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Journal of Nanomaterials
Volume 2011 (2011), Article ID 863631, 6 pages
Research Article

Tailored 3D CuO Nanogrid Formation

Department of Material Science and Engineering, Center for Nanomaterials and Sensor Development, State University of New York, Stony Brook, NY 11794, USA

Received 20 April 2010; Accepted 6 July 2010

Academic Editor: Quanqin Dai

Copyright © 2011 Jusang Lee and Pelagia I. Gouma. 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.


This paper reports on the controlled synthesis of 3D CuO nanogrids by the combined use of electrospinning and thermal oxidation of a composite metal mesh/polymer mat architecture. The obtained nanogrids result from three steps encompassing: (i) Cu atom clusters diffusing into the nanofibers producing polymer-metal “core-shell”-type fibers (ii) decomposition of the polymeric shell; (iii) oxidation of the metallic core of the nanofibers to form self-supported, open nanogrids consisting of continuous nanofibers of CuO nanoparticles with an average diameter of 20 nm. The calculated band gap energy of the cupric oxide nanogrids was determined from the UV-Vis spectrum to be 1.32 eV. The unique 3D CuO nanogrids may be used as key components of 3D nanobatteries, photocatalysts, and p-type chemosensors.

1. Introduction

Cupric oxide (CuO) is a p-type semiconducting oxide with a monoclinic crystal structure and an indirect band gap of 1.2 eV, with interesting electrochemical, photovoltaic, and catalytic properties [13]. CuO have been applied to various applications including heterogeneous catalysis, [1] solar cells, [3] gas sensors, [4] magnetic storage media, [5] and in lithium ion electrodes [6]. Nanostructured CuO offers highly reactive surfaces, and improved optical, electrical, and catalytic properties compared to bulk crystals [7]. The reported variation of the bandgap energy, reducibility, and catalytic reactivity of CuO nanocrystals as a function of crystal shape and size has stimulated interest in exploring novel synthesis methods for this oxide [810]. A variety of CuO nanostructures, from nanoneedles and nanoribbons to nanowires, nanorods, and nanosheet configurations, have been fabricated by pulsed laser deposition, sol-gel routes, hydrothermal processing and thermal oxidation [1120].

Recently, there has been success in producing 3D nano-architectures. Liu and Zeng synthesized “dandelion-like” 3D CuO microspheres by a hydrothermal synthesis method, mixing copper nitrate Cu(NO3)2·3H2O in ethanol solvent, followed by the addition of NaOH, NaNO3, and ammonia in Teflon-lined stainless steel autoclave at C for 24–36 h [11]. Zhang et al. [12] also fabricated 3D hierarchical CuO “butterfly-like” structures in a solution of cupric chloride (CuCl2·2H2O) and NaOH at C for 15 h by using sodium dodecylbenzene sulfonate (SDBS) as surfactant. However, to the best of our knowledge, there have been no prior reports on the synthesis of 3D CuO nanogrids by the combined use of electrospinning and thermal oxidation.

It was previously shown by other workers that copper clusters can nucleate the growth of copper nanostructures within carbon nanotubes by diffusing through them [21]. In our approach, electrospinning was used to form a nanofibrous template on Cu grids in order to produce interconnected and self-supported 3D nanogrids of pure CuO for the first time by the diffusion and oxidation of Cu inside the polymeric fibers, as discussed below. Transmission electron microscopy studies of metal nanocrystals have shown that the heating effect of a focused electron beam triggers the diffusion of the metal atoms of the material under study within the organic layer of the support grid. This observation led to the hypothesis that tailoring the shape of an organic template to control the diffusion path of Cu atoms under thermal activation along with the synergistic oxidation of the metal may produce controlled 3D nanogrid structures. Organic (polyvinylpyrolidone (PVP) or cellulose acetate (CA)) nanofibers were thus deposited onto the surface of a copper grid (whether an uncoated TEM grid or a plain copper mesh). The obtained 3D CuO nanostructures (continuous and self-supported material, with high porosity and surface area) seem ideal for 3D nanobattery electrodes, catalysts, and p-type chemosensors.

