CC BY
23
DIELECTRIC PROPERTIES OF AURIVILLIUS PHASE BiioFe6Ti3O3o WITH A NANO-SIZED PSEUDO-PEROVSKITE BLOCKS
N. A. Lomanova
Ioffe Institute, 26 Polytekhnicheskaya Str., Saint Petersburg 194021, Russia
natus@hotbox.ru
PACS 61.66.Fn
Distinctive features of dielectric properties of a ceramic material based on Aurivillius phase BiioFe6Ti3O3o have been studied.
Keywords: ceramics, Aurivillius phases, dielectric properties. Received: 20 November 2014 Revised: 3 December 2014
1. Introduction
In general, the structure of Aurivillius phases Bim+1Fem_3Ti3O3m+3 can be regarded as alternating fluorite-like layers F={(Bi2O2)2+}^ and pseudo-perovskite blocks P={(Bim+1 Fem _3Ti3O3TO+i)2 consisting of m pseudo-perovskite layers [1, 2]. According to experimental data from papers [3-5], the number of octahedral layers in a pseudo-perovskite block of Aurivillius phases Bim+1Fem_3Ti3O3m+3 may reach m=9, which corresponds to the compound Bi10Fe6Ti3O30. The thickness of the pseudo-perovskite block in this compound is ~3.7 nm [3]. In this context, the Bi2O3-TiO2-Fe2O3 system represents a unique object, since for the majority of layered pseudo-perovskite compounds, m cannot exceed 6 (E.g., see [6, 7]). The extremely high stability of compounds Bim+1Fem_3Ti3O3m+3 with a great number of pseudo-perovskite layers in the structure was analyzed in papers [4, 5, 8].
Following the data of papers [9-11], Aurivillius phases Bi2O3-TiO2-Fe2O3 possess mul-tiferroic properties. Compounds Bim+1Fem_3Ti3O3m+3 experience high-temperature phase conversion (Curie point) accompanied by transition from an orthorhombic structure to a tetragonal one [13-15], for Bi10Fe6Ti3O30, this occurs at 953 K [3, 16, 17].
Papers [3, 16] describe the preparation of Bi10Fe6Ti3O30 using solid-state chemical reactions. As shown in papers [4, 17], given the limiting value of m, multilayered Aurivillius phases will be in a state close to indifferent equilibrium. Such objects are of interest when regarded as transition nanostructures from a chemical compound to a heterogeneous system.
The study of the properties of Aurvillius phases with a great number of pseudo-like layers in the structure is of particular interest. The physical and chemical properties of compounds Bim+1Fem_3Ti3O3m+3, including Bi10Fe6Ti3O30, are described in papers [3-8, 16, 17]. Dielectric properties of some compounds Bim+1Fem_3Ti3O3m+3 are described in papers [15, 18-23], however, only papers [24, 25] provide a system-oriented approach.
This paper aims to study the nature of the electric relaxation for a ceramic material Bi10Fe6Ti3O30 using electric modulus formalism for analyzing dielectric data. Combined
with the data on composition and structure of the compound BiioFe6Ti3O30, the said research is required to forecast a possibility for preparing new multiferroic materials using that compound.
2. Experimental
For the synthesis of Bi10Fe6Ti3O30, solid-state chemical reactions were employed. The purity of initial reagents Bi2O3, TiO2 and Fe2O3 was 99.9% or higher. Papers [3, 26] describe the procedure in detail. Phase state was studied using the X-ray diffractometry (XRD) employing XRD-7000 Shimadzu. The elemental composition of the samples was determined by the energy dispersive X-ray microanalysis (FEI Quanta 200 SEM with the EDAX attachment).
Electrical measurements were taken for samples in tablet form, 7 mm in diameter, 3 mm thick, with platinum electrodes on the end face. Investigation was carried out in the open air using RCL-meter Fluke PM6063 (USA), within the temperature range 70-470°C, in the range f 10 kHz to 1MHz. Temperature was regulated using a tube furnace SNOL (Latvia) containing a double-pin cell with a sample. Toward that end, resistance R, module Z, and impedance phase shift angle p were measured, and these values subsequently served as a basis for the determination of real and imaginary parts of the complex electrical module M, complex specific conductivity a, complex dielectric permeability e and loss-angle tangent tg^=e"/e' according to the following ratios:
__c_
M = luso j Z = M' + jM", (1)
a = ~S~Z-1 = a' + jo", (2)
s = — ■ S-Z-1 = e' - js'', (3)
jSou S
where M' and M" are real and imaginary constituents of M; o7 and o " are real and imaginary constituents of e; u = 2nf is circular frequency, e0 is vacuum dielectric permeability, S and l are the sample area and thickness, correspondingly. The measuring procedure is described in papers [24, 25].
