Inhibition zones of Ag and Au NSs.
Abstract
Biosynthesized silver (Ag) and gold nanoparticles (Au NPs) were synthesized by using Punica granatum and Citrus reticulata extracts and these extracts act as stabilizer. The average sizes of the Silver and Gold NPs were in the range of 8–10 nm and 30–40 nm, respectively. The confirmation of NPs was done by UV-visible absorption spectra, X-ray diffraction (XRD), transmission electron microscope (TEM), and Fourier transform infrared spectra (FTIR) techniques. The luminescence studies of europium and samarium complexes with NPs were studied. Emission intensities of complexes with the presence of silver enhanced and quenched with gold due to the reabsorption. The toxicity and antimicrobial studies of nanostructures were studied.
Keywords
- eco-friendly green synthesis
- metal nanostructures
- luminescence
- MTT assay
- antimicrobial activity
1. Introduction
Nanomaterials exhibit chemical, physical, and biological features that are not found in other materials. In the food industry, electrical and chemistry industry, and cosmetics industry metal nanostructures have unique applications. In medicinal and industrial uses, Ag and Au nanoparticles comprise the backbone. The food sector [1, 2], catheters [3], dressings of wound [4], surgery equipment [5], synthetics [6], and optical limiter applications [7] all use silver nanostructures. Sensors [8], catalytic [9], and electrical applications [10] are only a few of the applications for gold nanoparticles. The usage of Au and Ag nanostructures as drug delivery systems demonstrated as bactericidal against Gram-positive and negative [11].
By-products from traditional synthesis techniques can be hazardous [12]. As a result, a variety of environmental and green synthesis strategies are being researched [7, 13]. Nanomedicine has had a huge influence as a result of these biosynthesized nanomaterials, and they have become the elementary units for upcoming medications to treat many ailments [14]. Plant extracts, enzymes, fungi, bacteria, and other eco-friendly synthesis processes have been using to synthesize Ag NSa and Au NSs [7, 15, 16]. Papaya, tansy, and citrus fruits are antioxidants found in fruit extracts that are used as stabilizers in the production of Ag and Au NPs [17].
Pomegranate is the scientific name for
Ag NSs have exceptional antibacterial action, which explains why so much work is being put into developing these nanostructures. The use of Ag NPs in medicine is becoming more common. Various investigations have found that Ag NPs significantly reduce mitochondrial activity, resulting in cell apoptosis or necrosis in a variety of cells [21, 22, 23]. Interactions between Ag NPs and cells, on the other hand, have been limited. The surfaces of Au NPs are modified by DNA and amino acids when they are coupled with thiol and amine groups [24, 25]. The biocompatibility of Au NPs in therapeutic applications is critical. The size, shape, and surface modification of Au NPs determine whether they are hazardous or benign to cells [26].
Due to larger Stokes shift, narrower bandwidth of emission, and longer lifetimes emission, lanthanide ions have attracted for various applications like bio-labeling and optical amplification [27], solar cells [28], light-emitting diode (LED) [29], cancer photodynamic therapy [30], and fluoroimmunoassay [31].
Many scientists are interested in the metal enhanced fluorescence (MEF) of metal NSs and rare-earth ions because they need significantly low input intensities, and hence their applications in diagnostics have increased [32, 33]. The fluorophore’s emission intensity is increased by 10–103 when it is near metal particles with subwavelength sizes [34]. The MEF is caused by two methods: (1) fluorophores’ coupling with SPR, and (2) fluorophores’ coupling to the SPR. The influence of a local electric field [35]. Fluorophores with metal particles at 10 nm spacing are acted on by increasing electric fields surrounded the particles, increasing their absorption cross-section and, ultimately, enhanced radiation. The energy transmits from surface plasmonic resonance to the rare-earth ion, and vice versa, results in either enhanced reduction or reabsorption in emission in the other mechanism. The fluorescence increase is primarily influenced by the shape and diameter of nanostructures, fluorophore’s dipole orientations, and the overlap of the fluorophore luminescence intensity and absorption with the plasmonic band of nanostructures [36]. Because of the rivalry of the highly enhanced field surrounding nanoparticles and nonradiative transition due to the dampening of dipole oscillators by metal surfaces, MEF is mostly dependent on the spacing among metal structures and fluorophores [37].
