Francesca
Petronella
*a,
Daniela
De Biase
b,
Federica
Zaccagnini
b,
Vanessa
Verrina
b,
Seok-In
Lim
c,
Kwang-Un
Jeong
c,
Selenia
Miglietta
d,
Vincenzo
Petrozza
b,
Viviana
Scognamiglio
a,
Nicholas P.
Godman
e,
Dean R.
Evans
e,
Michael
McConney
e and
Luciano
De Sio
*bf
aInstitute of Crystallography CNR-IC, National Research Council of Italy, Via Salaria Km 29,300, Monterotondo - Rome, Italy. E-mail: francesca.petronella@ic.cnr.it
bDepartment of Medico-Surgical Sciences and, Biotechnologies Sapienza University of Rome, Latina, Italy. E-mail: luciano.desio@uniroma1.it
cDepartment of Polymer-Nano Science and Technology, Department of Nano Convergence Engineering, Jeonbuk National University, Jeonju, Republic of Korea
dDepartment of Anatomy, Histology, Forensic Medicine and Orthopaedics, Sapienza University of Rome, Rome, Italy
eAir Force Research Laboratory, Materials and Manufacturing Directorate, Wright-Patterson Air Force Base, Ohio, 45433, USA
fCenter for Biophotonics Research, Department of Medico-Surgical Sciences and Biotechnologies, Sapienza University of Rome, Latina, Italy
First published on 12th August 2022
The growing spread of pathogens, caused by anthropogenic activities, pushes the interest of the scientific community towards developing biosensors with improved performance for rapid, simple, and on-site pathogen detection. In this study, we present and discuss a label-free gold nanorod (Au NR) array for the rapid detection of Escherichia coli cells in water, resulting in an effective optical transducer, based on the phenomenon of localized surface plasmon resonance (LSPR). Au NRs with different aspect ratios are functionalized with a suitable antibody by an electrostatic-linking method, resulting in two different Au NR-based bioconjugates. We investigate the ability of the two bioconjugates to detect and spectroscopically recognize E. coli cells dispersed in water by specific antigen–antibody interaction. The results allow selecting the Au NR morphology more suited for preparing the Au NR bioactive array on a glass substrate with excellent optical and morphological properties. The antibody-functionalized Au NR array can detect E. coli cells with high sensitivity and a limit of detection of 8.4 CFU mL−1, resulting in an excellent label-free spectroscopic biosensor. In addition, the multicolor thermoplasmonic properties of the Au NR array, triggered by appropriate light sources, are suited to enable on-demand photothermal disinfection, thus providing an extraordinary capacity for the biosensor to be both disinfected and, more importantly, reutilized.
Environmental significanceMicrobial contamination of water produces relevant human-health problems, spanning from infectious diseases to biosecurity. Currently available techniques for pathogen detection require a long workflow, specialized personnel, and considerable waste. This manuscript reports a breakthrough in monitoring microbial contamination by developing a fast, user-friendly, compact, and reusable in situ biosensor to detect pathogens in water. The nano-inspired device uses an antibody-functionalized Au NR array for identifying and quantifying Escherichia coli. It exhibits a limit of detection of 8.4 CFU mL−1, which turns out to be one order of magnitude lower than that of conventional plasmonic biosensors. In addition, the photothermal properties of the Au NR array are investigated to enable on-demand photothermal disinfection, thus providing reusability and sustainability. |
Biosensors are a promising tool to outclass conventional analytical techniques. They ensure constant monitoring and rapid response times, sensitivity, and selectivity and minimize sample pretreatment processes.8,10 Nanotechnology offers a ground-breaking toolbox for designing and fabricating miniaturized biosensors suitable for point of-care, end of-use, and sampling applications. Advanced nano-biosensor design and fabrication opportunities are offered by plasmonic gold nanoparticles (Au NPs).11 Au NPs exhibit optimal colloidal stability, effective interaction with biomolecules, easy processable surface chemistry, high electron density, and unique optical properties.12 The optical properties of Au NPs are associated with the localized surface plasmon resonance (LSPR) phenomenon, i.e., the collective oscillation of electrons localized at the metallic/dielectric interface produced by suitable light irradiation. The LSPR generates sharp and intense absorption peaks (plasmons) in the visible/near-infrared (NIR) range of the electromagnetic spectrum, whose frequency and profile are strongly dependent on the specific morphology and surface chemistry of Au NPs, described by the Mie and Gans theory.13,14 In addition, the LSPR frequency is susceptible to the local refractive index (n) change.15 Such a relation is the physical basis underlying LSPR biosensing, making Au NPs excellent optical transducers for monitoring the local change of the surrounding medium.15 The general scheme of Au NP-based LSPR biosensors consists of Au NPs appropriately functionalized with a biorecognition element, including antibodies, aptamers, peptides, DNA, and bacteriophages, resulting in a bioconjugate.16 In the presence of the specific target bio-entity, the biorecognition element triggers an interaction with the surface of Au NPs that alters the local n, thus inducing an optical shift (a change of the LSPR frequency) in the absorption spectrum of Au NPs.17 LSPR biosensors for spectroscopic recognition of pathogens can provide real-time, quantitative detection, with high sensitivity and selectivity, which makes them extremely appealing for developing early-warning, compact, and portable sensing platforms.15,17 However, a step forward is needed to realize functional Au NP arrays on substrates to be integrated into optical devices for the development of LSPR spectroscopic biosensors. Recently, Au NP arrays were employed for the optical detection of pathogens. Salmonella typhimurium was detected in food samples using an LSPR biosensor consisting of a monolayer of Au NPs self-assembled on a glass substrate and then functionalized with an aptamer.18S. typhimurium was also detected by an Ω-shaped fiber-optic LSPR biosensor, using an array of Au NPs functionalized with a suitable aptamer as an optical transducer.19 In a different approach, a fiber-optic functionalized with Au NPs was created to capture, recognize and quantify E. coli cells using a bacteriophage as a biorecognition element.20 An LSPR biosensor based on an array of Au NPs was also developed to monitor the kinetics of E. coli biofilm generation.21 Although robust and reliable, currently available LSPR biosensors, displaying a limit of detection (LOD) in a range from 102 and 104 CFU mL−1,18,19 are still unsuitable for real-time monitoring of pathogens in water. In light of WHO and European Union requirements, imposing no E. coli cells in 100 mL of water,22 more efforts are needed to design and realize LSPR biosensors with superior performance.
