# Structure and Property Investigation of Composite ZnO/SnO2 Nanocrystalline Particles after High-Pressure Treatment

Authors: Sun Zhenya; Deng Yundi; Zhang Weiying
Journal: Journal of Nanomaterials
 (2008)

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## Abstract

Composite ZnO/SnO2 nanocrystalline particles (ZnO/SnO2) were synthesized by sol-gel method and with treatment of high pressure at 6 GPa. The crystallinity and the particle size of the prepared samples were analyzed by X-ray diffraction (XRD) spectroscopy. The results indicated that all the samples had the good crystallinity, and the particle size of ZnO and ZnO/SnO2 decreased after high-pressure treatment. The infrared (IR) spectra showed that the distance of crystal lattice was shortened after high-pressure treatment, and the size distribution became more uneven after SnO2 doping. With the high-resolution transmission electron microscope (HRTEM), we got some morphology information and evidence to support the IR and XRD analysis results. The results of ultraviolet-visible absorption (UV-Vis) spectra showed that ZnO/SnO2 might improve the photocatalytic property of the samples after high-pressure treatment.


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## Body

## 1. Introduction

People gradually realize that pollutants in water should be removed urgently.
There are two common techniques to treat such wastewater: one is adsorption and
the other is chemical coagulation. However, these methods merely transfer
pollutants from the liquid to the solid phase causing secondary pollution and
requiring further treatment.On the other hand, as a new technique the photocatalytic
method can be conveniently applied toward the degradation of pollutants such as
dye, without causing secondary pollution. Photogenerated carriers (electrons
and holes) in a semiconductor particle can tunnel to a reaction medium and can participate in
chemical reactions. Photocatalysis depends on the energy of the electron-hole
pairs and the extent of their separation. While TiO2 is widely
employed as a photocatalyst, composite material may be more suitable than TiO2 attributing to different band gap which can effectively reduce the
recombination of electron-hole pairs [1]. High-pressure treatment is a new
attempt to improve photocatalytic property which may change particle structure
and excite particle quantum effect to induce decreasement of the recombination
of electron-hole pairs.ZnO/SnO2 is a kind of excellent photocatalyst [2].
Many experiments proved that simple ZnO/SnO2 mixture system [3, 4]
and complex system (e.g., SnO2 gel/ZnO system [5], Zn2SnO4(ZnSnO3) nanocrystal [6, 7]) both have very good effect. However,
their structure and properties after high-pressure treatment were not reported
so far. In this study, ZnO/SnO2 was prepared by sol-gel method,
using zinc acetate dihydrate, oxalic acid, and stannous chloride as raw
materials. Then, samples were treated under high pressure at 6 GPa.


## 2. Experimental

### 2.1. Preparation of ZnO/SnO2

ZnO/SnO2 was prepared by the following method.
Oxalic acid ((COOH)2·2H2O)
solution and stannous chloride(SnCl2·2H2O)
solution were prepared with absolute ethyl alcohol as the solvent. The stannous
chloride solution was slowly added to the oxalic acid solution with stirring.
Then, zinc acetate dihydrate solution was slowly added to the mixture solution
(with the molar ratio of ZnO : SnO2 = 100 : 3). The resultant solution
was aged for 2 hours to obtain the required sol. The sol was heated at 75°C for 12 hours to produce the gel which should
be dried over for at least one day, followed by annealing in air at 500°C for 2 hours and
cooling to room temperature at last. Pure ZnO was also prepared by a similar
method [8].


### 2.2. High-Pressure Procedure

Cubic anvil press was used as high-pressure equipment which
can generate a pressure up to 6 GPa. The samples were assembled in a cube block,
and the assembly steps were as follows [9]. At first, powder was processed into
a rotund piece using low-pressure molding which was then put into the carbon
pipe center with the sodium chloride (NaCl) piece filled in. At last, assembled
pipe was put into pyrophyllite block center and also was covered with pyrophyllite. Figure 1
shows the overall assembled cube block.Figure 1
sketch diagram of assembled cube block (1)
pyrophyllite, (2) carbon pipe, (3) NaCl piece, and (4) sample piece.Assembled sample was put into the
center of the cubic anvil press, boosted for 2 minutes, kept pressure for 30 minutes,
decompressed for 3 minutes, and then was taken out.


