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Time reversed optical waves by arbitrary vector spatiotemporal field generation
Lossless linear wave propagation is symmetric in time, a principle which can be used to create time reversed waves. Such waves are special “pre-scattered” spatiotemporal fields, which propagate through a complex medium as if observing a scattering process in reverse, entering the medium as a complic...
Autores principales: | , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group UK
2020
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7669854/ https://www.ncbi.nlm.nih.gov/pubmed/33199708 http://dx.doi.org/10.1038/s41467-020-19601-3 |
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author | Mounaix, Mickael Fontaine, Nicolas K. Neilson, David T. Ryf, Roland Chen, Haoshuo Alvarado-Zacarias, Juan Carlos Carpenter, Joel |
author_facet | Mounaix, Mickael Fontaine, Nicolas K. Neilson, David T. Ryf, Roland Chen, Haoshuo Alvarado-Zacarias, Juan Carlos Carpenter, Joel |
author_sort | Mounaix, Mickael |
collection | PubMed |
description | Lossless linear wave propagation is symmetric in time, a principle which can be used to create time reversed waves. Such waves are special “pre-scattered” spatiotemporal fields, which propagate through a complex medium as if observing a scattering process in reverse, entering the medium as a complicated spatiotemporal field and arriving after propagation as a desired target field, such as a spatiotemporal focus. Time reversed waves have previously been demonstrated for relatively low frequency phenomena such as acoustics, water waves and microwaves. Many attempts have been made to extend these techniques into optics. However, the much higher frequencies of optics make for very different requirements. A fully time reversed wave is a volumetric field with arbitrary amplitude, phase and polarisation at every point in space and time. The creation of such fields has not previously been possible in optics. We demonstrate time reversed optical waves with a device capable of independently controlling all of light’s classical degrees of freedom simultaneously. Such a class of ultrafast wavefront shaper is capable of generating a sequence of arbitrary 2D spatial/polarisation wavefronts at a bandwidth limited rate of 4.4 THz. This ability to manipulate the full field of an optical beam could be used to control both linear and nonlinear optical phenomena. |
format | Online Article Text |
id | pubmed-7669854 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2020 |
publisher | Nature Publishing Group UK |
record_format | MEDLINE/PubMed |
spelling | pubmed-76698542020-11-24 Time reversed optical waves by arbitrary vector spatiotemporal field generation Mounaix, Mickael Fontaine, Nicolas K. Neilson, David T. Ryf, Roland Chen, Haoshuo Alvarado-Zacarias, Juan Carlos Carpenter, Joel Nat Commun Article Lossless linear wave propagation is symmetric in time, a principle which can be used to create time reversed waves. Such waves are special “pre-scattered” spatiotemporal fields, which propagate through a complex medium as if observing a scattering process in reverse, entering the medium as a complicated spatiotemporal field and arriving after propagation as a desired target field, such as a spatiotemporal focus. Time reversed waves have previously been demonstrated for relatively low frequency phenomena such as acoustics, water waves and microwaves. Many attempts have been made to extend these techniques into optics. However, the much higher frequencies of optics make for very different requirements. A fully time reversed wave is a volumetric field with arbitrary amplitude, phase and polarisation at every point in space and time. The creation of such fields has not previously been possible in optics. We demonstrate time reversed optical waves with a device capable of independently controlling all of light’s classical degrees of freedom simultaneously. Such a class of ultrafast wavefront shaper is capable of generating a sequence of arbitrary 2D spatial/polarisation wavefronts at a bandwidth limited rate of 4.4 THz. This ability to manipulate the full field of an optical beam could be used to control both linear and nonlinear optical phenomena. Nature Publishing Group UK 2020-11-16 /pmc/articles/PMC7669854/ /pubmed/33199708 http://dx.doi.org/10.1038/s41467-020-19601-3 Text en © The Author(s) 2020 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/. |
spellingShingle | Article Mounaix, Mickael Fontaine, Nicolas K. Neilson, David T. Ryf, Roland Chen, Haoshuo Alvarado-Zacarias, Juan Carlos Carpenter, Joel Time reversed optical waves by arbitrary vector spatiotemporal field generation |
title | Time reversed optical waves by arbitrary vector spatiotemporal field generation |
title_full | Time reversed optical waves by arbitrary vector spatiotemporal field generation |
title_fullStr | Time reversed optical waves by arbitrary vector spatiotemporal field generation |
title_full_unstemmed | Time reversed optical waves by arbitrary vector spatiotemporal field generation |
title_short | Time reversed optical waves by arbitrary vector spatiotemporal field generation |
title_sort | time reversed optical waves by arbitrary vector spatiotemporal field generation |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7669854/ https://www.ncbi.nlm.nih.gov/pubmed/33199708 http://dx.doi.org/10.1038/s41467-020-19601-3 |
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