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Giant electron–phonon coupling of the breathing plane oxygen phonons in the dynamic stripe phase of [Formula: see text]

Doped antiferromagnets host a vast array of physical properties and learning how to control them is one of the biggest challenges of condensed matter physics. [Formula: see text] (LSNO) is a classic example of such a material. At low temperatures holes introduced via substitution of La by Sr segrega...

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Autores principales: Merritt, A. M., Christianson, A. D., Banerjee, A., Gu, G. D., Mishchenko, A. S., Reznik, D.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2020
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7351770/
https://www.ncbi.nlm.nih.gov/pubmed/32651413
http://dx.doi.org/10.1038/s41598-020-67963-x
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author Merritt, A. M.
Christianson, A. D.
Banerjee, A.
Gu, G. D.
Mishchenko, A. S.
Reznik, D.
author_facet Merritt, A. M.
Christianson, A. D.
Banerjee, A.
Gu, G. D.
Mishchenko, A. S.
Reznik, D.
author_sort Merritt, A. M.
collection PubMed
description Doped antiferromagnets host a vast array of physical properties and learning how to control them is one of the biggest challenges of condensed matter physics. [Formula: see text] (LSNO) is a classic example of such a material. At low temperatures holes introduced via substitution of La by Sr segregate into lines to form boundaries between magnetically ordered domains in the form of stripes. The stripes become dynamic at high temperatures, but LSNO remains insulating presumably because an interplay between magnetic correlations and electron–phonon coupling localizes charge carriers. Magnetic degrees of freedom have been extensively investigated in this system, but phonons are almost completely unexplored. We searched for electron–phonon anomalies in LSNO by inelastic neutron scattering. Giant renormalization of plane Ni–O bond-stretching modes that modulate the volume around Ni appears on entering the dynamic charge stripe phase. Other phonons are a lot less sensitive to stripe melting. Dramatic overdamping of the breathing modes indicates that dynamic stripe phase may host small polarons. We argue that this feature sets electron–phonon coupling in nickelates apart from that in cuprates where breathing phonons are not overdamped and point out remarkable similarities with the colossal magnetoresistance manganites.
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spelling pubmed-73517702020-07-14 Giant electron–phonon coupling of the breathing plane oxygen phonons in the dynamic stripe phase of [Formula: see text] Merritt, A. M. Christianson, A. D. Banerjee, A. Gu, G. D. Mishchenko, A. S. Reznik, D. Sci Rep Article Doped antiferromagnets host a vast array of physical properties and learning how to control them is one of the biggest challenges of condensed matter physics. [Formula: see text] (LSNO) is a classic example of such a material. At low temperatures holes introduced via substitution of La by Sr segregate into lines to form boundaries between magnetically ordered domains in the form of stripes. The stripes become dynamic at high temperatures, but LSNO remains insulating presumably because an interplay between magnetic correlations and electron–phonon coupling localizes charge carriers. Magnetic degrees of freedom have been extensively investigated in this system, but phonons are almost completely unexplored. We searched for electron–phonon anomalies in LSNO by inelastic neutron scattering. Giant renormalization of plane Ni–O bond-stretching modes that modulate the volume around Ni appears on entering the dynamic charge stripe phase. Other phonons are a lot less sensitive to stripe melting. Dramatic overdamping of the breathing modes indicates that dynamic stripe phase may host small polarons. We argue that this feature sets electron–phonon coupling in nickelates apart from that in cuprates where breathing phonons are not overdamped and point out remarkable similarities with the colossal magnetoresistance manganites. Nature Publishing Group UK 2020-07-10 /pmc/articles/PMC7351770/ /pubmed/32651413 http://dx.doi.org/10.1038/s41598-020-67963-x 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
Merritt, A. M.
Christianson, A. D.
Banerjee, A.
Gu, G. D.
Mishchenko, A. S.
Reznik, D.
Giant electron–phonon coupling of the breathing plane oxygen phonons in the dynamic stripe phase of [Formula: see text]
title Giant electron–phonon coupling of the breathing plane oxygen phonons in the dynamic stripe phase of [Formula: see text]
title_full Giant electron–phonon coupling of the breathing plane oxygen phonons in the dynamic stripe phase of [Formula: see text]
title_fullStr Giant electron–phonon coupling of the breathing plane oxygen phonons in the dynamic stripe phase of [Formula: see text]
title_full_unstemmed Giant electron–phonon coupling of the breathing plane oxygen phonons in the dynamic stripe phase of [Formula: see text]
title_short Giant electron–phonon coupling of the breathing plane oxygen phonons in the dynamic stripe phase of [Formula: see text]
title_sort giant electron–phonon coupling of the breathing plane oxygen phonons in the dynamic stripe phase of [formula: see text]
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7351770/
https://www.ncbi.nlm.nih.gov/pubmed/32651413
http://dx.doi.org/10.1038/s41598-020-67963-x
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