# Synthesis and Characterization of Single-Crystalline SnO2 Nanowires

Authors: Dezhou Wei; Yanbai Shen; Mingyang Li; Wengang Liu; Shuling Gao; Lijun Jia; Cong Han; Baoyu Cui
Journal: Journal of Nanomaterials
 (2013)

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## Abstract

Tin oxide (SnO2) nanowires were synthesized on oxidized silicon substrates by thermal evaporation of tin grains at 900°C in Ar flow at ambient pressure. Structural characterization using X-ray diffraction and transmission electron microscopy shows that SnO2 nanowires have a single crystal tetragonal structure. Scanning electron microscopy observation demonstrates that SnO2 nanowires are 30–200 nm in diameter and several tens of micrometers in length. The surface vibration mode resulting from the nanosize effect at 565.1 cm−1 was found from the Fourier transform infrared spectrum. The formation of SnO2 nanowires follows a vapour-solid (VS) growth mechanism. The gas sensing measurements indicate that SnO2 nanowire gas sensor obtains peak sensitivity at a low operating temperature of 150°C and shows reversible response to H2 gas (100–1000 ppm) at an operating temperature of RT-300°C.


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## Body

## 1. Introduction

In recent years, much more attention has been focused on the research field of quasi-one-dimensional nanostructural materials due to their importance for understanding the fundamental properties of low dimensionality and the wide range of their potential applications in nanodevices [1, 2]. SnO2, as an n-type wide band gap semiconductor material (Eg=3.6 eV at 300 K), is a key functional material that has been used extensively for transparent conductors [3, 4], gas sensors [5, 6], transistors [7], solar cells [8], and optoelectronic devices [9, 10]. So far, considerable efforts have been devoted to the research on the synthesis and characterization of SnO2 nanomaterials such as nanowires [11, 12], nanotubes [13], nanorods [14], and nanobelts [15, 16] by using various synthetic methods. Among these methods, thermal evaporation is widely used because of its simple operation, low cost in preparation, and large-scale production.Sn
O
2 nanomaterials are very promising for gas sensors due to their advantageous characteristics of large surface-to-volume ratio and great surface activity. Gas sensors based on SnO2 nanomaterials have shown higher sensitivity, faster response, and enhanced capability to detect low concentration gases compared with the corresponding thin film materials [16, 17]. However, most of them are effective at high temperature above 200°C, which results in high power consumption and complexities in integration. Therefore, there is a need to develop SnO2 nanomaterials for gas sensors that have good performance at a low temperature. In addition, much more efforts have been devoted to study the CO, NO2, or ethanol gas sensing properties of SnO2 nanomaterials [15–20], and only a few reports were related to H2 gas sensing properties [21–23]. Deshpande et al. [21] reported that Pt-catalyst SnO2 nanowires could detect 500 ppm H2 gas with response time as low as 10 sec at RT. Wang et al. [22] reported that the response of SnO2 naonwires to 500 ppm H2 gas could be repeated without observing major changes in the signal at RT. Kolmakov et al. [23] reported that individual Pd-functionalized SnO2 naonwires and nanobelts exhibited a dramatic improvement in the sensitivity toward oxygen and hydrogen at 200 and 270°C. However, in their works, the responses of SnO2 naonwires were investigated only under the fixed temperature and H2 concentration.In this study, single-crystallineSnO2 naonwires were synthesized by thermal evaporation of tin grains at 900°C in an Ar flow at ambient pressure. Structural characterization of the obtained SnO2 naonwires was investigated by using X-ray diffraction, scanning electron microscopy, and transmission electron microscopy. The Fourier transform infrared spectrum and growth mechanism of the nanowires were also investigated and discussed. The measurements of H2 gas sensing properties demonstrated that SnO2 nanowire gas sensor obtained peak sensitivity at a low operating temperature of 150°C and showed reversible response to H2 gas (100–1000 ppm) at an operating temperature of RT-300°C.


