Structural and Optical Properties of Al2O3 Nanostructures Prepared by Hot Water Treatment Method

Structural and Optical Properties of Al2O3 Nanostructures Prepared by Hot Water Treatment Method

Israa Abdullhasan Abbas Khalidah H. Al-Mayalee*

Department of Physics, Faculty of Education for Women, University of Kufa, Najaf 54001, Iraq

Corresponding Author Email: 
khalidah.almayali@uokufa.edu.iq
Page: 
527-532
|
DOI: 
https://doi.org/10.18280/rcma.340414
Received: 
24 June 2024
|
Revised: 
9 August 2024
|
Accepted: 
19 August 2024
|
Available online: 
27 August 2024
| Citation

© 2024 The authors. This article is published by IIETA and is licensed under the CC BY 4.0 license (http://creativecommons.org/licenses/by/4.0/).

OPEN ACCESS

Abstract: 

Aluminum oxide (Al2O3) nanostructures were synthesized on an aluminum foil substrate by green synthesis method using the hot water treatment method at 75°C for 1, 7, 15, and 30 minutes. In this study, growth time was varied to study its effect on the Al2O3 nanostructure’s size and density. The morphological and structural properties of the as-prepared Al2O3 nanostructures were investigated using SEM imaging and XRD analysis, and the optical properties were studied through UV-Vis spectroscopy. Scanning electron microscopy (SEM) investigations revealed porous agglomerated Al2O3 nanostructures, and the porous nanostructured particle size decreased in the 80 nm-35 nm range as the synthesis reaction time increased from 1 to 30 minutes. X-ray diffraction (XRD) analysis indicated the crystalline behavior increased with increasing time. The optical properties results showed that Al2O3 nanostructures display a relatively broad absorption spectrum across the ultraviolet region. Furthermore, the energy gap (Eg) increased from 3.44 to 3.78 eV when the immersion time increased from 1 minute to 30 minutes, respectively. These results have a significant impact on the Al2O3-assisted electronic application based on HWT Al2O3 nanostructures for a sustainable green earth.

Keywords: 

Aluminum oxide (Al2O3), HWT method, nanostructures, high porosity, optical properties

1. Introduction

Nanostructured materials have been intensively researched during the last few decades due to their unique physical and chemical properties such as temperature stability, melting point, electrical and thermal conductivity, catalytic activity, light absorption, and wettability [1]. Nanostructures like nanowires, nanosheets, and nanoparticles provide immense technological advantages to be used in potential industrial and biomedical applications such as sensors, optical devices, catalysts, and drug delivery system [2]. The smaller size of metal oxide nanostructures (NSs) leads to high stability, high surface to volume ratio, high carrier capacity, high chemical reactivity and biological activity, and tunable size for wide range of beneficial applications [3]. For example, Al2O3 nanostructured materials showed remarkable applications such as surface passivation, wear protection, ant-reflection coating, gas diffusion barrier, and catalyst. This is due to good optical properties, high corrosion resistance, surface catalysis, thermal stability, and high surface area of the Al2O3 NSs [4, 5]. Aluminium oxide (Al2O3) is an inorganic chemical compound of aluminum and oxygen and is commonly referred to as alumina. It is also called corundum due to the crystalline form of aluminum oxide, in which six oxygen atoms surround one aluminum atom, resulting in porous structures [6]. Al2O3 is a light white powder that can be found in amorphous and polycrystalline forms. Al2O3 has a melting point of around 2020℃; it is insoluble in water and organic materials but somewhat soluble in acids and alkalis. It is an excellent material with high chemical resistance and thermal stability [4, 6].

Recently, different techniques were used to produce aluminum oxide NSs, from those methods, HWT is a simple, a one-step, scalable, low fabrication temperatures (<100℃), and cost-effective process for preparing metal oxide nanostructures on the surface of their metals [6, 7]. The HWT process involves immersing the metal foils in hot deionized water without any chemical additives [8]. Since nanoparticle size and surface morphology are strongly correlated with the optical, mechanical, and electrical properties, the successful synthesis of the Al2O3 nanostructures and studying the growth parameters are very important because they will provide useful information that might help to improve their application performance. In this study, the effect of growth time on the structure and morphology of the aluminum oxide nanostructures was investigated thoroughly by scanning electron microscopy and X-ray diffraction measurement.

