Scholarly article on topic ' Synthesis and Characterization of     Sb  2   S 3    Nanorods via Complex Decomposition Approach '

Synthesis and Characterization of Sb 2 S 3 Nanorods via Complex Decomposition Approach Academic research paper on "Nano-technology"

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Academic research paper on topic " Synthesis and Characterization of Sb 2 S 3 Nanorods via Complex Decomposition Approach "

Hindawi Publishing Corporation Journal of Nanomaterials Volume 2011, Article ID 414798, 6 pages doi:10.1155/2011/414798

Research Article

Synthesis and Characterization of Sb2S3 Nanorods via Complex Decomposition Approach

Abdolali Alemi,1 Younes Hanifehpour,1,2 and Sang Woo Joo2

1 Department of Inorganic Chemistry, Faculty of Chemistry, University of Tabriz, Tabriz 51664, Iran

2 WCUNano Research Center, School of Mechanical Engineering, Yeungnam University, Gyeongsan 712-749, Republic of Korea Correspondence should be addressed to Sang Woo Joo, swjoo@yu.ac.kr

Received 27 May 2011; Accepted 17 July 2011 Academic Editor: Somchai Thongtem

Copyright © 2011 Abdolali Alemi 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.

Based on the complex decomposition approach, a simple hydrothermal method has been developed for the synthesizing of Sb2S3 nanorods with high yield in 24h at 150°C. The powder X-ray diffraction pattern shows the Sb2S3 crystals belong to the orthorhombic phase with calculated lattice parameters a = 1.120nm, b = 1.128nm, and c = 0.383 nm. The quantification of energy dispersive X-ray spectrometric analysis peaks give an atomic ratio of 2 : 3 for Sb: S. TEM and SEM studies reveal that the appearance of the as-prepared Sb2S3 is rod-like which is composed of nanorods with the typical width of 30-160 nm and length of up to 6 ,wm. High-resolution transmission electron microscopic (HRTEM) studies reveal that the Sb2S3 is oriented in the [10-1] growth direction. The band gap calculated from the absorption spectra is found to be 3.29 ev, indicating a considerable blue shift relative to the bulk. The formation mechanism of Sb2S3 nanostructures is proposed.

1. Introduction

Recently, metal chalcogenides have attracted considerable attention due to their proven and potential applications in electronic, optical, and superconductor devices. Among these materials, antimony sulfide (Sb2S3) is a kind of semiconductor with its interesting high photosensitivity and high thermoelectric power. Antimony sulfide is a layer-structured direct bandgap semiconductor with orthorhombic crystal structure [1]. Sb2S3 is considered as a promising material for solar energy due to its band gap which covers the range of the solar spectrum [2]. Sb2S3 has been extensively investigated for its special applications as a target material for microwave devices [3], television cameras and switching devices [4], rechargeable storage cell [5], and various optoelectronic devices [6]. Over the past two decades, many methods have been employed to prepare Sb2S3 including thermal decomposition [7], solvothermal reaction [8-11], microwave irritation [12], hydrothermal reaction [13, 14], and vacuum evaporation [15]. Besides an elemental reaction and vacuum evaporation, Sb2S3 can be prepared by chemical

routes. SbCl3 reacts with different sulfide ion sources, such as ammonium sulfide, thiourea, sodium thiosulfate, and thioacetamide as well as with complexing agents in aqueous or nonaqueous solutions [16, 17]. However, most of the as-prepared Sb2S3 materials are amorphous, and they need to be annealed at high temperature in air or in N2 atmosphere in order to crystallize. In addition, crystalline Sb2S3 can be obtained directly via two-heater method [18] and liquidmediated metathetical reactions [19]. But different method has its disadvantage. For the vacuum evaporation and direct elemental reaction methods, it is difficult to obtain exact stoichiometric compositions because of the differences in the vapor pressures of the reaction species. Consequently, exploring a convenient synthesis method is significant [20]. Recently, we have reported a new method via redox mechanism by using starting materials in elemental form [14]. Several morphologies of Sb2S3 have been reported, for example, microspheres, microtubes [21], dendrite or feather [22], dumbbell-like [23], and also peanut-shaped superstructures [24]. In this study, Sb2S3 nanorods were prepared by complex decomposition approach via hydrothermal method.

1-1-1-1-r

4 7 10 13 16 19 22 25 28 31 34 37 40 43 46 49 52 55 58 61 64 67 70

Figure 1: XRD patterns of the Sb2S3 nanorods synthesized at 150° C for 24 h.

Energy (KeV)

Figure 2: EDX patterns of synthesized Sb2S3 nanorods synthesized at 150°C for 24 h.

