Skip to main content
PMC home page
Nature Communications logoLink to Nature Communications
. 2016 Oct 11;7:13089. doi: 10.1038/ncomms13089

Giant piezoelectric voltage coefficient in grain-oriented modified PbTiO3 material

Yongke Yan 1,2,a, Jie E Zhou 3, Deepam Maurya 1, Yu U Wang 3, Shashank Priya 1,2,b
PMCID: PMC5062610  PMID: 27725634

Abstract

A rapid surge in the research on piezoelectric sensors is occurring with the arrival of the Internet of Things. Single-phase oxide piezoelectric materials with giant piezoelectric voltage coefficient (g, induced voltage under applied stress) and high Curie temperature (Tc) are crucial towards providing desired performance for sensing, especially under harsh environmental conditions. Here, we report a grain-oriented (with 95% <001> texture) modified PbTiO3 ceramic that has a high Tc (364 °C) and an extremely large g33 (115 × 10−3 Vm N−1) in comparison with other known single-phase oxide materials. Our results reveal that self-polarization due to grain orientation along the spontaneous polarization direction plays an important role in achieving large piezoelectric response in a domain motion-confined material. The phase field simulations confirm that the large piezoelectric voltage coefficient g33 originates from maximized piezoelectric strain coefficient d33 and minimized dielectric permittivity ɛ33 in [001]-textured PbTiO3 ceramics where domain wall motions are absent.

Inline graphicHigh piezoelectric voltage coefficients drive the sensitivity of piezoelectric sensors. Here, the authors synthesized textured Sm- and Mn-doped PbTiO3 ceramics and demonstrate significant enhancement in voltage coefficient.

The arrival of the Internet of Things is generating opportunities for smart sensors that can operate in varying environmental conditions with ultrahigh performance1,2. A piezoelectric sensor utilizes the piezoelectric effect to measure changes in strain or force, acoustic pressure, and acceleration, by converting the mechanical energy into an electrical charge. Piezoelectric sensors have advantage of operating over a wide range of frequency, providing an excellent linearity over a range of input mechanical amplitude. Furthermore, they are insensitive to electromagnetic fields and radiation and can perform reliably under harsh environmental conditions (temperature, pressure and corrosion)3. The value of piezoelectric voltage coefficient (g, induced voltage under applied stress) represents material figure of merit for piezoelectric sensors3,4.

Most of the state-of-the-art piezoelectric materials are based on perovskite-structured ferroelectrics, such as BaTiO3, PbTiO3 (denoted as PT), Pb(Zr,Ti)O3 (denoted as PZT) and Pb(Mg1/3Nb2/3)O3-PbTiO3 (denoted as PMN-PT). Among them, PZT-based piezoelectric ceramics have been widely utilized due to their superior piezoelectric performance and they can be easily tailored to meet the requirements for different application through compositional modifications4. The piezoelectric voltage coefficient g33 of PZT ceramics is usually in the range of 20 to 30 × 10−3 Vm N−1, as shown in Fig. 1a. The <001> oriented relaxor-PbTiO3 ferroelectric single crystals have ultrahigh piezoelectric strain coefficient d33 and electromechanical coupling factor k33 on the order of 2,000 pC N−1 and 0.9, respectively5,6. However, its g33 coefficient is still <40 × 10−3 Vm N−1. Considering the relation between d and g (g=d/ɛ), it is challenging to have higher value of g, because, any increase in piezoelectric response d is usually accompanied by even larger increase in the dielectric permittivity ɛ.

Figure 1. Comparison of piezoelectric voltage coefficient and phase transition temperature.

Figure 1

Open in a new tab

(a) Piezoelectric voltage coefficient (g33) for well-known perovskite structured piezoelectric oxide single crystal (PMN-PT13 and PMN-PZT13) and ceramics (BaTiO3 (ref. 4), PZT-4 (ref. 4), PZT-5H4, PMN-PT9, PMN-PZT10 and SM-PT). Black bars: single crystal; gray bars: ceramics; blue bars: textured ceramics; blue bar with red border: textured SM-PT in this study. (b) phase transition temperature above room temperature (TR-T: rhombohedral-to-tetragonal ferroelectric phase transition; Tc: Curie temperature) for well-known perovskite structured piezoelectric oxide materials (BaTiO3 (ref. 4), PZT-4 (ref. 4), PZT-5H4, PMN-PT13, PMN-PZT13 and SM-PT). Blue bar with red border: textured SM-PT in this study.

To achieve high g33, the most widely used method has been fabrication of piezoelectric composites containing high d piezoelectric material (such as PZT ceramic, PMN-PT single crystal) with low ɛr polymers (such as epoxy, polyvinylidene fluoride (PVDF))7. It is worth mentioning that PVDF polymer itself has very large g33 due to a very small ɛr (d33=33 pC N−1, ɛr=13, yielding g33=286.7 × 10−3 Vm N−1)8. However, the application of such piezoelectric composites and PVDF is limited to the temperature regime below the melting temperature (166 °C)8. Furthermore, it is difficult to integrate polymeric materials with other functional materials or component normally synthesized by thin/thick film fabrication process requiring high temperature.

