Orientational glassification in fullerite C₆₀ saturated with H₂: photoluminescence studies
Using one-photon excitation we studied photoluminescence of C₆₀ saturated with molecular hydrogen over
 a temperature range 10 to 230 K. Saturation of samples was done at a pressure of 30 atm and at temperatures low
 enough (T < 250 °C) to exclude chemical sorption. The sample...
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| Опубліковано в: : | Физика низких температур |
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| Дата: | 2012 |
| Автори: | , , , , , |
| Формат: | Стаття |
| Мова: | Англійська |
| Опубліковано: |
Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
2012
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| Онлайн доступ: | https://nasplib.isofts.kiev.ua/handle/123456789/117426 |
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| Назва журналу: | Digital Library of Periodicals of National Academy of Sciences of Ukraine |
| Цитувати: | Orientational glassification in fullerite C₆₀ saturated with H₂: photoluminescence studies / P.V. Zinoviev, V.N. Zoryansky, N.B. Silaeva, Yu.E. Stetsenko, M.A. Strzhemechny,
 K.A. Yagotintsev // Физика низких температур. — 2012. — Т. 38, № 8. — С. 923-931. — Бібліогр.: 39 назв. — англ. |
Репозитарії
Digital Library of Periodicals of National Academy of Sciences of Ukraine| _version_ | 1862699296540852224 |
|---|---|
| author | Zinoviev, P.V. Zoryansky, V.N. Silaeva, N.B. Stetsenko, Yu.E. Strzhemechny, M.A. Yagotintsev, K.A. |
| author_facet | Zinoviev, P.V. Zoryansky, V.N. Silaeva, N.B. Stetsenko, Yu.E. Strzhemechny, M.A. Yagotintsev, K.A. |
| citation_txt | Orientational glassification in fullerite C₆₀ saturated with H₂: photoluminescence studies / P.V. Zinoviev, V.N. Zoryansky, N.B. Silaeva, Yu.E. Stetsenko, M.A. Strzhemechny,
 K.A. Yagotintsev // Физика низких температур. — 2012. — Т. 38, № 8. — С. 923-931. — Бібліогр.: 39 назв. — англ. |
| collection | DSpace DC |
| container_title | Физика низких температур |
| description | Using one-photon excitation we studied photoluminescence of C₆₀ saturated with molecular hydrogen over
a temperature range 10 to 230 K. Saturation of samples was done at a pressure of 30 atm and at temperatures low
enough (T < 250 °C) to exclude chemical sorption. The samples were saturated during periods of varied duration
τ to reach different occupancy levels. To check reliability of our luminescence results and interpretation, our
spectra for pure C₆₀ were compared with data known in the art, demonstrating good compatibility. The luminescence
spectra were attributed according to the approach of Akimoto and Kan,
no by separating total spectra in
two components of different origin. The A-type spectra, which are associated with exciton transport to deep
traps, above 70 K become prevail over the B-type emission. Until saturation times did not exceed a certain value
(for one, 50 h for a saturation temperature of 200 °C) the integrated intensity I as a function of the temperature T
of luminescence measurements, I(T), remained at a constant level up to the orientational vitrification point of
about 100 K and then went rather steeply down with increasing T. However, at longer τ the intensity I(Τ) persisted
in constancy to higher T (the higher, the longer τ) and then dropped with increasing T. This finding made
us to reexamine more closely the lattice parameter vs saturation time dependence for saturation temperatures 200
and 230 °C. As a result, additional evidence allowed us to infer that after completion of the single-molecule filling
of O-voids (specifically, after roughly 50 h for Tsat = 200 °C) a slower process of double filling sets in.
Double filling entails an anisotropic deformation of the octahedral cage, which modifies rotational dynamics
stronger than single filling. Further, we argue that singlet exciton transport to traps (which is responsible for the
A-type emission) can be crucially hampered by rotational jumps of one of the molecules over which a travelling
exciton is spread. Such jumps break coherence and the exciton stops thereby increasing the probability of emissionless
deactivation. If so, then the temperature, at which the rotational jumps occur sufficiently frequently, may
be by inference considered the unfreezing point for the orientational glass state (essentially coinciding with the
inverse critical point Tg where the rotational system freezes into the orientational glass). This treatment of Tg differs
from that existing in the art according to which the glass state is destroyed owing to the increased density of
phonon states. Keeping to our reasoning, we conclude that the orientational glass state does not disappear but,
instead, is conserved almost unchanged under one-molecule feeling and persists to appreciably higher temperatures
in the case of double filling, which affects exciton dynamics stronger.
