Conduction and relaxation mechanisms in gadolinium oxide nanoparticle doped polyvinyl alcohol films

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Highlights

  • Doping in nano form decreases ε in contrast to doping with ions which were reported to increase ε.

  • Activation energy decreases monotonically where as resistivity increases with increasing concentration.

  • The films exhibit negative resistance co-efficient with temperature.

  • Relaxation is seen to be non-Debye in nature.

  • Correlated Barrier Hopping is the preferred mechanism for conduction.

Abstract

Concentration dependent dielectric and electrical properties of PVA-Gd2O3 nanocomposite films over a wide range of frequencies (100Hz-1 MHz) and temperatures (303 K–423 K) is reported here. TEM of the Gd2O3 nanoparticles showed that they could be indexed to the cubic phase. The frequency variation of the dielectric permittivity and dielectric loss could be explained by the Maxwell Wagner Sillar’s model. The dielectric permittivity decreased in the composite films contrary to observations in other similar systems. The complex impedance showed Arrhenius behavior and the activation energies decreased monotonically with increasing concentration. However the resistivity of the nanocomposite films shows an increase with concentration, the 4 wt% film showing the highest resistivity which indicates other contributions to conductivity. The Nyquist plot could be fitted to a simple parallel RC circuit showing the presence of long range conduction in these samples. The relaxation times varied from 10−4 to 10−6s and indicated a non-Debye type of relaxation. The master curve showed good overlap indicating that the same relaxation processes were active at all temperatures. The ac conductivity obeys Jonscher’s law and the exponent shows a monotonic decrease with temperature. This indicates that Correlated Barrier Hopping is the probable mechanism for conduction in these samples.

Introduction

The combination of inorganic nanoparticles and organic polymers forms an interesting class of materials called polymer nanocomposites. Polymers contribute properties such as ease of processing, low cost and flexibility while small quantities of the dopant nanoparticles add useful properties which help to tailor the material for specific applications [[1], [2], [3], [4]]. Nanocomposites using a wide variety of polymers have been studied [[1], [2], [3], [4], [5], [6], [7]] and the ones using the polymer poly vinyl alcohol (PVA) are biodegradable and environment friendly. PVA has high mechanical strength, good environmental stability and forms nanocomposites with ease. There is abundant literature reporting the effect of inorganic dopants like ZnBr2, nano ZnO, nano CeO2, CdS, Gd3+, Mn2+, EuCl3, TbCl3, YCl3, Ag [[8], [9], [10], [11], [12], [13], [14], [15], [16]] etc. on the structural, optical, dielectric and electrical properties of PVA so as to enhance the suitability of the material for particular applications. The addition of semiconductor nanoparticles such as ZnO and HgSe to PVA have shown increased conductivity in these films paving the way for possible applications in the electronic industry [9,16]. The addition of nanoparticles of the rare earth oxide CeO2 to PVA gave rise to enhanced photoluminescence even at low concentrations of the dopant [10]. Rare earth sesquioxides are one of the highly studied materials that have a wide range of applications in optoelectronics [[17], [18], [19]]. They are chemically and thermally very stable. Among them Gd2O3 is of particular interest due to its completely half filled 4f electronic shell which is expected to give rise to interesting optical, dielectric and electrical properties. The photoluminescence (PL) in lanthanides are in general sharp and intense as these arise from transitions within the f shell energy levels as well as from defect centers, and this is true in gadolinium also. Amongst the lanthanides, half filled shell has the maximum magnetic moment of I = 7/2 as all the electron spins are parallel. This makes it useful as a contrast agent in MRI [18]. The large magnetic moment also affects its electrical properties [20]. Recently Sudip Mukherjee et.al [21] reported high dielectric constant and low loss in a system of Gd2O3 nanocrystal dispersed in a silica matrix. Other reports with similar results are also available in literature [22]. These types of materials are promising candidates for memory device applications. Researchers such as Taha A. Hanafy [23] and M. Obula Reddy et.al [20] have reported the effect of lanthanide ions like La3+, Gd3+ and Er3+ on the dielectric relaxation and ac conductivity of PVA matrix. They observed significant increase in the dielectric permittivity and conductivity of PVA. The effect of Gd2O3 nanoparticles and Sm2O3 nanoparticles on PVA films was to give rise to good photoluminescence in the blue and red region with sufficient color purity for optoelectronic applications [24,25]. Because these materials have such a multitude of applications it is of interest to study the conductivity and relaxation mechanisms operative in them. The ac conductivity in such nanocomposites can be modeled in many ways, the main mechanisms being quantum mechanical tunneling (QMT), small and large poloron assisted tunneling and Correlated Barrier Hopping (CBH). The most suitable model can be inferred from the temperature dependence of the exponent obtained from fitting the dielectric data to Jonscher’s power law. An analysis of the dielectric data in the light of various formalisms helps delineate the relaxation processes in the material and gives an idea of the mechanisms occurring in these materials. Hence it was felt that a detailed dielectric analysis of this material will enhance our understanding of the processes taking place and lead to a better design of materials for new applications. With this view, a concentration dependent study of the dielectric and electrical properties of nanocomposite films of Gd2O3 with PVA was undertaken and to the best of our knowledge this is the first report on such a rare earth system. The results of the study point to an uncommon decrease in the value of dielectric permittivity and an increase in the resistivity of the films with concentration of Gd2O3.

Section snippets

Experimental

Polyvinyl alcohol ((C2H4O)x, average molecular weight 13,000–23,000, 98 % hydrolyzed), Gadolinium(III) nitrate hexahydrate [Gd(NO3)3.6H2O], glycine [C2H5NO2] of purity 99.99 % were obtained from Sigma Aldrich and used as obtained. Gd2O3 nanoparticles were synthesized by solution combustion method and PVA-Gd2O3 nanocomposite films were prepared by solution casting technique. The detailed procedure for sample preparation is given elsewhere [24]. The structural details of the pure PVA and PVA-Gd2O3

FTIR analysis

The intermolecular interaction and the structural modifications induced by the dopant in the polymer matrix were analyzed by FTIR spectra. The FTIR spectra of pure PVA and PVA-Gd2O3 nanocomposites with dopant concentration of 2 wt%, 4 wt% and 6 wt% are shown in Fig.1. All the composites exhibit the characteristic bands of pure PVA along with few other new bands. The assignments of all the bands are tabulated in Table 1 and are in good agreement with previously reported work [9,25]. A broad and

Conclusion

Dielectric studies on PVA-Gd2O3 nanocomposite films as a function of frequency at various temperatures is reported here. FTIR and TEM were used to characterize the films and nanoparticles respectively and are seen to agree with the XRD and Raman data published by us earlier [24] and confirm the formation of the nanocomposite films. Dielectric permittivity of the nanocomposite films decrease with increasing dopant concentration up to 4 wt% and increases again for 6 wt%. This is contrary to the

Declaration of Competing Interest

The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

Acknowledgement

S. N. Madhuri is thankful to INUP, IISc, CeNSE, Bengaluru funded by Meity, Govt. of India for providing characterization facilities for FTIR and TEM.

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