On the polyamorphism of fullerite-based orientational glasses

A dilatometric investigation in the temperature range 2–28 K shows that a first-order polyamorphous transition occurs in the orientational glasses based on C 60 doped with H 2 , D 2 and Xe. A polyamorphous transition is also detected in C 60 doped with Kr and He. It is observed that the hysteresis o...

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Veröffentlicht in:Low temperature physics (Woodbury, N.Y.) N.Y.), 2005-05, Vol.31 (5), p.429-444
Hauptverfasser: Aleksandrovskii, A. N., Dolbin, A. V., Esel’son, V. B., Gavrilko, V. G., Manzhelii, V. G., Bakai, A. S., Cassidy, D., Gadd, G. E., Moricca, S., Sundqvist, B.
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Sprache:eng
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Zusammenfassung:A dilatometric investigation in the temperature range 2–28 K shows that a first-order polyamorphous transition occurs in the orientational glasses based on C 60 doped with H 2 , D 2 and Xe. A polyamorphous transition is also detected in C 60 doped with Kr and He. It is observed that the hysteresis of thermal expansion caused by the polyamorphous transition (and, hence, the transition temperature) is essentially dependent on the type of doping gas. Both positive and negative contributions to the thermal expansion are observed in the low-temperature phase of the glasses. The relaxation time of the negative contribution turns out to be much longer than that of the positive contribution. The positive contribution is found to be due to phonon and libron modes, while the negative contribution is attributed to tunneling states of the C 60 molecules. The characteristic time of the phase transformation from the low- T phase to the high- T phase is found for the C 60 – H 2 system at 12 K. A theoretical model is proposed to interpret these observed phenomena. The theoretical model proposed includes a consideration of the nature of polyamorphism in glasses, as well as the thermodynamics and kinetics of the transition. A model of noninteracting tunneling states is used to explain the negative contribution to the thermal expansion. The experimental data obtained are considered within the framework of the theoretical model. From the theoretical model the order of magnitude of the polyamorphous transition temperature is estimated. It is found that the late stage of the polyamorphous transformation is described well by the Kolmogorov law with an exponent of n=1. At this stage of the transformation, the two-dimensional phase boundary moves along the normal, and the nucleation is not important.
ISSN:1063-777X
1090-6517
DOI:10.1063/1.1925371