Nanoscale thermal biofunctionalization: the NanoBioFET platform
To implement a scalable strategy capable of locally functionalizing individual FETs at sub-100 nm resolution with desired bioreceptors (from antibodies to aptamers), and applicable to any channel material (e.g., graphene, oxides or silicon), we use thermal scanning probe lithography (tSPL) [23, 24]. In our approach, tSPL uses a hot nanotip to expose amine groups with nanoscale resolution on a thermally sensitive biocompatible polymer resist [25–29], which is spin coated on a fully-fabricated array of FETs (see Fig. 1b). This spatially selective activation process enables subsequent modification of individual or a group of FETs with a desired bioreceptor, resulting in an array of FET-based biosensors configured for simultaneously detecting various target analytes (see Fig. 1a). We name this platform NanoBioFET.
The implementation of the NanoBioFET platform begins by fabricating a FET array. As shown in Fig. 1b, we adopt monolayer graphene for realizing the FET-based sensors (see Methods), due to its potential for ultrahigh sensitivity [30, 31]. We then cover the fully fabricated graphene FETs (gFETs) by spin coating two thermally sensitive polymer resist films (see Methods). The stack comprises a first film of about 70-nm-thick polymethacrylate-carbamate-cinnamate copolymer (PMCC) [26–28], which provides amine groups on demand in designated FET regions upon local heating by tSPL. PMCC can be locally patterned through local heat-induced deprotection of amine groups from tetrahydropyranyl carbamates in the carbamate block of PMCC [25–29] (see Methods). The second film is poly(phthalaldehyde) (PPA) [23, 32] which serves as a top layer resist (10–20 nm thick) to reduce non-specific binding outside the FET channel region (see Supplementary Note 1).
After forming the bilayer polymer resist stack, we proceed with the localized functionalization of individual FETs with desired bioreceptors. Employing tSPL, we modify the bilayer polymer resist stack atop the channel region of each target gFET with amine groups. This process utilizes a hot nano-tip in a commercial tSPL system (see Methods), which removes PPA completely above the channel region, while simultaneously applying heat to the PMCC polymer surface above the amine deprotection temperature (~ 120 C), exposing amine groups in the desired area (Fig. 1b). For differential sensing, we pattern only the FET used as a sensor, while leaving un-patterned the FET used as a control. Ensuring signal fidelity is a key challenge for commercialization of FET-based biosensors. Hence, providing a platform that allows for in-situ differential sensing is a key milestone. Using standard conjugation strategies, the amine groups in the channel region can subsequentially be functionalized with ad-hoc bioreceptors such as antibodies or aptamers (see Methods for details). At this point, the sensor/control FETs are ready for biodetection of a specific target, such as SARS-CoV-2 virus. As discussed later, when the FET sensor is exposed to a specific target, the target is immobilized by the bioreceptor near the polymer surface, giving rise to a change in the electronic signal of FET-based sensors.
In Fig. 1c, we demonstrate the resolution of the NanoBioFET fabrication method. Specifically, Fig. 1c shows an in-situ tSPL topographical image (see Methods) of an amine pattern produced by tSPL in a PPA/PMCC bilayer polymer resist stack deposited on a SiO2/Si wafer (without graphene). The pattern consists of a 10 x 10 matrix of 15 nm-diameter amine circles with 40 nm pitch. This image shows a resolution compatible with the 5 nm-node silicon FET technology and below. Importantly, this image is taken in-situ during the tSPL patterning process, since thermal probes can also allow local nanoscale imaging (Methods). This feature enables localization of target regions on a chip with nanoscale precision without requiring sophisticated and costly pattern alignment procedures.
To demonstrate the ability of the NanoBioFET fabrication method to pattern relevant biomarkers with high reproducibility and precision, Figs. 1d and 1e present two fluorescence optical microscopy images of one-hundred squares (with 5 µm and 500 nm sides, respectively) of biotinylated anti-SARS-CoV-2 aptamers, which have been fluorescently tagged with a red dye (see Methods for details on the aptamers used here). These aptamer patterns have been produced first by exposing amine groups by tSPL on the surface of the PPA/PMCC polymer resist, and then by conjugating the amine groups to NHS-biotin, followed by streptavidin, and biotinylated aptamers (the details of the chemical functionalization steps are reported in the Methods). The PPA/PMCC double polymer stack is here spin-coated on a silicon oxide/silicon wafer.
In Figs. 1f and g, we show how the NanoBioFET fabrication process is implemented on a gFET array chip. For this purpose, we fabricate an array of four gFETs with a channel length of 1 µm, where each sensor FET is adjacent to a control FET. The PPA and PMCC resists are then spin-coated on the gFETs, and tSPL is used to remove PPA and pattern amine groups in the channel region of the two gFET sensors, leaving the FET controls unpatterned. In Figs. 1f and g we show, respectively, an in-situ tSPL topographical image, and an ex-situ friction atomic force microscopy (AFM) image of the resulting gFET sensors and controls after tSPL patterning. The graphene region underneath the polymer is indicated with a dashed red rectangle. In Fig. 1f, the tSPL topography image shows that the patterns above the channel region of the gFET sensors are at a depth of approximately 10 nm, corresponding to the thickness of the PPA film, which is sublimated during tSPL patterning. It is important to note that since tSPL allows in-situ imaging of the FET underneath the dual polymer stack, we are able to locate the channel region of each FET and pattern where required without the need of markers. The AFM friction image in Fig. 1g is particularly revealing since it shows clear friction contrast in the sensor area due to the change in hydrophilicity upon the thermal deprotection of the amine moiety. This agrees with a more hydrophilic surface where the amine groups have been exposed, and the consequent presence of larger friction forces at the nanoscale due to larger capillary forces [24, 33].
