Teresa
Bosch-Tamayo
,
Tamara M.
Iakimova
,
Amy Q.
Shen
* and
Mark V.
Sullivan
*
Micro/Bio/Nanofluidics Unit, Okinawa Institute of Science and Technology Graduate University, 1919-1 Tancha, Onna-son, Okinawa 904-0495, Japan. E-mail: mark.sullivan@oist.jp
First published on 31st October 2025
Molecularly imprinted polymer nanoparticles (nanoMIPs) represent a promising class of synthetic recognition elements with growing potential as robust alternatives to antibodies in diagnostic and sensing technologies. Despite widespread use, limited attention has been given to how solid-phase synthesis parameters, particularly the nature of the solid support and template identity, affect nanoMIP composition and function. Herein, we present a systematic investigation comparing popular glass bead and magnetic nanoparticle solid-phase protocols for nanoMIP synthesis targeting protein templates bovine haemoglobin (BHb) and bovine serum albumin (BSA). Using an identical functional monomer feed and surface plasmon resonance (SPR)-based affinity assays, we demonstrate that the choice of solid-phase significantly influences particle size, yield, and binding affinity, with nanoMIPs synthesized on glass beads exhibiting up to a tenfold enhancement in binding performance compared to those produced on magnetic nanoparticles. Furthermore, 1H NMR analysis reveals substantial deviations between initial monomer feed ratios and final polymer compositions, with polymer structure being highly dependent on both the solid phase and template characteristics. These findings highlight the importance of rational nanoMIP design, by challenging assumptions of uniform polymer composition and revealing how template and solid-phase interactions shape material properties. Our work establishes a framework for engineering high-performance synthetic receptors with tuneable properties and offers key insights for the optimisation of nanoMIP-based applications and sets new benchmarks for material consistency, reproducibility, and potential commercialisation.
Antibodies are probably the most used natural recognition materials and are particularly used in medical diagnostics, especially in biosensors, lateral flow tests, and biochemical assays for disease diagnostics and monitoring.10–12 This is due to their long-standing reputation for a high degree of recognition and specificity towards a chosen target. This means that numerous standardized protocols have already been established for the production and application of antibodies in medical diagnostics.13 For all their success, antibodies can have issues particularly around their stability and long-term usability.13 Antibodies are Y-shaped proteins, which means they are susceptible to denaturation from the effects of UV light exposure, high temperature, and high/low pH, thus significantly affecting their performance.14,15 This has resulted in the search for more stable synthetic alternatives.
Molecularly imprinted polymers (MIPs) are a class of synthetic recognition materials that are often touted as a viable alternative to antibodies and have found success in the areas of biosensing and diagnostics.16 MIPs are generally produced using a self-assembly methodology, whereby a series of functional monomers are mixed with a template (target of choice) and allowed to preassemble, thereby forming a favourable complex. The monomers are then linked together with a suitable crosslinker, typically via free radical polymerisation.17 While the MIPs synthesized through conventional methods offered an acceptable level of performance, the development of molecularly imprinted nanoparticles (nanoMIPs), additionally being more suited for solid-phase extraction and chromatography,18 have drastically increased the success and versatility of these synthetic recognition materials.19,20 While there are multiple ways to produce MIP nanoparticles, e.g., via core–shell,21 precipitation,22 electrochemical23 and emulsion polymerisation,24 the use of a solid-phase synthesis has gained prominence due to its ability to yield uniform and high-affinity particles.
The solid-phase protocol for nanoMIP production involves the immobilisation of the template/target molecule onto a solid support before polymerisation and because of polymerization reactions around the template/target molecule, subsequent nanoMIP is produced.25 Immobilisation of the template onto a solid support allows for a directional template, thus offering more control over the production of the imprinted binding cavities. This provides more uniform binding sites and the potential for 1
:
1 binding kinetics with higher performance. Additionally, the solid phase serves as a means for MIP/template separation method, allowing for the template to be easily removed from a high affinity nanoMIP. Magnetic nanoparticles and glass bead microparticles are the most used solid support, as they are easily functionalised with amino/carboxy silanes. This enables the use of a range of coupling chemistry (EDC/NHS, succinimidyl iodoacetate, glutaraldehyde) thus a variety of templates (small molecules, peptides and proteins) with bearing different functionality (carboxyl, thiol, or amino groups) are easily immobilised. The overall process is illustrated in Fig. 1, which schematically depicts key stages of solid-phase nanoMIP synthesis.