Prior studies have shown that d33 and g33 of piezoelectric ceramics can be simultaneously improved by a cost-effective texturing process called templated grain growth (TGG)9,10,11,12. For example, the piezoelectric charge/strain coefficient d33 of <001> textured PMN-PT and PMN-PZT ceramics was found to exceed 1,000 pC N−1, which is about two to five times higher than that of the non-textured ceramics9,10. The g33 magnitude also increased by a factor of two compared to that of the non-textured ceramics, as shown in Fig. 1a. The increase of d33 was attributed to engineered domain state in <001> textured ceramics in similar fashion as that of <001> oriented single crystal. In a rhombohedral single crystal, the domain configurations consisting of the equivalent <111> polarizations exhibit high piezoelectric response along the <001> direction. The enhanced g33 was related to the reduced dielectric constant of textured materials due to the presence of templates with low dielectric permittivity9,10. This phenomenon is analogous to the high g33 obtained in piezoelectric single crystal–polymer composite. Although <001> textured PMN-PT and textured PMN-PZT ceramics exhibit relatively large g33 than that of their non-textured counterparts, the temperature range of application is limited by phase transition between rhombohedral and tetragonal phases (TR-T)13,14,15, as shown in Fig. 1b. The g33 of these textured ceramics was also much lower than that of piezoelectric ceramic/single crystal–polymer composite.

In this work, we provide fundamental insight in the design of high g33–high Tc material by considering anisotropy/composition/phase structure selection, tailored microstructure and domain engineering. First, we select tetragonal PT as starting composition and phase. PT has high Curie temperature (Tc=490 °C), small dielectric constant, and large piezoelectric anisotropy16. It has been widely used for high-temperature–high-frequency sensor and transducer applications. However, due to its large crystal anisotropy (tetragonality c/a=1.064), it is very difficult to sinter PT ceramics. It is also challenging to pole pure PT ceramics due to low resistivity and high coercivity. To overcome these challenges, several dopants have been attempted and it has been shown that the mechanical properties and electrical resistance of PT ceramic can be improved via Sm and Mn doping17. Here we report a Sm and Mn modified PT ceramic (denoted as SM-PT) with grains textured along <001> crystallographic direction to achieve a high Tc (364 °C) and an extremely large g33 (115 × 10−3 Vm N−1) in comparison with other known single-phase oxide materials, as shown in Fig. 1.

Results

Synthesis of textured ceramics

The textured SM-PT ceramic was fabricated by TGG method. In this process, PT plate-like template crystals were aligned in SM-PT ceramic matrix powder by the tape casting method. During sintering, the SM-PT matrix grains grew from aligned PT templates and resulted in textured/grain-oriented SM-PT ceramics. The perovskite PT templates were synthesized using topochemical conversion method. Direct synthesis of PT templates with high aspect ratio morphology is difficult due to its cubic symmetry at the synthesis temperature (1,050 °C). To fabricate the perovskite PT template, layered perovskite structured PbBi4Ti4O15 (PBiT) precursors were first synthesized and then converted into perovskite structured PT. Layered structured PBiT microcrystal can be easily grown into plate-like shape due to its strong structural anisotropy. Figure 2a shows the scanning electron microscopy (SEM) images of the PBiT precursors and PT templates after the conversion reaction. The PBiT precursors had a plate-like high-aspect ratio with a diameter of around 10 μm and a thickness of around 0.3 μm. The final product PT template was able to maintain the platelet shape inherited from the PBiT precursor due to their topotactic relationship. Figure 2b shows the X-ray diffraction patterns of synthesized PBiT precursors and PT templates. It can be seen that PBiT can be converted into PbTiO3 by the topochemical chemical conversion reaction with a little impurity phase denoted by the extra peak near 31° (2θ). It should be noted here that the synthesis of pure PT is much more difficult than BaTiO3, NaNbO3 and so on, using same topochemical conversion method18. Poterala et al.19 have systematically studied the reaction process of the PBiT in a NaCl/Bi2O3/PbO flux system. The results show that the presence of Na+ in the reaction flux will facilitate the perovskite phase formation because the incorporation of Na+ charge balances Bi3+ on the perovskite A-site (forming PbTiO3-Na0.5Bi0.5TiO3 solid solution).

Figure 2. Microstructures and crystal structures of templates and textured ceramics.

Figure 2

Open in a new tab

(a) SEM images of PBiT precursors and PT templates. (b) X-ray diffraction patterns of synthesized PBiT precursors and PT templates. (c) Backscattered electron (BSE)-SEM images of PT textured SM-PT ceramics sintered at different temperature for 2 h. (d) X-ray diffraction patterns of calcined SM-PT matrix powders and textured SM-PT ceramics sintered at different temperature and soaking time.

Figure 2c shows the microstructure evolution and the texture development during sintering in SM-PT ceramics with 5 wt% PT seeds. It can be seen that PT templates were extremely well aligned in SM-PT matrix having particle size in the range of 200–300 nm. The high template-to-matrix grain size ratio (more than 20) is desirable for achieving large driving force for TGG. On increasing temperature up to 1,000 °C, the matrix grains start to nucleate on the templates, which eventually leads to the TGG at further higher temperatures. Although the PT template had a slight composition difference from the SM-PT, this compositional difference was homogenized via elemental diffusion at high temperature (which is the advantage of the reactive TGG), as evidenced by the uniform contrast in the back scattered electron–SEM image (Fig. 2c) and single dielectric peak in the dielectric spectra (Fig. 3a). On increasing temperature up to 1,250 °C, all the randomly oriented matrix grains disappeared leaving well-oriented templated grains. On further increasing the temperature, the sample was over-sintered and the density decreased due to higher porosity. The X-ray diffraction patterns in Fig. 2d confirm the texture development during the sintering process. The intensity of the (110)pc (pc: pseudocubic, parent phase) peak was the highest for the randomly oriented (or non-textured) ceramics. With increasing degree of texture, the intensity of (110)pc Bragg reflections continuously decreased while the intensity of (001)pc and (002)pc reflections increased, manifesting strong preferred crystallographic orientation along <001>pc. To achieve high density and high texture, final samples were sintered at 1,230 °C for 10 h. The samples showed 99% relative density and 95% texture degree in terms of Lotgering factor20.

