 Open Access Article
 Open Access Article
Muhammad Ikram *ab, 
Yasir Shabirc, 
Ali Haider
*ab, 
Yasir Shabirc, 
Ali Haider *d, 
Iram Shahzadie, 
Muhammad Bilala, 
Anwar Ul-Hamid
*d, 
Iram Shahzadie, 
Muhammad Bilala, 
Anwar Ul-Hamid *f, 
Ahmed M. Foudag and 
Salamat Alih
*f, 
Ahmed M. Foudag and 
Salamat Alih
aSolar Cell Applications Research Lab, Department of Physics, Government College University Lahore, Lahore, 54000, Punjab, Pakistan. E-mail: dr.muhammadikram@gcu.edu.pk
bAdvance Nanomaterials Research Lab, Department of Physics, Government College University Lahore, Lahore, 54000, Punjab, Pakistan
cDepartment of Physics, Riphah Institute of Computing and Applied Sciences (RICAS), Riphah International University, 14 Ali Road, Lahore, Pakistan
dDepartment of Clinical Medicine, Faculty of Veterinary and Animal Sciences, Muhammad Nawaz Shareef, University of Agriculture, 66000, Multan, Punjab, Pakistan. E-mail: ali.haider@mnsuam.edu.pk
eSchool of Pharmacy, University of Management and Technology, Lahore, 54770, Pakistan
fCore Research Facilities, King Fahd University of Petroleum & Minerals, Dhahran, 31261, Saudi Arabia. E-mail: anwar@kfupm.edu.sa
gChemistry Department, Faculty of Science, King Khalid University, P. O. Box 9004, Abha, 61413, Saudi Arabia
hDepartment of Physics, The University of Lahore, 54000, Pakistan
First published on 26th September 2024
Developing multifunctional nanomaterials is crucial to rising global concerns over environmental contamination caused by dye effluents and antibiotic resistance. This work presents cesium (Cs)-doped Y2O3 nanostructures (NSs) as viable options for catalytic dye degradation and antibacterial action. This study prepared yttrium oxide (Y2O3) and various (2, 4, and 6 wt%) concentrations of Cs-doped Y2O3 NSs via co-precipitation technique. The pure and Cs-doped Y2O3 NSs were used to degrade methylene blue (MB) at different pH levels and assess the antibacterial properties against multidrug-resistant (MDR) Escherichia coli (E. coli). The X-ray diffraction spectra of the pure and Cs-doped Y2O3 revealed the presence of cubic and monoclinic structures. The UV-vis absorption spectra displayed distinct peaks at 274 nm and a reduction in band gap energy (from 4.94 eV to 4.41 eV) upon incorporation of Cs. Maximum degradation efficiency of up to 99% attributed to 6% Cs-doped Y2O3. The bactericidal activity against MDR E. coli exhibited 4.15 mm inhibition zones at higher concentrations of Cs-doped Y2O3. The bactericidal mechanism of Cs-Y2O3 NSs was further investigated by molecular docking studies for β-lactamase and DNA gyrase enzymes.
The composition and structure of nanomaterials significantly impact most of their applications.12–14 Rare earth elements have attracted much interest in pharmacology and medicine due to their antitumor, antibacterial, antiemetic, anticoagulant, and anticancer activities.15 Yttrium oxide (Y2O3), one of the 17 rare earth oxides, exists in different cubic, hexagonal, and monoclinic structural phases.16–18 Modified Y2O3 can be a reliable option for developing multifunctional nanomaterials. Various techniques can be used to synthesize Y2O3 nanoparticles. For homogeneity and size control, the co-precipitation approach is discovered as an effective synthesis method.19 For modification, the huge atom size of the cesium (Cs) as a doping element was anticipated to have considerable effects on adjusting the physical characteristics of materials.20 The present study investigates the potential of Cs-doped Y2O3 NSs as a feasible solution to these important research areas. The objective is to produce a multipurpose material that can degrade organic contaminants and fight pathogens that are resistant to antibiotics by fusing the catalytic qualities of Y2O3 with the distinctive characteristics of cesium. The significance of this work stems from its ability to give an extended and effective solution to two major global concerns.
