2006
DOI: 10.1103/physreva.73.012312
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Entanglement-induced state ordering under local operations

Abstract: We analyze how entanglement between two components of a bipartite system behaves under the action of local channels of the form E ⊗ I. We show that a set of maximally entangled states is by the action of E ⊗ 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 what is the input state of the composite system. We show that within this bound the the entanglement… Show more

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Cited by 22 publications
(14 citation statements)
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“…In this paper, we extend these results to the case of general local unital channels Υ A 1 (t) ⊗ Υ B 2 (t) and prove that the maximally entangled state + is optimal for the transmission of entanglement through such channels. It is tempting to conclude that the maximally entangled state + exhibits ultimate robustness to general local two-qubit noises Φ A 1 (t) ⊗ Φ B 2 (t); however, this is not true [38][39][40] and we show that explic- arXiv:1708.08208v2 [quant-ph] 21 Jan 2018 itly in this paper. Moreover, we analytically find the initial two-qubit state , which is the most robust to a given nonunital local two-qubit dynamical map Φ 1 (t) ⊗ Φ 2 (t).…”
Section: Introductionmentioning
confidence: 63%
“…In this paper, we extend these results to the case of general local unital channels Υ A 1 (t) ⊗ Υ B 2 (t) and prove that the maximally entangled state + is optimal for the transmission of entanglement through such channels. It is tempting to conclude that the maximally entangled state + exhibits ultimate robustness to general local two-qubit noises Φ A 1 (t) ⊗ Φ B 2 (t); however, this is not true [38][39][40] and we show that explic- arXiv:1708.08208v2 [quant-ph] 21 Jan 2018 itly in this paper. Moreover, we analytically find the initial two-qubit state , which is the most robust to a given nonunital local two-qubit dynamical map Φ 1 (t) ⊗ Φ 2 (t).…”
Section: Introductionmentioning
confidence: 63%
“…We now give two useful lemmas which are applicable to any quantum channel Λ. The first lemma was proved in [14].…”
Section: Resultsmentioning
confidence: 99%
“…. In [14,15], specific examples were given which showed that the ordering of entangled states may change under one-sided local action of a qubit channel and the maximum output entanglement may not be achieved for an input maximally entangled state [shown for a system of four qubits having configuration C 2 ⊗ C 2 ⊗ C 2 ⊗ C 2 ]. A more systematic way supporting these observations can be found in [12,13,19].…”
Section: Introductionmentioning
confidence: 99%
“…(5) is that the entanglement of any initial maximally entangled state vanishes when | R 1 | + | R 2 | + | R 3 | ≤ 1. Based on the presented calculation, we can not conclude that when | R 1 | + | R 2 | + | R 3 | ≤ 1, the channel is an entanglement breaking channel (i.e., the systems become separable for any initial state) 18 . Nevertheless, this condition coincides with the entanglement breaking condition for the general unilocal case 12 .…”
Section: Theoretical Modelmentioning
confidence: 79%