The SPR value is altered by different shapes, various sizes, and dielectric functions of NSs as well as the host [38]. The optimal spacing between fluorophore ions and NPS for emission enhancement exists. Based on the different energy between the rare-earth ions and the metal SPR, quenching of luminescence may occur even at relatively short distances. The number of NSs, SPR, and number of phonon states of fluorophores all affect the luminescence efficiency. The plasmon-mediated augmentation of luminescence-based on the antenna effect has been found, it boosts the excitation effect and emission rate [39]. Metal nanoparticles (donor) absorb energy, which is subsequently transferred nonradiatively to rare-earth ions (acceptor) in the Forster process [40]. One group concluded that energy transmit is the primary cause of emission amplification near metal objects [41]. Other research has found that nanoparticles can stop rare-earth ions from transferring non-radiative energy to metal nanostructures [42, 43]. These are dependent on the luminophore-nanoparticle distance, nanoparticle size, and metal particle concentration.
The goal of this research is to investigate the binding of enhanced fluorescence from Eu(TTFA)3 and Sm(TTFA)3 complexes to metal nanostructures such as silver and gold NSs in greater detail. We discovered a robust link among SPR of NSs and rare-earth molecules, as well as metal nanoparticle reabsorption by the SPR. The MTT assay is being used to investigate the cytotoxicity of metal NSs on cancer cell lines. The findings could aid in the development of biomedication delivery systems that are less hazardous than toxic ones.
2. Materials and synthesis methods
2.1 Materials
Sigma Aldrich provided silver nitrate (AgNO3) and chloroaurate (HAuCl4), which were used without additional purification. The
2.2 Fruit extracts
Fresh
2.3 Synthesis of NSs
30 ml of 1 mM AgNO3/HAuCl4 aqueous solution was produced, and 6 ml of extracts were mixed to the 30 ml of solution at 24°C. The solution was first colorless, then progressively turned ashy, indicating the formation of Ag NPs. In the instance of Au NPs, the yellow solution turned ruby red, it showed that the forming of Au NPs. It is conducted three times to ensure that it is repeatable.
2.4 MTT assay
The MTT (3-(4,5-dimethylthiazol-2-yl)-2,5-diphenyltetrazolium bromide) test was used to investigate the cytotoxic effects of Ag NPs and Au NPs on A549 (lung) and HCT116 (colon) cancer cells. In a 96-well plate, the cell lines were plated at a density of 1 × 104 cells/well in DMEM/1% FBS. For 24 h, cells were incubated at 37°C in an environment of air and CO2 (95% + 5%). When the cells had reached around 80% confluence, they were treated with Ag NPs and Au NPs in various concentrations of 25, 50, 75, 100, and 125 M. MTT assay was used to determine cell vitality after 24 h. MTT solution was added to each cell in a volume of 20 L and incubated for 3–4 h. The formazan was then diffused in dimethyl sulfoxide (DMSO), and optical densities were measured on an ELISA plate reader at 550 nm. As a control, cells were grown without nanoparticles. The ratio of mean optical density to the control was calculated after the measurements were repeated twice. The following calculation was used to calculate cell viability for each well: CV = optical density (OD) of treated well/OD value of nontreated control well) × 100%. The cytotoxicity of Ag NPs and Au NPs was compared to a positive control drug, Oxaliplatin (OXP).