Using a co-precipitation approach, this study synthesized Y2O3 and various concentrations (2, 4 and 6 wt%) of Cs-doped Y2O3. The catalytic degradation of methylene blue (MB) dye and antibacterial efficacy against MDR E. coli were investigated to evaluate their potential. Moreover, in silico investigations for β-lactamase and DNA gyrase enzymes were also carried out to understand the underlying mechanisms of antibacterial activity.
| % degradation = (C0 − Ct)/C0 × 100 | (1) | 
![[2 with combining macron]](https://www.rsc.org/images/entities/char_0032_0304.gif) ), 32.2° (310), 33.1° (11
), 32.2° (310), 33.1° (11![[2 with combining macron]](https://www.rsc.org/images/entities/char_0032_0304.gif) ), 34.6° (112), 37.1° (
), 34.6° (112), 37.1° (![[4 with combining macron]](https://www.rsc.org/images/entities/char_0034_0304.gif) 11), 42.6° (004), 54.7° (71
11), 42.6° (004), 54.7° (71![[2 with combining macron]](https://www.rsc.org/images/entities/char_0032_0304.gif) ) and 56.5° (711) were ascribed to monoclinic Y2O3 (m-Y2O3), (JCPDS: 00-044-0399/00-039-1063). The peaks appeared at 2θ = 36.0° (411), 40.0° (332), and 55.0° (026), referring to cubic phase Y2O3 (JCPDS: 01-074-1828). A distinct peak is observed at an angle of 29.73° (100) attributed to 2 wt% incorporation of Cs. Similarly, a peak is observed at an angle of 50.11° (106) assigned to 4 wt% concentration of Cs. Furthermore, when the doping concentration of Cs is enhanced to 6 wt%, multiple peaks are observed at angles of 29.27° (004), 39.6° (104), 44.6° (105), 50.1° (106), 53.7° (112), and 56.0° (113). These peaks correspond to the hexagonal cesium yttrium oxide phase match with the JCPDS: 01-077-1611. In the 6% Cs-doped Y2O3 the extra peaks appeared at 29.5° (014) and 48.0° (
) and 56.5° (711) were ascribed to monoclinic Y2O3 (m-Y2O3), (JCPDS: 00-044-0399/00-039-1063). The peaks appeared at 2θ = 36.0° (411), 40.0° (332), and 55.0° (026), referring to cubic phase Y2O3 (JCPDS: 01-074-1828). A distinct peak is observed at an angle of 29.73° (100) attributed to 2 wt% incorporation of Cs. Similarly, a peak is observed at an angle of 50.11° (106) assigned to 4 wt% concentration of Cs. Furthermore, when the doping concentration of Cs is enhanced to 6 wt%, multiple peaks are observed at angles of 29.27° (004), 39.6° (104), 44.6° (105), 50.1° (106), 53.7° (112), and 56.0° (113). These peaks correspond to the hexagonal cesium yttrium oxide phase match with the JCPDS: 01-077-1611. In the 6% Cs-doped Y2O3 the extra peaks appeared at 29.5° (014) and 48.0° (![[1 with combining macron]](https://www.rsc.org/images/entities/char_0031_0304.gif) 08) were matched with JCPDS No. 00-021-1447, revealing a monoclinic structure of yttrium hydroxide. The average crystallite size in the range of 45–60 nm was assessed using the Scherrer formula.33 The observed peak shifted towards lower 2θ values can be accredited to an increase in crystallite size as the dopant concentration increases and is also associated with the greater ionic radii (2.49 Å) of Cs.
