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Observation of excellent photocatalytic and antibacterial activity of Ag doped ZnO nanoparticles

Vaishali Amrutea, Monikaa, K. K. Supinbc, M. Vasundhara*bc and Anupama Chanda*a
aDepartment of Physics, Dr. Harisingh Gour Vishwavidyalaya (A Central University), Sagar, M.P. 470003, India. E-mail: achanda@dhsgsu.edu.in
bPolymers and Functional Materials Department, CSIR-Indian Institute of Chemical Technology, Hyderabad 500007, India. E-mail: mvas@iict.res.in
cAcademy of Scientific and Innovative Research (AcSIR), Ghaziabad 201002, India

Received 17th July 2024 , Accepted 26th September 2024

First published on 17th October 2024


Abstract

Nanotechnology is the platform with the greatest promise for scientific advancements. One of the advancement is improvement in photocatalytic and antibacterial performance. This work was undertaken to synthesize un-doped and silver (Ag) doped zinc oxide (ZnO) nanoparticles (NPs) using an inexpensive wet chemical method and to investigate the structural and optical properties, photocatalytic and antibacterial activity. The structural analysis from X-ray diffraction (XRD) pattern of un-doped and Ag-doped ZnO NPs displayed hexagonal wurtzite crystal structure and shifting in the peak position confirms the incorporation of Ag in ZnO lattice. Morphological study done by scanning electron microscope reveals spherical shaped NPs and an increase in grain size with Ag doping, the HRTEM images showed the nanocrystalline nature of particle. The Raman spectra showed variation in vibrational characteristics of the nanoparticles with Ag doping. The functional groups were analyzed using Fourier transform-infrared spectroscopy (FTIR). The optical properties were investigated by UV-visible and photoluminescence (PL) spectroscopic techniques. The Ag-doped ZnO NPs have a notably lower band gap than that of un-doped ZnO NPs, i.e. from 3.04 eV to 2.81 eV as studied by UV-visible spectra. The PL study showed decrease in intensity at near band edge emission with increase in Ag doping concentration indicating reduction in the free charge carrier recombination. These variations in the properties play major role in the enhancement of photocatalytic and antibacterial activity with increase in Ag doping concentration as compared to un-doped zinc oxide nanoparticles. The photo degradation efficiency of 99.12 ± 1% against Methylene Blue dye was achieved in the shortest period of 45 minutes ever reported when irradiated under the solar light and efficiency of 97.33 ± 1% was achieved in 15 min under Xenon Short Arc lamp. The antibacterial study was conducted using the Agar well diffusion method where the diameter of the zone of inhibition (ZOI) was increased from 14 mm to 20 mm and 13 mm to 18 mm against the bacteria Escherchia coli and Bacillus subtilis respectively, rendering this material suitable for photocatalytic degradation and antibacterial applications.