The nanoMIPs synthesized via this solid-phase approach typically incorporate acrylamide and acrylic acid-based monomers, with ammonium persulfate (APS) and tetramethylethylenediamine (TEMED) as the free radical initiator and catalyst, respectively. This provides relatively mild reaction conditions, whereby water is typically the solvent of choice. Using these conditions, a hydrogel-based nanoMIP is produced with particle sizes that range between 50–250 nm and have been successfully used in sensing and assay-based applications.26–28 Whilst application and performance of these particles is widely studied, knowledge is limited with regards to the material composition. Furthermore, little is reported on the molecular weight (MW) of the material, with the work of Guerreiro et al., making the best approximation of apparent molarities, using the expression given in eqn (1):
![]() | (1) |
Although this approximation is regularly used for estimating nanoMIPs molarities, and subsequent binding affinities, it relies on multiple simplifying assumptions. This model assumes that one nanoMIP constitutes one particle, and that each particle is uniform in shape and size, thus having the same molecular weight (MW). However, nanoMIPs typically exhibit polydispersity, with varying size range distributions depending on the synthesis conditions. Furthermore, the model assumes that the density of the particle is consistent throughout, with the density (ρ) estimation based on a non-imprinted nanoparticle consisting of N-tert-butylacrylamide (TBAm), N-isopropylacylamide (NIPAm), acrylic acid (AAc), crosslinked with N,N′-methylenebisacrylamide (BIS), without the mention of monomer crosslinker ratios.30 This density (ρ) estimation neglects changes in polymer composition with the use and addition of different functional monomers. Moreover, it also fails to consider the effects of the imprinting and resulting binding cavity on particle density and assumes that the monomer: assuming the final polymer composition mirrors the initial monomer feed. These assumptions could seriously affect the molarity estimations and can have majority implications, especially when used for binding affinity calculations, such as those produced by surface plasmon resonance (SPR) when the target is immobilised to the sensor surface.31,32 Henderson et al. addressed these challenges by immobilizing the nanoMIP on the sensor chip, thereby avoiding the need for precise molarity estimates. This, however, also presents potential issues, predominantly arising from the binding of a small molecule onto the immobilised, much larger nanoMIP.33,34 This generates smaller differences in binding signal intensities, which become more difficult to interpret, potentially limiting the sensitivity of detection and the reliability of the kinetic data.
These issues highlight the broader challenge in the field: the lack of standardized methodologies for nanoMIP synthesis, and a lack of consistency when evaluating their affinity and subsequent binding performance.35 This negatively impacts the use of these materials, particularly within commercial settings that rely on consistency within a product.36
This study aims to systematically evaluate the influence of commonly used solid-phase carriers (glass bead vs. magnetic nanoparticle) and with template characteristics on the synthesis of molecularly imprinted nanoparticles (nanoMIPs). The proteins bovine haemoglobin (BHb) and bovine serum albumin (BSA) were used as exemplary templates due to their similarity in size and hydrophobic solvent accessible surfaces areas (SASA),37,38 whilst having significantly different surface residues and surface binding cavities. These differences potentially affect functional monomer binding within the self-assembly phase. A mixture of functional monomers, acrylic acid, acrylamide, N-(hydroxyl methyl) acrylamide (chosen due to their hydrogen bond donor and acceptor) and N-isopropyl acrylamide (chosen due to its thermosensitive properties) (Fig. 2), were used.39,40 By understanding the relationship between sold-phase, template and monomer choice will lay the groundwork for rational nanoMIP design with improved reproducibility and performance.
