Heat treatments performed in the cylindrical samples.
The current progress in communication technologies is leading to extensive studies on the development of miniaturized electronic devices with high electromagnetic performances, reliability, and low cost. Contributing to this purpose, the development and study of new materials, with promising electric properties in radio and microwave ranges, have been subject of our research in particular niobate-based materials. Bismuth niobate, BiNbO4, is a low-firing ceramic that has been studied for a variety of applications in the microelectronic industry. In this work, the microwave dielectric characterization of (Bi1−x Fex )NbO4 (0.00 ≤ x ≤ 1.00) samples, prepared by the sol-gel method and heat treated at specific temperatures, is performed and related with their structure and morphology. The structural data were obtained by X-ray diffraction and Raman spectroscopy and the morphology by scanning electron microscopy. The dielectric characterization in the microwave region was made using the small perturbation theory, with a resonant cavity operating in TE105 mode, at the frequency of 2.7 GHz. The results show that the sol-gel method has the advantage of allowing the formation of α-BiNbO4 phase at lower temperatures when compared with conventional preparation methods, and that the inclusion of iron inhibits the formation of low- and high-temperature β-BiNbO4 phases.
- bismuth niobate
- X-ray diffraction
- dielectric properties
1. Introduction: state of the art
In the modern communication systems, where microwave frequencies are used, wireless equipment are indispensable . Therefore, the development of smaller, faster, and multifunctional equipment, with high electromagnetic performances and reliability, is an important technological challenge . Since this goal can be achieved using ceramics technology, in the last decades a lot of research has been devoted to the improvement of dielectric ceramic materials that can be sintered at low temperature .
Bismuth oxides are recognized as low temperature-cofired ceramics (LTCC) and are considered promising materials for applications in the microelectronic industry . In particular, bismuth niobate, BiNbO4, has been studied to be used as resonators and filters in satellite and mobile communication systems .
The sintering temperatures of these microwave dielectrics cannot be high, since they need to cofire with low-loss conductors and low melting point electrodes, such as copper, silver, and gold . Moreover, it is desirable that these ceramics have a high dielectric constant (
Bismuth niobate exists in two polymorph structures, an orthorhombic (α) phase (space group Pnna) and a triclinic (β) phase (space group P1).
Figure 1 shows the crystal structures of (a) α-BiNbO4 and (b) β-BiNbO4. There are four formula units in the unit cell in both structures. The α structure consists of layers of vertex-sharing NbO6 octahedra, which is normal to the
According to previous studies, the transition of low temperature β-BiNbO4 to α-BiNbO4 occurs at temperatures between 600 and 750°C, with the opposite, and supposed irreversible, transition occurring at 1020/1050°C [10, 11]. In 2007, Zhou et al.  reported the transformation from high temperature β-BiNbO4 to α-BiNbO4 in bulk samples; however, this transition is still considered irreversible in powder samples.
BiNbO4 ceramics can have low sintering temperature; however, they are difficult to densify without sintering aids . The first attempt to improve the bismuth niobate properties was developed by Kagata et al.  in 1992. They used V2O5 and CuO as additives, with the purpose of densifying the ceramic materials without compromising their dielectric properties. Since then, in order to obtain higher densification, better dielectric properties, and reduce the sintering temperature, various attempts have been undertaken to improve the bismuth niobate properties as a microwave dielectric ceramic . Besides the addition of different oxides, such as CuO , ZnO , V2O5 [14, 15], PbO, Bi2O3 , and Fe2O3 , several researchers tried to improve bismuth niobate properties through the substitution of bismuth for metals or lanthanides. In order to accomplish this task, (Bi1−
The solid-state reaction has been the most common method to process bismuth niobate [1, 7, 8], which means its benefits and drawbacks are already documented in the literature. BiNbO4 powders prepared by solid-state reaction result in high crystallinity, but not always in pure and homogeneous phases, because some metastable phases can be obtained under the same conditions . This method may cause other problems such as large grain growth, segregation of components, and loss of stoichiometry due to the volatilization of bismuth at a high temperature .
The wet-chemical techniques, such as co-precipitation, alkoxide and citrate sol-gel methods, and flux method, were found to present several advantages: nanosize particles, high reactivity, very good homogeneity in composition, and lower energy consumption, because they operate in mild temperatures. However, in these methods, metastable phases can also be formed [1, 7, 10].