Introduction

Nanotechnology1 has emerged as a powerful tool for advancing materials science and addressing critical challenges across various fields. Scaling down a material from macro to nano size has significant effects on its properties, such as optical, magnetic, electrical, antibacterial, and mechanical properties, among others. Nanoparticles (NPs) are defined as particles with a diameter varying from 1 to 100 nm2. The development of metal oxide nanostructures, including TiO2, ZnO, SnO2, MnO2, Co3O4, Fe2O3, NiO, has a significant impact in material science and many other fields due to their extraordinary physiochemical properties, such as density, melting/boiling points, electrical conductivity, magnetism, basicity, and reactivity etc.3–8Among all metal oxides, ZnO stands out as a significant nanomaterial because of its excellent optoelectronics, piezoelectric, gas sensing, photocatalytic, and antibacterial properties. These properties are attributed to unique characteristics like a broad energy gap of 3.37 eV, high intrinsic electron mobility of 300 cm2 V−1 s−1, large excitonic binding energy of 60 meV, a melting point as high as 2248 K, and a cohesive energy of 1.89 eV.9–12 Photocatalysis emerges as one of the most efficient and sustainable approach for environmental remediation, enabling the decomposition of pollutants by harnessing solar energy.13,14 Among these pollutants, the cationic compound Methylene blue (MB), a common dye used in various industries has been found to be toxic and hazardous to the environment.15–17 Additionally, antibacterial strategies aim to tackle the challenges posed by bacterial infections, which remain a constant threat to global health. Although ZnO exhibits promising qualities as a photocatalytic, biocompatible, and antibacterial agent, the rapid recombination of photo-generated electron–hole pairs presents a constraining factor that retards the activity of ZnO NPs. In response to this challenge, significant efforts have been devoted to improvement. Doping ZnO NPs with metals has demonstrated effectiveness in producing highly active reactive agents. ZnO doped with metals like Ni, Mn, Fe, Co, Cr and Ag and synthesized via hydrothermal method show good photocatalytic activity due to narrowing of the band gap.18,19 Doping with other novel metals with suitable work functions, such as Pt, Pd, Au also increases photodegradation and antimicrobial efficiency.20–23 Currently, the production of Ag-doped ZnO NPs has become an exciting area of research for both photocatalytic and antibacterial activities. Among all the metals/novel metals Ag shows better enhancement in both the activities. Since the band gap of ZnO is relatively large, the integration of Ag ions (Ag+) in ZnO host lattice enhances absorption capacity, improves charge separation capabilities, and offers significant potential for enhancement. Ag NPs have been utilized for degradation of pollutants found in industrial waste and control of bacterial growth on various materials such as medical devices, dental composite materials, and textiles. Silver (Ag) can enhance the photocatalytic activity of ZnO nanoparticles by improving surface properties such as O vacancies, crystal deficiencies and increased specific surface area.24 The reported photodegradation efficiency due to reactive oxygen species (ROS) production and band gap of Ag-doped ZnO NPs was 98% in 120 minutes.1 Various studies reported the degradation efficiency of 89% at 140 min25 of Ag-doped ZnO NPs against ponceau, removal of CB dye about 65% after 120 min,26 100% degradation efficiency against MB dye after 300 minutes,27 2% increase in degradation efficiency on Ag doped ZnO compared to ZnO against the MV dye.28 The antibacterial activity against the bacterial strain of Escherichia coli, Bacillus subtilis, Pseudomonas aeruginosa, Staphylococcus aureus, Enterococcus faecalis were also reported.2,29,30 Surface characteristics, including oxygen vacancies and crystal defects contribute to the enhanced photocatalytic and antibacterial activity of the particles.31,32 Consequently, Ag-doped ZnO NPs have been utilized as both photocatalytic and antibacterial agents owing to the alteration in crystallite size/particle size resulting from the incorporation of Ag into the ZnO lattice. Ag NPs exhibit a large surface-to-volume ratio, which enhances their effectiveness in supporting these activities.

Several methods have been employed for the development of ZnO NPs, including the sol–gel method,33,34 hydrothermal and solvothermal methods,35,36 electrochemical method37 microwave method38,39 and others. Yet, these methods often entail significant time and complexity. The current study primarily emphasizes a simple and cost-effective synthesis technique for un-doped and Ag-doped ZnO NPs using the wet chemical method. While there is an abundance of literature on nanoparticle synthesis via the wet chemical route, only a limited number of studies offer comprehensive analysis of the photocatalytic and antibacterial activity of Ag-doped ZnO NPs. This study reports a photodegradation efficiency of 99.12 ± 1% in Ag-doped ZnO NPs within 45 minutes, and 97.33 ± 1% in 15 min under solar light and Xenon Short Arc lamp respectively marking the shortest span ever reported. The objective of this approach is to explore the structural and optical properties, as well as the photocatalytic activity for degrading MB and the antibacterial effectiveness against bacterial strains, including Gram-negative Escherichia coli and Gram-positive Bacillus Subtilis, of Ag-doped ZnO NPs.

Experimental procedure

Materials

Un-doped and Ag-doped ZnO (Ag/ZnO) NPs were synthesized using the following chemicals: zinc acetate (Zn(CH3COO)2·2H2O, 98.0%, M.W. – 219.50, Lobagens), sodium hydroxide pellets (NaOH, 98.0%, M.W. – 40, Himedia), silver nitrate (AgNO3, M.W. – 169.87, Fisher), and deionized (DI) water, which was also used in the experiment.

Synthesis method

Un-doped and Ag-doped ZnO (with Ag at. wt%: 1, 3, 5 and 7%) NPs were synthesized using the wet chemical method. For ZnO synthesis, a 1 M solution was prepared through dissolution of zinc acetate ((CH3COO)·2Zn·2H2O) in 50 ml of deionized (DI) water, stirred for 30 minutes. Another solution of the reducing agent, 1 M NaOH, was prepared. After 30 minutes, this solution was gradually introduced to the zinc acetate solution under the same stirring conditions until a white precipitate formed, maintaining a pH of 5–6. The solution was subsequently stirred for two hours at ambient temperature. Once the precipitate had fully formed, the solid and liquid phases were separated employing a centrifuge for 10 minutes at 6000 rpm. The precipitate was washed 3–4 times with deionized water and ethanol to remove impurities, subsequently dried in an oven for 20 hours at 80 °C. The dried precipitate was then ground, and finally, the resulting powder was annealed in a muffle furnace at 400 °C for 2 hours, producing un-doped ZnO NPs. For the synthesis of Ag-doped ZnO NPs, the required amount of silver nitrate (AgNO3), corresponding to the doping at. wt% (1%, 3%, 5%, 7%), was added to the zinc acetate solution in the above reaction. The entire procedure remained the same. Finally, Ag/ZnO NPs were formed with various concentrations of Ag at. wt%. Henceforth Ag-doped ZnO NPs (Zn1−xAgxO:X = 0.01, 0.03, 0.05, 0.07) are denoted as AZO-1, AZO-3, AZO-5, AZO-7 respectively.

