Paola
Gagni‡
a,
Alessandro
Romanato‡
a,
Greta
Bergamaschi‡
a,
Paolo
Bettotti
b,
Renzo
Vanna
c,
Chiara
Piotto
b,
Carlo F.
Morasso
c,
Marcella
Chiari
a,
Marina
Cretich
*a and
Alessandro
Gori
*a
aNational Research Council of Italy, Istituto di Chimica del Riconoscimento Molecolare (ICRM), Via Mario Bianco, 9, 20131-Milano, Italy. E-mail: alessandro.gori@icrm.cnr.it; marina.cretich@icrm.cnr.it
bNanoscience Laboratory, Department of Physics, University of Trento, Via Sommarive 14, 38123 Povo, Italy
cIstituti Clinici Scientifici Maugeri IRCCS, Via Maugeri 4, 27100, Pavia, Italy
First published on 22nd October 2018
Biosensing analytical platforms rely on the intimate structure–function relationship of immobilized probes. In this context, hydrogels are appealing semi-wet systems to locally confine biomolecules while preserving their structural integrity and function. Yet, limitations imposed by biomolecule diffusion rates or fabrication difficulties still hamper their broad application. Here, using a self-assembling peptide, a printable and self-adhesive hydrogel was obtained and applied to fabricate arrays of localized bio-functional 3D microenvironments on analytical interfaces. This soft matrix represents a robust and versatile material, allowing fast and selective tuning of analyte diffusion, which is exploited here to run in-gel immunoassays under solution-like conditions in an unprecedented (<10 min) time frame. The developed material overcomes major limitations associated with hydrogels for bioassays, widening the prospects for easy fabrication of multifunctional bio-interfaces for high-throughput, molecular recognition assays.
In recent years, self-assembling peptides have experienced widespread and different applications in nanoscience.28–32 The spontaneous bottom-up assembly of monomer peptide motifs can drive the formation of ordered supramolecular architectures in a tuneable and controlled manner, that can easily generate new functional soft materials, including peptide hydrogels.33–36 These materials are usually formed by entangled self-assembled nanofibers that bundle to form a stable network that entraps water within it. Ordered noncovalent interactions are the key driving force for the assembly process, and they can confer stunning robustness to these fibrillar nanostructures.37
In the present work, using micromolar concentrations of a self-assembling peptide we obtained a soft hydrogel matrix with controlled permeability properties for the straightforward confinement of biomolecular probes in arrayed 3D microenvironments. Using this strategy, we obtained a stable and yet highly permeable nano-scaffold that enabled us to run fluorescence immunoassays under solution-like conditions within an ultrashort timeframe (<10 min) and a pM detection limit. The supramolecular hydrogel forms rapidly and spontaneously, it is printable using a piezoelectric microarray spotter and it self-adheres onto poly(methyl methacrylate) (PMMA) slides, so that neither post-spotting cross-linking nor polymerization is required for gel formation and surface attachment, greatly simplifying the fabrication process. Overall, our platform is user-friendly, robust and cost-effective and possesses a combination of favorable features that are unique in the area of 3D multiplexed bioassays in hydrogels.
