The phase stability, elastic behavior, and pressure-induced structural evolution of a natural metamorphic kalsilite (ideal formula KAISiO(4)) from Punalur (Kerala district in southern India), with P31 c symmetry and a K/Na molar ratio of similar to 350, has been investigated by in situ X-ray single-crystal diffraction up to similar to 7 GPa with a diamond-anvil cell under hydrostatic conditions. At high-pressure, a previously unreported iso-symmetric first-order phase transition occurs at similar to 3.5 GPa. The volume compression of the two phases is described by third-order Birch-Murnaghan equations-of-state: V-o = 201.02(1) angstrom(3), K-To = 59.7(5) GPa, K' = 3.5(3) for the low-P polymorph, and V-o = 200.1(13) angstrom(3), K-To = 44(8) GPa, K' = 6.4(20) for the high-P polymorph. The pressure-induced structural evolution in kalsilite up to 7 GPa appears to be completely reversible. The compression of both phases involves tetrahedral rotations around [0001], which close up the channels within the framework. In addition, compression of the low-pressure phase involves tilting of the tetrahedra. The major structural change at the phase transition is an increase in the tilting of the tetrahedra, but with a reversion of the tetrahedral rotations to the value found at ambient conditions. This behavior is in distinct contrast to that of nepheline, which has a tetrahedral framework of the same topology.
Phase stability, elastic behavior, and pressure-induced structural evolution of kalsilite: A ceramic material and high-T/high-P mineral
Angel Ross J;
2011
Abstract
The phase stability, elastic behavior, and pressure-induced structural evolution of a natural metamorphic kalsilite (ideal formula KAISiO(4)) from Punalur (Kerala district in southern India), with P31 c symmetry and a K/Na molar ratio of similar to 350, has been investigated by in situ X-ray single-crystal diffraction up to similar to 7 GPa with a diamond-anvil cell under hydrostatic conditions. At high-pressure, a previously unreported iso-symmetric first-order phase transition occurs at similar to 3.5 GPa. The volume compression of the two phases is described by third-order Birch-Murnaghan equations-of-state: V-o = 201.02(1) angstrom(3), K-To = 59.7(5) GPa, K' = 3.5(3) for the low-P polymorph, and V-o = 200.1(13) angstrom(3), K-To = 44(8) GPa, K' = 6.4(20) for the high-P polymorph. The pressure-induced structural evolution in kalsilite up to 7 GPa appears to be completely reversible. The compression of both phases involves tetrahedral rotations around [0001], which close up the channels within the framework. In addition, compression of the low-pressure phase involves tilting of the tetrahedra. The major structural change at the phase transition is an increase in the tilting of the tetrahedra, but with a reversion of the tetrahedral rotations to the value found at ambient conditions. This behavior is in distinct contrast to that of nepheline, which has a tetrahedral framework of the same topology.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.