3. Results and discussion
Fig. 1 a, b present an X-ray diffraction pattern and a microstructure of a Bi10Fe6Ti3O30 sample, correspondingly. The data obtained testify to a single phase of the tested material and to good agreement between real chemical composition and stoichiometric one. At room temperature, Aurivillius phase has a rhombic elementary cell (space group D4h17-14/mmm), with parameters a=4.7 A, b=5.2 A, c=81.8 A.
The dielectric properties of Bi10Fe6Ti3O30 were studied using electric modulus formalism. Such an approach is informative for studying volumetric response from ceramic materials in a case when increased conductivity of a sample complicates analysis of dielectric relaxation processes [27, 28]. As shown in papers [24, 25], Aurivillius phases' conductivity will increase with an increase in the number of pseudo-perovskite layers in the structure.
Fig. 2 shows typical frequency dependencies for the overall specific electric conductivity oac(f) for Bi10Fe6Ti3O30 at different temperatures. This behavior reflects the interrelation between the relaxation process in charge carriers and conductivity in grain volume. The nature of the curves oac(f) corresponds to the "universal dynamic response" [29]:
Fig. 1. X-ray diffractograms ( A= 1.54056 A) (a) and electron micrographs (b) for BiioFeeTiaOsc
a(f ) = ^ + Afa, (4)
where adc - direct current specific conductivity, A- pre-exponential factor, f - frequency, a - an index denoting the degree of interrelation between charge carriers and crystal lattice (0<a<1).
For Aurivillius phases, this type of aac(f) dependency characterizes slow relaxation mechanisms for polarization and polaron "hopping" movement [20], for which a hop frequency (fp) between self-localization states corresponds to the change in the slope of oac(f) curves, it being <100 kHz at temperatures < 400°C. As the temperature rises, the curves enter a plateau phase.
Fig. 3 a, b represent frequency dependencies between a real (e7) and imaginary (e") constituent parts of complex dielectric permeability of the compound Bi10Fe6Ti3O30 at different temperatures. The e',e"(f) dependencies are given as smooth curves with a single peak at temperatures ^370°C, and with different dispersion in areas of low and high frequencies, increasing with increased temperature. Peaks of curves e7, e"(f) for temperatures exceeding 370°C are apparently beyond the frequency range of measurements. In the low frequency range, e7 values are reasonably high, while they sharply decrease when frequencies exceed 100 kHz. The e"(f) dependency is of a similar nature, however, at lower frequencies (< 100 kHz), its value is an order of magnitude greater, which points to conductivity contribution towards direct current [27, 31]. Within the low frequency range, a rise in temperature will cause extreme dispersion of dielectric permeability determined by the presence of thermally activated charges (e.g. volume charge, charged defects, etc.) [9].
Dielectric losses within the temperature range under consideration are relatively insignificant (loss tangent is tgp=e"/e' <0.15). Frequency dependencies of tg<p(f) are characterized by dispersion within the low frequency range, they sharply decrease at higher frequencies (Fig. 3c). Increased tgp values in the low frequency range testify to the presence
Fig. 2. Frequency dependence of the ac-conductivity Bi10Fe6Ti3O30
of direct current electric conductivity (adc) [31]. Dielectric losses will increase as temperature rises, which, apparently, are determined by recrystallization processes in the sample volume, or by reduced oxygen vacancies.
To analyze relaxation processes of the electric field, the frequency dependencies of the imaginary part of the electric module M" (f) was examined (Fig. 4a). At the temperatures specified, for dependencies M" (f), single peaks of the same height are recorded, which differ in the position with respect to the frequency axis. Their nature points to a single relaxation process in the sample volume and for an increase in electric conductivity with temperature rise. This is also proved by the nature of diagram M"-M' (Fig. 4b), represented by semicircles centered on the X-axis, which agrees with Debye relaxation [29]. As the temperature rises, peaks of the curves M"(f) will shift to higher frequencies. The frequency range below the peak will determine the range where the charge carriers are mobile at long distances, while the frequency range above the peak means that the carriers are in a "trap", in a potential pit, with mobility at short distances preserved. The frequency range, where peaks are recorded on the curves M" (f) are characterized by a change in the movement of charge carriers from long to short distances. In this case, the asymmetry of the peak, denoting relaxation processes with different time responses, is not observed [32].
According to the position of the high-frequency peak on the M"(f) curves, the relaxation time of dielectric polarization, tm = , was determined, with temperature dependence following the Arrhenius law:
TM = To exp
( AE
M
V kT
(5)
Fig. 3. Frequency dependence of the real, e7 (a) and imaginary, e"(b) parts of the dielectric permittivity (a, b) and dielectric, tgp, for Bi10Fe6Ti3O30, measured at various temperatures
where tm is relaxation time in the grain volume determined by the peak of the curves M"(f), t0 is a pre-exponential factor, EM is energy of activation of the charge carriers in the grain volume determined by the curve slope tm(1/T), k is Boltzmann constant, and T is absolute temperature.