2. Experimental

2.1. Synthesis of Sb2 S3 Nanorods. All the reagents were of analytical grade and were used without further purification. In a typical procedure, 0.4 g CS2, 0.6 g EDTA, and 1 g NaOH were added to 50 mL distilled water and stirred well for 20 min at room temperature. Then, 1 mmol of SbCl3 was added to above mixture and the mixture was transferred into a 100 mL Teflon-lined autoclave. The autoclave was sealed a, maintained at 150° C for 24 h, and cooled at room temperature, naturally. The black precipitate was filtered and washed with dilute chloride acid and water. Then, it was dried at room temperature. Yields for the products were 96%. Finally, the obtained sample was dried at room temperature and used for characterization. The best conditions for this reaction are pH = 10, temperature 150° C, and time of reaction 24 h. Under other conditions, some impurity is seen in XRD patterns and EDS related to unreacted raw elements or formation of antimony oxides. The crystal structure of the product was characterized by X-ray diffraction (XRD D500 Simens) with CuKa radiation

Figure 3: SEM images of the Sb2S3 nanorods in (a) low and (b) high magnifications synthesized at 150° C and 24 h.

35 30 25 20 15 10 5

(25.2 nm) 40.5 nm Si

Figure 4: AFM image of Sb2S3 nanorods synthesized at 150°C for 24 h.

(A = 1.5418 A). The morphology of materials was examined by a scanning electron microscope SEM (Hitachi S-4200).The HRTEM image and SAED pattern were recorded by a Cs-corrected high-resolution TEM (JEM-2200FS,JEOL) operated at 200 kV. The TEM sample was prepared by using an FIB (Helios Nanolab, FEI). Elemental analysis was carried out using a linked ISIS-300, Oxford EDS (energy dispersion

300 350 400 450 400 450 500 550 600 650

Wavelength (nm) Wavelength(nm)

(a) (b)

Figure 6: (a) Excitation spectra and (b) emission spectra of Sb2S3 nanorods.

Figure 7: UV/Vis spectra of Sb2S3 nanorods.

spectroscopy detector). Optical measurements were carried out by a Perkin-Elmer lambda UV/Vis spectrophotometer (model specord 400) and the photoluminescence were done by a perkin-Elmer Ls 55 luminescence spectrometer.

3. Results and Discussion

A typical XRD of the as-prepared Sb2S3 is shown in Figure 1. All the peaks in the pattern can be indexed to an orthorhombic phase with lattice parameters a = 1.122nm, b = 1.128 nm, and c = 0.384 nm. The intensity and positions of the peaks are in good agreement with the values reported in the literature (JCPDS card File: 42-1393). No characteristic peaks are observed for other impurities such as antimony oxides, or SbOCl.

Figure 2 shows a typical EDXA spectrum recorded on single crystals, whose peaks are assigned to Sb and S. The EDX analysis of the product confirms the ratio of Sb/S to be 2:3, as expected. According to EDX analysis, no impurity such as elemental antimony, antimony oxides or SbOCl is observed.

The crystal size (CS) is calculated from X-ray diffraction patterns using Scherer's formula (CS = KX/fi cos в, where в is the full width at the half maximum of peak corrected for instrumental broadening, X is the wavelength of the X-ray and K is Scherrer's constant) [25]. The grain size was

+ S=C=S + NaOH

^Na+eS:

SbCl3 + 3H2O

Sb(OH)3 + 3HCl

Sb(OH)3 + S--

S Sb S

—S S^—S o. O-^S

Temperature

-> Sb2S3

Pressure

S^TO O S

Scheme 1: Possible chemical reaction in the synthesis of Sb2S3 nanorods.

22 nm. The morphology of the prepared Sb2S3 was examined by scanning electron microscopy. SEM images with different magnification shows that the length of Sb2S3 nanorods is up to 6^m and 30-160 nm as diameter (Figures 3(a) and 3(b)).

Also, Figure 4 shows atomic force microscopic image of as-prepared Sb2S3 with rode like structure and phase homogeneity.

Figure 5(a) shows TEM image of as-prepared Sb2S3 nanorods. Also, the typical HRTEM image recorded from the same nanorods is shown in Figure 5(b). The crystal lattice fringes are clearly observed and average distance between the neighboring fringes is 0.79 nm, corresponding to the [1 1 0] plane lattice distance of orthorhombic-structured Sb2S3, which suggests that Sb2S3 nanorods grow along the [1 0 -1] direction. The SAED pattern of the nanorods indicates that its single-crystal nature and long axis is [1 0 -1] (Figure 5(c)).

To explain the synthesis process, possible chemical reaction involved in the synthesis of Sb2S3 could be listed in Scheme 1.

