Table of Contents Author Guidelines Submit a Manuscript
Journal of Nanomaterials
Volume 2015, Article ID 825021, 8 pages
Research Article

Suspension Synthesis of Surfactant-Free Cuprous Oxide Quantum Dots

1Key Laboratory of Advanced Textile Materials and Manufacturing Technology, Ministry of Education, Zhejiang Sci-Tech University, Hangzhou 310018, China
2National Engineering Lab of Textile Fiber Materials and Processing Technology, Zhejiang Sci-Tech University, Hangzhou 310018, China

Received 20 October 2014; Revised 17 January 2015; Accepted 21 January 2015

Academic Editor: Shou-Yi Kuo

Copyright © 2015 Dongzhi Lai 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.


Suspension methods were used to synthesize surfactant-free Cu2O quantum dots (Cu2O-QDs) in high precursor concentrations using sodium hypophosphite as a reducing agent. Transmission electron microscopy (TEM) observations indicated that a large amount of Cu2O-QDs were synthesized with diameters ranging from 7 to 10 nm. We propose a mechanism where DMSO acts as a surface passivation agent, explaining the possible formation of Cu2O-QDs. Noticeably, the Cu2O-QDs exhibited high and stable catalytic activity for the reduction of rhodamine B.

1. Introduction

Cuprous oxide (Cu2O) is an important transition metal oxide with potential applications in a range of technological fields. Being a p-type oxide semiconductor with a direct band gap of 2.17 eV, Cu2O has been found in wide ranging applications including photon-activated water splitting [1], solar cells [2], gas sensing [3], low-temperature CO oxidation [4], negative-electrode materials [5], solar energy conversion [6], and photodegradation of organic pollutants [7].

The synthesis of Cu2O has been previously reported by several groups [1, 2, 4, 810]. Normally, a template (soft or hard) or capping agent is used to control the growth direction and dimensions of Cu2O in the solution-based route [1113]; however, the template or capping agents may have an undesirable role in the final applications. It is therefore highly beneficial to develop an alternative method to produce Cu2O which excludes templates or capping agents. Pan and colleagues reported that both cubic and octahedral Cu2O nano- and microcrystals can be selectively synthesized by a simple wet chemical and capping-agent-free reduction route at room temperature [14]. Xu et al. reported a facile room temperature surfactant-free solution chemical route to fabricate Cu2O nanocrystals, through reducing newly prepared Cu(OH)2 using hydrazine hydrate or sodium ascorbate [15]. In both methods, the Cu2O nanoparticle sizes are between 200 and 500 nm showing the larger particles size weakened the nanoparticle size effect. On the other hand, the precursor concentrations in literature [15] are low, at only 0.0032 mol/L which reduces the productivity of the particles and whilst increasing production costs.

Singhal et al. [16] reported a surfactant-free solvothermal approach for the preparation of Cu2O nanocrystals involving the reaction of copper (II) acetylacetonate in acetone with a reaction temperature that reaches up to 140°C, resulting in higher production costs. It is therefore desirable to design a low cost, room-temperature, convenient, high precursor concentration, and simple approach to produce surfactant-free Cu2O-QDs.

In this report, we develop a surfactant (or polymer) free room temperature suspension approach for the synthesis of Cu2O-QDs with high precursor concentrations. It is shown that Cu2O-QDs can be successfully fabricated through reducing copper sulfate pentahydrate using sodium hypophosphite in the dimethyl sulfoxide. Furthermore, the precursor quantity has little effect on the particle size and morphology of the Cu2O-QDs, which can be applicable to large-scale production of Cu2O-QDs. Rhodamine B (RhB) is one of the most commonly used xanthenes dyes in the textile industry due to its good stability. In this study, degradation of RhB by Cu2O-QDs is applied to test the catalytic activity of Cu2O-QDs.