The present work tackles this challenge by designing and realizing a miniaturized, label-free, antibody-functionalized Au NR array on a glass substrate to rapidly detect E. coli cells in water with improved sensitivity. To accomplish the desired sensing performance, rod-like Au NPs (Au NRs) were selected as E. coli LSPR probes instead of the spherical Au NPs conventionally used to fabricate sensing platforms.
The anisotropic morphology of Au NRs results in an absorption spectrum characterized by two LSPR bands: the transverse plasmon (LSPRt) typically centered at 520 nm and the longitudinal plasmon (LSPRl), centered at higher wavelengths and tunable according to the Au NR aspect ratio. Remarkably, the LSPRl is more sensitive to n alterations with respect to the LSPRt;15 indeed, several Au NR bioconjugates were used in colloidal LSPR sensors for spectroscopic detection of pathogens.23–25 In this study a novel bioactive array of Au NRs with optimal optical and morphological properties for LSPR biosensing of a model pathogen, E. coli, was developed. As a first step, the biosensing performance of two bioconjugates prepared with Au NRs at different aspect ratios was investigated to determine the more effective Au NR morphology for E. coli LSPR biosensing. The two Au NR-based bioconjugates were functionalized with a suitable antibody (anti-E. coli Ab or Ab) able to target surface antigens of E. coli. The bioconjugation was realized by modifying an electrostatic linking method26–28 that allows promoting the electrostatic attractions between the Au NR surface and the anti-E. coli Ab by interposing a polyelectrolyte (PE) layer, namely a polymer carrying numerous charged (ionizable) groups, resulting in a polycation or a polyanion.28 The two bioconjugates were carefully characterized and their ability to spectroscopically recognize and quantify E. coli cells in water dispersions was investigated. Based on experimental results, the Au NR morphology more suited for preparing Au NR-based bioactive substrates was identified. The substrates were realized by exploiting the electrostatic layer-by-layer (LbL) assembly method,30,31 characterized both from an optical and a morphological point of view, (bio)activated by incorporating the anti-E. coli Abs by physisorption, and finally investigated for the recognition and quantification of E. coli cells dispersed in water. In addition, a multicolour thermoplasmonic investigation was performed to assess the capability of the substrates to be photothermally disinfected and reutilized.
Control experiments were performed applying the same protocol for pristine Au NR 660, Au NR 800, Au NR 660/PAH, and Au NR 800/PAH.
Finally, the substrate was washed three times with a 0.15 M NaCl solution (2 mL) to remove cells, rinsed with water, and dried under a nitrogen flow before collecting the absorption spectrum.
Au NR-based bioconjugates were obtained using the electrostatic linking method.26 This method simultaneously preserves two essential aspects for effective n sensing, i.e., the unique spectroscopic properties of Au NRs and the structure of the Ab as a probe molecule.
In contrast with conventional physisorption-based approaches, the electrostatic linking method promotes the interactions between the nanostructure surface and the biomolecules by interposing one or more layers of PEs covering the NP surface.26,27,37 Indeed, PEs provide a high density of charged groups accessible to polar functional groups of biomolecules to boost electrostatic attractions between the NP surface and the desired probe molecules.26,37,38
Although the electrostatic linking method provides limited control over Ab orientation at the NP surface,37 it has been extensively exploited for therapeutic and sensing purposes.32,38–40 Importantly, it can be regarded as a green approach for preparing bioconjugates because PEs are biocompatible functional materials,41,42 allowing the circumvention of health and environmental hazardous chemicals such as 1-ethyl-3-(3-dimethylaminopropyl)carbodiimide. Moreover, the electrostatic linking method offers several degrees of freedom to optimize bioconjugation, which include pH, ionic strength, number of PE layers, and PE, Ab and NP concentrations.27
Fig. 1a shows a schematic representation of the experimental approach for achieving the bioconjugation of Au NRs with the Ab by the electrostatic linking method. Essentially, a two-step preparation protocol was used: in the first step, Au NRs were functionalized with PAH molecules resulting in the Au NR/PAH complex that, once isolated by centrifugation, was incubated for 30 min in the presence of the Ab to promote the electrostatic attractions between the PAH and the Ab. The resulting Au NR/PAH/Ab bioconjugate was collected by centrifugation, diluted in water, and characterized by spectroscopic and morphological techniques.
