Preparation and Characterization of Nanostructured CaCu 2.90 Zn 0.10 Ti 4 O 12 Ceramic

Abstract

Nanostructure CaCu_2.90Zn_0.10Ti₄O₁₂ (CCZTO) electronic ceramic was synthesized by semi-wet route. The objective of this route is to enable the calcination and sintering processes to go for completion in shorter time and at lower temperature.***The samples were characterized by XRD, TEM, SEM and EDX analyses. The crystallite size of the CCZTO ceramic, obtained by XRD using Debye Scherrer formula, range from 38-74nm which is in good agreement with the particle size observed by TEM analysis. It was observed clearly that the grain size significantly increased with an increase in sintering duration. Dielectric measurements were carried out by LCR meter in the temperature range, 300–500K, at few selected frequencies. It was also observed that the dielectric constant and dielectric loss of CCZTO are temperature independent in higher frequency whereas temperature dependent in low frequency region. The ceramics exhibit high dielectric constant of 1.35 × 10⁴ at 1 kHz.

Keywords

Ceramics nanoparticles dielectric properties

1. Introduction

Nanosized materials with high dielectric constant are in the focus of interest, not only for purely academic reasons but also because new high ε_r materials are urgently sought for the further development of modern electronics. The high dielectric constant material is desirable to miniaturize capacitor required for integerated circuit. BaTiO₃ and SrTiO₃ based ferroelectric materials exhibit high dielectric constant but these materials show strong temperature dependence of their dielectric constant which is not desirable from the device points of view [1–2]. On the other hand, CaCu₃Ti₄O₁₂ (CCTO) ceramic has high dielectric constant (ε_r ∼ 10⁴ −10⁵) independent of frequency (10² - 10⁶ Hz) and temperature (100-600K) which is desired for microelectronic applications [3–4]. Unfortunately, the CCTO ceramic with giant dielectric constant exhibits higher dielectric loss that limits its practical applications. It has been previously reported that the dielectric properties of CCTO are largely influenced by factors such as doping schemes [5 –7] as well as stoichiometric variations [8–9]. Recently much work based on partial substitution at Cu or Ti ions site in CCTO ceramic has been carried out in order to improve the dielectric properties and to understand the origin of gaint dielectric response in CaCu₃Ti₄O₁₂ ceramic [10 –12]. Partial isovalent ionic substitutions of Cu by Zn or Mg in CaCu₃Ti₄O₁₂ ceramic have enhanced the dielectric response due to modification of its structure [13 –15]. In these cases, compared to the slight change of Cu⁺/Cu⁺² ratio which also increases Ti⁺³/Ti⁺⁴ ratio, may be the primary factor for the enhanced dielectric response in CCTO ceramic. The dielectric constant (ε_r) and loss tangent (tanδ) of CCTO are strongly dependent upon the processing conditions such as sintering temperature [16], sintering time [17], cooling rate and partial pressure of sintering atmosphere. The traditional solid-state reaction method is usually used to prepare crystalline CCTO with starting materials, CaCO₃, CuO and TiO₂, in stoichiometric ratio at high temperature. The mixtures are calcined for long duration with several intermediate grindings. This procedure requires tedious work, relatively long reaction time and high temperature condition. In addition, some other secondary phases also appear during synthesis because of limited atomic diffusion through micrometer sized grains. On the other hand, the wet chemical methods provide atomic level mixing of individual components and result in the formation of nanocrystalline materials at much lower temperature compared with solid state reactions. There are many chemical methods, such as, sol-gel, co-precipitation, precursor solution technique and hydrothermal process [18 –20] which have already been reported for the synthesis of CCTO ceramics. But in these chemical methods Ti is used as Ti(OR)₄ which is very costly.

In the present communication we report a new successful route to synthesize nanocrystalline CCZTO by semi-wet route at low sintering temperature and short duration. In this method, the mixing process is performed in solution state as nitrate solutions along with solid TiO₂ which is very cheap. This is one of the most advantages over the other methods. We also report the dielectric properties of this ceramic.