2. Experiments

2.1. Materials

All chemicals used were of analytical grade and commercially obtained without further purification. Copper sulfate pentahydrate (CuSO4·5H2O, Hangzhou Gaojing Fine Chemical Co. Ltd.) acted as the precursor for the formation of Cu2O-QDs and sodium hypophosphite (NaH2PO2, Taicang Meida Reagent Co., Ltd.) acted as a reductant. Dimethyl sulfoxide (DMSO, Tianjin Yongda Chemical Reagent Co., Ltd.) was used as the solvent.

2.2. Synthesis
2.2.1. Suspension Phase Synthesis

4, 8, or 12 g of copper sulfate pentahydrate and 20 g of sodium hypophosphite were added to 1 L of DMSO. The mixture was vigorously stirred for 3 hours at 25°C. The yellow/green coloured mixture turned drab gradually with the addition of 1.5 mL of H2SO4. The nanoparticles produced were then washed three times in deionized water followed by washing in ethanol, then centrifuged, and vacuum-dried at 40°C overnight.

DMSO is a good ligand for Cu(II) [17, 18]. In the reaction system, DMSO complexed with Cu(II) and to form hexakis (dimethylsulfoxide) copper(II) complex as in [19]

[Cu(OS(CH3)2)6]SO4 was suspended in DMSO solution. This was confirmed by the addition of the copper sulfate pentahydrate into DMSO solution which becomes grass green under vigorous stirring (Figure 1(a)). However, when stirring was stopped, the [Cu(OS(CH3)2)6]SO4 solid particles settled to the bottom of the vessel after 24 hours and the DMSO solution became transparent (Figure 1(b)). Similarly, sodium hypophosphite was insoluble in DMSO; therefore the reaction occurred on the surface of the [Cu(OS(CH3)2)6]SO4 or the sodium hypophosphite.

Figure 1: Copper sulfate pentahydrate in DMSO ((a) under stirring, (b) standing for 24 h).
2.3. Catalytic Oxidation Experiment

The catalytic oxidation of RhB (2.5 × 10−5 mol/L) was conducted using Cu2O (2.5 g/L) and H2O2 (2.5 mmol/L) at 50°C. At given time intervals, the decoloration efficiency of the RhB was determined using a UV-vis spectrometer.

2.4. Characterization

X-Ray Diffraction (XRD). The crystal structure of Cu2O-QDs was characterized using a Switzerland Thermo ARL XTRA X-ray powder diffraction system using a Cu Kα radiation source at 35 kV with a scan rate of 0.05°/s in the 2θ range of 10–80°.

Fourier Transform Infrared Spectroscopy (FTIR). The Cu2O-QDs powders were spread on KBr pellets individually and dried under an infrared lamp. The FTIR analysis was measured using a Nicolet 5700 FTIR spectrometer.

Transmission Electron Microscopy (TEM). The Cu2O-QDs were suspended in ethanol and dropped on an ultra-thin carbon coated copper grid and dried under infrared lamp for 5 minutes. Images were acquired using a JSM-2100 transmission electron microscopy (TEM, JEOL, Japan) at an accelerating voltage of 200 kV.

Ultraviolet-Visible Spectroscopy (UV-Vis). The spectra were collected using a UV-3010 spectrophotometer across a wavelength range of 450–625 nm.

Copper, carbon, sulfur, and oxygen atomic content and their bonds on the surface of nanoparticles were obtained from the XPS spectra. XPS spectra were acquired using a PHIl600 X hemispherical analyzer equipped with an Al Ka (1486.6 eV) X-ray source.

3. Results and Discussion

3.1. Phase Composition and Morphology of the Products

The phase composition of the products was determined via XRD (Figure 2). Bragg’s reflections at 2θ value of 29.5°, 36.4°, 42.3°, 61.3°, and 73.5° represent (110), (111), (200), (220), and (311) planes of Cu2O (PDF#05-0667). No trace of Cu metal or CuO could be detected under the detection limits used for the X-ray diffractometer. This indicated that the as-synthesized samples were of single phase Cu2O.