Co-precipitation is considered one of the most successful techniques for the synthesis of ultrafine ceramic powders, having narrow particle size distribution. It is a less time-consuming method, since that can avoid complex steps such as refluxing of alkoxides. Nonetheless, an important drawback of co-precipitation is that all the cations should have similar solubility product [7, 10, 26].
The flux method is an alternative process that uses low-temperature liquid-phase reaction. According to previous studies, the BiNbO4 prepared by the flux method exhibits higher crystallinity than that obtained by solid-state reaction; however, the successful application of this method depends on a large number of factors, like eutectic temperatures and solubility of solid components in the eutectic melts. Besides that, the decrease of the sintering temperature is not always achieved, since a proper combination of material/dopant is needed. In some cases, the mechanical separation between product and flux can be difficult [27, 28].
The sol-gel method, through citrate route, is considered a simple way to obtain stable precursors and stoichiometric fine powders which have been employed in the production of various oxides. This method is considered promising for achieving high homogeneity, since the formation of citrate complexes allows mixing the component cations in an atomic scale, thus they can immediately react with each other at relatively low temperatures [10, 13, 25].
In this work, the microwave dielectric properties of (Bi1−
Since it is recognized that the dielectric properties can be related with density, porosity, and grain boundaries , the density of the samples was measured, using Archimedes method, and the morphology data was obtained by scanning electron microscopy (SEM).
2. Case study
2.1. Samples preparation
The obtained solutions were dried to evaporate the solvent: the solution of the reference sample,
2.2. Experimental methods
The structural characterization was performed using X-ray diffraction (XRD). The patterns data was obtained on a X’Pert MPD Philips diffractometer and on an Empyrean diffractometer (CuK α radiation,
Raman spectroscopy measurements were performed at room temperature, in backscattering geometry, with a 441.6 nm laser line using a HR-800-UV Jobin Yvon Horiba spectrometer. A microscope objective focused the exciting light onto the sample.
The ceramics bulk density was measured using the Archimedes method in reference to water.
The morphology of the sintered samples was analyzed by scanning electron microscopy (SEM), using a TESCAN-Vega III. The samples were covered with carbon before microscopic observation.
The measurement of the complex permittivity was made using the small perturbation theory, with a cavity operating in TE105 mode, at resonant frequency of 2.7 GHz. These measurements were made using a HP 8753D coupled to the cavity resonator.
Microwave resonant cavities have been used for evaluating the dielectric properties of geometrically defined samples, when the cavity is calibrated with dimensionally identical sample of known permittivity.
For a given cavity and a sample of regular shape and well-defined dimensions, it is possible to determine the permittivity of the material. The permittivity values of a sample can be obtained through the changes in the resonant frequency, Δ
The shift in the resonant frequency of the cavity, Δ
2.3. Results and discussion
The DTA data of the powders with
The powders with 0.25 ≤
The heat treatments were made in agreement with these results, as shown in Table 1.
|Treatment temperatures (°C)|
2.3.2. XRD pattern analysis
Analyzing the diffraction patterns shown in Figure 3(a), for the powders treated at 500°C, there are two secondary phases Bi2O3 and BiOCl, and the beginning of the β and α phases formation. The sample treated at 650°C is a combination of α- and β-BiNbO4 phases, with the secondary phase BiOCl still present. After the treatment of the samples at 850°C, the X-ray diffraction pattern shows the formation of pure orthorhombic BiNbO4 and, with a further temperature increase, this phase is converted to triclinic BiNbO4. For the highest treatment temperature, the volatile nature of Bi3+ ions, at elevated temperatures, promotes the formation of a non-stoichiometric phase of bismuth niobate, Bi3.54Nb7.09O22.7.
Therefore, the DTA exothermic band centered at 649°C can be due to the formation of α-BiNbO4, and the exothermic reaction occurring at 1043°C can be attributed to the conversion of α-BiNbO4 to β-BiNbO4. The thermal treatment at 1200°C promoted the fusion of the samples; consequently, there is no exact information about the exothermic phenomenon at 1181°C. However, the formation of a non-stoichiometric phase, due to the volatile nature of bismuth , is predictable.
