Journal of Nanomaterials

Journal of Nanomaterials / 2017 / Article

Research Article | Open Access

Volume 2017 |Article ID 6308174 | 12 pages | https://doi.org/10.1155/2017/6308174

Influence of Irradiation Time on Structural, Morphological Properties of ZnO-NRs Films Deposited by MW-CBD and Their Photodiode Applications

Academic Editor: Miguel A. Garcia
Received02 May 2017
Accepted17 Jul 2017
Published22 Aug 2017

Abstract

Microwave-assisted chemical bath deposition (MW-CBD) was used to deposit zinc oxide nanorods (ZnO-NRs) films by using different microwave irradiation time. The films exhibit a good crystallinity having a hexagonal wurtzite phase formation. Although the dominant preferred orientation was not observed for the ZnO-5 and ZnO-10, ZnO-8 showed (002) preferred orientation. The emission scanning electron microscope (FESEM) showed almost randomly oriented hexagonal nanorods on the surface. A slight decrease in the length of the observed hexagonal nanorods due to the increase in the irradiation time was observed, changing from 550 nm to 300 nm. The p-Si/n-ZnO-NRs heterojunction photodiodes were fabricated. The current-voltage characteristics of these photodiodes were investigated under dark and different illumination intensity. An increase in the reverse current with increasing illumination intensity confirmed that the fabricated photodiodes exhibited a photoconducting behavior. In addition, the barrier height and series resistance values of the photodiodes were determined from capacitance-voltage measurements.

1. Introduction

In modern materials science, nanostructured ZnO films are versatile material to make in numerous novel applications, owing to their several unique features, including the wide band gap (3.37 eV), good transparency and electrical conductivity, excellent electron mobility, and low thermal expansion. So they have been extensively studied and applied in many applications, such as sensors [1, 2], light-emitting diodes [3, 4], thin film transistors [5, 6], photodetectors [7], and solar cells [8, 9].

Over the past two decades, materials scientists have developed various synthetic means for preparing nanostructured ZnO films. These films in forms of nanoparticle, nanowire, nanorod, nanotube, nanoflower, and so on can now be easily obtained with most of methods and techniques, such as sol-gel [1012], spray pyrolysis [13, 14], chemical bath deposition (CBD) [15], SILAR [16], electrochemical deposition [17, 18], sputtering [19, 20], atomic layer deposition [21], and microwave-assisted chemical bath deposition (MW-CBD) [22]. Currently world-wide works continue intensively in both the basic and applied areas and with the advent of modern oxide film deposition methods [23]. The deposition method of the film is the very first important step in material research. So these developments are very important because the better deposition methods would lead to the better quality of the film. There are a several solution methods for deposition of high quality films. MW-CBD method is one of them [22, 24, 25]. Some of the most important advantages of this method are to have short deposition time and that does not require any further thermal annealing, unlike conventional CBD.

To the best of our knowledge, there are no accessible reports related to photodiode applications of the ZnO-NRs films deposited by MW-CBD. But, there are many reports about ZnO photodiodes fabricated by other methods. Among these reports, Orak et al. [26] deposited ZnO layer onto -Si by atomic layer deposition technique. They fabricated Au/ZnO/n-Si photodiode and investigated its current-voltage and capacitance-voltage characteristics. Authors reported that the photovoltaic parameters of device such as short circuit current (), open circuit voltage (), fill factor (FF), and conversion efficiency () are found to be 342 mV, 34.7 A, 32%, and 0.48% under 100 mW/cm2 light intensity. Al-Hardan et al. [27] prepared ZnO nanorods on p-type silicon (p-Si) using low-temperature hydrothermal processing. They investigated current-voltage and capacitance-voltage characteristics of fabricated photodiodes. Authors reported that the rectifying ratio is found to be 370 at 10 V. Yakuphanoglu et al. [28] used the sol-gel spin coating method to prepare nanostructure ZnO film on to p-Si substrate. In their report, it was emphasized that the nanostructure of the ZnO improved the quality of ZnO/p-Si interface. They found the ideality factor and barrier height of the diode to be 3.18 and 0.78 eV, respectively. They also reported that the diode showed a photovoltaic behavior with a maximum open circuit voltage of 0.26 V and short-circuits current of  A under 100 mW/cm2. Yuan and Ren [29] fabricated well-aligned ZnO nanowire arrays on ITO substrates by a spray coating process. In their work, the crystallinity, structure, and morphology of ZnO nanowire arrays were characterized. They investigated current-voltage characteristics of fabricated photodiodes. Authors reported that the RR of this photodiode increased with increasing illumination power from 40 to 100 mW/cm2. And also, Au/ZnO/n-GaAs Schottky barrier diodes were fabricated by Tan et al. In their works, it was emphasized that the device exhibited a photodiode behavior and the serial resistance exhibited a decreasing trend with increasing illumination [30].

