Proceeding of the First Scientific Conference on Nanotechnology , Advanced Materials and Their Applications2009 Structure and Morphology of Nanocrystalline BZT Powders Prepared Using Hydrothermal Method M. M. Ismaila, b, *, Sabah. M. Alib, Z. S. Ahmedc and Wan. Q. Cao a, Abstract The nanocrystalline of BaZrxTi1-xO3 (BZT) (where x= 0, 0.001 and 0.008) powders have been prepared by hydrothermal method at 150oC for 2h using as prepared titanium tetraclouride, zirconium oxyclouride and barium hydroxide as starting materials. They were investigated by x-ray diffraction XRD, transmission electron microscopy TEM, selection area electron diffraction SAED and high resolution transmission electron diffraction HRTEM. The BaTiO3 (BT) nanocrystals have a cubic perovskite structure and they convert to tetragonal perovskite after annealing at temperature 700oC while BZT convert it at higher than 700oC as revealed by XRD. It is found that the increased in Zr content caused a decreased in tetragonallity factor. The morphology of BT powders showed a star shape and dendrites pattern, not very smooth surfaces and non uniform in contrast while the dendrites pattern is absence in BZT as a result of TEM. There is a high contract variation in the TEM images of BT and BZT which indicates the presence of strains inside the lattice. The SAED results indicate a perfect crystal structure and HRTEM images revealed the presence BZT powders that showed small nucleated islands at the edges of the faceted particles of the prepared BT. Keywords: Nanocrystalline, BZT, Hydrothermal a School of Physics and Electronic, Hubei University, Wuhan 430062, China School of Applied Science, University of Technology, Baghdad, Iraq c Ministry of Science and Technology, Baghdad, Iraq b 115 Proceeding of the First Scientific Conference on Nanotechnology , Advanced Materials and Their Applications2009 those of mixing oxide synthesis due to finer scale of mixing at relatively low temperatures. In hydrothermal method, most of researchers have used alkali metal hydroxides namely KOH or NaOH as mineralized. The usage of aqueous ammonia instead of NaOH or KOH in hydrothermal process will get many advantageous. Aqueous ammonia does not have been a tendency to get incorporated into the oxide matrix and any residual ammonia entrained in BT powders can be easily driven off during the powders at 100oC[10]. In the present work, we report on a hydrothermal method to prepare nanocrystalline BaTiO3 (BT), BaZr0.001Ti0.999O3 (BZT1) and BaZr0.008Ti0.992O3 (BZT2) powders and discuss the tetragonality, structural and morphology of obtained powders. Introduction Tetragonal BaTiO3 has excellent dielectric properties, which makes it the most important ferroelectric material used in the manufacture of thermistors, ceramic capacitor and especially multi-layer ceramic capacitors (MLCCs)[1]. Substitution of Ti4+ (atomic weight of 49.9, ionic radius of 0.0745 nm) with Zr4+ (atomic weight of 91.2, ionic radius of 0.086 nm) exhibits several interesting features in the dielectric behavior for BT ceramic. When the Zr content is less than 10%, the BZT ceramics show normal ferroelectric behavior and dielectric anomalies corresponding to cubic to tetragonal (Tc), tetragonal to orthorhombic (T2) and orthorhombic to rhombohedra (T3) phase transition [2]. This lead free relaxor material (BZT) presents a great interest both for applications in the field of environmental protection and for fundamental studies. The conventional method involves repeated milling and calcinations (>1200 oC) of BaCO3 and TiO2 powders. This method, however, results in the formation of nonequimolar barium titanate, such as Ba2TiO4, BaTi2O5 and BaTi4O9, which often lead to a compositional inhomogeniety [3]. Recently, wet chemical technologies such as the solgel method[4], oxalate method [5, 6] and hydrothermal method [7, 8, 9] have been replaced the classical solid state reaction for the synthesis of BT. Wet chemical methods have led to homogeneous, phase pure BT with comparatively finer particle size than Experimental Appropriate amounts of Ba(OH)2.8H2O (98%) and TiCl4 (99%) were weighted and used as precursor. The dilution procedure consists of adding the concentration TiCl4 slowly to the distilled water, which is kept close to freezing temperature (~5oC) by water bath, under the constant stirring conditions. The result is TiOCl2, which needs to be used immediately as its shelf life is only a few hours at room temperature. Therefore, TiOCl2 is kept in water bath at temperature ~5oC. The result is mixed with ZrOCl2 solution. Reactive gels were precipitated by the dropping of aqueous ammonia solution to TiOCl2 and ZrOCl2 solution. 