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arXiv:quant-ph/0510017 · Physical Review A

Entanglement-induced state ordering under local operations

Mário Ziman, Vladimír Bužek

Published Jan 1, 2006• 24 citations
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Abstract

We analyze how entanglement between two components of a bipartite system behaves under the action of local channels of the form $\mathcal{E}\ensuremath{\bigotimes}\mathcal{I}$. We show that a set of maximally entangled states is by the action of $\mathcal{E}\ensuremath{\bigotimes}\mathcal{I}$ transformed into the set of states that exhibit the same degree of entanglement. Moreover, this degree represents an upper bound on entanglement that is available at the output of the channel irrespective of what the input state of the composite system is. We show that within this bound the entanglement-induced state ordering is ``relative'' and can be changed by the action of local channels. That is, two states ${\ensuremath{\varrho}}_{1}^{(\mathrm{in})}$ and ${\ensuremath{\varrho}}_{2}^{(\mathrm{in})}$ such that the entanglement $E[{\ensuremath{\varrho}}_{1}^{(\mathrm{in})}]$ of the first state is larger than the entanglement $E[{\ensuremath{\varrho}}_{2}^{(\mathrm{in})}]$ of the second state are transformed into states ${\ensuremath{\varrho}}_{1}^{(\mathrm{out})}$ and ${\ensuremath{\varrho}}_{2}^{(\mathrm{out})}$ such that $E[{\ensuremath{\varrho}}_{2}^{(\mathrm{out})}]>E[{\ensuremath{\varrho}}_{1}^{(\mathrm{out})}]$.