The relaxation time t within the temperature range under consideration ranged from 5-10-4 —1-10-3 s. The activation energy EM of the charge carriers in the grain volume, estimated by ratio (5), was 0.8±0.1 eV, which is a typical value for compounds of Aurivillius phases type [18-25], with electric conductivity determined, primarily, by oxygen vacancy movement. The presence of oxygen vacancies in the structure of bismuth-containing Aurivillius phases is caused by the partial evaporation of Bi3+ ions under the high synthetic temperatures of these materials. This contributes to the overall electric conductivity, along
0.6 ' 400
- 450
/- kTu
Fig. 4. Frequency dependence of the imaginary part of the electric modulus, M" (a), and the M"-M' diagram (b) for Bi10Fe6Ti3O30 measured at various temperatures
with the phenomenon of hopping polarons between the Fe3+-O-Fe2+ positions at elevated temperatures [3, 26].
4. Conclusion
Based on the Aurivillius phase Bi10Fe6Ti3O30, distinctive features of dielectric behavior of a ceramic material prepared using solid-state chemical reactions have been studied. The presence of a single process of Debye-type dielectric relaxation in a bulk sample (EM=0.8±0.1 eV) has been shown.
Acknowledgments
The author would like to acknowledge Victor.V. Gusarov (Ioffe Institute) for his help in this work.
References
[1] Aurrivillius B. Mixed bismuth oxides with layer lattices. I. Ark. Kemi. 1(1), P. 463-471 (1949).
[2] Smolenskii G.A., Isupov V.A., Agranovskaya A.I. A New Group of Ferroelectrics (with Layered Structure) I. Fiz. Tverd. Tela., 1(1), P. 169-170 (1959).
[3] Lomanova N. A., Morozov M. I., Ugolkov V. L., Gusarov V. V. Properties of Aurivillius phases in the Bi4Ti3Oi2-BiFeO3 system. Russ. J. Inorganic Materials, 42(2), P. 189-195 (2006).
[4] Lomanova N.A., Gusarov V.V. On the limiting thickness of the perovskite-like block in the Aurivillius phases in the Bi2O3-TiO2-Fe2O3 system. Nanosystems: physics, chemistry, mathematics, 2(3), P. 93101 (2011).
[5] Lomanova N.A., Semenov V.G., Panchuk V.V., Gusarov V.V. Structural features and stability of the Aurivillius phases Bin+1Fen-3Ti3O3n+3. Dokl. Chem., 447(2), P. 293-295 (2012).
[6] Yu W. J., Kim Y. I., Ha D. H., Lee J. H., Park Y. K., Seong S., Hur N. H. A new manganese oxide with the Aurivillius structure: Bi2Sr2Nb2MnO12—. Solid State Commun, 111(12), P. 705-709 (1999).
[7] Miyayama M., Yi I.-S. Electrical anisotropy in single crystals of Bi-layer structured ferroelectrics. Ceramics International, 26, P. 529-533 (2000).
[8] Lomanova N.A., Semenov V.G., Panchuk V.V., Gusarov V.V. Structural changes in the homologous series of the Aurivillius phases Bin+1Fe„_3Ti3O3n+3. J. Alloys and Compounds., 528, P. 103-108 (2012).
[9] Bai W., Chen G., Zhu J. Y., Yang J., Lin T., Meng X.J., Tang X.D., Duan C.G., Chu J.H. Dielectric responses and scaling behaviors in Aurivillius Bi6Ti3Fe2O18 multiferroic thin films. Appl. Phys. Lett. 100(8), P. 082902-082906 (2012).
10] Jiang P.P., Zhang X.L., Chang P., Hu Z. G., Bai W., W. Li Y., Chu J.H. Spin-phonon interactions of multiferroic Bi4Ti3O12-BiFeO3 ceramics: Low-temperature Raman scattering and infrared reflectance spectra investigations. J. Appl. Phys., 115, P. 144101-144106 (2014).
11] Keeney L., Maity T., Schmidt M., Amann A., Deepak N., Petkov N., Roy S., Pemble M. E., Whatmore R. W. J. Am. Ceram. Soc., 96(8), P. 2339-2357 (2013).
12] Isupov V.A. Curie Temperatures of Am-1Bi2MmO3m+3 layered ferroelectrics Russ. J. Neorg. Mater., 33(9), . 1106-1110 (1997).
13] Snedden A., Hervoches Ch. H., Lightfoot Ph. Ferroelectric phase transition in SrBi2Nb2O9 and Bi15Ti3FeO15: a powder neutron diffraction study. Phys. Rew., 67, P. 092102 (2003).
