Elsevier

Journal of Alloys and Compounds

Volume 587, 25 February 2014, Pages 553-559
Journal of Alloys and Compounds

Synthesis, structural characterization and dielectric properties of Nb doped BaTiO3/SiO2 core–shell heterostructure

https://doi.org/10.1016/j.jallcom.2013.10.228Get rights and content

Highlights

  • Optimal parameters for preparation by sol–gel of core–shell (BT-Nb0.005)/SiO2 are presented in this paper.

  • Single crystalline BT-Nb0.005/SiO2 core–shell composite with ∼34 nm shell thick was prepared.

  • The core–shell ceramic exhibits good dielectric properties and ferroelectric characteristics.

Abstract

Perovskite complex ceramic oxides, BaTiO3 doped with 0.5 mol%Nb2O5 and then nanocoated with SiO2 (abbreviated as BT-Nb0.005/SiO2) was successful prepared using conventional sol–gel processing. Phase composition, particle morphology, structure, and electric properties of BT-Nb0.005 core and BT-Nb0.005/SiO2 core–shell were examined and compared, using X-ray diffraction, transmission electron microscopy and, dielectric and ferroelectric measurements. Core–shell composite with well-defined perovskite tetragonal phase of BaTiO3 was achieved. Furthermore, single crystalline BT-Nb0.005/SiO2 core–nanoshell heterostructure with ∼34 nm shell thick was prepared, which is a novelty in ferroelectrics field. The ferroelectric quality of BT-Nb0.005 has suffered an alteration when the (BT-Nb0.005)/SiO2 core–shell heterostructure was realized. One-dimensional BT-Nb0.005/SiO2 core–shell heterostructure exhibits an improvement of dielectric losses and a decrease of dielectric constant, compared to uncoated BT-Nb0.005. The (BT-Nb0.005)/SiO2 core–shell material could be interesting for application in the composite capacitors.

Introduction

Barium titanate (BaTiO3) is extensively investigated because it is chemically stable, exhibits good ferroelectric and dielectric properties in the frequency range 100 Hz–1 MHz. Based on these characteristics, BaTiO3 has applications in high performance capacitors, multilayer capacitors, energy storage devices and thermistors [1], [2], [3], [4], [5], [6], [7]. Very interesting properties for various applications of barium titanate can be obtained by adding dopants and by an appropriate modification of the grains and grain boundary characteristics due to the recent developments in synthesis of materials [7]. Many rare earth oxides are used as dopants in order to modify the Curie point temperature and to improve the electrical characteristics of the capacitors by controlling the microstructure and the grain size of BaTiO3 [7], [8], [9], [10], [11], [12], [13]. It is known that BaTiO3 can be doped with donors like the trivalent ions (e.g. yttrium, europium, lanthanum) on Ba-ion sites or a pentavalent ions (e.g. niobium, tantalum) on Ti-ion sites [11], [12], [13], [14]. There are several reports on the doping BaTiO3 with niobium [7], [8], [9], [15], [16], [17], [18], [19]. The phase composition, microstructure and dielectric properties of BaTiO3 show a strong dependence on the amount of added niobium [7]. We have chosen a concentration of Nb of 0.5 at% because it found that the dielectric constant of Nb-doped BaTiO3 increase with the increase of niobium concentration from 0.4 to 0.6 mol%, in the presence of a small amount of manganese (0.01 mol%Nb5+) as acceptor dopant [7]. There are substantial discrepancies in reported properties of Nb-doped BaTiO3 [20], [21], [22], [23]. The differences are due to a slow rate of Nb incorporation into the BaTiO3 lattice [24] and the temperature range at which the processing is effective [25]. It was found that at temperatures lower than 1225 °C, Nb cannot be incorporated into the BaTiO3 lattice due to kinetic reason [25]. Niobium has a significant effect on densification and microstructure evolution of BaTiO3 [7]. It was reported that small concentrations of niobium (<0.06 mol%Nb) enhance grain growth, while above this limit it inhibits the grain growth of barium titanate [26], [27].

The dielectric characteristics (especially dielectric losses) of ferroelectric materials can be improved also by coating the ferroelectric grain with an insulating material with low dielectric loss, i.e. Al2O3, SiO2, MgO, Ta2O5 [1], [28], [29], [30], [31], [32]. Coating the ferroelectric particles with amorphous silica is often the first choice for the assembly process since dense-coating of amorphous silica improves the chemical stability and reduces the growth rate of the core particles in the fabricating process [33], [34]. Generally, the grains with core–shell architecture combine diverse functionalities into a single hybrid composite and show improved or new physical properties over their single-component counterparts. Core–shell particles can be used for the fabrication of dense dielectric, ferroelectric and multiferroic composites with 3–0 connectivity or ceramics with controlled composition and property gradients at the level of the single grains [35].

