Er. Losilla et al., UNDERSTANDING NA MOBILITY IN NASICON MATERIALS - A RIETVELD, NA-23 AND P-31 MAS NMR, AND IMPEDANCE STUDY, Chemistry of materials, 10(2), 1998, pp. 665-673
The structures and electrical properties of four NASICON compositions,
Na1.4M1.6In0.4(PO4)(3) (M = Ti, Sn, I-If Zr), have been determined an
d compared. Rietveld refinement of powder X-ray diffraction data confi
rmed the basic rhombohedral NASICON structure with random occupancy of
the octahedral In/M sites, full occupancy of the Na(1) sites and part
ial occupancy of the Na(2) sites. For three compositions, M = Zr, Sn,
and Hf, the P-31 MAS NMR peak intensities of the four detected signals
, attributed to four different phosphorus environments [P(OM)(4-n)(OIn
)(n) (n = 0-3)], were close to the ratios expected for a random distri
bution of In/M. For M = Ti, some departures from statistical occupancy
were apparent. Na-23 MAS NMR data gave evidence for two Na+ positions
at room temperature for M = Ti, Sn, attributable to occupation of Na(
1) and Na(2) sites. For M = Hf, Zr, only a single signal could be reso
lved at room temperature, which splits into two signals on cooling to
-50 degrees C, indicating high Na mobility at room temperature. Impeda
nce data obtained on pressed sintered pellets over the range 25-300 de
grees C showed that bulk ionic conductivities increased and activation
energies decreased in the sequence Ti, Sn, Hf, Zr. The geometry of th
e M1M2 bottleneck has been determined from structural data, and a dire
ct correlation found between activation energy for ion conduction and
the bottleneck size.