1. Introduction
Transition metal oxide nanoparticles (NPs), such as Cu2O, MnO2, NiO, TiO2, Co3O4, SnO2, and Fe2O3, are excellent candidates for use in electrocatalytic activity as they promote electron-transfer reactions and in medicinal applications. Among these, semiconductor nanoparticles such as NiO are promising materials in advanced research because of their utility in catalysis, gas sensors, and optoelectronics [1,2]. Metal oxides are low-cost materials for a wide range of optical applications and NiO is a p-type semiconductor with a wide bandgap (3.6–4.0 eV) [3,4]. Owing to its excellent chemical stability and its magnetic and optical properties, NiO has been tested as an active material for use in chemical sensors [5,6], pseudo-capacitor electrodes [7], photocathodes in dye-sensitized solar cells [8], catalysts [9], magnetic materials [10], and random-access memory devices [11,12]. Currently, several physical, chemical, biological, and hybrid methods are available for the synthesis of different types of metal oxide nanoparticles. The development of clean, non-toxic, and eco-friendly techniques has resulted in the observation of biological systems [13,14]. In particular, there has been more focus on plant-based materials, owing to their easy availability, low cost, and abundance of biomolecules such as polyphenols, flavonoids, proteins, terpenoids, and amines.
In the last decade, few attempts have been made to employ lanthanum doping of nanoparticle oxides. Numerous surface defects occur when La3+ ions are applied as doping elements, hindering the recombination of photo-induced electron-hole pairs. The recombination is hampered due to the creation of trap energy levels by the dopant. Similarly, La3+ ion-doped TiO2 nanoparticles have attracted significant attention in photocatalytic processes for the degradation of organic pollutants [15]. Moreover, La3+ absorbs light in the infrared region and can tune the bandgap of wide-bandgap materials such as NiO. Recently, La3+ ion-doped NiO has attracted considerable attention, owing to its interesting applications. La-doped NiO nanofibers were synthesized by the electrospinning method and evaluated as potential electrode materials for application in high-performance supercapacitors and other applications [16,17,18].
Herein, the green synthesis of rare earth (La) ion-doped NiO nanoparticles was carried out using Sesbania grandiflora leaf extract for antimicrobial studies, and their characteristics were analyzed. The optical properties of the La-doped NiO nanostructures were analyzed by UV–Vis diffuse reflectance spectroscopy (DRS), and their altered bandgaps were estimated. The structural properties of the prepared materials were observed by X-ray diffraction analysis. The morphological features of the prepared nanostructures were determined by scanning and electron microscopy. The chemical composition and oxidation states of elements were studied through X-ray photoelectron spectroscopy. Moreover, the prepared nanostructures were adopted for medicinal applications, and their efficiency in antibacterial activity was preliminarily studied. 2. Materials and Methods 2.1. Synthesis of Lanthanum-Doped Nickel Oxide Nanoparticles
Nickel chloride hexahydrate (NiCl2.6H2O) (Sigma Aldrich, St. Louis, MO, USA), lanthanum (III) chloride heptahydrate (LaCl3.7H2O), and NaOH were used to synthesize NiO nanoparticles (NPs). To prepare the La-doped NiO nanostructures, 2 g of NiCl2.6H2O with various amounts of LaCl3.7H2O (0, 2, 4, 6, 8, and 10 wt%) was dissolved in 250 mL of distilled water to obtain a homogeneous solution at room temperature by constant high-speed stirring at 500 rpm. After solution was prepared, 25 mL of plant extract was added to the solution. Then, 2 M NaOH was added dropwise until the pH reached 12, and stirring was continued for 6 h. Finally, a green gel was formed, which was heated at 80 °C for 24 h to obtain a precipitate. The precipitate was washed with water and ethanol repeatedly and centrifuged to remove any residue or impurities. Subsequently, the obtained samples were annealed at 500 °C for 2 h to obtain pure nanoparticles [6].