First, EDTA was reacted with CS2 in water for 12 h to give a clear solution, which was precipitated in ethanol. The product was recrystallized in methanol: chlorophorm (1:1) mixture and characterized by FTIR spectroscopy. This is a thiocarbonate ester of EDTA, which seems to act as a ligand to form an intermediate complex of Sb3+, as confirmed by similar FTIR spectroscopy. Such an intermediate complex is isolated by heating of a reaction mixture of CS2, EDTA, NaOH, and SbCl3 in water under hydrothermal condition for 1 h. The resultant mixture was filtered and the obtained precipitate was identified by FTIR spectroscopy.

Comparison of the FTIR spectra shows that the same bands indicate some shift due to the complexation of the ligand. The line positions (in cm-1) of v = 691 C-S stretching, v = 1174 esteric band, v = 1250 C-N stretching (tertiary amine) in case of ligand shifts to v = 888 C-S stretching, v = 1119 esteric band, v = 1283 C-N stretching (tertiary amine) due to complexation. After 24 h exposing to heat and pressure, the resultant Sb3+ complex will be degraded completely to form the Sb2S3 compound. The

EDX result (see Figure 2) shows that no organic compound remains in the sample. In semiconductors, band gaps have been found to be particle-size dependent and increase with decreasing of particle size [26]. As Sb2S3 is a narrow band gap semiconductor (Eg is 1.7 ev for bulk), with decreasing in diameter into nanoscale, novel optical properties may be observed. The photoluminescence (PL) spectrum of synthesized antimony sulfide, shown in Figure 6, has an excitation peak at 390nm (Figure 6(a)), and the emission peak can be observed at 415, 442 and 475nm (Figure 6(b)).

The absorption spectra of Sb2S3 (prepared by dispersion of Sb2S3 nanorods in ethanol) show an intense absorption band at 315 nm with band gap around 3.29 ev (Figure 7). A blue shift phenomena is seen for Sb2S3 nanorods.

Most of the materials have different structural defects that create defect energy levels between band gaps of material. These defects result in difference of the UV absorption and PL excitation spectra.

4. Conclusion

In summary, a complex decomposition approach in hydrothermal condition has been developed to prepare Sb2S3 nanorods with high yield. The length of the nanorods is up to 6 ^m and their diameter is around 30-160 nm. Single crystals could be obtained by increasing of heating time up to 48 h. High-resolution transmission electron microscopic (HRTEM) studies reveal that the Sb2S3 is oriented in the [10-1] growth direction. A blue shift was observed in the case of optical absorption and PL, common feature for na-nomaterials.

Acknowledgments

This work is funded by the World Class University Grant KRF R32-2008-000-20082-0 of the National Research Foundation of Republic of Korea. Y. Hanifehpour thanks the Council of the University of Tabriz for their invaluable guidance.

References

[1] I. H. Kim, "(Bi,Sb)2(Te,Se)3-based thin film thermoelectric generators," Materials Letters, vol. 43, no. 5-6, pp. 221-224, 2000.

[2] L. Chen, W. Zhu, Q. Han,X. Yang, L. Lu, andX. Wang, "Preparation of rod-like Sb2S3 dendrites processed in conventional hydrothermal," Materials Letters, vol. 63, no. 15, pp. 12581261,2009.

[3] J. Grigas, J. Meshkauskas, and A. Orliukas, "Dielectric properties of Sb2S3 at microwave frequencies," Physica Status Solidi A, vol. 37, no. 1, pp. k39-k41, 1976.

[4] K. Y. Rajpure and C. H. Bhosale, "Sb2S3 semiconductor-septum rechargeable storage cell," Materials Chemistry and Physics, vol. 64, no. 1, pp. 70-74, 2000.

[5] M. J. Chockalingam, K. Nagaraja, and N. Rangarajan, "Studies on sintered photoconductive layers of antimony trisulphide," Journal of Physics D, vol. 3, no. 11, pp. 1641-1645, 1970.

[6] L. M. Sander, "Fractal growth processes," Nature, vol. 322, no. 1,pp. 789-793, 1986.

[7] M. Lalia-Kantouri, A. G. Marison, and G. E. Manoussakis,

"Thermal decomposition oftris(N, N-disubstituted dithiocar-bamate) complexes of As(III), Sb(III) and Bi(III)," Journal of Thermal Analysis and Calorimetry, vol. 29, no. 5, pp. 11511169,1984.

[8] J. Yang, J. H. Zeng, S. H. Yu, L. Yang, and Y. H. Zhang, "Pressure-controlled fabrication of stibnite nanorods by the solvothermal decomposition ofa simple single-source precursor," Chemistry of Materials, vol. 12, no. 10, pp. 2924-2929, 2000.