2.5 Antibacterial test
Antibacterial activities of Ag and Au NPs against Gram-negative (Acinetobacter
3. Experimental details
UV-vis absorbance spectra, X-ray diffraction (XRD), transmission electron microscopy (TEM), photoluminescence, cytotoxicity, and antibacterial methods were used. The NP solutions were placed in a 10 mL cuvette and their linear absorption spectra were found with a JASCO-V670 UV/VIS/NIR spectrometer with a wavelength range of 200–800 nm and a 1 nm resolution. Samples were drop casted onto carbon grids and cured at RT for transmission electron microscopy (TEM) examinations. To assess the size of the nanoparticles, the TEM investigation was performed on an FEI model TECHNAI G2 S-Twin. The NPS were analyzed using a Bruker D8 diffractometer at 40 kV, 30 mA, using Cu-K radiation at 1° min-1 scan rate and 0.02 step size across 2 = 20–80°. Eu and Sm complexes with Ag NPs and Au NPs had their photoluminescence spectra recorded on a HORIBA JOBIN YVON fluorescence spectrometer with excitation at 350 nm.
4. Results and analysis
4.1 UV-visible absorbance spectra
The surface plasmon resonance, which is the interaction between free electrons surrounded by metal nanostructures and radiation, was used to validate the formation and stability of Ag and Au NPs. Fruit extracts reduce aqueous silver and gold ions. From Figure 1 shows the well-dispersed formation of Ag and Au NPs, resulted in the SPR peaks were observed in the visible region in the ranges of 350–600 nm and 500–700 nm, respectively. Due to the excitation of SPR vibrations,
4.2 TEM images
The TEM images in Figure 2a and b shows that Ag nanostructures are in spherical shape and range in size from 30 to 70 nm (average size 62 nm). Ag NPs have crystalline FCC structure in their SAED (selected area electron diffraction) patterns. The circular planes corresponding to (1 1 1), (2 0 0), (2 2 0), and (3 1 1) match the XRD pattern very well. With a spherical dimension of 26 nm and edge length of a triangle 52 nm, Au NPs have spherical and triangular shape. Crystallinity of Au NPs with SAED patterns are shown in the planes (1 1 1), (2 0 0), (2 2 0), and (3 1 1). Similarly, the TEM images of Ag and Au NPs by citrus reticulata are shown in Figure 2c and d. The Ag NPs had a diameter of 56 nm and were spherical. The circular rings in the SAED pattern revealed that the produced Ag NPs were of crystalline structure. Figure 2d shows the presence of triangles in addition to spherical nanoparticles. Au NPs had a mean spherical particle size of 21 nm and a triangle edge size of 48 nm. The crystalline structure of Au NPs is revealed by the SAED pattern, which was indexed to (1 1 1), (2 0 0), (2 0 2) and (3 1 1) reflections.
4.3 XRD
Figure 3a–d reveals the XRD of
4.4 Luminescence emission
In Figure 4a and c showed that emission of europium with Ag NPs excited at 350 nm. The Ag concentrations varied from 5 to 300 μl at 15 μl of Eu. The emission at 577 nm, 590 nm (magnetic), and 614 nm (electric) are contributing to 5D0 → 7F0, 5D0 → 7F1, 5D0 → 7F2 transitions respectively. These emission bands were enhanced but emission wavelengths were remains unaltered. With concentration increment of Ag, intensities increased and decreased with further increment of Ag. Similarly, Figure 4b and d shows the emission of Samarium with Au. The emissions at 645 nm(4G5/2 → 6H9/2), 566 and 602 nm (4G5/2 → 6H5/2 and 4G5/2 → 6H7/2) correspond to electric and magnetic dipole transitions respectively. In the inset of Figure 4b and d, we show the effect of silver concentration on different transitions.
