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dc.contributor.author |
Bagatskii, M.I. |
|
dc.contributor.author |
Sumarokov, V.V. |
|
dc.contributor.author |
Barabashko, M.S. |
|
dc.contributor.author |
Dolbin, A.V. |
|
dc.contributor.author |
Sundqvist, B. |
|
dc.date.accessioned |
2017-12-31T17:08:58Z |
|
dc.date.available |
2017-12-31T17:08:58Z |
|
dc.date.issued |
2015 |
|
dc.identifier.citation |
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. |
uk_UA |
dc.identifier.issn |
0132-6414 |
|
dc.identifier.other |
PACS: 65.40.Ba, 65.80.–g, 81.05.ub |
|
dc.identifier.uri |
http://dspace.nbuv.gov.ua/handle/123456789/127965 |
|
dc.description.abstract |
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). |
uk_UA |
dc.description.sponsorship |
The authors are indebted to A.I. Prokhvatilov, A.I. Krivchikov
and S.B. Feodosyev for a fruitful discussion. |
uk_UA |
dc.language.iso |
en |
uk_UA |
dc.publisher |
Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України |
uk_UA |
dc.relation.ispartof |
Физика низких температур |
|
dc.subject |
Наноструктуры при низких температурах |
uk_UA |
dc.title |
The low-temperature heat capacity of fullerite C₆₀ |
uk_UA |
dc.type |
Article |
uk_UA |
dc.status |
published earlier |
uk_UA |
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