## 2. Experimental

Sn
O
2 nanowires were synthesized on oxidized Si substrates by thermal evaporation of tin grains. Tin grains with high purity of 99.9% were placed on oxidized Si substrates in an alumina boat. No catalysts or impurities were introduced. The alumina boat was introduced at the center of a quartz tube that was inserted in a horizontal tube furnace. Ar gas with a flow rate of 50 mLmin-1 was introduced into the quartz tube at ambient pressure. Then, the furnace was heated to 900°C and maintained at this temperature for 1 h. After the furnace was cooled down to room temperature naturally, a layer of wire-shaped products was obtained on the substrates around the tin grains, as shown in Figure 1(a).(a) Photograph of the obtainedSnO2 nanowires. (b) Schematic illustration of SnO2 nanowire gas sensor device.
(a)
(b)The crystallographic structure ofSnO2 nanowires was studied by means of glancing angle X-ray diffractometer (GAXRD) (Shimadzu XRD-6100) with Cu Kα radiation. The morphology was observed by field emission scanning electron microscope (FESEM) (JEOL JSM-6700F). The microstructure and components were investigated by transmission electron microscope (TEM) (JEOL EM002B) with an energy dispersive X-ray spectrometer (EDX). The Fourier transform infrared (FTIR) spectrum was measured by infrared spectrometer (Shimadzu IRPrestige-21).Sn
O
2 nanowire gas sensor was fabricated by pouring a few drops of nanowire-suspended ethanol onto oxidized Si substrate with a pair of interdigitated Pt electrodes. The schematic illustration of a SnO2 nanowire gas sensor device is shown in Figure 1(b). H2 gas sensing properties were measured in a quartz tube inserted in an electric furnace at the operating temperatures ranging from room temperature (RT ≈ 25°C) to 300°C. As shown in Figure 2, dry synthetic air mixed with the desired concentration of H2 gas flowed through the quartz tube at a rate of 200 mL min-1. The electrical measurement was carried out by a volt-amperometric method at a constant bias of 10 V, and a multimeter (Agilent 34970A) was used to monitor the change of electrical resistance upon turning H2 gas on and off. In this study, the sensor sensitivity was defined as  S=(Ra-Rg)/Rg, where Ra and Rg were the electrical resistances before and after the introduction of H2 gas, respectively.Figure 2
Apparatus used for the measurement ofH2 gas sensing properties.


## 3. Results and Discussion

### 3.1. Structure and Morphology

The XRD pattern of the obtainedSnO2 nanowires is shown in Figure 3. All the diffraction peaks can be indexed to the tetragonal SnO2 structure with lattice constants of a=b=0.4738 nm and c=0.3187 nm according to JCPDS card no. 41-1445. Moreover, no other crystalline forms such as Sn or SnO are detected, indicating that single phase SnO2 nanowires are obtained.Figure 3
XRD pattern ofSnO2 nanowires.Figure4(a) is a typical FESEM image of SnO2 nanowires, showing that a large quantity of wire-shaped nanostructures can be produced. It is found that SnO2 nanowires have diameters ranging from 30 to 200 nm and have lengths of several tens of micrometers. A high magnification FESEM image shown in Figure 4(b) indicates that SnO2 nanowires have smooth sidewalls.(a) Low magnification and (b) high magnification FESEM images ofSnO2 nanowires.
(a)
(b)Figure5(a) is a typical TEM image of a single SnO2 nanowire with a diameter of 96 nm. A high-resolution TEM (HRTEM) image of this nanowire is shown in Figure 5(b), in which the lattice planes can be clearly seen, indicating a single crystal structure. The interplanar spacing of 0.34 nm corresponds to the (110) plane in a tetragonal SnO2 structure. The corresponding selected area electron diffraction (SAED) pattern shown in Figure 5(c) also supports the formation of single crystal tetragonal SnO2 nanowires. The growth direction of SnO2 nanowires is found to be [301], which is consistent with previous reports [24, 25]. To demonstrate the chemical composition of the nanowire, EDX analysis was performed, and the EDX spectrum is illustrated in Figure 5(d). We can see that, except for the Cu element from the copper grid, only peaks of Sn and O elements are observed.Figure 5
(a) TEM image of a single SnO2 nanowire with a diameter of 96 nm. (b) HRTEM image of this nanowire. (c) SAED pattern of this nanowire. (d) EDX analysis of this nanowire.


