Li0.4K0.6NbO3 (LKN) belongs to the completely filled tungsten bronze-t
ype ferroelectrics and undergoes a diffuse phase transition at around
420 degrees C. LKN has two thermal hystereses in the heating and cooli
ng cycles, above and below the transition point. Hysteresis above T-C
is wider than the one below T-C and the width of the hysteresis decrea
ses as frequency increases. The Curie range of Li0.4K0.6NbO3 is wider
than that of Pb(Mg1/3Nb2/3)O-3 (PMN) and (Sr,Ba)Nb2O6 (SBN) and it imp
lies that Li0.4K0.6NbO3 needs a wider temperature range to reach an eq
uilibrium phase than PMN and SBN. In pyroelectric measurements using t
he current method, P-s = 20 mu C/cm(2) in the ferroelectric phase, and
the temperature of the pyroelectric current maximum is by 108 K highe
r than that of the dielectric constant maxima. Dielectric constants do
not obey Devonshire's law (Curie-Weiss law) I/epsilon proportional to
(T-C - T) and in pyre-measurements, the mean field exponent (n = 0.4)
is less than 1/2. These imply that Li0.4K0.6NbO3 does not satisfy the
single order parameter mechanism.