Dorota
Sklenárová‡
a,
Antonín
Hlaváček‡
*b,
Jana
Křivánková
b,
Julian C.
Brandmeier
ac,
Julie
Weisová
b,
Michal
Řiháček
d,
Hans H.
Gorris
a,
Petr
Skládal
a and
Zdeněk
Farka
*a
aDepartment of Biochemistry, Faculty of Science, Masaryk University, Kamenice 5, 625 00 Brno, Czech Republic. E-mail: farka@mail.muni.cz
bInstitute of Analytical Chemistry of the Czech Academy of Sciences, Veveří 97, 602 00 Brno, Czech Republic. E-mail: hlavacek@iach.cz
cInstitute of Analytical Chemistry, Chemo- and Biosensors, University of Regensburg, Universitätsstraße 31, 930 53 Regensburg, Germany
dDepartment of Laboratory Methods, Faculty of Medicine, Masaryk University, Kamenice 5, 625 00 Brno, Czech Republic
First published on 24th June 2024
Early-stage diagnosis of prostatic carcinoma is essential for successful treatment and, thus, significant prognosis improvement. In laboratory practice, the standard non-invasive diagnostic approach is the immunochemical detection of the associated biomarker, prostate-specific antigen (PSA). Ultrasensitive detection of PSA is essential for both diagnostic and recurrence monitoring purposes. To achieve exceptional sensitivity, we have developed a microfluidic device with a flow-through cell for single-molecule analysis using photon-upconversion nanoparticles (UCNPs) as a detection label. For this purpose, magnetic microparticles (MBs) were first optimized for the capture and preconcentration of PSA and then used to implement a bead-based upconversion-linked immunoassay (ULISA) in the microfluidic device. The digital readout based on counting single nanoparticle-labeled PSA molecules on MBs enabled a detection limit of 1.04 pg mL−1 (36 fM) in 50% fetal bovine serum, which is an 11-fold improvement over the respective analog MB-based ULISA. The microfluidic technique conferred several other advantages, such as easy implementation and the potential for achieving high-throughput analysis. Finally, it was proven that the microfluidic setup is suitable for clinical sample analysis, showing a good correlation with a reference electrochemiluminescence assay (recovery rates between 97% and 105%).
Magnetic microparticles (MBs) represent a promising alternative solid phase in immunoassays. They typically consist of one or more magnetite (Fe3O4) nanocores surrounded by a polymer layer. The resulting core–shell structure is usually larger than 1 μm in diameter and has superparamagnetic properties.11 MBs additionally provide a large surface-to-volume ratio, low toxicity, and biocompatibility.12 Surface-modified MBs have found a plethora of applications, including drug delivery, cancer therapy,13,14 and immunoassays.15–17 For immunoassays, the MBs are commonly conjugated with antibodies, allowing for the magnetic preconcentration and separation of the MB-bound immunocomplexes from sample matrix and unbound reagents.18
Different kinds of nanomaterials can be used as advanced immunoassay labels. In particular, photon-upconversion nanoparticles (UCNPs) exhibiting anti-Stokes luminescence (i.e., the ability to convert low-energy NIR excitation to higher energy emission)19,20 are gaining popularity, as they enable sensitive detection without optical background interferences.21 As UCNPs are typically synthesized in organic solvents, a surface modification and conjugation with biorecognition molecules, such as antibodies or streptavidin, are required to render them dispersible in aqueous media and make them available as immunoassays labels.22–24 Highly sensitive UCNP-based assays for the detection of various analytes were previously reported.25 Digital immunoassays based on detecting and counting individual immunocomplexes are a promising way to achieve exceptional sensitivity and further improve assay performance.26 For example, we used epiluminescence microscopy to count individual UCNP-labeled immunocomplexes on the MTP surface.19
While MTP-based immunoassays typically require relatively large sample volumes and offer only limited throughput, modern miniaturization techniques reduce the sample consumption and may also improve other assay parameters (e.g., sensitivity, signal-to-background (S/B) ratio, and working range).27,28 In particular, microfluidics only requires minimal amounts of sample and enables rapid sample processing with a high throughput. The fundamental principle of microfluidics lies in the manipulation of fluids in channels of sub-millimeter dimensions, ranging from hundreds to tens of micrometers,29 allowing for the manipulation of exceptionally small volumes (10−9 to 10−18 L).30 There are several reports of microfluidic devices for immunoanalysis based on conventional organic fluorophore labels in the literature.31–33 Microfluidics-based methods for magnetic bead-based immunoassays have also been previously reported.34–36 In all cases, however, the immunoreaction took place on a chip, which required applying an external magnetic force during the experiments and prolonged the readout. Thus, in order to detect single analyte molecules as labeled complexes while maintaining the advantages of microfluidics (e.g., high throughput, effective manipulation, low sample consumption), it is necessary to develop simple yet effective techniques such as droplet microfluidics for digital detection.37,38
We have previously reported the use of MBs in immunoassays for the detection of PSA based on various labels to fully optimize the MB-based upconversion-linked immunosorbent assay (ULISA) and to explore the possibilities for sensitivity enhancement.10 Moreover, we have employed massively parallel spectroscopy of UCNPs for detecting single analyte molecules free in dispersion.39 To the best of our knowledge, however, no studies have been conducted on the digital detection combining UCNP labels with MBs.
