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Full Length Article
07 2024
:36;
103222
doi:
10.1016/j.jksus.2024.103222

Hierarchically synthesis of M@CeO2 (M = Ba, Er) nanoparticles for Antibacterial efficacy

Department of Chemistry, Vivekananda College of Arts and Sciences for Women (Autonomous) Elayampalayam, 637 205 Tamilnadu, India
Department of Chemistry , K.S.Rangasamy College of Arts and Science (Autonomous) Tiruchengode, 637211, Tamilnadu, India
Department of Chemistry, College of Science, King Saud University, P.O. Box 2455, Riyadh 11451, Saudi Arabia
Department of Allied Health Sciences, Faculty of Science, University Tunku Abdul Rahman, Jalan University, Bandar Barat, Kampar 31900, Malaysia
Biomedical Research Unit and Lab Animal Research Centre, Saveetha Dental College, Saveetha Institute of Medical and Technical Sciences, Saveetha University, Chennai 602 105, India
Faculty of Health and Life Sciences, INTI International University, Nilai 71800 Malaysia
Faculty of Bioeconomics and Health Sciences, University Geomatika Malaysia, Kuala Lumpur 54200, Malaysia
School of Nursing, Shinawatra University, 99, Moo 10, Bangtoey, Samkhok, Pathum Thani 12160, Thailand

⁎Corresponding authors at: Department of Chemistry, Vivekananda College of Arts and Sciences for Women (Autonomous) Elayampalayam, 637 205 Tamilnadu, India (K. Loganathan). Department of Allied Health Sciences, Faculty of Science, University Tunku Abdul Rahman, Jalan University, Bandar Barat, Kampar 31900, Malaysia (S. Djearamane). drkloganathan@vicas.org (K. Loganathan), sinouvassane@utar.edu.my (Sinouvassane Djearamane)

Disclaimer:
This article was originally published by Elsevier and was migrated to Scientific Scholar after the change of Publisher.

Abstract

Cerium oxide fine particles injected with metallic nanoparticles were produced using the co-precipitation method and characterized using various techniques such as XRD, SEM, FTIR, UV–Vis, and PL. Both injected and non-doped ceria nanoparticles exhibited a crystallographic structure similar to calcium fluoride. The nanoparticles ranged in size from 25 to 74 nm and had an inconsistent spherical shape. EDX analysis confirmed the presence of Erbium (Er) and Barium (Ba) in the ceria nanocrystal lattices. UV–Vis experiments showed that the optical band gap efficiency of purified CeO2 NPs was 3.1 eV, while doped CeO2 NPs had an energy level of 2.9 eV. The nanoparticles exhibited a sharp emission peak at approximately 347 nm. The synthesized CeO2 NPs showed antibacterial activity against Gram-positive and Gram-negative bacteria, including Bacillus subtilis, Staphylococcus aureus, Escherichia coli and Pseudomonas aeruginosa. Overall, the results demonstrate that the doping of ceria nanoparticles with metallic nanoparticles can significantly enhance their antibacterial properties. This research paves the way for the development of novel antibacterial agents with potential applications in various fields such as medicine, food packaging, and water treatment.

Keywords

CeO2 NPs
Ba / Er @ CeO2 NPs
Co-precipitation method
SEM/EDX
1

1 Introduction

A large number of bacteria are present in our daily living environment, and the uncontrolled growth and spread of pathogenic bacteria can cause several human diseases and wound infections (Kumar et al., 2014). The discovery of penicillin has enabled humans to defend themselves against bacteria to some extent, and the extensive application of antibiotics has made a significant contribution to society. However, due to the heavy use of antibiotics, a high number of resistant bacteria strains have developed (Kumar et al., 2021), and the emergence of such drug-resistant bacteria has left traditional antibiotics inadequate in destroying them; hence, developing new antimicrobial agents to treat bacteria is urgently required. A promising alternative to combat bacterial resistance comes from metal oxide nanoparticles (NPs). Metal oxide NPs have high chemical and biological activity due to different factors, mainly their small size and their high surface-to-volume ratio. As a result, they have been widely used in biology and medicine.