Before NiO NP preparation, an extract was prepared from Sesbania grandiflora leaves. In a 1000 mL conical flask, 10 g of dried plant leaves was mixed with 500 mL of water, and the mixture was boiled for 5 min and decanted. Finally, the leaf extract was filtered and stored in a bottle for future use. 2.2. Characterization X-ray diffraction (XRD) analysis was used to characterize the crystalline nature of the nanostructures, and Bragg diffraction peaks were obtained using a PANalytical X’Pert PRO diffractometer equipped with Cu-Kα radiation of 1.54 Å. The functional groups of biomolecules were confirmed by an attenuated total reflectance (ATR) mode Fourier transform infrared (FTIR) spectrophotometer (Thermo Scientific, Waltham, MA, USA) in the range 400–4000 cm−1. The optical properties of the prepared nanomaterials were studied using a UV–Vis-NIR spectrometer (Varian Cary 5000). The morphological features of the prepared nanomaterials were studied using scanning electron microscopy (SEM, S-4800 Hitachi) and transmission electron microscopy (TEM, H-7600 Hitachi). The oxidation states of the elements were analyzed using an X-ray photoelectron spectrometer (XPS, Thermo Scientific, Waltham, MA, USA). 2.3. Antimicrobial Activity
The antibacterial activity of NiO NPs was studied using the zone inhibition method. Gram-positive and Gram-negative bacterial strains, E. coli and Bacillus spp., respectively, were selected as test organisms. The bacterial cultures were inoculated in Luria broth (liquid phase) in 100 mL conical flasks, and the flasks were incubated overnight at 37 °C. The overnight active Escherichia coli (E. coli) and Bacillus spp. cultures were seeded into Luria agar medium using spread plate techniques. Later in the Luria agar plates, cavities were made with the help of a metallic borer. All cavities were filled with 100 µL of NiO NP solution, and the petri plates were then incubated at 37 °C overnight. The standard antibiotic streptomycin was used as a positive control. The zone of inhibition was measured using digital Vernier calipers, and the values were reported in centimeters [7].
3. Results and Discussion 3.1. Structural Properties
XRD analysis was used to investigate the crystal structure, lattice parameters, and crystallite sizes of La3+ ion-doped NiO nanoparticles. Figure 1a shows the XRD patterns of pure NiO and La3+ ion-doped NiO nanoparticles. The spectra show the presence of well-defined peaks attributable to the (111), (200), (220), and (311) planes, corresponding to the cubic NiO phase (JCPDS 040-835) [6]. Note here that no peaks related to other crystalline phases (such as Ni2O3) were found in these spectra at the resolution limit of the apparatus, indicating that the structure of NiO was not altered by lanthanum doping. In addition, there are no peaks associated with lanthanum oxide (La2O3) or lanthanum nickel oxide (LaNiO3) in the XRD spectra probably because of the low La content. The size of the particles at different doping concentrations can be calculated from the X-ray peaks of La3+ ion-doped NiO nanoparticles using the Scherrer formula [7]:
D = kλ/βcosθ
where K = the Scherrer constant (0.89), λ=1.5406 Å is the wavelength of the Cu Kα line used by the instrument, and βhkl is the peak full width at half maximum can be calculated from a graph of intensity vs. diffraction angle θ of the X-rays. The average crystallite size values of NiO: La were found to vary between 23 and 10 nm (Figure 1b) depending on the La3+ ion content. This shows that doping with La inhibits the growth of crystallites, leading to a depressed crystallinity phenomenon. Moreover, the intensity of the diffraction peaks decreases, and the full width at half maximum increases, implying that the size of the crystallites decreases. As seen from the XRD pattern, the intensity of the peaks decreases with increasing lanthanum concentration, which may destroy the crystal structure. This decrease in grain size with doping can improve the performance of many nickel oxide-based devices.
