Process of intercalation of C₆₀ with molecular hydrogen from XRD data

The process of normal hydrogen infusion into a C₆₀ powder at 1 bar and room temperature was monitored using x-ray diffraction. The effect of the intercalation on the lattice proved to be rather weak: the volume expansion upon complete saturation does not exceed 0.13%. The characteristic saturation t...

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Published in:Физика низких температур
Date:2009
Main Authors: Yagotintsev, K.A., Stetsenko, Yu.E., Legchenkova, I.V., Prokhvatilov, A.I., Strzhemechny, M.A., Schafler, E., Zehetbauer, M.
Format: Article
Language:English
Published: Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України 2009
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Online Access:https://nasplib.isofts.kiev.ua/handle/123456789/117052
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Journal Title:Digital Library of Periodicals of National Academy of Sciences of Ukraine
Cite this:Process of intercalation of C₆₀ with molecular hydrogen from XRD data / K.A. Yagotintsev, Yu.E. Stetsenko, I.V. Legchenkova, A.I. Prokhvatilov, M.A. Strzhemechny, E. Schafler, M. Zehetbauer // Физика низких температур. — 2009. — Т. 35, № 3. — С. 315-319 . — Бібліогр.: 25 назв. — англ.

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Digital Library of Periodicals of National Academy of Sciences of Ukraine
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author Yagotintsev, K.A.
Stetsenko, Yu.E.
Legchenkova, I.V.
Prokhvatilov, A.I.
Strzhemechny, M.A.
Schafler, E.
Zehetbauer, M.
author_facet Yagotintsev, K.A.
Stetsenko, Yu.E.
Legchenkova, I.V.
Prokhvatilov, A.I.
Strzhemechny, M.A.
Schafler, E.
Zehetbauer, M.
citation_txt Process of intercalation of C₆₀ with molecular hydrogen from XRD data / K.A. Yagotintsev, Yu.E. Stetsenko, I.V. Legchenkova, A.I. Prokhvatilov, M.A. Strzhemechny, E. Schafler, M. Zehetbauer // Физика низких температур. — 2009. — Т. 35, № 3. — С. 315-319 . — Бібліогр.: 25 назв. — англ.
collection DSpace DC
container_title Физика низких температур
description The process of normal hydrogen infusion into a C₆₀ powder at 1 bar and room temperature was monitored using x-ray diffraction. The effect of the intercalation on the lattice proved to be rather weak: the volume expansion upon complete saturation does not exceed 0.13%. The characteristic saturation time was found to be 320 h; the corresponding diffusion coefficient amounts to (2.8 ± 0.8)·10⁻¹⁴ cm²/s. The integrated reflection intensity calculations for completely saturated sample suggest that only octahedral voids are filled under the conditions of experiment. The effect of complete saturation on the rotational subsystem of the C₆₀ fullerite is rather weak: the orientational phase transition shifts by 6 to 7 K to lower temperatures; no essential hysteresis is noticeable. The dopant shows reluctance to leave the sample under a vacuum of 10⁻³ Torr at room temperature.
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last_indexed 2025-11-24T04:19:02Z
publishDate 2009
publisher Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
record_format dspace
spelling Yagotintsev, K.A.
Stetsenko, Yu.E.
Legchenkova, I.V.
Prokhvatilov, A.I.
Strzhemechny, M.A.
Schafler, E.
Zehetbauer, M.
2017-05-19T09:37:24Z
2017-05-19T09:37:24Z
2009
Process of intercalation of C₆₀ with molecular hydrogen from XRD data / K.A. Yagotintsev, Yu.E. Stetsenko, I.V. Legchenkova, A.I. Prokhvatilov, M.A. Strzhemechny, E. Schafler, M. Zehetbauer // Физика низких температур. — 2009. — Т. 35, № 3. — С. 315-319 . — Бібліогр.: 25 назв. — англ.
0132-6414
PACS: 61.05.cp, 61.48.–c, 61.72.J-, 61.72.U-
https://nasplib.isofts.kiev.ua/handle/123456789/117052
The process of normal hydrogen infusion into a C₆₀ powder at 1 bar and room temperature was monitored using x-ray diffraction. The effect of the intercalation on the lattice proved to be rather weak: the volume expansion upon complete saturation does not exceed 0.13%. The characteristic saturation time was found to be 320 h; the corresponding diffusion coefficient amounts to (2.8 ± 0.8)·10⁻¹⁴ cm²/s. The integrated reflection intensity calculations for completely saturated sample suggest that only octahedral voids are filled under the conditions of experiment. The effect of complete saturation on the rotational subsystem of the C₆₀ fullerite is rather weak: the orientational phase transition shifts by 6 to 7 K to lower temperatures; no essential hysteresis is noticeable. The dopant shows reluctance to leave the sample under a vacuum of 10⁻³ Torr at room temperature.
The authors are grateful to P.V. Zinoviev for critical
 reading of the manuscript. This work was supported by
 the Ukrainian-Austrian grant M/140-2007.
en
Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
Физика низких температур
Динамика кристаллической решетки
Process of intercalation of C₆₀ with molecular hydrogen from XRD data
Article
published earlier
spellingShingle Process of intercalation of C₆₀ with molecular hydrogen from XRD data
Yagotintsev, K.A.
Stetsenko, Yu.E.
Legchenkova, I.V.
Prokhvatilov, A.I.
Strzhemechny, M.A.
Schafler, E.
Zehetbauer, M.
Динамика кристаллической решетки
title Process of intercalation of C₆₀ with molecular hydrogen from XRD data
title_full Process of intercalation of C₆₀ with molecular hydrogen from XRD data
title_fullStr Process of intercalation of C₆₀ with molecular hydrogen from XRD data
title_full_unstemmed Process of intercalation of C₆₀ with molecular hydrogen from XRD data
title_short Process of intercalation of C₆₀ with molecular hydrogen from XRD data
title_sort process of intercalation of c₆₀ with molecular hydrogen from xrd data
topic Динамика кристаллической решетки
topic_facet Динамика кристаллической решетки
url https://nasplib.isofts.kiev.ua/handle/123456789/117052
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