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Nonreciprocal second harmonic generation in a magnetoelectric material
Mirror symmetries are of particular importance because they are connected to fundamental properties and conservation laws. Spatial inversion and time reversal are typically associated to charge and spin phenomena, respectively. When both are broken, magnetoelectric cross-coupling can arise. In the o...
Autores principales: | , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Association for the Advancement of Science
2021
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8051877/ https://www.ncbi.nlm.nih.gov/pubmed/33863720 http://dx.doi.org/10.1126/sciadv.abe2793 |
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author | Toyoda, Shingo Fiebig, Manfred Arima, Taka-hisa Tokura, Yoshinori Ogawa, Naoki |
author_facet | Toyoda, Shingo Fiebig, Manfred Arima, Taka-hisa Tokura, Yoshinori Ogawa, Naoki |
author_sort | Toyoda, Shingo |
collection | PubMed |
description | Mirror symmetries are of particular importance because they are connected to fundamental properties and conservation laws. Spatial inversion and time reversal are typically associated to charge and spin phenomena, respectively. When both are broken, magnetoelectric cross-coupling can arise. In the optical regime, a difference between forward and backward propagation of light may result. Usually, this nonreciprocal response is small. We show that a giant nonreciprocal optical response can occur when transferring from linear to nonlinear optics, specifically second harmonic generation (SHG). CuB(2)O(4) exhibits SHG transmission changes by almost 100% upon reversal of a magnetic field of just ±10 mT. The observed nonreciprocity results from an interference between magnetic-dipole and electric-dipole SHG. Although the former is inherently weaker than the latter, a resonantly enhanced magnetic-dipole transition has a comparable amplitude as a nonresonant electric-dipole transition, thus maximizing the nonreciprocity. Multiferroics and magnetoelectrics are an obvious materials platform to exhibit nonreciprocal nonlinear optical functionalities. |
format | Online Article Text |
id | pubmed-8051877 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2021 |
publisher | American Association for the Advancement of Science |
record_format | MEDLINE/PubMed |
spelling | pubmed-80518772021-04-26 Nonreciprocal second harmonic generation in a magnetoelectric material Toyoda, Shingo Fiebig, Manfred Arima, Taka-hisa Tokura, Yoshinori Ogawa, Naoki Sci Adv Research Articles Mirror symmetries are of particular importance because they are connected to fundamental properties and conservation laws. Spatial inversion and time reversal are typically associated to charge and spin phenomena, respectively. When both are broken, magnetoelectric cross-coupling can arise. In the optical regime, a difference between forward and backward propagation of light may result. Usually, this nonreciprocal response is small. We show that a giant nonreciprocal optical response can occur when transferring from linear to nonlinear optics, specifically second harmonic generation (SHG). CuB(2)O(4) exhibits SHG transmission changes by almost 100% upon reversal of a magnetic field of just ±10 mT. The observed nonreciprocity results from an interference between magnetic-dipole and electric-dipole SHG. Although the former is inherently weaker than the latter, a resonantly enhanced magnetic-dipole transition has a comparable amplitude as a nonresonant electric-dipole transition, thus maximizing the nonreciprocity. Multiferroics and magnetoelectrics are an obvious materials platform to exhibit nonreciprocal nonlinear optical functionalities. American Association for the Advancement of Science 2021-04-16 /pmc/articles/PMC8051877/ /pubmed/33863720 http://dx.doi.org/10.1126/sciadv.abe2793 Text en Copyright © 2021 The Authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original U.S. Government Works. Distributed under a Creative Commons Attribution License 4.0 (CC BY). https://creativecommons.org/licenses/by/4.0/This is an open-access article distributed under the terms of the Creative Commons Attribution license (https://creativecommons.org/licenses/by/4.0/) , which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. |
spellingShingle | Research Articles Toyoda, Shingo Fiebig, Manfred Arima, Taka-hisa Tokura, Yoshinori Ogawa, Naoki Nonreciprocal second harmonic generation in a magnetoelectric material |
title | Nonreciprocal second harmonic generation in a magnetoelectric material |
title_full | Nonreciprocal second harmonic generation in a magnetoelectric material |
title_fullStr | Nonreciprocal second harmonic generation in a magnetoelectric material |
title_full_unstemmed | Nonreciprocal second harmonic generation in a magnetoelectric material |
title_short | Nonreciprocal second harmonic generation in a magnetoelectric material |
title_sort | nonreciprocal second harmonic generation in a magnetoelectric material |
topic | Research Articles |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8051877/ https://www.ncbi.nlm.nih.gov/pubmed/33863720 http://dx.doi.org/10.1126/sciadv.abe2793 |
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