The density and structure of MgSiO(3) glass (v-En) recovered from a series of annealing experiments up to 1000 degrees C at 2.0, 5.5 and 8.5 GPa have been investigated using Archimedes' method and Raman spectroscopy, respectively. The densities of recovered glasses are found to be a complex function of pressure and temperature. At room temperature, compression up to 8.5 GPa, followed by decompression, yields a glass with a density within 0.6 % of the 1-atm value. Likewise, the 1-atm density is fully recovered in glass heated up to similar to 500 degrees C at 2.0 GPa at higher pressures. A sharp increase in recovered density is observed between 500 degrees C and 800 degrees C at 2.0 GPa, 200 degrees C and 500 degrees C at 5.5 GPa and from room-T and 300 degrees C at 8.5 GPa. At higher annealing temperatures the changes in density are more modest. This break in slope occurs for a glass density of 2.89 g/cm(3) at 2.0 GPa and 2.95 g/cm(3) at 5.5 and 8.5 GPa. Above similar to 900 degrees C v-En crystallizes at all pressures. Raman spectra for annealed glasses show a progressive shift in the Si-O-Si bending mode to higher wave number with recovered density. From these data we estimate a similar to 4.5 % decrease in the Si-O-Si bond angle with densification from 2.75 g/cm(3) (1-atm, room T) to 3.0 g/cm(3).
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Department of Physics, University of Bath, BathDepartment of Physics, University of Bath, Bath
Salmon P.S.
Moody G.S.
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Department of Physics, University of Bath, BathDepartment of Physics, University of Bath, Bath
Moody G.S.
Ishii Y.
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Division of Chemical Engineering, Graduate School of Engineering Science, Osaka University, 1-3 Machikaneyama-cho, Toyonaka, OsakaDepartment of Physics, University of Bath, Bath
Ishii Y.
Pizzey K.J.
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Department of Physics, University of Bath, BathDepartment of Physics, University of Bath, Bath
Pizzey K.J.
Polidori A.
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Department of Physics, University of Bath, Bath
Institut Laue Langevin, 71 Avenue des Martyrs, Grenoble Cedex 9Department of Physics, University of Bath, Bath
Polidori A.
Salanne M.
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Sorbonne Université, CNRS, Physico-Chimie des Électrolytes et Nanosystèmes Interfaciaux, ParisDepartment of Physics, University of Bath, Bath
Salanne M.
Zeidler A.
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Department of Physics, University of Bath, BathDepartment of Physics, University of Bath, Bath
Zeidler A.
Buscemi M.
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Department of Physics, University of Bath, BathDepartment of Physics, University of Bath, Bath
Buscemi M.
Fischer H.E.
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Institut Laue Langevin, 71 Avenue des Martyrs, Grenoble Cedex 9Department of Physics, University of Bath, Bath
Fischer H.E.
Bull C.L.
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ISIS Facility, Rutherford Appleton Laboratory, Chilton, Didcot, OX11 0QX, OxonDepartment of Physics, University of Bath, Bath
Bull C.L.
Klotz S.
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Sorbonne Université, UMR 7590, IMPMC, ParisDepartment of Physics, University of Bath, Bath
Klotz S.
Weber R.
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Advanced Photon Source, Argonne National Laboratory, 9700 South Cass Avenue, Argonne, 60439, IL
Materials Development, Inc., Arlington Heights, 60004, ILDepartment of Physics, University of Bath, Bath
Weber R.
Benmore C.J.
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Advanced Photon Source, Argonne National Laboratory, 9700 South Cass Avenue, Argonne, 60439, ILDepartment of Physics, University of Bath, Bath
Benmore C.J.
MacLeod S.G.
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AWE, Aldermaston, RG7 4PR, ReadingDepartment of Physics, University of Bath, Bath