| Protein | Molecular weight (KDa) | pI Value |
|---|---|---|
| BHb | 66.5 | 7.1 |
| BSA | 64.5 | 4.7 |
The nanoMIPs were produced using a range of functional monomers at the constant molar ratio feed shown in Table 2. The functional monomers were chosen due to their water solubility and range of functional groups (NH2, CO, COOH, OH), and their well-established selective binding properties as hydrogen-bond donor and acceptor for protein-based hydrogel nanoMIPs.39 Furthermore, the inclusion of NIPAm as a functional monomer, enables temperature-controlled responsive properties, thus allowing the easy release of the template/target molecule, by increasing the temperature.33 This ratio is considered a bona fide favourable ratio for the popular solid-phase nanoMIP methodologies45 and produces a total monomer
:
crosslinker percentage ratio of 34
:
1. This is widely used for a range of targets that includes low molecular weight molecules (antibiotics, drugs of interest, performance and image enhancing drugs),33,46 peptides,19 and large macromolecules (proteins, enzymes, antibodies, viruses).47,48
| Monomer | Monomer ratio (%) | |
|---|---|---|
| Functional monomer | NIPAm | 57.0 |
| AAm | 19.9 | |
| NHMAm | 13.6 | |
| AAc | 6.6 | |
| Crosslinker | BIS | 2.8 |
To establish a comparative protocol between the solid-phases, 5 g of template-derivatized magnetic nanoparticles was used vs. 30 g of template-derivatized glass beads. As well as different template amounts for immobilisation (7.5 mg for template-derivatized magnetic nanoparticles vs. 10 mg for template-derivatized glass beads). This difference reflects the substantially higher surface area and template loading capacity of the magnetic nanoparticles., which provides a greater reactive interface per unit mass compared to glass beads.20 Consequently, a smaller quantity of magnetic nanoparticles was sufficient to achieve an equivalent level of template presentation and comparative polymerisation yield. The yields reported were normalised to the amount of template-derivatised solid phase used in each synthesis, allowing direct comparison between the two supports. This proportional scaling is consistent with previous nanoMIP synthesis methodologies.20,42
NanoMIP materials were successfully produced and developed using a magnetic and glass bead solid-phase approach for the targets BHb and BSA. Approximately 100 mL of nanoMIP solution was produced for each nanoMIP, with the yield of the material estimated by taking a 3 mL sample and incubating in a drying oven at 60 °C until dry and measuring the particle masses with a 6-point balance. The hydrodynamic diameter of the nanoMIPs was then estimated using dynamic light scattering (DLS), to measure a dilute solution of the nanoMIPs. Table 3 and Fig. 3 present the comparative yield (in mg) and size (in nm) of nanoMIPs synthesized using magnetic nanoparticles or glass beads, for both BHb and BSA templates.
| Protein template | Glass bead | Magnetic nanoparticle | ||
|---|---|---|---|---|
| Yield (mg) | Size (nm) | Yield (mg) | Size (nm) | |
| BHb | 19.53 ± 3.2 | 25.8 ± 3.8 | 9.85 ± 3.8 | 49.0 ± 7.0 |
| BSA | 13.04 ± 2.8 | 23.2 ± 2.9 | 9.50 ± 1.3 | 53.8 ± 13.8 |
Table 3 shows significant differences between the yield and size of the nanoMIPs produced by the different solid-phase protocols (magnetic nanoparticles vs. glass bead). The nanoMIPs produced using the glass bead method produces a much smaller size (25.8 nm and 23.2 nm for BHb and BSA, respectively) compared with the nanoMIPs produced using the magnetic nanoparticle as the solid-phase (49.0 nm and 53.8 nm for BHb and BSA, respectively). These nanoMIPs are overall much smaller than those presented in literature,29,31 potentially due differences in polymer composition. Additionally, this is the first demonstration of nanoMIP size differences as result of different solid phase used for production. The SEM images (Fig. 4) show that the magnetic solid-phase nanoparticles form clusters (when dried), whereas more uniform and spherical nanoparticles in appearance can be appreciated via the glass bead solid-phase, furthermore estimation of nanoMIP size these images (Fig. 4), confirm the sizes from DLS (Fig. S1 and Table S1). The yield of the nanoMIPs produced also show a variation that is dependent of the solid phase used, with the glass bead method producing 19.53 mg and 13.04 mg (for BHb and BSA, respectively) compared with the magnetic nanoparticle method producing 9.85 mg and 9.50 mg (for BHb and BSA, respectively). Although these yields are consistent with that the amount of nanoMIPs that are typically produced using a solid-phase protocol,46 this work demonstrates yet another clear difference in the nanoMIPs produced via the different protocols. With these observed differences in nanoMIP yield and particle size potentially attributed to variations in the physicochemical properties of the solid-phase carriers. Magnetic nanoparticles possess a highly curved, high surface–area interface that allows for greater monomer diffusion and polymer chain extension before detachment, resulting in larger particles. Whereas the relatively flat and less reactive surface of the glass beads promotes localised polymerisation with restrictive chain growth leading to the formation of smaller more uniform nanoMIPs.20,44
