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      A dynamical quantum Cheshire Cat effect and implications for counterfactual communication

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          Abstract

          Here we report a type of dynamic effect that is at the core of the so called “counterfactual computation” and especially “counterfactual communication” quantum effects that have generated a lot of interest recently. The basic feature of these counterfactual setups is the fact that particles seem to be affected by actions that take place in locations where they never (more precisely, only with infinitesimally small probability) enter. Specifically, the communication/computation takes place without the quantum particles that are supposed to be the information carriers travelling through the communication channel or entering the logic gates of the computer. Here we show that something far more subtle is taking place: It is not necessary for the particle to enter the region where the controlling action takes place; it is enough for the controlled property of the particle, (i.e., the property that is being controlled by actions in the control region), to enter that region. The presence of the controlled property, without the particle itself, is possible via a quantum Cheshire Cat type effect in which a property can be disembodied from the particle that possesses it. At the same time, we generalize the quantum Cheshire Cat effect to dynamical settings, in which the property that is “disembodied” from the particle possessing it propagates in space, and leads to a flux of “disembodied” conserved quantities.

          Abstract

          In quantum mechanics, counterfactual behaviours are generally associated with particles being affected by events taking place where they can’t be found. Here, the authors consider extended quantum Cheshire cat scenarios where a particle can be influenced in regions where only its disembodied property has entered.

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          Quantum mechanical interaction-free measurements

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            Counterfactual quantum computation through quantum interrogation.

            The logic underlying the coherent nature of quantum information processing often deviates from intuitive reasoning, leading to surprising effects. Counterfactual computation constitutes a striking example: the potential outcome of a quantum computation can be inferred, even if the computer is not run. Relying on similar arguments to interaction-free measurements (or quantum interrogation), counterfactual computation is accomplished by putting the computer in a superposition of 'running' and 'not running' states, and then interfering the two histories. Conditional on the as-yet-unknown outcome of the computation, it is sometimes possible to counterfactually infer information about the solution. Here we demonstrate counterfactual computation, implementing Grover's search algorithm with an all-optical approach. It was believed that the overall probability of such counterfactual inference is intrinsically limited, so that it could not perform better on average than random guesses. However, using a novel 'chained' version of the quantum Zeno effect, we show how to boost the counterfactual inference probability to unity, thereby beating the random guessing limit. Our methods are general and apply to any physical system, as illustrated by a discussion of trapped-ion systems. Finally, we briefly show that, in certain circumstances, counterfactual computation can eliminate errors induced by decoherence.
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              Violation of Heisenberg’s Measurement-Disturbance Relationship by Weak Measurements

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                Author and article information

                Contributors
                s.popescu@bristol.ac.uk
                Journal
                Nat Commun
                Nat Commun
                Nature Communications
                Nature Publishing Group UK (London )
                2041-1723
                6 August 2021
                6 August 2021
                2021
                : 12
                : 4770
                Affiliations
                [1 ]GRID grid.12136.37, ISNI 0000 0004 1937 0546, School of Physics and Astronomy, , Tel Aviv University, ; Tel Aviv, Israel
                [2 ]GRID grid.254024.5, ISNI 0000 0000 9006 1798, Schmid College of Science and Technology and Institute for Quantum Studies, , Chapman University, ; Orange, CA USA
                [3 ]GRID grid.22098.31, ISNI 0000 0004 1937 0503, Faculty of Engineering and the Institute of Nanotechnology and Advanced Materials, , Bar Ilan University, ; Ramat Gan, Israel
                [4 ]GRID grid.5337.2, ISNI 0000 0004 1936 7603, H. H. Wills Physics Laboratory, , University of Bristol, ; Bristol, UK
                Article
                24933
                10.1038/s41467-021-24933-9
                8346505
                34362884
                5ed2c394-b6ef-45bc-b995-bafa6d13f0ab
                © The Author(s) 2021

                Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/.

                History
                : 6 July 2020
                : 9 July 2021
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                © The Author(s) 2021

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                quantum information,quantum mechanics
                Uncategorized
                quantum information, quantum mechanics

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