Figure 3. Dielectric, ferroelectric and piezoelectric properties.

Figure 3

Open in a new tab

(a) Dielectric permittivity and (b) dielectric loss as a function of temperature for non-textured and textured SM-PT samples. The vertical dash-dot lines are used for indicating Curie temperature. (c) Polarization, (d) bipolar strain, and (e) unipolar strain as a function of electric field at 75 °C for non-textured and textured samples. (f) X-ray diffraction patterns of non-textured matrix, unpoled and poled textured ceramics, where Ic is the intensity of (002) peak and Ia is the intensity of (200)/(002) peaks.

Enhanced piezoelectric properties with high Curie temperature

Figure 3a shows the dielectric permittivity as a function of temperature for non-textured and textured SM-PT samples. The modification with Sm and Mn decreased the Tc of PbTiO3 from 490 °C to 343 °C for the non-textured sample. The textured ceramic had a little higher Tc (364 °C) due to slightly less concentration of Sm and Mn (template had no Sm and Mn). However, the Curie temperature of SM-PT ceramic was much higher than most of the PZT based ceramics (PZT-4: 328 °C; PZT-5H: 193 °C)4. The dielectric permittivity of textured samples was found to be lower than that of their non-textured counterparts. From Fig. 3b, it can also be seen that the dielectric loss of textured samples is slight lower than that of non-textured sample. Furthermore, it can be observed that both the samples had higher dielectric losses especially at low frequency and high temperature. Previous studies have indicated that pure PT had high dielectric losses but Mn doping was found to significantly increase the resistivity and reduce the dielectric losses. However, oxygen vacancies become mobile at high temperature, thereby, contributing to the dielectric losses. Figure 3c shows the polarization–electric field (P–E) hysteresis plots for the non-textured and textured samples. It can be seen that the polarization of the textured samples was higher than that of the non-textured samples. Theoretically, the intrinsic polarization value Ps along the polar axis of the mono-domain crystal for the tetragonal phase follows the relationship Ps,<001>= (3)1/2 Ps,<111> (ref. 21). Due to the averaging of polarization in three-dimensional space, the non-textured ceramic has a P between that of <001> and <111> textured ceramics. It can be seen that the polarization values Ps derived from the measured hysteresis loops are well consistent with the theoretical estimation.

Table 1 summarizes the dielectric, ferroelectric and piezoelectric properties of the non-textured and textured samples. It can be seen that the piezoelectric strain coefficient d33 was increased from 53 pC N−1 (non-textured ceramics) to 127 pC N−1 in textured ceramics. More importantly, a large magnitude of g33 (115 × 10−3 Vm N−1) was obtained in textured samples, which was significantly higher than that of PT, PZT and PMN-PT ceramics or single crystals as shown in Fig. 1a.

Table 1. Dielectric, ferroelectric and piezoelectric properties of nontextured, textured PT ceramics and PT single crystal.

Samples ɛr tanδ (1 kHz) Tc (°C) d33 (pC N−1) d31 (pC N−1) g33 ( × 10−3 VmN−1) g31 ( × 10−3 VmN−1) g33/g31 Ref.
La,Mn-doped PbTiO3 ceramic 170 0.008 470 51 4.4 34 2.9 11.7 36
Sm,Mn-doped PbTiO3 ceramic 196 0.009 321 59 1.7 34 1.0 34 37
PbTiO3 single crystal 125 — — 143 26.9 129 24 5.4 38
PbTiO3 single crystal 126 — — 117 25 105 22 4.8 39
Non-textured ceramic 202 0.010 343 53 5.8 30 3.2 9.4 This study
82% textured ceramic 146 0.013 364 95 8.6 74 6.7 11 This study
95% textured ceramic 124 0.010 364 127 26.8 115 24.4 4.7 This study
Open in a new tab

Anisotropy of dielectric and piezoelectric properties

Figure 4a shows the dependence of dielectric and piezoelectric properties on the degree of texture. With the increase in <001> texture degree, it can be found that the d33 increases, ɛr decreases, resulting in a large magnitude of g33 in textured samples.

Figure 4. Piezoelectric properties of doped PT ceramics as a function of texture degree.

Figure 4

Open in a new tab

(a) ɛr, d33 and g33 and (b) k31, g31 and g33/g31.

To better understand the effects of crystallographic orientation of grains on the piezoelectric properties, the orientation dependence was calculated using structural relationships. Using spherical coordinates for 4mm tetragonal crystal, the longitudinal dielectric permittivity and piezoelectric strain coefficient as a function of angle θ away from the polar axis is given as (refs 22, 23):

graphic file with name ncomms13089-m1.jpg
graphic file with name ncomms13089-m2.jpg

The values for PbTiO3 were taken from ref. 24. Figure 5 shows the orientation dependence of dielectric permittivity and piezoelectric strain coefficient. It can be seen that ɛr has the minimum value along [001] direction while d33 has the maximum value along [001] direction. On the basis of the relation g=d/ɛr, the g33 is maximized along [001] direction.

Figure 5. Anisotropy of dielectric and piezoelectric properties.