### 3.2. The Growth Mechanism

Two models have been proposed to describe the growth mechanism ofSnO2 nanowires: the catalyst-assisted vapour-liquid solid (VLS) and the vapour-solid (VS) growth mechanisms [2]. The VLS mechanism was first proposed by Wagner and Ellis in 1964 [26]. The important feature of the VLS growth process is the existence of metal nanoparticles. The nanoparticles serve as catalysts between the vapour feed and the solid product and usually locate at the ends of the produced nanowires [27]. In this study, no metal catalysts were employed, and no metal nanoparticles were observed at any ends of SnO2 nanowires. Therefore, the growth process might be dominated by the VS growth mechanism. At a high temperature of 900°C, tin grains are vaporized and then directly condensed on the substrates. Once the condensation process happens, the initial condensed molecules form seed crystals serving as the nucleation sites. As a result, they facilitate directional growth to minimize the surface energy [2]. Therefore, SnO2 nanowires tend to be produced by continuous aggregation of more molecular SnO2 on the growth front of the initial SnO2 nuclei via the VS growth mechanism [28].


### 3.3. FTIR Spectrum

The FTIR spectrum ofSnO2 nanowires is shown in Figure 6. Compared with the data published in the literatures [29–31], the peaks observed can be determined. The peaks located at 603.7 and 692.4 cm-1 can be attributed to the Sn–O stretching vibration in SnO2. The peaks at 665.4 and 705.9 cm-1 can be assigned to O–Sn–O bending vibration. The peak at 565.1 cm-1 is noticeable because it cannot be found in the FTIR spectrum of bulk SnO2 and is similar to the surface vibration mode of the peak at 564 cm-1 in SnO2 nanopowders resulting from the nanosize effect [32]. This surface vibration mode is related to the change of the surface structure. When the influence of the volume atoms on the lattice energy of surface atoms decreases, the surface tensile stress decreases, leading to the renormalization of the surface atoms and forming the new vibration mode [31, 32].Figure 6
FTIR spectrum ofSnO2 nanowires.


### 3.4. H2 Gas Sensing Properties

Sn
O
2 nanowires are very promising due to their large surface-to-volume ratio and great surface activity, which make them ideal candidates for gas sensing materials. Figure 7 shows the sensitivity of SnO2 nanowire gas sensor as a function of the operating temperature upon exposure to 1000 ppm H2 gas. It is found that the sensitivity increases with increasing operating temperature below 150°C, but reverse tendency is observed after 150°C. At this optimum temperature of 150°C, the highest sensitivity of 5.54 is obtained. It should be noted that the value of this peak sensitivity is larger than that of a porous SnO2 sputtered thin film deposited at 24 Pa and RT upon exposure to 1000 ppm H2 gas [33]. In addition, the sensitivity value is comparable to the one found in [22] and is even higher than the value reported in [21, 23] for SnO2 nanowires, showing that the obtained SnO2 nanowires are good for gas sensing application.Figure 7
The sensitivity ofSnO2 nanowire gas sensor as a function of the operating temperature upon exposure to 1000 ppm H2 gas.Figure8 shows the dynamic responses of SnO2 nanowire gas sensor to H2 gas with various concentrations at 150°C. One can see that the resistance decreases upon exposure to H2 gas and the resistance further decreases with increasing H2 concentration. In addition, the resistance can recover to its initial value after removing H2 gas, indicating a good reversibility of SnO2 nanowire gas sensor. The resistance changes of 0.86, 1.68, 2.98, 3.61, 4.19, and 5.54 times with respect to the baseline are observed towards 100, 200, 400, 600, 800, and 1000 ppm H2 gas, respectively. The sensor also shows reversible response to H2 gas with different concentrations at an operating temperature of RT-300°C, although the corresponding data are not shown in this figure.Figure 8
Dynamic response ofSnO2 nanowire gas sensor to H2 gas with various concentrations at 150°C.The relationship between the sensor sensitivity andH2 concentration at the operating temperature of 150°C is shown in Figure 9. It is found that the sensitivity increases as H2 concentration increases. Such a variation implies that the sensitivity Scan be described as a function of gas concentration C by an empirical model of S=aCb, where a and b are constants for a given gas. In this study, “a” and “b” were found to be 0.065±0.034 and 0.629±0.079, respectively. We see that the experimental data and the theoretical curve obtained from the empirical model show good agreement.Figure 9
The relationship between the sensor sensitivity andH2 concentration at the operating temperature of 150°C.


