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Coherence in the Ferroelectric A(3)ClO (A = Li, Na) Family of Electrolytes

Coherence is a major caveat in quantum computing. While phonons and electrons are weakly coupled in a glass, topological insulators strongly depend on the electron-phonon coupling. Knowledge of the electron−phonon interaction at conducting surfaces is relevant from a fundamental point of view as wel...

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Autor principal: Braga, Maria Helena
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8125208/
https://www.ncbi.nlm.nih.gov/pubmed/34062993
http://dx.doi.org/10.3390/ma14092398
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author Braga, Maria Helena
author_facet Braga, Maria Helena
author_sort Braga, Maria Helena
collection PubMed
description Coherence is a major caveat in quantum computing. While phonons and electrons are weakly coupled in a glass, topological insulators strongly depend on the electron-phonon coupling. Knowledge of the electron−phonon interaction at conducting surfaces is relevant from a fundamental point of view as well as for various applications, such as two-dimensional and quasi-1D superconductivity in nanotechnology. Similarly, the electron−phonon interaction plays a relevant role in other transport properties e.g., thermoelectricity, low-dimensional systems as layered Bi and Sb chalcogenides, and quasi-crystalline materials. Glass-electrolyte ferroelectric energy storage cells exhibit self-charge and self-cycling related to topological superconductivity and electron-phonon coupling; phonon coherence is therefore important. By recurring to ab initio molecular dynamics, it was demonstrated the tendency of the Li(3)ClO, Li(2.92)Ba(0.04)ClO, Na(3)ClO, and Na(2.92)Ba(0.04)ClO ferroelectric-electrolytes to keep phonon oscillation coherence for a short lapse of time in ps. Double-well energy potentials were obtained while the electrolyte systems were thermostatted in a heat bath at a constant temperature. The latter occurrences indicate ferroelectric type behavior but do not justify the coherent self-oscillations observed in all types of cells containing these families of electrolytes and, therefore, an emergent type phenomenon where the full cell works as a feedback system allowing oscillations coherence must be realized. A comparison with amorphous SiO(2) was performed and the specific heats for the various species were calculated.
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spelling pubmed-81252082021-05-17 Coherence in the Ferroelectric A(3)ClO (A = Li, Na) Family of Electrolytes Braga, Maria Helena Materials (Basel) Review Coherence is a major caveat in quantum computing. While phonons and electrons are weakly coupled in a glass, topological insulators strongly depend on the electron-phonon coupling. Knowledge of the electron−phonon interaction at conducting surfaces is relevant from a fundamental point of view as well as for various applications, such as two-dimensional and quasi-1D superconductivity in nanotechnology. Similarly, the electron−phonon interaction plays a relevant role in other transport properties e.g., thermoelectricity, low-dimensional systems as layered Bi and Sb chalcogenides, and quasi-crystalline materials. Glass-electrolyte ferroelectric energy storage cells exhibit self-charge and self-cycling related to topological superconductivity and electron-phonon coupling; phonon coherence is therefore important. By recurring to ab initio molecular dynamics, it was demonstrated the tendency of the Li(3)ClO, Li(2.92)Ba(0.04)ClO, Na(3)ClO, and Na(2.92)Ba(0.04)ClO ferroelectric-electrolytes to keep phonon oscillation coherence for a short lapse of time in ps. Double-well energy potentials were obtained while the electrolyte systems were thermostatted in a heat bath at a constant temperature. The latter occurrences indicate ferroelectric type behavior but do not justify the coherent self-oscillations observed in all types of cells containing these families of electrolytes and, therefore, an emergent type phenomenon where the full cell works as a feedback system allowing oscillations coherence must be realized. A comparison with amorphous SiO(2) was performed and the specific heats for the various species were calculated. MDPI 2021-05-05 /pmc/articles/PMC8125208/ /pubmed/34062993 http://dx.doi.org/10.3390/ma14092398 Text en © 2021 by the author. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Review
Braga, Maria Helena
Coherence in the Ferroelectric A(3)ClO (A = Li, Na) Family of Electrolytes
title Coherence in the Ferroelectric A(3)ClO (A = Li, Na) Family of Electrolytes
title_full Coherence in the Ferroelectric A(3)ClO (A = Li, Na) Family of Electrolytes
title_fullStr Coherence in the Ferroelectric A(3)ClO (A = Li, Na) Family of Electrolytes
title_full_unstemmed Coherence in the Ferroelectric A(3)ClO (A = Li, Na) Family of Electrolytes
title_short Coherence in the Ferroelectric A(3)ClO (A = Li, Na) Family of Electrolytes
title_sort coherence in the ferroelectric a(3)clo (a = li, na) family of electrolytes
topic Review
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8125208/
https://www.ncbi.nlm.nih.gov/pubmed/34062993
http://dx.doi.org/10.3390/ma14092398
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