Elastic phase transitions in solids. High pressure effect

At high pressures (the pressure is comparable with the bulk modulus) the crystalline lattice may become unstable relative to the uniform shear deformations, and in a result the low symmetric crystalline structures will appear (the so-called “elastic phase transitions”). The order parameters at these...

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Published in:Физика низких температур
Date:2018
Main Authors: Vekilov, Yu.Kh., Krasilnikov, O.M.
Format: Article
Language:English
Published: Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України 2018
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Online Access:https://nasplib.isofts.kiev.ua/handle/123456789/176171
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Journal Title:Digital Library of Periodicals of National Academy of Sciences of Ukraine
Cite this:Elastic phase transitions in solids. High pressure effect / Yu.Kh. Vekilov, O.M. Krasilnikov // Физика низких температур. — 2018. — Т. 44, № 6. — С. 758-764. — Бібліогр.: 30 назв. — англ.

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Digital Library of Periodicals of National Academy of Sciences of Ukraine
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author Vekilov, Yu.Kh.
Krasilnikov, O.M.
author_facet Vekilov, Yu.Kh.
Krasilnikov, O.M.
citation_txt Elastic phase transitions in solids. High pressure effect / Yu.Kh. Vekilov, O.M. Krasilnikov // Физика низких температур. — 2018. — Т. 44, № 6. — С. 758-764. — Бібліогр.: 30 назв. — англ.
collection DSpace DC
container_title Физика низких температур
description At high pressures (the pressure is comparable with the bulk modulus) the crystalline lattice may become unstable relative to the uniform shear deformations, and in a result the low symmetric crystalline structures will appear (the so-called “elastic phase transitions”). The order parameters at these transitions are the components of the finite deformations tensor. The stability of the high-pressure phases is defined by the nonlinear elasticity of the lattice (the third, fourth etc. order elastic constants). Here the different cases of the stability loss at hydro-static pressure for the cubic structures are considered. The relation between the second, third and fourth order elastic constants is given, which defines the possibility of the first order deformation phase transition. The jump of the order parameter and the height of the potential barrier are defined by the third and fourth order elastic constants. As an example, the experimentally observed elastic phase transition in vanadium at P ≈ 69 GPa from bcc to the rhombohedral phase is analyzed, and the possible structural transitions in bcc Mo and W at P ≥ 700 GPa are also considered.
first_indexed 2025-12-07T17:22:38Z
format Article
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institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
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language English
last_indexed 2025-12-07T17:22:38Z
publishDate 2018
publisher Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
record_format dspace
spelling Vekilov, Yu.Kh.
Krasilnikov, O.M.
2021-02-03T19:43:48Z
2021-02-03T19:43:48Z
2018
Elastic phase transitions in solids. High pressure effect / Yu.Kh. Vekilov, O.M. Krasilnikov // Физика низких температур. — 2018. — Т. 44, № 6. — С. 758-764. — Бібліогр.: 30 назв. — англ.
0132-6414
PACS: 61.50.Ks, 61.66.Bi, 62.20.D–, 62.50.–p
https://nasplib.isofts.kiev.ua/handle/123456789/176171
At high pressures (the pressure is comparable with the bulk modulus) the crystalline lattice may become unstable relative to the uniform shear deformations, and in a result the low symmetric crystalline structures will appear (the so-called “elastic phase transitions”). The order parameters at these transitions are the components of the finite deformations tensor. The stability of the high-pressure phases is defined by the nonlinear elasticity of the lattice (the third, fourth etc. order elastic constants). Here the different cases of the stability loss at hydro-static pressure for the cubic structures are considered. The relation between the second, third and fourth order elastic constants is given, which defines the possibility of the first order deformation phase transition. The jump of the order parameter and the height of the potential barrier are defined by the third and fourth order elastic constants. As an example, the experimentally observed elastic phase transition in vanadium at P ≈ 69 GPa from bcc to the rhombohedral phase is analyzed, and the possible structural transitions in bcc Mo and W at P ≥ 700 GPa are also considered.
The work is executed at financial support of the Ministry of Education and Science of the Russian Federation
 (Grant No. 14.Y26.31.0005) and the Russian Foundation
 for Basic Research (Grant 16-02-00699 and Grant 16-02-
 01027).
en
Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
Физика низких температур
Специальный выпуск К 90-летию со дня рождения A.A. Абрикосова
Elastic phase transitions in solids. High pressure effect
Article
published earlier
spellingShingle Elastic phase transitions in solids. High pressure effect
Vekilov, Yu.Kh.
Krasilnikov, O.M.
Специальный выпуск К 90-летию со дня рождения A.A. Абрикосова
title Elastic phase transitions in solids. High pressure effect
title_full Elastic phase transitions in solids. High pressure effect
title_fullStr Elastic phase transitions in solids. High pressure effect
title_full_unstemmed Elastic phase transitions in solids. High pressure effect
title_short Elastic phase transitions in solids. High pressure effect
title_sort elastic phase transitions in solids. high pressure effect
topic Специальный выпуск К 90-летию со дня рождения A.A. Абрикосова
topic_facet Специальный выпуск К 90-летию со дня рождения A.A. Абрикосова
url https://nasplib.isofts.kiev.ua/handle/123456789/176171
work_keys_str_mv AT vekilovyukh elasticphasetransitionsinsolidshighpressureeffect
AT krasilnikovom elasticphasetransitionsinsolidshighpressureeffect