In this work, we have developed an MB-based ULISA for the single-molecule detection of PSA utilizing a flow-through microfluidic device. The immunoassay was performed in microtubes to enable sample introduction into the device (Fig. 1A). The samples were introduced to a microfluidic chip with a flow-through cell and individual immunocomplexes were counted (Fig. 1B), utilizing a microfluidic chip with a flow-through cell (Fig. 1C).
Following our previous report on detecting single UCNPs in a free dispersion,39 the method developed here allows for counting single labels on the freely dispersed MBs. Moreover, it enables the single-molecule readout in liquid, the native environment of proteins, eliminating the risk of possible structural changes or aggregation, which may cause an increase in non-specific binding and complicate the evaluation of results. Thus, while maintaining simplicity in terms of operation, the microfluidic setup allowed for enhancing the assay sensitivity further.
The solutions used included coating buffer (50 mM NaHCO3/Na2CO3, 0.05% NaN3; pH 9.6), phosphate buffer (50 mM NaH2PO4/Na2HPO4; pH 7.4), phosphate-buffered saline (PBS; phosphate buffer with 150 mM NaCl; pH 7.4), washing buffer (50 mM Tris, 0.05% NaN3, 0.05% Tween 20, 1 mM KF; pH 7.5), and assay buffer (50 mM NaH2PO4/Na2HPO4, 10% SuperBlock, 0.05% NaN3, 0.01% Tween 20, 150 mM NaCl, 1 mM KF; pH 7.5). All buffers were prepared using deionized water and filtered using a 0.22 μm membrane (Millipore Express Plus, Merck, Germany).
The protocols for the synthesis and characterization of UCNPs (NaYF4:Yb3+,Er3+) and their bioconjugates with streptavidin and the anti-PSA polyclonal antibody, conjugation of MBs with the anti-PSA monoclonal antibody, and the procedure of MTP-based ULISA for the analog readout are provided in the ESI.†
First, serial dilutions of the PSA antigen (10−4 to 102 ng mL−1) in the volume of 450 μL were prepared in 50% bovine serum in assay buffer. The total sample volume was enough for approximately 10 to 20 microfluidic measurements, depending on the setup parameters (utilizing 20 to 40 μL of sample per measurement); however, a larger volume was used in the sample preparation steps to enable easier manipulation with the MBs. The procedure for the clinical sample analysis was identical to the one carried out to obtain the calibration curve. The spiked serum was mixed with 50 μL of the MB-ab403 bioconjugate (50 μg mL−1) to capture the PSA from the sample. In the next step, the BAF1344 biotinylated anti-PSA polyclonal antibody (500 μL, 0.25 μg mL−1) was added to each microtube. Then, the UCNP-SA bioconjugates (500 μL, 2 μg mL−1) were added, followed by the resuspension of the MB-bound immunocomplexes in 500 μL of assay buffer. The samples for the microfluidic measurements were stored at 4 °C until the readout was performed. The second set was immediately transferred to a non-binding MTP (Greiner Bio-One, Austria) and, after short shaking at 1000 rpm, left to dry at room temperature.
