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NANOSYSTEMS: PHYSICS, CHEMISTRY, MATHEMATICS, 2016, 7 (4), P. 599-603
Dielectric studies of nanocrystalline calcium tungstate
N. Aloysius1*, M. S. Rintu2, E. M. Muhammed2, T. Varghese1'3
1 Department of Physics, Newman College Thodupuzha-685 585, Kerala, India
(Affiliated to M. G. University, Kottayam) 2Department of Physics, Maharajas College, Ernakulam-682 011, Kerala, India 3Nanoscience Research Centre (NSRC), Department of Physics, Nirmala College, Muvattupuzha - 686 661, Kerala, India
PACS 78.67.Bf, 81.16.Be, 73.63.-b DOI 10.17586/2220-8054-2016-7-4-599-603
Nanocrystalline samples of CaWO4 were prepared at room temperature by simple chemical precipitation. The samples were characterized by X-ray diffraction and scanning electron microscopy. Energy dispersive X-ray analysis confirmed the elements present in the sample. The frequency and temperature dependence of the dielectric constant and ac electrical conductivity of the nanomaterial were investigated. Very low dielectric loss in nanocrystalline CaWO4 powder was observed at high frequencies. The values of ac electrical conductivity calculated from the permittivity studies were found to increase as frequency increased, conforming to small polaron hopping.
Keywords: Chemical precipitation, dielectric constant, ac electrical conductivity, polaron hopping.
Received: 29 January 2016 Revised: 21 May 2016
1. Introduction
Nanocrystalline CaWO4 has attracted particular interest because of its practical applications, such as laser host materials in quantum electronics and scintillators in medical devices [1-6]. It has been reported that CaWO4 of scheelite-like structures is an excellent blue-emitting phosphor by their radiation of ultraviolet (UV) light [7]. Also, CaWO4 has shown considerable promise as a fiber-matrix interlayer in oxide ceramic composites [8]. The lower dielectric constant and low loss make nanostructured CaWO4 a promising candidate for applications as a low temperature co-fired ceramic (LTCC), substrate, and electronic packaging material [9]. Pullar et al. explained the microwave dielectric properties of AWO4 (A = Mg, Zn, Ni and Co) compounds with extrinsic parameter, such as density [10]. Sreedevi et al. reported that Ag2WO4 nanoparticles can be a promising material for the high dielectric constant gate in Si-based complementary metal oxide semiconducting devices [11]. The influence of processing methods on the characteristics of CdWO4 powders and the related microwave dielectric properties were reported by Bao-Chun Guo et al. [12]. The study of dielectric properties of samples as a function of temperature and frequency may help in identifying their potential applications [13]. The characterization of dielectric behavior is very important not only to the theory of the polarization mechanism but also from an application point of view, where knowledge of the temperature and the frequency dependence of dielectric constant are very important. The relative dielectric constant of the material determines its ability to store electrostatic energy.
Dielectric studies of CaWO4 nanoparticles are incomplete and need further investigation. In the present work, we synthesized CaWO4 nanoparticles by chemical precipitation followed by calcination. The samples were then characterized by X-ray diffraction (XRD) and scanning electron microscopy (SEM). The frequency and temperature dependence of dielectric properties of sintered pellets made out of the products were then investigated.
2. Materials and methods
Calcium nitrate Ca(NO3)2-4H2O (99.8 %, Sigma Aldrich) and sodium tungstate Na2WO4^O) (99.9 %, Alfa Aesar) analytical grade reagents were used for the preparation of CaWO4 nanocrystals. The samples were prepared by reacting aqueous solutions of calcium nitrate and sodium tungstate (0.1 M each) at room temperature. The precipitate formed was centrifuged, filtered, washed with distilled water a number of times, and dried in an oven to get fine powders of calcium tungstate. S1 and S2 are samples of nanocrystalline CaWO4 were calcined at 650 and 750 °C, respectively. XRD studies of these samples were conducted using Bruker D8 Advance X-ray diffractometer (A = 1.5406 A) with CuKa radiation in 26 range from 20 to 80 °. The morphological analysis of CaWO4 nanoparticles was carried out with a scanning electron microscope JEOL MODEL JSM-6390LV, operating at 20 kV measurements.