In this work we used a colloidal chemistry method (sol–gel) in order to prepare BaNb0.005Ti0.995O3 coated with SiO2 (abbreviated as BT-Nb0.005/SiO2). The dielectric behaviour of BT-Nb0.005/SiO2 core–shell was studied and compared with that of the BT-Nb0.005 base material. The sintering behavior of SiO2 shell was investigated also in this paper.

Section snippets

Samples preparation

Barium titanate BaTiO3 doped with 0.5 mol%Nb was prepared by solid state reaction method from BaTiO3 to Nb2O5. Firstly, BaTiO3 was synthesized by sol–gel technique starting from barium acetate, 99%, [Ba(CH3COO)2] (Aldrich) and titanium (IV) isopropoxide, 97% solution in 2-propanol [Ti{OCH(CH3)2}4] (Aldrich). Barium acetate was firstly dissociated in water to obtain a concentrated solution (1 M). Acetic acid glacial was added to the barium acetate solution, in molar ratio 2:1. Propanol-2 and

X-ray diffraction

BT-Nb0.005 powder, crystallized on the tetragonal lattice of BaTiO3, (Pattern 81-2202) [40], was obtained by firing the mixture of the appropriate proportions of BaTiO3 and Nb2O5 at 1300 °C, for 3 h in air (Fig. 1(a)).

The tetragonal BaTiO3 structure of BT-Nb0.005 powder is indicated by the splitting of cubic peak (200) corresponding to 2θ = 45.235° (Pattern 79-2263) [41] in the two tetragonal peaks (0 0 2) and (2 0 0) centered at 2θ = 44.887° and 2θ = 45.359°, respectively (Pattern 81–2202) [40]. X-ray

Conclusions

Core–shell structured (BT-Nb0.005)/SiO2 particles have been prepared via sol–gel technique. A comparative dielectric characterization of pure BT-Nb0.005 and coated BT-Nb0.005 particles with SiO2 nanoshell (∼34 nm thick) has carried out. (BT-Nb0.005)/SiO2 core–shell composite exhibits smaller dielectric constant which can be explained by weaker densification due to SiO2 shell, smaller dissipation factor and higher temperature of Curie point compared to uncoated BT-Nb0.005. Both dielectric

Acknowledgement

The authors gratefully acknowledge the Romanian Ministry of Education and Research, Project: NUCLEU PN09-450101, Contract No.: 45 N/1.03.2009; Act ad. 2/2013, for financial support.

References (43)

  • J. Kim et al.

    Mater. Sci. Eng. B

    (2011)
  • T. Hiramatsu et al.

    Mater. Sci. Eng. B

    (2005)
  • L.Y. Li et al.

    Mater. Chem. Phys.

    (2009)
  • X.K. Wei et al.

    J. Alloys Comp.

    (2010)
  • S. Fuentes et al.

    J. Alloys Comp.

    (2013)
  • M. Ganguly et al.

    J. Alloys Comp.

    (2013)
  • K. Kowalski et al.

    J. Phys. Chem. Solids

    (2001)
  • I.A. Velasco-Davalos et al.

    J. Alloys Comp.

    (2013)
  • G.H. Jonker et al.

    Mater. Res. Bull.

    (1982)
  • J. Nowotny et al.

    Ceram. Int.

    (1994)
  • B. Stojanovic et al.

    J. Eur. Ceram. Soc.

    (1999)
  • T. Li et al.

    Mater. Lett.

    (2000)
  • N. Wada et al.

    Ceram. Int.

    (2008)
  • G. Pigozzi et al.

    J. Alloys Comp.

    (2014)
  • N. Yin et al.

    J. Alloys Comp.

    (2013)
  • W. Stöber et al.

    J. Colloid Interface Sci.

    (1968)
  • J. Wagner et al.

    J. Magn. Magn. Mater.

    (2002)
  • G.H. Bogush et al.

    J. Colloid Interface Sci.

    (1991)
  • M.C. Wang et al.

    J. Cryst. Growth

    (2002)
  • S. Yanez-Vilar et al.

    Nanotechnology

    (2006)
  • D.I. Woodward et al.

    Appl. Phys. Lett.

    (2004)
  • Cited by (0)

    View full text