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How to build a device that cannot be built
In this paper, we show how the GHZ paradox can be used to design a computing device that cannot be physically implemented within the context of classical physics, but nonetheless can be within quantum physics, i.e., in a quantum physics laboratory. This example gives an illustration of the many subt...
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Formato: | Online Artículo Texto |
Lenguaje: | English |
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Springer US
2015
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5591609/ https://www.ncbi.nlm.nih.gov/pubmed/28955190 http://dx.doi.org/10.1007/s11128-015-1206-7 |
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author | Lomonaco, Samuel J. |
author_facet | Lomonaco, Samuel J. |
author_sort | Lomonaco, Samuel J. |
collection | PubMed |
description | In this paper, we show how the GHZ paradox can be used to design a computing device that cannot be physically implemented within the context of classical physics, but nonetheless can be within quantum physics, i.e., in a quantum physics laboratory. This example gives an illustration of the many subtleties involved in the quantum control of distributed quantum systems. We also show how the second elementary symmetric Boolean function can be interpreted as a quantification of the nonlocality and indeterminism involved in the GHZ paradox. |
format | Online Article Text |
id | pubmed-5591609 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2015 |
publisher | Springer US |
record_format | MEDLINE/PubMed |
spelling | pubmed-55916092017-09-25 How to build a device that cannot be built Lomonaco, Samuel J. Quantum Inf Process Article In this paper, we show how the GHZ paradox can be used to design a computing device that cannot be physically implemented within the context of classical physics, but nonetheless can be within quantum physics, i.e., in a quantum physics laboratory. This example gives an illustration of the many subtleties involved in the quantum control of distributed quantum systems. We also show how the second elementary symmetric Boolean function can be interpreted as a quantification of the nonlocality and indeterminism involved in the GHZ paradox. Springer US 2015-12-28 2016 /pmc/articles/PMC5591609/ /pubmed/28955190 http://dx.doi.org/10.1007/s11128-015-1206-7 Text en © The Author(s) 2015 Open AccessThis article is distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium, provided 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. |
spellingShingle | Article Lomonaco, Samuel J. How to build a device that cannot be built |
title | How to build a device that cannot be built |
title_full | How to build a device that cannot be built |
title_fullStr | How to build a device that cannot be built |
title_full_unstemmed | How to build a device that cannot be built |
title_short | How to build a device that cannot be built |
title_sort | how to build a device that cannot be built |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5591609/ https://www.ncbi.nlm.nih.gov/pubmed/28955190 http://dx.doi.org/10.1007/s11128-015-1206-7 |
work_keys_str_mv | AT lomonacosamuelj howtobuildadevicethatcannotbebuilt |