Journal of Nanomaterials

Volume 2013 (2013), Article ID 690639, 5 pages

http://dx.doi.org/10.1155/2013/690639

Research Article

Facile Hydrothermal Approach to ZnO Nanorods at Mild Temperature

Yang Jiao, Yang Liu, Bosi Yin, Siwen Zhang, Fengyu Qu, Xiaodan Wu, and Xiang Wu

Key Laboratory for Photonic and Electronic Bandgap Materials, Ministry of Education, College of Chemistry and Chemical Engineering, Harbin Normal University, Harbin 150025, China

Received 26 June 2013; Accepted 9 July 2013

Academic Editor: Renzhi Ma

Copyright © 2013 Yang Jiao 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.

Abstract.

In this work, ZnO nanorods are obtained through a facile hydrothermal route. The structure and morphology of the resultant products are characterized by X-ray diffraction (XRD) and scanning electron microscope (SEM). The experimental results indicated that the as-synthesized ZnO nanorods have an average diameter of approximate 100 nm. A possible growth mechanism for ZnO nanorods was proposed based on the experimental results and found that Zn powder plays a critical role for the morphology of the products. Room temperature photoluminescence property of ZnO nanorods shows an ultraviolet emission peak at 390 nm.

1. Introduction

Recently, Zinc oxide (ZnO) nanostructures have received more attention due to their versatile applications in photoluminescence (PL) [1, 2], field emission [3], and piezoelectronics [4–6]. The one-dimensionality of these structures leads to some of their interesting properties, along with the potential for novel applications. So far, ZnO nanorods (NWs) [7], nanobelts [8, 9], nanotubes [10], nanowindmills [11], hierarchical nanostructures [12–17], and so on have been reported. These nanostructures are potential candidates for UV light sources, sensors [18], and solar cells [19]. Various physical and chemical routes have been used to prepare a wide range of ZnO nanostructures. Raula et al. reported a simple wet-chemical approach to the growth of hierarchical ZnO nanostructures with different shapes [20]. Ma’s group used carbothermal reduction method to fabricate large-scale ZnO nanowires [21]. Wang and his coworkers synthesized exotic zigzag ZnO nanoribbons by thermal evaporation [22]. Liu’s group fabricated a highly flexible, sensitive photodetector built on flexible nanoparticle-assembled ZnO cloth via a carbon cloth templated hydrothermal method [23]. Among these methods, hydrothermal method has been used widely due to its simple, low cost and little pollution.

In recent years, ZnO semiconductor nanomaterials are regarded as one of the most important photonic materials owing to its direct wide bandgap (3.37 eV) and large excitation binding energy (60 meV at room temperature). In this paper, we explore a simple one pot hydrothermal route for the controlled growth of ZnO nanorods. The morphology, size, and structure of the ZnO nanorods have been investigated in detail. A possible mechanism has been suggested to explain the formation and growth of the nanorods structures. Room temperature photoluminescence (PL) properties of the as-prepared ZnO products were also investigated.

2. Experimental

All reagents were of analytical grade and used without further purification. For the preparation of ZnO nanomaterials, a typical process was as follows. Firstly, 0.65 g metallic Zn powder was added into 10 mL deionized water with continuous stirring at room temperature. Subsequently, 20 mL Zn solution (2.97 g Zn(NO₃)₂ and 5.6 g KOH) was prepared. The mixture was then introduced into a Teflon vessel (50 mL capacity) sealed in a stainless-steel autoclave. The autoclave was heated and maintained at the desired temperature 180°C for 5 h and then cooled to room temperature. The white product was collected and rinsed with deionized water and ethanol and was finally purified by self-sedimentation. Finally the product was dried in a chamber at 80°C for 5 h.

The obtained product was characterized by scanning electron microscope (SEM, Hitachi-4800), X-ray powder diffraction (XRD, Rigaku Dmax-2600/pc, Cu Kα radiation, = 0.1542 nm, 40 KV, and 100 mA). Optical property of the as-synthesized ZnO nanostructures was investigated by a standard UV-VIS-NIR spectrophotometer (JASCO V-670).