08) were matched with JCPDS No. 00-021-1447, revealing a monoclinic structure of yttrium hydroxide. The average crystallite size in the range of 45–60 nm was assessed using the Scherrer formula.33 The observed peak shifted towards lower 2θ values can be accredited to an increase in crystallite size as the dopant concentration increases and is also associated with the greater ionic radii (2.49 Å) of Cs.
|  | ||
| Fig. 3 (a) XRD analysis (b) FTIR analysis and (c–f) SAED micrograph of Y2O3, Cs (2, 4 and 6 wt%) doped Y2O3 NSs. | ||
Fourier transform infrared spectroscopy (FTIR) analysis conducted in the frequency range of 450–4000 cm−1 to investigate the chemical composition and functional groups analysis of pristine and Cs-doped Y2O3 can be represented in Fig. 3(b). The bands appeared at 500 and 550 cm−1 attributed to the metal oxygen band, as previously reported.34 A Y-OH bond was attributed to the observed band at 950 cm−1. The nanostructure exhibits a distinctive asymmetric stretching of Y–O–Y attributed to the band observed at 1060 cm−1.35 The observed spectral bands at around 1500 cm−1 ascribed to asymmetric stretching of the C–O bond and can be attributed to the absorption of CO2 from the surrounding atmosphere. The spectral bands detected within the wavelength range of 3800–3350 cm−1 and at 1450 cm−1 are associated with OH stretching and bending vibration modes, respectively. The occurrence of this phenomenon can be accredited to the existence of hydroxyl groups and molecular water that are firmly adsorbed within the yttrium hydroxide crystal lattice.34 The peak at 650 cm−1 with high intensity is credited to the stretching vibration of Y–O bonds, as reported earlier.36
Selected area electron diffraction (SAED) analysis revealed the presence of distinct bright circular rings that indicate the polycrystalline nature of synthesized Y2O3 and Cs-Y2O3 (Fig. 3(c–f)). These concentric rings show that the NSs have a high degree of crystallinity that matches XRD results.
UV-visible spectroscopy was employed to examine the absorption characteristic of the produced NSs in the spectral range of 250–600 nm, as represented in Fig. 4(a). The absorption spectrum of Y2O3 exhibits a prominent peak at 274 nm. The addition of (2, 4 and 6 wt%) Cs led to a noticeable shift in absorption towards longer wavelengths (redshift), suggesting a reduction in the bandgap energy (Eg) that is associated with the enhancement in the crystallite size.37 The Eg was calculated using Tauc plot equation38 (Fig. 4(b)). The direct Eg of pure NSs was determined as 4.94 eV. The addition of Cs in Y2O3 resulted in additional energy levels. There are only minor changes observed in the Eg of 2 wt% Cs-doped NSs. For instance, at higher concentrations of Cs, the Eg was approximately 4.41 eV. The decrease in Eg observed in doped samples can be attributed to the increase in crystallite size. This phenomenon may be attributed to the diminished orientation realignment and low crystallinity of the resultant materials.39
|  | ||
| Fig. 4 (a) Absorption spectra, (b) band gap energy, and (c) emission spectra of Y2O3 and Cs (2, 4, and 6 wt%) doped Y2O3 NSs. | ||
Photoluminescence (PL) spectroscopy emission spectra have been used to examine the mechanism of recombination and separation of electron and hole pairs of synthesized NSs can be depicted in Fig. 4(c). The excited electrons in valence band migrate to the conduction band at a specific excitation wavelength and then recombine to produce emission.40 The Y2O3 NSs exhibit extensive emission peaks within the observable spectrum ranging from 260 to 290 nm. These emission peaks are mostly related to the presence of Y3+ ions observed at 274 nm. The decrease in peak intensity was attributed to the incorporation of Cs concentration, reflecting a greater potential for separating electron–hole pairs for photo-generated charge carriers. The increase in separation of photo-generated charge carriers exhibits maximum degradation of organic dye.
The chemical composition of pure and CS-Y2O3 NSs have been measured by energy-dispersive X-ray spectroscopy (EDS) analysis can be indicated in Fig. S1(a–d).† Prominent peaks corresponding to Y, O, and Cs were detected, providing conclusive evidence of Cs into Y2O3 NSs. The presence of Au peaks may be accredited to the deposition of Au coating to reduce the charging effects.41 The EDS mapping determines the elements involved in pure and CS-Y2O3 NSs with various color combinations (Fig. S1(e–h)†). The higher doped concentrations exhibited the dispersion of three components, Y, O, and Cs, confirming the synthesis of pristine and doped NSs.