2. Experimental Procedure

Hot water treatment (HWT) method was used to prepare Al2O3 nanostructures by immersing the aluminum plate (99.99% purity) 1.5 cm×2c m in hot (75℃) deionized water (DI). First, the samples were prepared using conventional polishing techniques (4000 grit papers). The aluminum metal foils were cleaned in an ultrasonic bath using acetone and then subsequently rinsed with deionized water to remove any surface impurities and dried with an air gun. Al foils were placed in DI water at 75℃ for different growth times: 1 min, 7 min, 15, and 30 min as shown in Figure 1. After that, the treatment samples were dried for 6 hours in air. X-ray diffraction (XRD) and scanning electron microscopy (SEM) are used to characterize the structural and morphological properties of the prepared samples.

Figure 1. Al foils treated in hot water treatment at 75℃ for 7 minutes, 15 minutes, and 30 minutes

3. Results and Discussion

3.1 Morphological and structural characterization

Figure 2 shows the X-ray diffraction patterns of the (a) aluminum metal foils and treated aluminum metal foils in hot water at 75℃ temperatures for different durations (b) 1 minute, (c) 7 minutes, (d) 15 minutes, and (e) 30 minutes.

Figure 2. XRD spectra of Al metal substrate, $\alpha$-Al2O3 nanostructures prepared by HWT at 1minute, 7 minutes, 15 minutes, and 30 minutes

The XRD pattern for Al metal substrate shows intense peaks located at 2$\theta$ = 38.70°, 44.94°, 65.25°, 78.41° which are attributed to the Al (111), (200), (220), and (311) plans respectively. These observations are similar to those published by [9-11]. The obtained peaks were compared with typical diffraction data to identified $\alpha$-Al2O3 NSs. As shown in Figure 1, there are five recorded diffraction peaks corresponding to (104), (113), (024), (116), (214). These observations are matched well the same structure reported in [9, 12-14]. These standard data are attributed to the rhombohedral structure [15]. Also, XRD results showed that the intensity of the peaks increased when the depositing time increased from 1min to 30 min and became sharper, this is due to decreasing the crystallite size [14].

The XRD experimental results revealed that the diffraction intensity increases with increasing the hot water treatment time from 1 to 30 min. The sharp and high-intensity peaks suggested an increase in grain size and improved crystallinity and surface texture of nanostructures [16].

The mean crystallite size of $\alpha$-Al2O3 calculated from the full width at half-maximum (FWHM) of the XRD peak $\beta$ (in rad), X-ray radiation wavelength used ($\lambda$ = 1.54060A), Scherrer constant (K = 0.9), and the diffraction angle $\theta$, using Scherer equation ($\text{D}=\text{K }\!\!~\!\!\text{  }\!\!\lambda\!\!\text{ }/\text{ }\!\!\beta\!\!\text{ }\cos \text{ }\!\!\theta\!\!\text{ }$) [15]. The calculated average crystalline grain size of $\alpha$-Al2O3 for the most intense peaks are summarized in the Table 1. From Table 1, it is observed that the crystallite size increases with increasing treatment time due to the grain coalescence with increasing growth rate [7, 14].

Table 1. Average crystal size of $\alpha$-Al2O3 nanostructures for different HWT times

HWT Time

2θ° (113)

FWHM (β) Deg

Average Crystal Size (nm)

1 minute

42.90

0.72

11.85

7 minutes

42.80

0.30

28.43

15 minutes

42.90

0.25

34.13

30 minutes

42.90

0.24

35.6

The morphological characteristics of the as-grown Al2O3 nanostructures were investigated using scanning electron microscopy (Thermo ScientificTM Quattro SEM). Figure 3 shows SEM images of Al2O3structures grown on Al metal substrate at 75℃ for 1, 7, 15, and 30 minutes.

From Figure 3, Al2O3 nanostructures are formed after one minute treatment of the Al metal substrates with average nanoparticles size about 66 nm. With increasing treatment time to 7 minutes, overlapped, highly porous (macroporous alumina) nanostructures with an average particle size about 55 nm are observed [17]. Also, as we can see from Figure 2, after 15 minutes of HWT, the density of NSs significantly increased due to high aggregated Al2O3 nanoparticles with average size about 42 nm. A uniform distribution of 3D aluminum oxide NSs with average particles size about 40 nm was achieved after 30 minutes. All the sample structures of the alumina particles shown in Figure 2 look like a porous network. The reason for this is that the individual alumina particles with high activity and high surface energy tend to stick with each other to form agglomerates as a neck-formation [17, 18]. These results are in good agreement with previous reported studies [19, 20]. Also, it can notice that the porosity increased with increasing treatment time due to the nanoparticle’s agglomeration.

Figure 3. Surface morphology images of the Al metal sheet treated in hot deionized water with various time

Figure 4. (a) Scanning Electron Microscopy (SEM) image; (b) EDS analysis data for Al metal sheet treated in hot deionized water for 15 minutes

The chemical compositions of the aluminum oxide sample which formed on Al metal sheets surface after HWT at 75℃ for 30 minutes were determined by Energy Dispersive Spectroscopy (EDS) and shown in Figures 4(a) and (b). Spectrum analysis Figure 4(b) reveals that the weight percentages of aluminum and oxygen elements were 32 and 68 atomic after hot water treatment for 15 minutes.