The average particle size decreases with increasing doping concentration, while the average strain increases [19]. Xu et al. [17] reported that La can be incorporated into metal (M) oxides by the formation of M–O–La bonds on the surface of small particles. This inhibits the movement of surface Ni atoms and results in coarser particles by restricting direct contact of neighboring crystallites, thus preventing the agglomeration of NiO nanoparticles and inhibiting coagulation.
3.2. FTIR Analysis
The FTIR spectra, shown in Figure 2, indicates the functional groups in the La3+ ion-doped NiO nanoparticles. The peak around 3299 cm−1 is due to symmetric and asymmetric O–H stretching. The peak positioned at 1628 cm−1 is associated with carbonyl C=O bending. The intense peak at 1320 cm−1 is attributed to the symmetric stretching of C-H. The carbonyl group stretching (>C=O) may cause the NiO nanoparticles to play a role in bridging networks [20]. The sharp peaks at 834 cm−1 are due to the combined effects of in-plane deformation of NiO and stretching vibrations of the metal oxide bonds (-M–O, M–La). The absorption bands at 995 and 1428 cm−1 are due to carbonate groups and that at 2995 cm−1 is due to C–H stretching. After the sample was annealed at 500 °C, the absorption band at 1421 cm−1 (Figure 2b) is still present, confirming its association with a carbonyl group. A significant peak at 436 cm−1 is due to the Ni-O bond in the sample. The peaks at 485 and 865 cm−1 are associated with Ni-O vibration and Ni-O-H stretching, indicating bridging and non-bridging vibrations of these bonds. [21,22,23]. Moreover, after drying the sample, the peaks from the biomolecules disappeared, and the remaining carbon is associated with NiO or NiOLa.
3.3. Optical Properties
The optical properties of lanthanum (La3+) ion-doped NiO nanoparticles and pristine NiO nanoparticles were studied. Absorption spectra were recorded by a UV–Vis-NIR spectrometer in the range 200–750 nm, as shown in Figure 3a. From the spectra, it can be seen that the absorption band is slightly shifted towards a higher wavelength (redshift) with La3+ addition, which denotes the formation of trap energy levels due to the dopant atoms. When the concentration of La is 2–10 wt%, the absorption intensity also increases with increasing La3+ ion concentration.
In the UV–Visible-absorption spectra, the characteristic band edges are shifted towards lower energy regions (Figure 3b), which, due to quantum confinement, may have caused the absorbed wavelength to shift to a lower energy state with an increase in the doping concentration. As the concentration of lanthanide ions increases, the fundamental absorption edge tends to shift to higher wavelengths. In addition, the shift of the absorption band to lower energy could be attributed to the decreasing formation of non-bridging oxygen, which binds the electrons from formless energy in non-bridging oxygen to bridging oxygen [24,25,26,27]. It can be seen that the maximum absorption edge of the La3+ ion-doped NiO nanoparticles appears to be at 272 nm. The energy gap of the La3+ ion-doped NiO nanoparticles can be determined using the Tauc relation [4].
(αhν)n = A (hν–Eg)
where n is a number depending on the nature of the transition process, and A is the coefficient of absorbance. For direct transition, n = 2, and for an indirect transition, n = 0.5. Therefore, the direct bandgap of La3+ ion-doped NiO nanoparticles can be obtained by extrapolating the linear portion of the (αhʋ)2 versus hʋ curve to the energy axis, as shown in Figure 3b. The bandgap of La3+ ion-doped NiO nanoparticles calculated from this plot is between 3.17 and 3.79 eV, increasing with a higher concentration of the La3+ ion [28].
The value of the direct energy bandgap (Eg) can be obtained from the intercepts by extrapolating the linear portion of the curve to the linear axis representing the photon energy. The optical bandgaps of the direct and indirect bandgaps depend on changes in the structure of the former (NiO) with the modifier (La3+). The formation of NiO leads to tight binding of oxygen anions to the host materials. Hence, the optical band gap decreases with an increasing number of bridging La3+ ions in the network system. Moreover, the decreasing value of the optical bandgap might be due to the increasing number of non-bridging oxygens [29,30,31].
