Many-body interactions and high-pressure equations of state in rare-gas solids
The T 0K equations of state (EOS) of rare-gas solids (RGS) (He, Ne, Ar, Kr, and Xe) are calculated in the experimentally studied ranges of pressures accounting for two- and three-body interatomic forces. Solid-state corrections to the pure two-body Aziz et al. potentials included the long-range...
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Дата: | 2007 |
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Мова: | English |
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Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
2007
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Цитувати: | Many-body interactions and high-pressure equations of state in rare-gas solids / Yu.A. Freiman, S.M. Tretyak // Физика низких температур. — 2007. — Т. 33, № 6-7. — С. 719-727. — Бібліогр.: 48 назв. — англ. |
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irk-123456789-1217732017-06-17T03:02:54Z Many-body interactions and high-pressure equations of state in rare-gas solids Freiman, Yu.A. Tretyak, S.M. Classical Cryocrystals The T 0K equations of state (EOS) of rare-gas solids (RGS) (He, Ne, Ar, Kr, and Xe) are calculated in the experimentally studied ranges of pressures accounting for two- and three-body interatomic forces. Solid-state corrections to the pure two-body Aziz et al. potentials included the long-range Axilrod–Teller three-body interaction and short-range three-body exchange interaction. The energy-scale and length-scale parameters of the latter were taken as adjustable parameters of theory. The calculated T 0K EOS for all RGS are in excellent agreement with experiment in the whole range of pressures. The calculated EOS for Ar, Kr, and Xe exhibit inflection points where the isothermal bulk moduli have non-physical maxima indicating that account of only three-body forces becomes insufficient. These points lie at pressures 250, 200, and 175 GPa (volume compressions of approximately 4.8, 4.1, and 3.6) for Ar, Kr, and Xe, respectively. No such points were found in the calculated EOS of He and Ne. The relative magnitude of the three-body contribution to the ground-state energy with respect to the two-body one as a function of the volume compression was found to be non-monotonic in the sequence Ne–Ar–Kr–Xe. In a large range of compressions, Kr has the highest value of this ratio. This anomally high three-body exchange forces contributes to the EOS so large negative pressure that the EOS for Kr and Ar as a function of compression nearly coincide. At compressions higher approximately 3.5, the curves intersect and further on the EOS of Kr lies lower than that of Ar. 2007 Article Many-body interactions and high-pressure equations of state in rare-gas solids / Yu.A. Freiman, S.M. Tretyak // Физика низких температур. — 2007. — Т. 33, № 6-7. — С. 719-727. — Бібліогр.: 48 назв. — англ. 0132-6414 PACS: 64.60.Cn; 67.80.–s; 67.90.+z http://dspace.nbuv.gov.ua/handle/123456789/121773 en Физика низких температур Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України |
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Digital Library of Periodicals of National Academy of Sciences of Ukraine |
collection |
DSpace DC |
language |
English |
topic |
Classical Cryocrystals Classical Cryocrystals |
spellingShingle |
Classical Cryocrystals Classical Cryocrystals Freiman, Yu.A. Tretyak, S.M. Many-body interactions and high-pressure equations of state in rare-gas solids Физика низких температур |
description |
The T 0K equations of state (EOS) of rare-gas solids (RGS) (He, Ne, Ar, Kr, and Xe) are calculated in
the experimentally studied ranges of pressures accounting for two- and three-body interatomic forces.
Solid-state corrections to the pure two-body Aziz et al. potentials included the long-range Axilrod–Teller
three-body interaction and short-range three-body exchange interaction. The energy-scale and length-scale
parameters of the latter were taken as adjustable parameters of theory. The calculated T 0K EOS for all
RGS are in excellent agreement with experiment in the whole range of pressures. The calculated EOS for Ar,
Kr, and Xe exhibit inflection points where the isothermal bulk moduli have non-physical maxima indicating
that account of only three-body forces becomes insufficient. These points lie at pressures 250, 200, and 175
GPa (volume compressions of approximately 4.8, 4.1, and 3.6) for Ar, Kr, and Xe, respectively. No such
points were found in the calculated EOS of He and Ne. The relative magnitude of the three-body contribution
to the ground-state energy with respect to the two-body one as a function of the volume compression
was found to be non-monotonic in the sequence Ne–Ar–Kr–Xe. In a large range of compressions, Kr has the
highest value of this ratio. This anomally high three-body exchange forces contributes to the EOS so large
negative pressure that the EOS for Kr and Ar as a function of compression nearly coincide. At compressions
higher approximately 3.5, the curves intersect and further on the EOS of Kr lies lower than that of Ar. |
format |
Article |
author |
Freiman, Yu.A. Tretyak, S.M. |
author_facet |
Freiman, Yu.A. Tretyak, S.M. |
author_sort |
Freiman, Yu.A. |
title |
Many-body interactions and high-pressure equations of state in rare-gas solids |
title_short |
Many-body interactions and high-pressure equations of state in rare-gas solids |
title_full |
Many-body interactions and high-pressure equations of state in rare-gas solids |
title_fullStr |
Many-body interactions and high-pressure equations of state in rare-gas solids |
title_full_unstemmed |
Many-body interactions and high-pressure equations of state in rare-gas solids |
title_sort |
many-body interactions and high-pressure equations of state in rare-gas solids |
publisher |
Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України |
publishDate |
2007 |
topic_facet |
Classical Cryocrystals |
url |
http://dspace.nbuv.gov.ua/handle/123456789/121773 |
citation_txt |
Many-body interactions and high-pressure
equations of state in rare-gas solids / Yu.A. Freiman, S.M. Tretyak // Физика низких температур. — 2007. — Т. 33, № 6-7. — С. 719-727. — Бібліогр.: 48 назв. — англ. |
series |
Физика низких температур |
work_keys_str_mv |
AT freimanyua manybodyinteractionsandhighpressureequationsofstateinraregassolids AT tretyaksm manybodyinteractionsandhighpressureequationsofstateinraregassolids |
first_indexed |
2023-10-18T20:40:17Z |
last_indexed |
2023-10-18T20:40:17Z |
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1796150807884726272 |