The Ag NPs’ concentration dependence on the emission enhancement for Eu(TTFA)3 is shown in the inset of Figure 4a, where the normalized intensity is the intensity ratio of Eu(TTFA)3 solution containing Ag NPs to pure Eu(TTFA)3 solution for the 5D0 → 7F2 transition. The luminescence enhancement gets strongly affected by the Ag NPs concentration, the maximum enhancement factor was 23 at 70 μl Ag concentration. For 5D0 → 7F0 and 5D0 → 7F1, the enhancement factor was observed as 3. The luminescence enhancement is greater for electric dipole transitions than for magnetic dipole transitions, according to this. The hyper-sensitive transition is influenced by changes in the refractive index and ligand fields around rare-earth ions caused by interactions with metal NPs [44].
The emission of rare-earth ions near NSs are affected by the near-field environment, which induces enhancement or quenching relay on the distance between nanoparticles and rare-earth ions [45]. Rare-earth ions transfer non-radiative energy to metal particles through very low distances between NPs and molecules. Because of plasmonic resonances in metal NPs, magnetic field enhancement occurs only until a certain distance [46]. More Eu ions can be closer to NSs and the distance between Eu ions and Ag NPs can be reduced by increment in number of Ag NSs. With more NPs or reabsorption of SPR, the emission intensity is quenched by energy transmit between europium and NSs. The electric dipole transition (5D0 7F2) and magnetic dipole transitions (5D0 7F0 and 5D0 7F1), on the other hand, had distinct concentration dependence on luminescence intensities. The enhancement is considered to be caused to a hard coupling between SPR and probes. Figure 1 shows that the absorption spectra of Ag NPs are in the wavelength range of 350–600 nm, which corresponds to the absorption of rare-earth ions. The enhancement resulted from a sensitive balance between surface Plasmon resonance reabsorption and local electromagnetic (EM) field enhancement.
Figure 4e and g presents the emission of 20 μl europium with Au NSs and excited at 350 nm. The emission bands at 614 nm is 5D0 → 7F2 electric dipole and at 577 nm (5D0 → 7F0), and 590 nm (5D0 → 7F1) are magnetic dipole transitions. The dependency of emission of europium at 10, 20, 30 μl with gold at 5 to 300 μl is shown in the inset of Figure 4e and g. Similarly, Figure 4f and h displays the emission of samarium with Au NTs. The band at 645 nm (4G5/2 → 6H9/2) is an electric dipole and 566 nm (4G5/2 → 6H5/2) and 602 nm (4G5/2 → 6H7/2) are magnetic dipole transitions. In Figure 4e and g inset, emission of samarium 10, 20, 30 μl with Au at 5 to 300 μl is shown. The emission is quenched exponentially for Eu3+ at 10 and 30 μl and Sm3+ at 100 and 120 μl. The quenching is owing to the re-absorption of nanoparticles.
4.5 In vitro cytotoxicity
Green Ag and Au NTs were tested in MTT assays to see how they affected the growth of cancer cell lines. This is the first study to test the cytotoxicity of Ag NPs and Au NTs generated from
4.6 Antimicrobial studies
Figure 6 and Table 1 indicate the inhibitory effect of Ag and Au NSs derived from
Ag/Au NPs concentration (μl) | Zone of inhibition (cm) | ||
---|---|---|---|
P-Ag | 10 | 1.3 | 1.0 |
20 | 1.5 | 1.5 | |
30 | 1.8 | 2 | |
P-Au | 10 | 0 | 0 |
20 | 0 | 0 | |
30 | 0 | 0 | |
O-Ag | 10 | 2 | 1.8 |
20 | 2 | 2.2 | |
30 | 2.5 | 2.4 | |
O-Au | 10 | 0 | 0 |
20 | 0 | 0 | |
30 | 0 | 0 |
5. Conclusions
The effect of metal nanostructures on emission of rare-earth compounds is reported in brief research. The emission of rare-earth ions is increased initially, but then decreased when the Ag NPs concentration was increased further. The dependence of Ag NPs on emission intensity reveals a strong linkage of luminescence centers and Plasmon resonance of NSs, as well as reabsorption of SPR of Ag NPs. The anticancer and antibacterial properties of the nanoparticles were remarkable.
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