Field emission scanning electron microscopy (FESEM) examines the surface morphology of synthesized Y2O3 and CS-Y2O3 NSs can be revealed in Fig. 5(a–d). Y2O3 indicates that particles are agglomerated particles and huge chunk was found can be seen in Fig. 5(a). The presence of a significant concentration of yttrium ions with Cs at varying percentages concentration of CS (2, 4, and 6 wt%) caused the initial homogenous nucleation can be disrupted. The active sites on the surface of Y2O3 aggregates would progressively increase in a specific direction as the reaction proceeds, and Y2O3 monomer concentration diminishes.42 As the concentration of Cs increases, the surface of Y2O3 is distorted, and particles appear on the surface of cluster. The nanorods-like morphology with a rough surface appeared upon insertion of 6 wt% Cs.
The pictorial representation of transmission electron microscopy (TEM) was used to describe the internal structural morphology of Y2O3 and (2, 4, and 6 wt%) Cs-doped Y2O3 can be depicted in Fig. 6. Y2O3 revealed surface of atoms forming agglomerated nanocluster-like morphology. Incorporation of Cs, the morphology undergoes a transition to a dense nanocluster morphology. 4 wt% doped exhibit Y2O3, the shape of generated nanocluster transforms a rod-like morphology. As the percentage concentration of Cs increases the agglomerated nanoparticles (NPs), a nanorod-like (NRs) morphology of Cs appeared on the surface of the nanocluster.
Interlayer d-spacing of pure and (2, 4, 6 wt%) Cs-doped Y2O3 were measured as 0.270, 0.264, 0.267, and 0.298 nm, using high-resolution transmission electron microscopy (HRTEM) micrographs respectively indicated in Fig. 7. The measured interlayer d-spacing exhibit strong concurrence with the XRD results.
The catalytic activity of synthesized NSs was evaluated with the assistance of a reducing agent to degrade MB. The % age degradation was measured as 78.25–81.32% at pH ∼ 7 for a neutral medium, 76.96–79.17% for an acidic medium at pH ∼ 4, and 95.94–98.58% at pH ∼ 12 in a basic medium can be depicted in Fig. 8(a–c). As illustrated in Fig. 8, dye degradation without a catalyst attained the maximum of 4.3%, 3.91%, and 2.52% in 8 min in acidic, basic, and neutral environments, respectively. The pH is significantly important in determining the properties of dyes and mechanisms involve hydroxyl radicals and direct oxidation by H+.43 The pH value significantly affects the surface area and surface charge of the catalyst.44 MB is a cationic dye that will adsorb onto a catalyst with a strong negative charge in a basic medium.45 This leads to a higher degradation of organic dye attributed to a positive charge that enhanced electrostatic attraction between the catalyst surface and dye in the basic medium.
