Article ID: 1003-6326(2005)03-0702-04
Preparation of antimony-doped nanoparticles
by hydrothermal method
JIANG Ming-xi(江名喜)1, YANG Tian-zu(杨天足)1, GU Ying-ying(古映莹)1,
DU Zuo-juan(杜作娟)1, LIU Jian-ling(刘建玲)2
(1. School of Metallurgical Science and Engineering,
Central South University, Changsha 410083, China;
2. College of Chemistry and Chemical Engineering, Hunan University, Changsha 410082, China)
Abstract: Antimony-doped tin oxide(ATO) nanoparticles were prepared by the mild hydrothermal method at 200℃ using sodium stannate, antimony oxide, sodium hydroxide and sulfuric acid as the starting materials. The doped powders were examined by differential thermal analysis(DTA), X-ray diffractometry(XRD) and transmission electron microscopy(TEM). The doping levels of antimony were determined by volumetric method and iodimetry. The results show that antimony is incorporated into the crystal lattice of tin oxide and the doping levels of antimony in the resulting powders are 2.4%, 4.3% and 5.1%(molar fraction). The mean particle size of ATO nanoparticles is in the range of 25-30nm. The effects of antimony doping level on the crystalline size and crystallinity were also discussed.
Key words: hydrothermal process; nanoparticle; antimony; doping; tin oxide CLC
number: TF123 Document code: A
1 INTRODUCTION
Tin oxide is an n-type semiconductor with a wide band gap of about 3.6eV and with the highest carrier mobility among the oxides[1]. Due to the advantageous electrical and optical properties, SnO2 ultrafine powders have been widely used for technical applications, such as gas sensors, burglar alarms and catalyst[2]. In order to improve the electrical and optical properties further, the doped tin oxide has been extensively investigated, especially for antimony and fluorine-doped tin oxide. The introduction of some amount of antimony into the crystal lattice of tin oxide can greatly increase the electronic conductivity and depress the growth of particles, while the optical property is not devastated. Antimony-doped tin oxide is widely used as the high-performance materials for the production of transparent electrodes[3, 4], energy storage device[5, 6], printed displays, liquid crystal displays, electrochromic displays[7-9], heating elements in aircraft, special furnaces and luminescent lamps etc[10-12].
At present, the main methods used for the synthesis of ATO nanometer powders are as follows: the solid-state reaction method[13], the sol-gel method[7], the coprecipitation method[14-17] and the hydrothermal method[18-20]. At the high reaction temperature for the solid-state method, the resulting powders are inhomogeneous distribution of the doped elements, large particle size and easiness to introduce other impurities, so it is rarely used for the preparation of ATO nanoparticles. For the co-precipitation method, a post-calcination at over 500℃ is required and this causes a large particle size and heavy agglomeration. Among the investigations on the preparation of ATO nanoparticles, the chlorides of tin and antimony, such as SnCl4, SnCl2, SbCl3 and SbCl5 are commonly employed as the starting materials. Chlorine ions are easily adsorbed on tin hydroxide and very difficult to be washed off. The residual chlorine ions are usually eliminated by calcinations at high temperature, which leads to the volatilization of antimony and tin, affects the surface and electrical properties of powders, introduces a random n-type doping in the material, and causes agglomeration among particles and difficulty for sintering[19]. So the starting materials free from chlorides should be considered for the preparation of ATO powders. The ATO powders with narrow particle size distribution, low coacervation, high purity and fine crystallization can be synthesized directly by the hydrothermal method without the necessity of calcination.
In this paper, sodium stannate, antimony oxide, sodium hydroxide and sulfuric acid are used as the starting materials for the preparation of ATO nanoparticles by the mild hydrothermal method.
2 EXPERIMENTAL
2.1 Preparation process
Given amounts of antimony oxide and sodium stannate were dissolved in 100mL sodium hydroxide solution of 200g/L and 100mL de-ionized water respectively. NaSbO2 solution and Na2SnO3 solution were mixed proportionally depending on the antimony doping level required. 35mL of the mixed solution was then dropped from a burette into a 100mL conical flask with 5mL de-ionized water in concurrent addition of 33%(volume fraction) sulfuric acid from the other burette, which was intensively agitated and heated at 60℃ by a magnetic stirrer.
The final pH value of the solution was kept at 1.5 for getting a light yellow suspensions of ATO precursor, and then the precursor was poured into a 100mL polytetrafluoroethylene-lined autoclave and heated at 200℃ for 8h. After that, the autoclave was quenched by tap water to the room temperature. The blue color powders were isolated by centrifugation, washed with de-ionized water until no SO2-4 could be detected(by 0.1mol/L BaCl2 solution). The final powders were rinsed three times with absolute alcohol and dried at 80℃, then ground in an agate mortar. The preparation process of ATO nanoparticles is shown in Fig.1.