116 Proceeding of the First Scientific Conference on Nanotechnology , Advanced Materials and Their Applications2009 The gels were washed from free of chloride ions and were mixed with 0.6M Ba(OH)2 solution with vigorous stirrer. The molar ratio of Ba/(Ti+Zr) and ph are kept at 1.6 and 13 respectively. The hydrothermal reaction was carried out in Teflon-lined stainless steel autoclave and the degree of fill was 80 %. The sealed vessel was heated to 150oC for 2h. After cooling dawn to room temperature, the resultant precipitated was washed with distilled water for several times and finally dried at 60oC for 24h.Crystal structure of the produced particles was analyzed at room temperature using XRD (D/Max-RB Model). The powder morphology was performed by TEM (JEM-100SX NEC). cubic BT, BZT and BZT2 with lattice constant 4.0189, 4.021 and 4.0225Ao respectively. Because of radius of Zr is lager than Ti, the increasing of lattice constant with increase of Zr content is shown. It is known from the literature that BT is a stable tetragonal phase at room temperature with lattice o constants a = 3.98A and c = 4.02Ao. To discuss the expanding of lattice constants for BT and BZT, it is important to study the reasons of suppression of tetragonality phase. The different between cubic and tetragonal phase of BT is a Brage angle at 45o on XRD pattern, therefore, it is better to study the limited range of XRD especially between 44 and 46o. This region of the diffraction pattern is characteristic of the tetragonal versus cubic from BT. Fig. 3 shows that the XRD pattern of as prepared BT and BZT powders at limited range from 44.6 to 46o with different annealing temperature (500, 700 and 1000oC). it is found the splitting of the (200) peak with the lower angle shoulder indexed at (002) when annealing temperature at 700oC is observed in BT as shown in Fig. 3a while in BZT the splitting is taken place at higher than 700oC as shown in Fig. 3b and c. In the cubic form, this peak remains unsplit. It is apparent from the Fig.3, annealing temperature at 700oC expels some defects which incorporated inside the lattice, and therefore the lattice constant becomes a smaller. At 1000oC, all the defects were removed and the lattice constant (a) of BT becomes smaller and close with standard tetragonal BT. Results and Discussion XRD results Fig.1 shows that the XRD pattern of the BZT using TiO2, ZrOCl2.8H2O and Ba(OH)2.8H2O at 150oC for 2h which hydrothermally treated. It is found the BaTiO3 (BT) and BaZrO3 (BZ) was formed while the BZT does not form and there are some peaks refer to TiO2. It is likely the reason of this result is that the particle size of raw materials is not fine, especially TiO2, so it is better to use a fine TiO2. Fig. 2 shows the XRD pattern of BT. BZT1 and BZT2 using TiO2 and ZrO2 gels with Ba(OH)2.8H2O using hydrothermal method at 150oC for 2h. This result indicates the addition of Zr is forming a stable solid solution with BT lattice. The XRD pattern is fit well with the peak positions of standard 117 Proceeding of the First Scientific Conference on Nanotechnology , Advanced Materials and Their Applications2009 Fig. 3 b and c show the BZT1 and BZT2 have the same behavior of BT, in other words, at a temperature higher than 700oC, the peak of (200) splits and phase transition was observed. The diffuse of Zr in BT was caused the retarding of appearance the tetragonal phase because of the BZT need a higher temperature to form in compare with the formation of BT so BZT contains more defects than BT. Fig. 4 shows the lattice constants of as prepared BT, BZT1 and BZT2 powders as a function of annealing temperature. The lattice constants were calculated from XRD results. It is found the lattice constant (a) decreased with an increase of annealing temperature particularly