3.2 Optical characterization

The optical properties of porous $\alpha$-Al2O3 nanostructures on Al metal substrates were carried out using UV-Vis spectrometer. The measurements have been taken in the wavelength range 200-1000 nm. Figure 5 displays the optical absorbance vs. wavelength spectra of $\alpha$-Al2O3 NSs obtained from surface hot water treatment at various times. Results revealed that Al2O3 samples exhibited a strong absorption near 292, 290, 290, and 290 nm at 1, 7, 15, and 30 minutes, respectively. The absorption peaks intensity increased with increasing Al2O3 NSs synthesized time in hot de-ionized water due to increasing the oxidation rate of aluminum surface atoms [21, 22]. This means more atoms of aluminum metal are converted to its oxide (alumina) with nonporous and transparent structures.

Figure 5. UV–Vis spectra of as-prepared Al2O3 nanostructures synthesized at varied synthesis times

Figure 6 displays the absorption coefficient values of NSs at different synthesis times (1, 7, 15, and 30) min that can be estimated from the absorbance (A) and thickness (d) using this relation $\text{ }\!\!\alpha\!\!\text{ }=(2.303\text{ }\!\!~\!\!\text{ A}/\text{d})$ [23, 24]. The extinction coefficient values of Al2O3 NSs synthesized at 1, 7, 15, and 30 min that were obtained from the equation (k= $\text{ }\!\!\alpha\!\!\text{ }\frac{\text{ }\!\!\lambda\!\!\text{ }}{4\text{*}3.14}$) [28] are presented in Figure 7.

Figure 6. The absorption coefficient of as-prepared Al2O3 nanostructures synthesized at varied synthesis times

Figure 7. Extinction coefficient of Al2O3NSs synthesized at varied synthesis times

A graph in Figure 8 was drawn between log ($\alpha$hν) and log (hν) of Al2O3 nanostructures for all synthesized samples. The optical band gaps Eg were calculated from photon energy (hν) using the Tauc’s equation [25, 26]:

$\alpha h v=A\left(h v-E_g\right)^n$

where, A is a proportionality constant, $\text{ }\!\!\alpha\!\!\text{ }$ is the absorption coefficient. n is the exponent factor that characterizes the nature of electronic transition causing the absorption and can take the values 1/2 and 2, which corresponds to direct or indirect transition, respectively [27]. As shown in Figure 8, the observed results clearly indicated that there is decrease in the band gap values with varying hot water treatment times. The band gaps of aluminum oxide NSs were found to be 4.02 eV, 4.06 eV, 4.05 eV, 4.047 eV for 1 min, 7 min, 15min, and 30 min respectively. The lower band gap of the pores Al2O3 NSs may be indicated enhanced oxidation, due defect states, and depending on the shape, size of the nanoparticles [28, 29].

Figure 8. The $[\alpha \mathrm{h} v]^2$ versus hυ plots (using Tauc’s equation) Al2O3 NSs with different deposition time

4. Conclusions

In conclusion, a simple and low cost HWT method was used to synthesized aluminum oxide nanostructures on Al metal substrate at low temperature and deferent fabrication times. The obtained surface morphology properties confirm the successful growth and formation of Al2O3 nanostructures. Effects of time on the nanostructure growth rate have also been studied. Variation in the HWT treatment time of Al sheets led to the formation of nanostructured semiconducting/metal (Al2O3/Al) surfaces. we noticed the nanostructures forming at a faster rate. The formation alumina nanostructured materials took one minute and developed in 7 minutes [20]. This study indicated that the immersion time of Al foils in hot deionized water has a significant effect on the morphology and pore size of alumina. Al2O3 samples showed direct band gaps of about 4.04eV, 4.06eV, 4.05eV, and 4.047eV for 1 min, 7 min, 15 min, and 30 min, respectively. The Al2O3/Al and nanostructured semiconducting materials prepared in this study could be useful for a wide range of applications, such as solar cells, sensors, optoelectronic devices, catalysis, adsorption, and electronic devices or biomaterials, due to their adjustable pore structure, large surface area, and porous structures.

Acknowledgment

The authors would like to acknowledge the staff of the Physics Department at the Faculty of Education for Women, University of Kufa, for their support of this research. Additionally, the authors extend their gratitude to Dr. Adel H. Omran Alkhayatt from the Physics Department at the Faculty of Science, University of Kufa, for his assistance with UV-Vis analysis.

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