To assess the binding affinity and specificity of the synthesized nanoMIPs, we employed surface plasmon resonance (SPR), a label-free optical technique capable of quantifying real-time molecular interactions.49 Each nanoMIP formulation was immobilized onto a carboxymethyl dextran-coated gold chip via EDC/NHS coupling, exploiting the presence of primary amine groups within the polymer matrix. This immobilization strategy enables direct evaluation of target binding without requiring assumptions about the nanoMIP's molar concentration, which is often poorly defined due to particle polydispersity and uncertain internal density.
Unlike conventional approaches where the target is immobilized and nanoMIPs are injected as analytes,31 our setup of immobilizing the nanoMIPs on to the surface, circumvents uncertainties in molarity estimates and allows for more accurate determination of binding constants. Although the total quantity of nanoMIP bound to the chip is not precisely known, the use of excess material during immobilization ensures maximal surface coverage. Given the design of solid-phase nanoMIPs and their expected monovalent architecture (one dominant binding site per particle), we modelled the interaction using a 1
:
1 Langmuir binding framework.
Fig. 5 presents representative SPR sensorgrams showing the interaction of five different concentrations of each protein target with their corresponding immobilized nanoMIP. Panels A and B illustrate BHb binding to nanoMIPs synthesized on glass beads and magnetic nanoparticles, respectively; panels C and D show the equivalent for BSA. In all cases, the sensorgrams exhibit concentration-dependent association and dissociation phases, allowing for robust determination of equilibrium binding constants.
The KD values derived from Fig. 5 and presented in Table 4 show that, overall, the nanoMIPs display excellent affinity towards the chosen targets, with KD values within the nanomolar range. These values are consistent with those currently presented in literature for protein targeted nanoMIPs, albeit with a different functional monomer construction. The values presented in Table 4 also show that differences in the affinity of the materials produced occur dependent upon the solid-phase used. While these differences are minor, it appears that the nanoMIPs produced using the glass bead solid-phase show an approximately 10-fold improvement in affinity compared with the nanoMIPs produced using the magnetic nanoparticle solid-phase. This could potentially be due to the differences in size of the nanoMIPs that were produced, with the glass bead methodology producing a smaller nanoMIP compared with the magnetic nanoparticle methodology. Typically, the smaller nanoMIP size produces a higher surface-to-volume ratio. These smaller particles expose more binding sites on their surface, allowing faster mass transfer and recognition, leading to an increase in sensitivity and binding affinity.20 Furthermore, the use of a solid-phase to immobilise templates, allows for precise control over the polymerisation conditions and binding site formations. This leads to highly reproducible affinity characteristics, and with the well optimised synthesis methodology, KD values remain within a single order of magnitude between batches.20,42 Thus when immobilisation and washing steps are carefully standardised, batch-to-batch variation becomes negligible.50
| Imprinted nanoMIP | K D (M) | |
|---|---|---|
| Glass bead | Magnetic nanoparticle | |
| BHb | 2.57 × 10−9 | 2.96 × 10−8 |
| BSA | 5.30 × 10−8 | 8.43 × 10−7 |
The specificity of the nanoMIPs was investigated through the binding of a non-target protein onto the nanoMIP coated chips. This allows for cross-reactivity and non-specific binding exploration, with BHb binding to a BSA imprinted nanoMIP and BSA binding to a BHb imprinted nanoMIP. The KD values for these interactions are present in Table 5, with the comparative SPR sensorgrams shown in Fig. S2.