3. Results and Discussion

Low magnification SEM image (Figure 1(a)) presents the overall morphology of the as-synthesized samples, clearly observing that as-prepared samples consisted of many nanorods. Further observation finds that the diameter of nanorods is about 100 nm as shown in Figure 1(b). Figure 2 shows XRD pattern of the as-obtained product. All of the diffraction peaks are in accordance with the standard bulk ZnO pattern (JCPDS number 36-1451) and can be straightforwardly indexed to hexagonal wurtzite type ZnO. No peaks of other phases were detected, indicating high purity of the as-synthesized product. The strong and sharp peaks indicate that the as-prepared product is highly crystalline.

(a)

(b)

Figure 1: SEM images of ZnO nanorods (a) low magnification SEM image and (b) high magnification SEM image.

Figure 2: XRD pattern of the as-synthesized samples.

To investigate the formation mechanism of the as-prepared ZnO products, a series of controlled experiments were conducted. First, keeping the other growth parameters constant, no addition of Zn power, and the shape of the as-obtained ZnO products are not regular, and some of the products are small particles, as shown in Figures 3(a) and 3(b). Figures 3(c) and 3(d) showed the SEM images of the product without addition of Zn(NO₃)₂, revealing that as-prepared samples consisted of many nanorods, but the nanorods are uneven, demonstrating that Zn powder plays a very important role in the formation of nanorods. The above results indicate that tailoring the growth parameters deliberately is essential to obtain the desiring nanostructures. Based on the above experiment results, a possible growth mechanism for ZnO nanorods may be proposed as follows:

(a)

(b)

(c)

(d)

Figure 3: SEM images of the products at different experiment parameters ((a)-(b)) without the addition of Zn powder and ((c)-(d)) the addition of Zn powder, without the addition of Zn(NO₃)₂.

In the initial stage, Zn²⁺ and react with each other to form and Zn(OH)₂, respectively. Because of an excess of alkali, Zn(OH)₂ will further react with to form . During the stage of hydrothermal condition, and Zn(OH)2 will turn to ZnO small particles. These particles have a tendency to aggregate due to large surface energy. Surface energy is substantially reduced when the neighboring nanoparticles are grown [24]. With the crystal growth continuing, each nanoparticle in the aggregates or nanorods has its own orientation and acts as a nucleus for further growth. These growth processes are not only related to the anisotropic ZnO crystal structure but also the involved reaction conditions. The growth habit of ZnO crystals can control the ZnO crystals to grow into the nanorods. Without Zn powder, the morphology of the products is irregular. Zn powder provides enough Zn resource to induce ZnO nanoparticles further growth into the nanorods according to the experiment results. Figure 4 demonstrates a growth schematic for the as-synthesized ZnO nanorods.

Figure 4: Growth Schematic of the as-synthesized ZnO nanorods.

Finally, room temperature photoluminescence property of the as-synthesized ZnO nanorods was investigated. Figure 5 presents a PL spectrum of the as-synthesized products. The spectrum reveals a sharp emission band located at 390 nm. The UV band gap emission results from the radiative recombination of an excited electron in the conduction band with the valence band hole . It can be commonly assigned as the near band gap exciton emission in ZnO [25]. The visible (or deep trap) photoluminescence (PL) is commonly defined as the recombination of the electron-hole pair from localized states with energy levels deep in the band gap, resulting in lower energy emission. These alternate energy levels are usually attributed to dopants, structural features, or surface defects, such as singly ionized oxygen vacancies, zinc vacancies, and zinc interstitials, or extrinsic impurities [26–29].

Figure 5: Room temperature photoluminescence spectrum of the as-synthesized ZnO nanorods.

4. Conclusion

ZnO nanorods with high yield have been successfully obtained by a simple hydrothermal approach. The average diameter of the as-synthesized nanorods is about 100 nm. The possible growth mechanism of the ZnO nanosheets is proposed based on the experimental results. Room temperature photoluminescence spectrum demonstrates that ZnO nanorods show a strong and sharp UV band edge emission peak at 390 nm. It is expected that such ZnO nanorods may have applications in optoelectronic micro/nanodevices.

Acknowledgments

This work was supported by the Foundation for Key Project of Ministry of Education, China (no. 211046), Program for New Century Excellent Talents in Heilongjiang Provincial University (1252-NCET-018), the Scientific Research Fund of Heilongjiang Provincial Education Department (12531179, 12511168), Youth Skeleton Teacher Fund of Harbin Normal University (KGB201014), and Program for Scientific and Technological Innovation Team Construction in Universities of Heilongjiang (no. 2011TD010).

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