Samples of fullerene CsO submitted previously to temperatures and pressures up to 973 K and 9.5 GPa have been heated in a differential scanning calorimeter in the interval 220-725 K. In nearly all of them, the first heating showed an irreversible endothermic peak extending between 450 and 550 K whic
Structural studies of C60 transformed by temperature and pressure treatments
✍ Scribed by V.A. Davydov; L.S. Kashevarova; A.V. Rakhmanina; V. Agafonov; R. Céolin; H. Szwarc
- Publisher
- Elsevier Science
- Year
- 1997
- Tongue
- English
- Weight
- 868 KB
- Volume
- 35
- Category
- Article
- ISSN
- 0008-6223
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✦ Synopsis
Raman spectroscopy,
X-ray and electron diffractions have been applied to study samples of fullerene C,, after they have undergone pressure and temperature treatments up to 8 GPa and 1073 K. It is confirmed that mixtures of rhombohedral and tetragonal structures are formed in the 2-4 GPa and 673-1073 K pressure-temperature domain. Traces of a hexagonal phase are also observed in the same range. Only the rhombohedral one is obtained in the 4-8 GPa range in the same temperature interval. The material obtained at temperatures between 473 and 673 K in the whole pressure range which has previously been described in terms of a cubic structure can be understood in terms of an orthorhombic one. It may also contain mixtures of different phases including a cubic one and even a cubic superstructure. The widened poorly resolved X-ray profiles indicate the existence of disorder within the materials formed and the increasing complexity of Raman spectra as temperature increases at fixed pressures (from 2 to 8 GPa) suggests that this disorder is related to phase mixtures in almost all samples. A rhombohedral sample formed at 6 GPa-873 K reverted to a mixture of rhombohedral and tetragonal phases at 2.5 GPa-873 K. Thus thermodynamic equilibrium between these two kinds of systems could exist.
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Vibrational Raman studies on Cse up to 18.0 GPa and between 4 and 360 K are presented. No significant changes are observed up to IO GPa; mode-Grthteisen parameters are calculated. The low pressure, temperature-dependent Raman spectrum shows a sharp shift in peak position and width at 240 K. This is