Research Letter  Open Access
Effect of Sm Substitution on Structural, Dielectric, and Transport Properties of PZT Ceramics
Abstract
The polycrystalline samples of (PSZT) (where ??=??0.00,??0.03,??0.06, and 0.09) were prepared by a hightemperature solidstate reaction technique. Preliminary Xray structural analysis of the materials at room temperature has confirmed their formation in singlephase with tetragonal crystal structure. The temperature dependence of dielectric response of the samples at selected frequencies has exhibited their phase transition well above the room temperature. The variation of ac conductivity with temperature and the value of activation energy reveal that their conduction process is of mixed type (i.e., singly ionized in ferroelectric region and doubly ionized in paraelectric phase).
1. Introduction
Lead zirconate titanate (PZT) is a wellknown ferroelectric material with a perovskite ABO_{3} structure (A??=??mono or divalent and B??=??trihexavalent ions) [1–3]. It is widely used for many applications such as actuators, transducers, and pyroelectric detectors. It is a solidstate solution of ferroelectric PbTiO_{3} and antiferroelectric PbZrO_{3} exhibiting two ferroelectric phases: a tetragonal phase in titanium rich and a rhombohedra phase in zirconiumrich compositions [4, 5]. The separation line between these two phases is called morphotropic phase boundary (MPB) where the electrical properties of the materials rise to a great extent [6]. However above and below MPB, it has many interesting properties useful for devices.
The physical properties and device parameters of PZTbased compounds are greatly influenced by chemical substitutions, synthesis process, and some other factors. It is well observed that the Lamodified PZT has tremendous applications in electronics and electrooptics [7, 8].
The literature survey on pure and modified PZT materials reveals that no systematic studies have been reported on physical properties and device parameters of Smsubstituted PZT (i.e., PSZT) with Zr/Ti ratio 45/55 [9–13]. In view of the above, we have studied the effect of samarium substitution on structural, dielectric, and ac conductivity properties of PZT (Zr/Ti: 45/55) ceramics, which is reported here.
2. Experimental Details
The polycrystalline samples of Smmodified PZT (i.e., PSZT) (Zr_{0.45}Ti_{0.55}O_{3} (where x??= 0.00, 0.03, 0.06, and 0.09) were prepared by a hightemperature solidstate reaction technique using highpurity (99.9%) oxides (i.e., PbO, ZrO_{2}, TiO_{2}, and Sm_{2}O_{3}) in a suitable stoichiometry with 3% more PbO (to compensate lead loss at high temperatures). The homogeneous mixed ingredients were calcined at an optimized temperature and time (1100^{°}C, 10 hours) in an alumina crucible. The calcined powders, with small amount of polyvinyl alcohol (PVA) as binder, were converted into pellets at a pressure of 4??×??10^{6}?N/m^{2} using hydraulic press. These pellets were sintered in an alumina crucible at an optimized temperature and time (1200^{°}C, 10 hours) aiming to get nearly 97% of theoretical density.
The Xray diffraction (XRD) data on the calcined powders were recorded using Xray diffractometer (Rigaku Miniflex, Japan) with in a wide range of Bragg’s angles () at a scanning rate of 3^{°}/minute. The dielectric data of the materials were obtained on silverelectroded samples using phase sensitive multimeter (PSM; Model 1735) in a wide range of frequency (10^{2}–10^{6}?Hz) and temperature (room temperature 500^{°}C) at a potential difference of 1?V with the stabilized temperature at an interval of 2.5^{°}C.
3. Results and Discussion
3.1. Structural Analysis
The nature of room temperature XRD patterns of (Zr_{0.45}Ti_{0.55}O_{3} (PSZT) with x??=??0.00, 0.03, 0.06, and 0.09 (Figure 1) as compared to the reported ones [14, 15] confirms the formation of single phase with tetragonal crystal structure. All the reflection peaks were indexed in tetragonal crystal system using computer software POWDMULT [16]. On the basis of best agreement between the observed (obs) and the calculated (cal) dspacing (i.e., ), all the PSZT compounds were found to be in tetragonal crystal system with their refined lattice parameters given in Table 1. In the XRD patterns, there is an additional peak (for ) usually referred as secondary or pyrochlore phase [17, 18]. Though these peaks are undesirable, it is some time essential for formation of the perovskites [19]. The percentage of pyrochlore phase in PSZT for x??=??0.06 and 0.09 was estimated [20] as 3% and 7%, respectively.

