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The amplitudes and the structure of the charge density wave in YBCO

We find unknown s- and d-wave amplitudes of the recently discovered charge density wave (CDW) in underdoped cuprates. To do so we perform a combined analysis of experimental data for ortho-II YBa(2)Cu(3)O(y). The analysis includes data on nuclear magnetic resonance, resonant inelastic X-ray scatteri...

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Autores principales: Kharkov, Y. A., Sushkov, O. P.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2016
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5056359/
https://www.ncbi.nlm.nih.gov/pubmed/27721385
http://dx.doi.org/10.1038/srep34551
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author Kharkov, Y. A.
Sushkov, O. P.
author_facet Kharkov, Y. A.
Sushkov, O. P.
author_sort Kharkov, Y. A.
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description We find unknown s- and d-wave amplitudes of the recently discovered charge density wave (CDW) in underdoped cuprates. To do so we perform a combined analysis of experimental data for ortho-II YBa(2)Cu(3)O(y). The analysis includes data on nuclear magnetic resonance, resonant inelastic X-ray scattering, and hard X-ray diffraction. The amplitude of doping modulation found in our analysis is 3.5 · 10(−3) in a low magnetic field and T = 60 K, the amplitude is 6.5 · 10(−3) in a magnetic field of 30T and T = 1.3 K. The values are in units of elementary charge per unit cell of a CuO(2) plane. We show that the data rule out a checkerboard pattern, and we also show that the data might rule out mechanisms of the CDW which do not include phonons.
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spelling pubmed-50563592016-10-19 The amplitudes and the structure of the charge density wave in YBCO Kharkov, Y. A. Sushkov, O. P. Sci Rep Article We find unknown s- and d-wave amplitudes of the recently discovered charge density wave (CDW) in underdoped cuprates. To do so we perform a combined analysis of experimental data for ortho-II YBa(2)Cu(3)O(y). The analysis includes data on nuclear magnetic resonance, resonant inelastic X-ray scattering, and hard X-ray diffraction. The amplitude of doping modulation found in our analysis is 3.5 · 10(−3) in a low magnetic field and T = 60 K, the amplitude is 6.5 · 10(−3) in a magnetic field of 30T and T = 1.3 K. The values are in units of elementary charge per unit cell of a CuO(2) plane. We show that the data rule out a checkerboard pattern, and we also show that the data might rule out mechanisms of the CDW which do not include phonons. Nature Publishing Group 2016-10-10 /pmc/articles/PMC5056359/ /pubmed/27721385 http://dx.doi.org/10.1038/srep34551 Text en Copyright © 2016, The Author(s) http://creativecommons.org/licenses/by/4.0/ This work is licensed under a Creative Commons Attribution 4.0 International License. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in the credit line; if the material is not included under the Creative Commons license, users will need to obtain permission from the license holder to reproduce the material. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/
spellingShingle Article
Kharkov, Y. A.
Sushkov, O. P.
The amplitudes and the structure of the charge density wave in YBCO
title The amplitudes and the structure of the charge density wave in YBCO
title_full The amplitudes and the structure of the charge density wave in YBCO
title_fullStr The amplitudes and the structure of the charge density wave in YBCO
title_full_unstemmed The amplitudes and the structure of the charge density wave in YBCO
title_short The amplitudes and the structure of the charge density wave in YBCO
title_sort amplitudes and the structure of the charge density wave in ybco
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5056359/
https://www.ncbi.nlm.nih.gov/pubmed/27721385
http://dx.doi.org/10.1038/srep34551
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