Figure 5

Open in a new tab

Orientation dependence of (a) dielectric permittivity ɛr*(θ), (b) piezoelectric strain coefficient d33*(θ), and (c) piezoelectric voltage coefficient g33*(θ) of tetragonal PbTiO3 crystal. (d) Cross-section of the surface of (a); (e) cross-section of the surface of (b); (f) cross-section of the surface of (c). The coordinate system indicates crystallographic axes. Numbers on axes indicate values of ɛr*(θ), d33*(θ), g33*(θ), respectively.

Interestingly, the PbTiO3 shows the maximum value of d33 along its polar axis, while the widely studied morphotropic phase boundary composition PMN-PT and PZT and even tetragonal BaTiO3 show their largest piezoelectric magnitude along non-polar direction. PbTiO3 is tetragonal below the Curie temperature without any intermediate ferroelectric–ferroelectric phase transitions. Because of the absence of a proximal phase transition, the shear coefficient d15/d33 of PbTiO3 is small, and the contribution of polarization rotation is very weak. A large d15/d33 is related to proximity to ferroelectric–ferroelectric phase transitions due to flattening of the free energy function whether induced by changes in composition or temperature, or by application of an electric field or stress25. These results suggest that the mechanism for enhanced piezoelectric response in PbTiO3 is polarization extension, which is different from polarization rotation observed in PMN-PT, PZT and BaTiO3 systems.

It should be noted that for PT materials, two types of anisotropy need to be considered. The first type of anisotropy refers to the magnitude change of a particular parameter, such as d33, g33, ɛr as a function of crystallographic orientation. As mentioned above, with increase in <001> texture degree, the value of d33 increases, ɛr decreases, and consequently g33 increases. The second type of piezoelectric anisotropy is the ratio of g33/g31. As listed in Table 1, the distinct macroscopic piezoelectric anisotropy (high g33/g31 or d33/d31) of the doped PT random ceramics may be not a property of the single crystal but of the ceramic26,27. In modified PT ceramics, the ratio of d33/d31 (or g33/g31) has been reported to be over 10; however, this ratio (d33/d31) is about 4.7 for a PT single crystal. Figure 4b shows the ratio of g33/g31 in <001> textured PT ceramics as a function of texture degree, where it can be found that the ratio of g33/g31 is about 10 at low texture degree, but rapidly decreases to 4.8 when the ceramic is highly textured (more than 0.9). In this study, the new finding is the record-breaking value of large g33, and our focus is to maximize g33 based on crystallographic anisotropy (first type) through maximized ratio of d33 and ɛr, not g33/g31. Nevertheless, it is worth noting that a combination of both large g33 (about 70 × 10−3 Vm N−1) and large g33/g31 (about 11) can be achieved at partial texture around f=0.8, which is an attractive performance.

Self-polarization and domain alignment

In addition to the calculation of intrinsic piezoelectric anisotropy (Fig. 5) of tetragonal PbTiO3 single crystal based on polarization rotation, we further investigated the effect of domain switching and domain wall motion on piezoelectric response in SM-PT ceramics. Domain switching and domain wall motion is generally used to explain the extrinsic contribution towards the piezoelectric response in polycrystalline ceramics. Figure 3d,e display the bipolar and unipolar electric field induced strains of non-textured and textured sample at 75 °C. The unipolar strains at 100 kV cm−1 are only 0.19% and 0.07%, for textured and non-textured ceramics, respectively, which suggests the absence of 90° domain switching. If 90° domain were switchable, SM-PT could have exhibited large electric field-induced strain around 6% in textured ceramics and around 2.5% in non-textured ceramics as shown by phase field model below. Li et al.28 used a combined theoretical and experimental approach to establish a relation between crystallographic symmetry and the ability of a ferroelectric polycrystalline ceramic to switch, and found that an equiaxed tetragonal polycrystal will not show 90° domain switching and macroscopic strains through domain switching.

To understand the non-180° domain switching, the X-ray diffraction patterns were recorded on poled and unpoled samples. Due to large tetragonality of PT ceramics, (002)pc (pc: pseudocubic, parent phase) peak splits into two peaks, (002) and (200). The relative intensity ratio of (002) and (200) peaks indicates the percentage of c-domain and a-domain. On the basis of the X-ray diffraction pattern shown in Fig. 3f, it can be seen that the percentage of c-domain and a-domain was not changed under electric field during poling process. Furthermore, for non-textured sample, the theoretical intensity ratio of (002) and (200) is 1:2. Interestingly, we noticed that the percentage of c-domain (Ic) in textured ceramic is much larger than a-domain (Ia). This phenomenon indicates that the <001>-textured SM-PT ceramic exhibits a strong polarization self-alignment or c-domain preferred orientation.

Observation of domain switching

To experimentally observe the domain motion under electric field, vertical and lateral piezoresponse force microscopy (PFM) was performed for both non-textured and textured samples, as shown in Fig. 6. Several inferences can be drawn from the observations in this figure: (a) From the amplitude in vertical mode, it can be seen that the amplitude of non-textured sample has much higher contrast than textured sample due to the wider orientation distribution of each grains; (b) From the phase in vertical mode, it can be seen that 180° domain switching occurred in both non-textured and textured sample; (c) From amplitude and phase in lateral mode, it can be seen that <001> textured sample has much weaker piezoresponse than non-textured samples; (d) Combined the phase contrast from vertical and lateral modes, it can be found that there is no 90° domain motion and only 180° domain switching occurred in both non-textured and textured samples. The difficulty in 90° domain switching can be attributed to the significantly higher activation energy for the non-180° domain switching in tetragonal PbTiO3, as discussed earlier. High activation energy of 90° domain switching can be also indicated from the domain structures of textured SM-PT ceramic under transmission electron microscopy (TEM) as shown in Supplementary Fig. 1 and described in Supplementary Note 1.