We tested our hypotheses in the fabrication of hydrogel microarrays using PMMA slides, a hydrophobic material that is widely used in Biological Micro-Electro-Mechanical Systems (BioMEMS).49 Upon preliminary screening of a set of Q11 analogues, we used a slightly modified Q11 sequence (Ac-YFQQKFQFQFEQQ-conh2, YF-Q11) that formed PMMA-adhesive soft hydrogels over a large micromolar concentration range (25–500 μM). Structural characterization of the new peptide by circular dichroism (CD) and ATR-FTIR analysis revealed that YF-Q11 preferentially shows a beta-sheet character (Fig. 2a–c and S2†), in accordance with the previously reported behaviour of the Q11 parent molecule.44 Spectrofluorimetric studies (Fig. 2b and S3†) using the hydrophobic fluorescent molecular probe 8-anilino-1-naphthalenesulfonic acid (ANS), widely used to sense micropolarity variation following the formation of supramolecular nanostructures, demonstrated that upon incubation at 40 °C the spontaneous assembly proceeds rapidly and reaches a stable level within a convenient operative time frame (1–4 hours).50,51 This behaviour was also observed using thioflavin (Fig. S4†). Atomic force microscopy (AFM) experiments were performed to confirm the presence of entangled fibrillar nanostructures responsible for hydrogel formation, which could be clearly detectable even at 25 μM concentration (Fig. 2d). Peptide chains hierarchically aggregate in fibrillary structures that, in turn, self-organize into larger micrometer sized bundle of fibers. The smallest detectable fibers were down to 1 nm in height (Fig. S1†), while the limited thickness of even the largest fibrils (about 10–30 nm) and their high aspect ratio are compatible with the typically observed structures assumed by the Q11 self-assembling peptide.45,52
Fig. 2 (a) CD spectra of 25 μM YF-Q11 in water upon incubation at 40 °C. Increasing traits of beta-sheet character are detectable over time. CD spectra at 50, 100 and 250 μM are reported in Fig. S2.† (b) Fluorescence spectra of ANS (1 μM) in water (red line) and in the presence of 250 μM YF-Q11 (blue and black lines) at different times (λex = 360 nm). The fluorescent signal rapidly appears and remains stable over time. (c) ATR-FTIR spectrum (dotted) and second derivative (solid). Major peaks at 1624 cm−1 and 1696 cm−1 indicate a predominant YF-Q11 beta-sheet character. A helical structure (1653 cm−1) is also present to a lower extent.53–55 (d) AFM representative image of 25 μM YF-Q11 showing the formation of entangled nanofibers. |
We then performed rheology characterization of the YF-Q11 hydrogel, showing that it behaves as a typical viscoelastic fluid under increasing strain excitation (Fig. 3a). The storage modulus (G′) remains constant up to approximately 0.4% strain when an oscillation at a constant frequency of 0.2 Hz is applied, after which it starts to decrease. Within such a range (LVER), changes to the gel microstructure are reversibly (instantaneously) recovered. The difference between the elastic and the viscous (G′′) modulus indicates that the peptide fibers are loosely connected. At larger shear strain, G′′ approaches G′ up to a point (at about 7%) at which the material behaves essentially like a liquid. These reduced interactions are confirmed by the limited viscosity of the material (Fig. 3b), which also displays shear-thinning properties, that make it compatible with robot-assisted spotting technology.
Fig. 3 (a) Measurement of the LVER (Linear Visco Elastic Region) for 250 μM YF-Q11. Oscillation amplitude table: frequency 0.2000 Hz, 1.000 × 10−4 Pa to 0.1000 Pa, 5 samples per decade. (b) Yield stress curve showing a decrease in viscosity starting at very low stress (around 0.02 Pa). This is indicative of the limited cohesive energy endowed by the material. Viscometry shear stress ramp: 0.000 Pa to 1.000 Pa, 500 samples, linear. (c) Drop shape analysis performed by contact angle measurements. YF-Q11 (25 μM) droplet volume observation by video capturing over three repeated drying/rehydration steps. (d) Sequential Raman images of two hydrogel drops (8 nL). Empty spot (left) and malachite-green labelled antibody containing spot (right) were acquired in parallel by a raster-scanning acquisition of the area of interest and by applying a 3 μm pitch in the Z direction. The false-color maps and intensities correspond to the presence of the typical Raman spectra of malachite-green used as a Raman label and automatically identified by direct classical least squares (DCLS) component analysis (see the ESI†). |
Interestingly, by visual inspection, spots produced by the arrayer rapidly dried out, but instantaneously rehydrated upon immersion in water regaining their 3D shape (Fig. S5†). To gain insight into this process, we used a drop shape analyser that allowed us to monitor microdroplet volume and to verify the full reversibility of this process (Fig. 3c). We confirmed that, upon an initial loss of hydrogel outer shell occurring within the first minute of incubation, microdroplets regain their initial volume over repeated cycles of drying and re-swelling. In this sense, the fibrillar matrix behaves like a supramolecular sponge.