2. Experimental

Analytical grade chemicals, Ca(NO₃)₂.4H₂O, Cu(NO₃)₂.3H₂O, (CH₃COO)₂Zn.2H₂O, titanium dioxide and citric acid, obtained from Merk, having purity of 99.95 % or better were used as starting materials. Standard solutions of metal nitrates were prepared using distilled water. Solutions of the metal nitrates in stoichiometric amount of these metallic ions were mixed in a beaker. Calculated amounts of TiO₂ and citric acid equivalent to metal ions were added to the solution. The solution was heated on a hot plate using a magnetic stirrer at 70-90 °C to evaporate water and then dried at 100-120°C in hot air oven for 12h to yield a blue gel. The gel was calcined in air at 800°C for 6h in a muffle furnace. The resultant mixture was ground into fine powder using a pestle and mortar. Cylindrical pellets were made using hydraulic press. The pellets, sintered at 950 °C for 6 h, 8h and 12h in air, were abbrebated as CCZTO-6h, CCZTO-8h and CCZTO-12h, respectively. The densities of samples were measured by Archimedes method. The crystalline phases of the sintered samples were identified using an X-ray Diffractometer (Rich-Siefert, ID-3000) employing Cu-Kα radiation. The microstructures of the fractured surfaces were examined using a Scanning Electron Microscope (SEM, Model JEOL JSM5410). The Energy Dispersive X-ray Analyzer (EDX, Model Kevex, Sigma KS3) was used for the elemental analysis of the sintered samples. Transmissions Electron Microscopic (TEM Technai 12 G2, FEI) studies of the sintered samples were carried out by placing the test sample on carbon-coated copper grid, operated at an accelerated voltage of 120 kV. The dielectric data of Zn doped CCTO ceramics were collected using the LCR meter (PSM 1735, Newton 4th Ltd, U.K) with variation in temperature at few selected frequencies.

3. Results and discussion

The relative densities of CaCu_2.90Zn_0.10Ti₄O₁₂ (CCZTO) ceramics sintered at 6h, 8h and 12h were found to be 91.16, 93.34 and 94.44%, respectively. It clearly shows that density increases with sintering time. XRD patterns of CaCu_2.90Zn_0.10Ti₄O₁₂ sintered at 950 °C with different sintering time (6h, 8h and 12h) are shown in Fig.1. X-Ray data were indexed on the basis of a cubic unit cell similar to undoped CCTO (JCPDS 75-2188), which confirm the formation of single phase. The lattice parameters and unit cell volume, determined using least square refinement method, are given in Table 1.

Figure 1.

X-ray diffraction patterns of CaCu_2.90Zn_0.10Ti₄O₁₂ Ceramics sintered at 950 ° C for 6h, 8h and 12h

Table 1.

Lattice parameter, unit cell volume and particle size obtained from XRD and TEM for CaCu_2.90Zn_0.10Ti₄O₁₂

Sintering time	Lattice Parameter (Å)	Lattice Volume (Å³)	Crystallite size from XRD (nm)	Particle size from TEM (nm)
6h	7.276±0.256	385	38± 13	54± 11
8h	7.321±0.008	392	69± 16	73± 23
12h	7.378±0.015	401	74± 18	84± 15

Fig. 2 shows the variation of lattice parameter with sintering time. It is observed from the figure that the lattice parameter increases with the increase in the sintering time. The change in unit cell parameter with time of annealing is due to increase in density. During the heat treatment each crystallite get enough dwelling time to get properly crystallized [21].

Figure 2.

Varaiation of lattice parameter with sintering time

There is no evidence of the presence of secondary phase. XRD patterns show the presence of split peaks for the reflections at 400, 422 and 440. This may be due to presence of Cu-Kα₂ along with Cu-Kα₁ in the X-ray radiations used for the diffraction. This is supported by the fact that in all these reflections the intensity of peaks due to Cu-Kα₂ is close to 50 % of intensity of peak due to Cu Kα₁ as expected. From the line broadening of the main peaks, the crystallite size of the ceramic was estimated using the Debye Scherrer formula [22]:

D = k λ / β cos θ

(1)

where λ is the wavelength of the X-ray, k is a constant taken as 0.89, θ is the diffraction angle and β is the full width at half maxima (FWHM). The crystallite size derived from the XRD data and TEM analysis are given in the Table 1.

It is clearly observed that the crystallite size increased with increasing sintering duration, which is confirmed by the TEM analysis. The increased crystallite size with increasing sintering time is mainly due to over grown grains resulting from the destruction of the grain boundaries at higher sintering time. These data clearly show that the sintering time is responsible for increasing crystallite size with increasing sintering time of CaCu_2.90Zn_0.10Ti₄O₁₂ ceramic.