### 2.3. Characterization of Assynthesized Samples

The mean crystallite size,d, was measured from the XRD (D/MAX-YB,
RIGAKU) peaks at a scanning rate of 15°/min based
on Scherrer's equation:(1)d=0.89λβ⁢cos⁡θ, where λ is the wavelength of the X-rays, θ is the diffraction angle, and β is the full width at half maximum.IR spectra (60SXB, Nexus) were also used to characterize the samples,
and the crystal morphology and micromechanism of the asprepared powder were
characterized by HRTEM (JEM-2100F,
JEOL Corporation). Absorption spectra were recorded with a spectrophotometer
(UV-Vis Spectrophotometer 754PC, Shanghai Spectrophotometer Instruments Co, LTD). The band gap energy was calculated by the following equation:(2)λg=1240Eg, where λg is the wavelength of the characteristic
absorption peak value; Eg is the band gap energy.


## 2.1. Preparation of ZnO/SnO2

ZnO/SnO2 was prepared by the following method.
Oxalic acid ((COOH)2·2H2O)
solution and stannous chloride(SnCl2·2H2O)
solution were prepared with absolute ethyl alcohol as the solvent. The stannous
chloride solution was slowly added to the oxalic acid solution with stirring.
Then, zinc acetate dihydrate solution was slowly added to the mixture solution
(with the molar ratio of ZnO : SnO2 = 100 : 3). The resultant solution
was aged for 2 hours to obtain the required sol. The sol was heated at 75°C for 12 hours to produce the gel which should
be dried over for at least one day, followed by annealing in air at 500°C for 2 hours and
cooling to room temperature at last. Pure ZnO was also prepared by a similar
method [8].


## 2.2. High-Pressure Procedure

Cubic anvil press was used as high-pressure equipment which
can generate a pressure up to 6 GPa. The samples were assembled in a cube block,
and the assembly steps were as follows [9]. At first, powder was processed into
a rotund piece using low-pressure molding which was then put into the carbon
pipe center with the sodium chloride (NaCl) piece filled in. At last, assembled
pipe was put into pyrophyllite block center and also was covered with pyrophyllite. Figure 1
shows the overall assembled cube block.Figure 1
sketch diagram of assembled cube block (1)
pyrophyllite, (2) carbon pipe, (3) NaCl piece, and (4) sample piece.Assembled sample was put into the
center of the cubic anvil press, boosted for 2 minutes, kept pressure for 30 minutes,
decompressed for 3 minutes, and then was taken out.


## 2.3. Characterization of Assynthesized Samples

The mean crystallite size,d, was measured from the XRD (D/MAX-YB,
RIGAKU) peaks at a scanning rate of 15°/min based
on Scherrer's equation:(1)d=0.89λβ⁢cos⁡θ, where λ is the wavelength of the X-rays, θ is the diffraction angle, and β is the full width at half maximum.IR spectra (60SXB, Nexus) were also used to characterize the samples,
and the crystal morphology and micromechanism of the asprepared powder were
characterized by HRTEM (JEM-2100F,
JEOL Corporation). Absorption spectra were recorded with a spectrophotometer
(UV-Vis Spectrophotometer 754PC, Shanghai Spectrophotometer Instruments Co, LTD). The band gap energy was calculated by the following equation:(2)λg=1240Eg, where λg is the wavelength of the characteristic
absorption peak value; Eg is the band gap energy.


