Advances in Materials Science and Engineering

Volume 2014 (2014), Article ID 685715, 5 pages

http://dx.doi.org/10.1155/2014/685715

Research Article

Structural, Electrical, and Ethanol-Sensing Properties of Nanoparticles

Nguyen Thi Thuy,¹ Dang Le Minh,² Ho Truong Giang,³ and Nguyen Ngoc Toan³

¹Physics Department, Hue University’s College of Education, Hue, Vietnam

²Faculty of Physics, Hanoi University of Science, VNU, Hanoi, Vietnam

³Institute of Material Science, Institute of Technology and Science, Hanoi, Vietnam

Received 21 March 2014; Accepted 23 June 2014; Published 18 August 2014

Academic Editor: Markku Leskela

Copyright © 2014 Nguyen Thi Thuy et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Abstract.

The nanocrystalline () powders with orthorhombic perovskite phase were prepared by sol-gel method. The average crystallite sizes of powders are about 20 nm. The resistance and gas-sensing properties of the based sensors were investigated in the temperature range from 160 to 300°C. The results demonstrated that the resistance and response of the perovskite thick films changed with the increase of Nd content.

1. Introduction

There has been much interest in perovskite structured compounds (of general formula ABO₃) because of their catalytic activity, colossal magnetoresistance effects, thermoelectric effects, gas-sensing properties, and so forth [1–8]. Specially perovskite oxides with AFeO₃ structure (A: rare earth) have shown the good gas-sensing properties such as LaFeO₃, , , , and . Among the modified perovskites, showed the best ethanol gas-sensing characteristics; its response to 100 ppm ethanol was more than 80% in the temperature range from 140 to 240°C; it was also found that the based sensor had the best response and selectivity to ethanol gas; the response to 500 ppm ethanol is 128 at 220°C or the highest response to 500 ppm ethanol gas reaches 57.8 at 260°C for sensor and so forth [9–12]. Numerous perovskites show p-type semiconductor properties in air. Oxygen adsorption enhances the conductivity of these materials on account of the increased concentration of holes, which are the main charge carrier species in p-type semiconductors. Furthermore, their resistance increases by applying reducing gases, such as ethanol. Interaction between the reducing gas and the oxygen adsorbed on the metal oxide surface leads to a change in conductance [13–16]. Perovskite powder AFeO₃, used in thick film gas sensors, can be manufactured by different chemical methods: coprecipitation method, sol-gel method, and hydrothermal method. They are used broadly due to their advantage in which precursors can be admixed at atomic scale. So, the products are pure and homogeneous. The products also have small grain size and great surface area and are compatible in metal oxide semiconductor (MOS) gas sensors.

In this paper,    perovskite oxides were prepared by a citrate-gel method. The influence of Nd doping on the A site of the crystalline structure of LaFeO₃ and also on their ethanol-sensing characteristics has been investigated in detail.

2. Experimental

Nanopowders of    were prepared by a sol-gel (citrate-gel) method, which is based on the chelation of the metal cations by citric acid in a solution of water. The specified amount of Fe(NO₃)₃·9H₂O; La(NO₃)₃·6H₂O; and Nd(NO₃)₃·6H₂O was first dissolved in citric acid solution and then mixture was stirred slowly and kept at a temperature of 70°C until the reaction mixture became clear. To completely create compound matters, ammonium solution was added drop by drop at a time until the pH reached 6 and 7. The complete dissolution of the salts resulted in a transparent solution. After continuously stirring for 2 hours the brown semitransparent sol was produced, and then the solution containing La, Fe, and Nd cations was homogenized; the solution became more viscous as the temperature was continuously kept at 70°C, without showing any visible phase separation. This resin was placed in a furnace and dried to 120°C for 4 h in air to pulverize into powders. The crystalline phase was obtained by heating the powder 500°C for 10 h in air.

Structural characterization was performed by means of X-ray diffraction using a D5005 diffractometer with Cu K radiation and with varied in the range of 10–70° at a step size of 0.02°. The particle size and morphology of the calcined powders were examined by SEM (-4800), Hitachi-Japan.

The fabrication of thick films, structure of sensor prototypes, and measuring conditions were described in [17]. In order to improve their stability and repeatability, the thick film sensors were calcined at 400°C for 2 h in air. The gas sensitivity of sensors was measured in a temperature range of 100°C–300°C. Their resistance was measured in air with test gas equipment. The response, , was defined by the following equation:

where is the resistance of sensor measured in air and is the resistance of sensors measured in the test gas equipment.

3. Result and Discussion

XRD patterns of the   samples were shown in Figure 1. All of them are single phase, with orthorhombic structure (space group Pnma). The wide diffraction peaks (in position of 2 about 32-33°) show that the samples have small grain size. The a-cell parameter versus Nd content is presented in Figure 2, and it can be seen that the a-cell parameter of the samples decreases with the increase of Nd doping concentration. The lattice distortion may be caused by the radius of (0.127 Å) that is smaller than one of (0.136 Å). It leads to the decrease of the lattice parameters with increase of the Nd concentration (Figure 2).