Figure 6. Domain structures and domain switching.

Figure 6

Open in a new tab

PFM images of (a) nontextured and (b) textured ceramics. The vertical (V) and lateral (L) PFM was measured under off resonance, f=17 kHz. The dimension of each scanning area is 10 × 10 μm. The square area with red dash line border was poled at DC bias of −60 V; the square area with white dash line border was poled at +60 V.

Phase field model of non-textured and textured SM-PT

To further quantitatively investigate the domain-level mechanisms for the enhanced piezoelectric voltage coefficient in [001]-textured PbTiO3 ceramics, we adopted a phase field model for ferroelectrics (see Supplementary Information for details)29,30,31,32,33. To analyse the mechanisms for enhanced piezoelectric voltage coefficient in [001]-textured PbTiO3 ceramics, we simulated both non-textured and [001]-textured Pb(Zr1-xTix)O3 polycrystals with the composition of x=1 (PT) and x=0.6 (PZT) at room temperature for comparison. PZT with x=0.6 has an equilibrium tetragonal phase as PT does but is closer to the morphotropic phase boundary and has a reduced electrocrystalline anisotropy than PT, thus serving as a good case study for comparison. The same grain structure (Supplementary Fig. 2a) and the two different textures (Supplementary Fig. 2b,c) are used in the simulations to exclude other varying factors that could complicate the comparison study. The simulation system is discretized into 512 × 512 computational grids with periodic boundary conditions. The piezoelectric voltage coefficient gij can be evaluated through either of the direct and converse piezoelectric effects using gij=−(∂Ei/∂σj)D and gij=(∂ɛj/∂Di)σ, respectively, which are equivalent thermodynamic definition via Maxwell's relation34. It is relatively easier to implement the stress free condition (σ=0) in the phase field simulation, thus we simulated the converse piezoelectric effect to evaluate g33=∂ɛ3/∂D3=d33/ɛ33 through the piezoelectric strain coefficient d33 and dielectric permittivity ɛ33.

The simulated polarization distributions and domain structures in non-textured and textured ceramics of PZT and PT that are poled in vertical direction were compared (Supplementary Fig. 3). In the non-textured ceramics shown in Supplementary Fig. 3a,b, both PZT and PT have polarization distributions significantly deviated from the poling direction, as expected for ceramics with random grain orientations. Nevertheless, PT possesses dominantly tetragonal phase, while PZT possesses significant fraction of rhombohedral phase and smaller fraction of orthorhombic phase that coexists with the tetragonal phase, as shown in Supplementary Fig. 4a,b. The non-equilibrium rhombohedral and orthorhombic phase distortions are caused by internal electric field and stress. Such internal fields are present in both non-textured PZT and PT, but the phase distortion is prominent only in PZT due to its significantly reduced electrocrystalline anisotropy with its composition closer to the morphotropic phase boundary. In contrast, in the textured ceramics shown in Supplementary Fig. 3c,d, both PZT and PT have polarization distributions aligned in the poling direction, as expected for [001] texturing where grain orientation is in the [001] poling direction. Slight deviation of polarization vectors from the poling direction is observed as shown in dimmer colors, which is caused by imperfect [001]-texturing. In the simulations the [001] axes of the grains are distributed within a cone of 5° half-apex angle. PT has larger polarization than PZT, as shown by longer vectors. Both textured PZT and PT possess only tetragonal phase as shown in Supplementary Fig. 4c,d, in contrast to phase coexistence in non-textured ceramics shown in Supplementary Fig. 4a,b. It is worth noting that while phase coexistence in non-textured PZT ceramics helps accommodate the electrostriction strain associated with non-uniform polarization distribution, PT has very stable tetragonal phase with lattice strain as large as about 6% that cannot be accommodated in non-textured ceramics thus often causing cracks in real samples (cracking is not considered in the computer simulations, where the very large internal stress instead causes local non-equilibrium phase distortion, which is different from real non-textured PT ceramics).

Figure 7 compares the simulated polarization-electric field and strain-electric field curves in non-textured and textured PZT and PT ceramics. It is observed that, while domain switching is easy in non-textured PZT, the coercive field in textured PZT is significantly increased, which makes domain switching more difficult. On the other hand, domain switching in PT for both non-textured and textured ceramic is always difficult due to the large coercive field. It is worthwhile to mention that in the computer simulation a very large electric field (above 1,600 kV cm−1) was applied on textured PT to observe domain switching without considering dielectric breakdown or mechanical cracking, which is not possible in real samples. Domain switching is also difficult in non-textured PT, since the applied electric field is usually below its coercive field (above 400 kV cm−1). As discussed earlier, if switchable, PT could exhibit large electric field-induced strain around 6% in textured ceramics and around 2.5% in non-textured ceramics, which were not observed as shown in Fig. 3d,e.

Figure 7. Phase field simulated polarization-electric field and strain-electric field curves.

Figure 7

Open in a new tab

(a) polarization-electric field curves of non-textured PZT and PT ceramics; (b) strain–electric field curves of non-textured PZT and PT ceramics; (c) polarization-electric field curves of textured PZT and PT ceramics; (d) strain–electric field curves of textured PZT and PT ceramics.