2. Experimental Procedure

The synthesis of 3D CuO nanogrids was carried out by thermal oxidation of copper mesh substrates (TWP Inc., 200 mesh, wire dia. 51 m) on which PVP (Sigma-Aldrich, , melting point 300) mats were deposited by means of electrospinning (The Cu mesh was first cleaned with ethyl alcohol, then rinsed with deionized water followed by an ultrasonic bath in acetone). PVP precursor solutions were prepared by mixing the powder with ethanol solvent by ultrasonication. The resulting solution was filled into a syringe with a stainless steel needle. The needle was connected to a high-voltage supply and positioned vertically 7 cm above a piece of aluminum foil which acts as a ground electrode. The syringe pump was programmed to dispense 5 mL of 8% (wt/vol) PVP solution at a flow rate of 30 L/min. Upon application of a high voltage (18 kV), a solution jet was formed at the needle tip. The solvent evaporated during flight and a nonwoven mat of fibers was deposited on the Cu mesh secured on aluminum foil.

Thermal oxidation of the pure Cu mesh as well as of the composite material (PVP-Cu) was carried out in a resistively heated furnace at a constant rate of C/min in the temperature range from C to C; heating times varied from 2 to 5 hours; and all samples were cooled to ambient temperature. The temperature of the specimen was monitored by placing a thermocouple in the vicinity.

In order to reveal the crystallographic characteristics and to confirm the origin of the CuO nanogrids, to assess the phase evolution involved and the mechanism of formation of the 3D architecture, detailed structural and chemical analyses were performed using high resolution (HRTEM), scanning transmission (STEM), and analytical electron microscopy (AEM). The morphology and microstructure of the samples were studied using scanning electron microscopy (SEM, LEO 1550) and high-resolution transmission electron microscopy (HRTEM, JEOL JEM-2100F). Scanning transmission electron microscopy (STEM, JEOL JEM-2100F) and energy dispersive spectroscopy (EDS, JEOL JEM-2100F) were used for the chemical characterization of the samples. The CuO nanogrid samples were deposited on holey carbon copper grids for the microscopy and microanalysis studies. The optical absorption spectra of the nanogrids were recorded using UV-Visible spectrometer (ThermoScientific Evolution 300) in the wavelength range of 250–1000 nm at room temperature.

3. Results/Discussion

Figure 1(a) shows a scanning electron micrograph of the as-received, pure Cu mesh. It is well-established in the literature [17], that thermal oxidation of the pure Cu mesh produces nanorod structures of copper oxides. Figure 1(b) shows a scanning electron micrograph of the Cu mesh of Figure 1(a) following a heat treatment at C for 5 hours. The Cu meshes treated in air at elevated temperature forms rod shaped nanostructures all over the surface. The diameter and length of these structures could be controlled by varying the temperature and annealing time [17].

Figure 1: (a) SEM image of Cu mesh at room temperature. (b) Cu mesh after thermal oxidation at for 5 h.

This is not the case when a nonwoven polymer mat is deposited on the Cu mesh. Figure 2(a) is a SEM viewgraph of the as-spun PVP nanofibers deposited onto the Cu mesh at ambient conditions. Smooth nanofibers form a non-woven mat on the Cu substrate; the PVP fiber diameters are 500 nm in average and some grew up to 0.8 m upon branching and at junctions. The structural evolution of the as-synthesized composite nanofiber network is given in Figures 2(b) and 2(c) as a function of processing conditions used. Figure 2(b) is an SEM image illustrating the characteristic morphology of the Cu-PVP structures oxidized in air at C for 2 h, while Figure 2(c) shows the same material following oxidation at C for 2 h. To get an understanding of the growth mechanism of 3D nanogrids, the thermal reaction products were captured and analyzed at different stages during their formation.

Figure 2: (a) SEM image of PVP nanofibers deposited on the Cu mesh substrate by electrospinning at ambient condition. (b) PVP nanofibers deposited on the Cu mesh substrate by electrospinning after thermal oxidation at C for 2 hrs. (c) PVP nanofibers deposited on the Cu mesh substrate by electrospinning after thermal oxidation at 400ºC for 2 hrs.

At the earliest formation stage of the reaction product while the PVP has not yet fully decomposed, that is after a thermal treatment at C for 2 h, the PVP fibers are already filled with Cu (see STEM image in Figure 3). AEM results in STEM mode confirmed the presence of Cu in the core of the “core-shell” configured composite nanofibers (see inset in Figure 3). Thus, copper has diffused and migrated within the fibers that the Cu mesh was in contact with, upon thermal activation. It was not that the Cu deposited onto the electrospun nanofibers by evaporation.

Figure 3: STEM image and EDS spectra of the as-prepared copper filled PVP nanofiber heated at C for 2 h. The “+” on the image shows the location of the spectra collected.

