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Localizable Entanglement
Quantum Physics · Submitted 17 Nov 2004
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We have numerical evidence that the ground state of the antiferromagnetic spin-1 Heisenberg chain can serve as a perfect quantum channel.
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The abstract, sentence by sentence
We consider systems of interacting spins and study the entanglement that can be localized, on average, between two separated spins by performing local measurements on the remaining spins. This concept of Localizable Entanglement (LE) leads naturally to notions like entanglement length and entanglement fluctuations. For both spin-1/2 and spin-1 systems we prove that the LE of a pure quantum state can be lower bounded by connected correlation functions. We further propose a scheme, based on matrix-product states and the Monte Carlo method, to efficiently calculate the LE for quantum states of a large number of spins. The virtues of LE are illustrated for various spin models. In particular, characteristic features of a quantum phase transition such as a diverging entanglement length can be observed. We also give examples for pure quantum states exhibiting a diverging entanglement length but finite correlation length. We have numerical evidence that the ground state of the antiferromagnetic spin-1 Heisenberg chain can serve as a perfect quantum channel. Furthermore, we apply the numerical method to mixed states and study the entanglement as a function of temperature.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We consider systems of interacting spins and study the entanglement that can be localized, on average, between two separated spins by performing local measurements on the remaining spins. | contribution 0.95 | 0.85 | 0.11 | asserted 0.68 |
| s1 | This concept of Localizable Entanglement (LE) leads naturally to notions like entanglement length and entanglement fluctuations. | interpretation 0.56 | 0.53 | 0.10 | asserted 0.96 |
| s2 | For both spin-1/2 and spin-1 systems we prove that the LE of a pure quantum state can be lower bounded by connected correlation functions. | result 0.79 | 0.95 | 0.20 | asserted 1.00 |
| s3 | We further propose a scheme, based on matrix-product states and the Monte Carlo method, to efficiently calculate the LE for quantum states of a large number of spins. | method 0.89 | 0.93 | 0.08 | asserted 0.74 |
| s4 | The virtues of LE are illustrated for various spin models. | contribution 0.65 | 0.80 | 0.06 | asserted 0.99 |
| s5 | In particular, characteristic features of a quantum phase transition such as a diverging entanglement length can be observed. | result 0.76 | 0.78 | 0.13 | asserted 0.79 |
| s6 | We also give examples for pure quantum states exhibiting a diverging entanglement length but finite correlation length. | result 0.97 | 0.89 | 0.08 | asserted 0.99 |
| s7 | We have numerical evidence that the ground state of the antiferromagnetic spin-1 Heisenberg chain can serve as a perfect quantum channel. | result 0.96 | 0.94 | 0.15 | hedged possibility 0.67 |
| s8 | Furthermore, we apply the numerical method to mixed states and study the entanglement as a function of temperature. | contribution 0.91 | 0.95 | 0.06 | asserted 0.97 |
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The paper
Original abstract
We consider systems of interacting spins and study the entanglement that can be localized, on average, between two separated spins by performing local measurements on the remaining spins. This concept of Localizable Entanglement (LE) leads naturally to notions like entanglement length and entanglement fluctuations. For both spin-1/2 and spin-1 systems we prove that the LE of a pure quantum state can be lower bounded by connected correlation functions. We further propose a scheme, based on matrix-product states and the Monte Carlo method, to efficiently calculate the LE for quantum states of a large number of spins. The virtues of LE are illustrated for various spin models. In particular, characteristic features of a quantum phase transition such as a diverging entanglement length can be observed. We also give examples for pure quantum states exhibiting a diverging entanglement length but finite correlation length. We have numerical evidence that the ground state of the antiferromagnetic spin-1 Heisenberg chain can serve as a perfect quantum channel. Furthermore, we apply the numerical method to mixed states and study the entanglement as a function of temperature.
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References
How the literature uses it
8 arXiv papers cite this in 9 sentences
Papers citing it · 6 sentences without a confident label
Cites it as background 3 papers
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Studies of localizable entanglement [ref] and single-round measurements [ref] have shown how local measurements can concentrate correlations or prepare nontrivial many-body states [ref] .
Exact Entanglement Swapping through Single-Occupancy Measurements in Gaussian Fermion States · Introduction · 0.82
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Finally, we note there exists a notion of localizable entanglement and associated entanglement length, [ref] whose divergence is connected to a string order parameter.
Spurious Long-range Entanglement and Replica Correlation Length · Discussion · 0.98
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Teleportation in many-body states is often quantified by the concept of measurement-induced entanglement (MIE) [ref] and localizable entanglement [ref] .
Nonlocal growth of quantum conditional mutual information under decoherence · Comparing Different Teleportation Metrics · 0.87
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