Characterization techniques

X-ray diffraction (XRD) patterns of the samples, utilized for phase identification and crystallinity determination, were obtained using a Bruker D8 Advance X-ray powder diffraction technique. CuKα radiation with a wavelength (λ) of 1.5404 Å was employed. A scanning electron microscope (SEM) specifically the NOVA NANOSEM 450 was utilized for morphological analysis. Elemental composition was studied using energy dispersive X-ray (EDX) analysis with the help of a NOVA NANOSEM 450 microscope working at a 200 kV accelerating voltage, Microstructure study was carried out using a transmission electron microscope (G2F30S – Twin model of HRTEM). The RAMAN analysis was done by LABRAM-HR 800 (Horibra) RAMAN spectrometer having a diode laser source of wavelength 473 nm. Bruker Alfa II instrument was employed for Fourier transforms infrared (FTIR) spectra analysis. Optical analysis was conducted using a Shimadzu UV 2401 PC spectrophotometer. Additionally, photoluminescence (PL) spectra were captured using a Spectro fluorophotometer, namely the Horiba Scientific Instrument Fluoromax-4 spectrofluorometer. A spectral slit width of 3.0 nm was used, and a 450 W xenon arc lamp served as the exciting source.

Photocatalytic studies

The photocatalytic experimental set-up was developed by exposing reaction mixture (Photocatalyst-MB dye solution) in sunlight under constant stirring of 500 rpm in a magnetic stirrer. Solar light intensity was gauged using a Lux meter. 5 mg of catalyst was introduced into the 50 mL of 10−5M MB dye solution. The solution was then stirred continuously under sunlight. At a regular interval of 15 minutes, 5 mL of reaction mixture was extracted using a micropipette by switching off the stirring process. Till 90 minutes, 6 such aliquots were taken and each mixture was centrifuged at 10[thin space (1/6-em)]000 rpm for 10 minutes. The same experiment was also performed using Xenon Short Arc lamp (150 watt, Air cooling) under constant magnetic stirring of 500 rpm. Here, samples were collected at a regular time interval of 5 minutes. The solution was then centrifuged at 10[thin space (1/6-em)]000 rpm. Then, each mixture was then analysed using the UV-visible spectroscopy over the wavelength range of 200–800 nm, to verify the absorbance values. The change in absorbance values is the guidance towards the MB degradation studies.

Antibacterial studies

For assessing the antibacterial potential of un-doped and Ag-doped nanoparticles, Agar well-diffusion method was employed. The antibacterial potency of nanoparticles was assessed on nutrient agar plates against E. coli and B. subtilis. The bacterial suspension was evenly distributed on the plates and 100 μL un-doped and Ag-doped ZnO NPs of suspension was poured on 6 mm wells made on agar surface from sterile cork borer. DI water was taken as a control. Plates were then incubated at 37 °C for 24 h and the inhibition zone was measured.

Results and discussion

X-ray diffraction examination

The structural analysis of un-doped and Ag-doped ZnO NPs was done using X-ray diffraction (XRD) technique. The XRD patterns of both un-doped and Ag-doped ZnO NPs, as shown in Fig. 1a, reveal that ZnO and AZO-1, AZO-3, AZO-5, AZO-7 exhibit hexagonal wurtzite structure, confirming in accordance with JCPDS No.- 800[thin space (1/6-em)]075. The diffraction peaks of ZnO NPs, observed at 2θ angles of 31.55, 34.21, 36.05, 47.38, 56.39, 62.69, 66.22, 67.77, and 68.94°, correspond to the diffraction planes (100), (002), (101), (102), (110), (103), (200), (112), and (201), respectively. The sharp and intense diffraction peaks indicate the crystalline nature of NPs. In the Ag-doped ZnO pattern, a right shift in the diffraction peak position was noted (Fig. 1b), which confirms the integration of Ag+ ions into the ZnO host lattice. This shift is attributed to the larger ionic radius of Ag+ (0.126 nm) compared to Zn2+ (0.074 nm). Upon Ag doping in the ZnO lattice, additional diffraction peaks at 37.97°, 44.17°, and 64.32° due to Ag were detected for higher Ag concentrations (3, 5 and 7 at%).
image file: d4ra05197a-f1.tif
Fig. 1 (a) XRD pattern of un-doped ZnO and Ag-doped ZnO (AZO-1 to AZO-7) NPs (b) enlarged view of XRD peak corresponding to diffraction plane (101).