Figure 8 compares the simulated piezoelectric strain coefficient, dielectric permittivity, and piezoelectric voltage coefficient in non-textured and textured PZT and PT ceramics. The value of d33 and ɛ33 were obtained from the simulated strain-electric field and polarization-electric field responses, respectively, from which the piezoelectric voltage coefficient was evaluated using relation,g33=d33/ɛ33. The simulated value of 130 × 10−3 Vm N−1 agrees well with the experimental value of 115 × 10−3 Vm N−1, thus confirming the giant piezoelectric voltage coefficient in [001]-textured PT ceramics. To further reveal the underlying mechanisms of such a significant enhancement in g33, simulations were also performed with domain walls frozen by setting the gradient coefficient β=0 in Supplementary Equation 1, which produces sharp domain walls that are pinned by discrete computational grids to imitate pinning effects. It is found that domain wall motions contribute about 50% to both d33 and ɛ33 in non-textured PT ceramics, thus have negligible effect on g33. On the other hand, domain wall motions do not play a role in textured PT ceramics, because polarizations are well aligned in [001] direction. The comparison study between textured and non-textured PT ceramics shows that PT has an intrinsically high value of d33 and low value of ɛ33 along [001] axis due to its high electrocrystalline anisotropy, which is in agreement with the experimental measurements shown in Fig. 4 and theoretical analysis shown in Fig. 5. Therefore, the [001]-texturing effectively reduces ɛ33 resulting in a significant enhancement in g33 of [001]-textured PT ceramics. The simulations show that similar mechanisms also improve g33 in textured PZT, but the achievable value is less than in textured PT. Thus, appropriate choice of PT composition combined with texture engineering and domain engineering effectively controls the grain structures and domain processes in [001]-textured PT ceramics to achieve giant piezoelectric voltage coefficient, which provides rational design and synthesis of piezoelectric materials for targeted applications.

Figure 8. Phase-field-simulated piezoelectric and dielectric properties.

Figure 8

Open in a new tab

(a) piezoelectric strain coefficient (d33), (b) dielectric permittivity (ɛ33/ɛ0), and (c) piezoelectric voltage coefficient (g33) in non-textured (gray bars) and textured (red bars) PZT and PT ceramics. To reveal contributions from domain wall motions, values of these coefficients are also plotted with domain walls frozen in the simulations, as shown by hatched blue bars.

Discussion

We report a grain-oriented (with 95% <001> texture) modified PbTiO3 material with high Tc (364 °C) and an extremely large g33 (115 × 10−3 Vm N−1) as compared with other known single-phase oxide materials. Diffraction and scanning probe microscopy studies reveal that self-polarization due to grain orientation along the spontaneous polarization direction plays an important role in achieving large piezoelectric response in a domain motion-confined material. The simulations using phase field model confirm that the large piezoelectric voltage coefficient g33 originates from maximized piezoelectric strain coefficient d33 and minimized dielectric permittivity ɛ33 in [001]-textured PbTiO3 ceramics where domain wall motions are absent.

Methods

Sample preparation

The composition of SM-PT was (Pb0.8725Sm0.085)(Ti0.98Mn0.02)O3. The SM-PT matrix powder was synthesized by conventional solid state reaction method. For this, PbO (99.9%, Sigma-Aldrich), Sm2O3 (99.9%, Alfa Aesar), TiO2 (Ishihara Sangyo Kaisha Ltd.), and MnO2 (99.9%, Alfa Aesar) was mixed and ball-milled in ethanol for 24 h. The mixture was dried at 80 °C and then calcined at 850 °C for 4 h. The calcined powders were ball-milled again with 1.5 wt% excess PbO for 24 h. The templates for texturing SM-PT ceramic are plate-like <001> PbTiO3 microcrystals. The <001> PbTiO3 templates were synthesized by topochemical microcrystal conversion method. In the first step, PbBi4Ti4O15 precursor was synthesized in molten salt. In the next step, PbBi4Ti4O15 precursor was mixed with PbO and NaCl salt, and then heated to 1,050 °C for 3 h. Bi3+ in PbBi4Ti4O15 was substituted by the Pb2+ from PbO, yielding PbTiO3 template and Bi2O3 byproduct. The Bi2O3 byproduct was removed by diluted nitric acid. To fabricate textured ceramics, the ceramic slurry was prepared by ball milling the SM-PT matrix powders with organic binder (Ferro 73225), and toluene/ethanol solvents. Next 5 wt% of PT templates were mixed into the slurry by magnetic stirring. Afterwards, the slurry was casted at the rate of 40 cm min−1 by using doctor blade with height of 250 μm. The dried green tapes were cut, stacked, and laminated at 80 °C under 20 MPa pressure for 15 min. The green samples were heated to 400 °C for 2 h with a heating rate of 0.3 °C min−1 to remove organic solvent and binder, and then isostatically pressed at 200 MPa for 1 min. Samples were subsequently sintered at 1,000–1,300 °C for 2–10 h. The detailed process for the synthesis of grain oriented/textured ceramics is provided elsewhere35.

Characterization

The phase and microstructure were characterized using X-ray diffraction (D8 Advanced, Bruker) and SEM (FEI Quanta 600 FEG, Philips). The degree of pseudo-cubic <001> texture was determined from the X-ray diffraction pattern in 2θ range of 20–60° by Lotgering factor method. The dielectric properties of poled samples were measured as a function of temperature by using a multi-frequency LCR meter (HP4274A). The piezoelectric properties of samples were obtained by resonance and anti-resonance technique using impedance/gain phase analyzer (HP 4194A) and d33-meter (YE 2730 A, APC Products, Inc., PA). Piezoresponse force microscopy (PFM, Bruker Dimension Icon) was used to image the ferroelectric domain structures. Conductive Platinum-Iridium silicon cantilevers (SCM-PIT, Bruker) were used for the PFM characterization. Standard grinding and ion-milling method was used to prepare the electron transparent TEM specimens, and FEI Titan 300 microscope was used to capture TEM images.