|  | ||
| Fig. 8 Catalytic activity of Y2O3 and Cs-Y2O3 (2, 4, and 6 wt%) in (a) acidic, (b) basic and (c) neutral media. | ||
An acidic medium with a lower pH value leads to a positive charge on the catalyst surface and MB is also a cationic dye in consequence, there is no redox reaction taking place. The degradation of dye on the nanocatalyst surface decreases.46 Using a doped nanocatalyst increased the percentage degradation in acidic and basic mediums. At higher concentrations of Cs, the catalytic activity for degradation of MB was increased. The dye degradation is affected by the crystallinity, shape, and surface area of synthesized NSs.47,48
The fundamental reaction steps comprise the catalytic reaction for the degradation of MB. The rate of reaction between MB and NaBH4 was slow. The synthesized catalyst enhanced the reaction that acts as a relay between reactants. The catalyst helps speed up the electron transfer from BH4− ions to MB, leading to the formation of intermediate radicals, and it is most likely the complex mechanism that mediates the degradation of MB with NaBH4. The redox reaction takes place between the reactants.49 The degradation of MB in the existence of NaBH4, and catalyst facilitates the transfer of electrons from the BH4− ions to the MB ions during dye degradation. The surface area and the number of active sites also play an effective role in degradation of dye molecules.50,51 High catalytic efficiency is typically associated with a large surface area of catalyst. Further research is required to fully understand the degradation pathway, particularly the involvement of free radicals in the degradation process and subsequent intermediates.52–55
The in vitro antibacterial activity of Y2O3 and Cs (2, 4, and 6 wt%)-doped Y2O3 was assessed using an agar-based diffusion approach to measure inhibitory zones against Gram −ve bacteria, MDR E. coli. Many antibiotic studies use E. coli as a model organism since it is a relatively well-understood bacterium.56 The inhibition zones were assessed between 1.65–3.15 mm and 2.50–4.15 mm, for low and high concentrations respectively. Additionally, ciprofloxacin exhibited an inhibition zone of 5.0 mm that acts as an efficient drug for microbial killing and DI water shows 0 mm can be depicted in Table 1. Moreover, Cs doped Y2O3 NSs effectively eliminated MDR E. coli bacteria. The Cs-doped Y2O3 exhibits enhanced bactericidal activity against MDR E. coli, compared to the findings obtained with pure.
| Samples | Inhibition zone (mm) | |
|---|---|---|
| 0.5 mg/50 μL | 1.0 mg/50 μL | |
| Y2O3 | 1.65 | 2.50 | 
| 2% Cs/Y2O3 | 2.25 | 3.05 | 
| 4% Cs/Y2O3 | 2.90 | 3.45 | 
| 6% Cs/Y2O3 | 3.15 | 4.15 | 
| Ciprofloxacin | 5.0 | 5.0 | 
| DIW | 0 | 0 | 
Efficacy (%) was determined by dividing the inhibition zone of the synthesized sample by the inhibition zone of ciprofloxacin, represented in Fig. 9. The measured efficiency for low concentration is 33%, 45%, 58%, and 63% and for high concentration 50%, 61%, 69%, and 83% respectively pure and doped NSs.
|  | ||
| Fig. 9 Graphical representations of bactericidal activity of MDR E. coli (a) inhibition zones measurements and (b) % age efficacy at low concentrations and high concentrations. | ||
Through interactions with the bacteria cell membrane, Y2O3 NSs produce toxicity and lead to bacterial cell death. Due to the robust electrostatic forces, Y2O3 nanoparticles have a notable affinity for the bacterial cell membrane, enabling them to efficiently constrain the growth of both Gram +ve and Gram −ve bacteria. Based on earlier reports on the formation pathways of Y2O3 nanoparticles, it has been observed that yttrium ions can permeate the cell wall of bacteria. This penetration leads to the inhibition of bacterial growth by down-regulating enzyme activity, ultimately causing the death of bacterial cells.35,57–59 The schematic diagram of doped nanocatalyst used during the antibacterial process (Fig. 10).
Recent studies have shown the importance of cell wall production (peptidoglycan synthesis) and the pathway different NSs use for nucleic acid biosynthesis for antibacterial activity. However, the exact mechanism still needs to be clarified. Fig. 11(a) illustrates the binding affinity of Cs-Y2O3 NSs within the active site of DNA gyrase in MDR E. coli. The Cs-Y2O3 NSs exhibited favorable binding score of 3.02, indicating the presence of hydrogen bonding with crucial amino acid residues Thr165, Gly75, Arg76, Pro79, and Gly77 (Fig. 11(b)). Additionally, the propensity of Cs-Y2O3 NSs to interact with beta-lactamase E. coli were examined (Fig. 11(c)) with binding scores of 2.01 for the proposed molecule in well-docked conformations. The interaction of Cs-Y2O3 NSs between Arg232 and Lys183 was observed (Fig. 11(d)).
Cs-Y2O3 NSs were shown to have binding affinity for β-lactamase and DNA gyrase, suggesting them effective inhibitors of these enzymes.
| Footnote | 
| † Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4ra05620e | 
| This journal is © The Royal Society of Chemistry 2024 |