We present the results of dielectric and anelastic spectroscopy measurements, together with X-ray diffraction investigations, which allow us to establish more precisely the phase diagram of Pb1-xLax(Zr0.9Ti0.1)(1-x/4)O-3 (PLZT x/90/10) in the compositional range around the AFE/FE phase boundary (0< x< 0.04). From structural analysis and polarization-electric field measurements, we have found that the ground state of PLZT samples with x< 0.025 is rhombohedral R3c, while samples with x> 0.032 are antiferroelectric with orthorhombic Pbam structure. In-between, for compositions with 0.025 <= x <= 0.032, a coexistence of the AFE/FE phases is evidenced. The use of complementary dielectric and anelastic techniques allows to follow the phase transitions shifts throughout all the interesting composition range and to construct the temperature-composition phase diagram. The tilt instability line, separating the R3c and R3m low and high temperature phases, has been evidenced. Moreover, the new transition, associated with the onset of disordered tilting preceding the long range order of the R3c phase, previously found in Zr-rich Pb(Zr, Ti)O-3, is confirmed in rhombohedral PLZT x/90/10 compositions. (c) 2015 AIP Publishing LLC.
Refining the phase diagram of Pb1-xLax(Zr0.9Ti0.1)(1-x/4)O-3 ceramics by structural, dielectric, and anelastic spectroscopy investigations
F Cordero;IV Ciuchi;C Galassi
2015
Abstract
We present the results of dielectric and anelastic spectroscopy measurements, together with X-ray diffraction investigations, which allow us to establish more precisely the phase diagram of Pb1-xLax(Zr0.9Ti0.1)(1-x/4)O-3 (PLZT x/90/10) in the compositional range around the AFE/FE phase boundary (0< x< 0.04). From structural analysis and polarization-electric field measurements, we have found that the ground state of PLZT samples with x< 0.025 is rhombohedral R3c, while samples with x> 0.032 are antiferroelectric with orthorhombic Pbam structure. In-between, for compositions with 0.025 <= x <= 0.032, a coexistence of the AFE/FE phases is evidenced. The use of complementary dielectric and anelastic techniques allows to follow the phase transitions shifts throughout all the interesting composition range and to construct the temperature-composition phase diagram. The tilt instability line, separating the R3c and R3m low and high temperature phases, has been evidenced. Moreover, the new transition, associated with the onset of disordered tilting preceding the long range order of the R3c phase, previously found in Zr-rich Pb(Zr, Ti)O-3, is confirmed in rhombohedral PLZT x/90/10 compositions. (c) 2015 AIP Publishing LLC.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.
