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Peculiarities of Phase Formation in Mn-Based Na SuperIonic Conductor (NaSICon) Systems: The Case of Na(1+2x)Mn(x)Ti(2–x)(PO(4))(3) (0.0 ≤ x ≤ 1.5)

[Image: see text] NAtrium SuperIonic CONductor (NASICON) structured phosphate framework compounds are attracting a great deal of interest as suitable electrode materials for “rocking chair” type batteries. Manganese-based electrode materials are among the most favored due to their superior stability...

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Autores principales: Snarskis, Gustautas, Pilipavičius, Jurgis, Gryaznov, Denis, Mikoliu̅naitė, Lina, Vilčiauskas, Linas
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2021
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8721591/
https://www.ncbi.nlm.nih.gov/pubmed/34992333
http://dx.doi.org/10.1021/acs.chemmater.1c02775
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author Snarskis, Gustautas
Pilipavičius, Jurgis
Gryaznov, Denis
Mikoliu̅naitė, Lina
Vilčiauskas, Linas
author_facet Snarskis, Gustautas
Pilipavičius, Jurgis
Gryaznov, Denis
Mikoliu̅naitė, Lina
Vilčiauskas, Linas
author_sort Snarskis, Gustautas
collection PubMed
description [Image: see text] NAtrium SuperIonic CONductor (NASICON) structured phosphate framework compounds are attracting a great deal of interest as suitable electrode materials for “rocking chair” type batteries. Manganese-based electrode materials are among the most favored due to their superior stability, resource non-criticality, and high electrode potentials. Although a large share of research was devoted to Mn-based oxides for Li- and Na-ion batteries, the understanding of thermodynamics and phase formation in Mn-rich polyanions is still generally lacking. In this study, we investigate a bifunctional Na-ion battery electrode system based on NASICON-structured Na(1+2x)Mn(x)Ti(2–x)(PO(4))(3) (0.0 ≤ x ≤ 1.5). In order to analyze the thermodynamic and phase formation properties, we construct a composition–temperature phase diagram using a computational sampling by density functional theory, cluster expansion, and semi-grand canonical Monte Carlo methods. The results indicate finite thermodynamic limits of possible Mn concentrations in this system, which are primarily determined by the phase separation into stoichiometric Na(3)MnTi(PO(4))(3) (x = 1.0) and NaTi(2)(PO(4))(3) for x < 1.0 or NaMnPO(4) for x > 1.0. The theoretical predictions are corroborated by experiments obtained using X-ray diffraction and Raman spectroscopy on solid-state and sol–gel prepared samples. The results confirm that this system does not show a solid solution type behavior but phase-separates into thermodynamically more stable sodium ordered monoclinic α-Na(3)MnTi(PO(4))(3) (space group C2) and other phases. In addition to sodium ordering, the anti-bonding character of the Mn–O bond as compared to Ti–O is suggested as another important factor governing the stability of Mn-based NASICONs. We believe that these results will not only clarify some important questions regarding the thermodynamic properties of NASICON frameworks but will also be helpful for a more general understanding of polyanionic systems.