decreased rapidly at 500oC for BT while in BZT1 and BZT2 this happen after 700oC. The annealed BZT powders up to 1000oC enable BZT unit cell to expel all the defects which incorporating inside it, so that the distortion of unit cell taken place and tetragonal phase was observed. Fig. 5 shows the tetragonallity factor (c/a) of BT, BZT1 and BZT2 powders with annealing temperature. It can be seen the tetragonallity factor increases with annealing temperature and decreases with increased of Zr content as shown in Fig. 6. many of tiny particles which tend to form a star and dendrites forms. Fig. 8b shows the SAED pattern recorded from Fig. 8a, which demonstrates good crystallinity comes from the regular spots and coordination. Fig. 9b depicts the HRTEM image taken from Fig. 9a. It is shown the different variations of HRTEM contract indicate the existence of high strain in particles. The large strains are indicated by a contract variation across the particle and this agreed with the results of Li et al [11]. The lattice fringes of HRTEM image was examined to be 2.84 nm, which close to the (110) lattice spacing of the cubic BT. It is also found there is a gradual contract from bright in the edge of particle to dark inside it which indicates a gradual strain inside the lattice. In addition, the surrounding edge is not very smooth, and some of surface steps are observed. The HRTEM images also revealed the presence BT powders showed a small nucleated island at the edges of the faceted particles The particle size and morphology of as prepared BZT2 powders synthesized at 150oC for 2h using hydrothermal method are shown in Fig 10 a and b. The particles have a mixture's shape (spherical and cubes with truncated edge) with the average size about 150 nm. It can be seen there is absence of a dendrites shape in BZT powders compared with the BT powders. This can be ascribed to the effect of adding Zr+4 to BT, which make expand of lattice constants of it. TEM results The TEM images of as prepared BT powders synthesized at 150oC for 2h using hydrothermal method was demonstrated in Fig. 7. Fig. 7 revealed the spherical aggregates composed of 118 Proceeding of the First Scientific Conference on Nanotechnology , Advanced Materials and Their Applications2009 The SAED pattern taken from the Fig. 11a is shown in Fig. 11b, which reflect the regular spot and good crystallinity of BZT. Fig. 12 (b) shows the HRTEM image taken from Fig. 12 (a) of as prepared BZT2 powders. There is a contract variation which indicates the existence of strain inside the particles. The lattice fringes is close to the (110) lattice spacing of the cubic BZT. References: [1] Lee J. H., Nersisyan H. H., H.H. Lee and Won C. W., “Structural change of Hydrothermal BaTiO3 powders” J. Mater. Sci., 39, 1397, 2004. [2] Moura F., Simoes A. Z., B. Stojanovic D., Zagheta M. A., E. Longo and Varela J. A., “Dielectric and Ferroelectric Characteristics of BZT Ceramics prepared from Mixed Oxide Method” J. Alloys compound, 462, 129, 2008. Conclusion Fine crystalline barium zrogonate titanate BaZrxTi1-xO3 powders (where x=0, 0.001 and 0.008) were hydrothermally synthesized from mixing TiO2 and ZrO2 gels with aqueous Ba(OH)2 at 150oC for 2h. It is found that the expanded of lattice constant in BT, BZT1 and BZT2 due to existence of defects inside the lattice. Increase in Zr content, the tetragonality factor (c/a) decreased. Annealing powders shows that the phase transition was occurred, for BT at 700oC and for BZT higher than 700oC according to XRD results. The dendrites pattern is shown in TEM image of BT but it is not clear in BZT image. It is shown the different variations of HRTEM contract indicate the existence of high strain inside the lattice. Lattice fringes in HRTEM images revealed that the nanocrystalline BT and BZT have a uniform and perfect crystal structure with the existence of strains inside the lattice. The surrounding edges of these particles are not very smooth and some surface steps are observed. [3] Beauger A., Mutin J. C. and Niepce J. C., “Synthesis Reaction of Metatitanate BaTiO3” J. Mater. Sci., 18, 3543, 1983. [4] Pfaff G., “Sol-Gel Synthesis of Barium Titante Powders of Various Compositions” J. Mater. Chem., 2, 591, 1992. [5] Sven Van Gijp, Louis Winnubst and Henk Verweij, “Anoxalate Preoxide Complex used in the Preparation of Doped Barium Titanate” J. Mater. Chem., 8, 1251, 1998. [6] Bera J., and Savkar D., “Formation BaTiO3 from Barium Oxalate and TiO2” J. Electrocaerm., 11, 131, 2003. [7] Verekanandan R., Philip S. and Kutty T. R. N., “Hydrothermal Preparation of Ba(Ti, Zr)O3 Fine Powders” Mater. Res. Bull., 22, 99, 1986. 