Improved dielectric properties of BaxSr1−xTiO3-based composite ceramics derived from core–shell structured nanopowders
Introduction
BaxSr1−xTiO3 (BST) has been considered to be an important material for tunable phase shifters, tunable filters, and high-Q resonators for radar and communication applications because of its large field tunability and variable Curie temperature [1], [2], [3], [4], [5], [6]. The Curie temperature of BST can be controlled by adjusting the ratio of Ba/Sr and/or doping ions to substitute for A or B sites in the ABO3 perovskite systems. The dielectric constants as well as dielectric loss are usually lower in the paraelectric phases than in the ferroelectric phases, owing to the disappearance of hysteresis. In microwave device applications, the optimum materials should have moderate dielectric constant (ɛ), large tunability, a low loss dissipation factor (tan δ), and low temperature dependence of ɛ. Thus far, composite materials, including ferroelectric BST phases and non-ferroelectric oxides with a low loss (MgO, Al2O3, etc.), have attracted considerable attention [7], [8], [9], [10], [11].
The hydrothermal process is one of the commonly used methods for preparing nanoscaled powders because of its low synthesis temperature, low equipment cost and simple synthesis procedures. Qi et al. developed a new and simple method of directly synthesizing nano-BaTiO3 powders from solution at 60 °C with an average particle size of about 25 nm [12]. A process for fabricating the core–shell MgO-wrapped–BST (BST–MgO) nanopowders, with a grain size close to 17–20 nm, was developed in our previous work [13]. Nanoscaled BST powders were used as the core materials and the core–shell structure was formed by a chemical solution method, by adding magnesium nitrate solution into the BST dispersed base solution by an ultrasonic process.
In the conventional composite, the sintering characteristics usually depend on the easily sintered phase: e.g. in the MgO–BST system, BST can be easily sintered at much lower temperatures than MgO. In MgO-wrapped–BST, however, the sintering behavior was dominated by MgO, making sintering difficult for BST. Some modifications were made in order to solve this difficulty in sintering. In this work, easily sintered Mg0.9Zn0.1O2 (MZO) shell material was used as a substitute for MgO, and a two-step synthesis processing was employed to obtain BST nanopowder uniformly wrapped with Mg0.9Zn0.1O (BST–MZO). The core–shell structure of BST nanoparticles wrapped with zinc doped MgO was also analyzed and confirmed elsewhere [14].
Section snippets
Experimental
Barium hydroxide octahydrate (Ba(OH)2·8H2O), strontium hydroxide octahydrate (Sr(OH)2·8H2O), and tetrabutyl titanate (Ti(OC4H9)4) were used as starting materials. The nanoscaled BST powder was dispersed in ethanol by ball-grinding for 2 h. Detailed information about the synthesis of BST powder can be found elsewhere [13]. Deionized water was then added to magnesium nitrate hexahydrate (Mg(NO3)2·6H2O) and zinc nitrate hexahydrate (Zn(NO3)2·6H2O) in the stoichiometric Mg/Zn ratio of 0.9/0.1. The
Results and discussion
Fig. 1 shows the XRD patterns of (a) as-prepared BST50, (b) 500 °C dried BST50–40%MZO, and (c) BST50–40%MZO ceramic sintered at 1350 °C for 2 h. XRD investigations have shown that the as-precipitated BST powder is crystallized in a single perovskite phase (Ba0.5Sr0.5TiO3), as shown in Fig. 1(a). No other phases, such as BaO, SrO, and TiO2 have been detected except for a weak peak of (Ba,Sr)CO3. BaCO3 was also found in the nano-BST powder prepared using the DSS method [13]. The peak from (Ba,Sr)CO3
Conclusions
Using nanoscaled BST powder as a starting material, core–shell structured nanopowder was formed by wrapping BST with a non-ferroelectric oxide derived from a chemical solution route under ultrasonic dispersion at room temperature. BST–MZO composite ceramics were then sintered using the core–shell structured nanopowders. The Curie temperatures of BST–MZO composite ceramics shifted to a lower temperature compared with pure BST ceramics. The dielectric constant and loss decreased sharply depending
Acknowledgments
This research was supported by the postdoctoral fellowship program (G-YX03 and G-YX12) of The Hong Kong Polytechnic University.
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