Figure 1: XRD patterns of nanoparticles after annealing in air at 500°C for 10 hours.

Figure 2: a-Cell parameter versus Nd content.

The crystalline sizes (nm) of the samples are calculated by Scherrer formula:

where is the average size of crystalline particle, assuming that particles are spherical, , is the wavelength of X-ray radiation, is full width at half maximum of the diffracted peak, and is angle of diffraction.

The cell parameters and the crystalline sizes of powdersare shown in Table 1. These small grain sizes of the    nanopowders are favourable for preparing the thick film sensors.

Table 1: The cell parameters and crystallite sizes of powders.

Compounds
(Å)
(Å)
(Å)
(Å)³
(nm)

0
LaFeO₃
5.5656
5.2544
7.5659
221.256
20.31

0.15
La0.85Nd0.15FeO₃
5.5538
5.2432
7.5498
219.850
19.62

0.30
La0.7Nd0.3FeO₃
5.54500
5.2350
7.5379
218.811
21.24

0.50
La0.5Nd0.5FeO₃
5.5406
5.2308
7.5319
218.280
19.34

1
NdFeO₃
5.5046
5.1967
7.4829
214.050
17.40

The thick film sensors were prepared by using the nanopowder and their ethanol-sensing characters were studied. The resistance of these sensors was examinated with the different temperatures and ethanol concentrations. Figure 3 presents the temperature dependence of resistance of thick film sensors based on the nanosized in the temperature range from 160°C to 300°C in air. It is suggested that the electrical conductivity mechanism is small polaron hopping process [18, 19] following the equation

where is constant relating to carrier concentration, is the temperature, is the Boltzmann constant, and is activation energy. Figure 4 shows the temperature dependent on conductivity and Figure 5 demonstrates the Arrhenius plots of conductivities of the samples. From Figure 5 the activation energy can be calculated (Table 2).

Table 2: The Activation energy () of the electrical conduction process.

(0 ≤ ≤ 1.0)
= 0.0
= 0.15
= 0.3
= 0.5
= 1.0

(kJ mol⁻¹)
27
28
26
27
20

Figure 3: Resistance versus temperature of  () measured in air.

Figure 4: Electrical conductivity versus temperature of  () measured in air.

Figure 5: Arrhenius plots of electrical conductivity for   ().

It is noted that the resistance was decreased with increasing temperature due to an intrinsic characteristic of a semiconductor. This would result from the ionization of oxygen vacancies. LaFeO₃ and doped-LaFeO₃ are the kind of p-type semiconductive material [20].

When the sensor is exposed to ethanol, the ethanol reacts with the chemisorbed oxygen, releasing electrons back to the valence band, decreasing the holes concentration, and increasing resistance [16]. Figure 6 depicts the response and recovery curve of when exposed to 0.25 mg/L ethanol at 212°C. The response and recovery times of this sensor are relatively short. The doping at A site caused a disorder in structure and oxygen deficiency can occur during heating sample at high temperature. On the other hand, interacts with the oxygen, by transferring the electrons from the valence band to adsorbed oxygen atoms, forming ionic species such as or . The electron transferring from the valence band to the chemisorbed oxygen results in an increase in holes concentration and a reduction in resistance of these sensors.

Figure 6: Response and recovery curve of when exposed to 0.25 mg/L ethanol at 212°C.

The temperature dependence of the sensor responses to 0.25 mg/L ethanol is shown in Figure 7. We found that the sensors’ sensitivity increases with Nd replaced concentration. On the other hand, the temperature, at which sensor responses reach maximum value, decreases with increasing Nd replaced concentrations. All sensors showed excellent ethanol-sensing characteristics. The response of was positive; this suggests that the semiconductivity is p-type behavior. Mechanism of gas-sensing is based on the oxidation-reduction on the surface of the material. The absorbed accelerates the reaction:

This should give an increase in and thus increase the sensitivity of these sensors [9–13].

Figure 7: Temperature dependence of the response in 0.25 mg/L ethanol of sensors.

Figure 8 presents the dependence of the response upon the concentration of ethanol at 182°C for the sensor. The change of electric resistance of the sensor is strongly affected by an increase in ethanol gas concentration.

Figure 8: Ethanol concentration dependence of response of at 182°C.

4. Conclusion

The perovskite compounds with orthorhombic perovskite structure were prepared successfully by gel-citrate method. With increasing of the Nd replaced concentrations, both the particle size and a-cell parameter of the samples decrease. The nanocrystallite materials were manufactured thick film sensors and studied ethanol-sensing characters. All sensors showed excellent ethanol-sensing characteristics. The lattice structure of is strongly distorted, and this leads to the change of the ethanol-sensing characters as function of replaced Nd concentrations.

Conflict of Interests

The authors declare that there is no conflict of interests regarding the publication of this paper.

Acknowledgment

This work was supported by Vietnam’s National Foundation for Science and Technology Development (NAFOSTED) with the project code “103.03.69.09.”

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