The calcined powder sample was cold pressed in the form of cylindrical pellets of diameter 13 mm and thickness d ~ 1.5 mm by applying a pressure of ~ 10 GPa using a hand operated hydraulic press. The pellets were then sintered at 500 °C. The density of the pellet was determined to be 4.88 g/cm3. The circular faces of the pellets were made electrically conducting by coating with silver paste. Dielectric measurements as a function of frequency in the range of 100 Hz - 1 MHz were measured at various selected temperatures from 303 - 423 K using an LCR meter (Wayne Kerr H-6500 model) in conjunction with a portable furnace and temperature controller (±1 K).
3. Results and discussion
The powder XRD spectra of CaWO4 nanoparticle samples are shown in Fig. 1. Both the samples showed characteristic peaks of scheelite structure with tetragonal unit cell. The 'd' values taken from the JCPDS file No. 77-2235 for CaWO4 are in close agreement with the observed'd' values.
10 20 30 40 50 60 70 80 26(degree)
Fig. 1. XRD spectra of CaWO4 samples
In general, the nanocrystallite size can be estimated from the Scherrer's formula: Dhkl = KA/(3 cos 0), where A is the x-ray wavelength (0.15405 nm), 3 the full-width at half maximum, 0 the diffraction angle, K is a constant (0.89) and Dhkl the size along the (hkl) direction. From the analysis, the average crystallite size obtained was 39 nm for Si and 44 nm for S2.
The SEM image of CaWO4 nanoparticles calcined at 650 °C is shown in Fig. 2(a). They are clusters shaped like dumb-bells. The elemental analysis of the sample S1 was done by energy dispersive X-ray (EDX) spectroscopy. Fig. 2(b) shows typical EDX spectrum of synthesized CaWO4 nanoparticles. The peaks of the spectrum confirmed that the product contains Ca, W and O. The intense signal near at 1.774 keV indicates that W is the major element.
The dielectric constant and ac conductivity (aac) were calculated by using equations e' = Cd/e0A and aac = e'e0w tan S, respectively, where A is the face area, C the measured capacitance of the pellet, eo the permittivity of vacuum, w the angular frequency and tan S the loss tangent. Fig. 3(a) shows the variation of dielectric constant with frequency for temperatures from 303 to 423 K of sample S1. It is seen that the dielectric constant for all temperatures are high at low frequencies which decreased rapidly as frequency increased, attaining a constant value at higher frequencies. For 303 K, the value of e was 24.74 at 100 Hz, which decreased to 7.11 at 1 MHz. At 393 K, the values were 30.08 (100 Hz) and 7.15 (1.0 MHz). The corresponding values for 423 K were 39.54 at 100 Hz and 7.20 at 1.0 MHz. Fig. 3(b) shows a similar variation for samples S1 and S2, at 393 K. At lower frequencies the dielectric constant is found to be higher for the sample having smaller grain size (S1), but approaches a constant value beyond 0.1 MHz. When temperature is increased, more and more dipoles are oriented, resulting in an increase in the dielectric constant for a given value of frequency [14]. At very high frequencies (MHz), the charge carriers would have started to move before the field reversal occurs and e' falls to a small value at higher frequencies.
Fig. 2. (a) SEM image of CaWO4 (S1) and (b) EDX spectrum of CaWO4
Fig. 3. The variation of dielectric constant with frequency of (a) sample S1 at temperatures 303, 393 and 423 K and (b) samples S1 and S2 at 393 K
Space charge polarization and reversal of the polarization direction contributes much to the e' [15]. With the increase in volume of the particle, the volume of the interfaces decreases. When volume increases, the contribution to e' by electronic relaxation polarization inside the particles increases.
