Skip to main content

Solvothermal Synthesis of Ternary Sulfides of Sb2 − xBi x S3(x = 0.4, 1) with 3D Flower-Like Architectures


Flower-like nanostructures of Sb2 − xBi x S3(x = 0.4, 1.0) were successfully prepared using both antimony diethyldithiocarbamate [Sb(DDTC)3] and bismuth diethyldithiocarbamate [Bi(DDTC)3] as precursors under solvothermal conditions at 180 °C. The prepared Sb2 − xBi x S3 with flower-like 3D architectures were characterized by X-ray diffraction (XRD), scanning electron microscopy (SEM), energy dispersive X-ray spectrometry (EDS), high-resolution transmission electron microscopy (HRTEM), and selected area electron diffraction (SAED). The flower-like architectures, with an average diameter of ~4 μm, were composed of single-crystalline nanorods with orthorhombic structures. The optical absorption properties of the Sb2 − xBi x S3 nanostructures were investigated by UV–Visible spectroscopy, and the results indicate that the Sb2 − xBi x S3 compounds are semiconducting with direct band gaps of 1.32 and 1.30 eV for x = 0.4 and 1.0, respectively. On the basis of the experimental results, a possible growth mechanism for the flower-like Sb2 − xBi x S3 nanostructures is suggested.


Semiconductor nanocrystals have attracted much attention in the past few decades [1, 2]. Among them, binary chalcogenide semiconductors of the A2VE3VI type (A=Sb, Bi; E=S, Se, Te) have aroused great interest due to their potential and practical applications in thermoelectric and optoelectronic devices. For example, bismuth sulfide (Bi2S3), which crystallizes in the orthorhombic system, is a direct band gap semiconductor with E.g. = 1.3 eV and can be applied in photovoltaic converters [3] and thermoelectric cooling technologies based on the Peltier effect [4]. At the same time, Bi2S3 nanocrystalline films have been found to significantly alter the performance of photochemical cells due to quantum size effects [5]. Moreover, antimony sulfide (Sb2S3), which is isostructural to Bi2S3, shows interesting high photosensitivity and high thermoelectric power [6], and its direct band gap of 1.5–2.50 eV covers the visible and near infrared range of the solar spectrum [79]. As a result, Sb2S3 has wide applications in solar energy conversion, thermoelectric cooling technologies, television cameras, microwave devices, switching devices, rechargeable storage cells, and optoelectronics in the infrared (IR) region [1013].

The band gap of a material determines its applicability as an optoelectronic material; therefore, tailoring of the band gap is very helpful. A usual approach to adjust the band gap is to synthesize materials on the nanoscale to take advantage of the quantum confinement effect. However, due to the low Bohr radius of most materials, the method is often far from effective. As an alternative, the band gap can also be tailored by adjusting the composition of materials. It is well known that in doped compound semiconductors, in contrast to undoped ones, the impurity states play a special role in the electronic energy structures and transition probabilities [14]. For doped nanocrystalline semiconductor compounds, confinement effects in the energy states also produce unusual physical and optical behavior. Recently, several research groups have reported the effects of the composition on the quantum efficiency of Zn1 − xMn x S and Cd x Zn1 − xS nanoparticles [1518]. In this paper, for the first time, we report the synthesis and band gap of Bi-doped Sb2S3 ternary sulfides, Sb2 − xBi x S3 (x = 0.4, 1.0) with flower-like nanostructures, prepared by a facile solvothermal method.


All the chemical reagents used in our experiments were of analytical grade and were used without further purification. The molecular precursors, antimony and bismuth diethyldithiocarbamate, Sb(DDTC)3 and Bi(DDTC)3, were prepared as follows: 0.01 mol of SbCl3[or Bi(NO3)3] and 0.02 mol of (C2H5)2NCS2Na·3H2O were dissolved in 100 mL of distilled water, respectively. Then, the two solutions were mixed by stirring in a 500-mL beaker. The resulting white precipitates were filtered, washed with distilled water, and dried in air at 60 °C.

