Show simple item record

dc.contributorMaterials Science and Engineering Laboratory, Ceramics Division National Institute of Standards and Technology, Gaithersburg, MD USAen_US
dc.contributor.authorBurton, Benjamin P.
dc.contributor.otherbenjamin.burton@nist.goven_US
dc.date.accessioned2013-04-03T17:37:00Z
dc.date.accessioned2014-08-05T19:24:46Z
dc.date.available2013-04-03T17:37:00Z
dc.date.available2014-08-05T19:24:46Z
dc.date.issued2013-04-03
dc.identifier.citationPhysics and Chemistry of Minerals (2003) 30: 88 - 97en_US
dc.identifier.urihttp://hdl.handle.net/11115/105
dc.description.abstractPlanewave pseudopotential calculations of supercell total energies were used as bases for first-principles calculations of the CaCO3–MgCO3 and CdCO3–MgCO3 phase diagrams. Calculated phase diagrams are in qualitative to semiquantitative agreement with experiment. Two unobserved phases, Cd3Mg (CO3)4 and CdMg3(CO3)4, are predicted. No new phases are predicted in the CaCO3–MgCO3 system, but a low-lying metastable Ca3Mg(CO3)4 state, analogous to the Cd3Mg(CO3)4 phase is predicted. All of the predicted lowest-lying metastable states, except for huntite CaMg3(CO3)4, have dolomite-related structures, i.e. they are layer structures in which A m B n cation layers lie perpendicular to the rhombohedral [111] vector.en_US
dc.description.sponsorshipNational Science Foundation DMR-0080766 and NISTen_US
dc.relation.urihttp://dx.doi.org/10.1007/s00269-002-0294-yen_US
dc.rightsAttribution-NonCommercial-ShareAlike 3.0 United States*
dc.rights.urihttp://creativecommons.org/licenses/by-nc-sa/3.0/us/*
dc.subjectCaCO3–MgCO3en_US
dc.titleCaCO3-MgCO3 CdCO3–MgCO Subsolidus phase diagramsen_US
dc.typeDataseten_US


Files in this item

Icon
Icon

This item appears in the following Collection(s)

Show simple item record

Attribution-NonCommercial-ShareAlike 3.0 United States
Except where otherwise noted, this item's license is described as Attribution-NonCommercial-ShareAlike 3.0 United States