## 3.1. Structure and Morphology

The XRD pattern of the obtainedSnO2 nanowires is shown in Figure 3. All the diffraction peaks can be indexed to the tetragonal SnO2 structure with lattice constants of a=b=0.4738 nm and c=0.3187 nm according to JCPDS card no. 41-1445. Moreover, no other crystalline forms such as Sn or SnO are detected, indicating that single phase SnO2 nanowires are obtained.Figure 3
XRD pattern ofSnO2 nanowires.Figure4(a) is a typical FESEM image of SnO2 nanowires, showing that a large quantity of wire-shaped nanostructures can be produced. It is found that SnO2 nanowires have diameters ranging from 30 to 200 nm and have lengths of several tens of micrometers. A high magnification FESEM image shown in Figure 4(b) indicates that SnO2 nanowires have smooth sidewalls.(a) Low magnification and (b) high magnification FESEM images ofSnO2 nanowires.
(a)
(b)Figure5(a) is a typical TEM image of a single SnO2 nanowire with a diameter of 96 nm. A high-resolution TEM (HRTEM) image of this nanowire is shown in Figure 5(b), in which the lattice planes can be clearly seen, indicating a single crystal structure. The interplanar spacing of 0.34 nm corresponds to the (110) plane in a tetragonal SnO2 structure. The corresponding selected area electron diffraction (SAED) pattern shown in Figure 5(c) also supports the formation of single crystal tetragonal SnO2 nanowires. The growth direction of SnO2 nanowires is found to be [301], which is consistent with previous reports [24, 25]. To demonstrate the chemical composition of the nanowire, EDX analysis was performed, and the EDX spectrum is illustrated in Figure 5(d). We can see that, except for the Cu element from the copper grid, only peaks of Sn and O elements are observed.Figure 5
(a) TEM image of a single SnO2 nanowire with a diameter of 96 nm. (b) HRTEM image of this nanowire. (c) SAED pattern of this nanowire. (d) EDX analysis of this nanowire.


## 3.2. The Growth Mechanism

Two models have been proposed to describe the growth mechanism ofSnO2 nanowires: the catalyst-assisted vapour-liquid solid (VLS) and the vapour-solid (VS) growth mechanisms [2]. The VLS mechanism was first proposed by Wagner and Ellis in 1964 [26]. The important feature of the VLS growth process is the existence of metal nanoparticles. The nanoparticles serve as catalysts between the vapour feed and the solid product and usually locate at the ends of the produced nanowires [27]. In this study, no metal catalysts were employed, and no metal nanoparticles were observed at any ends of SnO2 nanowires. Therefore, the growth process might be dominated by the VS growth mechanism. At a high temperature of 900°C, tin grains are vaporized and then directly condensed on the substrates. Once the condensation process happens, the initial condensed molecules form seed crystals serving as the nucleation sites. As a result, they facilitate directional growth to minimize the surface energy [2]. Therefore, SnO2 nanowires tend to be produced by continuous aggregation of more molecular SnO2 on the growth front of the initial SnO2 nuclei via the VS growth mechanism [28].