Data availability

The data that support the findings of this study are available from the corresponding authors on request.

Additional information

How to cite this article: Yan, Y. et al. Giant piezoelectric voltage coefficient in grain-oriented modified-PbTiO3 material. Nat. Commun. 7, 13089 doi: 10.1038/ncomms13089 (2016).

Supplementary Material

Supplementary Information

Supplementary Figures 1-4, Supplementary Notes 1-2 and Supplementary References.

ncomms13089-s1.pdf (1MB, pdf)
Peer Review File
ncomms13089-s2.pdf (583.4KB, pdf)

Acknowledgments

We gratefully acknowledge the financial supports from AFOSR (S.P., FA9550-14-1-0376), AFOSR STTR program (Y.Y.), National Science Foundation (D.M., PHY-1242637), and DOE (J.Z. and Y.W., DE-FG02-09ER46674). The parallel computer simulations were performed on XSEDE supercomputers. The authors would like to thank the Center for Energy Harvesting Materials and Systems for providing access to industrial experts and equipment.

Footnotes

Author contributions Y.Y. and S.P. conceived the idea; Y.Y. prepared samples, conducted X-ray diffraction, SEM, PFM characterization and performed dielectric/ferroelectric/piezoelectric measurement; J.E.Z. & Y.U.W. conducted modelling analysis; D.M. performed TEM characterization and analysis; S.P. supervised the research. All authors contributed discussion and revised the manuscript; Y.Y., Y.U.W. and S.P. wrote the manuscript.