## 3. Results and Discussion

### 3.1. XRD Spectra Analysis

Figure2 shows the XRD spectra of different samples: pure
ZnO, pure ZnO after high-pressure procedure, ZnO/SnO2, and ZnO/SnO2 after high-pressure procedure. The Sn peaks were not observed in the spectra
because the concentration of Sn was too low. The diffraction peaks were in good
agreement with those given in the standard data (PCPDF, 79-0207) for ZnO and
showed a good crystallinity. This means that asprepared materials had
crystallized in a hexagonal wurtzite ZnO (see Table 1).Table 1
the XRD parameters of (h k l), andd-value of standard wurtzite phase ZnO and samples.
(h k l)Int-fPCPDF79-0207ZnOZnO/6GZnO/SnO2ZnO/SnO2/6Gd(nm)d(nm)d(nm)d(nm)d(nm)(1 0 0)5700.282040.282200.282720.282200.28203(0 0 2)4160.260620.261070.261510.260920.26078(1 0 1)9990.248060.248200.248600.248200.24793(1 0 2)2100.191410.191400.191630.191400.19133(1 1 0)2910.162840.162680.162840.162680.16263(1 0 3)2510.147930.147840.148010.147880.14835(1 1 2)2030.138100.137960.138030.140820.14052Figure 2
X-ray diffraction spectra of pure ZnO, pure ZnO
after high pressure, ZnO/SnO2, and ZnO/SnO2 after high-pressure procedure.As shown in Figure2, the peak width of pure ZnO/6G and ZnO(SnO2)/6G is obviously wider than that of ZnO
and ZnO(SnO2) because of high-pressure effect. For the mean
crystallite size, d is in inverse proportion to the full width at half maximum β(d=0.89λ/(β⁢cos⁡θ)), indicating that the high-pressure
procedure can cause the initial grain size to decrease. Table 2 lists the
calculation results of the average particle size of the samples. About the
reason for the particle size decreasing, there are two possibilities. One is
that the high pressure can smash the particles and the other is that the high
pressure can make the crystallite more dense by grain squeeze.Table 2
Average particle size of different sample.
SampleZnOZnO/6GZnO(SnO2)ZnO(SnO2)/6GSize17.2216.2019.6814.50The peak intensity of pure ZnO and ZnO/SnO2 also
changed after high-pressure procedure, which reveals that the high pressure may
affect the orientation of the samples, but this part needs further in-depth
study.


### 3.2. IR Spectra Analysis

Figure3 shows the IR spectra of different samples. From the
figure, it can be seen that peaks occur around wavenumber 400 cm-1 and 500 cm-1 which are
due to stretching mode of ZnO. After high-pressure treatment, the
characteristic peak of ZnO moved from wavenumber 438 cm-1 to 451 cm-1, and the characteristic
peak of ZnO/SnO2 moved from wavenumber 441 cm-1 to 453 cm-1. It
was said that the characteristic peaks of both pure ZnO and ZnO/SnO2 showed blue shift after high-pressure treatment. It was also noticed that the
characteristic peak width of ZnO/6G is broader than that of ZnO, and the peak width of ZnO(SnO2) and
ZnO(SnO2)/6G is wider than that of ZnO and ZnO/6G.Figure 3
IR spectra of pure ZnO, pure ZnO after high-pressure
procedure, ZnO/SnO2 and ZnO/SnO2 after high-pressure
procedure.There are a few reasons to explain the above two phenomena. Peaks occurred with blue shift indicate
that high pressure may improve the samples crystallinity and shorten the
distance of crystal lattice, which causes enhancing of the field effect of
crystal and increasing of the band vibration frequency. In this theory, we
exclude the assumption that the decrease of particle size is caused by smashing
effect. On the peaks width, it may be caused by interfacial effect and size
distribution effect. After high-pressure treatment, the particle interface
defects increased, and the size distribution was more disordered. The
characteristic peaks of ZnO(SnO2) and ZnO(SnO2)/6G are wider than those of ZnO and ZnO/6G,
respectively, because of interfacial effect and size distribution effect.


