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The phase transition of Pb(8)F(14)I(2)

ABSTRACT: The reversible phase transition of Pb(8)F(14)I(2) is of continuous type and takes place at about 107 °C as monitored by temperature-dependent single crystal and powder X-ray diffraction measurements, optical microscopy, and differential scanning calorimetry. The low-temperature ferroelasti...

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Autor principal: Weil, Matthias
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Springer Vienna 2016
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5281681/
https://www.ncbi.nlm.nih.gov/pubmed/28203033
http://dx.doi.org/10.1007/s00706-016-1854-z
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author Weil, Matthias
author_facet Weil, Matthias
author_sort Weil, Matthias
collection PubMed
description ABSTRACT: The reversible phase transition of Pb(8)F(14)I(2) is of continuous type and takes place at about 107 °C as monitored by temperature-dependent single crystal and powder X-ray diffraction measurements, optical microscopy, and differential scanning calorimetry. The low-temperature ferroelastic phase crystallizes in the orthorhombic crystal system (23 °C, Bmmb, Z = 2, a = 6.0699(6) Å, b = 6.0165(6) Å, c = 25.077(2) Å, 1487 structure factors, 41 parameter, R(F (2)) = 0.0346, wR(F (2)) = 0.0771) and changes its symmetry to the tetragonal crystal system into the high-temperature paraelastic phase (130 °C, I4/mmm, Z = 1, a = 4.2667(12) Å, c = 25.388(7) Å, 430 structure factors, 303 parameter, R(F (2)) = 0.0575, wR(F (2)) = 0.1564). Group–subgroup relationships between the two structures and a hypothetical intermediate structure are presented. GRAPHICAL ABSTRACT: [Image: see text]
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spelling pubmed-52816812017-02-13 The phase transition of Pb(8)F(14)I(2) Weil, Matthias Monatsh Chem Original Paper ABSTRACT: The reversible phase transition of Pb(8)F(14)I(2) is of continuous type and takes place at about 107 °C as monitored by temperature-dependent single crystal and powder X-ray diffraction measurements, optical microscopy, and differential scanning calorimetry. The low-temperature ferroelastic phase crystallizes in the orthorhombic crystal system (23 °C, Bmmb, Z = 2, a = 6.0699(6) Å, b = 6.0165(6) Å, c = 25.077(2) Å, 1487 structure factors, 41 parameter, R(F (2)) = 0.0346, wR(F (2)) = 0.0771) and changes its symmetry to the tetragonal crystal system into the high-temperature paraelastic phase (130 °C, I4/mmm, Z = 1, a = 4.2667(12) Å, c = 25.388(7) Å, 430 structure factors, 303 parameter, R(F (2)) = 0.0575, wR(F (2)) = 0.1564). Group–subgroup relationships between the two structures and a hypothetical intermediate structure are presented. GRAPHICAL ABSTRACT: [Image: see text] Springer Vienna 2016-10-28 2017 /pmc/articles/PMC5281681/ /pubmed/28203033 http://dx.doi.org/10.1007/s00706-016-1854-z Text en © The Author(s) 2016 Open AccessThis article is distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium, provided 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.
spellingShingle Original Paper
Weil, Matthias
The phase transition of Pb(8)F(14)I(2)
title The phase transition of Pb(8)F(14)I(2)
title_full The phase transition of Pb(8)F(14)I(2)
title_fullStr The phase transition of Pb(8)F(14)I(2)
title_full_unstemmed The phase transition of Pb(8)F(14)I(2)
title_short The phase transition of Pb(8)F(14)I(2)
title_sort phase transition of pb(8)f(14)i(2)
topic Original Paper
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5281681/
https://www.ncbi.nlm.nih.gov/pubmed/28203033
http://dx.doi.org/10.1007/s00706-016-1854-z
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