14] Krzhizhanovskya M., Filatov S., Gusarov V., Paufler P., Bubnova R., Morozov M., Meyer D. C. Aurivillius phases in the Bi4Ti3O12/BiFeO3 system: thermal behaviour and crystal structure. Z. Anorg. Allg. Chem., 631, P. 1603-1608 (2005).
15] Subbanna G.N., Guru Row T.N., Rao C.N.R. Structure and dielectric properties of recurrent inter-growth structures formed by the Aurivillius family of bismuth oxides of the formula Bi2 An-1BnO3n+3. J. Solid State Chem., 86(2), P. 206-211 (1990).
16] Lomanova N.A., Ugolkov V. L., Gusarov V. V. Thermal behavior of layered perovskite-like compounds in the Bi4Ti3O12-BiFeO3 system. Glass Physics and Chemistry, 33, P. 608-612 (2007).
17] Lomanova N.A., Gusarov V.V. Phase states in the Bi4Ti3O12-BiFeO3 section in the Bi2O3-TiO2-Fe2O3 system. Russ. J. Inorg. Chem., 56, P. 616-620 (2011).
18] Srinivas A., Kumar M., Suryanarayana S.V., Bhimasankaram T. Investigation of dielectric and magnetic nature of Bi7Fe3Ti3O21. Mater. Res. Bull., 34(6), P. 989-996 (1999).
19] Srinivas A., Kima Dong-Wan, Honga Kug Sun, Suryanarayana S.V. Study of magnetic and magneto-electric measurements in bismuth iron titanate ceramic-Bi8Fe4Ti3O24. Mater. Res. Bull., 39, P. 55-61 (2004).
20] Srinivas K., Sarah P., Suryanarayana S.V. Impedance spectroscopy study of polycrystalline Bi6Fe2Ti3O18, Bull. Mater. Sci., 26(2), P. 247-253 (2003).
21] Bucko M. M., Polnar J., Kozielski L. Dielectric Properties of Some Aurivillius Phases in the Bi4Ti3O12-BiFeO3 System. Materials Science Forum., 730, P. 88-93 (2013).
22] Patwe S. J., Achary S. N., Manjanna J., Tyagi A. K., Deshpande S. K., Mishra S. K., Krishna P. S. R., Shinde A. B. Observation of a new cryogenic temperature dielectric relaxation in multiferroic Bi7Fe3Ti3O21. Appl. Phys. Lett., 103, P. 12290-112296 (2013).
23] Dercz J., Starczewska A., Dercz G. Dielectric and structural properties of Bi5Ti3FeO15 ceramics obtained by solid-state reaction process from mechanically activated precursors. Int. J. Thermophys., 32, P. 746-761 (2011).
24] Lomanova N.A., Gusarov V.V. Electrical properties of perovskite-like compounds in the Bi2O3-TiO2-Fe2O3 system. Russ. J. Inorg. Mater., 47, P. 420-425 (2011).
25] Lomanova N.A., Gusarov V.V. Impedance spectroscopy of polycrystalline materials based on the Aurivillius phase system Bi4Ti3O12-BiFeO3. Nanosystems: physics, chemistry, mathematics, 3, P. 112-122 (2012).
26] Morozov M. I., Gusarov V.V. Synthesis of Am-1Bi2MmO3m+3 compounds in the Bi4Ti3O12-BiFeO3 system. Russ. J. Inorg. Mat., 38, P. 723-729 (2002).
27] Molak A., Paluch M., Pawlus S., Klimontko J., Ujma Z., Gruszka I. Electric modulus approach to the analysis of electric relaxation in highly conducting (Na0.75Bi0 25)(Mn0 25Nb0.75)O3 ceramics. J. Phys. D: Appl. Phys., 38, P. 1450-1460 (2005).
28] Yi Z. G., Li Y. X., Wang Y., Yin Q. R. Spectroscopies of mixed-layer Aurivillius phase Bi5Ti15W15O15 dielectric, impedance, and electric modulus. J. Electrochem. Soc., 153(6), P. F100-F105 (2006).
29] Jonscher A.K. The 'universal' dielectric response. Nature, 267, P. 673-679 (1977).
30] Jonscher A.K. Dielectric relaxation in solids. J. Phys. D: Appl. Phys., 32, P. R57-R70 (1999).
31] Gerhardt R. Impedance and dielectric spectroscopy revisited: Distinguishing localized relaxation from long-range conductivity. J. Phys. Chem. Solids., 55, P. 1491-1506 (1994).
[32] Pattanayak S., Parida B.N., Das P. R., Choudhary R.N.P. Impedance spectroscopy of Gd-doped BiFeO3 multiferroics. Appl.Phys. A., 112, P. 387-395 (2013).
