SiM=\sum_i R_i \otimes S_iM=∑i​Ri​⊗Si​ and Schmidt rank KKK. We prove that the conjecture holds for MMM with K=3K=3K=3 and some special MMM with arbitrary KKK.
The bipartite quantum states ρ, with rank strictly smaller than the maximum of the ranks of the reduced states ρ A and ρ B , are distillable by local operations and classical communication (Horodecki P, Smolin J A, Terhal B M and Thapliyal A V 2003 Theor. Comput. Sci. 292 589–96; 1999 arXiv:quant-ph/9910122). Our first main result is that this is also true for NPT states with rank equal to this maximum. (A state is PPT if the partial transpose of its density matrix is positive semidefinite, and otherwise it is NPT.) This was conjectured first in 1999 in the special case when the ranks of ρ A and ρ B are equal (see (Horodecki P, Smolin J A, Terhal B M and Thapliyal A V 2003 Theor. Comput. Sci. 292 589–96; 1999 arXiv:quant-ph/9910122). Our second main result provides a complete solution of the separability problem for bipartite states of rank 4. Namely, we show that such a state is separable if and only if it is PPT and its range contains at least one product state. We also prove that the so-called checkerboard states are distillable if and only if they are NPT.
Two important subsets of tripartite pure states, namely {\\em triseparable} states (i.e. states such that the bipartite density matrices obtained by tracing out any party's subsystem are separable) and {\\em triorthogonal} states (i.e. states with a three-party Schmidt-like decomposition) are introduced. It is proved that any triseparable state is triorthogonal and vice-versa. The relevance of this result to quantifying tripartite pure-state entanglement is discussed. It is also proved that any purification of a bipartite bound entangled state with positive partial transpose is {\\em tri-inseparable}. This is a new necessary condition for such bound entanglement.
Assume that Alice, Bob, and Charlie share a tripartite pure state$ \vert \psi _{ABC}\rangle .WeprovethatifAlicecannotdistillentanglementwitheitherBoborCharlieusing. We prove that if Alice cannot distill entanglement with either Bob or Charlie using.WeprovethatifAlicecannotdistillentanglementwitheitherBoborCharlieusing \vert \psi _{ABC}\rangle andlocaloperationswithanyoneofthefollowingconfigurationsforclassicalcommunication:and local operations with any one of the following configurations for classical communication:andlocaloperationswithanyoneofthefollowingconfigurationsforclassicalcommunication:(A\to B, A\leftrightarrow C), (A\leftrightarrow B, A\to C),and, and,and(A\leftrightarrow B, A\leftrightarrow C),thenthesameisalsotruefortheothertwoconfigurations.Moreover,thishappenspreciselywhenthestateissuchthatbothitsreductionsonsystems, then the same is also true for the other two configurations. Moreover, this happens precisely when the state is such that both its reductions on systems,thenthesameisalsotruefortheothertwoconfigurations.Moreover,thishappenspreciselywhenthestateissuchthatbothitsreductionsonsystemsABandandandAC$are separable, which is further equivalent to the reductions being PPT. This, in particular, implies that any NPT bipartite state is such that either the state itself or its complement is 2-way distillable. In proving these results, we first obtain an explicit lower bound on the 2-way distillable entanglement of low rank bipartite states. Furthermore, we show that even though not all low rank states are 1-way distillable, a randomly sampled low rank state will almost surely be 1-way distillable.
Characterizing the relations among the three bipartite reduced density operators$ \rho _{AB},,, \rho _{AC}andandand \rho _{BC}ofatripartitemixedstateof a tripartite mixed stateofatripartitemixedstate \rho _{ABC}hasbeenanopenprobleminquantuminformation.Oneofsuchrelationshasbeenreducedby[Cadneyetal,LAA.452,153,2014]toaconjecturedinequalityintermsofmatrixrank,namelyhas been an open problem in quantum information. One of such relations has been reduced by [Cadney et al, LAA. 452, 153, 2014] to a conjectured inequality in terms of matrix rank, namelyhasbeenanopenprobleminquantuminformation.Oneofsuchrelationshasbeenreducedby[Cadneyetal,LAA.452,153,2014]toaconjecturedinequalityintermsofmatrixrank,namelyr(\rho _{AB}) \cdot r( \rho _{AC})\ge r( \rho _{BC})foranyfor anyforany \rho _{ABC}$. It is denoted as open problem 41 in the website “Open quantum problems-IQOQI Vienna”. We prove the inequality, and thus establish a complete picture of the four-party linear inequalities in terms of the 0-entropy. Our proof is based on the construction of a novel canonical form of bipartite matrices under local equivalence. We extend our result to inequalities in multipartite systems, as well as the condition when the inequality is saturated.
The operator Schmidt rank is the minimum number of terms required to express a state as a sum of elementary tensor factors. Here we provide a new proof of the fact that any bipartite mixed state with operator Schmidt rank two is separable, and can be written as a sum of two positive semidefinite matrices per site. Our proof uses results from the theory of free spectrahedra and operator systems, and illustrates the use of a connection between decompositions of quantum states and decompositions of nonnegative matrices. In the multipartite case, we prove that any Hermitian Matrix Product Density Operator (MPDO) of bond dimension two is separable, and can be written as a sum of at most four positive semidefinite matrices per site. This implies that these states can only contain classical correlations, and very few of them, as measured by the entanglement of purification. In contrast, MPDOs of bond dimension three can contain an unbounded amount of classical correlations.