References

  1. Atzori L., Iera A. & Morabito G. The Internet of Things: A survey. Comput. Netw. 54, 2787–2805 (2010). [Google Scholar]
  2. Gubbi J., Buyya R., Marusic S. & Palaniswami M. Internet of Things (IoT): A vision, architectural elements, and future directions. Future Gener. Comput. Syst. 29, 1645–1660 (2013). [Google Scholar]
  3. Tressler J. F., Alkoy S. & Newnham R. E. Piezoelectric sensors and sensor materials. J. Electroceram. 2, 257–272 (1998). [Google Scholar]
  4. Uchino K. Ferroelectric Devices 2nd edn CRC Press (2010). [Google Scholar]
  5. Park S. E. & Shrout T. R. Ultrahigh strain and piezoelectric behavior in relaxor based ferroelectric single crystals. J. Appl. Phys. 82, 1804–1811 (1997). [Google Scholar]
  6. Zhang S. J. & Li F. High performance ferroelectric relaxor-PbTiO3 single crystals: Status and perspective. J. Appl. Phys. 111, 031301 (2012). [Google Scholar]
  7. Newnham R. E., Bowen L. J., Klicker K. A. & Cross L. E. Composite piezoelectric transducers. Mater. Design 2, 93–106 (1980). [Google Scholar]
  8. Li M. et al. Revisiting the δ-phase of poly(vinylidene fluoride) for solution-processed ferroelectric thin films. Nat. Mater. 12, 433–438 (2013). [DOI] [PubMed] [Google Scholar]
  9. Yan Y., Wang Y. U. & Priya S. Electromechanical behavior of <001>-textured Pb(Mg1/3Nb2/3)O3-PbTiO3 ceramics. Appl. Phys. Lett. 100, 192905 (2012). [Google Scholar]
  10. Yan Y. et al. Giant energy density in <001>-textured Pb(Mg1/3Nb2/3)O3-PbZrO3-PbTiO3 piezoelectric ceramics. Appl. Phys. Lett. 102, 042903 (2013). [Google Scholar]
  11. Messing G. L. et al. Templated grain growth of textured piezoelectric ceramics. Crit. Rev. Solid State 29, 45–96 (2004). [Google Scholar]
  12. Saito Y. et al. Lead-free piezoceramics. Nature 432, 84–87 (2004). [DOI] [PubMed] [Google Scholar]
  13. Zhang S. J., Lee S. M., Kim D. H., Lee H. Y. & Shrout T. R. Temperature dependence of the dielectric, piezoelectric, and elastic constants for Pb(Mg1/3Nb2/3)O3-PbZrO3-PbTiO3 piezocrystals. J. Appl. Phys. 102, 114103 (2007). [Google Scholar]
  14. Yan Y. et al. Enhanced temperature stability in <111> textured tetragonal Pb(Mg1/3Nb2/3)O3-PbTiO3 piezoelectric ceramics. J. Appl. Phys. 118, 104101 (2015). [Google Scholar]
  15. Yan Y., Cho K. H. & Priya S. Piezoelectric properties and temperature stability of Mn-doped Pb(Mg1/3Nb2/3)-PbZrO3-PbTiO3 textured ceramics. Appl. Phys. Lett. 100, 132908 (2012). [Google Scholar]
  16. Shirane G. & Hoshino S. On the phase transition in lead titanate. J. Phys. Soc. Jpn. 6, 265–270 (1951). [Google Scholar]
  17. Ito Y., Nagatsuma K., Takeuchi H. & Jyomura S. Surface acoustic wave and piezoelectric properties of (Pb,Ln)(Ti,Mn)O3 ceramics (Ln = rare earths). J. Appl. Phys. 118, 4479–4486 (1981). [Google Scholar]
  18. Poterala S. F., Chang Y. F., Clark T., Meyer R. J. & Messing G. L. Mechanistic interpretation of the aurivillius to perovskite topochemical microcrystal conversion process. Chem. Mater. 22, 2061–2068 (2010). [Google Scholar]
  19. Poterala S. F., Meyer R. J. Jr & Messing G. L. Synthesis of high aspect ratio PbBi4Ti4O15 and topochemical conversion to PbTiO3-based microplatelets. J. Am. Ceram. Soc. 94, 2323–2329 (2011). [Google Scholar]
  20. Logtering F. K. Topotactical reactions with ferrimagnetic oxides having hexagonal crystal structures - I. J. Inorg. Nucl. Chem. 9, 113–123 (1959). [Google Scholar]
  21. Cao H., Fang B. J., Xu H. Q. & Luo H. S. Crystal orientation dependence of dielectric and piezoelectric properties of tetragonal Pb(Mg1/3Nb2/3)O3-38%PbTiO3 single crystal. Mater. Res. Bull. 37, 2135–2143 (2002). [Google Scholar]
  22. Damjanovic D., Budimir M., Davis M. & Setter N. Piezoelectric anisotropy: enhanced piezoelectric response along nonpolar directions in perovskite crystals. J. Mater. Sci. 41, 65–76 (2006). [Google Scholar]
  23. Davis M., Budimir M., Damjanovic D. & Setter N. Rotator and extender ferroelectrics: Importance of the shear coefficient to the piezoelectric properties of domain-engineered crystals and ceramics. J. Appl. Phys. 101, 054112 (2007). [Google Scholar]
  24. Haun M. J., Furman E., Jang S. J., McKinstry H. A. & Cross L. E. Thermodynamic therory of PbTiO3. J. Appl. Phys. 62, 3331–3338 (1987). [Google Scholar]
  25. Budimir M., Damjanovic D. & Setter N. Piezoelectric anisotropy-phase transition relations in perovskite single crystals. J. Appl. Phys. 94, 6753–6761 (2003). [Google Scholar]
  26. Wersing W., Lubitz K. & Mohaupt J. Anisotropic piezoelectric effect in modified PbTiO3 ceramics. IEEE Trans. Ultrason. Ferr. 36, 424–433 (1989). [DOI] [PubMed] [Google Scholar]
  27. Turik A. V. & Topolov V. Yu Ferroelectric ceramics with a large piezoelectric anisotropy. J. Phys. D Appl. Phys. 30, 1541–1549 (1997). [Google Scholar]
  28. Li J. Y., Rogan R. C., Ustundag E. & Bhattacharya K. Domain switching in polycrystalline ferroelectric ceramics. Nat. Mater. 4, 776–781 (2005). [DOI] [PubMed] [Google Scholar]
  29. Yang W. & Chen L. Q. Computer simulation of the dynamics of 180° ferroelectric domains. J. Am. Ceram. Soc. 78, 2554–2556 (1995). [Google Scholar]
  30. Hu H. L. & Chen L. Q. Computer simulation of 90° ferroelectric domain formation in two-dimensions. Mater. Sci. Eng. A 238, 182–191 (1997). [Google Scholar]
  31. Hu H. L. & Chen L. Q. Three-dimensional computer simulation of ferroelectric domain formation. J. Am. Ceram. Soc. 81, 492–500 (1998). [Google Scholar]
  32. Semenovskaya S. & Khachaturyan A. G. Development of ferroelectric mixed states in a random field of static defects. J. Appl. Phys. 83, 5125–5136 (1998). [Google Scholar]
  33. Wang Y. U. Field-induced inter-ferroelectric phase transformations and domain mechanisms in high-strain piezoelectric materials: insights from phase field modeling and simulation. J. Mater. Sci. 44, 5225–5234 (2009). [Google Scholar]
  34. Lines & Glass A. M. Principles and Applications of Ferroelectrics and Related Materials Clarendon Press (1977). [Google Scholar]
  35. Yan Y., Cho K. H. & Priya S. Templated grain growth of <001 >-textured 0.675Pb(Mg1/3Nb2/3)O-0.325PbTiO3 piezoelectric ceramics for magnetic field sensors. J. Am. Ceram. Soc. 94, 1784–1793 (2011). [Google Scholar]
  36. Ikegami S., Ueda I. & Nagata T. Electromechanical properties of PbTiO3 ceramics containing La and Mn. J. Acoust. Soc. Am. 50, 1060–1066 (1971). [Google Scholar]
  37. Suwannasiri T. & Safari A. Effect of rare-earth additives on electromechanical properties of modified lead titanate ceramics. J. Am. Ceram. Soc. 76, 3155–3158 (1993). [Google Scholar]
  38. Topolov V. Y., Bisegna P. & Bowen C. R. Piezo-Active Composites: Orientation Effects and Anisotropy Factors Springer (2014). [Google Scholar]
  39. Gavrilyachenko V. G. & Fesenko E. G. Piezoelectric effect in lead titanate single crystal. Sov. Phys. Crystallogr. 16, 549 (1971). [Google Scholar]

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Supplementary Information

Supplementary Figures 1-4, Supplementary Notes 1-2 and Supplementary References.

ncomms13089-s1.pdf (1MB, pdf)
Peer Review File
ncomms13089-s2.pdf (583.4KB, pdf)

Data Availability Statement

The data that support the findings of this study are available from the corresponding authors on request.

Articles from Nature Communications are provided here courtesy of Nature Publishing Group

RESOURCES