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American Mineralogist; February 2002; v. 87; no. 2-3; p. 302-306
© 2002 Mineralogical Society of America
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The crystal structure and cation ordering of Phase-X-(K1–x–n)2(Mg1–n[Al,Cr]n)2Si2O7H2x: A potential K- and H-bearing phase in the mantle*

Franco Mancini1,{dagger}, George E. Harlow1 and Christopher Cahill2

1 Department of Earth and Planetary Sciences, American Museum of Natural History, Central Park West at 79th Street, New York, New York 10024-5192, U.S.A.
2 Department of Chemistry, George Washington University, 725 21st Street, N.W. Washington, D.C. 20052, U.S.A.

Correspondence: {dagger} E-mail: mancini{at}amnh.org

Phase-X, a potassium di-magnesium acid disilicate, is a high-pressure synthetic compound—a potential K-bearing silicate in the mantle—with space group P63cm (no. 185), a = b = 5.028(2) Å, c = 13.216(3) Å, V = 289.34 Å3, Z = 2. The structure has been determined with 1521 CCD measured intensities and refined by the least-square method to R = 0.0187. The structure is built up of octahedral MgO sheets and layers containing disilicate groups, Si2O7, (with distinct Si1 and Si2 tetrahedra linked by the apical O2 atom) alternating along the c axis. The octahedral sheet is based on a hexagonal closest-packed array of two layers of non-equivalent O atoms, O1 and O3; two-thirds of all edge-sharing M octahedra are filled. Within the framework of the Si2O7 groups are channel structures parallel to [100], [010], and [110] that contain K atoms disordered in the middle of a large trigonal cavity (the A site). The FTIR spectrum in the OH stretching region shows a sharp peak at 3602 cm–1 due to OH ordered in one anion site; the position of hydrogen, which operates in a charge-balancing substitution for the partial occupancy of the A site (K1–x{square}x)A {leftrightarrow} Hx{square}1–x)H, is undetermined. Densification in phase-X is affected by the greater compression of the empty octahedra in the octahedral layer and by constraining the trigonal A cavity containing the K atom to the size of the Si2O7 disilicate group. This dense packing contributes to the relatively high zero-pressure calculated density of 3.38 g/cm3.




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