In a typical procedure for synthesizing Sb2 − xBi x S3, the molecular precursors of Sb(DDTC)3 and Bi(DDTC)3 in the appropriate ratios (1 mmol in all) were put into a Teflon-lined stainless steel autoclave (30 mL capacity) to which 20 mL of ethylene glycol was added. The autoclave was sealed and maintained at 180 °C for 12 h; then it was allowed to cool to room temperature naturally. The as-formed black precipitates were separated by centrifugation, washed with ethanol and distilled water several times, and dried at 60 °C for 3 h.

The phase of the as-synthesized products was characterized using X-ray diffraction (XRD, Shimadzu XRD-6000) with Cu Kα radiation (λ = 1.5406 Å) at a scanning rate of 4º min −1. The X-ray tubes were operated with electric current of 30 mA and voltage of 40 kV. The composition, morphology, and sizes of the products were examined by field emission scanning electron microscopy (FESEM; JSM-7001), energy dispersive X-ray spectroscopy (EDS), and transmission electron microscopy (TEM; JEOL-2100). Samples for TEM were prepared by dropping the products on a carbon-coated copper grid after ultrasonic dispersion in absolute ethanol. The band gap energy of the products was determined from the onset of the absorbance spectra of the samples on a UV–Visible (UV–Vis) spectrophotometer with near IR (NIR) capability (Shimadzu UV-4100).

Results and Discussion

Figure 1 shows the XRD patterns of the as-synthesized products, and the diffraction peaks of both Sb2 − xBi x S3 samples can be indexed as orthorhombic phase structures with lattice constants of a = 11.182 Å,b = 11.378 Å, and c = 3.991 Å, and a = 11.151 Å,b = 11.375 Å, and c = 4.026 Å for x = 0.4 and 1.0 (Sb1.6Bi0.4S3 and SbBiS3), respectively. The XRD patterns are consistent with the orthorhombic phases Sb2S3(JCPDS: 42-1393) and Bi2S3(JCPDS: 17-0320). EDS analyses were employed to determine the chemical composition of the products. The EDS spectra (Fig. 2a, 2b) taken from the nanoflowers in SEM measurements show that both the samples are composed of S, Bi, and Sb elements with molar ratios (Bi:Sb) of about 1:4 and 1:1, respectively. To clarify whether the nanorods were pure Sb2 − xBi x S3 or a mixture of Bi2S3 and Sb2S3, EDS from individual nanorods was examined using TEM. As shown in Fig. 2c and 2d, each of the nanorods contained S, Bi, and Sb elements with a molar ratio similar to the case in SEM. The signals for Cu and C in the EDS spectra came from the carbon-coated copper grid used for TEM measurement. These results confirmed the successful preparation of bismuth and antimony ternary sulfides.

Figure 1
figure 1

XRD patterns of the flower-like Sb2 − xBi x S3: (a)x = 0.4; (b)x = 1

Figure 2
figure 2

EDS spectra of the Sb2 − xBi x S3 nanoflowers and individual nanorods shown in the respective insets: a, c x = 0.4; b, d x = 1

The overall morphology of the Sb1.6Bi0.4S3 is shown in Fig. 3a, which illustrates that the obtained products consist of a large number of flower-like nanostructures. After careful observation (Fig. 3b), it was found that the flower-like architectures consist of several nanorod bundles that are ~4 μm in length and extend toward many different directions. Furthermore, every nanorod bundle is made up of nanorods with a diameter of ~80 nm. The overall morphology of the SbBiS3 is shown in Fig. 3c. It can be seen that similar to the Sb1.6Bi0.4S3, the SbBiS3 products also consist of a large number of flower-like nanostructures. However, as shown in Fig. 3d, the flower-like architectures of SbBiS3 have a highly regular sphere-like morphology, which is obviously different from that of Sb1.6Bi0.4S3. The sphere-like structure with an average diameter of about 4 μm is composed of large numbers of nanorods, which grow radially from the central core and have a length of 2 μm and a diameter of about 100 nm.