| Imprinted nanoMIP | K D (M) | |
|---|---|---|
| Glass bead | Magnetic nanoparticle | |
| BHb | 4.76 × 10−6 | 2.23 × 10−5 |
| BSA | 1.26 × 10−6 | 3.03 × 10−5 |
When investigated with non-target proteins, the nanoMIPs materials show that they are specific for the target proteins, with an approximately 100–1000-fold decrease in affinity towards a non-target protein. This is to be expected with nanoMIPs produced using a solid-phase, as other works also show similar decreases in affinities towards a non-target protein. These affinity differences are also consistent across different solid phases (glass bead vs. magnetic nanoparticle). In this case, the nanoMIPs produced using a magnetic solid phase show an approximate 10-fold decrease in affinity, compared with the nanoMIPs produced using the glass bead solid phase. This suggests that the nanoMIPs that are produced using the magnetic solid phase are overall less selective (by approximately 10-fold) compared with those produced using the glass bead solid phase. The proteins used in this study where specifically chosen based on their structural and functional similarity, allowing for comparative analysis. Thus, representing the most stringent and physiologically relevant challenge to the biding sites. The use of the solid-phase protocol has consistently shown to produce nanoMIPs with homogeneity and low non-specific binding.20,42 Since the nanoMIPs in this work demonstrated negligible cross-reactivity under these conditions, it should be expected that less related proteins would also not show any binding.
There is a current assumption that the polymer composition of the nanoMIP, produced via the solid-phase, is consistent (in terms of molar ratios) with the monomer mixture feed. However, this assumption neglects any impact the template may have on the polymer composition during nanoMIP formation. With differences in template surface functionality, it is then logical to suggest that different functional monomers will be attracted to these binding sites, particularly during a self-assembly process. The variation in target molecule should therefore significantly impact the final output on nanoMIP polymer composition, with variation in template molecules. NMR spectroscopy is a well-established method for the characterization of polymers and has been applied for the determination of monomer sequence and reactivity ratios and polymer microstructure.51 Utilising 1H NMR, an assessment on the number of repeating units in the overall nanoMIP was achieved with an estimation of the relative composition of the nanoMIP. The calculation of the relative number of moles of a polymer block (denoted as x) can be calculated using eqn (2):
![]() | (2) |
With, for one type of polymer block, Ip being the integration value of the polymer block's corresponding peak, and Np being the total number of H protons (or active nuclei) for that polymer block. By determining the relative number of moles per polymer block, the composition of the nanoMIP as ratio can be estimated.51
The 1H NMR spectra shown in Fig. S3–S6, show the polymer composition of the nanoMIPs, with a specific resonance for each monomer. Utilising eqn (2), the overall polymer composition of the nanoMIPs was estimated and shown in Table 6, with a full breakdown of calculations showin in eqn (S1)–(S9).
