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Dielectric properties of Ba1-xSrxZrO3 (0 ≤ x ≤ 1) nanoceramics developed by citrate precursor route

Published online by Cambridge University Press:  03 April 2013

Omar A. Al-Hartomy*
Affiliation:
Department of Physics, Faculty of Science, University of Tabuk, Tabuk 71491, Saudi Arabia; and Department of Physics, Faculty of Science, King Abdulaziz University, Jeddah 21589, Saudi Arabia
Mohd Ubaidullah
Affiliation:
Department of Chemistry, Nanochemistry Laboratory, Jamia Millia Islamia, New Delhi 110025, India
Dinesh Kumar
Affiliation:
Department of Chemistry, Banasthali University, Tonk, Rajasthan 304022, India
Jamal H. Madani
Affiliation:
Department of Physics, Faculty of Science, University of Tabuk, Tabuk 71491, Saudi Arabia
Tokeer Ahmad*
Affiliation:
Department of Chemistry, Nanochemistry Laboratory, Jamia Millia Islamia, New Delhi 110025, India
*
a)Address all correspondence to these authors. e-mail: [email protected]
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Abstract

Nanosized oxides of barium strontium zirconate of general formula Ba1-xSrxZrO3 (0 ≤ x ≤ 1) have been prepared over the entire range of x for the first time by polymeric precursor route using citric acid and ethylene glycol. These solid solutions were investigated by means of powder x-ray diffraction, transmission electron microscopy, scanning electron microscope and Brunauer, Emmett and Teller surface area studies. X-ray diffraction studies reveal the monophasic nature of the powders at 1000 °C. The grain size was found to be in the range of 17–52 nm for all the oxides at 1000 °C. Specific surface area of these solid solutions comes out to be in the range of 49.1–94.4 m2/g. Smallest particle size with highest surface area has been achieved for x = 0.25 and comes out to be 17 nm and 94.4 m2/g respectively. Dielectric constant (ε) and dissipation factor (D) were investigated as a function of frequency and temperature. The room temperature dielectric constant of Ba1-xSrxZrO3 was found to be maximum 105 for x = 0.20 at 1 MHz.

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Articles
Copyright
Copyright © Materials Research Society 2013

