Understanding the Conduction Mechanism of the Protonic
Conductor CsH<sub>2</sub>PO<sub>4</sub> by Solid-State NMR Spectroscopy
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Abstract
Local dynamics and hydrogen bonding
in CsH<sub>2</sub>PO<sub>4</sub> have been investigated by <sup>1</sup>H, <sup>2</sup>H, and <sup>31</sup>P solid-state NMR spectroscopy
to help provide a detailed
understanding of proton conduction in the paraelectric phase. Two
distinct environments are observed by <sup>1</sup>H and <sup>2</sup>H NMR, and their chemical shifts (<sup>1</sup>H) and quadrupolar
coupling constants (<sup>2</sup>H) are consistent with one strong
and one slightly weaker H-bonding environment. Two different protonic
motions are detected by variable-temperature <sup>1</sup>H MAS NMR
and <i>T</i><sub>1</sub> spin–lattice relaxation
time measurements in the paraelectric phase, which we assign to librational
and long-range translational motions. An activation energy of 0.70
± 0.07 eV is extracted for the latter motion; that of the librational
motion is much lower. <sup>31</sup>P NMR line shapes are measured
under MAS and static conditions, and spin–lattice relaxation
time measurements have been performed as a function of temperature.
Although the <sup>31</sup>P line shape is sensitive to the protonic
motion, the reorientation of the phosphate ions does not lead to a
significant change in the <sup>31</sup>P CSA tensor. Rapid protonic
motion and rotation of the phosphate ions is seen in the superprotonic
phase, as probed by the <i>T</i><sub>1</sub> measurements
along with considerable line narrowing of both the <sup>1</sup>H and
the <sup>31</sup>P NMR signals