The surface functionalization of Au NR 660 with PAH molecules produced the Au NR 660/PAH complex, whose absorption spectroscopic profile is very close to that of the pristine Au NR 660. Indeed, as reported in Fig. 1b, Au NR 660 shows an absorption spectrum characterized by two typical plasmon bands of elongated NPs: the LSPRl centered at 673 nm and the LSPRt at 512 nm. After the functionalization step, the resulting Au NR 660/PAH complex exhibited a red-shift of the LSPRl of 10 nm. In contrast, the position of the LSPRt remained almost unchanged as it is less sensitive to local n variation.13 Therefore, the 10 nm red-shift of the LSPRl band for the Au NR 660/PAH is associated with an increase of the local n,13 indicating the generation of a PAH monolayer on the Au NR 660 surface. The assembly of such a monolayer can be promoted by electrostatic attractions between the negatively charged carboxylic groups of citrate molecules surrounding the surface of Au NR 660 and the positively charged amine groups of the PE. Moreover, the spectroscopic profile suggested that the Au NR 660/PAH preserved the colloidal stability and the monodispersity of pristine Au NR 660, considering that the spectroscopic fingerprints of pristine Au NR 660, namely LSPRl and LSPRt, in the gray track of Fig. 1b, are well defined in the absorption spectrum of the Au NR 660/PAH complex (cyan track in Fig. 1b).
The absorption spectrum of the Au NR 660/PAH/Ab bioconjugate (green track in Fig. 1b) pointed to a further shift of about 22 nm (with respect to Au NR 660) for the LSPRl. The red-shift of the LSPRl, in agreement with the Gans theory,13 implies an alteration of the dielectric constant of the surrounding medium, clearly indicating the electrostatic accumulation of Ab molecules on the surface of the Au NR 660/PAH complex.
A photoluminescence (PL) spectroscopy investigation was carried out to assess whether, upon the bioconjugation by the electrostatic linking method, the Ab in the Au NR 660/PAH/Ab preserves its conformational stability and, therefore, its biological functions to recognize antigens on the E. coli cell's surface are preserved.
In particular, this investigation was performed by exciting the amino acid residues with intrinsic fluorescence, namely, phenylalanine (Phe), tyrosine (Tyr), and tryptophan (Trp), whose PL spectrum is sensitive to alterations of the secondary and tertiary structure, especially for Trp.43 The characterization of the Au NR 660/PAH/Ab bioconjugate by PL spectroscopy is shown in Fig. 1c and d. Fig. 1c shows the PL spectra of the Au NR 660/PAH/Ab collected by exciting the bioconjugate at 256 nm to analyze the emission from Phe, at 280 nm to evaluate the emission from Tyr and Trp, and at 295 nm to selectively measure the emission from Trp. The PL spectra clearly show the typical emission signals associated with Phe, Tyr, and Trp residues. In particular, by exciting the sample at 280 nm, an intense and broad emission band associated with Tyr and Trp appeared. The photoluminescence spectra in Fig. 1d were collected by selectively exciting the Tyr and Trp residues, both for the Au NR 660/PAH/Ab (black track) and for the free Ab (blue track), respectively. By exciting the Au NR 660/PAH/Ab bioconjugate at 280 nm, a blue shift of the emission, from 341 nm (for the free Ab) to 336 nm (for the Au NR 660/PAH/Ab bioconjugate) was measured (Fig. 1d). The observed blue shift indicates that the Tyr and Trp groups within the Au NR 660/PAH/Ab bioconjugate are less exposed to the solvent than the Tyr and Trp residues in the free Ab.43 Accordingly, Tyr and Trp residues may play a relevant role in achieving the electrostatic binding between Au NR 660/PAH and the Ab. We can infer that Tyr and Trp residues can promote electrostatic attractions involving the positively charged PAH amine groups and the hydroxyl groups carried on the benzene ring of Tyr as well as π-interactions involving the aromatic rings of Tyr and Trp.
The morphological analysis of the bioconjugate Au NR 660/PAH/Ab, carried out by TEM, is reported in Fig. 1e. The Au NR 660/PAH/Ab bioconjugate (Fig. 1e) is characterized by an outer surface layer (5–7 nm) with higher contrast to the micrograph background. The formation of the “corona layer” highlighted in Fig. 1e has been very often reported in the literature as proof of an effective NP surface functionalization with high molecular weight compounds,44,45 thus indicating the formation of an antibody layer on the Au NR 660/PAH NPs' surface.