In the present study, ZnO-NRs films have been deposited by MW-CBD at different irradiation times (5, 8, and 10 min) and fabricated a photodiodes based ZnO. The effect of irradiation time on the structural, morphological properties of ZnO film has been investigated and the electrical properties of -Si/n-ZnO-NRs photodiodes fabricated by MW-CBD method have also been investigated.

2. Experimental Details

The ZnO-NRs films were deposited by MW-CBD method onto silicon substrates which is p-type (boron-doped) single crystal with (100) surface orientation, having a thickness of 600 m and a resistivity of 1–10  cm. Before the deposition process, p-Si substrates were cleaned chemically by using deionized water and acetone and then were dried with N2 flow. After that they were etched in argon plasma ambient for 10 minutes in HARRICK Plasma Cleaner. Zinc nitrate hexahydrate (ZnN2O6·6H2O; ZnNt) and hexamethylenetetramine (C6H12N4; HMTA) in equal molarity were dissolved in 100 ml deionized water. The certain amount of HMTA catalyst was added to accelerate the reaction, and supply of OH as capping agent promotes anisotropic growth. The solution was stirred at room temperature for 20 min. The substrate was inserted in a beaker containing this solution and transferred into a CEM Mars 6 model microwave oven and irradiated at 600 W for different times (5, 8, and 10 min). Therefore, the obtained samples are named ZnO-5, ZnO-8, and ZnO-10. After MW-CBD treatment, coatings were removed from the solution and rinsed with deionized water and dried under flow. Finally, coatings dried at 60°C for 1 h. By evaporation of high-purity aluminum (Al, 99.999%) under the pressure of Torr, metal contacts were formed on the films. The contacts, which were formed in the form of circular dots of 1 mm in diameter, have 100 nm thicknesses. In this coating process, we used silver paint for a bottom contact after the coating of ZnO because of not forming the ohmic contact on the back surface of silicon wafer before MW-CBD process. Also, any annealing process was not applied to get low resistivity of ohmic contact because of having high eutectic temperature (<830°C) of silver, because such a high temperature can change all the physical properties of the samples. But, not applying any annealing process will lead to the occurrence of a high series resistance. The obtained photodiodes are named PD-5, PD-8, and PD-10. The schematic diagram of these heterojunction diodes is given in Figure 1.

The structure and crystalline quality of the ZnO-NRs films were determined by X-ray diffraction (XRD) using radiation ( Å, Bruker D2 Phaser) at RT with a scanning step size of 0.02°. The surface morphologies of the ZnO-NRs films were analyzed by field emission scanning electron microscopy (Zeiss Ultraplus, FESEM). The current-voltage (-) and capacitance-voltage (-) measurements were taken with Keithley 4200SCS and Signatone Probe Station. The intensity of illumination measurements was carried out using a solar simulator (Sciencetech).

3. Results and Discussion

The crystallinity of the ZnO-NRs films was analyzed by the XRD method. Figure 2 shows the XRD spectra of all the films. The characteristics peaks of zincite phase (JCPDS card file number 36-1451, zincite phase) that have hexagonal wurtzite structure are shown in this figure. Five peaks between 30° and 60° for the ZnO are indicated (100), (002), (101), (102), and (110) planes. The observed peaks at about 32.7°, 54.3°, and 56.5° belong to Si substrate. The preferred orientation of the ZnO-NRs films was evaluated by the texture coefficient (TC) calculated from the XRD data using the well-known formula [31]. The bar graphs inset in Figure 2 show the calculated TC values of ZnO-NRs films irradiated with different irradiation times for each main five (hkl). As seen in this graph, although a dominant preferred orientation has not been observed for ZnO-5 and ZnO-10, ZnO-8 has (002) preferred orientation. Also, the peak, which belongs to Si substrate at 32.7 degree and is observed in the XRD patterns of ZnO-5 and ZnO-10, disappears in the ZnO-8 pattern, meaning that its coating property is better than the others.

The surface morphology of the ZnO-NRs films was examined by using FESEM. Both top view and 50°-tilted view FESEM images of the ZnO-NRs are presented in Figure 3(a)3(f). In these figures, for each film deposited by MW-CBD at three different irradiation times, almost randomly oriented hexagonal nanorods on the surface are observed. At the end of the detailed SEM investigations, we can easily say that almost all the surface was coated with ZnO-NRs, although very few voids on the surface were detected. Particularly, the amount of these voids in ZnO-10 is a bit more than the others, resulting in deterioration in the surface coating. As seen from 50°-tilted views in Figure 3, the length of the observed hexagonal nanorods decreases slightly depending on the increase in the irradiation time. The average lengths of hexagonal nanorods for each irradiation time were measured from the both top and tilted images and these values are approximately 550 nm, 450 nm, and 300 nm for ZnO-5, ZnO-8, and ZnO-10, respectively. Although any significant change in the diameter of the nanorods is not observed, it is seen that the diameters of the nanorods slightly increase, especially at ZnO-8 and ZnO-10, as decreasing their lengths. Furthermore, the obtained XRD and SEM results for three samples support each other greatly.