To investigate the impact of Ag dopant on the crystallite size (D), the Debye–Scherrer equation (eqn (1)) was utilized for estimating the crystallite size, as outlined in Table 1.

 
D = [thin space (1/6-em)]cos[thin space (1/6-em)]θ (1)
where k = 0.9, X-ray wavelength λ = 1.54 Å, β = FWHM, θ = Bragg angle. With increase in Ag content the crystallite size increases for AZO-1 but after that it decreases for AZO-3 and AZO-5 and again it increases for AZO-7 sample. The increase in crystallite size may have attributed to ionic size difference between the Ag+ (0.126 nm) and Zn2+ (0.074 nm) ions.28 In AZO-1, there is substitution of Ag ions on Zn2+ ions and due to ionic size difference the crystallite size may have increased. The crystallite size decreases due to the lattice stress induced by the presence of Ag within the ZnO structure.40 Due to incorporation of more Ag ions in ZnO lattice, stress is created due to which crystallite size has reduced in AZO-3 and AZO-5.

Table 1 Parameters derived from XRD analysis
Sample For miller diffraction plane (101)
FWHM d-spacing (Å) Crystallite size D (nm) Dislocation density (δ × 10−3) Microstrain (ε × 10−3)
ZnO 0.406 2.487 20.55 2.367 5.445
AZO-1 0.353 2.478 23.68 1.784 4.709
AZO-3 0.405 2.479 20.61 2.354 5.412
AZO-5 0.427 2.478 19.56 2.613 5.7
AZO-7 0.318 2.484 26.31 1.444 4.249


The d-spacing was determined using Bragg's equation (eqn (2)).

 
2d[thin space (1/6-em)]sin[thin space (1/6-em)]θ = (2)

The dislocation density was calculated using the eqn (3) (ref. 41)

 
δ = 1/D2 (3)

The microstrain was evaluated using the eqn (4) (ref. 42)

 
ε = β/4 × tan[thin space (1/6-em)]θ (4)

The Rietveld refinement of structural parameters was performed by full proof software. The crystal space group P63mc and Pseudo-Voigt background mode were employed with the 100 refinement cycles. As a representative of the series, the refinement plots of un-doped ZnO and AZO-3 are shown in Fig. 2, where the XRD experimental data are indicated by red circle, the fitted data by black colour line whereas the blue line indicate the difference between above two and green vertical line shows Braggs position. The output data are presented in Table 2.


image file: d4ra05197a-f2.tif
Fig. 2 Rietveld refinement of (a) Un-doped ZnO and (b) AZO-3.
Table 2 Parameters observed from Rietveld refinement
Parameters ZnO AZO-1 AZO-3 AZO-5 AZO-7
χ2 1.977 2.019 3.614 5.665 7.401
Lattice parameters a 3.258 3.256 3.255 3.258 3.258
b 3.258 3.256 3.255 3.258 3.258
c 5.219 5.217 5.214 5.218 5.219
R factors (%) Rp 15.2 13.8 15.8 19.0 19.1
Rwp 11.2 9.96 11.6 16.9 19.8
Re 7.93 7.01 6.10 7.08 5.88
Volume (Å3) 47.97 47.91 47.83 47.96 47.98
Bragg R factor 1.87 2.26 5.26 4.46 3.04
RF factors 1.02 1.30 3.63 2.23 1.08


Throughout the refinement process, the χ2 shows the Goodness of fitting and the three R-factor show the reliability of fitting, given in the table as Profile Residual (Rp), Weighted Profile (Rwp) and Expected Value (Rexp). Rietveld analysis showed a slight decrease in a and c lattice parameter for AZO-1 and AZO-3 and after that it increased for AZO-5 and AZO-7 samples. Same trend occurred for cell volume also. This may have happened due to formation of silver nanocollection and part substitution by Ag+ ions28 and existence of microstructural strain from defects in Ag–ZnO.

SEM analysis

As a representative of the series, the surface morphology of both un-doped ZnO and AZO-3 NPs was analysed through SEM analysis [Fig. 3a and b]. Spherical grains were observed on the surface of both un-doped and doped samples. The average grain size was determined using ImageJ software. According to the particle distribution curve [Fig. 3c and d], the average particle size of un-doped ZnO and AZO-3 NPs is found to be 46.89 nm and 67.33 nm, with standard deviations σSD of 1.22 nm and 1.32 nm, respectively. The presence of elements was confirmed by the elemental mapping through EDX images [Fig. 3e–m].
image file: d4ra05197a-f3.tif
Fig. 3 SEM images of (a) un-doped ZnO and (b) AZO-3, (c and d) Particle Distributions curve, (e–m) elemental mapping of Un-doped ZnOs and AZO-3 NPs respectively.