In Figure 3(b), it is observed the formation of monoclinic FeNbO4, even at the lowest heat-treatment temperature. For the treatment temperatures from 500 to 1000°C, one additional phase was detected, Fe2O3, with a content equal or inferior at 5%. For the 1200°C heat treatment, single-phase FeNbO4 sample was obtained. Therefore, the DTA exothermic phenomena appearing at 747°C can be related with an improvement of the crystallization process of FeNbO4 and the phenomena visible at 1151°C can be attributed to the decomposition of the Fe2O3, and consequent formation of FeNbO4, with the niobium still present in the amorphous form. The increase of the amplitude and decrease of the half-width of the obtained XRD peaks, and of the Raman bands, shows that the increase of the heat treatment temperature promotes an increase of the crystallinity.
The samples with 0.25 ≤
|HT 500||HT 650||HT 800||HT 1100|
Confronting the X-ray diffraction data with the DTA, it is possible to assume that for the samples with
In the present study, one can conclude that the sol-gel method has the advantage of forming the orthorhombic BiNbO4 phase at even lower temperatures, since the sample with
2.3.3. Raman spectroscopy analysis
The Raman spectroscopy data of (Bi1−
In Figure 5(a), we can see that the Raman spectrum of the sample treated at 850°C, pure orthorhombic BiNbO4, is less complex than the spectra were the triclinic BiNbO4 is present. This result was expected since the lowered symmetry of the triclinic phase produces more Raman active modes . The samples treated at 500, 650, 1050, and 1150°C possess peaks at 102, 450, and 687 cm−1 attributed to the vibration modes of β-BiNbO4. This means that both low and high temperature β-BiNbO4 have identical vibration modes. In the sample treated at 850°C, where only α-BiNbO4 was detected, these peaks are absent. Furthermore, the peaks at 139 and 199 cm−1 are distinctive of the orthorhombic BiNbO4, which explains their absence in the spectra of the samples treated at 1050 and 1150°C. All the peaks present in these two samples are attributed to triclinic BiNbO4 [10, 34]. No vibration that can be assigned to non-stoichiometric phase Bi3.54Nb7.09O22.7 was detected.
In the spectra presented in Figure 5(b), all the detected bands are attributed vibrations of the base units of the monoclinic FeNbO4 phase. The Nb
The Raman spectroscopy data of (Bi1−
In the samples with
The bulk density values of (Bi1−
The bulk density increase with the treatment temperature increase is clearly visible for both the series of samples, and it allows to predict that porosity decreases at higher treatment temperatures.
The theoretical density of β-BiNbO4 ceramic (7.5 g/cm3) is higher than that of α-BiNbO4 ceramic (7.345 g/cm3) [21, 22]. Thus, and considering the samples with
Considering now the samples with
For the remaining samples, the evolution of the bulk density values with the treatment temperature is shown in Figure 8. In this case, we can see the same trend for this set of samples. The bulk density increases when the treatment temperature increases for 650°C, decreases for the treatment at 800°C, reaching a minimum value, and increases again with the higher treatment temperature. Regardless of the heat treatment, the samples with higher bulk density are the ones with
2.3.5. Morphological characterization
In Figure 9, SEM micrographs of the samples with
2.3.6. Microwave dielectric properties
In Figure 10 is presented the transmission results obtained with the 2.7 GHz cavity, for the cases of the cavity only with the sample holder, with the sample holder filled with PTFE and filled with the samples with 0.25 ≤ x ≤ 0.75, treated at 650°C. The expected shift in the resonant frequency of the cavity, Δ
Since this shift, Δ
Figure 11 shows the real and the imaginary parts of the complex permittivity at 2.7 GHz, as function of the treatment temperatures, for the samples with
For the samples with
Figure 11(b) shows that for the samples with
In Figure 12, it is presented the dielectric constant for the samples with 0.25 ≤
Table 3 resumes the calculated
|x||HT 500||HT 650||HT 800||HT 850||HT 1000||HT 1050||HT 1100||HT 1150||HT 1200|
We can conclude that the (Bi1−
Furthermore, the density of the obtained samples was very promising, since no additives were used in the host samples.
The substitution of bismuth by iron was successful, since the two non-stoichiometric phases, Bi1.34Fe0.66Nb1.34O6.35 and Bi1.721Fe1.056Nb1.134O7, were obtained. Moreover, one can conclude that the inclusion of iron inhibits the formation of low- and high-temperature triclinic bismuth niobate.
Concerning the dielectric characterization, the small perturbation technique proved to be very practical for dielectric measurements on ceramic materials, featuring important advantages, as the easy sample preparation, the absence of measurement contacts, and the simplicity of the calculations.
The dielectric study revealed that, for
With the inclusion of iron, the highest
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