The features of the single crystals 0.76PMN-0.24PT in dielectric, ferroelec
tric, pyroelectric properties and domain structures indicate that they are
located between typical ferroelectrics and normal ones. The unpoled crystal
s present a transitional domain configuration between microdomains and typi
cal macrodomains while the crystals on (001) cuts undergo field-induced pha
se transition under poling, showing two special temperature points T-d and
T-m during the succedent heating procedure. The dielectric constant starts
to decrease drastically at T-d during cooling, or the transformation from i
nduced macrodomain to transitional domain takes place at T-d during heating
. Ferroelectric-paraelectric phase transition or depolarization continues w
ithin the whole temperature range of T-d-T-m, where ferroelectric phase in
the form of transitional macrodomains coexists with paraelectric phase. The
n the crystals macroscopically transoform into paraelectric phase containin
g ferroelectric microdomains at a temperature above T-m. However, owing to
the influence of crystallite orientation on field-induced phase transition,
the temperature Td does not appear in the same temperature-electric field
history in multicrystal ceramics with the same composition as the above sin
gle crystals.