It was not necessary to remove the MBs not carrying PSA and UCNPs from the solution, as the measured signal was provided only by the specifically bound UCNP-SA label. The MBs not carrying the labeled immunocomplex did not display any luminescence and, therefore, did not disrupt the obtained data. Furthermore, as the microfluidic setup allowed for the specific counting of the immunocomplex-bound UCNPs, no further purification of the MBs during the sample preparation was necessary.
For each measurement, the microscope objective CFI Plan Apo Lambda (60× magnification, NA 1.40; Nikon, Japan) was focused 10 μm below the substrate glass slide of the chip. A 976 nm laser (10 W; Roithner Lasertechnik, Austria) with a 950 nm long-pass filter served as the excitation source; the beam was reflected to the microscope objective via a 900 nm short-pass dichroic mirror. The power output measured from the microscope objective was set to 1.3 W, resulting in the average excitation intensity of 9.4 kW cm−2 in the detection point, which was characterized as reported previously.39 An 875 nm short-pass filter was inserted before the microscope tube lens, enabling the detection of both the green and the red emission from the UCNPs as a single spot. The images of UCNPs from the microfluidic chip were taken by a Zyla 5.5 sCMOS camera (Andor Technology – Oxford Instruments, UK) using the sensor area of 1024 px × 1024 px (imaging area of 111 μm × 111 μm in the sample plane). As the imaging area did not fully cover the flow region, the resulting number of UCNPs represents an estimated number.
The MicroManager software (Laboratory for Optical and Computational Instrumentation, University of Wisconsin, USA) was used to control the camera. With an exposure time of 5 ms, 10 images were recorded per second, and three sets of 500 frames were recorded for each sample. For counting individual immunocomplexes, the images of single UCNPs were localized using a U-net convolutional neural network,40 which was trained and tested as reported previously with minor modifications (Fig. S1†).39 In the analysis, the average numbers of UCNPs and standard deviations (error bars in the graphs) were calculated from 3 independent measurements.
The LODs were estimated from the regression curves as the concentrations corresponding to the sum of the background value obtained by the logistic fit (A1) and three times the standard deviation of the blank (s0):
y(LOD) = A1 + 3s0 |
Utilizing the DLS software, the number-based distribution was also evaluated (Fig. S2†). The maximum in the number distribution was found at 50.7 ± 5.9 nm and 43.8 ± 0.2 nm for UCNP-Ab and UCNP-SA, respectively. The data showed only one size fraction for both bioconjugates, proving that the second peak in the UCNP-Ab intensity distribution represented only a small number of strongly scattering particles.
Furthermore, MBs in various environments were characterized via DLS. The sizes determined from the intensity-based distribution (Fig. 2D) were 1357 ± 206 nm for unbound MBs, 1481 ± 156 nm for the mixture of MBs and UCNP-SA, and 1505 ± 143 nm for the full sandwich immunocomplex of MBs with PSA and UNCPs. Number-based distribution (Fig. S2†) revealed sizes of 1329 ± 193 nm, 1446 ± 142 nm, and 1478 ± 140 nm, respectively. It must be noted that relatively large standard deviations were obtained, caused by the sedimentation of the relatively large MBs during the measurement. Nevertheless, the comparable size values confirm that the presence of PSA and UCNP-SA did not cause any aggregation of the MB dispersion.
The MB-based ULISA experiments were optimized regarding the MB concentration (Fig. S4A†), the ratio of MBs and UCNPs (Fig. S4B†), and the evaluation of assay performance in the whole concentration range of fetal bovine serum (Fig. S4C†). The data showed that the MB concentration of 50 μg mL−1 combined with 2 μg mL−1 of UCNP-SA was optimal for the sensitive detection of PSA and that serum did not significantly affect the assay performance. The assay specificity was further verified by studying the effect of three other biomolecules, including human serum albumin (HSA), bovine serum albumin (BSA), and carcinoembryonic antigen (CEA), on the MB-based ULISA (Fig. S5†). The results showed no cross-reactivity with the other biomolecules, demonstrating the exceptional specificity of the assay.