Figure 2: XRD pattern of Cu2O-QDs freshly produced. (CuSO4·5H2O: (a) 4 g/L; (b) 8 g/L; (c) 12 g/L).

The morphology of the products was characterized by TEM (Figure 3). Cu2O-QDs were shown to have an average diameter of 7 nm when the precursor quantity was 4 g/L (seeing Figure 3(a)). No obvious change took place in the morphology and size of Cu2O-QDs when the precursor quantity was increased to 8 or 12 g/L (shown in Figure 3(b) or Figure 3(c)). These results revealed that the precursor quantity had little effect on morphology and size of the samples.

Figure 3: TEM images of synthesized samples (CuSO4·5H2O: (a) 4 g/L; (b) 8 g/L; (c) 12 g/L).
3.2. The FT-IR Spectra of Cu2O-QDs and DMSO

The FT-IR spectra of Cu2O-QDs and DMSO are presented in Figure 4. Several bands could be distinguished in the region of 4000–400 cm−1, a detailed assignment of which had been reported in a previous study. Briefly, the intense band of FT-IR spectra of DMSO at 1028 cm−1 was attributed to the S=O bond vibration stretching modes and the peak located at 1308 cm−1 was due to the symmetric vibrations of −CH3 groups. The bands at 1399 and 1432 cm−1 were assigned to the asymmetric vibrations of −CH3 groups, and the peak split attributed to the vibration coupling effects. The bands at 2909 and 2992 cm−1 were characteristic of the −CH3 bond vibrations in the region of 4000–2500 cm−1.

Figure 4: FTIR spectra of Cu2O-QDs and DMSO.

Correspondingly, the intense band of the FTIR spectra of Cu2O-QDs at 1096 cm−1 was attributed to the S=O bond vibration stretching modes. The bands at 1374 and 1461 cm−1 were assigned to the symmetric and asymmetric vibrations of −CH3 groups, respectively. The bands at 2847 and 2917 cm−1 were characteristic of the −CH3 bond vibrations in the region of 4000–2500 cm−1. The peak at 628 cm−1 corresponded to the Cu–O bond (due to optically active lattice vibration in the oxide) [20]. As these data show, DMSO was adsorbed on the surface of Cu2O-QDs. The peak at 1067 cm−1 was assigned to the S=O group which interacted with the Cu2O surface via the oxygen atom of DMSO.

The different peak positions of S=O and methyl in the FT-IR spectra of Cu2O-QDs and DMSO are mainly due to the following reasons: the FT-IR spectra of Cu2O-QDs were tested under solid conditions compared to the dimethyl sulfoxide under liquid conditions which resulted in the FTIR peak positions of S=O and methyl of Cu2O-QDs being shifted to a high wave number; the force constant of the S=O increases with the characteristic frequency of the S=O shifting to the high wavenumber displacement due to the inductive effect of the Cu+ [21].

3.3. The XPS Spectra of Cu2O-QDs

The surface properties of the nanoparticles were studied by XPS analysis. Figure 5 shows the complete XPS spectra from 0 to 1350 eV for the sample. The XPS spectra from a wide scan showed that the surface of the Cu2O-QDs consisted of copper, sulfur, carbon, and oxygen elements.

Figure 5: The complete XPS spectra of the sample.

The Cu 2p3/2 core level was used to investigate the Cu2O-QDs surface. Figure 6(a) showed the main and satellite peaks of Cu 2p1/2 and Cu 2p3/2 in the samples. Cupric oxide (CuO) and cuprous oxide (Cu2O) are the two semiconducting phases of copper oxide. In Figure 6(a), the spectrum displayed a Cu 2p3/2 peak at 931.88 eV with a shoulder at 934.48 eV, which corresponded to Cu and/or Cu2O and CuO, respectively. A shake-up satellite peak at 943.48 eV and some peaks above 950 eV were detected arising from spin-orbit coupling [22, 23]. Cu and Cu2O cannot be resolved due to their binding energies being very close, differing by only 0.1 eV [24]. It was not easy to distinguish the binding energy of Cu 2p between Cu and Cu2O, but they could be distinguished from the position of their corresponding LMM-2 auger transition in the XPS spectra at 568 eV and 570 eV for Cu and Cu2O, respectively [25]. In Figure 6(b), a peak is observed at close to 570 eV in the XPS spectra of the sample. According to the above descriptions, the peak at 931.88 eV relates to Cu2O. The relative intensities of the shakeup satellites from these levels were indicative of the presence of CuO at the surface [26]. The fact that XRD did not show evidence of CuO phase whilst XPS indicated the surface presence of Cu2+ ions suggests that CuO was present only on the surface of the Cu2O-QDs d forms a thin amorphous outer shell [27].

