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High pressure phase transitions of paracelsian BaAl(2)Si(2)O(8)

Three new polymorphs of aluminosilicate paracelsian, BaAl(2)Si(2)O(8), have been discovered using synchrotron-based in situ high-pressure single crystal X-ray diffraction. The first isosymmetric phase transition (from paracelsian-I to paracelsian-II) occurs between 3 and 6 GPa. The phase transition...

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Autores principales: Gorelova, Liudmila A., Pakhomova, Anna S., Krivovichev, Sergey V., Dubrovinsky, Leonid S., Kasatkin, Anatoly V.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2019
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6718520/
https://www.ncbi.nlm.nih.gov/pubmed/31477776
http://dx.doi.org/10.1038/s41598-019-49112-1
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author Gorelova, Liudmila A.
Pakhomova, Anna S.
Krivovichev, Sergey V.
Dubrovinsky, Leonid S.
Kasatkin, Anatoly V.
author_facet Gorelova, Liudmila A.
Pakhomova, Anna S.
Krivovichev, Sergey V.
Dubrovinsky, Leonid S.
Kasatkin, Anatoly V.
author_sort Gorelova, Liudmila A.
collection PubMed
description Three new polymorphs of aluminosilicate paracelsian, BaAl(2)Si(2)O(8), have been discovered using synchrotron-based in situ high-pressure single crystal X-ray diffraction. The first isosymmetric phase transition (from paracelsian-I to paracelsian-II) occurs between 3 and 6 GPa. The phase transition is associated with the formation of pentacoordinated Al(3+) and Si(4+) ions, which occurs in a stepwise fashion by sequential formation of Al-O and Si-O bonds additional to those in AlO(4) and SiO(4) tetrahedra, respectively. The next phase transition occurs between 25 and 28 GPa and is accompanied by the symmetry change from monoclinic (P2(1)/c) to orthorhombic (Pna2(1)). The structure of paracelsian-III consists of SiO(6) octahedra, AlO(6) octahedra and distorted AlO(4) tetrahedra, i.e. the transition is reconstructive and associated with the changes of Si(4+) and Al(3+) coordination, which show rather complex behaviour with the general tendency towards increasing coordination numbers. The third phase transition is observed between 28 and 32 GPa and results in the symmetry decreasing from Pna2(1) to Pn. The transition has a displacive character. In the course of the phase transformation pathway up to 32 GPa, the structure of polymorphs becomes denser: paracelsian-II is based upon elements of cubic and hexagonal close-packing arrangements of large O(2−) and Ba(2+) ions, whereas, in the crystal structure of paracelsian-III and IV, this arrangement corresponds to 9-layer closest-packing with the layer sequence ABACACBCB.
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spelling pubmed-67185202019-09-17 High pressure phase transitions of paracelsian BaAl(2)Si(2)O(8) Gorelova, Liudmila A. Pakhomova, Anna S. Krivovichev, Sergey V. Dubrovinsky, Leonid S. Kasatkin, Anatoly V. Sci Rep Article Three new polymorphs of aluminosilicate paracelsian, BaAl(2)Si(2)O(8), have been discovered using synchrotron-based in situ high-pressure single crystal X-ray diffraction. The first isosymmetric phase transition (from paracelsian-I to paracelsian-II) occurs between 3 and 6 GPa. The phase transition is associated with the formation of pentacoordinated Al(3+) and Si(4+) ions, which occurs in a stepwise fashion by sequential formation of Al-O and Si-O bonds additional to those in AlO(4) and SiO(4) tetrahedra, respectively. The next phase transition occurs between 25 and 28 GPa and is accompanied by the symmetry change from monoclinic (P2(1)/c) to orthorhombic (Pna2(1)). The structure of paracelsian-III consists of SiO(6) octahedra, AlO(6) octahedra and distorted AlO(4) tetrahedra, i.e. the transition is reconstructive and associated with the changes of Si(4+) and Al(3+) coordination, which show rather complex behaviour with the general tendency towards increasing coordination numbers. The third phase transition is observed between 28 and 32 GPa and results in the symmetry decreasing from Pna2(1) to Pn. The transition has a displacive character. In the course of the phase transformation pathway up to 32 GPa, the structure of polymorphs becomes denser: paracelsian-II is based upon elements of cubic and hexagonal close-packing arrangements of large O(2−) and Ba(2+) ions, whereas, in the crystal structure of paracelsian-III and IV, this arrangement corresponds to 9-layer closest-packing with the layer sequence ABACACBCB. Nature Publishing Group UK 2019-09-02 /pmc/articles/PMC6718520/ /pubmed/31477776 http://dx.doi.org/10.1038/s41598-019-49112-1 Text en © The Author(s) 2019 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
Gorelova, Liudmila A.
Pakhomova, Anna S.
Krivovichev, Sergey V.
Dubrovinsky, Leonid S.
Kasatkin, Anatoly V.
High pressure phase transitions of paracelsian BaAl(2)Si(2)O(8)
title High pressure phase transitions of paracelsian BaAl(2)Si(2)O(8)
title_full High pressure phase transitions of paracelsian BaAl(2)Si(2)O(8)
title_fullStr High pressure phase transitions of paracelsian BaAl(2)Si(2)O(8)
title_full_unstemmed High pressure phase transitions of paracelsian BaAl(2)Si(2)O(8)
title_short High pressure phase transitions of paracelsian BaAl(2)Si(2)O(8)
title_sort high pressure phase transitions of paracelsian baal(2)si(2)o(8)
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6718520/
https://www.ncbi.nlm.nih.gov/pubmed/31477776
http://dx.doi.org/10.1038/s41598-019-49112-1
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