The spectroscopic and morphologic characterization of the Au NR 800/PAH/Ab bioconjugate is reported in Fig. 1f. The wrapping with the PAH layer shifted the position of the LSPRl of Au NR 800 from 790 nm (Fig. 1f, magenta track) to 794 nm (Fig. 1f, green track). After the bioconjugation process occurred, the LSPRl was centered at 838 nm, with an overall red-shift of 48 nm (Fig. 1f, red track). Such a plasmonic red-shift, more intense than the one obtained for the Au NR 660/PAH/Ab bioconjugate (22 nm), accounts for the higher sensitivity to n changes, confirming the strong correlation between the aspect ratio of Au NRs and their n sensitivity.13
Moreover, in the red track of Fig. 1f, the increase of the absorption intensity at lower wavelengths can be associated with the presence of the Ab molecules linked to the Au NR 800/PAH surface.16
The analysis of the conformational stability of the Ab in the Au NR 800/PAH/Ab bioconjugate, carried out by PL spectroscopy, is shown in Fig. 1g and h. On exciting the bioconjugate at 256 nm, 280 nm, and 295 nm, the emission bands of Phe, Tyr/Trp, and Trp, respectively, were detected (Fig. 1g). The PL spectra in Fig. 1h were collected by selectively exciting the Tyr and Trp residues, both for the Au NR 800/PAH/Ab and the free Ab.
Experimental results point out that the emission peak position moved from 340 nm (for the free Ab) to 337 nm for Au NR 800/PAH/Ab. Likewise, for the Au NR 660/PAH/Ab, such a result indicates that the binding between the Au NR 800/PAH and the Ab could involve the hydroxyl groups carried on Tyr and aromatic moieties of Tyr and Trp that induce π-interactions. The TEM analysis of the Au NR 800/PAH/Ab bioconjugate reported in Fig. 1i highlighted the occurrence of high aspect ratio Au NRs. Moreover, also Au NR 800/PAH/Ab bioconjugates are characterized by a “corona layer” associated with the presence of the Ab assembled on the Au NR 800/PAH surface, as previously reported for Au NR 660/PAH/Ab.
The characterization techniques demonstrated the electrostatic linking method's effectiveness in producing Au NR-based bioconjugates with properties suitable for LSPR biosensing applications in terms of spectroscopic, colloidal, and structural features. Accordingly, a simple assay in a water dispersion was carried out to assess the LSPR biosensing properties of the Au NR-based bioconjugates. In particular, the assay examined the ability of the bioconjugates to produce spectroscopic response upon recognition of E. coli cells.
After the preparation step, the dispersions of both the bioconjugates were suitably diluted to achieve the same absorption intensity for the LSPRl (0.5 absorption units). After that, aliquots of E. coli cells from a 103 CFU mL−1 water dispersion were sequentially added to the bioconjugate dispersions. The absorption spectrum was collected after keeping the mixture under vigorous stirring for 10 min. The total volume of E. coli cells produced a 10% increase of the total volume of the dispersion, resulting in a minor experimental error on the concentration of the bioconjugate at the end of the experiment.
Experimental results reported in Fig. 2a depict that both LSPRt and LSPRl of Au NR 660/PAH/Ab are detectable regardless of the E. coli cell concentration. The concentration range of E. coli examined in this assay (from 4 to 70 CFU mL−1) did not produce Au NR aggregation, as the presence of aggregates would cause a broadening and a significant shift (greater than 200 nm (ref. 46)) of the plasmon bands. Fig. 2b highlights how the LSPRl of the Au NR 660/PAH/Ab is progressively red-shifted as the concentration of E. coli cells increased from 1 nm at 8 CFU mL−1 to 4 nm at 70 CFU mL−1. Fig. 2c clearly shows that also Au NR 800/PAH/Ab maintains unaltered its spectroscopic features (for both LSPRt and LSPRl bands) despite the progressive increase of the E. coli concentration. However, it is worth noting the occurrence (Fig. 2d) of an evident and gradual red-shift of the LSPRl of Au NR 800/PAH/Ab in the range from 5 nm (at 4 CFU mL−1) to 16 nm (at 70 CFU mL−1).
The LSPRl position is considered a sensing parameter because this plasmonic mode is more sensitive to n variations.15Fig. 2b–d highlight that the progressive increase of E. coli cell concentration produces a shift of the corresponding LSPRl band towards higher wavelength values for both the bioconjugates. This behavior is associated with the gradual increase of the surrounding n, associated with the gradual increase of E. coli cell amount, induced by the presence of the Ab on the Au NR.
The Ab loaded on the Au NR surface effectively promotes the accumulation of Au NR-based bioconjugates on the bacterial surface through the univocal and selective antigen–Ab recognition, as sketched in Fig. 2e.
Still, instead, it is preferentially promoted by the univocal antigen/antibody recognition occurring on the proximity of the Au NR surface. According to the reported experimental data in Fig. 2a–d, the spectroscopic behaviour of both Au NR 660/PAH/Ab and Au NR 800/PAH/Ab in the presence of E. coli cells highlighted the ability of the bioconjugates to recognize E. coli cells and produce a spectroscopic response consistent with the bacterial concentration. As demonstrated by experimental data, the measured red-shift is proportional to the bacterial loading, as shown by similar studies.23,46
The plot in Fig. 2f aims at comparing the sensing performance of the Au NR 660/PAH/Ab and Au NR 800/PAH/Ab bioconjugates by reporting the respective Δλ (defined as the optical shift of the LSPRl of each bioconjugate after the stepwise introduction of an E. coli aliquot) as a function of the E. coli cell concentration.
