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Structure and microhardness of low pressure polymerized fulleriteC60

 

作者: A. P. Isakina,   S. V. Lubenets,   V. D. Natsik,   A. I. Prokhvatilov,   M. A. Strzhemechny,   L. S. Fomenko,   N. A. Aksenova,   A. V. Soldatov,  

 

期刊: Low Temperature Physics  (AIP Available online 1998)
卷期: Volume 24, issue 12  

页码: 896-903

 

ISSN:1063-777X

 

年代: 1998

 

DOI:10.1063/1.593524

 

出版商: AIP

 

数据来源: AIP

 

摘要:

We have carried out low-temperature x-ray diffraction studies onC60fullerite polymerized by low quasi-hydrostatic pressure of 1.1 GPa atT=563 K.It is established that at room temperature in freshly prepared samples three phases mainly coexist, viz. a compressed cubic phase with the lattice parametera=13.94 Å,an orthorhombicO′phase with the lattice parametersa=9.12 Å,b=9.82 Å,c=14.60 Å,and a rhombohedral phase of symmetryR3mwith the parametersa=9.20 Åandc=24.27 Å.Mechanical grinding or annealing at 573 K entails depolymerization of sintered samples and restoration of the fcc structure of pristineC60.During annealing in air, intercalation of fullerite lattice by oxygen molecules occurs as well as a substantial amount of some new phase is formed, most probably with tetragonal symmetry, the chemical composition and structure of which have not been determined. The microhardness of polymerizedC60is higher than that of single crystal samples roughly four-fold at room temperature and by a factor of 2.6 at liquid nitrogen temperature. Analysis shows that polymerization and grain boundaries give contributions to the microhardness of sintered samples but we did not succeed in separating these two contributions. The temperature dependence of the microhardness of polymerized samples exhibits a jump in the vicinity of 260 K, where pristineC60fullerite undergoes the fcc-sc phase transition. We think that this jump is due to a partial destruction of the polymerized state under indentor as a result of shear straining in inhomogeneous stress fields. Annealing of polymerizedC60at a temperature of 573 K, which restores the fcc phase, leads to a considerable decrease in microhardness, the hardness “jump” near the fcc-sc transition extends in temperature and shifts to lower temperatures. ©1998 American Institute of Physics.

 

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