Structure and Physical Properties of PZT-PMnN-PSN Ceramics Near the Morphological Phase Boundary

The 0.9Pb(ZrxTi1−x)O3-0.07Pb(Mn1/3Nb2/3)O3-0.03Pb(Sb1/2Nb1/2)O3 (PZT-PMnN-PSN) ceramics were prepared by columbite method. The phase structure of the ceramic samples was analyzed. Results show that the pure perovskite phase is in all ceramics specimens. The effect of the Zr/Ti ratio on the region of morphotropic phase boundary for PZT-PMnN-PSN ceramics was studied. Experimental results show that the phase structure of ceramics changes from tetragonal to rhombohedral with the increase of the content of Zr/Ti ratio in the system. The composition of PZT-PMnN-PSN ceramics near the morphotropic phase boundary obtained is the ratio of Zr/Ti: 49/51. At this ratio, the ceramic has the optimal electromechanical properties: the , the , the  pC/N, the , high remanent polarization ( μC·cm−2), and low coercive field  kV·cm−1.

In ceramics manufacturing technology, piezoelectric PZT system ceramics compositions are mostly near the tetragonalrhombohedral (T-R) morphotropic phase boundary (MPB).The electromechanical response of these ceramics is known to be most pronounced at the MPB.So, there have been many investigations on the coexistence of two phases near MPB in PZT system [3].The reports suggested the existence of a range of compositions where both tetragonal and rhombohedral phases are thermodynamically stable [7,12].
In this study, 0.9Pb(Zr tetragonal and rhombohedra phases and the exact composition of the MPB in chemically homogeneous PZT-PMnN-PSN ceramics were determined.

Experimentals
The polycrystalline samples of PZT-PMnN-PSN were synthesized by columbite precursor method.The raw materials including powders (high purity) of PbO (99%), ZrO The ground materials were pressed into disk 12 mm in diameter and 1.5 mm in thickness under 100 MPa.The samples were sintered in a sealed alumina crucible with PbZrO 3 coated powder at temperature 1150 ∘ C for 2 h.Scanning electron micrograph of the sample was taken at room temperature.The sintered pellet was polished and silver electroded and connected to an LCR meter (Hioki, Japan) for dielectric measurement.The frequency dependence of dielectric constant and loss tangent were obtained using the LCR meter in the frequency range from 0.1 kHz to 500 kHz.The polarization-electric field (P-E) hysteresis loops were measured by a Sawyer-Tower circuit at 50 Hz.
As-sintered samples were ground and polished to remove the surface layer for X-ray diffraction (XRD, D/MAX-RB, Rigaku, Japan).Cu K radiation with a step of 0.01 s was used.The microstructure of the samples was examined by using a scanning electron microscope (SEM).The electromechanical coupling factor (  ), mechanical quality factor (  ), and piezoelectric coefficient ( 31 ) were calculated by using the resonance-antiresonance method.The dielectric constant was calculated from the capacitance and the dimension of the samples.
A transition from tetragonal phase to rhombohedra phase is observed as Zr/Ti ratio increases.The multiple peak separation method was used to estimate the relative fraction of coexisting phases.The relative phase fraction was then calculated by the following equations [14]: . ( With increasing Zr/Ti ratio, tetragonal relative fraction decreases and rhombohedra relative fraction increases.The analysis of the relative phase fraction in the PZT-PMnN-PSN system indicates that tetragonal and rhombohedra phases coexist in the composition range for 0.48 ≤  ≤ 0.52 as shown in Figure 2.
Figure 3 shows the SEM image of the fractured surface of PZT-PMnN-PSN ceramics at different Zr/Ti ratios.It is observed from the micrographs that the average grain size of samples are increased with the increasing amount of Zr/Ti ratio.However, when further increasing the Zr/Ti ratio to 51/49, the average grain size is reduced.These results are in good agreement with the reported in the literature [15].

The Influence of Zr/Ti Ratio on the Dielectric Properties.
Figure 4 shows the temperature dependence of dielectric permittivity and dielectric loss tan  of PZT-PMnN-PSN system (1 kHz) with Zr/Ti ratios 46/54 up to 54/46, respectively.As shown in Figure 4, all the samples in morphotropic phase boundary region (Zr/Ti = 48/52−52/48) exhibit typical relaxor ferroelectric behavior around.The dielectric responses are characterized by diffuse dielectric peaks and a slight shift of permittivity of maximum toward higher temperature with increasing frequencies.
By comparing the curves in Figure 1, we see that the broadness of dielectric response increases with an increase in Zr/Ti ratio and the largest is at Zr/Ti = 49/51.The temperature of dielectric permittivity maximum also increases with increase of Zr/Ti ratio.All samples have a temperature called Burn temperature at which dielectric response starts complying Curie-Weiss law and the system starts the transition into paraelectric phase.
Figure 5 shows Curie-Weiss dependence of the permittivity of the samples at temperatures start to   .The fitting parameters [14] are given in Table 1.
From Table 1, we can see that all the temperature values extend to decrease with the increase of Zr/Ti ratio.

The Influence of Zr/Ti Ratio on the Ferroelectric Properties.
Figure 6 shows - hysteresis loops of all samples.The well-saturated hysteresis loops were observed, and the values of remanent polarization (  ) and coercive field (  ) were presented in Table 2.
It's demonstrated that the hysteresis loops of all samples are of typical forms characterizing ferroelectric materials.The remanent polarization (  ) reaches the maximum value of 49.2 C/cm 2 and The coercive field (  ) reaches the minimum value of 10.28 kV⋅cm −1 at Zr/Ti = 49/51 (Figure 7).Simple diagram phase of PZT-PMnN-PSN ceramics near MPB, which is attractive system displaying excellent piezoelectric and dielectric properties, good electrostrictive effects, and relaxation of ferroelectric phase transition is shown in Figure 9.

Conclusion
The results obtained from the experiment are as follows.
(2) The structure of ceramics sintered at 1150 ∘ C shows the pure perovskite structure in all ceramics specimens; the structure of PZT-PMnN-PSN ceramics was transformed from tetragonal to rhombohedra, with Zr/Ti ratio increased in system.
(4) The piezoelectric ceramic with Zr/Ti ratio of 49/51 may be suitable for piezoelectric transformer applications and other high power devices.

Figure 3 :
Figure 3: Surface morphologies observed by SEM of PZT-PMnN-PSN ceramics at various ratios of Zr/Ti.

Figure 8 Figure 4 :Figure 5 :Figure 6 :
Figure8shows the piezoelectric and dielectric properties as a function of Zr/Ti ratio.PZT-PMnN-PSN exhibits high

Figure 7 :Figure 8 :Figure 9 :
Figure 7: The   and the   as a function of Zr/Ti ratios.
piezoelectric coefficient and electromechanical coupling factor around the MPB.From the trend of the variation of piezoelectricity, it reaches the maximum values of  31 = −236 pC/N,   = 0.61 at Zr/Ti = 49/51.

Table 2 :
Calculated   and   values of samples.