Figure 3
figure 3

FESEM images of the flower-like Sb2 − xBi x S3: a, b x = 0.4; c, d x = 1

A further investigation of the Sb2 − xBi x S3 products was made by TEM. Figure 4a shows a typical TEM image of Sb1.6Bi0.4S3 flower-like architectures, which is consistent with the FESEM observations. After long ultrasonic treatment during the preparation of the TEM specimens, the flower-like structures were substantially unaffected. This suggests that the formation of the flower-like architectures is not due to aggregation. The microstructures of the Sb1.6Bi0.4S3 nanorods were investigated by high-resolution TEM (HRTEM) and selected area electron diffraction (SAED). The SAED pattern (Fig. 4b) taken from an individual nanorod indicated in the inset shows regular diffraction spots, which can be indexed as a orthorhombic Sb1.6Bi0.4S3 single crystal recorded from the [11–1] zone axis and demonstrates that the Sb1.6Bi0.4S3 nanorod grows along the [1-10] direction. As shown in Fig. 4c, the HRTEM image of the Sb1.6Bi0.4S3 nanorod shows clear lattice fringes with a d -spacing of 0.79 nm, which corresponds to the (110) lattice distance. Figure 4d shows a TEM image of the SbBiS3 sample. It can be seen that the SbBiS3 has a perfect sphere-like architecture consisting of nanorods, which is agreement with the FESEM observations. The nanorods extend radially from the central core and have less regular shapes (Fig. 4e). The SAED pattern (inset in Fig. 4e) taken from an individual nanorod shows that the SbBiS3 nanorod is single-crystalline. Figure 4f depicts a HRTEM image of the SbBiS3 nanorod. The clear lattice fringes with a d -spacing of 0.31 nm are consistent with that of the (211) planes of orthorhombic SbBiS3, further confirming that the SbBiS3 nanorod is single-crystalline.

Figure 4
figure 4

TEM, HRTEM, and SAED images of the Sb2 − xBi x S3: ac x = 0.4; df x = 1

In our previous study, Bi(DDTC)3 and Sb(DDTC)3 have been used as single-source molecular precursors for the syntheses of Bi2S3[19] and Sb2S3[20] nanomaterials, respectively. Considering the highly similar crystal structures of Bi2S3 and Sb2S3, we herein synthesized ternary sulfides Sb2 − xBi x S3 by using both Bi(DDTC)3 and Sb(DDTC)3 as precursors in a one-pot reaction. Based on the experimental observations, we infer that the formation process of the flower-like Sb2 − xBi x S3 nanostructures can be divided into three steps: First, under the solvothermal action, the precursors of Bi(DDTC)3 and Sb(DDTC)3 were decomposed and produced Sb2 − xBi x S3, which would form Sb2 − xBi x S3 crystal nuclei when the degree of supersaturation of the Sb2 − xBi x S3 reached a certain critical point. Secondly, these crystal nuclei grew and/or aggregated into a bigger core, which was thermodynamically favorable due to the decrease in the surface energy. Finally, the as-formed cores may serve as the substrates for epitaxial growth of the Sb2 − xBi x S3 nanorods. As a result, the flower-like architecture with Sb2 − xBi x S3 nanorods on its surface was formed. To check the proposed mechanism, we have done several parallel experiments with shorter reaction time of 10 and 6 h with the other synthetic conditions remaining unchanged. It was found that with the decrease of the reaction time, there were more separated nanorods in the products. This result is consistent with the formation mechanism of the Sb2 − xBi x S3 flowers.