### 3.3. Morphology and Micromechanism

From the HRTEM image of ZnO (a), it can be seen that the
particles show a homogeneous size of 18 nm, consistent with the XRD results
(17.22 nm). Figure4(b) shows the good crystallinity of ZnO, also consistent
with the XRD results.HRTEM images of different samples. (a) ZnO morphology
image, (b) ZnO crystal lattice image, (c) ZnO/6G crystal lattice image, (d) ZnO/6G crystal lattice image.
(a)(b)(c)(d)Compared with ZnO images, there was some difference in ZnO/6G images (Figures4(c) and 4(d)).
Deformation area near the crystal grain boundary is obvious in Figures 4(c) and
4(d). Maybe it was caused by squeezing between crystals. From Figure 4(c), it
can be seen that the crystal lattice was distorted by the grain squeeze below,
while the area in Figure 4(d) was distorted by the grain squeeze above, which
reveals that deformation always occurs around crystalline exterior. So, it can
be supposed that the decrease of particle size was caused partially by particle
squeeze.Figures5(a) and 5(b) show the ZnO/SnO2 morphology and
microstructure. In Figure 5(a), the big particles are ZnO which
are about 20 nm, while SnO2 particles are much smaller about several nanometers.
The ZnO particles were surrounded by SnO2 particles. So, this
microstructure could improve photocatalytic properties [1]. Because of uneven
size, the characteristic peak of ZnO/SnO2 in IR spectra was wider than that of pure ZnO.HRTEM image of different samples. (a) ZnO/SnO2 morphology image, (b) ZnO/SnO2 crystal lattice image, (c) ZnO (SnO2)/6G crystal lattice image, and (d) ZnO
(SnO2)/6G crystal
lattice image.
(a)(b)(c)(d)In Figures5(c) and 5(d), the
deformation areas of ZnO/SnO2 particles were obvious. Compared with
pure ZnO after high-pressure treatment, the deformation area of ZnO/SnO2 was more complicated. Probably, the particle size of ZnO/SnO2 was
more uneven than that of pure ZnO, and the grain squeeze was more complicated.
Moreover, the particle gap was smaller than that of pure ZnO, indicating a
greater degree of compression, which was in agreement with the XRD result
(Table 2).


### 3.4. UV-Vis Spectra and Band Gap Energy

The UV-Vis spectra of the samples are displayed in Figure6.
The top absorption peak of both ZnO and ZnO/SnO2 occurs at the
wavelength of 380 nm (3.26 eV). The band gap energy of ZnO/SnO2 was little
changed after doping SnO2 particles, and the intrinsic absorption peak of SnO2 did not
appear, which may be due to the reunion phenomenon of the SnO2 particles. For the
composite structure, the UV absorption strength of ZnO/SnO2 was
higher than that of ZnO. After high-pressure treatment, the characteristic
absorption peak values of ZnO and ZnO/SnO2 increased with obvious blue
shift, which are at wavelength of 368 nm (3.37 eV) and 366 nm (3.39 eV),
respectively. It revealed that after high-pressure procedure, the band gap
energy of ZnO and ZnO/SnO2 increased so that it can decrease the
recombination of electron-hole pairs effectively. For the inverse relationship
between the recombination efficiency of electron-hole pairs and the
photocatalytic property, it can be inferred that after high-pressure procedure ZnO/SnO2 has some benefits
for photocatalytic property.Figure 6
UV-Vis absorption spectra of pure ZnO, pure ZnO
after high-pressure procedure, ZnO/SnO2, and ZnO/SnO2 after high-pressure procedure.