3.4. Morphological Analysis
The morphological features of prepared nanoparticles were analyzed by SEM and the obtained results are shown in Figure 4. The SEM images reveal the typical nanostructure of La-doped NiO with spherical and other irregular shapes. The nanoparticles appear to be spherical or cubical, as shown in the SEM images of Figure 4. In the existing literature, spherical nanoparticles have been reported using a green synthesis method [30,31,32]. EDS analysis confirms that La3+ ions are doped into NiO nanoparticles, as shown in Figure 4g. The size of the nanoclusters was difficult to estimate from the SEM images in Figure 4. Some of the nanoparticles become agglomerated after the annealing process, as an effect of the heating. The distribution of nanoparticles (NiOLa-04) was easier to observe by TEM analysis, and the results are shown in Figure 5. The prepared nanoparticles have very small spherical and cubical structures and few are agglomerated nanoparticles. Generally, the size and shape of nanoparticles play a significant role in catalytic applications and other chemical/biological applications owing to their large surface area.
3.5. XPS Analysis
The oxidation states and chemical composition of the prepared La-doped nanostructures (NiOLa-04) were determined by XPS, and the results are presented in Figure 6. The survey scan (Figure 6a) shows the presence of C, N, O, Ni, and La in the fabricated sample. The deconvoluted components of carbon (Figure 6b) are denoted as C1 (284.2 eV), C2 (284.8 eV), C3 (287.9 eV), C4 (288.9 eV), and C5 (293.0 eV). The binding energies of 284.2 and 284.8 eV represent non-oxygenated hydrocarbons with C-H sp2 and sp3 bonds from biomolecules. The peaks at 287.9 and 288.9 eV correspond to carbonyl and carboxylic groups in biomolecules, respectively, which are strongly bound to the surface of the prepared nanoparticles. Moreover, the carbon peaks also suggest carboxylic C-O-Ni linkages, where biomolecules derived from leaf extract may act as capping agents. Furthermore, the broad spectrum (Figure 6c) of La contains doublet peaks La1 and La2 at 834.4 and 837.9 eV, respectively, owing to La 3d, indicating the presence of La in the prepared sample. The deconvoluted spectrum of Ni (Figure 6d) contains six peaks, which are represented as Ni1 (853.4 eV), Ni2 (855.4 eV)—attributed to the doublet of Ni2+ 2p 3/2, and a satellite peak observed at 860.5 eV (Ni3); peaks at 870.6 eV (Ni4), 872.5 eV (Ni5)—ascribed to Ni2+ 2p 1/2, and its satellite peak located at 878.6 eV (Ni6), which strongly support the formation of NiO NPs [33,34]. The deconvoluted peaks (Figure 6e) O1 (529.5 eV), O2 (530.8 eV), and O3 (535.2 eV) can be attributed to the oxygen in NiO, with O2 and O3 representing Ni-O-Ni/Ni-O-C, i.e., carboxylic group-containing functional groups of biomolecules such as protein groups in the leaf extract bonding with Ni.
3.6. Antibacterial Activity
The antibacterial activity of NiO NPs was studied using the zone inhibition method and both Gram-positive and Gram-negative bacterial strains, E. coli and Bacillus spp., respectively, were used as test organisms. The antimicrobial and antifungal activities of nanoparticles depend on the physicochemical properties of nanoparticles and the type of bacteria and fungi, which can significantly affect the functions of the bacterial cell. Bacillus spp. are nonpathogenic bacteria and contain a thicker peptidoglycan (PG) layer; therefore, the toxicity of NiO NPs is less than that of Bacillus spp., as shown in Table 1.
By observing the inhibition zones, it can be stated that La3+ ion-doped NiO NPs exhibit good antibacterial activity against the Gram-positive and Gram-negative bacterial strains (Table 1). The maximum sizes of the inhibition zone observed for the 4% La sample against Gram-positive Bacillus spp. and Gram-negative E. coli bacterial strains, grown in nutrient agar medium, are 1.00 cm and 1.15 cm, respectively, similar to those of the standard antibiotic streptomycin.