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References

REFERENCES

Yang, L., Wang, Y., Wang, Y., Wang, X., Guo, X., and Han, G.: Synthesis of single-crystal Ba1−xSrxTiO3 (x = 0–1) dendrites via a simple hydrothermal method. J. Alloys Compd. 500, L1L5 (2010).Google Scholar
Hench, L.L. and West, L.K.: Principles of Electronic Ceramics (John Wiley & Sons Inc., New York, NY, 1990).Google Scholar
Zhang, Q. and Whatmore, R.W.: Sol–gel PZT and Mn-doped PZT thin films for pyroelectric applications. J. Phys. D: Appl. Phys. 34, 22962301 (2001).CrossRefGoogle Scholar
Guo, Y., Kakimoto, K.I., and Ohsato, H.: Phase transitional behavior and piezoelectric properties of (Na0.5K0.5)NbO3–LiNbO3 ceramics. Appl. Phys. Lett. 85(18), 41214123 (2004).Google Scholar
Ahmad, T. and Ganguli, A.K.: Structural and dielectric characterization of nanocrystalline (Ba, Pb)ZrO3 developed by reverse micellar synthesis. J. Am. Ceram. Soc. 89(10), 31403146 (2006).CrossRefGoogle Scholar
Shirpour, M., Rahmati, B., Sigle, W., van Aken, P.A., Merkle, R., and Maier, J.: Dopant segregation and space charge effects in proton-conducting BaZrO3 perovskites. J. Phys. Chem. C 116, 24532461 (2012).Google Scholar
Giannici, F., Shirpour, M., Longo, A., Martorana, A., Merkle, R., and Maier, J.: Long-range and short-range structure of proton-conducting Y: BaZrO3. Chem. Mater. 23, 29943002 (2011).Google Scholar
Pornprasertsuk, R., Yuwapattanawong, C., Permkittikul, S., and Tungtidtham, T.: Preparation of doped BaZrO3 and BaCeO3 from nanopowders. Int. J. Precis. Eng. Manuf. 13(10), 18131819 (2012).Google Scholar
Souza, E.C.C. and Muccillo, R.: Properties and applications of perovskite proton conductors. Mater. Res. 13(3), 385394 (2010).Google Scholar
Haile, S.M., Staneff, G., and Ryu, K.H.: Non-stoichiometry, grain boundary transport and chemical stability of proton conducting perovskites. J. Mater. Sci. 36, 11491160 (2001).Google Scholar
Erb, A., Walker, E., Genoud, J.Y., and Flukiger, R.: 10 years of crystal growth of the 123- and 124- high Tc superconductors: From Al2O3 to BaZrO3. Progress in crystal growth and sample quality and its impact on physics. Physica C 282287, 459460 (1997).Google Scholar
Howard, C.J., Knight, K.S., Kennedy, B.J., and Kisi, E.H.: The structural phase transitions in strontium zirconate revisited. J. Phys. Condens. Matter 12, L677L683 (2000).Google Scholar
Ahtee, A., Ahtee, M., Glazer, A.M., and Hewat, A.W.: The structure of orthorhombic SrZrO3 by neutron powder diffraction. Acta Crystallogr. B32, 32433246 (1976).Google Scholar
Garbhage, B., Marques, F.M.B., and Frade, J.R.: Electrochemical behaviour of SrZr1-xDyxO3-δ in atmospheres containing H2 and H2O. Electrochim. Acta 43, 26872692 (1998).Google Scholar
Journet, C., Maser, W.K., Bernier, P., Loiseau, A., Chapelle, M.L.D.L., Lefrant, S., Deniard, P., Lee, R., and Fischer, J.E.: Large-scale production of single-walled carbon nanotubes by the electric-arc technique. Nature 388, 756758 (1997).Google Scholar
Hwang, N.M. and Lee, D.K.W.: Charged nanoparticles in thin film and nanostructure growth by chemical vapour deposition. J. Phys. D: Appl. Phys. 43, 483001 (2010).Google Scholar
Kabashina, A.V. and Meunier, M.: Synthesis of colloidal nanoparticles during femtosecond laser ablation of gold in water. J. Appl. Phys. 94, 79417943 (2003).Google Scholar
Ganguly, A., Tring, P., Ramanujachary, K.V., Mugweru, A., Ahmad, T., and Ganguli, A.K.: Microemulsion-based synthesis of MgO nanoparticles(8-10 nm) and their catalytic properties. J. Colloid Interface Sci. 353, 137142 (2011).CrossRefGoogle Scholar
Ganguly, A., Ahmad, T., and Ganguli, A.K.: Silica mesostructures: Control of pore size and surface area using a surfactant-templated hydrothermal process. Langmuir 26(18), 1490114908 (2010).Google Scholar
Boopathy, K. and Rajendran, V.: Dielectric properties of Ba1-xSrxZrO3 (0 = x = 0.20). J. Metall. Mater. Sci. 49(4), 227235 (2007).Google Scholar
Pechini, M.P.: Method of preparing lead and alkaline earth titanates and niobates and coating method using the same to form a capacitor. U.S. Patent No. 330697, July 11, 1967.Google Scholar
Bernardi, M.I.B., Antonelli, E., Lourenco, A.B., Feitosa, C.A.C, Maia, L.J.Q., and Hernandes, A.C.: BaTi1–xZrxO3 nanopowders prepared by the modified Pechini method. J. Therm. Anal. Calorim. 87(3), 725730 (2007).CrossRefGoogle Scholar
Al-Hartomy, O., Ubaidullah, M., Khatoon, S., Madani, J., and Ahmad, T.: Synthesis, characterization and dielectric properties of nanocrystalline Ba1-xPbxZrO3 (0 ≤ x ≤ 0.75) by polymeric citrate precursor route. J. Mater. Res. 27(19), 24792488 (2012).CrossRefGoogle Scholar
Shannon, R.D.: Revised effective ionic radii and systematic studies of interatomic distances in halides and chalcogenides. Acta Crystallgr. A32, 751767 (1976).Google Scholar
Li, J.G., Ikegami, T., Wang, Y., and Mori, T.: 10-mol%-Gd2O3-Doped CeO2 solid solutions via carbonate coprecipitation: A comparative study. J. Am. Ceram. Soc. 86, 915921 (2003).Google Scholar
Wani, I.A., Khatoon, S., Ganguly, A., Ahmed, J., Ganguli, A.K., and Ahmad, T.: Silver nanoparticles: Large scale solvothermal synthesis and optical properties. Mater. Res. Bull. 45(8), 10331038 (2010).Google Scholar
Azam, A., Ahmad, A.S., Chaman, M., and Naqvi, A.H.: Investigation of electrical properties of Mn doped tin oxide nanoparticles using impedance spectroscopy. J. Appl. Phys. 108, 094329 (2010).CrossRefGoogle Scholar
Pokhral, B.P. and Pandey, D.: High temperature x-ray diffraction studies on antiferroelectric and ferroelectric phase transitions in (Pb1−xBax) ZrO3 (x=0.05, 0.10). J. Appl. Phys. 90, 29852994 (2001).Google Scholar