Mc. Foster et al., BA6CONB9O30 AND BA6FENB9O30 - 2 NEW TUNGSTEN-BRONZE-TYPE FERROELECTRICS - CENTROSYMMETRY OF BA5.2K0.8U2.4NB7.6O30 AT 300 K, Journal of applied crystallography, 30, 1997, pp. 495-501
Ba6CoNb9O30 and Ba6FeNb9O30 in space group P4bm are shown to satisfy t
he structural criteria for ferroelectricity. Ba6CoNb9O30 undergoes a d
iffuse phase transition at 660 (11) K, as observed calorimetrically, i
n addition to a dielectric permittivity anomaly with an onset temperat
ure of 685 (10) K. The demonstration of dielectric hysteresis at room
temperature under the application of a varied DC field reaching a maxi
mum of +/- 300 kV m(-1), correspondign to a spontaneous polarization o
f 1.2(5) x 10(-2)C m(-2), provides unambiguous Verification that it is
a new ferroelectric. Ba6FeNb9O30 also undergoes a diffuse phase trans
ition at 605(16)K, with a dielectric anomaly at 583(5)K, and exhibits
dielectric hysteresis at room temperature under a varied DC field rang
ing to +/-310 kV m(-1) corresponding to a spontaneous polarization of
2.2(5) x 10(-2) C m(-2); it too is demonstrably a new ferroelectric. A
lthough Ba5.2K0.8U2.4Nb7.6O30 has also been reported in space group P4
bm, all atomic displacements from the corresponding centrosymmetric po
sitions are less than their refined root-mean-square thermal or static
amplitudes. Such an arrangement is likely to be thermodynamically uns
table. Either its space group has been incorrectly assigned, and reinv
estigation will show the space group is P4/mbm, or the structural refi
nement is incomplete.