TEM analysis

The microstructural image of AZO-3 nanoparticles presented in Fig. 4, was analyzed using high-resolution transmission electron microscopy (HRTEM). The TEM image of AZO-3 reveals that the synthesized nanoparticles possess a hexagonal topology (a). The average particle size was calculated to be 58.09 nm, with a standard deviation of σSD = 1.39 nm (b). The HRTEM image of AZO-3 nanoparticles distinctly shows the lattice fringes (c), confirming the crystalline nature of the nanoparticles,43 with a measured d-spacing of 2.3846 Å (0.23846 nm). The nanocrystalline nature of AZO-3 nanoparticles is further corroborated by the appearance of dispersed ring patterns in the selected area electron diffraction (SAED) images (d).1
image file: d4ra05197a-f4.tif
Fig. 4 (a) TEM images (b) particle distributions curve (c) HRTEM image (d) SAED image of AZO-3 NPs.

Raman spectra analysis

The additional structural information of un-doped ZnO and Ag-doped ZnO (AZO-1 to AZO-7) was collected through Raman scattering spectra [Fig. 5]. The effect of Ag on the vibrational properties of ZnO NPs was observed. Wurtzite structure of ZnO belongs to P63mc space group. From the analysis of group theory, the modes are defined for observed peaks. The peak observed at 437 cm−1 attributed to E2(high) mode confirms the wurtzite structure of ZnO.44 On Ag doping in ZnO, the intensity of E2 (high) phonon mode decreases indicating decrease in crystallinity due to incorporation of Ag in ZnO lattice. The E1(LO) mode observed at 560–580 cm−1 is caused by defects in the ZnO lattice. These defects and disorder are introduced due to Ag incorporation in ZnO lattice.45 The peak at 332 cm−1 corresponds to E2(high)–E2(low) mode, observed due to the second order Raman spectrum, and A1(TO) mode and Raman inactive mode B1(low) are assigned at 385 cm−1 and 279 cm−1 respectively.46 The peak at 207 cm−1 assigned with 2E2(low) mode arises due to the vibration of oxygen atom.47 Due to variation of defects and disorder, there is shift in peak position and change in intensity.
image file: d4ra05197a-f5.tif
Fig. 5 Raman spectra of un-doped ZnO and Ag-doped ZnO (AZO-1 to AZO-7) NPs.

Fourier transform infrared (FTIR) spectra analysis

To investigate the functional group and the molecular interactions in un-doped and Ag-doped ZnO NPs FTIR spectra were analyzed in the range of 400–4000 cm−1 [Fig. 6]. The peaks observed at 527 cm−1 and 870 cm−1 in the un-doped ZnO NPs confirm the formation of metal oxide bond which arise due to vibrational stretching of Zn–O bond.48 The absorption peak at 1434 cm−1 represents the C[double bond, length as m-dash]O stretching mode.49 The peak at 2886 cm−1 corresponds to C–H bond.48,50 The hydroxyl group of metal oxide is present in the range of 3768–3679 cm−1 which arises due to stretching vibration of O–H bond51 and the peak at 2312 cm−1 shows the impurity of IR spectra.40,49 From the IR spectra the slight shift in the absorption peak with Ag doping can be associated with the substitution of Ag+ ions in the ZnO lattice28
image file: d4ra05197a-f6.tif
Fig. 6 FTIR spectra of un-doped ZnO and Ag-doped ZnO (AZO-1 to AZO-7) NPs.

UV-visible absorption spectra analysis

Optical absorption spectra of both un-doped and Ag-doped ZnO NPs were recorded using a room temperature UV-visible spectrometer in the range of 200–600 nm [Fig. 7a]. A distinct absorption peak was observed at 372 nm for un-doped ZnO NPs. Upon Ag doping, peaks were shifted to positions 374 nm, 375 nm, 376 nm and 378 nm, for AZO-1 to AZO-7 respectively. These peaks were attributed to the excitonic absorption peak of zinc oxide nanoparticles.52 The introduction of Ag through doping resulted in a red shift, moving the absorption edge towards higher wavelengths. The shift in absorption peak suggests a change in the energy band gap (Eg) due to the doping process. The optical energy band gap of the particles was determined using Tauc plot method.53 This involved plotting photon energy () against (αhν)2 graphs using eqn (5) and the extrapolation of the linear portion of the above graph gives the energy bandgap.
 
(αhν)n = A(Eg) (5)
where α = absorption coefficient, h = Plank's constant, ν = light frequency, A = constant, Eg is the optical bandgap, n = 2 for direct electronic transition and n = 1/2 for indirect transition.

image file: d4ra05197a-f7.tif
Fig. 7 (a) UV-vis absorption spectra (b) energy band gap by Tauc plot method of un-doped ZnO and Ag-doped ZnO (AZO-1 to AZO-7) NPs.

