Journal of Nanomaterials

Volume 2012 (2012), Article ID 957035, 6 pages

doi:10.1155/2012/957035

Research Article

Enhancement of Photoluminescence Lifetime of ZnO Nanorods Making Use of Thiourea

Erdal Sönmez1,2 and Kadem Meral2,3

¹Department of Physics, Faculty of Education, Atatürk University, 25240 Erzurum, Turkey

²Advanced Materials Research Laboratory, Department of Nanoscience & Nanoengineering, Graduate School of Natural and Applied Sciences, Atatürk University, 25240 Erzurum, Turkey

³Department of Chemistry, Faculty of Science, Atatürk University, 25240 Erzurum, Turkey

Received 7 March 2012; Revised 10 May 2012; Accepted 13 May 2012

Academic Editor: Vo-Van Truong

Copyright © 2012 Erdal Sönmez and Kadem Meral.

Abstract.

We have investigated correlation of photoluminescence lifetime between zinc oxide (ZnO) nanorods and thiourea-doped ZnO nanorods (tu: CH₄N₂S). Aqueous solutions of ZnO nanorods were deposited on glass substrate by using pneumatic spray pyrolysis technique. The as-prepared specimens were characterized by X-ray diffraction (XRD), scanning electron microscopy (SEM), and time-resolved photoluminescence spectroscopy (TRPL). The photoluminescence lifetime of ZnO nanorods and ZnO nanorods containing thiourea was determined as  ns and  ns , respectively. The calculated lifetime values of ZnO nanorods revealed that the presence of thiourea in ZnO nanorods resulted in increasing the exciton lifetime. In addition to the optical quality of ZnO nanorods, their exciton lifetime is comparable to the longest lifetimes reported for ZnO nanorods. The structural improvement of ZnO nanorods, containing thiourea, was also elucidated by taking their SEM images which show the thinner and longer ZnO nanorods compared to those without thiourea.

1. Introduction

Zinc oxide (ZnO) is a wide-band gap ( 3.37 eV at 300 K) semiconductor with good carrier mobility and can be doped n-type or p-type. It has many applications in a very important area such as ultraviolet light-emitting diodes and nanolaser [1]. ZnO shows pronounced excitonic effects at high temperatures (>300 K) due to its large exciton binding energy (60 meV) [2]. Optically pumped lasing has been successfully demonstrated for the ZnO nanostructures, which have resulted in the intense attention to ZnO optical properties [3–21]. For example, the optical properties of ZnO nanostructures at different morphologies are reported at varying temperatures and the performance-structure relation for ZnO nanostructures are evaluated for some applications. Further improvement in the quality of ZnO is necessary to achieve the superior device performance [22]. In this regard, main progress has been made toward the growth of good-quality ZnO nanostructures for the fabrication of light-emitting diodes [8].

The material quality and optical properties of the nanostructures, such as ZnO, are commonly followed by using the photoluminescence (PL) and time-resolved photoluminescence (TRPL) measurements [23]. Especially, TRPL provides significant information in relation to the exciton lifetime which is an important indicator for the material quality and efficiency of the radiative recombination [6]. It is known that the lifetime is related to the radiative decay of the exciton and various nonradiative processes such as leak by deep-level traps, low-lying surface states and multiphonon scattering [24, 25]. In this regard, the separation of the radiative recombination and nonradiative processes is difficult [26]. However, the radiative excitation lifetime () is improved by decreasing the structural defect of ZnO nanostructures. Therefore, different morphologies of ZnO nanostructures exhibit very different lifetimes, with some showing very fast decay, while others have decay times as long as comparable to those of good-quality. As a result of these explanations, it is concluded that the morphologies and dimensions of ZnO nanostructures affect the exciton lifetimes [15, 18]. For example, the high-quality ZnO single crystals have several nanoseconds exciton lifetime at room temperature [6]. Therefore, the exciton lifetime of ZnO nanostructures is changed by the controlling of their morphologies and dimensions. The structure of ZnO is controlled by precious parameters such as the starting zinc compound, chemical composition of solvent, nature of the precipitating agent, pH, temperature, and aging time [27]. In addition to growth conditions, deposition methods of ZnO onto solid surface play a key role for ZnO nanostructures. Therefore, different deposition methods have been developed to fabricate a variety of ZnO nanostructures such as well-known metal organic chemical vapor [28, 29], pulsed laser [30, 31], electrochemical deposition techniques [32, 33], vapor-liquid, solid [34, 35], and wet chemical methods [36–38]. In addition to those methods, the important one is chemical spray pyrolysis system which is one of the most elegant methods to the preparation of good-quality ZnO nanostructures. This method has several advantages over the other methods such as providing short time, being cost-effective and template-free [39]. Consequently, a variety of ZnO nanostructures are easily fabricated by tuning of material growth conditions. If the optimal conditions are determined, various ZnO nanostructures can be prepared such as nanowires, nanoribbons, tetrapods, and nanorods, which exhibit excellent optical properties [5].

