Influence of BaTiO3 nanoparticles/clusters on the structural and dielectric properties of glasses-nanocomposites

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Abstract

Glass nanocomposite (GNCs) samples in the composition [(90-x) Li2B4O7- xBaTiO3- 10Nb2O5] with x = 5, 7.5, 10, 12.5 and 15 (in mol%) were prepared. Rietveld refinement of the data for the reagent grade of the BaTiO3 revealed that the structure is a tetragonal phase (space group P4mm). The energy dispersive X-Ray (EDX) spectra and scanning electron microscopic (SEM) micrographs exhibit the two phases (BaTiO3 nanopatricles/clusters phase and residual glass phase) of the GNCs samples. The BaTiO3 nanoparticles/clusters in the glass matrix were confirmed by transmission electron microscopic (TEM) and Fourier transform infrared (FTIR) studies. The deconvolution of the FTIR spectra of the GNCs samples reveals the presence of BO3, BO4, NbO4 and NbO6 units. The dielectric results exhibit the ferroelectric of BaTiO3 nanoparticles/clusters in the GNCs samples at x = 10, 12.5 and 15 mol%. The dielectric constant, dielectric loss and ac conductivity for the GNCs samples as a function of temperature at various frequencies in 120Hz−100 k Hz range have been studied.

Introduction

In recent years, BaTiO3 nanoparticles/clusters embedded in the glass matrix (the so called GNCs) have attracted much attention due to their promising technological properties and relatively easy preparation method [[1], [2], [3]]. These GNCs exhibit mixed properties for the two components, BaTiO3 nanoparticles and host glass matrix, such as ferroelectric and high dielectric which are used to develop modern electronics [1,2,4]. BaTiO3 nanoparticles/clusters in the GNCs samples can be prepared by conventional melt quenching method in many reports [[4], [5], [6]]. Moreover, these samples undergo structural phase transitions as a function of temperature; therefore the GNCs can be used in capacitors, piezoelectric transducers, etc [1,7]. BaTiO3 in polycrystalline has three phase transitions with the decrease in the temperature from a cubic phase (space group Pm3 m) to a tetragonal phase (space group P4mm), then to an orthorhombic phase (space group Amm2) and to a rhombohedral phase (space group R3m) at 403, 278 and 183 K, respectively [8,9]. The glass forming ability of BaTiO3 is weak and its melting temperature is high (1898 K) so to obtain GNCs containing BaTiO3 nanoparticles/clusters, it is required to add a host glass matrix such as lithium tetraborate (Li2B4O7) [2,5,10]. Abdel-Khalek et al. [2,3] studied the structural and dielectric properties of high concentration of BaTiO3 embedded in Li2B4O7 glass matrix [(100-x) Li2B4O7- xBaTiO3] with x = 0, 20 and 60 mol%. They found that the GNCs containing BaTiO3 nanoparticles exhibited dielectric anomalies (ferroelectric nature). The addition of Nb2O5 oxide into the glass composition led to the change in the structure and physical properties such as electrical and dielectric constant. The change in the structure due to Nb2O5 which acts as an intermediate, one as a glass former with NbO4 in Nb4+ (glass is blue) and other as a glass modifier with NbO6 in Nb5+ (glass is yellow) [11,12]. The change in the electrical and dielectric constant is due to Nb2O5 ions which have high polarizability and the change in the glass network (NbO4 and NbO6) [13]. Moreover, the volume of nonbridging oxygens (NBOs) sites formed by the addition of Nb2O5 into the glass network is larger than that formed by alkaline earth [11]. Wang et al. [14] studied the structure of niobium alkali borate glass. They found that the glass structural units are NbO6, BO3 and BO4. Sanghi et al. [11] studied the influence of Nb2O5 on the structural, optical and electrical properties of alkaline earth borate glasses [xNb2O5- (30-x) MO- 70B2O3] where M = Ca, Sr and Ba with 0 ≤ x ≤ 12 mol%. They found that from the IR spectra the presence of NbO4 and NbO6 units for Ca and Sr and NbO6 units for Ba glasses. The conductivity results show that the conductivity is varying with the concentration of Nb2O5 (up to 8 and for Nb2O5 ≥ 8 mol %) and depend on the presence of NbO4 and NbO6 units in these glasses which support by the IR analysis. In view of the aforementioned aspects, we reported the ferroelectricity of tetragonal BaTiO3 nanoparticles/clusters in GNCs at a low concentration of BaTiO3 in the presence of Nb2O5 compared to previous studies [2,3]. In the present work, we study the influence of BaTiO3 nanopatricles/clusters on the structural and dielectric properties of [(90-x) Li2B4O7- x BaTiO3-10 Nb2O5] (where x = 5, 7.5, 10, 12.5 and 15 (in mol %)) GNCs samples.