Genuinely, Cerium oxide (CeO2) nanoparticles have an emerged as an exciting emerging substance with potential applications in therapeutics and electroluminescent technologies (Pelletier et al., 2010; Alpaslan et al., 2017). Among the many applications of nanostructured CeO2-based composites in ecological and energy technology includes outgas cleansing, fuel cells made of solid oxide, oxygen gases detectors, electrochromic components, ultraviolet (UV) protective coatings, and electrochromic devices (Farias et al., 2018). According to oxygen shortages in the crystal structure of either pristine or loaded ceria are associated with the distinctive features of cerium dioxide. Modern study has concentrated on transistor photo catalysis, with TiO2 being a popular photographic catalyst for waste from agriculture and industries due to its good characteristics (Malleshappa et al., 2015). According to, the band gap interaction between visible light, non-metallic the addition of doping and the photocatalyst's catalytic function and the movement of photo-induced pairs of electron-holes from the catalyst's interior to its exterior being narrowed (Cuahtecontzi-Delint et al., 2013). Therefore, doping of cerium oxide nanostructures improves their chemical and thermal stability, high ionic conductivity, and better UV absorption. The numerous reports of doping of various metals such as Co, Mg, Cd, Fe, Ni, Ag, and Zn with CeO2 nanoparticles have been presented that are associated with improving the properties of new nanostructures. The erbium particles employed in optoelectronic cores for converting the energy of captured infrared rays into visible wavelengths are hosted inside the low-phonon material ceria (Khadar et al., (2019,)).

With the addition of alkaline metals onto the surfaces of CeO2 matrices, which can change the optical and biocidal properties of nanomaterials, due to bandgap illumination, the electrons (e) of NMs are excited via the bandgap to the conduction band, producing holes (h+) in the valence band. As a result, the conduction band electrons and the valence band holes produce highly active reducing and oxidizing agents. These oxidizing agents (OH and (O2) are responsible for the antibacterial activity of CeO2 NPs, which could be altered by doping the CeO2 NPs with alkali metal ions (AMIs) because they (Ba ions) act as electron traps that can inhibit the rate of (e-/h+) pair recombination by augmenting the bandgap energy (Nithya and Sundrarajan, 2020). This stimulates the formation of ROS and increases the antibacterial efficacy. Therefore, the main objective of this research is to develop and compare the results of pristine and injected CeO2 nanoparticles through precipitation approach employing polyethylene glycol (PEG) as a surfactant.

  • Experimental

    • Materials

Cerium nitrate hexahydrate (Ce (NO3)3·6H2O > 99.8 %), Erbium nitrate hexahydrate (ErH12N3O15 > 99.9 %) and Barium nitrate pentahydrate (BaH2N2O5 > 98.9 %) were procured from sigma Aldrich, India. And bacterial strains were obtained from the microbial collection of the microbiology laboratory of Bharathidasan University, Tamilnadu, India. All the chemicals and reagents were used as AR grade. The whole experiment used as deionized water and without further sanitation.

1.1

1.1 Hierarchically fabrication of pristine MCeO2 (M = Ba, Er) nanoparticles

Following dissolving 0.095 mg of cerium nitrate hexahydrate, 0.005 mg of Erbium nitrate hexahydrate, along with 0.8 mg of sodium hydroxide in their respective choices, the first step was to evenly combine the two solutions. The polyethylene glycol (PEG), which can function as a surfactant, is injected into the resultant combination mentioned earlier and subsequently lowered by a NaOH solution, resulting in a transparent yellow precipitate. After mixing the solution including the light-yellow precipitate for thirty minutes at the surrounding temperature, it was heated to 60 °C and fed for a total of four hours. After one day at a reasonable humidity, the combination of reaction fluid was refluxed to provide a clear solution. After many washing with deionized water over time, the resultant combination was finally diluted with alcohol. The resulting precipitates were dried at 120 °C as a consequence. Er-doped nanoparticles of CeO2 were synthesized and heated at 400 °C for 4 h since the power obtained from warmth can enhance oscillations and transfer of lattice-like elements during crystallization. The exact test methods were used to produce Barium-doped CeO2 using barium nitrate hexahydrate (Khadar et al., 2019; Masui et al., 1997).