Nanogrids prepared by heat-treating the PVP covered Cu mesh in air at C for 2 hrs were shown to consist of numerous nanocrystals, ranging in size between 16 and 60 nm, connected to each other to form a 3D nanofiber network with open porosity. Figure 4(a) is a montage of five HRTEM micrographs acquired in a sequence illustrating the inner details of the structure of a single nanofiber in the grid (The cropped SEM image is the detailed morphology of the polycrystalline nanofiber originated from Figure 2(c)). Figure 4(b) is an enlarged view of the first micrograph in the sequence of Figure 4(a) and clearly shows that the crystals are interconnected and that pores exist along each individual polycrystalline nanofiber. During these processed the PVP selectively burned so only oxide 3D nanogrids remained. Figure 4(c) is a further enlarged view of the particle arrangements within the fiber. Measurements of the spacing of their respective lattice planes shown here reveal that they are indeed CuO nanocrystals (the measured lattice spacings are 0.275 and 0.253 nm corresponding to the CuO (110) and CuO (-110) planes, resp.). The corresponding FFT patterns (insert in Figure 4(c)) are consistent with the HRTEM observation. The nanogrids consist of 3D, self-supporting, porous networks of continuous polycrystalline nanowires of CuO equiaxed nanoparticles. Thus, a novel “templating” method has been devised for the synthesis of CuO nanogrids.

Figure 4: (a) Montage of five HRTEM image of the structure of a single nanofiber in the grid oxidized at C for 2 h in air (the cropped SEM image originated from Figure 2(c)). (b) and (c) enlarged view of the particle arrangements within the fiber, corresponding FFT patterns are consistent with the HRTEM observation.

In summary, on the basis of combined SEM, HRTEM, STEM, and AEM analyses, the growth mechanism of CuO nanogrids involves the migration and diffusion of Cu atoms/clusters from the metallic substrate through the original polymer nanofibers which act as templates for the development of 3D networks of core-shell type Cu-PVP nanowires; the polymer shell decomposes and the metallic core oxidizes producing porous CuO arrangements upon further thermal treatment. Figure 5 provides a schematic illustration of the suggested process.

Figure 5: A schematic illustration and overlapped tem images of the formation of CuO 3D nanogrids. (a) PVP nanofibers on the mat deposit on Cu mesh by electrospinning at room temperature; (b) “core-shell” type Cu-PVP nanofiber formation by Cu diffusion and migration through PVP nanofibers (after thermal treatment at C for 2 h (Figure 3)); and (c) Polycrystalline CuO nanowire formed by removal of PVP and oxidation of Cu core (after thermal treatment at C for 2 hrs (Figure 4)).

The formation of Cu clusters inside the PVP fibers implies that the total free energy of polymer is lowered by the presence of metal atoms, according to the fundamental nucleation theory [22]. This is the case when PVP undergoes the phase transformation, such the transition to glass. The glass transition temperature of PVP is C. The presence of Cu clusters inside the polymer fibers after a heat-treatment at C (Figure 3) supports the argument made above.

After the calcinations of polymer fiber, the Cu clusters go through these possible oxidation steps: The oxidation of aggregated Cu cluster and the shrinkage of the fiber structure upon transition from Cu to CuO [20], may explain the formation of the porous nanostructure.

This synthesis method may be applied to other functional metal/metal oxide systems. The high surface area of the nanogrids and the self-supported nature of these nanostructures make them suitable to gas-sensing applications, used as catalysts and potentially as electrodes in 3D miniaturized batteries. With respect to their electronic properties, the band gap energy of the CuO nanogrids has been calculated. The UV-Visible spectrum of CuO 3D nanogrids is presented in Figure 6(a), which shows the optical absorption edge near 940 nm. The optical bandgap energy is estimated using the Kubelka-Munk function where is the reflectance, absorption coefficient, and scattering coefficient, respectively, [23]. Figure 6(b) shows a plot of () spectrum versus photon energy derived from Kubelka-Munk function. The extrapolated value of photon energy at indicates a bandgap energy () 1.32 eV. The calculated band gap is slightly larger than the previous reported value for bulk CuO (eV) [1]. According to other workers, these such narrow bandgap materials have many applications in the infrared [24]; therefore, these nanogrids might also be important to photothermal and photoconductive applications [25].