Optical absorption experiments were carried out to elucidate the band gap energy, which is one of the most important electronic parameters for semiconductor nanomaterials. Figure 5 shows typical UV–Vis absorption spectra of the two samples. The λonset of the spectra recorded from the two samples are about 940 and 955 nm for x = 0.4 and 1.0, respectively. The band gap of the Sb2 − xBi x S3 may be estimated using the following formula:

where,α is the absorption coefficient, is the photon energy, B is a constant characteristic of the material, and E.g. is the band gap. The value of extrapolated to α = 0 gives the absorption band gap energy. The band gaps of the Sb2 − xBi x S3 are calculated to be 1.32 and 1.30 eV for x = 0.4 and 1.0, respectively, which are smaller than the values reported for pure Sb2S3, but are near to that of Bi2S3. The change in band gap energy probably result from the change in the composition of the Sb2 − xBi x S3, since the flower-like Sb2 − xBi x S3 nanostructures in our dimensional range should not show a quantum confinement effect due to the low Bohr radius of these materials. The flower-like Sb2 − xBi x S3 nanostructures with a narrow band gap may be very promising for applications in solar energy and photoelectronics.

Figure 5
figure 5

UV–Vis spectra of the Sb2 − xBi x S3: a x = 0.4; b x = 1. The insets contain the corresponding (αhν)2versus curves


In summary, we have developed a facile and mild solvothermal method for the large-scale preparation of ternary sulfide Sb2 − xBi x S3(x = 0.4, 1.0) flower-like nanostructures. The possible formation mechanism of the flower-like Sb2 − xBi x S3 is suggested. The optical properties of the Sb2 − xBi x S3 products were evaluated by UV–Vis spectroscopy at ambient temperature. The results indicate that the Sb2 − xBi x S3 compounds are semiconducting with direct band gaps of 1.32 and 1.30 eV for x = 0.4 and 1.0, respectively. This method can probably be extended to the fabrication of other ternary sulfide semiconductors nanostructures with various morphologies and functions.


  1. Tang KJ, Zhang JN, Yan WF, Li ZH, Wang YD, Yang WM, Xie ZK, Sun TL, Fuchs H: J. Amer. Chem. Soc.. 2008, 130: 2676. COI number [1:CAS:528:DC%2BD1cXhsFehsLk%3D] 10.1021/ja0778702

    Article  Google Scholar 

  2. Liu Y, Shen Q, Yu D, Shi W, Li J, Zhou J, Liu X: Nanotechnology. 2008, 19: 245601. COI number [1:CAS:528:DC%2BD1cXptFSiurs%3D]; Bibcode number [2008Nanot..19x5601L] 10.1088/0957-4484/19/24/245601

    Article  Google Scholar 

  3. Black J, Conwell EM, Seigle L, Spencer CW: J. Phys. Chem. Solids. 1957, 2: 240. COI number [1:CAS:528:DyaG1cXpvF2m]; Bibcode number [1957JPCS....2..240B] 10.1016/0022-3697(57)90090-2

    Article  Google Scholar 

  4. Chen BX, Uher C, Iordanidis L, Kanatzidis MG: Chem. Mater.. 1997, 9: 1655. COI number [1:CAS:528:DyaK2sXktlGqu74%3D] 10.1021/cm970033m

    Article  Google Scholar 

  5. Mane RS, Sankapal BR, Lokhande CD: Mater. Chem. Phys.. 1999, 60: 196. COI number [1:CAS:528:DyaK1MXkvVOlsrc%3D] 10.1016/S0254-0584(99)00085-1

    Article  Google Scholar 

  6. Yu Y, Wang RH, Chen Q, Peng LM: J. Phys. Chem. B. 2005, 109: 23312. COI number [1:CAS:528:DC%2BD2MXht1WmtLvI] 10.1021/jp055132z

    Article  Google Scholar 

  7. Roy B, Chakraborty BR, Bhattacharya R, Dutta AK: Solid State Commun.. 1978, 25: 937. COI number [1:CAS:528:DyaE1cXitVWrsL4%3D]; Bibcode number [1978SSCom..25..937R] 10.1016/0038-1098(78)90306-X

    Article  Google Scholar 

  8. Savadogo O, Manda KC: Solar Cells. 1992, 26: 117. COI number [1:CAS:528:DyaK38XksF2hs70%3D] 10.1016/0927-0248(92)90131-8