The frequency dependence of dielectric loss of sample S1 is shown in Fig. 4(a). The loss factor represented by tanS has a value of 3.26 at 100 Hz which decreases slowly to zero at higher frequencies. At 393 K, the corresponding variation is not very different. For 423 K, tan S has a value of 9.53 at 100 Hz which gradually decreases almost to 0 at frequencies beyond 0.10 MHz. At 393 K the corresponding variation is not very different. The decrease in tan S takes place when the jumping rate of charge carriers lags behind the alternating electric field beyond a certain critical frequency.The inhomogeneities present in the interface layers in CaWO4 nanocrystals produce an absorption current resulting in dielectric loss. This absorption current decreases with increase in frequency of the applied field. The hopping probability per unit time increases with increase in temperature. Correspondingly, the loss tangent also increases with increase of temperature [16]. The variation of tan S with frequency at 393 K for samples S1 and S2 with different grain sizes is shown in Fig. 4(b). At 100 Hz, the value is 3.4 for S1 which decreases to 0.9 for S2. This variation of tanS for different grain sizes is due to size effect [17]. The low value of tan S indicates its potential for microwave applications.
The loss in CaWO4 can be explained using the electronic hopping model, which considers the frequency dependence of the localized charge carriers hopping in a random array. This model is applicable for materials in which the polarization responds rapidly to the appearance of an electron on any one site so that the transition may be said to occur effectively into the final state [17]. In the high frequency region tan S becomes almost zero because the electron exchange interaction (hopping) cannot follow the alternatives of the applied ac electric field beyond a critical frequency.
Fig. 4. The variation of loss tangent with frequency of (a) sample S1 at temperatures 303, 393 and 423 K and (b) samples S1 and S2 at 393 K
Figure 5(a) shows the variation of ac conductivity (aac) of sample S1with frequency. Initially, it has a small value which increased at higher frequencies. The nature of variation is similar for other temperatures, but the values are shifted upwards as the temperature is raised. For 303 K, aac has a value of 5.001 x 10-7 S/m at 100 Hz which increased slowly at higher frequencies to 1.4 x 10-3 S/m at 0.10 MHz. At 393 K, the corresponding variation was not very different. For 423 K, the values were 2.236 x 10-6 S/m at 100 Hz and 2.781 x 10-5 S/m at 1.0 MHz. The variation of aac with frequency at 393K for different grain sizes is shown in Fig. 5(b). At 100 Hz, aac is found to be 5.002 10-7 S/m for S 1 which increased to 6.88 x 10 5 S/m at 1.0 MHz. For S2, the corresponding values were 5.823 10-8 S/m and 7.671 x 10-6 S/m. It is clear from the figure that the conductivity increased as frequency increased conforming to small polaron hopping [18]. Also, there is a possibility of conduction due to impurities at low temperature. It is found that at given temperature and frequency, aac is higher for particle having smaller size. According to Elliot's barrier hopping model, ac conductivity increases with hopping distance [19]. Therefore, it may be concluded that in CaWO4 hopping distance increased with reduction in particle size.
Fig. 5. The variation of ac electrical conductivity with frequency of (a) sample S1 at temperatures 303, 393 and 423 K; (b) samples S1 and S2 at 393 K
4. Conclusion
The CaWO4 nanoparticles were prepared at room temperature by simple chemical precipitation reaction without any catalyst, surfactant, or templates. The dielectric properties of CaWO4 were determined as a function of frequency from 100 Hz to 1.0 MHz for temperatures ranging from 303 to 423 K. At lower frequencies, e' and tan S have higher values while at higher frequencies the values reached steady lower values. Similar variation was observed when the temperature was raised but the values of e' and tan S were elevated. The ac conductivity increased as frequency was increased conforming to small polaron hopping. The values of e', tan S and aac showed considerable increase as the particle size was reduced. The very low value of loss tangent obtained for
CaWO4 nanocrystals suggests that it is potentially useful for microwave applications. It was found that the applied frequency, temperature and particles size affect the dielectric properties of the CaWO4 nanocrystals.
Acknowledgements
The authors are indebted to NSRC, Nirmala College, Muvattupuzha and Newman College, Thodupuzha for the support to undertake this study. The financial support from the University Grants Commission, New Delhi, India (FIP/12th Plan/KLMG020 TF03) is greatly acknowledged.