## 3.3. FTIR Spectrum

The FTIR spectrum ofSnO2 nanowires is shown in Figure 6. Compared with the data published in the literatures [29–31], the peaks observed can be determined. The peaks located at 603.7 and 692.4 cm-1 can be attributed to the Sn–O stretching vibration in SnO2. The peaks at 665.4 and 705.9 cm-1 can be assigned to O–Sn–O bending vibration. The peak at 565.1 cm-1 is noticeable because it cannot be found in the FTIR spectrum of bulk SnO2 and is similar to the surface vibration mode of the peak at 564 cm-1 in SnO2 nanopowders resulting from the nanosize effect [32]. This surface vibration mode is related to the change of the surface structure. When the influence of the volume atoms on the lattice energy of surface atoms decreases, the surface tensile stress decreases, leading to the renormalization of the surface atoms and forming the new vibration mode [31, 32].Figure 6
FTIR spectrum ofSnO2 nanowires.


## 3.4. H2 Gas Sensing Properties

Sn
O
2 nanowires are very promising due to their large surface-to-volume ratio and great surface activity, which make them ideal candidates for gas sensing materials. Figure 7 shows the sensitivity of SnO2 nanowire gas sensor as a function of the operating temperature upon exposure to 1000 ppm H2 gas. It is found that the sensitivity increases with increasing operating temperature below 150°C, but reverse tendency is observed after 150°C. At this optimum temperature of 150°C, the highest sensitivity of 5.54 is obtained. It should be noted that the value of this peak sensitivity is larger than that of a porous SnO2 sputtered thin film deposited at 24 Pa and RT upon exposure to 1000 ppm H2 gas [33]. In addition, the sensitivity value is comparable to the one found in [22] and is even higher than the value reported in [21, 23] for SnO2 nanowires, showing that the obtained SnO2 nanowires are good for gas sensing application.Figure 7
The sensitivity ofSnO2 nanowire gas sensor as a function of the operating temperature upon exposure to 1000 ppm H2 gas.Figure8 shows the dynamic responses of SnO2 nanowire gas sensor to H2 gas with various concentrations at 150°C. One can see that the resistance decreases upon exposure to H2 gas and the resistance further decreases with increasing H2 concentration. In addition, the resistance can recover to its initial value after removing H2 gas, indicating a good reversibility of SnO2 nanowire gas sensor. The resistance changes of 0.86, 1.68, 2.98, 3.61, 4.19, and 5.54 times with respect to the baseline are observed towards 100, 200, 400, 600, 800, and 1000 ppm H2 gas, respectively. The sensor also shows reversible response to H2 gas with different concentrations at an operating temperature of RT-300°C, although the corresponding data are not shown in this figure.Figure 8
Dynamic response ofSnO2 nanowire gas sensor to H2 gas with various concentrations at 150°C.The relationship between the sensor sensitivity andH2 concentration at the operating temperature of 150°C is shown in Figure 9. It is found that the sensitivity increases as H2 concentration increases. Such a variation implies that the sensitivity Scan be described as a function of gas concentration C by an empirical model of S=aCb, where a and b are constants for a given gas. In this study, “a” and “b” were found to be 0.065±0.034 and 0.629±0.079, respectively. We see that the experimental data and the theoretical curve obtained from the empirical model show good agreement.Figure 9
The relationship between the sensor sensitivity andH2 concentration at the operating temperature of 150°C.


## 4. Conclusions

Single-crystallineSnO2 nanowires were synthesized on oxidized silicon substrates by thermal evaporation of tin grains at 900°C. The structural characteristics, growth mechanism, and H2 gas sensing properties of SnO2 nanowires were investigated. SnO2 nanowires with a tetragonal structure are 30–200 nm in diameter and several tens of micrometers in length. The nanosize effect induced FTIR surface vibration mode with peak at 565.1 cm-1 was observed. The formation of SnO2 nanowires follows a vapour-solid (VS) growth mechanism. SnO2 nanowire gas sensor shows reversible response to H2 gas at an operating temperature of RT-300°C. The peak sensitivity is found at a low operating temperature of 150°C. The sensor sensitivity increases empirically with an increase of H2 gas concentration. The results demonstrate the potential of SnO2 nanowires for gas sensor applications.



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*Source: 761498-2013-10-29.xml*