Evidence
from 900 MHz <sup>1</sup>H MAS NMR of Displacive Behavior of the Model
Order–Disorder Antiferroelectric
NH<sub>4</sub>H<sub>2</sub>AsO<sub>4</sub>
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Abstract
NH<sub>4</sub>H<sub>2</sub>AsO<sub>4</sub> (ADA) is a model compound for
understanding the mechanism of phase transitions in the KH<sub>2</sub>PO<sub>4</sub> (KDP) family of ferroelectrics. ADA exhibits a paraelectric
(PE) to antiferroelectric (AFE) phase transition at <i>T</i><sub>N</sub> ∼ 216 K whose mechanism remains unclear. With
the view of probing the role of the various protons in the transition
mechanism, we have employed the high-resolution technique of magic
angle spinning at the high Zeeman field of 21.1 T (<sup>1</sup>H resonance
at 900 MHz). We measured the temperature dependence of the isotropic
chemical shift and spin–lattice relaxation time, <i>T</i><sub>1</sub>, of the O–H···O and NH<sub>4</sub><sup>+</sup> protons through the <i>T</i><sub>N</sub>.
As <i>T</i> → <i>T</i><sub>N</sub>, NMR
peaks from the PE and AFE phases are seen to coexist over a temperature
range of about 3 K, showing formation of nearly static (lifetime >
milliseconds) pretransitional clusters in this lattice as it approaches
its <i>T</i><sub>N</sub>, consistent with the near first-order
nature of the phase transition. The isotropic chemical shift of the
O–H···O protons exhibited a steplike anomaly
at <i>T</i><sub>N</sub>, providing direct evidence of displacive
character in this lattice commonly thought of as an order–disorder
type. No such anomaly was noticeable for the NH<sub>4</sub><sup>+</sup> protons. Both sets of protons exhibited order–disorder characteristics
in their <i>T</i><sub>1</sub> data, as analyzed in terms
of the standard Bloembergen, Purcell, and Pound (BPP) model. These
data suggest that the traditionally employed classification of equilibrium
phase transitions into <i>order–disorder</i> and <i>displacive</i> ones, should rather be “<i>order–disorder
cum displacive</i>” type