Figure 6: XPS (a) Cu 2p and (b) the L3MM Auger core-level spectra of the samples.

Figure 7 shows the S 2p (Figure 7(a)), C 1s (Figure 7(b)), and O 1s XPS spectra. Figure 7(a) shows the S 2p peak at 167.88 eV which is attributed to S=O bonds [28, 29]. In Figure 7(b), the main peak at 284.28 eV of C 1s was attributed to C–H bonds [24]. From the position of the peak at 530.88 eV in the O 1s spectra in Figure 7(c), this assigned the O 1s spectral to the Cu-O bonds [30]. XPS characterization indicated that the surface of the Cu2O-QDs was mainly Cu2O phase with CuO and DMSO covering a thin layer.

Figure 7: S 2p (a), C 1s (b), and O 1s (c) line of XPS spectra of the samples.
3.4. The Catalytic Activity of Cu2O-QDs

Cu2O can catalyze H2O2 to generate hydroxyl radicals [3133]. The catalytic activity of Cu2O-QDs is evidenced by the oxidation experiments of the model compound RhB. Degradation of RhB was carried out at 50°C in the presence of hydrogen peroxide and Cu2O-QDs. The absorption spectra of RhB solution during degradation is illustrated in Figure 8. The concentration of RhB was calculated from the absorption in = 555 nm. As shown in Figure 8, the main absorption bands decreased with increasing reaction time which was consistent with the gradual colour change of the solution from red to colourless. The RhB was reduced to less than 4% after 240 minutes, indicating that Cu2O-QDs possessed remarkable reductive ability.

Figure 8: Concentration changes of RhB under different conditions. (inset: absorption spectra of RhB aqueous solution).

The phase composition of Cu2O-QDs after ten cycles of catalysis was further investigated by XRD (Figure 9). Results showed that the phase composition of the samples still matched to Cu2O (PDF#05-0667). The height of each diffraction peak had decreased indicating that the Cu2O crystal structure was destroyed partly with the degree of crystallinity decreasing after repeated catalysis.

Figure 9: The phase composition of Cu2O-QDs before (a) and after (b) ten cycles of use.
3.5. A Plausible Mechanism of the Reaction

If polymers or surfactants are absent in the reaction system, the nanoparticles would grow at the expense of the smaller particles due to Ostwald ripening. As the prepared Cu2O-QDs were small in size and narrow in size distribution, this indicated that DMSO played a central role in controlling the morphology of Cu2O-QDs.

It is known that the smaller the particle size, the larger the surface energy of the particle. The initial cuprous oxide crystal nuclei were small and had a high surface energy during the crystals growth stage. The DMSO adsorbed on the surface of the cuprous oxide particles via the oxygen atom of the S=O group reduced the surface energy, which was verified by the FT-IR of Cu2O-QDs. The greater steric resistance of DMSO made the cuprous oxide surfaces incompletely passivated, so the similar cuprous oxide particles grew up via Ostwald ripening. When the cuprous oxide particles reached a certain size, the surface energy became low as the surfaces were completely passivated by DMSO. This made the surface energy too small to drive the particles towards increased size causing the particles to remain small.