1.2

1.2 Antibacterial activity

Bacterial cultures containing Bacillus subtilis, Staphylococcus aureus, E. coli, and P. aeruginosa, among others, were acquired from the Eumic Analytic Lab and Research Institute in Tiruchirappalli. Bacterial strains were cultivated on nutrient agar slants (Hi medium) at 4 °C. Bacterial cultures were subculture in a liquid medium (nutrient broth) at 37 degrees Celsius for 8 h before being tested for 105–106 CFU/Ml. All of these suspensions were made shortly before the examination was performed. Nutrient agar medium is one of the most used media for a variety of regular bacteriological applications. After combining all of the components with the filtered water, it is heated to completely disintegrate the medium and then autoclaved at 15 psi pressure (121 °C) for 15 min. The nutritional broth was made using the same ingredients except agar. The nutrient broth was made, and identified bacterial colonies were added to the broth and cultivated for antimicrobial properties. The nutritional agar solution was produced and sterilized by steam sterilization at 121 °C and 15 lb of pressure for fifteen minutes before aseptically pouring it into sterile petri plates and allowing it to harden. The bacterial broth culture was swabbed on each petri plate with clean buds. The wells were then dug by a well cutter. Pure and doped CeO2 has been added to every sample aseptically. This method was repeated for each petri-plate which was subsequently incubated at 37 °C for 24 h. Following the incubation process the glass plates were examined for the zone of inhibition.

1.3

1.3 Analytical characterization

The granule specimens have been examined for phase makeup and quantity employing an X-ray diffractometer (Bruker D8 Advance) with CuKα radiation and a Bruker Lynx Eye detector. PANalytical, Netherlands, was also employed for the exact same objective, utilizing a 3 kW X-ray tube with a copper objective as the radiation source and real-time multiple-strip solid-state detectors equipped with graphite crystals for K beta screening. X-ray spectra have been obtained from 5˚ to 50˚. The results of the XRD were processed to identify the crystallized components. The surface morphology and crystallographic orientation of the samples were investigated using scanning electron microscopy and an energy-dispersive X-ray spectrometer. SEM photos were captured with the model JEOL-JSM-35 LF, which has a voltage range of 5–35 kilo Volts of KV and a resolution of 5000 X. and the size of Nanoparticles can be accurately measured from SEM images using image J analysis software with proper calibration and measurement techniques. Fourier transform infrared spectroscopy (FTIR, Bruker Optic GmbH, Tensor 27, Germany) was used to identify the functional groups in the produced samples. 1 % of the powder was combined with 99 % KBr and formed into pellets with a diameter of 3 mm at 5 MPa/torr, which was then examined in the 400–4000 cm−1 area. A UV–visible photometer (Shimadzu, Model UV-1800) was used to measure the optical characteristics of nanoparticles of metal oxide in the 200–850 nm spectrum, with a resolution of 1 nm. Photo luminescence has been determined utilizing a luminescence spectrophotometer (Perkin Elmer, Model: LS-5513, USA) using a xenon lamp as the excitation source at ambient temperature.

2

2 Results and discussion

2.1

2.1 XRD finding

The crystalline state of produced pure CeO2 Er and Ba-doped CeO2 nanoparticles was observed using XRD analysis. Fig. 1 (a-c) depicts the XRD criteria for the produced pure and doped CeO2. The ceria nanoparticles are a common calcium fluoride crystal form with the space group Fm3m (Abbas et al., 2015; Azad et al., 2005). The XRD pattern shows well-set peaks for (1 1 1), (2 0 0), (2 2 0), (3 1 1), (2 2 2), (4 0 0), (3 1 1), and (4 2 0) at 2θ values = 28.68°, 33.23°, 47.45°, 56.45°, 59.39°, 69.49°, 76.77°, and 79.02°, indicating a cubic fluorite structure for CeO2 (Fig. 1 a-c). This is also supported by JCPDS data (card no. 00–34-0394) (Khulbe et al., 2020; Pinna et al., 2012). Furthermore, no XRD patterns of any other group phase were discovered as impurities, showing that the substituted along with untreated particles are very pure and crystalline (Fig. 1 a-c). In comparison to the pure CeO2 sample, the Barium and Erbium doped CeO2 nanoparticles shows no significant change in diffraction peak values. The change reflects the amount of distortion caused by the substitution of Ba and Er ions with Ce ions in each compound owing to the ionic radius of the specific metal ions, which occurs at boiling heat. The mean size of ordered pure CeO2 nanoparticles is given using Debye-Scherrer's formula, as shown following (Pinna et al., 2020).