Although both the bioconjugates were able to produce a spectroscopic response concomitant with the increase of E. coli cell amount, Fig. 2f highlights a superior sensing performance of Au NR 800/PAH/Ab to that of Au NR 660/PAH/Ab.
As such, in all the investigated concentration ranges, the Δλ values produced by Au NR 800/PAH/Ab were higher than the ones measured for Au NR 660/PAH/Ab.
As an example, an E. coli loading of 16 CFU mL−1 determined a Δλ of 11 nm for Au NR 800/PAH/Ab and a Δλ of 3 nm for Au NR 660/PAH/Ab. Moreover, the Au NR 800/PAH/Ab bioconjugate was able to detect also a lower concentration of E. coli cells. Indeed, a concentration of 4 CFU mL−1 did not affect the position of the LSPRl of Au NR 660/PAH/Ab but shifted with a Δλ of 5 nm the LSPRl of the Au NR 800/PAH/Ab bioconjugate. Both the curves of Δλ values as a function of E. coli concentration showed an initial increase of Δλ, followed by a plateau for E. coli concentration values above 24 CFU mL−1. To better investigate the sensing ability of the bioconjugates Au NR 660/PAH/Ab and Au NR 800/PAH/Ab, the experimental points of Fig. 2f were interpolated using a four-parameter logistic equation47,48 from the software OriginPro 2020 (logistic fit function), resulting in eqn (1).
(1) |
Furthermore, the p value calculated for the assay carried out in the presence of Au NR 660/PAH/Ab is 2.56 ± 0.64, while the p value obtained from the interpolation of the results from Au NR 800/PAH/Ab is 1.04 ± 0.21. This difference indicates a progressive decrease in the affinity between the bioconjugate and the E. coli antigens with the increase of the cell concentration. Such a negatively cooperating binding appeared less intense for the Au NR 800/PAH/Ab bioconjugate. Moreover, it was possible to estimate a LOD (corresponding to the IC10 value calculated from the four-parameter logistic curve fit)48 of 5.07 CFU mL−1 for Au NR 660/PAH/Ab and a LOD of 1.4 CFU mL−1 for Au NR 800/PAH/Ab. The ensemble of the experimental results pointed out the superior sensing performance of the Au NR 800/PAH/Ab bioconjugate to that of the Au NR 660/PAH/Ab bioconjugate under the investigated experimental conditions. Indeed, based on interpolation results, for the same E. coli cell concentration, the Au NR 800/PAH/Ab bioconjugate produced higher values of Δλ. Accordingly, Au NR 800 NPs were selected as plasmonic NPs to fabricate an LSPR biosensor on rigid substrates.
The electrostatic layer-by-layer (LbL) assembly technique was here employed as a suitable and well-established fabrication approach to obtain the desired morphological and optical features.32,51–53
As shown in Fig. 3a, the modification of the glass substrate was realized by depositing a PE multilayer with the sequence PAH/PSS/PAH.
The sequential alternation of a weak positively charged PE (PAH) and a strong negatively charged PE (PSS) minimizes PE interdiffusion and provides a more uniform surface charge density that cannot be obtained from utilizing a monolayer.54,55 An even distribution of surface charges results in uniform distribution of the Au NR 800, promoted by the electrostatic attractions between PAH and the carboxylic groups exposed on the Au NR surface. Moreover, previous investigations demonstrated that PAH, having a chemical structure characterized by a linear backbone, can facilitate the generation of a uniform Au NR layer of isolated NPs, thus obtaining the features of a monodisperse colloidal dispersion on a solid support.32,56
After building the PE multilayer, the incorporation of Au NR 800 was realized by immersing the PE-modified glass substrate in an Au NR colloidal dispersion for 16 h, thus achieving a homogeneous substrate with a uniform pink tone, indicating the loading of Au NRs (inset of Fig. 4a).
The morphological characterization performed by atomic force microscopy (AFM) (Fig. 3b–d) and SEM (Fig. 3e) depicts the presence of a uniform Au NR 800 layer over a large area (1 cm2). Indeed, the topographic investigation shows asperities of anisotropic shape, with an even distribution over the investigated area of 1 μm × 1 μm. Interestingly, the analysis of the height profile results in an average value of 10 nm (Fig. 3d), in agreement with the dimension of the short side of Au NR 800 measured by TEM (Fig. 1f).
Such a result supports the occurrence of an Au NR monolayer on the substrate. It is strongly consistent with the SEM analysis (Fig. 3f) reporting the presence of individual Au NRs separated from each other and the absence of aggregates. The statistical analysis performed on SEM micrographs reveals that the Au NR 800 on substrates possess a fill fraction of 5.9% ± 0.2% along with an interparticle distance of 142 ± 50 nm and a density of about 215 Au NRs per μm2.