Afterward, the MB-based ULISA was optimized for immunocomplex formation in microtubes, and the data were analyzed utilizing the analog readout mode (Fig. 3B). The assay reached an LOD of 11 pg mL−1 and a working range from 4.5 to 71.1 ng mL−1. The results showed a minimal background signal in 50% serum, with an S/B ratio of 353. The assay parameters were comparable to the MTP-based ULISA, though the S/B ratio was 1.8 times lower. The possible explanation lies within the use of the MBs, which yielded a higher maximum signal, albeit also a higher background. In our previously published study,10 the LOD achieved by an MB-based ULISA of 3.87 pg mL−1 was comparable, albeit slightly lower. In the cited paper, the assay was performed within the MTP wells with automatic washing, whereas here, the assay format revolved around the use of microtubes with manual washing in order to introduce the samples into the microfluidic device effectively. The difference in the assay procedures, as well as the lower MB concentration utilized here to prevent the microfluidic channel from clogging, may also have resulted in the variations.
The optimization measurements (Fig. S6†) were performed at the UCNP-SA concentration of 2 μg mL−1. However, in this experiment, the MBs carrying higher PSA concentrations (>1 ng mL−1) tended to adsorb to the PDMS surface of the flow cell. Therefore, the laser beam was not able to penetrate through the otherwise transparent PDMS, and the accumulated energy absorbed by the MB layer damaged parts of the microfluidic chip due to the excess heat. Consequently, the obtained data were inconsistent, with large standard deviations because the flow cell did not function appropriately, resulting in an LOD of 40 pg mL−1 and a narrow working range from 0.07 to 0.9 ng mL−1. Moreover, the average number of UCNPs was below 120, even for the highest PSA concentration, resulting in a low S/B ratio of 12. Albeit higher UCNP-SA concentrations could further improve the LOD, they were not tested, as it was previously reported that individual particle counting in an MTP-based single-molecule ULISA was rather tricky at high label concentrations.9 Moreover, a high label concentration could lead to aggregate formation within the microfluidic channel and thus decrease the reliability of the method.
In order to confirm that the chip damage was caused mainly by the MBs and not by the UCNP-SA label, a direct bioconjugate of the UCNPs with the AF1344 anti-PSA polyclonal antibody (UCNP-Ab) was prepared. After optimizing the UCNP-Ab concentration in an MTP-based assay (Fig. S7†), the concentration of 12 μg mL−1 was used for the microfluidic setup. The direct conjugate allowed for a one-step detection without using a biotinylated antibody, though its most effective concentration was 6 times higher than the effective concentration of the SA-UCNP label. The lower required label concentration in the case of UCNP-SA compared to UCNP-Ab is connected with the higher affinity of the streptavidin-biotin interaction compared to the weaker antibody–antigen interaction.9
To further confirm that the chip damage was induced by the MBs and not the UCNPs, absorption spectra of both dispersions in concentrations identical to those utilized in the microfluidic measurements were analyzed using the Specord 210+ spectrometer (Analytik Jena, Germany). The results (Fig. S10†) showed that the absorbance of UCNPs under NIR wavelength of 980 nm was negligible (value close to zero) in comparison to that of the MBs (0.35 a.u.), confirming that MBs were responsible for absorbing the excitation light leading to the thermal damage of the chip.
More intense mixing was introduced to prevent the MBs from sedimenting within the sample mixture. Even though the first measurements (Fig. S8A†) showed improved standard deviations, the resulting data were inconsistent. The relatively high background led to the S/B of 3.3, a very narrow working range of 13 to 21 ng mL−1, and a relatively high LOD of 13.0 ng mL−1. As the unfavorable results may have been caused by the high UCNP label concentration, it was lowered to 4 μg mL−1 for the subsequent optimizations. Fig. S8B† shows an improvement in both the curve and the parameters, reaching the S/B ratio of 21, a working range from 2.6 to 22.8 ng mL−1, and an LOD of 0.39 ng mL−1. However, due to the relatively high LOD as well as the concentration of the UCNP-Ab compared to the UCNP-SA required for a successful assay outcome, it was concluded that the UCNP-Ab conjugate was not suitable for this setup.