## 3.1. XRD Spectra Analysis

Figure2 shows the XRD spectra of different samples: pure
ZnO, pure ZnO after high-pressure procedure, ZnO/SnO2, and ZnO/SnO2 after high-pressure procedure. The Sn peaks were not observed in the spectra
because the concentration of Sn was too low. The diffraction peaks were in good
agreement with those given in the standard data (PCPDF, 79-0207) for ZnO and
showed a good crystallinity. This means that asprepared materials had
crystallized in a hexagonal wurtzite ZnO (see Table 1).Table 1
the XRD parameters of (h k l), andd-value of standard wurtzite phase ZnO and samples.
(h k l)Int-fPCPDF79-0207ZnOZnO/6GZnO/SnO2ZnO/SnO2/6Gd(nm)d(nm)d(nm)d(nm)d(nm)(1 0 0)5700.282040.282200.282720.282200.28203(0 0 2)4160.260620.261070.261510.260920.26078(1 0 1)9990.248060.248200.248600.248200.24793(1 0 2)2100.191410.191400.191630.191400.19133(1 1 0)2910.162840.162680.162840.162680.16263(1 0 3)2510.147930.147840.148010.147880.14835(1 1 2)2030.138100.137960.138030.140820.14052Figure 2
X-ray diffraction spectra of pure ZnO, pure ZnO
after high pressure, ZnO/SnO2, and ZnO/SnO2 after high-pressure procedure.As shown in Figure2, the peak width of pure ZnO/6G and ZnO(SnO2)/6G is obviously wider than that of ZnO
and ZnO(SnO2) because of high-pressure effect. For the mean
crystallite size, d is in inverse proportion to the full width at half maximum β(d=0.89λ/(β⁢cos⁡θ)), indicating that the high-pressure
procedure can cause the initial grain size to decrease. Table 2 lists the
calculation results of the average particle size of the samples. About the
reason for the particle size decreasing, there are two possibilities. One is
that the high pressure can smash the particles and the other is that the high
pressure can make the crystallite more dense by grain squeeze.Table 2
Average particle size of different sample.
SampleZnOZnO/6GZnO(SnO2)ZnO(SnO2)/6GSize17.2216.2019.6814.50The peak intensity of pure ZnO and ZnO/SnO2 also
changed after high-pressure procedure, which reveals that the high pressure may
affect the orientation of the samples, but this part needs further in-depth
study.


## 3.2. IR Spectra Analysis

Figure3 shows the IR spectra of different samples. From the
figure, it can be seen that peaks occur around wavenumber 400 cm-1 and 500 cm-1 which are
due to stretching mode of ZnO. After high-pressure treatment, the
characteristic peak of ZnO moved from wavenumber 438 cm-1 to 451 cm-1, and the characteristic
peak of ZnO/SnO2 moved from wavenumber 441 cm-1 to 453 cm-1. It
was said that the characteristic peaks of both pure ZnO and ZnO/SnO2 showed blue shift after high-pressure treatment. It was also noticed that the
characteristic peak width of ZnO/6G is broader than that of ZnO, and the peak width of ZnO(SnO2) and
ZnO(SnO2)/6G is wider than that of ZnO and ZnO/6G.Figure 3
IR spectra of pure ZnO, pure ZnO after high-pressure
procedure, ZnO/SnO2 and ZnO/SnO2 after high-pressure
procedure.There are a few reasons to explain the above two phenomena. Peaks occurred with blue shift indicate
that high pressure may improve the samples crystallinity and shorten the
distance of crystal lattice, which causes enhancing of the field effect of
crystal and increasing of the band vibration frequency. In this theory, we
exclude the assumption that the decrease of particle size is caused by smashing
effect. On the peaks width, it may be caused by interfacial effect and size
distribution effect. After high-pressure treatment, the particle interface
defects increased, and the size distribution was more disordered. The
characteristic peaks of ZnO(SnO2) and ZnO(SnO2)/6G are wider than those of ZnO and ZnO/6G,
respectively, because of interfacial effect and size distribution effect.