As reported in Fig. 4a (magenta track), the spectral analysis of the realized sample clearly shows two spectroscopic fingerprints of Au NRs, i.e., the LSPRt centered at 514 nm and the LSPRl centered at 756 nm. The LSPRl of the Au NR 800-functionalized substrate is 34 nm blue-shifted to the Au NR 800 colloidal dispersion, in agreement with previously reported results.56,57 In addition, the observed blue-shift is promoted by the change (decrease) of the n of the chemical medium surrounding13 the Au NR 800 that changed from water (n = 1.33) to air (n = 1).20
It is noteworthy that the spectral response of the Au NR 800-functionalized substrate (Fig. 4a, magenta curve) did not show any visible absorption signal in the long NIR range, suggesting that due to relatively long distances among the immobilized nano-objects, the multipolar couplings among surface plasmon resonances are minimized.56,58
The absorption spectra of ten different Au NR-modified glass samples (Fig. 4b), fabricated by reproducing the same protocol, demonstrated the repeatability of the fabrication process.
As shown in Fig. 4b, the ten spectral profiles almost overlap; moreover, the LSPRl position is distributed around the mean value of 752 nm ± 8 nm (Fig. 4c), while according to experimental data reported in Fig. 4d, the mean value of the FWHM is 145 ± 18 nm. The two standard deviation values suggested that the adopted protocol is suitable for the large-scale production of Au NR-modified glass substrates with excellent reproducibility.
Using Au NR 800-functionalized substrates as rigid platforms, we fabricated glass cells (Fig. 4e) that were subsequently infiltrated with several media possessing different n (Table S2 in ESI†) to quantify, by absorption spectroscopy, the n bulk sensitivity of randomly immobilized Au NR 800.
The absorption spectra reported in Fig. 4f, beyond showing the interference fringes59 accounting for the micrometer size gap between the Au NR 800 substrate and the glass cover, point out a gradual red-shift (Δλ) of both LSPRt and LSPRl of Au NRs with the increase of the n of the infiltrating medium.
The resulting Δλ measured at the plasmon band positions of the empty cells are reported as a function of n values in Fig. 4f. Following theoretical predictions focusing on colloidal dispersions of Au NRs, experimental results highlight a linear correlation between the n of the infiltrating medium and the Δλ (ref. 14) on a rigid substrate. In particular, a bulk sensitivity (S)60 of 456 nm per refractive index unit (RIU) and a figure of merit (evaluated as S/FWHM)60 of 3.1 were calculated for the LSPRl.
The morphological and optical investigation of Au NR 800-functionalized substrates and a stability test reported in Fig. SI3† highlighted that the immobilization approach was suitable for achieving the desired properties as an LSPR-based biosensor.
Indeed, the topographic, morphological, and optical investigation pointed out the occurrence of a uniform layer of a Au NR 800 array. In this array, Au NR 800 appeared as individual nano-objects, and hence their exposed surface available for interaction with the biorecognition element and the analyte is maximized, resulting in high-quality sensing performance.28,29 Indeed, the S value refereed to the LSPRl was calculated to be higher than previously reported results for analogous plasmonic-based platforms.21,57,61
The Ab promotes the confinement of E. coli cells on the Au NR 800 array through the univocal antigen–antibody recognition that alters the n experienced by the immobilized Au NR 800. As a result, the recognition mechanism triggers a plasmonic-based color change, similar to the previously demonstrated water dispersions (Fig. 2).
Fig. 5a shows a schematic of the incorporation of the Ab on the Au NR 800 array. However, the Ab's incorporation can also be promoted by the electrostatic interactions between the PAH layer underlying Au NRs, which covers about 94% of the surface, and the negatively charged functional groups of the Ab. The absorption spectra (Fig. 5b) point out a 40 nm red-shift of the LSPRl of the substrate following the Ab physisorption step, thus indicating the accomplishment of Ab incorporation.
The ability of the resulting substrates to attract and recognize E. coli cells at different concentration levels was investigated by performing microscopy and spectroscopy analysis. To this end, the bioactive substrates were incubated for 30 min in E. coli dispersions at several concentrations ranging from 10 CFU mL−1 to 104 CFU mL−1, washed, dried, and finally characterized. Experimental data from substrate characterization are reported in Fig. 6, showing, for each bioactive substrate, the contrast phase images, the corresponding fluorescence microscopy images, and the absorption spectroscopy investigation.
The contrast phase images in Fig. 6(a, d, g, and j) display bright spots (red circles) of elongated shape, showing an average length of 1.9 ± 0.2 μm that can be associated with E. coli cells accumulated on the bioactive substrates. The corresponding fluorescence microscopy images in Fig. 6(b, e, h, and k) highlight the presence of progressively increasing green spots (red circles) uniformly distributed on the surface of the biofunctionalized plasmonic substrates. They are associated with E. coli cells stained by the SYTO 9™ fluorescent dye. The number of the E. coli cells captured by each substrate, according to the scheme reported in Fig. 7a, was estimated from fluorescence microscopy images (using ImageJ microscopy software) by counting cells in a region of interest of 90000 μm2. As a result, despite the washing procedure, the number of E. coli cells deposited on each bioactive plasmonic substrate increased with the increase of E. coli cell concentration in the respective dispersion (as reported in Fig. SI4†), thus demonstrating the ability of the bioactive substrates to capture E. coli cells and to accumulate several bacteria proportional to the utilized E. coli cell concentration (Fig. SI4†). In contrast, only a few green spots were observed for the Au NR 800 substrate without bioactivation, as reported in the control experiments (Fig. SI5b†). Subsequently, to assess whether the accumulation of E. coli cells can also produce a spectroscopic response, the absorption spectra of the active Au NR 800-modified substrates were collected and reported in Fig. 6c, f, i, and l. They show the absorption spectra of:
1. The Au NR 800-functionalized glass substrate (red tracks).
2. The bioactive substrates after incorporating the Ab (yellow tracks).
3. The bioactive substrates after the incubation in E. coli dispersions at different bacterial concentrations (green tracks).
The green curves (Fig. 6c, f, i, and l) exhibit an absorption signal between 400 nm and 500 nm, associated with SYTO 9™ molecules that bind to E. coli DNA. It is noteworthy that the LSPRl of each Au NRs800/Ab substrate shifted toward higher wavelengths following the incubation in the E. coli dispersion. In particular, the 10 CFU mL−1 dispersion resulted in a red-shift of 21 nm, while 102 CFU mL−1, 103 CFU mL−1, and 104 CFU mL−1 dispersions produced a red-shift of 14 nm, 5 nm, and 3 nm, respectively.
Hence, the sensitivity of Au NR 800/Ab decreases as the E. coli concentration increases. To explain this behaviour, different from the results illustrated in Fig. 2f, it is worth considering the complexity of the phenomena occurring at the solid/liquid interfaces.
Under the investigated experimental conditions, the E. coli cells accumulate on the Au NR 800/Ab substrates by a diffusion-driven process. Due to the biofunctionalization, the cells progressively layer Au NR 800/Ab substrates in an amount proportional to the cells' concentration for each dispersion (see Fig. SI4†). As a consequence of the increase in the thickness of the material, over-layering the array of Au NRs produced a decrease in electric field intensity that reduces LSPR sensitivity occurring at higher E. coli concentrations.62,63
Indeed, the sensitivity of Au NR arrays is affected by the distance from the Au NR surface.64,65 Moreover, the E. coli cells progressively occupy the Au NR 800/Ab surface sites available for antigen–Ab recognition, thus reducing the sensitivity as the E. coli concentration increases, accounting for the decrease of Δλ values.
Furthermore, by plotting the resulting Δλ values as a function of the E. coli cell concentration (Fig. 7b), it was possible to determine a linear correlation that allowed us to estimate a LOD33,34 of 8.4 CFU mL−1.
Notably, the decrease in sensitivity with the increase of the E. coli concentration was also evidenced in control experiments performed without STYO 9™ molecules. Experimental results reported in Fig. SI6† highlighted the efficiency of the bioactive substrates to respond even at very low CFU mL−1.
For instance, the immersion in the 10 CFU mL−1E. coli dispersion produced a Δλ of 34 nm (Fig. SI6a†). Moreover, the linear fit resulting from plotting the Δλ as a function of E. coli concentration allowed us to estimate a LOD of 8.7 CFU mL−1 and a sensitivity66 of 9.5 nm mL CFU−1 (Fig. 7c).
Further control experiments were performed to clarify the effect of SYTO 9™ molecules, which plays the twofold role of (i) demonstrating that the spectroscopic shifts are a consequence of a biorecognition event and (ii) enabling a cross-check on the presence of E. coli on the Au NRs/800 Ab substrate.
Experimental results reported in Fig. SI7a and b† demonstrated that in the absence of E. coli cells, the SYTO 9™ molecules determined a red-shift of the LSPRl. Moreover, the comparison between the data reported in Fig. 7b and c indicated that the SYTO 9™ molecules show the drawback of behaving as a passivation layer, thus limiting the sensitivity of the bioactive substrates.
It is noteworthy that the proposed LSPR biosensor displayed higher values of the LSPRl shifts for the lower concentration of bacteria. The Au NR 800/Ab-based biosensor even demonstrated a 1.5 times higher sensitivity in the absence of the fluorescent dye, thus revealing a highly efficient label-free nanoplatform for detecting E. coli at low concentrations. Remarkably, it showed a LOD lower than that of previously reported LSPR biosensors based on immobilized plasmonic NPs.18–20
In addition, we performed a specificity experiment by testing the optical response of the Au NR 800/Ab substrates in the presence of another coliform: the Salmonella enterica serovar Typhimurium LT2. Experimental results reported in Fig. SI8† demonstrate that the S. Thyphimurium did not alter the LSPRl position of Au NR 800/Ab, thus providing conclusive evidence of the high specificity of the biofunctionalized Au NR 800/Ab substrates.
The photothermal performance of the functionalized substrates was investigated with a two-color optical setup, as described in Fig. 8a.
It allows the investigation of the thermoplasmonic properties using a CW laser beam emitting at 532 nm (green laser) and 808 nm (NIR laser) that selectively excite LSPRt and LSPRl modes, respectively.
