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FeSiF6.6H2O above 240 K is described following the structural model previously proposed for MgSiF6.6H2O above 300 K: periodic antiphase built on the ordered monoclinic cell of the low-temperature form. In the present case a progressive ordering is observed and the antiphase boundaries are no longer planar but exhibit steps which lead to a mean boundary canted with respect to the c hexagonal axis (space group P3). Above 240 K a phase transformation occurs with a threefold twinning and a significant lattice deformation. The monoclinic cell (P21/c) is described.
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