In the present study, the smaller and longer ZnO nanorods were prepared by doping a little amount of thiourea (tu: CH₄N₂S) into zinc chloride (ZnCl₂) solution, ZnO nanorods with and without thiourea have been deposited on a glass substrates via chemical spray pyrolysis method at different temperatures. The optical and structural properties of ZnO nanorods have been examined by X-ray diffraction (XRD), scanning electron microscopy (SEM), and time-resolved photoluminescence (TRPL) techniques. The results showed that the exciton lifetime of ZnO nanorods was increased in the presence of thiourea.

2. Experimental

All chemicals were analytical grade and were used without further purification. ZnO was deposited using spray aqueous solutions by pneumatic spray pyrolysis technique. The solutions, used for the preparation of ZnO as thin films, were that the first contained ZnCl₂ while the second included ZnCl₂ and thiourea with molar ratios of 1 : 0.25. The starting solution was atomized at a frequency of 1.63 MHz by an ultrasonic nebulizer and by using dry air. The solution was mixed with magnetic mixer. Mixing process lasted for 20 min. The resultant amounts of each solution are 50 mL. The nozzle-substrate distance was maintained at 10 cm. The deposition temperature (temperature of substrate surface), in the range of 350–550°C, was varied by using electronic temperature controller (TET-612 temperature controller by product ColdfusionX Electronics) device on the hot plate metallic surface. The temperature of the metallic surface was totally stable throughout the process at 350, 450, and 550 ± 2°C, respectively. The substrates were not used at temperature above 550°C because they were physically being an irreparable disrupted. The substrates are ordinary microscope slides. Before loading into the system, the substrates were washed with detergent and then completely rinsed in methanol, acetone, and deionized water, respectively, and dried in air. Before being sprayed on the substrates they were progressively heated up to the required temperature. The solution flow rate and gas pressure were kept constant at 1 mL/min. Air was used as the carrier gas supplied by a filtered oil-free compressor. The duration of the film deposition was about 50 min. The color of ZnO film was white and it had a very good adhesion to glass substrates.

The structural characterization of deposited films structures of ZnO was carried out by X-ray diffraction (XRD) measurements using a Rigaku D/Max-IIIC diffractometer with CuKα1 radiation (), at 30 kV, 10 mA. The range, used in the measurement, was from 100 to 700 in steps of 0.02 s⁻¹. Surface morphology was examined by a JEOL JSM5610 model scanning electron microscope operating at 25 kV. Photoluminescence decays, for the exciton lifetime measurements, were carried out with a Laser Strobe Model TM-3 lifetime fluorometer from Photon Technology International. The excitation source consists of a pulsed nitrogen laser/tunable dye laser combination. Pulse width is about 800 ps and has repetition rate up to 20 pulses per second. The samples were excited at 337 nm nitrogen laser and, then, photoluminescence decays were monitored. The photoluminescence decays were analyzed with the lifetime distribution analysis software (Felix32) from the instrument-supplying company. The quality of fits was assessed by chi-square () values. Fitting with not more than 1.5 was taken as acceptable.

3. Results and Discussion

Firstly, the morphology of spray-deposited ZnO nanostructures was investigated as a function of the growth temperature, which is one of the most important experimental factor for the elucidation of nanostructures [27]. For this purpose, ZnO nanostructures were deposited on the glass substrate—at different temperatures (350, 450, and 550°C). The results of those experiments showed that elongated hexagonal prisms shaped ZnO nanostructures have been formed at 550°C. Therefore, the deposition temperature was optimized as 550°C for all sample preparations. Figure 1 illustrates the SEM images of ZnO deposited onto the glass substrates by the spray pyrolysis process using only ZnCl₂ (Figures 1(a)–1(c)) and ZnCl₂ containing thiourea additive with a molar ratio of Zn : tu = 1 : 0.25 (Figure 1(d)). SEM images demonstrated that the nanorod structures of ZnO on the glass substrate were formed at 550°C. Additionally, it can be seen the SEM images (Figure 1) that this deposition temperature is suitable for the formation of ZnO nanorods without or with thiourea. The addition of thiourea into the ZnCl₂ solution drastically influenced the ZnO nanorods dimensions as seen by the careful investigation of SEM images. The diameter of the ZnO nanorods was decreased from 1000 nm to 500 nm, while their lengths increased to about 200 nm by thiourea doped in the solution. As a result, the number of the nanorods and the width of the zinc oxide surface per unit area increased compared to those without thiourea. The molar ratio used for ZnO nanorods with thiourea is 1 : 0.25 (Zn : tu), since it is optimal condition for the growing of the nanorods at the highest aspect ratio. Besides, it is known that the amount of thiourea in solution is extremely important factor which determines the final rods dimensions and its addition, generally, leads to the formation of thinner rods [39, 40]. The possible mechanism in the morphological changes of the ZnO nanorods, which are produced from thiourea mixed ZnCl₂, solution is reported in the literature that in some crystallization processes. The growth rate of a crystal facet can be inhibited by an impurity adsorption during the front growth and incorporation of new molecules into that facet. For example, widening of the crystal is restricted by the adsorption of ZnS particles as the facet of the crystals is reported [40, 41]. As a result of this, longitudinal length in c-axis has increased that deteriorates optical properties of the crystals.