119 Proceeding of the First Scientific Conference on Nanotechnology , Advanced Materials and Their Applications2009 [8] Yonggang Wang, Gang Xu, Linlin Yang, Zhaohui Ren, Xiao Wei, Wenjian Weng, Piyi Du, Ge Shen and Gaorong Han, “Hydrothermal Synthesis of Single Crystal BaTiO3 Dendrites” Mater. Lett., 63, 239, 2009. [9] Changhua An, Chunying Liu, Shutao Wang and Yunqi Liu, “Generalized Large Scale Synthesis of MTiO3 (M=Ba, Sr, Pb) Nanocrystals” Mater. Res. Bull., 43, 932, 2008. [10] Tripathy S. K., Sahoo T., Mohapatra M., Anand S., and Das R. P., “XRD Studies on Hydrothermally Synthesized BaTiO3 from TiO2-Ba(OH)2NH3 System” Mater. Lett., 59, 3543, 2005. [11] Song Wei Lu, Burtrand I. Lee, Zhong Lin Wang and William D. Samuels, “Hydrothermal Synthesis and Structural Charactrization of BaTiO3 Nanocrystals” J. Crystal Growth, 219, 269, 2000. 121 Proceeding of the First Scientific Conference on Nanotechnology , Advanced Materials and Their Applications2009 180 160 140 BT 120 100 BZ 80 60 BT TiO2 BT 40 BZ BT BT BT BT BZ 20 BZ 0 -20 0 10 20 30 40 50 60 70 80 90 2 Fig. 1 XRD pattern of as prepared BZT using TiO2, ZrOCl2 and Ba(OH)2 hydrothermally treated at 150oC for 2h. 550 500 450 400 350 300 250 200 150 100 50 BZT2 BZT1 BT 0 -50 0 10 20 30 40 50 60 70 80 90 2 theta Fig. 2 XRD pattern of as prepared BT, BZT1 and BZT2 using TiO2 and ZrO2 gels with Ba(OH)2 hydrothermally treated at 150oC for 2h. 121 Proceeding of the First Scientific Conference on Nanotechnology , Advanced Materials and Their Applications2009 1600 1400 1 1200 2 1000 3 800 600 400 3 200 2 1 0 44.4 44.6 44.8 45.0 45.2 45.4 45.6 45.8 44.4 46.0 44.6 44.8 45.0 45.2 45.4 45.6 45.8 46.0 46.2 2 Theta 2 Theta (a) (b) 3 2 1 44.4 44.6 44.8 45.0 45.2 45.4 45.6 45.8 46.0 46.2 2 Theta (c) Fig. 3 XRD pattern at a limited range of 2 from 44.4 to 46o of a) BT, b) BZT1 and c)BZT2 at annealing temperature 1)500, 2) 700 and 3) 1000oC 122 Proceeding of the First Scientific Conference on Nanotechnology , Advanced Materials and Their Applications2009 4.030 4.025 lattice constant (a) lattice constant (c) 4.020 lattice constant (a) lattice constant (c) 4.028 4.026 4.024 4.022 4.015 lattice constant Lattice constant 4.020 4.010 4.005 4.000 3.995 4.018 4.016 4.014 4.012 4.010 4.008 4.006 4.004 3.990 4.002 4.000 3.985 3.998 0 200 400 600 800 0 1000 (a) lattice constants A 200 400 600 800 Temperature C Temperature C (b) 4.034 4.032 4.030 4.028 4.026 4.024 4.022 4.020 4.018 4.016 4.014 4.012 4.010 4.008 4.006 4.004 4.002 4.000 3.998 3.996 lattice constant (a) lattice constant (c) 0 200 400 600 800 1000 Temperature C (c) Fig. 4 Lattice constants with annealing temperature of a) BT, b) BZT1 and c) BZT2 123 1000 Proceeding of the First Scientific Conference on Nanotechnology , Advanced Materials and Their Applications2009 1.010 BT BZT1 BZT2 1.008 c/a 1.006 1.004 1.002 1.000 0 200 400 600 800 1000 Temperature C Fig. 5 Tetragonality factor (c/a) as a function of annealing temperature of BT, BZT1 and BZT2. 1.008 1.007 c/a 1.006 1.005 1.004 1.003 0.000 0.002 0.004 0.006 0.008 Zr content Fig. 6 Tetragonallity factor (c/a) as a function of Zr content at 1000oC. 124 Proceeding of the First Scientific Conference on Nanotechnology , Advanced Materials and Their Applications2009 (a) (b) Fig. 7 TEM images of as prepared BT powders (a) (b) Fig. 8 SAED image of as prepared BT powders 125 Proceeding of the First Scientific Conference on Nanotechnology , Advanced Materials and Their Applications2009 (a) (b) Fig. 9 HRTEM image of as prepared BT powders. (a) (b) Fig. 10 TEM images of as prepared BZT2 powders (a) (b) Fig.11 SAED image of as prepared BZT2 powders 126 Proceeding of the First Scientific Conference on Nanotechnology , Advanced Materials and Their Applications2009 (a) (b) Fig. 12 HRTEM image of as prepared BZT2 powders. 127
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