NaH2PO2 was used as the reduction in the overall reaction system. The fundamental reaction can be simplified as in [34]

4. Conclusions

We report a novel, inexpensive, room temperature, high precursor concentration suspension method for the synthesis of surfactant-free Cu2O-QDs. Experimental results showed that DMSO played a surface passivation role in the formation of Cu2O-QDs. In this reaction system, varying the amount of precursors had little impact on the size of the product. The surface of the Cu2O-QDs was mainly Cu2O phase with CuO and DMSO covering a thin layer. The Cu2O-QDs samples had a high catalytic activity of H2O2 for the reduction of RhB. The results in this paper provide evidence which support the suspension synthesis method for Cu2O-QDs, broadening the scope of Cu2O-QDs synthesis routes which may potentially be applied to the synthesis of other oxide materials.

Conflict of Interests

The authors declare that there is no conflict of interests regarding the publication of this paper.


This study was supported by the National Natural Science Foundation of China (nos. 51133006 and 21276243), the Open Fund for a Key Discipline of Zhejiang Province, and the Young Researchers Foundation of Key Laboratory of Advanced Textile Materials and Manufacturing Technology, Ministry of Education, Zhejiang Sci-Tech University (2012QN07).


  1. P. E. De Jongh, D. Vanmaekelbergh, and J. J. Kelly, “Cu2O: a catalyst for the photochemical decomposition of water?” Chemical Communications, no. 12, pp. 1069–1070, 1999. View at Google Scholar · View at Scopus
  2. K. Akimoto, S. Ishizuka, M. Yanagita, Y. Nawa, G. K. Paul, and T. Sakurai, “Thin film deposition of Cu2O and application for solar cells,” Solar Energy, vol. 80, no. 6, pp. 715–722, 2006. View at Publisher · View at Google Scholar · View at Scopus
  3. H. Zhang, Q. Zhu, Y. Zhang, Y. Wang, L. Zhao, and B. Yu, “One-pot synthesis and hierarchical assembly of hollow Cu2O microspheres with nanocrystals-composed porous multishell and their gas-sensing properties,” Advanced Functional Materials, vol. 17, no. 15, pp. 2766–2771, 2007. View at Publisher · View at Google Scholar · View at Scopus
  4. B. White, M. Yin, A. Hall et al., “Complete CO oxidation over Cu2O nanoparticles supported on silica gel,” Nano Letters, vol. 6, no. 9, pp. 2095–2098, 2006. View at Publisher · View at Google Scholar · View at Scopus
  5. P. Poizot, S. Laruelle, S. Grugeon, L. Dupont, and J.-M. Tarascon, “Nano-sized transition-metal oxides as negative-electrode materials for lithium-ion batteries,” Nature, vol. 407, no. 6803, pp. 496–499, 2000. View at Publisher · View at Google Scholar · View at Scopus
  6. A. O. Musa, T. Akomolafe, and M. J. Carter, “Production of cuprous oxide, a solar cell material, by thermal oxidation and a study of its physical and electrical properties,” Solar Energy Materials and Solar Cells, vol. 51, no. 3-4, pp. 305–316, 1998. View at Publisher · View at Google Scholar · View at Scopus
  7. H. L. Xu, W. Z. Wang, and W. Zhu, “Shape evolution and size-controllable synthesis of Cu2O octahedra and their morphology-dependent photocatalytic properties,” Journal of Physical Chemistry B, vol. 110, no. 28, pp. 13829–13834, 2006. View at Publisher · View at Google Scholar · View at Scopus
  8. M. J. Siegfried and K.-S. Choi, “Electrochemical crystallization of cuprous oxide with systematic shape evolution,” Advanced Materials, vol. 16, no. 19, pp. 1743–1746, 2004. View at Publisher · View at Google Scholar · View at Scopus