Therefore, identical measurements were performed utilizing the UCNP-SA conjugate at the previously optimized concentration of 2 μg mL−1. During these measurements, the MBs did not adsorb to the chip surface; however, the obtained curves (Fig. S9A†) again showed a similar outcome concerning the large standard deviations. Upon further analysis of the camera record, it was observed that due to the relatively high pressure applied to the cuvette and the downward slope of the capillary, the motion of the MB-bound UCNPs through the flow cell was too fast, causing them to appear as elongated lines instead of spots (Fig. S9B†). This has rendered the AI calculator incapable of reliably counting the UCNP labels attached to the MBs. Therefore, for the subsequent experiments, the tilt of the capillary was adjusted, and an otherwise identical measurement utilizing the UCNP-SA conjugate was performed.
The viscosity of the samples in various concentrations did not affect the measurements, as the viscosity is given almost exclusively by the buffer composition. All experiments were carried out in the same buffer, and the sample matrix – possibly causing viscosity changes – was washed out in the previous assay steps. Therefore, the viscosity changes can be neglected in our experimental setting. Moreover, the PSA concentrations in the samples were generally low.
The optimal flow rate was approximately 1 μm per 5 ms of exposure time, corresponding to 200 μm s−1. This flow rate was set by applying a pressure of 1 kPa to the cuvette. With a cross-section of the microfluidic channel of 30 μm × 200 μm, this is approximately 0.0012 μL s−1 (neglecting the slower liquid flow around the microfluidic channel walls in this approximation).
The 4-parameter logistic fit of the digital readout utilizing the microfluidic device (Fig. 4C) resulted in a low LOD of 1.04 pg mL−1 (36 fM). The obtained value marks an 11-fold improvement compared to the analog readout, thus significantly enhancing the assay sensitivity. The recurrence of prostate cancer may be indicated by an increase of PSA levels within an exceptionally narrow range of low concentrations (0.1–0.2 ng mL−1), often challenging to detect via conventional methods.42 The LOD achieved by the microfluidics-based assay verifies its practical potential for disease recurrence monitoring, which was later demonstrated via clinical sample analysis. The working range of the assay is not discussed here due to the absence of saturation in the curve, rendering the S/B ratio incomputable within the context of relevance.
As an alternative means of data evaluation, the results were plotted in a double logarithmic scale and fitted utilizing a linear function (Fig. S11†). However, as the plot did not yield any improvement (LOD of 12 pg mL−1), it was concluded that all the data would be fitted via the 4-parameter logistic function.
Due to the dependency of the digital readout precision on sampling error, the limited number of observed binding events (n) may not be representative of all binding events.9 This uncertainty can be calculated from the n and is known as Poisson noise. The Poisson noise values for all the concentrations are shown in Table S1.† The obtained data show that Poisson noise decreased with growing concentration, thus confirming the expected outcome. The calculated values were low and comparable to the experimental standard deviations within the curve. As reported previously, the Poisson noise may be further reduced by increasing the imaging area or analysis time, leading to a larger amount of data to be analyzed.9
It must be noted that at the concentration corresponding to the LOD, there is a relatively high surplus of PSA molecules over MBs. Considering the binding capacity, size, and weight of a single MB,43,44 each MB can bind approximately 6.0 × 104 to 7.8 × 104 antibody molecules. Therefore, with 50 μg mL−1 of MBs and a PSA concentration of 1.04 pg mL−1, there are approximately 400 PSA molecules per MB, which corresponds to a fractional antibody occupancy of 0.5–0.7%. Even though agreeing with the literature,45 the calculation, together with the experimental results, suggests relatively low efficiency of PSA binding and labeling. Therefore, the LOD might be further improved by increasing the immunochemical reaction efficiency, e.g., by optimizing the assay procedure or using different immunoreagents.