(1)
D = 0.9 λ / β c o s θ In this equation, D- represents Crystallite size, λ-is the wavelength of the radiation (1.5406 Å for CuKα), k is a constant (0.94), β- is Full Width Half Maximum (FWHM), and θ is the peak location. It was discovered that the average crystallite diameter of pure CeO2 nanoparticles is 25 nm. The average crystallite size increases in Ba and Er-CeO2 nanoparticles reached 74 nm and 40 nm, correspondingly. Increase in particle size observed may be due to the increase in calcination humidity. This increase in humidity could potentially lead to a reduction in particle size during the calcination process (Pop et al., 2020).
XRD pattern of (a) Pristine CeO2 (b) Er doped CeO2 (c) Ba doped CeO2 NPs.
Fig. 1
XRD pattern of (a) Pristine CeO2 (b) Er doped CeO2 (c) Ba doped CeO2 NPs.

2.2

2.2 SEM morphological analyses

Fig. 2 illustration (a–c) shows micrographs obtained using SEM of pure CeO2, Ba, and Er- CeO2 nanoparticles. The size of nanoparticles was calculated using image J software. The annealed nanoparticles between 350 and 400 °C were homogeneous in size, ranging from 20 to 30 nm for CeO2 and 35 to 75 nm for Ba and Er- CeO2. The typical widths of cubic particles for pure CeO2, Ba, and Er doped CeO2 particles are 26, 75, and 41 nm, respectively. Interestingly, the high-magnification SEM micrographs (Fig. 2(b)) have an irregular spherical form consistent with the literature, however, the corresponding Fig. 2(c) shows a nanowire-like structure instead of a spherical form. The reaction circumstances determine the difference between the two dopant topologies. According to this viewpoint, nanoparticles may exhibit mild aggregation due to inadequate annealing temperature and a lack of sonication. The average particle sizes of clean and modified nanoparticles match those calculated from XRD measurements (Mahalakshmi et al., 2024).

SEM photograph of (a) Pristine CeO2 (b) Er doped CeO2 (c) Ba doped CeO2 NPs.
Fig. 2
SEM photograph of (a) Pristine CeO2 (b) Er doped CeO2 (c) Ba doped CeO2 NPs.

2.3

2.3 EDX studies

The presence of doped rare earth metals on the ceria crystal surface was confirmed by its atomic weight percentage, which was determined utilizing EDAX. Fig. 3 (a-c) shows the EDAX spectra of pure CeO2 and CeO2 nanoparticles loaded with Er or Ba. Percentage of composition elements represents in Table 1.

EDX profile of (a) Pristine CeO2 (b) Er doped CeO2 (c) Ba doped CeO2 NPs.
Fig. 3
EDX profile of (a) Pristine CeO2 (b) Er doped CeO2 (c) Ba doped CeO2 NPs.
Table 1 Percentage of composition elements presents in as-fabricated pristine CeO2 and Er and Ba doped CeO2 NPs.