Figure 6: (a) UV-vis absorption spectrum of the 3D CuO nanogrids. (b) The corresponding versus curve, indicating that the band gap is 1.32 eV.

4. Conclusion

3D CuO nanogrids were synthesized by direct thermal oxidation of composite substrates consisting of a Cu mesh and electrospun PVP nanofibers deposited on it. The templating action of electrospun nanomats of polymers forms 3D self-organized structures. The average diameter of the CuO grains is 20 nm, while the diameter of the primary 3D nanogrids is 0.5 m. The estimated band gap energy is ~1.32 eV, which is larger than the reported value for bulk CuO (eV). Considering the simplicity of the synthesis method of such open 3D nanoarchitectures, the high surface areas of the nanogrids applications are envisioned as 3D nanobattery electrode, photocatalysts and advanced chemo sensors.


The authors wish to thank the Center for Functional Nanomaterials at the Brookhaven National laboratory (Dr. E. Sutter in particular) for access to transmission electron microscopy and microanalysis facilities, and the Lab of Consortium for Inter-Disciplinary Environmental Research (CIDER) (Dr. A. Orlov) for access to UV-Visible spectrometer. Part of this work was funded by the National Science Foundation.


  1. J. A. Switzer, H. M. Kothari, P. Poizot, S. Nakanishi, and E. W. Bohannan, “Enantiospecific electrodeposition of a chiral catalyst,” Nature, vol. 425, no. 6957, pp. 490–493, 2003. View at Publisher · View at Google Scholar · View at PubMed · View at Scopus
  2. K. Nagase, Y. Zheng, Y. Kodama, and J. Kakuta, “Dynamic study of the oxidation state of copper in the course of carbon monoxide oxidation over powdered CuO and Cu2O,” Journal of Catalysis, vol. 187, no. 1, pp. 123–130, 1999. View at Scopus
  3. E. Barrera-Calva, J. Méndez-Vivar, M. Ortega-López, L. Huerta-Arcos, J. Morales-Corona, and R. Olayo-González, “Silica-copper oxide composite thin films as solar selective coatings prepared by dipping sol gel,” Research Letters in Materials Science, vol. 2008, Article ID 190920, 5 pages, 2008. View at Publisher · View at Google Scholar
  4. J. Zhang, J. Liu, Q. Peng, X. Wang, and Y. Li, “Nearly monodisperse Cu2O and CuO nanospheres: preparation and applications for sensitive gas sensors,” Chemistry of Materials, vol. 18, no. 4, pp. 867–871, 2006. View at Publisher · View at Google Scholar · View at Scopus
  5. R. V. Kumar, Y. Diamant, and A. Gedanken, “Sonochemical synthesis and characterization of nanometer-size transition metal oxides from metal acetates,” Chemistry of Materials, vol. 12, no. 8, pp. 2301–2305, 2000. View at Publisher · View at Google Scholar · View at Scopus
  6. H. Wu, D. Lin, and W. Pan, “Fabrication, assembly, and electrical characterization of CuO nanofibers,” Applied Physics Letters, vol. 89, no. 13, Article ID 133125, 3 pages, 2006. View at Publisher · View at Google Scholar · View at Scopus
  7. Z.-S. Hong, Y. Cao, and J.-F. Deng, “A convenient alcohothermal approach for low temperature synthesis of CuO nanoparticles,” Materials Letters, vol. 52, no. 1-2, pp. 34–38, 2002. View at Publisher · View at Google Scholar · View at Scopus
  8. H.-M. Xiao, S.-Y. Fu, L.-P. Zhu, Y.-Q. Li, and G. Yang, “Controlled synthesis and characterization of CuO nanostructures through a facile hydrothermal route in the presence of sodium citrate,” European Journal of Inorganic Chemistry, no. 14, pp. 1966–1971, 2007. View at Publisher · View at Google Scholar · View at Scopus
  9. S. Anandan and S. Yang, “Emergent methods to synthesize and characterize semiconductor CuO nanoparticles with various morphologies—an overview,” Journal of Experimental Nanoscience, vol. 2, no. 1-2, pp. 23–56, 2007. View at Publisher · View at Google Scholar · View at Scopus