The two-color optical setup allows mimicking a solar-light disinfection process or better said a broadband photothermal disinfection process. The light-to-heat conversion efficiency was measured by a thermal camera that provides thermographic images that are reported in Fig. 8b and c for the green and the NIR laser, respectively.
From the analysis of thermographic images collected during the irradiation time, a plot reporting the maximum temperature increase (ΔTmax) as a function of irradiation time was obtained (time–temperature profiles), as shown in Fig. 8d and e.
In particular, the time–temperature profiles were collected at different light intensities (power densities) in the range from 4.3 W cm−2 to 25.7 W cm−2 for the green laser (Fig. 8d) and from 5 W cm−2 to 29 W cm−2 for the NIR laser (Fig. 8e). Fig. 8d and e show that under laser irradiation, irrespective of the light intensity, the samples promoted a progressive temperature increase for 2 min followed by gradual cooling, which occurred when the laser sources were turned off.
For both the light sources, as shown in Fig. 8f and g, the ΔTmax values increased linearly with the power intensity of the laser beam, in agreement with theoretical models.67 Notably, at a comparable power density, a different value of ΔTmax was achieved according to the laser source. Indeed, the irradiation with the green laser with a power density of 12.9 W cm−2 produced a ΔTmax of 5.6 °C, while setting the NIR laser at a similar intensity value (10 W cm−2) gave a ΔTmax of 11.6 °C. On increasing the light intensity of the green laser at 25.7 W cm−2, the ΔTmax rose at 11.1 °C, while at the intensity of 25 W cm−2, the 2 min irradiation with the NIR laser generated a ΔTmax of 30.3 °C. Such results accounted for the higher photo-thermal efficiency of the LSPRl (excited with the NIR laser) than that of the LSPRt (excited with the green laser).
The excellent ability of Au NR 800 substrates to behave as photothermal transducers68 is here highly advantageous considering that under the investigated experimental parameters it was possible to achieve with the NIR laser at 29 W cm−2 a maximum temperature value of 53.8 °C that is sufficient to produce a decrease of E. coli cell viability as demonstrated by a previous investigation.69
Accordingly, these experimental conditions were employed to assess the ability of the Au NR 800/Ab substrates to perform photothermal disinfection. To this end, the Au NR 800/Ab sample (Fig. 9a, track 2) was incubated for 20 min in a 103 CFU mL−1E. coli dispersion. After the washing and the drying steps, the absorption spectrum was recorded (Fig. 9a, track 3). As expected, a red-shift of 13 nm was measured. The photothermal disinfection experiment was performed following the procedure reported in the “Multicolor photothermal measurements” section, while the utilized optical setup is shown in Fig. 8a. The Au NR 800/Ab sample incubated with E. coli dispersion was irradiated for 2 min at 808 nm with the CW laser at a power density of 29 W cm−2, thus reaching a maximum temperature of 54 °C. Subsequently, a solution containing 2 μL of propidium iodide was introduced, and the sample was left to incubate for 10 min in the dark, with an additional washing and drying step.
Subsequently, the sample was analysed by fluorescence microscopy. The microscopy analysis reported in Fig. 9b shows red spots of elongated shape uniformly distributed on the surface of the biofunctionalized plasmonic substrate. These are associated with dead E. coli cells stained by propidium iodide. Accordingly, we can assert that the investigated experimental conditions are suitable for achieving photothermal disinfection. However, as reported in track 4 of Fig. 9a, the photothermal disinfection step determined a blue shift of 4 nm of the LSPRl without altering the absorption spectrum profile. At this stage, the substrate was washed three times with a NaCl solution to remove cells, rinsed with water, and dried under a nitrogen flow before collecting the absorption spectrum. The result, reported in track 5 of Fig. 9a, shows that the spectroscopic profile of the substrate (presence of the two LSPR bands, absorption intensity ratio between the two LSPRs and FWMH) remained unaltered after the entire procedure. Remarkably, track 5 of Fig. 9a overlaps track 2 of Fig. 9a, namely the absorption spectrum of the as-prepared Au NR 800/Ab substrate. These additional experiments pointed out that the photothermal heating conditions are suitable to induce E. coli cell killing and that the substrate is ready to be reused for other experiments.
Therefore, the ability of the Au NR800/Ab substrates to suppress the detected bacteria accumulated on the active surface can prevent the undesired release of pathogens in the environment, thus preventing unintentional pollution. Moreover, a suitable washing procedure enables the reuse of the functionalized substrate, thus reducing the costs associated with its production and making the proposed biosensor sustainable from both an environmental and an economic standpoint.
Sensing experiments performed on S. Thyphimurium evidenced the biosensor specificity. Furthermore, the Au NR array can generate a broadband thermoplasmonic heating sufficient for inducing the inactivation of E. coli cells. After the photothermal disinfection step and a suitable washing procedure, the Au NR 800/Ab substrate is ready to be reused for other experiments. Therefore, the proposed Au NR array offers a green and sustainable perspective for developing next-generation biosensors beyond the biosensing effectiveness. Indeed, the preparation protocol does not require hazardous chemicals, the undesired release of pathogens is avoided, and the Au NR array can be reused, thus representing an outstanding solution regarding environmental impact and solar light-based applications.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d2en00564f |
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