[9] W. Lou, M. Chen, X. Wang, and W. Liu, "Novel single-source precursors approach to prepare highly uniform Bi2S3 and Sb2S3 nanorods via a solvothermal treatment," Chemistry of Materials, vol. 19, no. 4, pp. 872-878, 2007.

[10] S. H. Yu, L. Shu, Y. T. Wu, and Y. T. Qian, "Benzene-thermal synthesis and characterization of ultrafine powders of antimony sulfide," Materials Research Bulletin, vol. 33, no. 8, pp. 1207-1211, 1998.

[11] X. Zheng, Y. Xie, L. Zhu, X. Jiang, Y. Jia, and W. Song, "Growth of Sb2E3 (E = S, Se) polygonal tubular crystals via a novel solvent-relief-self-seeding process," Inorganic Chemistry, vol. 41, no. 3, pp. 455-461,2002.

[12] Y. Yu, R. H. Wang, Q. Chen, and L. M. Peng, "High-quality ultralong Sb2S3 nanoribbons on large scale," Journal of Physical Chemistry B, vol. 109, no. 49, pp. 23312-23315, 2005.

[13] C. Li, X. Yang, Y. Liu, Z. Zhao, and Y. Qian, "Growth of crystalline Sb2S3 nanorods by hydrothermal method," Journal of Crystal Growth, vol. 255, no. 3-4, pp. 342-347, 2003.

[14] A. Alemi, S. W. Joo, Y. Hanifehpour, A. Khandar, A. Morsali, and B. Min, "Hydrothermal synthesis of Sb2S3 nanorods using iodine via redox mechanism," Journal of Nanomaterials, vol. 2011, Article ID 186528, 5 pages, 2011.

[15] O. Savadogo and K. C. Mandal, "Studies on new chemically deposited photoconducting antimony trisulphide thin films," Solar Energy Materials and Solar Cells, vol. 26, no. 1-2, pp. 117136, 1992.

[16] K. Y. Rajpure andC. H. Bhosale, "Effect of composition on the structural, optical and electrical properties of sprayed Sb2S3 thin films prepared from non-aqueous medium," Journal of Physics and Chemistry of Solids, vol. 61, no. 4, pp. 561-568, 2000.

[17] A. M. Salem and M.S. Selim, "Structure and optical properties of chemically deposited Sb2S3 thin films," Journal of Physics D, vol. 34, no. 1,pp. 12-17, 2001.

[18] C. Kaito, Y. Saito, and K. Fujita, "Studies on the structure and morphology of ultrafine particles of metallic sulfides," Journal ofCrystal Growth, vol. 94, no. 4, pp. 967-977, 1989.

[19] C. J. Carmalt, D. E. Morrison, and I. P. Parkin, "Liquidmediated metathetical synthesis of indium and antimony oxides and chalcogenides," Main Group Metal Chemistry, vol. 22, no. 4, pp. 263-268, 1999.

[20] H. Yang, X. Su, and A. Tang, "Microwave synthesis of nanocrystalline Sb2S3 and its electrochemical properties," Materials Research Bulletin, vol. 42, no. 7, pp. 1357-1363, 2007.

[21] Y. Xu, Z. Ren, G. Cao, W. Ren, K. Deng, and Y. Zhong, "A template-free route for controlled synthesis of dumbbell-like Sb2S3 microcrystals," Crystal Research and Technology, vol. 44, no. 8, pp. 851-856, 2009.

[22] H. Hu, Z. Liu, B. Yang, M. Mo, and W. Yu, "Solvothermal growth of Sb2S3 microcrystallites with novel morphologies," Journal ofCrystal Growth, vol. 262, no. 1-4, pp. 375-382, 2004.

[23] Q. Lu, H. Zeng, X. Cao, and L. Zhang, "Design of Sb2S3 nanorod-bundles: imperfect oriented attachment," Nanotech-nology, vol. 17, no. 9, pp. 2098-2104, 2006.

[24] Q. Han, L. Chen, W. Zhu, X. Yang, and L. Lu, "Synthesis of

Sb2S3 peanut-shaped superstructures," Materials Letters, vol. 63, no. 12, pp. 1030-1032, 2009.

[25] N. Benramdane, M. Latreche, and H. Tabet, "Structural and optical properties of spray-pyrolysed Bi2S3 thin films," Materials Science and Engineering B, vol. 64, no. 2, pp. 84-87, 1999.

[26] A. M. Qin, U. P. Fang, and W. X. Zhao, "Directionally dendritic growth of metal chalcogenide crystals via mild template-free solvothermal method," Journal of Crystal Growth, vol. 283, no. 1-2, pp. 230-241,2005.

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