DOI
10.1103/physreva.73.012312

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We analyze how entanglement between two components of a bipartite system behaves under the action of local channels of the form E\ensuremath⨂I\mathcal{E}\ensuremath{\bigotimes}\mathcal{I}E\ensuremath⨂I. We show that a set of maximally entangled states is by the action of E\ensuremath⨂I\mathcal{E}\ensuremath{\bigotimes}\mathcal{I}E\ensuremath⨂I transformed into the set of states that exhibit the same degree of entanglement. Moreover, this degree represents an upper bound on entanglement that is available at the output of the channel irrespective of what the input state of the composite system is. We show that within this bound the entanglement-induced state ordering is ``relative'' and can be changed by the action of local channels. That is, two states \ensuremathϱ1(in){\ensuremath{\varrho}}_{1}^{(\mathrm{in})}\ensuremathϱ1(in)​ and \ensuremathϱ2(in){\ensuremath{\varrho}}_{2}^{(\mathrm{in})}\ensuremathϱ2(in)​ such that the entanglement E[\ensuremathϱ1(in)]E[{\ensuremath{\varrho}}_{1}^{(\mathrm{in})}]E[\ensuremathϱ1(in)​] of the first state is larger than the entanglement E[\ensuremathϱ2(in)]E[{\ensuremath{\varrho}}_{2}^{(\mathrm{in})}]E[\ensuremathϱ2(in)​] of the second state are transformed into states \ensuremathϱ1(out){\ensuremath{\varrho}}_{1}^{(\mathrm{out})}\ensuremathϱ1(out)​ and \ensuremathϱ2(out){\ensuremath{\varrho}}_{2}^{(\mathrm{out})}\ensuremathϱ2(out)​ such that E[\ensuremathϱ2(out)]>E[\ensuremathϱ1(out)]E[{\ensuremath{\varrho}}_{2}^{(\mathrm{out})}]>E[{\ensuremath{\varrho}}_{1}^{(\mathrm{out})}]E[\ensuremathϱ2(out)​]>E[\ensuremathϱ1(out)​].
We analyze how entanglement between two components of a bipartite system behaves under the action of local channels of the form ExI. We show that a set of maximally entangled states is by the action of ExI transformed into the set of states that exhibit the same degree of entanglement. Moreover, this degree represents an upper bound on entanglement that is available at the output of the channel irrespective of what the input state of the composite system is. We show that within this bound the entanglement-induced state ordering is ''relative'' and can be changed by the action of local channels. That is, two states {rho}{sub 1}{sup (in)} and {rho}{sub 2}{sup (in)} such that the entanglement E[{rho}{sub 1}{sup (in)}] of the first state is larger than the entanglement E[{rho}{sub 2}{sup (in)}] of the second state are transformed into states {rho}{sub 1}{sup (out)} and {rho}{sub 2}{sup (out)} such that E[{rho}{sub 2}{sup (out)}]>E[{rho}{sub 1}{sup (out)}].
We derive an upper bound on the action of a direct product of two quantum maps (channels) acting on multi-partite quantum states. We assume that the individual channels ΛjΛ_jΛj​ affect single-particle states so, that for an arbitrary input ρjρ_jρj​, the distance Dj(Λj[ρj],ρj)D_j (Λ_j [ ρ_j ], ρ_j)Dj​(Λj​[ρj​],ρj​) between the input ρjρ_jρj​ and the output Λj[ρj]Λ_j [ ρ_j ]Λj​[ρj​] of the channel is less than εεε. Given this assumption we show that for an arbitrary {\em separable} two-partite state ρ12ρ_{12}ρ12​ the distance between the input ρ12ρ_{12}ρ12​ and the output Λ1⊗Λ2[ρ12]Λ_1\otimesΛ_2[ρ_{12} ]Λ1​⊗Λ2​[ρ12​] fulfills the bound D12(Λ1⊗Λ2[ρ12],ρ12)≤2+2(1−1/d1)(1−1/d2)εD_{12} (Λ_1 \otimes Λ_2 [ ρ_{12} ], ρ_{12}) \leq \sqrt{2+ 2 \sqrt{(1-1/d_1)(1-1/d_2)}} εD12​(Λ1​⊗Λ2​[ρ12​],ρ12​)≤2+2(1−1/d1​)(1−1/d2​)​​ε where d1d_1d1​ and d2d_2d2​ are dimensions of first and second quantum system respectively. On the contrary, entangled states are transformed in such a way, that the bound on the action of the local channels is D12(Λ1⊗Λ2[ρ12],ρ12)≤22−1/d εD_{12} (Λ_1 \otimes Λ_2 [ ρ_{12} ], ρ_{12}) \leq 2 \sqrt{2 - 1/d} \: εD12​(Λ1​⊗Λ2​[ρ12​],ρ12​)≤22−1/d​ε, where ddd is the dimension of the smaller of the two quantum systems passing through the channels. Our results show that the fundamental distinction between the set of separable and the set of entangled states results into two different bounds which in turn can be exploited for a discrimination between the two sets of states. We generalize our results to multi-partite channels.
A set of all states of a bi-partite quantum system can be divided into subsets each of which contains states with the same degree of entanglement. In this paper we address a question whether local operations (without classical communication) affect the entanglement-induced state ordering. We show that arbitrary unilocal channel (i.e., a channel that acts on one sub-system of a bi-partite system only) might change the ordering for an arbitrary nontrivial measure of entanglement. A slightly weaker result holds for the maximally entangled states. In particular, the maximally entangled states might not remain the most entangled ones at the output of a unilocal noise channel.
We analyze how a maximally entangled state of two qubits (e.g., the singlet ${\ensuremath{\psi}}_{s}$) is affected by the action of local channels described by completely positive maps E\mathcal{E}E. We analyze the concurrence and the purity of states ${\ensuremath{\varrho}}_{\mathcal{E}}=\mathcal{E}\ensuremath{\bigotimes}\mathcal{I}[{\ensuremath{\psi}}_{s}]$. Using the concurrence-versus-purity phase diagram we characterize local channels E\mathcal{E}E by their action on the singlet state ${\ensuremath{\psi}}_{s}$. We specify a region of the concurrence-versus-purity diagram that is achievable from the singlet state via the action of unital channels. We show that even the most general (including nonunital) local channels acting just on a single qubit of the original singlet state cannot generate the maximally entangled mixed states. We study in detail various time evolutions of the original singlet state induced by local Markovian semigroups. We show that the decoherence process is represented in the concurrence-versus-purity diagram by a line that forms the lower bound of the achievable region for unital maps. On the other hand, the depolarization process is represented by a line that forms the upper bound of the region of maps induced by unital maps.
We analyze how a maximally entangled state of two qubits (e.g., the singlet {psi}{sub s}) is affected by the action of local channels described by completely positive maps E. We analyze the concurrence and the purity of states {rho}{sub E}=ExI[{psi}{sub s}]. Using the concurrence-versus-purity phase diagram we characterize local channels E by their action on the singlet state {psi}{sub s}. We specify a region of the concurrence-versus-purity diagram that is achievable from the singlet state via the action of unital channels. We show that even the most general (including nonunital) local channels acting just on a single qubit of the original singlet state cannot generate the maximally entangled mixed states. We study in detail various time evolutions of the original singlet state induced by local Markovian semigroups. We show that the decoherence process is represented in the concurrence-versus-purity diagram by a line that forms the lower bound of the achievable region for unital maps. On the other hand, the depolarization process is represented by a line that forms the upper bound of the region of maps induced by unital maps.
Entanglement is one of the fundamental features of quantum information science.\nThough bipartite entanglement has been analyzed thoroughly in theory and shown to\nbe an important resource in quantum computation and communication protocols, the\ntheory of entanglement shared between more than two parties, which is called multipartite\nentanglement, is still not complete. Specifically, the classification of multipartite\nentanglement and the transformation property between different multipartite states by\nlocal operators and classical communications (LOCC) are two fundamental questions in\nthe theory of multipartite entanglement.\nIn this thesis, we present results related to the LOCC transformation between multipartite\nentangled states. Firstly, we investigate the bounds on the LOCC transformation\nprobability between multipartite states, especially the GHZ class states. By analyzing\nthe involvement of 3-tangle and other entanglement measures under weak two-outcome\nmeasurement, we derive explicit upper and lower bound on the transformation probability\nbetween GHZ class states. After that, we also analyze the transformation between\nN-party W type states, which is a special class of multipartite entangled states that\nhas an explicit unique expression and a set of analytical entanglement monotones. We\npresent a necessary and sufficient condition for a known upper bound of transformation\nprobability between two N-party W type states to be achieved.\nWe also further investigate a novel entanglement transformation protocol, the random\ndistillation, which transforms multipartite entanglement into bipartite entanglement\nii\nshared by a non-deterministic pair of parties. We find upper bounds for the random distillation\nprotocol for general N-party W type states and find the condition for the upper\nbounds to be achieved. What is surprising is that the upper bounds correspond to entanglement\nmonotones that can be increased by Separable Operators (SEP), which gives\nthe first set of analytical entanglement monotones that can be increased by SEP.\nFinally, we investigate the idea of a new class of multipartite entangled states, the\nAbsolutely Maximal Entangled (AME) states, which is characterized by the fact that\nany bipartition of the states would give a maximal entangled state between the two sets.\nThe relationship between AME states and Quantum secret sharing (QSS) protocols is\nexhibited and the application of AME states in novel quantum communication protocols\nis also explored.