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dc.contributor.authorKennedy, Catherine A.en_US
dc.contributor.authorWhite, Mary Anneen_US
dc.contributor.authorWilkinson, Angus P.en_US
dc.contributor.authorVarga, Tamasen_US
dc.date.accessioned2013-08-23T15:58:40Z
dc.date.available2013-08-23T15:58:40Z
dc.date.issued2007-06en_US
dc.identifier.citationKennedy, Catherine A., Mary Anne White, Angus P. Wilkinson, and Tamas Varga. 2007. "Heat capacity, lattice dynamics, and thermodynamic stability of the negative thermal expansion material HfMo2O8." Physical Review B 75(22): 224302-224302. Copyright © 2007 American Physical Society.en_US
dc.identifier.issn1098-0121en_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevB.75.224302en_US
dc.identifier.urihttp://hdl.handle.net/10222/36166
dc.description.abstractWe explore the lattice dynamics of the negative thermal expansion material, cubic HfMo2O8, through analysis of its heat capacity (measured from 0.5 to 300 K) and its room-temperature Raman spectrum. Its heat capacity is quantitatively very similar to that of ZrW2O8, as is its Raman spectrum. The heat capacity of HfMo2O8 can be well represented by the present lattice dynamical assignment and by C-P(HfW2O8)-C-P(ZrW2O8)+C-P(ZrMo2O8), but not by C-P(HfO2)+2C(P)(MoO3), likely because the AB(2)O(8) compounds have low-frequency optic modes, not present in HfO2 and MoO3. The present thermodynamic data also allow an analysis of the thermodynamic stability of cubic HfMo2O8, and it is shown to be unstable with respect to MoO3 and HfO2 at room temperature.en_US
dc.relation.ispartofPhysical Review Ben_US
dc.titleHeat capacity, lattice dynamics, and thermodynamic stability of the negative thermal expansion material HfMo2O8en_US
dc.typearticleen_US
dc.identifier.volume75en_US
dc.identifier.issue22en_US
dc.identifier.startpage224302en_US
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