2007
DOI: 10.1002/chem.200700056
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Alkaline Earth Chloride Hydrates: Chlorine Quadrupolar and Chemical Shift Tensors by Solid‐State NMR Spectroscopy and Plane Wave Pseudopotential Calculations

Abstract: A series of alkaline earth chloride hydrates has been studied by solid-state (35/37)Cl NMR spectroscopy in order to characterize the chlorine electric field gradient (EFG) and chemical shift (CS) tensors and to relate these observables to the structure around the chloride ions. Chlorine-35/37 NMR spectra of solid powdered samples of pseudopolymorphs (hydrates) of magnesium chloride (MgCl(2).6H(2)O), calcium chloride (CaCl(2).2H(2)O), strontium chloride (SrCl(2), SrCl(2).2H(2)O, and SrCl(2).6H(2)O), and barium … Show more

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Cited by 59 publications
(130 citation statements)
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References 66 publications
(134 reference statements)
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“…As evident from this figure, 1D experiments at 24 T result in excellent experimental powder lineshapes that fit extremely well with the simulated lineshape, which highlights the importance of the use of such ultra-high field. 19,22-24 a substantial disagreement is observed for the L-histidine·HCl·H2O. This should be attributed to the different crystalline form of L-histidine·HCl·H2O used here (purchased from Kanto Kagaku, Japan, and used without further purification) with respect to that reported earlier.…”
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confidence: 69%
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“…As evident from this figure, 1D experiments at 24 T result in excellent experimental powder lineshapes that fit extremely well with the simulated lineshape, which highlights the importance of the use of such ultra-high field. 19,22-24 a substantial disagreement is observed for the L-histidine·HCl·H2O. This should be attributed to the different crystalline form of L-histidine·HCl·H2O used here (purchased from Kanto Kagaku, Japan, and used without further purification) with respect to that reported earlier.…”
mentioning
confidence: 69%
“…Therefore, the quadrupolar and isotropic chemical shift (δiso) parameters were easily extracted from the spectrum observed at 24 T with a SIMPSON simulation: (χQ, η, δiso) = (4.26 MHz, 0.75, 110 ppm) despite these parameters hardly to obtain from that at 14.1 T. These parameters agree well with the previously reported values. 19,20 The distortions in the lineshape observed at 14.1 T are mainly due to the combined effect of the broad lineshape and the dead time in NMR measurements. The first few sampling points of the FID were found to be absent in the NMR experiments during the dead time due to some technical difficulty in observing the signal just after the rf pulses.…”
Section: Resultsmentioning
confidence: 99%
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