| NanoMIP | Polymer composition (%) | Monomer: crosslinker ratio | ||||
|---|---|---|---|---|---|---|
| NIPAm | AAm | NHMAm | AAc | BIS | ||
| BHb G | 30 | 11 | 41 | 4 | 14 | 6 : 1 |
| BHb M | 20 | 10 | 4 | 17 | 6 | 9 : 1 |
| BSA G | 20 | 11 | 39 | 0 | 30 | 2 : 1 |
| BSA M | 12 | 17 | 47 | 17 | 17 | 5 : 1 |
The polymer composition (%) shown in Table 6 reveal interesting differences between the composition of the monomer/crosslinker mixture inputted compared to the monomer/crosslinker composition of the polymers produced. The overall monomer
:
crosslinker ratio that is inputted was calculated to be 34
:
1 (monomer: crosslinker, respectively), which has been deemed favourable in either glass bead or magnetic nanoparticle-based solid phase protocols. Surprisingly, the overall monomer: crosslinker ratio that is produced within the nanoMIPs is drastically different compared to the ratio in the feed: the final monomer
:
crosslinker ratio is equal to a range of 2
:
1–9
:
1 (monomer
:
crosslinker, respectively). The monomer
:
crosslinker ratios are much more consistent with the monomer
:
crosslinker ratios (9
:
1) that were seen in traditional bulk polyacrylamide hydrogel-based MIPs,39,52 which themselves were adapted from polyacrylamide gels used for electrophoresis.53,54 This suggests that this lower monomer: crosslinker is favourable under these simple polymerisation conditions.
Table 6 also shows the polymer composition varies considerably between template used, as well as with varying solid phase. Differences between polymer composition with varying the target can be rationally explained due to differences in the surface of the protein targets. Sullivan et al. show that protein templates produce multiple potential binding cavities (for functional monomers) that are evenly distributed around the surface of the protein.39 These binding cavities are used by the functional monomers during monomer–template complexation with varying degrees of affinity depending on the site or monomer.39 Potential binding cavity analysis of the protein targets BHb and BSA performed by molecular modeling (CavitOmix) 655,56 reveal that BHb has 27 potential binding cavities evenly spaced around the surface of the protein (Fig. 6A), whereas BSA has 68 potential binding cavities around the surface of the protein (Fig. 6B). Along with having a significantly different amount of potential binding cavities, these cavities also differ in shape and size and amino acid functionality. This is shown with the differences in the solvent-accessible surface area (SASA) calculated using APBS (v3.4.1),57 and shown in Fig. 6C and D, for BHb and BSA, respectively, with BSA showing much more positive electrostatic potential (blue) regions compared with BHb. This means that different monomers will favourably bind to the different potential binding cavities,39 thus affecting the polymer composition of nanoMIP that is produced. More surprisingly, the changing of the solid phase, while keeping the same template, appears to be influencing the final polymer composition of the nanoMIP. Table 6 shows that using the glass bead as the solid-phase produces a polymer with a higher amount of NHMAm and a lower amount of AAc in the final composition compared to the magnetic solid-phase nanoparticles. These findings are also consistent for both the BHb and BSA template nanoMIPs, and potentially due to differences within the solid-phase size and composition.
![]() | ||
| Fig. 6 Potential binding cavity analysis of the target proteins BHb (A) and BSA (B) using CavitOmix and solvent-accessible surface area (SASA)55,56 of the target proteins BHb (C) and BSA (D) calculated using APBS (v3.4.1).57 The blue and red gradients correspond to positive electrostatic potential and negative electrostatic potential, respectively. The BSA shows much more positive electrostatic potential regions compared with BHb. | ||
The glass bead solid phase is predominately made of SiO2,58 while the magnetic nanoparticles are Fe3O4.59 Furthermore, the glass beads are also approximately 350 times larger than the magnetic nanoparticles. Glass beads present hydrophilic, hydroxyl-rich surfaces that differ in charge density and hydrogen-bonding capacity from the typically functionalised magnetic nanoparticles. These distinctions influence template immobilisation, local monomer orientation, and polymer chain propagation during polymerisation. Moreover, the markedly higher curvature and surface energy of magnetic nanoparticles alter monomer packing and radical diffusion dynamics at the interface, producing compositional and structural differences in the imprinted polymer layer.20,26,44 These differences will influence the functionalisation and immobilisation of the template to the solid-phase and thus will also impact the template–monomer interactions, along with solid-phase–monomer interactions, during the complexation process.
