DEHYDRATION BEHAVIOR OF KAňKITE AND THE CRYSTAL STRUCTURE OF THE DEHYDRATED KAňKITE
Kaňkite forms masses of minute (< 2 mm) platy crystals intergrown with each other and standard methods (e.g., single-crystal X-ray diffraction, XRD) were deemed inadequate for this problem. Crystal structure was solved by precession electron diffraction in a transmission electron microscope (TEM). The data were processed to yield the unit cell parameters and integrated reflection intensities. The structure was solved in the space group Cc with lattice parameters a = 5.6825 Å, b = 21.0912 Å, c= 9.119 Å, and b = 92.793°. The structure consists of corrugated heteropolyhedral layers in which arsenate tetrahedra attach to Fe-centered octahedra.
Surprisingly, this structural model failed to describe the synchrotron powder XRD data collected on the same kaňkite sample. After some ruminations, we arrived at a hypothesis that the solved structure belongs to a dehydration product of kaňkite because the TEM work is carried out in high vacuum. A series of in-house, powder XRD heating experiments confirmed this suspicion. Upon heating, kaňkite breaks down to its dehydration product at approximately 50 °C. The high-temperature phase possesses indeed the structure solved by precession electron diffraction and persists up to ~170 °C.
We assume that the crystal structure of kaňkite is closely related to that of its dehydration product but remains unknown. The reason for this assumption is a similar topology of the corrugated layers in the dehydrated kaňkite and lausenite [Fe2(SO4)3×5H2O], noting that lausenite reversibly hydrates to kornelite [Fe2(SO4)3×7.5H2O]. The structure of kornelite also consists of sheets, not as corrugated as in lausenite. It is possible that the structure of kaňkite could be captured by considering this analogy; we were not able to do so until now.