Basically, a photodiode is a device which converts incident light into an electric current by generating electron-hole pairs due to the absorption of light in the depletion region of p-n junction. In Figure 1, the working principle of a p-n junction photodiode is illustrated simply. As seen in this illustration, as a result of the absorption of the incident light in the depletion region, the inbuilt electric field of the depletion region causes the carriers to move away from the junction and photocurrent is generated. Since the total current of a photodiode consists of the sum of photocurrents and dark currents, the dark current must be reduced to increase the sensitivity of the photodiode [3234]. Figure 4 shows current-voltage (-) characteristics of the p-Si/n-ZnO-NRs photodiodes under dark and various illumination intensities. As seen in these figures, the current of the diodes in the reverse bias region increases with light illumination intensity, whereas the forward current does not change with the illumination. This indicates that photons create electron-hole pairs and the separation of photogenerated electron-hole pairs in reverse bias region is more effective than that of forward bias region. Therefore, the diodes exhibit the conventional photoconducting mechanism. As seen in Figure 4, among the three different photodiodes, PD-8 stands out within the scope of the generated photocurrent in the reverse bias region.

The - characteristics can be analyzed by thermionic emission theory by Bethe [35] that the current density of majority carriers over the potential barrier in this theory is expressed aswhere is the electronic charge, is the applied voltage, is the Boltzmann constant, is the ideality factor, is the temperature, is the series resistance, and is the reverse saturation current. Thanks to this saturation current, the barrier height () of the diodes can be calculated by the following relation:where is the diode contact area and is the Richardson constant (32 A/cm2K2 for p-Si). The and values of the photodiodes were determined from the intercepts and slopes of the forward bias and given in Table 1. The ideality factor values higher than unity are indicator of a nonideal diode behavior, but these values calculated less than or close to 2 are acceptable when the production method and the diode are thought to have heterojunction structure. The transport mechanism of these diodes consists of defect-assisted tunneling with conventional electron-hole recombination. An increase in illumination intensity leads to formation of more free carriers with an associated increase in the photocurrent.


Diode codeI-V characteristicsNorde equation
n  (eV)  (ohm)  (eV)

PD-51.880.770.81
PD-81.740.780.83
PD-102.110.780.79

The open circuit voltage () and short circuit current () of the photodiode under 100 mW/cm2 illumination are given in Table 2. The diode demonstrates a photoresponse behavior having low , low , and high photocurrent values. Naturally, the reason of this photoelectric effect in the structure is due to the light-induced electron generation at the depletion region [36].


Diode
code
  (mV) (A)/  ( V)
100 mW/cm2
RR

PD-54201.591376
PD-83901.567600
PD-101800.381333

To determine the photosensitivity of the photodiodes, / (photosensitivity) values under −2 V were determined and are given in Table 2. As seen in this table, the PD-8 photodiode exhibited the highest photosensitivity as previously observed in Figure 4. The illumination of the diode causes creating photogenerated charge carriers and an increase in the illumination increases the number of these carriers contributing to the current. After the terminating of the illumination, the number of free electrons is decreased and accordingly the current of the diode is also decreased. The trap centers present in the ZnO material play a crucial role to determine the photoconducting properties of the diode. Also, the reason of having maximum photosensitivity of PD-8 is to have a highest photocurrent and lowest dark current. The low photosensitivity values for PD-5 and PD-10 arise from the high dark current of PD-5 and the low photocurrent of PD-10, respectively. Actually, making a correlation between the ZnO-NRs properties and photodiode performance or explaining the exact reason of these results are difficult according to our results but we can say that the coating properties of the surface play an important role in the diode performance, because, as mentioned before in XRD and SEM results, the disappearing of Si peak at 32.7 degrees and being more dominant (002) preferred orientation in the XRD pattern of PD-8 show that the coating of PD-8 is better than the others. Also, according to the detailed SEM investigations, a little more voids on the surface of PD-10 may be the cause of reduction in photocurrent of PD-10.

For further evaluation of the photosensitivity behavior of the diode, the variation of photocurrent depending on the illumination intensity was investigated. In order to analyze the photoconducting mechanism, we used the following relation:where is a constant, is the photocurrent, is an exponent, and is the illumination intensity. Setting where is also constant and taking logarithms of both sides of (3) giveand to deduce the exponent of the illumination intensity, log-log plot of diode current versus illumination intensity can be used. The plots of versus curves are shown in Figure 5. The obtained values of the photodiodes were 1.03 (for PD-5), 0.94 (for PD-8), and 0.69 (for PD-10). The obtained results may be evaluated as a result of the existence of a continuous distribution of localized states in the mobility gap of these materials [37, 38].