## 3.3. Morphology and Micromechanism

From the HRTEM image of ZnO (a), it can be seen that the
particles show a homogeneous size of 18 nm, consistent with the XRD results
(17.22 nm). Figure4(b) shows the good crystallinity of ZnO, also consistent
with the XRD results.HRTEM images of different samples. (a) ZnO morphology
image, (b) ZnO crystal lattice image, (c) ZnO/6G crystal lattice image, (d) ZnO/6G crystal lattice image.
(a)(b)(c)(d)Compared with ZnO images, there was some difference in ZnO/6G images (Figures4(c) and 4(d)).
Deformation area near the crystal grain boundary is obvious in Figures 4(c) and
4(d). Maybe it was caused by squeezing between crystals. From Figure 4(c), it
can be seen that the crystal lattice was distorted by the grain squeeze below,
while the area in Figure 4(d) was distorted by the grain squeeze above, which
reveals that deformation always occurs around crystalline exterior. So, it can
be supposed that the decrease of particle size was caused partially by particle
squeeze.Figures5(a) and 5(b) show the ZnO/SnO2 morphology and
microstructure. In Figure 5(a), the big particles are ZnO which
are about 20 nm, while SnO2 particles are much smaller about several nanometers.
The ZnO particles were surrounded by SnO2 particles. So, this
microstructure could improve photocatalytic properties [1]. Because of uneven
size, the characteristic peak of ZnO/SnO2 in IR spectra was wider than that of pure ZnO.HRTEM image of different samples. (a) ZnO/SnO2 morphology image, (b) ZnO/SnO2 crystal lattice image, (c) ZnO (SnO2)/6G crystal lattice image, and (d) ZnO
(SnO2)/6G crystal
lattice image.
(a)(b)(c)(d)In Figures5(c) and 5(d), the
deformation areas of ZnO/SnO2 particles were obvious. Compared with
pure ZnO after high-pressure treatment, the deformation area of ZnO/SnO2 was more complicated. Probably, the particle size of ZnO/SnO2 was
more uneven than that of pure ZnO, and the grain squeeze was more complicated.
Moreover, the particle gap was smaller than that of pure ZnO, indicating a
greater degree of compression, which was in agreement with the XRD result
(Table 2).


## 3.4. UV-Vis Spectra and Band Gap Energy

The UV-Vis spectra of the samples are displayed in Figure6.
The top absorption peak of both ZnO and ZnO/SnO2 occurs at the
wavelength of 380 nm (3.26 eV). The band gap energy of ZnO/SnO2 was little
changed after doping SnO2 particles, and the intrinsic absorption peak of SnO2 did not
appear, which may be due to the reunion phenomenon of the SnO2 particles. For the
composite structure, the UV absorption strength of ZnO/SnO2 was
higher than that of ZnO. After high-pressure treatment, the characteristic
absorption peak values of ZnO and ZnO/SnO2 increased with obvious blue
shift, which are at wavelength of 368 nm (3.37 eV) and 366 nm (3.39 eV),
respectively. It revealed that after high-pressure procedure, the band gap
energy of ZnO and ZnO/SnO2 increased so that it can decrease the
recombination of electron-hole pairs effectively. For the inverse relationship
between the recombination efficiency of electron-hole pairs and the
photocatalytic property, it can be inferred that after high-pressure procedure ZnO/SnO2 has some benefits
for photocatalytic property.Figure 6
UV-Vis absorption spectra of pure ZnO, pure ZnO
after high-pressure procedure, ZnO/SnO2, and ZnO/SnO2 after high-pressure procedure.


## 4. Conclusion

In this work, the ZnO/SnO2 powders were synthesized by
sol-gel method and treated by high-pressure procedure. The X-ray diffraction
(XRD) spectra of the samples showed that the nanocrystals had good
crystallinity, and the size decreased after high-pressure treatment. The
infrared (IR) spectra showed that the distance of crystal lattice was shortened
after high-pressure treatment, and the size distribution became more uneven
after doping. Through high-resolution transmission electron microscope (HRTEM),
some morphology information and evidence support to IR spectroscopic analysis
results were obtained. The UV-Vis spectra of the samples showed that ZnO/SnO2 has some benefits
for photocatalytic property after high-pressure procedure.



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*Source: 286069-2008-05-08.xml*