The whole range of YF-Q11 hydrogel concentrations tested (25–500 μM) showed good stability over time. Indeed, after 10 min incubation in a typical wash buffer (0.05 M Tris/HCl pH 9, 0.25 M NaCl, 0.05% v/v Tween 20), spot fluorescence was basically unaltered (Fig. S6†). Biomolecule-containing spots behaved similarly to empty controls, suggesting that the YF-Q11 fibrillar network integrity is not affected by the nature of entrapped biomolecules, and that stability is preserved. After 60 minutes of washing, around 15% decay in the Cy3 signal was observed (Fig. S6†). However, this is largely outbalanced by the fact that complete biomolecule diffusion occurred in approximately 2 minutes (Fig. 4a). Notably, by using different YF-Q11 concentrations (i.e. varying the hydrogel microstructure), gel permeability can be selectively tuned to control differential analyte permeation and, under selected conditions, free and fast diffusion is allowed (Fig. 4). The V5 peptide was fully permeable at all tested concentrations, while streptavidin was entrapped in the 250–500 μM range but freely diffused below 100 μM. The same concentration allowed only for partial α-lactalbumin antibody diffusion, which was instead almost quantitative at 25 μM. These tuneable diffusion properties are likely related to the combined contribution of the hydrodynamic radii of the bioprobes and the occurrence of noncovalent interactions with the hydrogel matrix. When large molecules such as IgGs are confined within a relatively dense hydrogel microstructure, as seen at higher (>100 μM) YF-Q11 concentrations, probes are mostly retained. In contrast, the highly porous hydrogel microstructure at 25–50 μM YF-Q11 is ideal to avoid bioprobe entrapment due to nonspecific interactions, and to enable unimpaired diffusion. The simultaneous monitoring on the Cy3 channel allowed us to exclude a major contribution of hydrogel matrix disruption to the observed Cy5 fluorescence decrease.
Fig. 4 (a) Residual Cy5 fluorescence of hydrogel spotted labelled bioprobes upon increasing incubation time in 0.05 M Tris/HCl pH 9, 0.25 M NaCl, and 0.05% v/v Tween 20 buffer. Anti-LAC IgG (150 kDa; Rh = 5–6.5 nm, left) is mostly retained at >100 μM YF-Q11 hydrogel concentration, while almost complete signal loss indicates that it freely diffuses in the 25–50 μM range within 2 minutes. The hydrogel matrix is fully permeable to V5 peptide (2 kDa, right) over the entire range tested. Streptavidin (53 kDa, Rh = 2.5–3 nm, centre) shows intermediate properties, being residual fluorescence stable at >250 μM YF-Q11 hydrogel concentration. The Cy3 fluorescence channel was used to simultaneously monitor gel stability and exclude a major contribution of gel disruption to the observed Cy5 fluorescence decrease (Fig. S6†). (b) Graphical representation summary of hydrogel permeation to biomolecules. |
Overall, these experiments highlighted promising hydrogel features and, in view of real bioassays using complex samples, we verified that these properties were unaltered upon immersion of the slides into powdered skimmed milk prior to spotting, a common protocol used to block non-specific interactions of biomolecules that potentially occur on untreated PMMA surfaces.
To verify that the biomolecules are distributed in a 3D shell, confocal Raman imaging experiments were performed on an antibody-containing hydrogel. A malachite-labelled antibody was entrapped into a 250 μm YF-Q11 matrix and multiple images were directly captured in water using a 3 μm pitch in the Z direction (Fig. 3d and S7†). The results indicated that the labeled antibody was stably embedded in the hydrogel spots and uniformly distributed throughout the gel matrix, while the long acquisition time required for the experiment further supports hydrogel stability. As previously suggested by contact-angle experiments, the rendered images confirmed that spotted microdroplets assume a disc-like shape with a height of approximately 18 μm (8 nL spot, Fig. 3d). This is due to the low-viscosity properties of the hydrogel favoring spreading of the gel on the surface.