(a)

(b)

(c)

(d)

Figure 1: Typical SEM images of ZnO nanorods grown onto ordinary glass substrates at (a) 350°C (b) 450°C (c) 550°C and (d) 550°C with little amount of thiourea added.

Figure 2 shows the XRD pattern of the ZnO nanorods prepared in the absence and presence of thiourea. As shown in the XRD pattern, the peak of (002) is dominant in ZnO nanorods grown in the absence of thiourea. In the ZnO nanorods grown in the presence of thiourea, in addition to ZnO structures, emerging of second phases, like ZnS, caused an increase in the peak count. Some of the reflections at , 28.80, and 30.80° corresponding to Muller indices of 110, 111, and 200 detected in the XRD pattern can be attributed to the reflection of ZnS sphalerite phase in Figure 2, the ZnCl₂ and thiourea in aqueous solution yield a complex structure of thiourea zinc with molecular formula Zn(tu)₂Cl₂, which decomposes to the formation of zinc sulfide at temperatures above 300°C (as it has been reported in [40]). Besides, the possible growth mechanism for the formation of ZnO nanorods from the ZnCl₂ solution with thiourea at 550°C can be shown in Scheme 1.

Scheme 1:

Figure 2: XRD patterns of ZnO nanorods.

The quality of ZnO is commonly examined using time-resolved photoluminescence (TRPL) measurement as well as steady-state photoluminescence (PL). TRPL measurement provides significant information about the exciton lifetime, which represents efficiency of the radiative recombination. In order to determine the exciton lifetime of ZnO nanorods, the photoluminescence decay spectra of the samples were recorded at 337 nm excitation wavelength at room temperature. Next, the lifetime of the samples was calculated by using specific fit software that belongs to PTI (Photon Technology International). The obtained photoluminescence decay of ZnO nanorods were analyzed to single-, bi-, and three-exponential fits according to (1)

where is the number of exponentials, and and are the lifetime and the preexponential factor, for each components. The photoluminescence decay spectra of the samples with exponential fits were given in Figure 3. As a result of the exponential analyses, it was determined that the photoluminescence decay of ZnO nanorods indicates single-exponential fits with the acceptable values. Therefore, the single-exponential fit results for the evaluation of exciton lifetime of ZnO samples were used. The obtained single-exponential fit shows that ZnO nanorods also have a homogeny distribution onto the glass surface. The exciton lifetime of ZnO nanorods was determined as  ns (), when that of ZnO nanorods containing thiourea was calculated as  ns (). The calculated lifetime values revealed that the presence of thiourea in ZnO nanorods resulted in increasing the exciton lifetime, suggesting an enhancement in radiative recombination. As considered by the experimental results, it is clear that the changing in the exciton lifetimes is resulted from the presence of the morphological difference between pure ZnO nanorods and ZnO nanorods containing thiourea, since it is known that the different morphologies of ZnO nanostructure act a significant role in the exciton lifetimes [22]. Additionally, it is inferred that ZnO nanostructures doped with thiourea bring about growing good-quality nanorods. Tuning of the exciton lifetime of ZnO nanostructure, depending on morphology, is desirable result in nanotechnological applications.

Figure 3: Fluorescence decay of ZnO nanorods with exponential fit.

4. Conclusion

A little addition of thiourea into ZnCl₂ solution (ZnCl₂ : tu = 1 : 0.25) provides thinner ZnO nanorods with the higher aspect ratio compared to that obtained from pure ZnCl₂ solution. The diameter of the ZnO nanorods was decreased from 1000 nm to 500 nm, while their lengths increased to about 200 nm by thiourea doping as seen by SEM images. At the same time, the number of the nanorods and the width of the zinc oxide surface per unit area increased. As a result of time-resolved photoluminescence studies, the lifetime of ZnO nanorods and ZnO nanorods containing thiourea was determined as ns () and  ns (), respectively. The results indicated that the exciton lifetime of ZnO nanorods containing thiourea increased through an increase in radiative recombination. It is clearly seen that the lifetime of ZnO nanorods is strongly dependant on the presence of the morphological differences between ZnO nanorods and ZnO nanorods containing thiourea. Summary, it is mentioned that the doping material prevents the nucleation of the sample and improves the exciton lifetime of synthesized ZnO nanorods. Discussion on the presented results in this study has a great potential for the application of ZnO in optoelectronic systems.

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