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Graphitization of Glassy Carbon after Compression at Room Temperature.
Shiell, T B; McCulloch, D G; McKenzie, D R; Field, M R; Haberl, B; Boehler, R; Cook, B A; de Tomas, C; Suarez-Martinez, I; Marks, N A; Bradby, J E.
Affiliation
  • Shiell TB; Department of Electronic Materials Engineering, Research School of Physics and Engineering, The Australian National University, Canberra, Australian Capital Territory 2601, Australia.
  • McCulloch DG; Physics, School of Science, RMIT University, Melbourne, Victoria 3001, Australia.
  • McKenzie DR; RMIT Microscopy and Microanalysis Facility, RMIT University, Melbourne, Victoria 3001, Australia.
  • Field MR; School of Physics, The University of Sydney, New South Wales 2006, Australia.
  • Haberl B; RMIT Microscopy and Microanalysis Facility, RMIT University, Melbourne, Victoria 3001, Australia.
  • Boehler R; Neutron Scattering Division, Neutron Science Directorate, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA.
  • Cook BA; Neutron Scattering Division, Neutron Science Directorate, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA.
  • de Tomas C; Geophysical Laboratory, Carnegie Institution of Washington, 5251 Branch Road, Northwest Washington, D.C. 20015, USA.
  • Suarez-Martinez I; Physics, School of Science, RMIT University, Melbourne, Victoria 3001, Australia.
  • Marks NA; Department of Physics and Astronomy, Curtin University, Perth, Western Australia 6845, Australia.
  • Bradby JE; Department of Physics and Astronomy, Curtin University, Perth, Western Australia 6845, Australia.
Phys Rev Lett ; 120(21): 215701, 2018 May 25.
Article in En | MEDLINE | ID: mdl-29883140
Glassy carbon is a technologically important material with isotropic properties that is nongraphitizing up to ∼3000 °C and displays complete or "superelastic" recovery from large compression. The pressure limit of these properties is not yet known. Here we use experiments and modeling to show permanent densification, and preferred orientation occurs in glassy carbon loaded to 45 GPa and above, where 45 GPa represents the limit to the superelastic and nongraphitizing properties of the material. The changes are explained by a transformation from its sp^{2} rich starting structure to a sp^{3} rich phase that reverts to fully sp^{2} bonded oriented graphite during pressure release.

Full text: 1 Database: MEDLINE Language: En Journal: Phys Rev Lett Year: 2018 Type: Article Affiliation country: Australia

Full text: 1 Database: MEDLINE Language: En Journal: Phys Rev Lett Year: 2018 Type: Article Affiliation country: Australia