Section snippets

Samples preparation

The GNCs samples in the composition [(90-x) Li2B4O7- x BaTiO3- 10 Nb2O5] with x = 5, 7.5, 10, 12.5 and 15 (in mol %) were prepared by the melt quenching method. All the present compositions were prepared by using the amount of reagent grade Li2B4O7 (99.99%), Nb2O5 (99.2%) and BaTiO3 (99.99%). The mixed batches were melted well in porcelain crucible at 1373 K for one hour in an electric muffle furnace and quenched on a copper plate.

Samples characterization

The amorphous nature of the GNCs samples and the structure of

XRD, EDX, SEM and TEM

XRD patterns for the GNCs samples as a function of BaTiO3 are shown in Fig. 1(a). It is evident from the figure that XRD patterns exhibit a broad hump without any diffraction lines of crystalline phase thus clearly reveals the glassy character of all the present samples. Fig. 1(b) shows the XRD pattern for the reagent grade of the BaTiO3. It is evident from the figure that the BaTiO3 is a single phase without any impurities peaks. Rietveld refinement of the data (Fig. 1(b)) revealed that the

Conclusions

GNCs containing BaTiO3 nanoparticles/clusters have been successfully prepared. The existence of BaTiO3 nanoparticles/clusters in the glassy matrices (GNCs) has been confirmed by EDX, SEM, TEM, and FTIR studies. The ferroelectric nature of BaTiO3 nanoparticles/clusters in the GNCs samples at x = 10, 12.5 and 15 mol% has been deduced from the dielectric constant study. In the vicinity of Curie temperature (TC) in the GNCs samples, dielectric loss and ac conductivity exhibit anomalous behavior.

CRediT authorship contribution statement

E.A. Mohamed: Investigation, Formal analysis, Supervision, Writing - original draft, Writing - review & editing. E. Nabhan: Investigation, Supervision, Writing - original draft. A. Ratep: Investigation, Supervision, Writing - original draft. F.M. Hassan: Investigation, Methodology, Data curation, Formal analysis, Writing - original draft. K. Tahoon: Investigation, Supervision, Writing - original draft.

Acknowledgments

The authors are grateful to Professor M. Y. Hassaan for allowing the measurement of the dielectric.

References (51)

  • N.A. Szreder et al.

    J. Non-Cryst. Solids

    (2014)
  • E.K. Abdel-Khalek et al.

    Mater. Chem. Phys.

    (2012)
  • V. Thakur et al.

    Ceram. Int.

    (2015)
  • E.K. Abdel-Khalek et al.

    J. Non-Cryst. Solids

    (2014)
  • R. Harizanova et al.

    J. Non-Cryst. Solids

    (2014)
  • R. Ma et al.

    J. Alloys Compd.

    (2017)
  • C.J. Xiao et al.

    Mater. Chem. Phys.

    (2008)
  • S. Sanghi et al.

    Mater. Chem. Phys.

    (2010)
  • Y. Attafi et al.

    J. Non-Cryst. Solids

    (2016)
  • M. Muralidhar et al.

    Physica C

    (2009)
  • E.K. Abdel-Khalek et al.

    Phys. B

    (2018)
  • A. Bajaj et al.

    J. Non-Cryst. Solids

    (2009)
  • M.R. Reddy et al.

    J. Phys. Chem. Solid.

    (2000)
  • I.S. Yahia et al.

    J. Magn. Magn Mater.

    (2009)
  • Y.B. Saddeek et al.

    Mater. Chem. Phys.

    (2009)
  • G. Lakshminarayana et al.

    Spectrochim. Acta

    (2006)
  • I. Ardelean et al.

    Mater. Lett.

    (2004)
  • V. Naresh et al.

    Ceram. Int.

    (2012)
  • R.T. Karunakaran et al.

    Solid State Sci.

    (2009)
  • N. Syam Prasad et al.

    Mater. Sci. Eng. B

    (2002)
  • K. Suzuki et al.

    J. Alloys Compd.

    (2006)
  • O. Cozar et al.

    J. Mol. Struct.

    (2001)
  • E.K. Abdel-Khalek et al.

    J. Non-Cryst. Solids

    (2018)
  • A. Wagh et al.

    Trans. Nonferrous Metals Soc. China

    (2015)
  • A. Mogus-Milankovic et al.

    J. Non-Cryst. Solids

    (2007)
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