The low-temperature heat capacity of fullerite C₆₀

The heat capacity at constant pressure of fullerite C₆₀ has been investigated using an adiabatic calorimeter in
 a temperature range from 1.2 to 120 K. Our results and literature data have been analyzed in a temperature interval
 from 0.2 to 300 K. The contributions of the intramolec...

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Published in:Физика низких температур
Date:2015
Main Authors: Bagatskii, M.I., Sumarokov, V.V., Barabashko, M.S., Dolbin, A.V., Sundqvist, B.
Format: Article
Language:English
Published: Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України 2015
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Online Access:https://nasplib.isofts.kiev.ua/handle/123456789/127965
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Cite this:The low-temperature heat capacity of fullerite C₆₀ / М.I. Bagatskii, V.V. Sumarokov, M.S. Barabashko, A.V. Dolbin, B. Sundqvist// Физика низких температур. — 2015. — Т. 41, № 8. — С. 812–819. — Бібліогр.: 54 назв. — англ.

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Digital Library of Periodicals of National Academy of Sciences of Ukraine
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author Bagatskii, M.I.
Sumarokov, V.V.
Barabashko, M.S.
Dolbin, A.V.
Sundqvist, B.
author_facet Bagatskii, M.I.
Sumarokov, V.V.
Barabashko, M.S.
Dolbin, A.V.
Sundqvist, B.
citation_txt The low-temperature heat capacity of fullerite C₆₀ / М.I. Bagatskii, V.V. Sumarokov, M.S. Barabashko, A.V. Dolbin, B. Sundqvist// Физика низких температур. — 2015. — Т. 41, № 8. — С. 812–819. — Бібліогр.: 54 назв. — англ.
collection DSpace DC
container_title Физика низких температур
description The heat capacity at constant pressure of fullerite C₆₀ has been investigated using an adiabatic calorimeter in
 a temperature range from 1.2 to 120 K. Our results and literature data have been analyzed in a temperature interval
 from 0.2 to 300 K. The contributions of the intramolecular and lattice vibrations into the heat capacity of C₆₀
 have been separated. The contribution of the intramolecular vibration becomes significant above 50 K. Below
 2.3 K the experimental temperature dependence of the heat capacity of C60 is described by the linear and cubic
 terms. The limiting Debye temperature at T → 0 K has been estimated (Θ0 = 84.4 K). In the interval from 1.2 to
 30 K the experimental curve of the heat capacity of C₆₀ describes the contributions of rotational tunnel levels,
 translational vibrations (in the Debye model with Θ0 = 84.4 K), and librations (in the Einstein model with
 ΘE,lib = 32.5 K). It is shown that the experimental temperature dependences of heat capacity and thermal expansion
 are proportional in the region from 5 to 60 K. The contribution of the cooperative processes of orientational
 disordering becomes appreciable above 180 K. In the high-temperature phase the lattice heat capacity at constant
 volume is close to 4.5 R, which corresponds to the high-temperature limit of translational vibrations (3 R) and
 the near-free rotational motion of C60 molecules (1.5 R).
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publishDate 2015
publisher Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
record_format dspace
spelling Bagatskii, M.I.
Sumarokov, V.V.
Barabashko, M.S.
Dolbin, A.V.
Sundqvist, B.
2017-12-31T17:08:58Z
2017-12-31T17:08:58Z
2015
The low-temperature heat capacity of fullerite C₆₀ / М.I. Bagatskii, V.V. Sumarokov, M.S. Barabashko, A.V. Dolbin, B. Sundqvist// Физика низких температур. — 2015. — Т. 41, № 8. — С. 812–819. — Бібліогр.: 54 назв. — англ.
0132-6414
PACS: 65.40.Ba, 65.80.–g, 81.05.ub
https://nasplib.isofts.kiev.ua/handle/123456789/127965
The heat capacity at constant pressure of fullerite C₆₀ has been investigated using an adiabatic calorimeter in
 a temperature range from 1.2 to 120 K. Our results and literature data have been analyzed in a temperature interval
 from 0.2 to 300 K. The contributions of the intramolecular and lattice vibrations into the heat capacity of C₆₀
 have been separated. The contribution of the intramolecular vibration becomes significant above 50 K. Below
 2.3 K the experimental temperature dependence of the heat capacity of C60 is described by the linear and cubic
 terms. The limiting Debye temperature at T → 0 K has been estimated (Θ0 = 84.4 K). In the interval from 1.2 to
 30 K the experimental curve of the heat capacity of C₆₀ describes the contributions of rotational tunnel levels,
 translational vibrations (in the Debye model with Θ0 = 84.4 K), and librations (in the Einstein model with
 ΘE,lib = 32.5 K). It is shown that the experimental temperature dependences of heat capacity and thermal expansion
 are proportional in the region from 5 to 60 K. The contribution of the cooperative processes of orientational
 disordering becomes appreciable above 180 K. In the high-temperature phase the lattice heat capacity at constant
 volume is close to 4.5 R, which corresponds to the high-temperature limit of translational vibrations (3 R) and
 the near-free rotational motion of C60 molecules (1.5 R).
The authors are indebted to A.I. Prokhvatilov, A.I. Krivchikov
 and S.B. Feodosyev for a fruitful discussion.
en
Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
Физика низких температур
Наноструктуры при низких температурах
The low-temperature heat capacity of fullerite C₆₀
Article
published earlier
spellingShingle The low-temperature heat capacity of fullerite C₆₀
Bagatskii, M.I.
Sumarokov, V.V.
Barabashko, M.S.
Dolbin, A.V.
Sundqvist, B.
Наноструктуры при низких температурах
title The low-temperature heat capacity of fullerite C₆₀
title_full The low-temperature heat capacity of fullerite C₆₀
title_fullStr The low-temperature heat capacity of fullerite C₆₀
title_full_unstemmed The low-temperature heat capacity of fullerite C₆₀
title_short The low-temperature heat capacity of fullerite C₆₀
title_sort low-temperature heat capacity of fullerite c₆₀
topic Наноструктуры при низких температурах
topic_facet Наноструктуры при низких температурах
url https://nasplib.isofts.kiev.ua/handle/123456789/127965
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