  9. L. Gou and C. J. Murphy, “Solution-phase synthesis of Cu2O nanocubes,” Nano Letters, vol. 3, no. 2, pp. 231–234, 2003. View at Publisher · View at Google Scholar · View at Scopus
  10. X. J. Zhang and Z. L. Cui, “One-pot growth of Cu2O concave octahedron microcrystal in alkaline solution,” Materials Science and Engineering B: Solid-State Materials for Advanced Technology, vol. 162, no. 2, pp. 82–86, 2009. View at Publisher · View at Google Scholar · View at Scopus
  11. A. Radi, D. Pradhan, Y. Sohn, and K. T. Leung, “Nanoscale shape and size control of cubic, cuboctahedral, and octahedral Cu-Cu2O core-shell nanoparticles on Si(100) by one-step, templateless, capping-agent-free electrodeposition,” ACS Nano, vol. 4, no. 3, pp. 1553–1560, 2010. View at Publisher · View at Google Scholar · View at Scopus
  12. L. Gou and C. J. Murphy, “Controlling the size of Cu2O nanocubes from 200 to 25 nm,” Journal of Materials Chemistry, vol. 14, no. 4, pp. 735–738, 2004. View at Publisher · View at Google Scholar · View at Scopus
  13. H. Zhang and Z. Cui, “Solution-phase synthesis of smaller cuprous oxide nanocubes,” Materials Research Bulletin, vol. 43, no. 6, pp. 1583–1589, 2008. View at Publisher · View at Google Scholar · View at Scopus
  14. Z. Wang, H. Wang, L. Wang, and L. Pan, “Controlled synthesis of Cu2O cubic and octahedral nano-and microcrystals,” Crystal Research and Technology, vol. 44, no. 6, pp. 624–628, 2009. View at Publisher · View at Google Scholar · View at Scopus
  15. Y. Xu, H. Wang, Y. Yu, L. Tian, W. W. Zhao, and B. Zhang, “Cu2O nanocrystals: surfactant-free room-temperature morphology-modulated synthesis and shape-dependent heterogeneous organic catalytic activities,” Journal of Physical Chemistry C, vol. 115, no. 31, pp. 15288–15296, 2011. View at Publisher · View at Google Scholar · View at Scopus
  16. A. Singhal, M. R. Pai, R. Rao, K. T. Pillai, I. Lieberwirth, and A. K. Tyagi, “Copper(I) oxide nanocrystals—one step synthesis, characterization, formation mechanism, and photocatalytic properties,” European Journal of Inorganic Chemistry, vol. 14, pp. 2640–2651, 2013. View at Publisher · View at Google Scholar · View at Scopus
  17. D. D. Swank, C. P. Landee, and R. D. Willett, “Crystal structure and magnetic susceptibility of copper (II) chloride tetramethylsulfoxide [CuCl2(TMSO)] and copper (II) chloride monodimethylsulfoxide [CuCl2(DMSO)]: ferromagnetic spin-1/2 Heisenberg linear chains,” Physical Review B, vol. 20, no. 5, pp. 2154–2162, 1979. View at Publisher · View at Google Scholar · View at Scopus
  18. K. K. Spektor, G. L. Starova, Y. M. Skripkin, and L. V. Stepakova, “Influence of acido ligands on the structure of copper dihalide solvates with dimethyl sulfoxide and N,N-dimethylformamide,” Russian Journal of General Chemistry, vol. 81, no. 9, pp. 1772–1777, 2011. View at Publisher · View at Google Scholar · View at Scopus
  19. I. Persson, P. Persson, and M. J. Ullstrom, “Structure of Jahn-Teller distorted solvated copper(II) ions in solution, and in solids with apparently regular octahedral coordination geometry,” Journal of the Chemical Society, Dalton Transactions, vol. 31, no. 7, pp. 1256–1265, 2002. View at Google Scholar
  20. Z. C. Orel, A. Anžlovar, G. Dražić, and M. Žigon, “Cuprous oxide nanowires prepared by an additive-free polyol process,” Crystal Growth and Design, vol. 7, no. 2, pp. 453–458, 2007. View at Publisher · View at Google Scholar · View at Scopus