The optical energy band gap of un-doped ZnO was measured as Eg = 3.04 eV. Upon the addition of Ag, the bandgap was reduced to 3.00 eV, 2.94 eV, 2.88 eV and 2.81 eV for 1% to 7% doping respectively, as illustrated in Fig. 7b. The variation in the energy band gap can be attributed to the presence of oxygen vacancies, which facilitate the electron transitions from the valence band (VB) to the conduction band (CB).54 Due to the addition of Ag some intermediate states may have created between CB and VB in ZnO host matrix due to which band gap is reduced. Also Ag behaves like an acceptor in ZnO which lowers the band gap in Ag doped ZnO. This reduction in the energy band gap has implications for improving the optoelectronic, photocatalytic and antibacterial efficiency of the material.

Photoluminescence study

PL serves as a crucial tool for probing the optical and photochemical properties of materials, offering insights into structural imperfections such as oxygen vacancies and metal interstitials of semiconductor samples.50 PL spectra were recorded for both un-doped ZnO and AZO nanoparticles with varying concentrations of Ag doping. The PL spectra of samples taken at room temperature are presented in Fig. 8a, in the wavelength range of 370 to 650 nm, using an excitation wavelength of 350 nm. A distinctive peak at the edge of the UV spectrum is observed around 390 nm. The UV emission is attributed to the near-band-edge (NBE) emission, indicative of free exciton recombination corresponding to the exciton–exciton collision phenomenon.28,55 This recombination is associated with the high surface-to-volume ratio.56 A slight shift in the peak position is noted with Ag doping, and as the doping concentration increases, the intensity decreases due to interactions among ZnO and Ag NPs at the grain boundaries. These interactions lead to a reduction in the recombination of electrons and holes.28,57 Additionally, Ag acts as an acceptor, trapping electrons and reducing the electron–hole recombination rate, thereby decreasing the PL intensity.58
image file: d4ra05197a-f8.tif
Fig. 8 (a) PL spectra of un-doped and Ag-doped ZnO NPs with excitation wavelength of 350 nm, Gaussian fitting of PL spectra of un-doped ZnO (b) and AZO-3 NPs (c).

The spectra of ZnO and AZO-3 samples were deconvoluted by using Gaussian fitting [Fig. 8b and c]. A blue emission peak at 447 nm and 443 nm are discerned, which are due to electron transition from shallow donor levels to the acceptor levels to the top level of the VB,59 accompanied by a violet emission peak at 411 nm and 408 nm which might have arisen due to Zn vacancies (VZn)60 for un-doped ZnO and AZO-3 NPs respectively.

Photocatalytic activity

The synthesized un-doped and Ag-doped ZnO NPs are potent photocatalysts for the degradation of MB dye. The schematic diagram of photocatalytic mechanism is represented in Fig. 9. In this, the fermi energy of Ag-doped ZnO NPs is lower than that of un-doped ZnO NPs, causing electrons to move from ZnO to Ag.61,62 Radical production is the primary mechanism behind the photodegradation of MB dye using un-doped and Ag-doped ZnO photocatalyst. The highly reactive radicals generated in the solution attack the dye molecules, resulting in less toxic by products such as water and carbon dioxide. When the photocatalyst and dye solution are irradiated with solar light, electrons from the valence band (VB) jump to the conduction band (CB), leaving holes in the VB of the ZnO NPs. These electrons and holes serve as charge carriers for radical generation. The electrons in the conduction band react with ambient or adsorbed oxygen to form O2˙ (superoxide anion), while the holes in the valence band react with water molecules to produce H+ (protons) and OH˙ (hydroxyl radicals). Similarly, the holes can react with adsorbed hydroxyl anions (OH) to generate additional OH˙ radicals. These primary radicals generate further reactive oxygen species, such as HOO˙ (peroxide radicals), OH˙, and OH (hydroxyl anions). These radicals generated attack and degrade the dye molecules through reduction and oxidation processes, converting them into less harmful products like H2O and CO2. Hence, the electron–hole pair generation is the primary cause of dye degradation process.
image file: d4ra05197a-f9.tif
Fig. 9 Schematic diagram of Photocatalytic mechanism of Ag-doped ZnO NPs.

In this study the photocatalytic performance of un-doped and Ag-doped ZnO NPs (AZO-3, 5) were observed through UV-visible spectra [Fig. 10A and B]. In the beginning (at 0 min) the absorbance of the solution was observed at 663 nm in the presence of the synthesized photocatalysts and both sunlight and Xenon Short Arc lamp were used as the light source, the absorbance peaks were decreased with the irradiation time. The doped ZnO photocatalysts show faster decrease in the absorbance as compared to un-doped ZnO.


image file: d4ra05197a-f10.tif
Fig. 10 (A). Photocatalytic activity of Un-doped ZnO, AZO-3 and AZO-5 NPs in degradation of MB dye under sunlight. (B) Photocatalytic activity of Un-doped ZnO, AZO-3 and AZO-5 NPs in degradation of MB dye under Xenon Short Arc lamp.

