Abstract
The crystal structure of clinoatacamite, ideally Cu2(OH)3Cl, has been studied using single-crystal X-ray diffraction and Raman scattering at variable temperature between 150 and 490 K in natural samples with different degrees of Co and Ni substitution. The monoclinic clinoatacamite crystal structure is closely related to the trigonal crystal structures of herbertsmithite, Cu3Zn(OH)6Cl2, and paratacamite, Cu3(Cu, Zn)(OH)6Cl2. Disappearance of clinoatacamite superstructure reflections close to a temperature of 400 K indicates the transition to a trigonal herbertsmithite-type phase in all crystals containing Co and Ni impurities. In these crystals, which are invariably twinned at room temperature, an intermediate phase is observed in the temperature range 360–400 K, which has the trigonal paratacamite crystal structure. Untwinned end-member clinoatacamite directly transforms to the herbertsmithite-type at T c = 445 K. Probability density functions of the oxygen and copper atoms as well as details from the Raman scattering measurements indicate that the interlayer Cu-coordination environment remains locally Jahn–Teller-distorted in the trigonal crystal structures with space group symmetries \(R\overline{3}\) and \(R\overline{3} m\) and that the transition from monoclinic to trigonal symmetry is driven by the dynamic Jahn–Teller effect.
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Acknowledgements
The authors would like to thank Stefanie Heidrich and Peter Stutz for conducting the electron microprobe analysis and related sample preparation in Hamburg. M.D.W. would like to thank Dr. Marcus Origlieri (University of Arizona) for donating the exceptional clinoatacamite sample from the Lily Mine, Peru, for crystallographic study. The clinoatacamite sample from Chile was kindly provided by Mineralogisches Museum, CeNak, Universität Hamburg. Useful comments by Herta Effenberger and Luca Bindi helped to improve the manuscript.
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Crystal structure data (cif-format) with harmonic displacement factors for all temperatures and compositions given in Table 2, with anharmonic displacement factors for sample c2 at 435 K and with harmonic and anharmonic displacements for sample c0 at 490 K. Room-temperature crystal structure data for sample c1 and c3. Below is the link to the electronic supplementary material.
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Malcherek, T., Mihailova, B. & Welch, M.D. Structural phase transitions of clinoatacamite and the dynamic Jahn–Teller effect. Phys Chem Minerals 44, 307–321 (2017). https://doi.org/10.1007/s00269-016-0859-9
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DOI: https://doi.org/10.1007/s00269-016-0859-9