References
[1] Kobayashi M., Ishii M., Usuki Y., Yahagi H. Scintillation characteristics of PbWO4 single crystals at room temperature. Nuclear Instruments and Methods in Physics Research A, 1993, 333 (2-3), P. 429-433.
[2] Katelnikovas A., Grigorjeva L., et al. Sol-Gel Preparation of Nanocrystalline CaWO4 . Lithuanian J. of Physics, 2007, 47 (1), P. 63-68.
[3] Phuruangrat A., Thongtem T., Thongtem S. Synthesis, characterization and photoluminescence of nanocrystalline calcium tungstate. J. Exp. Nanosci., 2009, 5, P. 263-267.
[4] Lou Z., Cocivera M. Cathodoluminescence of CaWO4 and SrWO4 thin films prepared by spray pyrolysis. Mater. Res. Bull., 2002, 37, P. 1573-1582.
[5] Nagirnyi V., Feldbach E., et al. Excitonic and recombination processes in CaWO4 and CdWO4 scintillators under synchrotron irradiation. Radiat. Meas, 1998, 29, P. 247-250.
[6] Oishi S., Hirao M. Growth of CaWO4 whiskers from KCl flux. J.Mater.Sci, Lett., 1989, 8 (12), P. 1397-1398.
[7] Liping L., Yiguo S., Guangshe L. Size-induced symmetric enhancement and its relevance to scheelite CaWO4 nanocrystals. J. Appl. Phys. Lett., 2007, 90, P. 054105-054107.
[8] Mogilevsky P., Parthasarathy T.A., Petry M.D. Anisotropy in room temperature microhardness and fracture of CaWO4 scheelite. Acta Materialia, 2004, 52, P. 5529-5537.
[9] Vidya S., Sam Solomon., Thomas J.K. Synthesis of Nanocrystalline CaWO4 as Low-Temperature Co-Fired Ceramic Material: Processing, Structural and Physical Properties. Journal of Electronic Materials, 2012, 42, P. 129-137.
[10] Pullar R.C., Farrah S., Alford N.M. MgWO4, ZnWO4, N1WO4 and CoWO4 microwave dielectric ceramics. Journal of the European Ceramic Society, 2007, 27, P. 1059-1063.
[11] Sreedevi A., Priyanka K.P., et al. Nanophase a-Silver Tungstate for Potential Applications in Light Emitting Diodes and Gate Dielectrics. Advanced Science, Engineering and Medicine, 2015, 7, P. 498-505.
[12] Bao-Chun Guo, Peng Liu, et al. Effect of Preparation Methods on Microstructures and Microwave Dielectric Properties of CdWO4 ceramics. Integrated Ferroelectrics, 2015, 167, P. 107-114.
[13] Chi Kao K. Dielectric phenomena in Solids. Elsevier, New York, 2004.
[14] Kar T., Choudhary R.N., Sharma S., Singh K.S. Structural and electrical properties of Ba2Na3RNbioO3o Ceramics. Indian J. Phys. A, 1999, 73 (4), P. 453-459.
[15] Ravinder D., Vijayakumar K. Dielectric behaviour of erbium substituted Mn-Zn ferrites. Bull. Mater. Sci., 2001, 24 (5), P. 505-509.
[16] Potty S.N., Khader M.A. Dielectric Properties of nanophase Ag2Hgl4 and Ag2Hgl4-Al2O3 nanocomposites. Bull. Mater. Sci., 2000, 23 (5), P. 361-367.
[17] Murthy V., Sobhanadri J. Dielectric properties of some nickel-zinc ferrites at radio frequency. Phys Status Solidi (a), 1976, 36 (2), K133-K135.
[18] Priyanka K.P., Sunny J., et al. Dielectric properties and a. c. conductivity of nanocrystalline titania. J. Basic Appl. Phys., 2013, 2, P. 105-108.
[19] Elliot S.R. Temperature dependence of a.c. conductivity of chalcogenide glasses. Phil. Mag. Part B, 1978, 37 (5), P. 553.