Owing to their nano size and stability, the NPs showed better antibacterial activity in the present study. The small size usually enhances fusibility and penetration into the intracellular matrix, interacting with intracellular Ca2+ absorption, and causing cell damage. Attachment of nanoparticles with a reduced size initiates electrostatic interactions between the La-doped nickel ions released from the NPs and the cell membrane of the microbes, which causes cell membrane damage. A damaged cell membrane is more sensitive to further reactions and allows for the penetration of nanoparticles and the outflow of intracellular organelles. These sequential steps improve the inhibitory activity of the nanoparticles. A theoretical antimicrobial mechanism of NiO-NPs has been previously reported [35,36]. The penetration of NiO-NPs inside the microbial cell further enhances microbial inhibition by interacting with the electron transport and destroying DNA by separating the phosphate and hydrogen bonds, denaturing the protein by modifying the tertiary structure, and damaging the mitochondria by oxidative stress, generating reactive oxygen species (ROS) from interactions between the inorganic metal and La-doped NiO nanoparticles, which finally leads to cell death. The antibacterial activity is mainly governed by the size, phase, concentration, stability, and morphology of the nanoparticles, and reaction time. Hence, the activity and stability of La-doped NiO NPs are very effective against common pathogens and can also be utilized as an effective catalyst in wastewater treatment as an alternative to the bleaching process.
4. Conclusions In summary, La-doped NiO nanoparticles were successfully synthesized in Sesbania grandiflora leaf extract. The NiO nanoparticle crystallinity decreased with increasing dopant concentration, which led to a decrease in the particle size, as indicated by XRD analysis. SEM analysis revealed that the NiO nanoparticles possessed spherical and irregular shapes, and the size of the particles was decreased by increasing La3+ ion doping concentration. For a concentration of 4% La3+ ion-doped NiO nanoparticles, the direct bandgap was calculated to be 3.17 eV. The NiOLa-04 nanoparticles show appreciable antibacterial activity against both Gram-positive and Gram-negative bacteria; hence, these nanoparticles could be used as an effective bioremediation and as an antibacterial agent in current nanomedicine.
Figure 1.(a) X-ray diffraction analysis of NiO and La3+ ion-doped NiO nanoparticles. (b) Calculated average crystallite size with the dopant.
Figure 2. FTIR spectra of La3+ ion-doped NiO nanoparticles: (a) before annealing; (b) after annealing.
Figure 3.(a) UV-Vis spectra of NiO and La3+ ion-doped NiO nanoparticles. (b) The energy gap between NiO and La3+ ion-doped NiO nanoparticles.
Figure 4. SEM images and EDS spectrum of prepared nanostructures (a) NiO, (b) NiO-La-02, (c) NiOLa-04, (d) NiOLa-06, (e) NiOLa-08, and (f) NiOLa-10, and (g) EDS spectrum of NiOLa-04 nanoparticles.
Figure 5. TEM images of NiOLa-04 nanoparticles: (a) 100 nm magnification; (b) 20 nm magnification.
Figure 6. XPS spectra of NiOLa-04 nanoparticles: (a) survey scan; (b) carbon; (c) lanthanum; (d) nickel; and (e) oxygen elements.
Sample | Microorganisms | Zone of Inhibition (cm) |
---|---|---|
Bacillus subtilis | 0.65 | |
Pure NiO | Escherichia coli | 0.80 |
Bacillus subtilis | 0.8 | |
NiOLaO2 | Escherichia coli | 0.9 |
Bacillus subtilis | 1.0 | |
NiOLaO4 | Escherichia coli | 1.15 |
Bacillus subtilis | 0.85 | |
NiOLaO6 | Escherichia coli | 1.0 |
Bacillus subtilis | 1.25 | |
Standard antibiotic Streptomycin (AB) | Escherichia coli | 1.4 |
Author Contributions
S.S. performed the experiments; T.K. reviewed the manuscript and supervised the work; G.N. performed the antimicrobial experiments; H.S.A. and S.A.A. provided resources and funding; L.V.R. edited the manuscript; K.M. wrote the original manuscript; A.M. analyzed the data and supervised the work; V.S.V.P. provided instrumentation facility and edited the manuscript. All authors have read and agreed to the published version of the manuscript.