Fig. 5 (a and b) Histograms showing the fluorescence intensities detected in the Cy3 and Cy5 channels after 5 minutes incubation of hydrogel spots with the mixture of (a) Cy3-anti-V5 and Cy5-anti-LAC IgGs within the antibody-permeable matrix (25 μM YF-Q11) and (b) Cy3-V5 and Cy5-LAC peptides in the antibody-trapping 250 μM YF-Q11. Correctly, fluorescence is detected in the appropriate channel for the specific probe–antibody pair interaction; microarray scan images are reported on the right. Inappreciable signals detected in both experiments on the empty spots reveal the absence of fluorescence noise due to fluorophore interaction with the hydrogel matrix. (c) Dose–response curve to calculate the limit of detection using 20% Q11-V5 epitope. (d) Fluorescence signal and unpaired t test (p < 0.001) for two panels of 12 ZIKV+ individuals and 12 healthy controls screened for immunoreactivity on 20% ZEp1 co-assembled with YF-Q11. Experimental details are reported in the ESI.† |
The ultra-short antibody incubation time (5 minutes) used in the assay was optimized by following the kinetic curves for the saturation of the fluorescence signal of the V5-antibody pair. Comparison of the saturation kinetics profiles observed for the in-gel assay and on a flat surface confirms probe immobilization capacity within the 3D scaffold, as demonstrated by the higher fluorescence response (Fig. S8†). Antibody diffusion was not hindered by the soft peptide matrix, which conversely behaves as a solution-like environment. In addition, it allowed short incubation times, disfavoured nonspecific interactions and molecular adsorption on the surface, thus reducing the fluorescence background noise. Subsequently, in order to estimate the ideal probe content of hydrogels, we tested increasing amounts (from 0% to 50%) of co-assembled V5 epitope with 25 μM YF-Q11 and we calculated the LODs (limits of detection) for different concentrations (0 to 100 ng mL−1) of anti-V5 IgG spiked into human serum (Fig. S9†). The 20% V5 peptide content provided the lowest calculated LOD of 2 ng mL−1. The R2 (0.94) of the dose–response curve demonstrated the linearity of the assay outcome in a clinically relevant antibody concentration range (Fig. 5c).
As the final benchmark for our platform, we performed a real immunodiagnostic assay to detect Zika Virus (ZIKV) infection in human serum samples, using a previously described immunoreactive epitope (ZEp1) of ZIKV NS1 protein.60 Two panels of 12 ZIKV positive individuals and 12 healthy controls were screened for immunoreactivity against ZEp1 epitope and results were evaluated by an unpaired t test (Fig. 5d). Our test effectively enabled discrimination between the two populations at a statistically significant level (p < 0.001), confirming the feasibility of our system in the context of a real serological assay for infectious diseases. It is remarkable that the incubation times for ZEp1 recognition took less than 5 minutes, while the incubation time for the secondary antibody was 2 minutes. Overall, the total time required for the assay was <10 minutes.
Under selected conditions, biomolecule diffusion properties through the hydrogel matrix closely mimic solution conditions, so that ultrafast (<10 min) immunoassays, arguably one of the most challenging bioassay settings, can be run using this platform. This was demonstrated by running a real case diagnostic immunoassay for the detection of ZIKV infection. Importantly, the hydrogel matrix did not interfere with the molecular recognition properties of the entrapped probes, nor did it show nonspecific interactions in the presence of complex biological samples such as sera. Based on these results and given the unlimited opportunities for flexible molecular design of peptides, we envisage that analogous versatile peptide hydrogel platforms may find extensive applications as modular 3D microenvironments with solution-like properties in a wide range of automated and multiplex bio-assays, including lab-on-chip devices and cell-based biosensors.
Footnotes |
† Electronic supplementary information (ESI) available: Detailed procedures for the material synthesis, stability and biomolecule diffusion tests, and bioassays. See DOI: 10.1039/c8na00158h |
‡ These authors contributed equally. |
This journal is © The Royal Society of Chemistry 2019 |