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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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
Series:Физика низких температур
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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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spelling oai:nasplib.isofts.kiev.ua:123456789-1170522025-02-23T17:37:04Z 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 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. 2009 Article 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 en Физика низких температур application/pdf Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
collection DSpace DC
language English
topic Динамика кристаллической решетки
Динамика кристаллической решетки
spellingShingle Динамика кристаллической решетки
Динамика кристаллической решетки
Yagotintsev, K.A.
Stetsenko, Yu.E.
Legchenkova, I.V.
Prokhvatilov, A.I.
Strzhemechny, M.A.
Schafler, E.
Zehetbauer, M.
Process of intercalation of C₆₀ with molecular hydrogen from XRD data
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.
format Article
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.
author_sort Yagotintsev, K.A.
title 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_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_sort process of intercalation of c₆₀ with molecular hydrogen from xrd data
publisher Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
publishDate 2009
topic_facet Динамика кристаллической решетки
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.
series Физика низких температур
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