  10. K. Zhou, R. Wang, B. Xu, and Y. Li, “Synthesis, characterization and catalytic properties of CuO nanocrystals with various shapes,” Nanotechnology, vol. 17, no. 15, pp. 3939–3943, 2006. View at Publisher · View at Google Scholar · View at Scopus
  11. S. Q. Wang, J. Y. Zhang, and C. H. Chen, “Dandelion-like hollow microspheres of CuO as anode material for lithium-ion batteries,” Scripta Materialia, vol. 57, no. 4, pp. 337–340, 2007. View at Publisher · View at Google Scholar · View at Scopus
  12. Y. Zhang, W. O. Siu, X. Wang, T. Cui, W. Cui, Y. Zhang, and Z. Zhang, “Hydrothermal synthesis of three-dimensional hierarchical CuO butterfly-like architectures,” European Journal of Inorganic Chemistry, no. 1, pp. 168–173, 2009. View at Publisher · View at Google Scholar · View at Scopus
  13. H. Guan, C. Shao, B. Chen, J. Gong, and X. Yang, “A novel method for making CuO superfine fibres via an electrospinning technique,” Inorganic Chemistry Communications, vol. 6, no. 11, pp. 1409–1411, 2003. View at Publisher · View at Google Scholar · View at Scopus
  14. W. Qian, F. Wei, T. Liu, and Z. W. Wang, “The formation mechanism of the coaxial carbon-metal nanowires in a chemical vapor deposition process,” Solid State Communications, vol. 126, no. 7, pp. 365–367, 2003. View at Publisher · View at Google Scholar · View at Scopus
  15. A. Chen, H. Long, X. Li, Y. Li, G. Yang, and P. Lu, “Controlled growth and characteristics of single-phase Cu2O and CuO films by pulsed laser deposition,” Vacuum, vol. 83, no. 6, pp. 927–930, 2009. View at Publisher · View at Google Scholar · View at Scopus
  16. Y. Liu, L. Liao, J. Li, and C. Pan, “From copper nanocrystalline to CuO nanoneedle array: synthesis, growth mechanism, and properties,” Journal of Physical Chemistry C, vol. 111, no. 13, pp. 5050–5056, 2007. View at Publisher · View at Google Scholar · View at Scopus
  17. X. Jiang, T. Herricks, and Y. Xia, “CuO nanowires can be synthesized by heating copper substrates in air,” Nano Letters, vol. 2, no. 12, pp. 1333–1338, 2002. View at Scopus
  18. A. Kumar, A. K. Srivastava, P. Tiwari, and R. V. Nandedkar, “The effect of growth parameters on the aspect ratio and number density of CuO nanorods,” Journal of Physics: Condensed Matter, vol. 16, no. 47, pp. 8531–8543, 2004. View at Publisher · View at Google Scholar · View at Scopus
  19. J. F. Xu, W. Ji, Z. X. Shen, S. H. Tang, X. R. Ye, D. Z. Jia, and X. Q. Xin, “Preparation and characterization of CuO nanocrystals,” Journal of Solid State Chemistry, vol. 147, no. 2, pp. 516–519, 1999. View at Publisher · View at Google Scholar · View at Scopus
  20. S. Han, H.-Y. Chen, Y.-B. Chu, and H. C. Shih, “Phase transformations in copper oxide nanowires,” Journal of Vacuum Science & Technology B, vol. 23, no. 6, pp. 2557–2560, 2005. View at Publisher · View at Google Scholar · View at Scopus
  21. H. J. Hwang, O.-K. Kwon, and J. W. Kang, “Copper nanocluster diffusion in carbon nanotube,” Solid State Communications, vol. 129, no. 11, pp. 687–690, 2004. View at Publisher · View at Google Scholar · View at Scopus
  22. J. H. Das and J. E. Morris, “Diffusion and self-gettering of ion-implanted copper in polyimide,” Journal of Applied Physics, vol. 66, no. 12, pp. 5816–5820, 1989. View at Publisher · View at Google Scholar
  23. J. B. Gillespie, J. D. Lindberg, and L. S. Laude, “Kubelka-Munk optical coefficients for a barium sulfate white reflectance standard,” Applied Optics, vol. 14, no. 4, pp. 807–809, 1975. View at Publisher · View at Google Scholar
  24. T. C. McGill and D. A. Collins, “Prospects for the future of narrow bandgap materials,” Semiconductor Science and Technology, vol. 8, no. 1S, pp. S1–S5, 1993. View at Publisher · View at Google Scholar
  25. A. E. Rakhshani, “Preparation, characteristics and photovoltaic properties of cuprous oxide-a review,” Solid State Electronics, vol. 29, no. 1, pp. 7–17, 1986.