S.NO

MATERIAL
(%) Composition of Elements
Ce O Er Ba

1

Pristine CeO2

79.45 %

20.55 %



2

Ba doped CeO2

75.40 %,

3.92 %,


20.68 %,

3

Er doped CeO2

70.73 %,

4.15 %,

25.12 %,

2.4

2.4 FT-IR findings

The IR spectra of pure CeO2, Ba, and Er-doped CeO2 nanoparticles are given in Fig. 4 (a–c). For Er and Ba-doped CeO2, the bands at 3614 and 3464 cm−1 corresponds to the –OH groups, whereas the highest frequencies at 1621 and 1617 cm−1 correspond to the H-O–H twisting resonance of weakly charged or absorption water. The peak at 1339 cm−1 and 1335 cm−1 is due to the vibrational form of nitro compounds. The asymmetric stretching vibrations of COO were detected at 1547 cm−1 and 1540 cm−1. The distinctive metallic oxide movement, Er-O-Er and Ba-O-Ba, might be responsible for both of the major peaks at 479 cm−1 and 968 cm−1 for Er- CeO2and peaks at 457 cm−1 and 935 cm−1 for Ba- CeO2 in the IR spectra (Badi’ah et al., 2019; Parimi et al., 2019).

FT IR spectrum of (a) Pristine CeO2 (b) Er doped CeO2 (c) Ba doped CeO2 NPs.
Fig. 4
FT IR spectrum of (a) Pristine CeO2 (b) Er doped CeO2 (c) Ba doped CeO2 NPs.

2.5

2.5 Uv–visible spectroscopic investigations

Fig. 5 (a–c) depicts the UV–visible absorption spectrum of pure CeO2, Er, and Ba-doped CeO2 nanoparticles calcined at 400 °C. The stimulation maximum for pure nanoparticles of CeO2 was approximately 314 nm, whereas Er and Ba-doped CeO2 nanoparticles had wavelengths of excitation in the 314 & 312 nm spectrum ranges, as illustrated in Fig. 5 (b-c). The absorption spectrum of Er and Ba-doped CeO2 nanoparticles shifted to the longer frequency side when contrasted with pure CeO2 particles. This means that the band gap of CeO2 nanoparticles reduces when Er and Ba bonds develop with oxide at CeO2 grid sites. The optical band gap energy of Er and Ba-doped CeO2 nanoparticles is computed using the usual Tauc relationship (Nurhasanah et al., 2018; Habib et al., 2018).

(2)
α h v 1 / n = A ( h ν - E g ) Where, A − is a stable, n varies with the change, and Eg − represents the gap in the optical band. The value of n = 1/2, 3/2, 2, or 3 (order) varies according to the kind of electrical transfer. The sixth illustration (a-c) depicts a plot of (αhυ)2 vs photon energy (hυ) for Er and Ba-doped CeO2 nanoparticles after boiling at 400 degrees Celsius, taking into account the explicit group transitions. Extrapolating the linear area of these figures to (αhυ)2 = 0 yields the corresponding photon energy. The optical band gap energy of pure CeO2 nanoparticles is 3.1 eV, while Er and Ba-doped CeO2 nanoparticles have 2.8 eV. When matching the Er and Ba treated eV findings to CeO2 nanoparticles, the abrupt decrease in the band gap or red shift may be explained by the bottom of the Burstein-Moss (BM) effect, although the Fermi level changes occurred extremely close to the conduction band owing to the rise in transport density. The small transition of energy is forbidden and the frequency value gap narrows due to the amalgamation of Er and Ba ions in the CeO2 crystal lattice. No additional broadband emission is seen due to the reformation transition from the 4f band of Ce4+ ions to the valence band or the 5d-4f transition of Ce3+ ions (Sharma et al., 2020; Gopinath et al., 2015).
UV–Visible optical spectrum (a) Pristine CeO2 (b) Er doped CeO2 (c) Ba doped CeO2 NPs and (inset) band gap of Pristine CeO2, Ba and Er doped CeO2 NPs.
Fig. 5
UV–Visible optical spectrum (a) Pristine CeO2 (b) Er doped CeO2 (c) Ba doped CeO2 NPs and (inset) band gap of Pristine CeO2, Ba and Er doped CeO2 NPs.