Funding
This research received no external funding.
Institutional Review Board Statement
Not applicable.
Informed Consent Statement
Not applicable.
Data Availability Statement
Data available on request due to restrictions e.g., privacy or ethical.
Acknowledgments
This project was supported by researchers supporting the project number (RSP-2020/283), King Saud University Riyadh, Saudi Arabia.
Conflicts of Interest
The authors declare no conflict of interest.
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Srihasam Saiganesh
1,
Thyagarajan Krishnan
2,*,
Golla Narasimha
3,
Hesham S. Almoallim
4,
Sulaiman Ali Alhari
5,
Lebaka Veeranjaneya Reddy
6,
Koduru Mallikarjuna
7,8,
Arifullah Mohammed
9,10,* and
Vattikuti S. V. Prabhakar
11,*
1Department of Physics, JNTU Ananthapuramu, Anantapur 515002, India
2Department of Physics, JNTU College of Engineering Pulivendula, Pradesh 516390, India
3Department of Virology, S. V. University, Tirupati 517502, India
4Department of Oral and Maxillofacial Surgery, College of Dentistry, King Saudi University, PO Box-60169, Riyadh-11545, Saudi Arabia
5Department of Botany and Microbiology, College of Science, King Saudi University, PO Box-60169, Riyadh-11545, Saudi Arabia
6Department of Microbiology, Yogi Vemana University, Kadapa, Andhra Pradesh 516005, India
7Department for Management of Science and Technology Development, Ton Duc Thang University, Ho Chi Minh City 758307, Vietnam
8Faculty of Applied Sciences, Ton Duc Thang University, Ho Chi Minh City 758307, Vietnam
9Faculty of Agro-Based Industry, Universiti Malaysia Kelantan, Jeli 17600, Malaysia
10Institute of Food Security and Sustainable Agriculture, Universiti Malaysia Kelantan, Jeli 17600, Malaysia
11School of Mechanical Engineering, Yeungnam University, 280 Daehak-ro, Gyeongsan-si, Gyeongsangbuk-do 38533, Korea
*Authors to whom correspondence should be addressed.
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Abstract
Over the past few years, the photogenic fabrication of metal oxide nanoparticles has attracted considerable attention, owing to the simple, eco-friendly, and non-toxic procedure. Herein, we fabricated NiO nanoparticles and altered their optical properties by doping with a rare earth element (lanthanum) using Sesbania grandiflora broth for antibacterial applications. The doping of lanthanum with NiO was systematically studied. The optical properties of the prepared nanomaterials were investigated through UV-Vis diffuse reflectance spectra (UV-DRS) analysis, and their structures were studied using X-ray diffraction analysis. The morphological features of the prepared nanomaterials were examined by scanning electron microscopy and transmission electron microscopy, their elemental structure was analyzed by energy-dispersive X-ray spectral analysis, and their oxidation states were analyzed by X-ray photoelectron spectroscopy. Furthermore, the antibacterial action of NiO and La-doped NiO nanoparticles was studied by the zone of inhibition method for Gram-negative and Gram-positive bacterial strains such as Escherichia coli and Bacillus sublitis. It was evident from the obtained results that the optimized compound NiOLa-04 performed better than the other prepared compounds. To the best of our knowledge, this is the first report on the phytosynthetic fabrication of rare-earth ion Lanthanum (La3+)-doped Nickel Oxide (NiO) nanoparticles and their anti-microbial studies.
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