The rectification ratio (RR) of the forward current () to the reverse current () at  V applied voltage was calculated and given in Table 2. The reverse current is as large as the forward current as the increase of bias and the calculated values are larger than other related works in the literature [3941].

The barrier height and series resistance values of the photodiodes can also be obtained using a method developed by Norde. The following function has been characterized by the modified Norde’s method [42]:where is the integer (dimensionless) greater than and is the current obtained from the - characteristic. Once the minimum of the versus plot is determined from Figure 6, the value of barrier height can be obtained from (6), where is the minimum point of and is the corresponding voltage. The series resistance of the junctions can be calculated as follows: where is the corresponding current. By using the Norde method, the barrier height and series resistance values of the diodes were calculated and presented in Table 1. As seen in this table, the barrier height values calculated by Norde are very close to that of obtained from -. The values of series resistance are considerably high and the reason of being high of these calculated values, as mentioned before in the experimental section, is most likely due to the fact that no any annealing process was applied to get low resistivity for back ohmic contact.

To investigate the - characteristics of p-Si/n-ZnO-NRs, - and - plots taken at different frequencies were used. These graphs obtained between 10 kHz and 1 MHz are shown in Figure 7. As seen in these figures, all graphs illustrate same trend; that is, the capacitance value increases with the applied bias voltage, and also depending on the increase in frequency, the capacitance decreases. At the same time, the highest capacitance values belong to PD-8. In the range between 0.5 V and 1 V, a linear behavior of - curves has been observed and the reason of this linear behavior is the linear change in the depletion region of the heterojunction diode. Using the following relation, the - characteristics of the obtained heterojunction diodes can be analyzed [43]where is the built-in potential, is the dielectric constant of semiconductor (), and is the acceptor concentration. From the - measurements, the following relation was used to determine the barrier height of the diode [44],where is density of states in the valence band ( cm−3). At the stage of calculation of barrier height, the and values obtained from - plots, which are shown in Figure 8, were used. The obtained values for and   are given in Table 3 at different frequencies. As seen in this table, both and barrier height tend to increase with increasing frequency, and also, while values increase for PD-8, it decreases by about ten times in the PD-10. Considering the values obtained depending on the frequency from -, for PD-5 and PD-10, the values are larger than that of obtained from -, but PD-8’s are smaller. Probably, the presence of trap states and oxide layer at interfacial layer of the device and inhomogeneity that can be observed in terms of charge distributions and thickness in the interfacial layer may have caused these differences between them [4547]. The same reasons may have played an important role in the differences observed in values for three samples.


Diode codeFrequency (kHz)  (cm−3)  (V)  (eV)

PD-51001.490.87
2001.791.04
4001.951.10
5002.151.17
10002.061.14

PD-81000.570.57
2000.730.63
4000.700.62
5000.660.60
10000.720.62

PD-101000.510.58
2001.200.88
4001.490.99
5001.490.99
10001.691.07

Figure 9 shows the variation of the series resistance of the fabricated p-Si/n-ZnO-NRs photodiodes with applied bias. In this figure, a peak is observed and this peak decreases with increasing frequency, and also it shifts to the higher positive voltages. The decrease in the peak intensity and the shifting of this peak with increasing frequency mean that the interface charges follow the frequency of the applied voltage [32, 35].

4. Conclusion

To obtain ZnO-NRs, MW-CBD method was used. The structural and morphological properties of ZnO-NRs were investigated depending on the microwave irradiation time (5, 8, and 10 min). The XRD spectra of all the films exhibited polycrystalline nature. According to the calculated TC values, a dominant preferred orientation was only observed for ZnO-8 in (002) direction. The presence of randomly oriented ZnO nanorods for all the films was confirmed by FESEM results. Also, these results showed that the length of nanorods decreased slightly depending on the increase in the irradiation time. The p-Si/n-ZnO-NRs heterojunction structures were fabricated and their electrical characterizations were performed. According to the obtained results, it was determined that these p-n junctions exhibited both a good photosensitivity and photoconducting behavior with high photocurrent. Among these heterojunctions, the highest photosensitivity was determined to be 7600 for p-Si/n-ZnO-NRs (PD8) photodiode. Through the - measurements of p-Si/n-ZnO-NRs photodiodes, the barrier height and series resistance were calculated. The obtained results suggest that the p-Si/n-ZnO-NRs photodiodes can be used as a sensor in the optoelectronic applications.

Conflicts of Interest

The authors declare that they have no conflicts of interest.

Acknowledgments

This work was supported by Anadolu University Commission of Scientific Research Projects under Grant nos. 1305F082 and 1402F055.

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Copyright © 2017 Saliha Ilican 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.


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