Theoretical description and experimental simulation of quantum entanglement near open time-like curves via pseudo-density operators
Chiara Marletto (),
Vlatko Vedral,
Salvatore Virzì,
Enrico Rebufello,
Alessio Avella,
Fabrizio Piacentini,
Marco Gramegna,
Ivo Pietro Degiovanni and
Marco Genovese
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Chiara Marletto: University of Oxford
Vlatko Vedral: University of Oxford
Salvatore Virzì: Università di Torino
Enrico Rebufello: Istituto Nazionale di Ricerca Metrologica
Alessio Avella: Istituto Nazionale di Ricerca Metrologica
Fabrizio Piacentini: Istituto Nazionale di Ricerca Metrologica
Marco Gramegna: Istituto Nazionale di Ricerca Metrologica
Ivo Pietro Degiovanni: Istituto Nazionale di Ricerca Metrologica
Marco Genovese: INFN – sezione di Torino
Nature Communications, 2019, vol. 10, issue 1, 1-7
Abstract:
Abstract Closed timelike curves are striking predictions of general relativity allowing for time-travel. They are afflicted by notorious causality issues (e.g. grandfather’s paradox). Quantum models where a qubit travels back in time solve these problems, at the cost of violating quantum theory’s linearity—leading e.g. to universal quantum cloning. Interestingly, linearity is violated even by open timelike curves (OTCs), where the qubit does not interact with its past copy, but is initially entangled with another qubit. Non-linear dynamics is needed to avoid violating entanglement monogamy. Here we propose an alternative approach to OTCs, allowing for monogamy violations. Specifically, we describe the qubit in the OTC via a pseudo-density operator—a unified descriptor of both temporal and spatial correlations. We also simulate the monogamy violation with polarization-entangled photons, providing a pseudo-density operator quantum tomography. Remarkably, our proposal applies to any space-time correlations violating entanglement monogamy, such as those arising in black holes.
Date: 2019
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Persistent link: https://EconPapers.repec.org/RePEc:nat:natcom:v:10:y:2019:i:1:d:10.1038_s41467-018-08100-1
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DOI: 10.1038/s41467-018-08100-1
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