2.6

2.6 Photoluminescence research

Fig. 6 (a-c) Photoluminescence spectrum shows the emission spectra of pure CeO2 nanoparticles and Ba, Er-doped CeO2 nanoparticles, with an excitation wavelength of 312 & 314  nm compared to the absorption spectra data. The pure CeO2 nanoparticles display a significant emission spike at 348 nm; it is attributed to the passage of protons through the confined Ce4f state to the O2p of the valence band. Furthermore, a peak of radiation seen at 396 nm was caused by defective conditions that existed broadly between Ce4f states and the O2p of the valence band. Furthermore, the emission of CeO2:Er nanoparticles progressively reduced by concerning 399 nm as well as continued to a maximum of 494 nm. The localized Ce4f state to O2p of the valence band in CeO2:Er nanoparticles is associated with emission, which gradually reduces in the CeO2 crystal structure owing to Er ion doping. Furthermore, the emission band was gradually enlarged from 427 nm to 453 nm, and it was prolonged up to 471 nm for CeO2 and Ba nanoparticles. At the same time, the emission nature was red-shifted due to lower defect levels generated by Er and Ba ions. As a result, the intensity of emission of the CeO2 in the surroundings gradually decreased, owing to the formation of more oxygen defects or increases in surface defects, as well as the restraint of electron transfer from Ce4f to O2p levels as the content of doping increased (Mohan et al., 2021; Deepa et al., 2022).

Photoluminescence spectrum (a) Pristine CeO2 (b) Er doped CeO2 (c) Ba doped CeO2 NPs.
Fig. 6
Photoluminescence spectrum (a) Pristine CeO2 (b) Er doped CeO2 (c) Ba doped CeO2 NPs.

2.7

2.7 Antibacterial activity

The antibacterial activity of pure CeO2 and doped nanoparticles containing CeO2 was tested against the Gram-negative microbes E. coli and P. aeruginosa, in addition to the Gram-positive bacteria B. subtilis and S. aureus. Table 2 compares the antibacterial activity of pure CeO2 and doped nanoparticles of CeO2 against this bacterium. The aforementioned research shows that CeO2 and doped CeO2 nanoparticles are efficient in inhibiting a certain variety of bacterial growth. Fig. 8 shows the antibacterial activity of CeO2 and doped CeO2 nanoparticles against E. coli, P. aeruginosa, B. subtilis, and S. aureus using ZOI. The zone of inhibition (ZOI) of around 18 and 14 mm for CeO2, 20 mm and 16 mm for Ba-CeO2, and 16 and 12 mm for Er-CeO2 were observed for the Gram-positive bacteria strain B. subtilis and S. aureus (American Type Culture Collection 25923), and Fig. 7 display the determined ZOI for the Gram-negative bacteria strain E. coli and P. aeruginosa (American Type Culture Collection 25922) were 10 mm and 12 mm for CeO2, 12 mm and 15 mm for Ba- CeO2, and 18 and 15 mm for Er. Given these findings, it can be inferred that the produced pure CeO2 and doped CeO2 nanoparticles had a significant antibacterial impact on both Grade categories of bacteria. Pure CeO2 and doped CeO2 nanoparticles have better antibacterial action against Gram-positive bacteria (especially B. subtilis) than Gram-negative microbes, Er- CeO2 in the case of E-Coli. The variation in activities among these two species of bacteria might be linked to variances in cell membrane structure and composition (Agarwal et al., 2018; Cedervall et al., 2007). The CeO2 nanoparticles were shown to have antibacterial action because they can produce reactive oxygen species that can damage cells of bacteria. In this regard, several processes have been proposed to explain metal oxides' antibacterial properties. Bacterial susceptibility to O- CeO2 nanoparticles varies depending on particle size, synthesis temperature, bacterial cell wall structure, and degree of interaction with nanoparticle-containing organisms. Furthermore, the increased susceptibility of the two types of bacteria to CeO2 nanoparticles has been linked to the higher number of nitro and carboxyl groups on their cell walls, which increases the affinity of Ce ions for these groups. Smaller nanoparticle sizes and CeO2 nanoparticles generated at lower temperatures showed superior antibacterial activities in our present study. In this investigation, Gram-positive B. subtilis showed a greater inhibition zone than Gram-negative isolates used in the bacterial sensitivity test ( Sudhakaran et al., 2023).

Table 2 Zone of inhibition of pure and doped CeO2 nanoparticles against bacterial strains tested.