3.2. Dielectric Study
The variation of relative dielectric constant () of PSZT (having Sm contents x??=??0.00, 0.03, 0.06, and 0.09) with temperature at selected frequencies (10^{3}–10^{6}?Hz) is shown in Figure 2. It is found that decreases on increasing frequency which indicates a normal behavior of the ferroelectric and/or dielectric materials. The higher values of at lower frequency are due to the simultaneous presence of all types of polarizations (space charge, dipolar, ionic, electronic, etc.) which is found to decrease with the increase in frequency. At high frequencies (>10^{12}?Hz) electronic polarization only exists in the materials. When temperature of PSZT samples is increased, first increases slowly and then rapidly up to a maximum value (). Temperature of the material corresponding to is called Curie or critical temperature (T_{c}). As at this T_{c}, phase transition takes place between ferroelectricparaelectric phases so it is also called transition temperature. At the higher temperature (=T_{c}), the space charge polarization originates due to mobility of ions and imperfections in materials and thus contributes to a sharp increase in [21, 22]. The value of is found to be highest for PZT. As Sm content in PSZT increases, the value of exhibits a sharp decrease for x??=??0.03, then an increase for x??=??0.06, and again decrease for x??=??0.09. The value of T_{c} is found to be highest for PZT which decreases gradually on increasing Sm content in PSZT. However, for each PSZT samples T_{c} is found to be unaffected with the change in frequency supporting the nonrelaxor behavior of Smmodified PZT [23]. The values of and T_{c} of PSZT are compared in Table 1.
(a)
(b)
(c)
(d)
The frequencytemperature dependence of tangent loss () of PSZT is shown in Figure 2. With the increase in temperature, is found to be very low and almost remains constant up to T_{c} beyond which it indicates a significant increase. The nature of variation of at higher frequency and temperature can be explained by spacecharge polarization [23]. This decreases with the increase in frequency as expected [24].
3.3. ac Conductivity
The ac conductivity () of PSZT for x??=??0.00, 0.03, 0.06, and 0.09 at frequency 10?kHz was calculated using dielectric relation where is the angular frequency and the permittivity of free space. Figure 3 shows an increasing trend of ac conductivity around T_{c}. A sharp maximum in at T_{c} (observed by dielectric analysis) indicates a marked dispersion which may be due to the increase in polarizability. Above T_{c}, the conductivity data appears to fall on a straight line exhibiting a typical behavior of the dc component of the conductivity [23]. The linear variation of over a wide range of temperature supports the existence of thermally activated transport properties in the materials following the Arrhenius equation: where is the preexponential factor, K_{B} the Boltzmann constant and E_{a} the activation energy. The value of activation energy (E_{a}) of PSZT was found to be 0.93, 0.57, 1.45, and 0.79 for x??=??0.00, 0.03, 0.06, and 0.09, respectively, in the hightemperature paraelectric phase which suggests its dependence on ionization level of oxygen vacancy [25–27].
4. Conclusions
Preliminary structural analysis using room temperature Xray diffraction data obtained from the calcined powders of polycrystalline samples of Smmodified PZT (i.e., (Zr_{0.45}Ti_{0.55}O_{3}) has confirmed their tetragonal phase with the presence of a small amount of pyrochlore phase during higher concentration of Sm (3% for x??=??0.06 and 7% for 0.09). Detailed study of dielectric properties of PSZT as a function of temperature at selected frequencies has exhibited that maximum or peak dielectric constant, tangent loss, and transition temperature are strongly dependent on Sm content in PSZT. The electrical conductivity (ac) of PSZT may not only due to singly ionized in low temperature (ferroelectric phase) region but also due to doubly ionized in the hightemperature region.
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Copyright © 2009 Rajiv Ranjan et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.