To better understand lattice disorder in hydrozincite, natural hydrozincite samples and synthetic analogues were investigated by XRD, FTIR, 13C MAS, and 13C CPMAS NMR. The size of coherent diffraction domains ranges between ~10 nm (Synth1) and ~30 nm (Synth2). FTIR peaks from the antisymmetric CO32– stretching n3 mode were observed at 1383 and 1515 cm–1 in all samples. Peaks due to OH vibrations were observed for all the samples at 3234, 3303, and 3363 cm–1, and were sharp only for the samples having larger crystal domains. The 13C MAS and CPMAS NMR spectra showed a main carbon signal at 164 ppm in the Synth2 sample, while two main signals were observed at ~164 and ~168 ppm in the Synth1 sample. The intensity ratio of the latter signals were found to be independent of contact time, in the investigated range between 0.2 and 30 ms. In addition, 13C CPMAS dynamics indicates that the Synth1 sample has shorter T1r with respect to Synth2. This indicates a more effective process of spin diffusion of proton magnetization in the former due to different structural properties of Synth1 and Synth2 samples. In addition, chemical shift anisotropy analysis was attributed to a structural change in the carbonate group or hydrogen bonding for Synth1 and Synth2. This was interpreted as a deviation from the ideal structure generated by linear and planar lattice defects and/or grain boundaries

Investigation of the hydrozincite structure by infrared and solid-state NMR spectroscopy

SANNA, ROBERTA;DE GIUDICI, GIOVANNI BATTISTA;SCORCIAPINO, MARIANO ANDREA;FLORIS, COSTANTINO;CASU, MARIANO
2013-01-01

Abstract

To better understand lattice disorder in hydrozincite, natural hydrozincite samples and synthetic analogues were investigated by XRD, FTIR, 13C MAS, and 13C CPMAS NMR. The size of coherent diffraction domains ranges between ~10 nm (Synth1) and ~30 nm (Synth2). FTIR peaks from the antisymmetric CO32– stretching n3 mode were observed at 1383 and 1515 cm–1 in all samples. Peaks due to OH vibrations were observed for all the samples at 3234, 3303, and 3363 cm–1, and were sharp only for the samples having larger crystal domains. The 13C MAS and CPMAS NMR spectra showed a main carbon signal at 164 ppm in the Synth2 sample, while two main signals were observed at ~164 and ~168 ppm in the Synth1 sample. The intensity ratio of the latter signals were found to be independent of contact time, in the investigated range between 0.2 and 30 ms. In addition, 13C CPMAS dynamics indicates that the Synth1 sample has shorter T1r with respect to Synth2. This indicates a more effective process of spin diffusion of proton magnetization in the former due to different structural properties of Synth1 and Synth2 samples. In addition, chemical shift anisotropy analysis was attributed to a structural change in the carbonate group or hydrogen bonding for Synth1 and Synth2. This was interpreted as a deviation from the ideal structure generated by linear and planar lattice defects and/or grain boundaries
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11584/98126
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