Reference [ng mL−1] | Analog readout | Digital readout | ||
---|---|---|---|---|
Found [ng mL−1] | Recovery rate [%] | Found [ng mL−1] | Recovery rate [%] | |
2.08 | 1.82 ± 0.03 | 87.8 ± 1.6 | 2.0 ± 0.7 | 97 ± 33 |
9.23 | 10.0 ± 0.3 | 108.5 ± 2.8 | 8.9 ± 0.6 | 97 ± 6 |
30.64 | 34.1 ± 1.6 | 111 ± 5 | 32 ± 6 | 105 ± 20 |
Technique | LOD | Working range | Ref. |
---|---|---|---|
Analog and digital MTP-based ULISA (UCNP-Ab) | 20.3 pg mL−1 | 0.1–10 ng mL−1 | 19 |
1.2 pg mL−1 | 0.01–1 ng mL−1 | ||
Analog and digital MTP-based ULISA (UCNP-SA) | 380 fg mL−1 | 1–1000 pg mL−1 | 9 |
23 fg mL−1 | 0.1–100 pg mL−1 | ||
Upconversion- and infrared absorption-based assay utilizing UCNP nanoprobes | 0.05 pg mL−1 | 0.00002–50 ng mL−1 | 46 |
15.5 pg mL−1 | 0.02–200 ng mL−1 | ||
SERS-based droplet microfluidics | Below 0.1 ng mL−1 | 0.05–200 ng mL−1 | 47 |
MB-based droplet microfluidics | 7 pg mL−1 | Not provided | 38 |
Magnetic microfluidic chip with a magnetoimpedance sensor | 0.1 ng mL−1 | 0.1–20 ng mL−1 | 48 |
Analog MTP-based ULISA | 10.8 pg mL−1 | 1.7–14.8 ng mL−1 | This work |
Analog MB-based ULISA | 11.1 pg mL−1 | 4.5–71.1 ng mL−1 | This work |
Digital MB-based ULISA | 1.04 pg mL−1 | 13–100 ng mL−1 | This work |
Another study focused on the development of nanoprobes based on silica-coated UCNPs bioconjugated with an anti-PSA antibody, utilizing upconversion luminescence and infrared absorption readout.46 The obtained LODs were 0.05 pg mL−1 for upconversion luminescence and 15.5 pg mL−1 for infrared absorption, with a sample consumption of 2 mL. Even though the LOD obtained via the upconversion luminescence measurement was lower than the one reported here, the sample consumption and reagent concentrations were significantly higher. Here, although the volume of the prepared samples was 500 μL to enable easier manipulation with the MBs, the sample volume required for one microfluidic measurement was only 20–40 μL, depending on the measurement setup. Moreover, the sample preparation procedure offers potential for future optimizations to minimize sample consumption. Additionally, unlike the previously published studies on the UCNP-based single-molecule detection,19,49 the setup developed here renders the detection simple in terms of operation while enabling detection in free dispersion of MB-bound immunocomplexes.
There are also reports on various microfluidic formats for PSA detection. Gao et al.47 developed a surface-enhanced Raman scattering (SERS)-based droplet microfluidics device, achieving an LOD below 0.1 ng mL−1 (no further specification available). Others used of carboxylated MBs in a quartz capillary-based droplet microfluidic chip.38 The MB-bound sandwich immunocomplexes were introduced to a droplet-generating microfluidic chip, where the enzyme label reacted with a fluorescent substrate, achieving an LOD of 7 pg mL−1. In a study utilizing an integrated magnetic microfluidic chip with a magnetoimpedance sensor,48 the authors described a chip containing a reaction platform for immunocomplex formation. As immunomagnetic beads were used as a label, the presence of magnets was required throughout the experiments. The beads modified with streptavidin and biotinylated anti-PSA antibody were trapped in a self-assembled film within the chip. The generated stray magnetic field was measured by a magnetoimpedance sensor, reaching the LOD of 0.1 ng mL−1.
The LOD achieved via the flow-through microfluidic device developed here (1.04 pg mL−1, 36 fM) represents a significant improvement in comparison to each of the discussed microfluidic studies. In addition to the simple experiment design, no need for magnetic separation during the measurements, and easy implementation of the device itself, the method demonstrates sensitivity enhancement utilizing the UCNP-based labels. The comparative literature analysis further reinforces the conclusion that the method developed in our study exhibits significant sensitivity and represents a foundation for further development of microfluidics-based immunoassays.
Footnotes |
† Electronic supplementary information (ESI) available: Protocols for the preparation and characterization of UCNP and MB conjugates and processing of micrographs, results of the UCNP characterization and immunoassay optimization. See DOI: https://doi.org/10.1039/d4lc00346b |
‡ The authors contributed equally. |
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