|
| first_indexed | 2025-12-07T16:35:42Z |
| format | Article |
| fulltext | |
| id | nasplib_isofts_kiev_ua-123456789-117426 |
| institution | Digital Library of Periodicals of National Academy of Sciences of Ukraine |
| issn | 0132-6414 |
| language | English |
| last_indexed | 2025-12-07T16:35:42Z |
| publishDate | 2012 |
| publisher | Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України |
| record_format | dspace |
| spelling | Zinoviev, P.V. Zoryansky, V.N. Silaeva, N.B. Stetsenko, Yu.E. Strzhemechny, M.A. Yagotintsev, K.A. 2017-05-23T14:53:02Z 2017-05-23T14:53:02Z 2012 Orientational glassification in fullerite C₆₀ saturated with H₂: photoluminescence studies / P.V. Zinoviev, V.N. Zoryansky, N.B. Silaeva, Yu.E. Stetsenko, M.A. Strzhemechny,
 K.A. Yagotintsev // Физика низких температур. — 2012. — Т. 38, № 8. — С. 923-931. — Бібліогр.: 39 назв. — англ. 0132-6414 PACS: 81.05.ub, 78.55.–m, 61.43.–j, 78.55.Qr https://nasplib.isofts.kiev.ua/handle/123456789/117426 Using one-photon excitation we studied photoluminescence of C₆₀ saturated with molecular hydrogen over
 a temperature range 10 to 230 K. Saturation of samples was done at a pressure of 30 atm and at temperatures low
 enough (T < 250 °C) to exclude chemical sorption. The samples were saturated during periods of varied duration
 τ to reach different occupancy levels. To check reliability of our luminescence results and interpretation, our
 spectra for pure C₆₀ were compared with data known in the art, demonstrating good compatibility. The luminescence
 spectra were attributed according to the approach of Akimoto and Kan,
 no by separating total spectra in
 two components of different origin. The A-type spectra, which are associated with exciton transport to deep
 traps, above 70 K become prevail over the B-type emission. Until saturation times did not exceed a certain value
 (for one, 50 h for a saturation temperature of 200 °C) the integrated intensity I as a function of the temperature T
 of luminescence measurements, I(T), remained at a constant level up to the orientational vitrification point of
 about 100 K and then went rather steeply down with increasing T. However, at longer τ the intensity I(Τ) persisted
 in constancy to higher T (the higher, the longer τ) and then dropped with increasing T. This finding made
 us to reexamine more closely the lattice parameter vs saturation time dependence for saturation temperatures 200
 and 230 °C. As a result, additional evidence allowed us to infer that after completion of the single-molecule filling
 of O-voids (specifically, after roughly 50 h for Tsat = 200 °C) a slower process of double filling sets in.
 Double filling entails an anisotropic deformation of the octahedral cage, which modifies rotational dynamics
 stronger than single filling. Further, we argue that singlet exciton transport to traps (which is responsible for the
 A-type emission) can be crucially hampered by rotational jumps of one of the molecules over which a travelling
 exciton is spread. Such jumps break coherence and the exciton stops thereby increasing the probability of emissionless
 deactivation. If so, then the temperature, at which the rotational jumps occur sufficiently frequently, may
 be by inference considered the unfreezing point for the orientational glass state (essentially coinciding with the
 inverse critical point Tg where the rotational system freezes into the orientational glass). This treatment of Tg differs
 from that existing in the art according to which the glass state is destroyed owing to the increased density of
 phonon states. Keeping to our reasoning, we conclude that the orientational glass state does not disappear but,
 instead, is conserved almost unchanged under one-molecule feeling and persists to appreciably higher temperatures
 in the case of double filling, which affects exciton dynamics stronger. en Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України Физика низких температур Low Temperature Spectroscopy and Radiation Effects Orientational glassification in fullerite C₆₀ saturated with H₂: photoluminescence studies Article published earlier |
| spellingShingle | Orientational glassification in fullerite C₆₀ saturated with H₂: photoluminescence studies Zinoviev, P.V. Zoryansky, V.N. Silaeva, N.B. Stetsenko, Yu.E. Strzhemechny, M.A. Yagotintsev, K.A. Low Temperature Spectroscopy and Radiation Effects |
| title | Orientational glassification in fullerite C₆₀ saturated with H₂: photoluminescence studies |
| title_full | Orientational glassification in fullerite C₆₀ saturated with H₂: photoluminescence studies |
| title_fullStr | Orientational glassification in fullerite C₆₀ saturated with H₂: photoluminescence studies |
| title_full_unstemmed | Orientational glassification in fullerite C₆₀ saturated with H₂: photoluminescence studies |
| title_short | Orientational glassification in fullerite C₆₀ saturated with H₂: photoluminescence studies |
| title_sort | orientational glassification in fullerite c₆₀ saturated with h₂: photoluminescence studies |
| topic | Low Temperature Spectroscopy and Radiation Effects |
| topic_facet | Low Temperature Spectroscopy and Radiation Effects |
| url | https://nasplib.isofts.kiev.ua/handle/123456789/117426 |
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