The order-disorder ferrielectric-paraelectric transition in lamellar CuInP2
S6 is studied using P-31 solid-state MAS NMR spectroscopy. Spectra from a p
owder sample were recorded at various temperatures between 255 and 355 K wi
th a probe precalibrated for heating or cooling due to magic angle spinning
. Two center bands are observed at the lowest measured temperature while on
ly one is detected at the highest temperature. The former two represent the
inequivalent positions for the P atoms of the P2S6 group which reflect the
antiparallel displacements of the polar Cu-I and In-III sublattices in the
ferrielectric phase. The latter corresponds to the appearance of a 2-fold
axis through the P-P bond as the Cu-I ions undergo double-well hopping moti
ons, and the In-III ions occupy on-center sites in the paraelectric phase.
At intermediate temperatures, both ferrielectric and paraelectric type reso
nances contribute to the spectrum at ratios which are T-dependent, indicati
ng a transition temperature T-c = 312 +/- 1 K (310 +/- 1 K) for a warming (
cooling) cycle. The chemical shifts of the center bands characteristic of t
he ferrielectric phase are asymmetrically disposed with respect to that of
the paraelectric type signal and exhibit distinct thermal variations; the l
ine widths likewise evolve differently with temperature. Line-narrowing att
ributable to thermally enhanced motions is observed for the paraelectric ty
pe resonance upon warming across the transition. The temperature range for
the coexistence of the center bands representative of the two phases is unu
sually wide (approximate to 70 K), lying mostly below T-c. The presence of
the ferrielectric type resonance in the paraelectric regime may be ascribed
to the nucleation of polar order, while the persistence of the paraelectri
c signal well below T-c implies residual hopping motions occurring in the f
errielectric regime.