Collectively, these findings represent a rigorous investigation into how solid-phase choice and protein template impact nanoMIP synthesis at the compositional level. By linking physical imprinting conditions to polymer architecture and ultimately to functional performance, this study provides a framework for rational nanoMIP design. This work shows that the template and choice of solid phase can have a significant impact on the final polymer composition, which in turn can have a substantial impact on the performance of the nanoMIP. This suggests that the nanoMIPs should be rationally designed, with monomer choice dependent upon the solid phase used and the template needed, to achieve maximum performance. This highlights that there is no “one size fits all” with regards to pre-polymerisation monomer mixture or choice of solid phase, with careful considerations needed. Particularly, these highly specific and selectivity recognition materials offer a viable alternative in terms of performance to biological recognition materials (antibodies), but with the additional benefits of being low-cost, resistant to high and low pH and temperatures values, and having simple storage conditions (room temperature) without degradation that affects the performance.
Glass beads (35 μm) were purchased and used without purification from Axel (Japan).
Acetone, acetonitrile (anhydrous), ethanol (anhydrous), isopropanol, methanol, toluene (anhydrous), dipotassium phosphate, and disodium phosphate were all purchased and used without purification from Nacalai Tesque (Japan).
Particle size at 25 °C (effective hydrodynamic radius) and polydispersity index were measured using dynamic light scattering in MilliQ with Zeta-potential & Particle size Analyzer ELSZ-2000.
Scanning electron microscopy (JEOL JSM-7900F) was used to observe the morphology and dispersion of the synthesized nanoMIPs. The sample was prepared by mixing the MIPs with 1 mL MilliQ and vortexing the solution for 1 minute, then leaving one drop on one gold chip and leaving it to dry overnight. The next day, the chip is coated with gold and ready for SEM observation.
Kinetic analysis in rebinding of analyte (target and cross-reactivity) to the nanoMIP was performed in set pattern of 2 min association (PBST with analyte in range of 4.0–64.0 nM), 5 min dissociation (running buffer only), and a regeneration cycle (regeneration buffer 10 mM glycine–HCl, pH 2 for 1 min) followed by a final stabilization cycle (running buffer for 1 min). An initial injection of running buffer (blank) was used as the first run with increasing analyte concentration for subsequent runs. After the analyses were completed, signals from reference channel were subtracted from signals from the working. In all cases, rebinding was studied in triplicate. The SPR responses were fitted to a 1
:
1 Langmuir fit bio-interaction (BI) model using the Biacore T200 evaluation software. Association rate constants (ka), dissociation rate constants (kd), and maximum binding (Bmax) were fitted globally, whereas the BI signal was fitted locally. Equilibrium dissociation constants (KD) were calculated by kd/ka. For each nanoMIP/analyte combination, a calibration curve was generated across the concentration range 4.0–64.0 nM taking n = 3 average. Where signal saturation was observed (noted in more complex matrices), the linear section of the curve was used for this calculation.
The surface of the protein was analysed by using APBS (v3.4.1), with the protein initially prepared using PDB2PQR (v3.6.1) at a pKa of 7.0 and an AMBER forcefield, ensuring that waters are removed, new atoms not rebuilt too close to current aaatoms, and optimizing the hydrogen bonding network.57 Adaptive Poisson–Boltzmann solver (APBS) was then subsequently used with mg-auto calculation time, to determine electrostatic surface visualization.57
In parallel, protein surface analysis using computational cavity mapping and electrostatic surface potential modelling revealed that differences in the number, distribution, and physicochemical nature of binding sites on the template proteins likely contribute to template-specific polymer compositions. For instance, BSA, with its higher number of binding cavities and greater surface polarity, drove a distinct monomer incorporation profile compared to BHb.
Taken together, these findings challenge the assumption of compositional uniformity in nanoMIPs and highlight the importance of rational design in imprinted polymer synthesis. Our results suggest that template structure, solid-phase material, and monomer selection should be co-optimized to achieve high-performance nanoMIPs with enhanced affinity, selectivity, and reproducibility. This work lays the groundwork for more predictive and standardized approaches to nanoMIP fabrication, with broad implications for their application as synthetic recognition elements in diagnostics, sensing, and therapeutic platforms.
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