Fig.1 Flowsheet for preparation of ATO nanoparticles by hydrothermal method
2.2 Characterization
The ATO powders with different doping levels were characterized by X-ray diffractometry(XRD), transmission electron microscopy(TEM) and differential thermal analysis(DTA). The crystal sizes, lattice parameters and lattice distortion rates of the powders were calculated.
3 RESULTS AND DISCUSSION
The reactions during the preparation of antimony-doped tin oxide are summarized as follows.
The antimony doping levels of the samples were determined by volumetric method and iodimetry. The doping levels for sample A, B and C are 5.1%, 4.3% and 2.4%(molar fraction), respectively.
Fig.2 shows the DTA curves of the samples. There are neither endothermic peaks nor exothermic peaks found in the DTA curves. This indicates that neither adsorptive water nor bonding water exist in the powders and the dehydration of the ATO precursor is carried out completely at 200℃. It also illustrates that the crystallographic form of the powders is very stable as there is no changes till about 900℃.
Fig.2 DTA curves of samples
The X-ray diffraction patterns of ATO nanoparticles are shown in Fig.3. The X-ray diffraction peaks of tin oxide are in good agreement with those of the tetragonal phase of rutile of tin oxide, without additional peaks belonging to other phases such as Sb2O3. The X-ray diffraction patterns indicate that all the antimony ions have been incorporated into the crystal lattice of tin oxide. The diffraction peaks are intensively broadened and the full peak width increases with the increase of the antimony doping level. The crystalline size of the powders is very small and decreases with the increase of the antimony doping level, while the crystallinity of ATO powders becomes low with the rising of antimony doping content. The mean crystalline size of the particles can be calculated from the [110] crystal planes by the Scherrer formula [21] .
Dhkl=(Kλ)/(10β cos θB)(7)
The results are listed in Table 1.
Fig.3 X-ray diffraction patterns of ATO nanoparticles synthesized at various antimony doping levels
Table 1 Mean crystalline size and unit cell parameters of ATO nanoparticles
The calculated results are listed in Table 1 and Table 2. The cell volume increases with the increase of the antimony doping level. The ionic radii of Sn4+, Sb5+ and Sb3+ are 0.071nm, 0.062nm and 0.092nm respectively. When doping, if antimony is incorporated into the lattice of tin oxide to substitute Sn4+ in the form of Sb5+, the unit cell of ATO nanoparticles would shrink for the ionic radius of Sb5+ is smaller than that of Sn4+ and it would expand when antimony enter into the lattice of tin oxide in the form of Sb3+ for the ionic radius of Sb3+ is larger than that of Sn4+. It is reported[7] that at the low doing level, most of the antimony ions exist in the form of Sb5+, thus the volume of unit cell will be smaller than that of pure tin oxide. With the Sb doping level rising, part of the antimony ions enter into the lattice in the form of Sb3+ and the Sb3+/Sb5+ ratio will increase with the antimony doping level, so the cell volume of tin oxide will expand accordingly. The volume of unit cell becomes larger than that of pure tin oxide when the antimony doping level reaches a certain degree. In the doping levels in this paper, the cell volumes of all the samples are smaller than that of pure tin oxide (71.52×10-3nm3)[9]. This illustrates that the antimony ions doped mainly exist in the form of Sb5+. The lattice distortion rate increases with the increase of antimony doping level. This is why the crystallinity of the ATO powders becomes lower as the doping level rises.
Figs.4(a) and (b) show the TEM images of the synthesized ATO nanoparticles. The average particle sizes of samples A and B are about 25nm and 30nm respectively.
Table 2 Lattice distortion rate(〈ε2〉1/2110/10-3) of samples
Fig.4 TEM images of ATO nanoparticles synthesized at 200℃
4 CONCLUSIONS
ATO powders with the mean particle size ranging 25-30 nm have been successfully prepared by the mild hydrothermal method free from chloride. Sulfuric acid was used as the precipitating agent. The effects of antimony doping level on the crystalline size and the crystallinity of ATO powders are also investigated. The experimental results show that the crystalline size decreases and the crystallinity becomes lower with the increase of Sb doping level.
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(Edited by YANG Bing)
Foundation item: Project(2001BA901A09) supported by the Key Program of Scientific and Technology Action of West China Development
Received date: 2004-10-28; Accepted date: 2005-01-07
Correspondence: JIANG Ming-xi, PhD candidate; Tel: +86-731-8836791; E-mail: jmingxi@yahoo.com