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spelling pubmed-87215912022-01-04 Peculiarities of Phase Formation in Mn-Based Na SuperIonic Conductor (NaSICon) Systems: The Case of Na(1+2x)Mn(x)Ti(2–x)(PO(4))(3) (0.0 ≤ x ≤ 1.5) Snarskis, Gustautas Pilipavičius, Jurgis Gryaznov, Denis Mikoliu̅naitė, Lina Vilčiauskas, Linas Chem Mater [Image: see text] NAtrium SuperIonic CONductor (NASICON) structured phosphate framework compounds are attracting a great deal of interest as suitable electrode materials for “rocking chair” type batteries. Manganese-based electrode materials are among the most favored due to their superior stability, resource non-criticality, and high electrode potentials. Although a large share of research was devoted to Mn-based oxides for Li- and Na-ion batteries, the understanding of thermodynamics and phase formation in Mn-rich polyanions is still generally lacking. In this study, we investigate a bifunctional Na-ion battery electrode system based on NASICON-structured Na(1+2x)Mn(x)Ti(2–x)(PO(4))(3) (0.0 ≤ x ≤ 1.5). In order to analyze the thermodynamic and phase formation properties, we construct a composition–temperature phase diagram using a computational sampling by density functional theory, cluster expansion, and semi-grand canonical Monte Carlo methods. The results indicate finite thermodynamic limits of possible Mn concentrations in this system, which are primarily determined by the phase separation into stoichiometric Na(3)MnTi(PO(4))(3) (x = 1.0) and NaTi(2)(PO(4))(3) for x < 1.0 or NaMnPO(4) for x > 1.0. The theoretical predictions are corroborated by experiments obtained using X-ray diffraction and Raman spectroscopy on solid-state and sol–gel prepared samples. The results confirm that this system does not show a solid solution type behavior but phase-separates into thermodynamically more stable sodium ordered monoclinic α-Na(3)MnTi(PO(4))(3) (space group C2) and other phases. In addition to sodium ordering, the anti-bonding character of the Mn–O bond as compared to Ti–O is suggested as another important factor governing the stability of Mn-based NASICONs. We believe that these results will not only clarify some important questions regarding the thermodynamic properties of NASICON frameworks but will also be helpful for a more general understanding of polyanionic systems. American Chemical Society 2021-10-21 2021-11-09 /pmc/articles/PMC8721591/ /pubmed/34992333 http://dx.doi.org/10.1021/acs.chemmater.1c02775 Text en © 2021 American Chemical Society https://creativecommons.org/licenses/by/4.0/Permits the broadest form of re-use including for commercial purposes, provided that author attribution and integrity are maintained (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Snarskis, Gustautas
Pilipavičius, Jurgis
Gryaznov, Denis
Mikoliu̅naitė, Lina
Vilčiauskas, Linas
Peculiarities of Phase Formation in Mn-Based Na SuperIonic Conductor (NaSICon) Systems: The Case of Na(1+2x)Mn(x)Ti(2–x)(PO(4))(3) (0.0 ≤ x ≤ 1.5)
title Peculiarities of Phase Formation in Mn-Based Na SuperIonic Conductor (NaSICon) Systems: The Case of Na(1+2x)Mn(x)Ti(2–x)(PO(4))(3) (0.0 ≤ x ≤ 1.5)
title_full Peculiarities of Phase Formation in Mn-Based Na SuperIonic Conductor (NaSICon) Systems: The Case of Na(1+2x)Mn(x)Ti(2–x)(PO(4))(3) (0.0 ≤ x ≤ 1.5)
title_fullStr Peculiarities of Phase Formation in Mn-Based Na SuperIonic Conductor (NaSICon) Systems: The Case of Na(1+2x)Mn(x)Ti(2–x)(PO(4))(3) (0.0 ≤ x ≤ 1.5)
title_full_unstemmed Peculiarities of Phase Formation in Mn-Based Na SuperIonic Conductor (NaSICon) Systems: The Case of Na(1+2x)Mn(x)Ti(2–x)(PO(4))(3) (0.0 ≤ x ≤ 1.5)
title_short Peculiarities of Phase Formation in Mn-Based Na SuperIonic Conductor (NaSICon) Systems: The Case of Na(1+2x)Mn(x)Ti(2–x)(PO(4))(3) (0.0 ≤ x ≤ 1.5)
title_sort peculiarities of phase formation in mn-based na superionic conductor (nasicon) systems: the case of na(1+2x)mn(x)ti(2–x)(po(4))(3) (0.0 ≤ x ≤ 1.5)
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8721591/
https://www.ncbi.nlm.nih.gov/pubmed/34992333
http://dx.doi.org/10.1021/acs.chemmater.1c02775
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