    Article  Google Scholar 

  9. Nair MTS, Pena Y, Campos J, Garica VM, Nair PK: J. Electrochem. Soc.. 1998, 141: 2113. 10.1149/1.1838605

    Article  Google Scholar 

  10. Geroge J, Radhakrishnan MK: Solid State Commun.. 1980, 33: 987. Bibcode number [1980SSCom..33..987G] Bibcode number [1980SSCom..33..987G] 10.1016/0038-1098(80)90296-3

    Article  Google Scholar 

  11. Savadogo O, Mandal KC: Electron. Lett.. 1992, 28: 1682. COI number [1:CAS:528:DyaK38Xms1ags74%3D] 10.1049/el:19921069

    Article  Google Scholar 

  12. Salem AM, Selim MS: J. Phys. D Appl. Phys.. 2001, 34: 12. COI number [1:CAS:528:DC%2BD3MXlvFGgtg%3D%3D]; Bibcode number [2001JPhD...34...12S] 10.1088/0022-3727/34/1/303

    Article  Google Scholar 

  13. Rajpure KY, Lokhande CD, Bhosale CH: Mater. Res. Bull.. 1999, 34: 1079. COI number [1:CAS:528:DyaK1MXmt1Wrsb8%3D] 10.1016/S0025-5408(99)00095-1

    Article  Google Scholar 

  14. Soo YL, Ming ZH, Huang SW, Kao YH: Phys. Rev. B. 1994, 50: 7602. COI number [1:CAS:528:DyaK2cXntFant7Y%3D]; Bibcode number [1994PhRvB..50.7602S] 10.1103/PhysRevB.50.7602

    Article  Google Scholar 

  15. Son D, Jung DR, Kim J, Moon T, Kim CJ, Park B: Appl. Phys. Lett.. 2007, 90: 101910. COI number [1:CAS:528:DC%2BD2sXjsValtLs%3D]; Bibcode number [2007ApPhL..90j1910S] 10.1063/1.2711709

    Article  Google Scholar 

  16. Ge JP, Wang J, Zhang HX, Wang X, Peng Q, Li YD: Adv. Funct. Mater.. 2005, 15: 303. COI number [1:CAS:528:DC%2BD2MXitl2qtL4%3D] 10.1002/adfm.200400078

    Article  Google Scholar 

  17. Wang WZ, Germanenko I: Chem. Mater.. 2004, 149: 3028.

    Google Scholar 

  18. Petrov DV, Santos BS, Pereira GAL, de Mello Donegá C: J. Phys. Chem. B. 2002, 106: 5325. COI number [1:CAS:528:DC%2BD38Xjt12murk%3D] 10.1021/jp010617i

    Article  Google Scholar 

  19. Shen XP, Zhao H, Liu Q, Xu Z: Chin. J. Inorg. Chem.. 2007, 23: 1561. COI number [1:CAS:528:DC%2BD2sXhtFKmtLjP]

    Google Scholar 

  20. Shen XP, Yin G, Zhang WL, Xu Z: Solid State Commun.. 2006, 140: 116. COI number [1:CAS:528:DC%2BD28XpvFensL0%3D]; Bibcode number [2006SSCom.140..116S] 10.1016/j.ssc.2006.08.022

    Article  Google Scholar 

Download references


We are grateful for financial support from the Natural Science Foundation of Jiangsu Province (No. BK2009196) and the National Natural Science Foundation of China (No. 20875039).

Author information

Authors and Affiliations


Corresponding author

Correspondence to Xiaoping Shen.

Rights and permissions

Open Access This article is distributed under the terms of the Creative Commons Attribution 2.0 International License ( ), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Reprints and Permissions

About this article

Cite this article

Sun, J., Shen, X., Guo, L. et al. Solvothermal Synthesis of Ternary Sulfides of Sb2 − xBi x S3(x = 0.4, 1) with 3D Flower-Like Architectures. Nanoscale Res Lett 5, 364 (2010).

Download citation

  • Received:

  • Accepted:

  • Published:

  • DOI:


  • Nanostructures
  • Semiconductor
  • Ternary sulfide
  • Solvothermal
  • Optical properties