Organisms
100 µL DMSO Extract added and zone of inhibition (mm)
Bacillus subtilis Staphylococcus aureus E. Coli Pseudomonas aeruginosa
CeO2 18 14 10 12
Ba-CeO2 20 16 12 15
Er-CeO2 16 12 18 15
DMSO
Tetracycline 25 15 20 25
Bactericidal properties of pristine CeO2 NPs and Ba doped CeO2 NPs by co-precipitation approach.
Fig. 7
Bactericidal properties of pristine CeO2 NPs and Ba doped CeO2 NPs by co-precipitation approach.
Bactericidal properties of pristine CeO2 NPs and Er doped CeO2 NPs by Co-precipitation approach.
Fig. 8
Bactericidal properties of pristine CeO2 NPs and Er doped CeO2 NPs by Co-precipitation approach.

2.7.1

2.7.1 Bactericidal mechanism

It is possible that pure CeO2, Er and Ba doped CeO2 NPs could play a role in the redox transformation of Ce ions once they reach the cell walls of bacteria. Depending on the conditions within the cell, Ce4+ atoms may reduce to Ce3+ or inversely. For most cases, what keeps the Ce3+ to Ce4+ ratio constant is CeO2 (IV) + e− → CeO2(III) (Azzam and Zaki, 2016). The process that leads to enhanced antibacterial effectiveness is demonstrated in Fig. 9. Certain oxidizing agents, such as free radicals (OH*, H2O2, and O2*), possess the ability to cross the barrier formed by bacteria and cause damage by interfering with its permeability. The conversion of Ce4+ to Ce3+ also increases reactive oxygen species (ROS) generation. Both stresses caused by oxidative stress as well as the oxidation of lipids contribute to ROS-induced microbial cell extinction. Strong reactive oxygen species (ROS) have the potential to harm several bacterial ingredients, such as amino acids, mitochondrion and DNA. Because of this, the bacterial cell becomes damaged, and the microbes eventually die (Chatterjee et al., 2011; Pitchumani Krishnaveni and Annadurai, 2019; Pozharitskaya et al., 2020).

Bactericidal mechanism of pure CeO2, Er and Ba doped CeO2 NPs.
Fig. 9
Bactericidal mechanism of pure CeO2, Er and Ba doped CeO2 NPs.

3

3 Conclusion

The present study successfully developed small fragments composed of cerium oxide and cerium dioxide injected with doped elements Er and Ba using an affordable precipitation method. X-ray diffraction analysis revealed a cubic fluorite layout for the nanocrystals, while SEM images showed irregularly shaped nanoparticles ranging from 20 to 30 nm. Infrared spectra indicated the presence of Er and Ba oxides or hydroxide compounds in the particles, with optical band gap energies of 3.2 eV in pure CeO2 and 2.9 eV in doped CeO2 NPs. The addition of Er and Ba ions resulted in a redshift in frequency gap, with a strong emission peak at 348 nm in pure CeO2 nanoparticles. Additionally, the antimicrobial tolerance experiment showed a larger inhibiting area for the Gram-positive B. subtilis strain compared to other Gram-negative isolates. Overall, these findings demonstrate the potential applications of these doped nanoparticles in various fields.

CRediT authorship contribution statement

K. Loganathan: Conceptualization, Formal analysis, Resources, Software. R.P. Suresh Jeyakumar: Conceptualization, Data curation, Formal analysis. Natarajan Arumugam: Conceptualization, Data curation, Project administration, Software, Supervision, Validation, Writing – review & editing. Sinouvassane Djearamane: Resources, Supervision, Validation, Writing – review & editing. Ling Shing Wong: Conceptualization, Supervision, Validation, Visualization. Saminathan Kayarohanam: Data curation, Funding acquisition, Project administration, Software, Validation, Writing – review & editing.

Acknowledgement

The project was funded by Researchers Supporting Project number (RSP2024R143), King Saud University, Riyadh, Saudi Arabia. In addition to one of the authors Dr. K. Loganathan is thankful to the DST-FIST, New Delhi (SR/FST/COLLEGE/2022/1290) and the Principal of  Vivekanandha College of Arts and Sciences for Women (Autonomous) for providing necessary facilities.

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