Fig. 3 shows SEM images of surface microstructures for the ceramics sintered at different sintering times. As can be seen from Fig. 3(a)-(c), the microstructures of CaCu_2.9Zn_0.1Ti₄O₁₂ change significantly with sintering time. In specimen sintered at 950 °C for 6h a porous with small grain size 8-10 μm is observed. The grain size range varies from 10-15 μm and 15-25 μm of the ceramics sintered at 8h and 12h, respectively. It can be seen that the grain size increased with increase of sintering time and the correspondingly grain boundary was reduced. Increasing the sintering time significantly promotes the grain growth and microstructural densification. The microstructures show grain growth in the specimen sintered for 8h and 12h along with some liquid phase. Additionally, a small amount of CuO phase was found in grain boundary region. This phase was so small that XRD could not detect. It also seems that with increasing sintering time from 6h, 8h and 12h solid CuO phase start melting as shown in Fig. 3(b) and totally melted in at grain boundary as shown in Fig. 3(c). Copper oxide present at grain-boundary transforms into the liquid phase during sintering which leads to abnormal grain growth [23–24].

Figure 3.

SEM images of CCZTO ceramics sintered at 950 °C for (a) 6h, (b) 8h and (c) 12h

TEM images (Fig. 4) of the CCZTO sintered powders clearly show that all of the samples consist of nanocrystalline CCZTO particles whose size increases with increasing sintering time. A representative manually constructed histogram of particle size distribution of CaCu_2.90Zn_0.10Ti₄O₁₂ (CCZTO-8h) is shown in Fig.5. The particle size of the ceramics sintered at 950 °C for 6h, 8h and 12h were found to be 54±11, 73±23 and 84±15 nm, respectively. The crystallite size obtained using Debye Scherrer formula is smaller than the particle size obtained by TEM. This is due to fact that the Debye Scherrer formula does not take into account the effect of lattice strain and instrumental factors on peak broadening.

Figure 4.

TEM images of CCZTO ceramics sintered at 950 °C for (a) 6h, (b) 8h and (c) 12h

Figure 5.

Histogram of Particle size distribution curve of CaCu_2.90Zn_0.10Ti₄O₁₂ nanoparticles of CCZTO-8h

EDX spectra of CCZTO ceramic (Fig.6) sintered at 950 °C for 6h, 8h and 12h show the presence of Ca, Cu, Zn, Ti and an extra peak of Pt at 2.15 keV. Pt coating was performed by ion beam sputtering for increasing the conductivity which was necessary to avoid charging or charged up of samples. The atomic percentage of Ca, Cu, Zn and Ti in the CCZTO ceramics obtained from EDX data are given in Table 2. The Cu/Ca ratio for CCZTO-6h, CCZTO-8h and CCZTO-12h are 2.75, 2.73 and 2.73, respectively. The percentage error are found to be 5.45, 6.22 and 6.22%, respectively.

Figure 6.

EDX spectrum of CCZTO ceramics sintered at 950 °C for (a) 6h, (b) 8h and (c) 12h

Table 2.

Atomic percentage of elements for CaCu_2.90Zn_0.10Ti₄O₁₂ (CCZTO) sintered at 950 °C for 6h, 8h and 12h

Sintering duration	Atomic % of elements

	Ca	Cu	Zn	Ti	O
6h	4.76	13.11	0.38	17.04	64.71
8h	6.69	18.33	0.67	25.90	48.41
12h	6.72	18.37	0.70	24.29	49.92

The temperature dependence of dielectric constant (ε_r) and loss tangent (tanδ) of the CCZTO ceramic sintered for 6h at different frequencies 0.1, 1, 10 and 100 kHz are shown in Fig.7. Dielectric constant (ε_r) exhibits a step like increase from low value 4216 to a giant value 16560 at temperature above 350K, which is prominent in the low frequency region and diminishes on increasing the frequency. At above room temperature a broad dielectric peak appears between 350K to 425K which also shifts to higher temperature and decreases in amplitude with increasing higher frequencies. It shows a ferroelectric relaxor behavior in the ceramic [25]. It is observed from the Fig. 7 (b) that the corresponding peaks are also present in the temperature-dependent plot tanδ. The above characteristic behaviors of a ferroelectric relaxor is usually characterized by diffuse phase transition and strong relaxational dispersion in dielectric constant and loss tangent (tanδ).

Figure 7.