  21. H. Zhang, Modern Organic Spectroscopy Analysis, Chemical Industry Press, Beijing, China, 2005.
  22. J. Chastain and R. C. King Jr., Eds., Handbook of X-Ray Photoelectron Spectroscopy, Physical Electronics, Eden Prairie, Minn, USA, 1995.
  23. J. Ghijsen, L. H. Tjeng, J. van Elp et al., “Electronic structure of Cu2O and CuO,” Physical Review B, vol. 38, no. 16, pp. 11322–11330, 1988. View at Publisher · View at Google Scholar · View at Scopus
  24. T. Ghodselahi, M. A. Vesaghi, A. Shafiekhani, A. Baghizadeh, and M. Lameii, “XPS study of the Cu@Cu2O core-shell nanoparticles,” Applied Surface Science, vol. 255, no. 5, pp. 2730–2734, 2008. View at Publisher · View at Google Scholar · View at Scopus
  25. J. Y. Park, Y. S. Jung, J. Cho, and W. K. Choi, “Chemical reaction of sputtered Cu film with PI modified by low energy reactive atomic beam,” Applied Surface Science, vol. 252, no. 16, pp. 5877–5891, 2006. View at Publisher · View at Google Scholar · View at Scopus
  26. C. C. Chusuei, M. A. Brookshier, and D. W. Goodman, “Correlation of relative X-ray photoelectron spectroscopy shake-up intensity with CuO particle size,” Langmuir, vol. 15, no. 8, pp. 2806–2808, 1999. View at Publisher · View at Google Scholar · View at Scopus
  27. M. Yin, C.-K. Wu, Y. B. Lou et al., “Copper oxide nanocrystals,” Journal of the American Chemical Society, vol. 127, no. 26, pp. 9506–9511, 2005. View at Publisher · View at Google Scholar · View at Scopus
  28. L.-L. Ma, Z.-H. Qin, L. Zhang, X. Liu, and H. Chen, “Peak fitting methods and parameter settings in XPS analysis for organic sulfur in coal,” Journal of Fuel Chemistry and Technology, vol. 42, no. 3, pp. 277–283, 2014. View at Google Scholar · View at Scopus
  29. P. Chen, “Application of XPS in study forms of organic sulfur in macerals of Yanzhou coal,” Journal of Fuel Chemistry and Technology, vol. 25, no. 3, pp. 283–241, 1997. View at Google Scholar · View at Scopus
  30. P. E. Laibinis and G. M. Whitesides, “Self-assembled monolayers of n-alkanethiolates on copper are barrier films that protect the metal against oxidation by air,” Journal of the American Chemical Society, vol. 114, no. 23, pp. 9022–9028, 1992. View at Publisher · View at Google Scholar · View at Scopus
  31. A. N. Pham, G. Xing, C. J. Miller, and T. D. Waite, “Fenton-like copper redox chemistry revisited: hydrogen peroxide and superoxide mediation of copper-catalyzed oxidant production,” Journal of Catalysis, vol. 301, pp. 54–64, 2013. View at Publisher · View at Google Scholar · View at Scopus
  32. M. K. Eberhardt, G. Ramirez, and E. Ayala, “Does the reaction of Cu+ with H2O2 give OH radicals? A study of aromatic hydroxylation,” Journal of Organic Chemistry, vol. 54, no. 25, pp. 5922–5926, 1989. View at Publisher · View at Google Scholar · View at Scopus
  33. M. R. Gunther, P. M. Hanna, R. P. Mason, and M. S. Cohen, “Hydroxyl radical formation from cuprous ion and hydrogen peroxide: a spin-trapping study,” Archives of Biochemistry and Biophysics, vol. 316, no. 1, pp. 515–522, 1995. View at Publisher · View at Google Scholar · View at Scopus
  34. S. L. Xu, X. Y. Song, C. H. Fan et al., “Kinetically controlled synthesis of Cu2O microcrystals with various morphologies by adjusting pH value,” Journal of Crystal Growth, vol. 305, no. 1, pp. 3–7, 2007. View at Publisher · View at Google Scholar · View at Scopus