The photodegradation efficiency of the prepared nanoparticles against the MB dye was calculated using eqn (6).

 
Photo degradation efficiency (%) = (C0C)/C0% (6)
where C0 = initial concentration of MB and C = concentration of MB after degradation.

During the photo degradation of MB, under the sunlight the efficiency of ZnO was calculated to be 41.97 ± 1% after 15 min of irradiation time while the efficiency of AZO-3 and AZO-5 was calculated to be 86.17 ± 1% and 96.15 ± 1% respectively in 15 min. In the short span of 45 minutes, efficiency of Ag-doped ZnO NPs was determined to be 99.12 ± 1% [Fig. 11A] which is the shortest time period ever reported till the date to the best of our knowledge. Additionally, at the same time under Xenon Short Arc lamp the efficiency of ZnO was calculated to be 96.63 ± 1% after 60 min of irradiation time while the efficiency of AZO-3 and AZO-5 was calculated to be 97.33 ± 1% in 20 min and 15 min respectively [Fig. 11B]. This demonstrates that the Ag doping in ZnO NPs increases the production of hydroxyl radicals which promotes great photocatalytic performance. The photocatalytic kinetics was employed to determine the dye concentration [Fig. 12a and 13a] and rate constants (k) for the degradation reaction of dye which follows pseudo-first order kinetics eqn (7) [Fig. 12b and 13b].

 
In(C/C0) = −kt (7)
where t = irradiation time.


image file: d4ra05197a-f11.tif
Fig. 11 (A) The photodegradation efficiency of ZnO, AZO-3 and AZO-5 with the function of irradiation time under sunlight. (B) The photodegradation efficiency of ZnO, AZO-3 and AZO-5 with the function of irradiation time under Xenon Short Arc lamp.

image file: d4ra05197a-f12.tif
Fig. 12 (a) Dye concentration (b) photocatalyst kinetic plots of the photodegradation reaction of MB dye in the presence of catalysts ZnO, AZO-3 and AZO-5 NPs under sunlight.

image file: d4ra05197a-f13.tif
Fig. 13 (a) Dye concentration (b) photocatalyst kinetic plots of the photodegradation reaction of MB dye in the presence of catalysts ZnO, AZO-3 and AZO-5 NPs under Xenon Short Arc lamp.

The pseudo-first order plot reveals that the observed dye degradation rate constants for the catalyst AZO-3 and AZO-5 is found to be 0.07807 min−1 and 0.07423 min−1 respectively, which is higher than that of un-doped ZnO catalyst (0.0554 min−1) under the sunlight [Fig. 12b]. Where the rate constant for the catalyst AZO-3 and AZO-5 is found to be 0.15853 min−1 and 0.23597 min−1 respectively, and for un-doped ZnO catalyst it is 0.0483 min−1 under Xenon Short Arc lamp [Fig. 13b]. So, from the degradation efficiency and kinetics it is evident that Ag-doped ZnO NPs exhibit greater photocatalytic activity in contrast to ZnO NPs which is due to lower bandgap or due to larger surface area. Incorporating Ag into ZnO reduces the recombination of photogenerated electrons and holes, thereby resulting in improved photodegradation of MB dye. The PL studies showed reduction in intensity as the doping concentration of Ag increases indicating decrease in the free charge carrier recombination which enhances photocatalytic activity. Table 3 shows a comparison of literature survey on photocatalytic activity from which it is evident that our samples possess highest photodegradation efficiency in the shortest time ever reported.

Table 3 Photocatalytic activity of Ag-doped ZnO catalyst reported from the literature
S. no. Photocatalyst (mol/wt%) Synthesis method Catalyst; dye Light source Photodegradation efficiency (%) Time (min) Ref.
1 Ag–ZnO Co-precipitation 25 mg/50 ml; 10 mg L−1, MB Halogen lamp 93% 80 63
2 Ag–ZnO Sol–gel 0.1 g/100 ml; 2 × 10−5 M, MB Visible light 82.6% 240 64
3 Ag–ZnO Green synthesis 1.75 g L−1; 20 mg L−1, CR 440 W ultrasound 92.14% 60 65
4 Ag–ZnO Co-precipitation method 20 mg/100 ml; 20 ppm/30 ml, MB UV lamp 92.43% 150 15
5 Ag–ZnO (0.5%) Co-precipitation 0.05 g; 10−5 M, MB Visible light 98% 120 66
6 Ag–ZnO(3%) Hydrothermal method 50 ppm/100 ml, CB dye Visible light 65% 120 49
7 Ag–ZnO (0.14 to 0.88 wt%) Photodeposition method 0.15 g L−1; 50 mg L−1, phenol UV light 95% 180 67
8 Ag–ZnO (2.5%) Thermal solvent Direct blue 15 UV radiation 73.6% 120 14
9 Ag–ZnO (0–1%) Co-precipitation method 15 mg/25 ml; 2.5 mol L−1, MB Solar light 98% 120 13
10 Ag–ZnO(3, 5%) Wet chemical method 5 mg/50 ml; 10−5 M, MB Sunlight (100[thin space (1/6-em)]200 lux) 99.12% 45 Present work
Xenon short arc lamp 97.33% 20, 15


