Unprecedented phase transition sequence in the perovskite Li0.2Na0.8NbO3

The perovskite Li0.2Na0.8NbO3 is shown, by powder neutron diffraction, to display a unique sequence of phase transitions at elevated temperature. The ambient temperature polar phase (rhombohedral, space group R3c) transforms via a first-order transition to a polar tetragonal phase (space group P42mc...

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Main Authors: Charlotte A. L. Dixon, Jason A. McNulty, Steven Huband, Pamela A. Thomas, Philip Lightfoot
Format: Article
Language:English
Published: International Union of Crystallography 2017-05-01
Series:IUCrJ
Subjects:
Online Access:http://scripts.iucr.org/cgi-bin/paper?S2052252517002226
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spelling doaj-24498a21332b487b828f50a0f2020ed62020-11-24T22:37:14ZengInternational Union of CrystallographyIUCrJ2052-25252017-05-014321522210.1107/S2052252517002226fc5017Unprecedented phase transition sequence in the perovskite Li0.2Na0.8NbO3Charlotte A. L. Dixon0Jason A. McNulty1Steven Huband2Pamela A. Thomas3Philip Lightfoot4School of Chemistry and EaStCHEM, University of St Andrews, St Andrews KY16 9ST, ScotlandSchool of Chemistry and EaStCHEM, University of St Andrews, St Andrews KY16 9ST, ScotlandDepartment of Physics, University of Warwick, Coventry CV4 7AL, EnglandDepartment of Physics, University of Warwick, Coventry CV4 7AL, EnglandSchool of Chemistry and EaStCHEM, University of St Andrews, St Andrews KY16 9ST, ScotlandThe perovskite Li0.2Na0.8NbO3 is shown, by powder neutron diffraction, to display a unique sequence of phase transitions at elevated temperature. The ambient temperature polar phase (rhombohedral, space group R3c) transforms via a first-order transition to a polar tetragonal phase (space group P42mc) in the region 150–300°C; these two phases correspond to Glazer tilt systems a−a−a− and a+a+c−, respectively. At 500°C a ferroelectric–paraelectric transition takes place from P42mc to P42/nmc, retaining the a+a+c− tilt. Transformation to a single-tilt system, a0a0c+ (space group P4/mbm), occurs at 750°C, with the final transition to the aristotype cubic phase at 850°C. The P42mc and P42/nmc phases have each been seen only once and twice each, respectively, in perovskite crystallography, in each case in compositions prepared at high pressure.http://scripts.iucr.org/cgi-bin/paper?S2052252517002226perovskiteferroelectricpowder neutron diffraction
collection DOAJ
language English
format Article
sources DOAJ
author Charlotte A. L. Dixon
Jason A. McNulty
Steven Huband
Pamela A. Thomas
Philip Lightfoot
spellingShingle Charlotte A. L. Dixon
Jason A. McNulty
Steven Huband
Pamela A. Thomas
Philip Lightfoot
Unprecedented phase transition sequence in the perovskite Li0.2Na0.8NbO3
IUCrJ
perovskite
ferroelectric
powder neutron diffraction
author_facet Charlotte A. L. Dixon
Jason A. McNulty
Steven Huband
Pamela A. Thomas
Philip Lightfoot
author_sort Charlotte A. L. Dixon
title Unprecedented phase transition sequence in the perovskite Li0.2Na0.8NbO3
title_short Unprecedented phase transition sequence in the perovskite Li0.2Na0.8NbO3
title_full Unprecedented phase transition sequence in the perovskite Li0.2Na0.8NbO3
title_fullStr Unprecedented phase transition sequence in the perovskite Li0.2Na0.8NbO3
title_full_unstemmed Unprecedented phase transition sequence in the perovskite Li0.2Na0.8NbO3
title_sort unprecedented phase transition sequence in the perovskite li0.2na0.8nbo3
publisher International Union of Crystallography
series IUCrJ
issn 2052-2525
publishDate 2017-05-01
description The perovskite Li0.2Na0.8NbO3 is shown, by powder neutron diffraction, to display a unique sequence of phase transitions at elevated temperature. The ambient temperature polar phase (rhombohedral, space group R3c) transforms via a first-order transition to a polar tetragonal phase (space group P42mc) in the region 150–300°C; these two phases correspond to Glazer tilt systems a−a−a− and a+a+c−, respectively. At 500°C a ferroelectric–paraelectric transition takes place from P42mc to P42/nmc, retaining the a+a+c− tilt. Transformation to a single-tilt system, a0a0c+ (space group P4/mbm), occurs at 750°C, with the final transition to the aristotype cubic phase at 850°C. The P42mc and P42/nmc phases have each been seen only once and twice each, respectively, in perovskite crystallography, in each case in compositions prepared at high pressure.
topic perovskite
ferroelectric
powder neutron diffraction
url http://scripts.iucr.org/cgi-bin/paper?S2052252517002226
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