Variation of ε_r and tanδ vs temperature of CCZTO ceramic sintered at 950 °C for 6h

Figs.8 & 9 show the variation of dielectric constant and loss tangent (tanδ) with temperature at 0.1, 1, 10 and 100 kHz for CCZTO ceramics sintered at 950 °C for 8h and 12h, respectively. It is clearly shown from the figure that ferroelectric behavior is not present. It is also observed that the dielectric constant and dielectric loss of CCZTO 8h and 12h are temperature independent at higher frequency whereas temperature dependent in the low frequency region. It is also noted from the figures that the values of ε_r for CCZTO ceramic are 1083, 4751 and 4957 at 1kHz for 6h, 8h and 12h, respectively.

Figure 8.

Variation of ε_r and tanδ vs temperature of CCZTO ceramic sintered at 950 °C for 8h

Figure 9.

Variation of ε_r and tanδ vs temperature of CCZTO ceramic sintered at 950 °C for 12h

It is also inferred that ε_r increases with increasing sintering time. This is due to the fact that the longer sintering time produces more oxygen vacancies in the CCZTO ceramics and results high dielectric constant. It is observed from the figure that dielectric losses at 1 kHz for CCZTO are 1.07, 0.38 and 0.18 for 6h, 8h and 12h, respectively, at room temperature. A very clear picture of the sintering time dependence of dielectric constant value measured at 10 kHz is shown in Fig. 10. The high dielectric constant for CCZTO ceramics is due to interfacial space charge polarization [26]. This interfacial charge polarization arises due to accumulation of charge carriers at the interface of semiconducting grains and insulating grain boundary.

Figure 10.

Dielectric constant value as a function of sintering time measured at 10 kHz

4. Conclusion

It is immensely important that an adequate control of sintering time and temperature are needed to obtain the desired microstructure and dielectric properties. Dielectric constant increases with increasing sintering time and dielectric loss decreases. It is suggested that the longer sintering time may lead to more defect structures. The size of the particle increases with increasing sintering time. It is mainly due to formation of large size particles as a result of loss of grain boundaries of small size particles. These changes lead to stability to the large size particles due to loss in grain boundary.

Footnotes

5. Acknowledgements

Authors express their gratitude to Dr. Madhu, Scientist, Institute of Medical Science, BHU, Varanasi for extending the facility for TEM analysis.

References

Chou

X.J.

Zhai

J.W.

Jiang

H.T.

Yao

, “Dielectric properties and relaxor behaviour of rare earth (La, Sm, Eu, Dy, Y) substituted barium zirconium titanate ceramics,” J. Appl. Phys., Vol. 102, pp. 084106–084112, 2007

Zhao

Huang

X.Y.

Guan

Cao

C.H.

, “Effect of Y₂O₃ and Dy₂O₃ on dielectric properties of Ba_0.7Sr_0.3TiO₃ series capacitor ceramics,” J. Rare Earths, Vol. 25, pp.197–200, 2007.

Liu

Zhu

G.Q.

Bian

X.B.

, “Influence of Nb doping on the dielectric properties of CaCu₃Ti₄O₁₂ ceramics,” Acta Physica Sinica, Vol. 56, pp. 5489–5493, 2007.

Home

C.C.

Vogt

Shapiro

S.M.

Wakimoto

Ramirez

A.P.

, “Optical responses of high-dielectric-constant perovskite related oxide,” Science, Vol.293, pp.673–676, 2001.

Chung

S.Y.

Choi

S.Y.

Yamamoto

Ikuhara

kang

S.J.L.

, “Change in cation nonstoichiometry at interfaces during crystal growth in polycrystalline BaTiO₃,” Appl. Phys. Lett., Vol.88, pp.011909–3, 2006.

Kwon

Huang

C.C.

Patterson

E.A.

Alberta

E.F.

Hackenberger

W.S.

Cann

D.P.

, “The effect of Cr₂O₃, Nb₂O₅ and ZrO₂ doping on the dielectric properties of CaCu₃Ti₄O₁₂,” Mater. Lett., Vol.62, pp.633–636, 2008.

Kobayashi

Terasaki

, “Unusual impurity effects on the dielectric properties of CaCu_3-xMn_xTi₄O₁₂,” Physica B., Vol. 329, pp.771–772, 2003.

Fang

T.T.

Mei

L.T.

H.F.

, “Effects of Cu stoichiometry on the microstructures, barrier-layer structures, electrical conduction, dielectric responses, and stability of CaCu₃Ti₄O₁₂,” Acta Mater., Vol. 54,pp.2867–2875, 2006.

Shao

S.F.

Zhang

J.L.

Zheng

Wang

C.L.