Antibacterial activity

In this study, un-doped and Ag-doped ZnO NPs were investigated for their antibacterial activity against the Gram-negative bacterial strain E. coli and the Gram-positive strain B. subtilis using the Agar well diffusion method. The zone of inhibition (ZOI) around each well was measured [Fig. 14]. Table 4 illustrates that the ZOI of Ag-doped ZnO NPs has significantly increased in comparison to un-doped ZnO NPs. This enhancement is attributed to a synergistic effect that results in the production of reactive oxygen species (ROS), such as superoxide and hydroxyl radicals.1,2,28 These reactive entities trigger oxidative stress in bacterial cells, resulting in cell damage and bacterial death. Among the tested bacterial strains, the nanoparticles exhibited the highest inhibitory activity against E. coli, followed by B. subtilis, with ZOIs of 20 mm and 18 mm, respectively, at a concentration of 25 mg ml−1. The control, in contrast, showed no zone of inhibition, underscoring the inhibitory action of both un-doped and Ag-doped ZnO NPs.
image file: d4ra05197a-f14.tif
Fig. 14 Screen of un-doped and Ag-doped ZnO nanoparticles for antibacterial action against (a) E. coli (b) B. subtilis where A0 = un-doped ZnO NPs, A1 = AZO-1, A3 = AZO-3, A5 = AZO-5, A7 = AZO-7.
Table 4 Zone of Inhibition of synthesized NPs
S. no. Synthesized NPs Zone of inhibition (mm)
E. coli B. subtilis
1 ZnO 14 13
2 AZO-1 19 16
3 AZO-3 20 17
4 AZO-5 19 17
5 AZO-7 20 18


Conclusion

In summary, we investigated the structural, optical, photocatalytic and antibacterial properties of both un-doped and Ag-doped ZnO NPs. The samples were successfully synthesized employing a cost effective wet chemical method. The structural studies conducted by XRD, Raman spectra reveals the formation of phase pure hexagonal wurtzite structure and functional groups were analysed by FTIR spectroscopy. SEM images revealed spherical shaped NPs and HRTEM images showed the nanocrytalline nature of synthesized nanoparticles having diameter of 58.09 nm and calculated d-spacing of 2.3846 Å justifying the SEM and XRD results respectively. The optical properties were investigated through UV-vis and PL spectra. From UV-vis spectra, a reduction in energy band gap is observed with increase in Ag doping. The alteration in the energy band gap value relies on diverse factors, such as crystallite size and the placement of the dopant within the host lattice. With increase in Ag doping concentration, the free charge carrier recombination is decreased as observed in the PL spectra. The variations in the structural and optical properties of Ag-doped ZnO NPs, compared to un-doped ZnO NPs, contributed to the excellent photocatalytic and antibacterial activity. The photocatalytic study shows highest degradation efficiency of 99.12 ± 1% in the span of 45 min under sunlight and 97.33 ± 1% in 15 min under Xenon Short Arc lamp which are the shortest time ever reported. Therefore, Ag-doped ZnO NPs find extensive applications in waste water treatments and pharmaceutical manufacturing.

Data availability

The corresponding author (Dr Anupama Chanda) confirms that whenever required we will provide the original data used in this manuscript.

Author contributions

The first author (Vaishali Amrute) has contribution in methodology, investigation and original draft writing. Second author (Monika) has contributed in data curation. Third author (K. K. Supin) has contribution in data curation and investigation and editing. Fourth author (M. Vasundhara) has contribution in investigation, review and editing. Fifth author (Anupama chanda) has contribution in conceptualization, supervision, review and editing.

Conflicts of interest

The authors declare that there is no conflict of interest.

Acknowledgements

The first author (Vaishali Amrute) Acknowledges UGC-DAE CSR, Indore for RAMAN analysis, Department of Microbiology for antibacterial study and the Centre for Advanced Research (CAR) of Dr. Harisingh Gour Vishwavidyalaya, Sagar (M.P.) (A Central University) for XRD, SEM and TEM analysis. M. Vasundhara would like to acknowledge the support offered by Department of K & IM of Indian Institute of Chemical Technology (IICT/Pubs./2024/350).

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