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American Mineralogist; November 2005; v. 90; no. 11-12; p. 1835-1839; DOI: 10.2138/am.2005.1783
© 2005 Mineralogical Society of America
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The stability and Raman spectra of ikaite, CaCO3·6H2O, at high pressure and temperature

Anat Shahar1,2,*, William A. Bassett1,{dagger}, Ho-kwang Mao2, I-Ming Chou3 and Wendy Mao2

1 Department of Earth and Atmospheric Sciences, Cornell University, Ithaca, New York 14853, U.S.A
2 Geophysical Laboratory, Carnegie Institution of Washington, Washington D.C. 20015, U.S.A.
3 954 National Center, United States Geological Survey, Reston, Virginia 20192, U.S.A.

Correspondence: {dagger} E-mail: bassett{at}geology.geo.cornell.edu

Raman analyses of single crystals of ikaite, CaCO3·6H2O, synthesized in a diamond-anvil cell at ambient temperature yield spectra from 0.14 to 4.08 GPa; the most intense peaks are at 228 and 1081 cm–1 corresponding to Eg (external) and A1g (internal) modes of vibrations in CO2– 3 ions, respectively. These are in good agreement with Raman spectra previously published for ikaite in powder form at ambient temperature and pressure. Visual observations of a sample consisting initially of a mixture of calcite + water in a hydrothermal diamond-anvil cell yielded a P-T phase diagram up to 2 GPa and 120 °C; the boundary for the reaction ikaite {leftrightarrow} aragonite + water has a positive slope and is curved convexly toward the aragonite + water field similar to typical melt curves. This curvature can be explained in terms of the Clapeyron equation for a boundary between a solid phase and a more compressible liquid phase or largely liquid phase assemblage.







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