, “Effect of Cu-stoichiometry on the dielectric and electric properties in CaCu₃Ti₄O₁₂ ceramics,” Solid State Commun., Vol.142, pp.281–286, 2007.

10.

Hutagalung

S.D.

Ooi

L.Y.

Ahmad

Z.A.

, “Improvement in dielectric properties of Zn-doped CaCu₃Ti₄O₁₂ electroceramics prepared by modified mechanical alloying technique” Journal of Alloys and compounds, Vol.476, pp.477–481, 2009.

11.

Rai

Alok Kumar

Mandal

K. D.

Kumar

Parkash

, “Dielectric properties of CaCu₃Ti_4-xCo_xO₁₂ (x = 0.10, 0.20, 0.30) synthesized by Semi-wet Route” Materials Chemistry and Physics, Vol. 122, pp.217–220, 2010.

12.

Feteira

Sinclair

D. C.

West

A. R.

, “Influence of Mn doping on the semiconducting properties of CaCu₃Ti₄O₁₂ ceramics” Appl. Phys.Lett., Vol.88, pp.232903–912, 2006.

13.

Zhang

Cheng

X.N.

Fan

Yang

Yuan

H.M.

, “Dielectric properties of Zn Doped CCTO Ceramics by Sol-Gel Method” Advanced Materials Research, Vol. 197, pp.302–305, 201.

14.

Chen

X. L.

Zhang

D. F.

Wang

W. Y.

Wang

W. J.

, “Humidity sensitive properties of pure and Mg-doped CaCu₃Ti₄O₁₂“ Sensors and Actuators B: Chemical, Vol.147, pp.447–452, 2010.

15.

Cai

Gemei

Zhang

D. F.

Wang

W. Y.

Wang

W. J.

Chen

X. L.

, “Enhanced dielectric responses in Mg-doped CaCu₃Ti₄O₁₂“ Vol. 104, pp.074107–4, 2008.

16.

Aoyagi

Iwata

Maeda

, “Effect of Sintering Temperature on the Dielectric Properties of CaCu₃Ti₄O₁₂ Ceramics,” Ferroelectrics, Vol.356, pp.90–94, 2007.

17.

Prakash

B. Shri

Varma

K.B.R.

, “Effect of sintering conditions on the dielectric properties of CaCu₃Ti₄O₁₂ and La_2/3Cu₃Ti₄O₁₂ ceramics, A comparative study”, Physica B, Vol. 382, pp.312–319, 2006.

18.

Jha

Arora

Ganguly

A.K.

, “Polymeric citrate precursor route to the synthesis of the high dielectric constant oxide CaCu₃Ti₄O₁₂,” J.Mater. Lett., Vol.57, pp.2443–2446, 2003.

19.

Liu

Smith

R.W.

Mei

W.N.

, “Synthesis of the Giant Dielectric Constant Material CaCu₃Ti₄O₁₂ by Wet-Chemistry Methods,” Chem. Mater., Vol.19, pp.6020–6024, 2007.

20.

Masingbon

Thongbai

Maensiri

Yamwong

Seraphin

, “Synthesis and giant dielectric behavior of CaCu₃Ti₄O₁₂ ceramics prepared by polymerized complex method,” Mater. Chem. Phys., Vol. 109, pp. 262–270, 2008.

21.

Kaur

Narang

S. B.

, “Influence of increased sintering time on structure and dielectric behaviour of barium lanthanide titanates”, Ceramics-Silikaty, Vol. 54, pp.108–115, 2010.

22.

Culity

B.D.

Stock

S.R.

, “Elements of X-ray Diffraction”, Prentice Hall, New Jersey, Chapter 1, pp. 7–10, 2001.

23.

Kim

D.W.

Kim

T.G.

Hong

K.S.

‘Low firing of CuO doped anatase’

Mater. Res. Bull. Vol. 34, pp.771–781, 1999.

24.

Huang

C.L.

Chen

Y.C.

, ‘Low temperature sintering and microwave dielectric properties of SmAlO₃ ceramics’ Mater. Res. Bull. Vol. 37 pp.563–574, 2002.

25.

Veith

Ren

Wittmar

Bolz

, “Giant dielectric constant response of the composites in ternary system CuO-TiO2-CaO,” J.Solid State Chem., Vol.182 pp.2930–2936, 2009.

26.

Birey

, “Dielectric properties of aluminum oxide films,” J. Appl. Phys., Vol. 49, pp.2898–2904, 1978.