The NanoBioFET platform for parallel biochemical sensing
To fully exploit the potential of having a massive number of FET biosensors in a microchip, it is necessary to functionalize each FET with distinct bioreceptors so as to allow detection of different types of target biomolecules, such as different viruses. In Fig. 2, we demonstrate the capability of the NanoBioFET fabrication process to pattern each FET with an independent bioreceptor to permit parallel sensing on the same chip. Figure 2a shows a schematic representing the steps required for patterning the different FETs with distinct bioreceptors. Initially, we fabricate an array of FETs and we spin-coat a PPA/PMCC polymer stack on them. Then a first round of NanoBioFET fabrication, as depicted in Fig. 1b, is performed on FET-1 to attach bioreceptor-1 (red square), followed by a second round to attach bioreceptor-2 (green square) to FET-2, and so on until all FETs are functionalized up to the desired n-number of bioreceptors. Each round of NanoBioFET fabrication includes: first, in-situ tSPL topographical imaging of the surface to locate where the pattern needs to be made (e.g., the desired FET); second, tSPL local patterning of an individual FET channel; third, a series of biochemical functionalization steps, and selective attachment of the desired bioreceptor to the required FET as described in the Methods part.
In Fig. 2b we present a fluorescence optical microscopy image of biochemical patterns generated by four sequential rounds of NanoBioFET fabrication as depicted in Fig. 2a. In particular, Fig. 2b shows the fluorescence of four types of NHS-esters terminated dyes (red, yellow, green and sky-blue) attached directly to the amine moieties exposed during the tSPL process on the surface of the PPA/PMCC polymer resist deposited on a silicon oxide/Si wafer. Figure 2c shows the implementation of the multiplexed chemical patterning in an array of gFETs. Specifically, four representative gFETs channel regions have been functionalized with four different types of NHS-esters terminated dyes (red, yellow, green, and sky-blue) attached directly to the amine moieties exposed by tSPL on the surface of a PPA/PMCC polymer resist spin-coated on a gFET chip.
Figures 2d and e demonstrate the capability of the NanoBioFET fabrication method to produce independent patterns of different types of bioreceptors sensitive to different types of target molecules, e.g., different viruses. In particular, here we show a fluorescence image of patterns of two types of fluorescently labelled aptamers, influenza A anti-hemagglutinin (HA) aptamer tagged with a green fluorophore, and anti-SARS-CoV-2 aptamer (tagged with a red fluorophore). The patterns are created by exposing amine groups by tSPL, and subsequently by attaching NHS-ester biotin to the amine patterns. Biotin patterns are then exposed to streptavidin, and finally to the biotinylated HA aptamer (green). A second identical round of NanoBioFET fabrication is performed to attach the biotinylated CoV-2 aptamer (red) to the desired area on the surface. The details are reported in the Methods.
Figures 2e and f demonstrate the high spatial resolution with which patterns/bits of different bioreceptors can be fabricated on the channel of parallel FETs with this approach. In particular, following the same process as in Figs. 2d and e, we produce patterns of two types of aptamers (HA and CoV-2 aptamers). The fluorescence image in Fig. 2e shows green-aptamer and red-aptamer patterns with a “bit” dimension of 500 nm. Because of the limited resolution offered by optical microscopy, we also fabricate two-aptamer circle/dash patterns with a 20 nm width and a minimum 200 nm pitch, i.e., minimum distance between circle (HA aptamer) and dash (CoV-2 aptamer) pattern centers. We then image them in-situ by tSPL imaging (Fig. 2f). We perform three measurements on the PPA/PMCC surface. First, we image pattern type-circle after a first round of tSPL. Second, we functionalize pattern type-circle with NHS-biotin/streptavidin/HA aptamer and image the pattern region after a second round of tSPL to produce pattern type-dash. Third, we image the polymer surface after functionalization of pattern type-dash with NHS-biotin/streptavidin/CoV-2 aptamer. The cross-sections show the high registry and robustness of the fabrication process and the change in depth of the patterns after functionalization due to the filling of each pattern with the NHS-biotin/streptavidin/aptamer molecules (approximately 10–15 nm). The two types of patterns have been produced with different shapes to add clarity to the image and show that tSPL can also produce patterns at different depths and shape. See also supplementary Figure S8.
Electronic sensing using the NanoBioFET platform
Having established the versatility and nanoscale spatial precision of the NanoBioFET fabrication strategy, we next examine its feasibility in electronic detection of target analytes. As a proof-of-concept, we implement electronic sensors based on gFETs. Our sensing experiments are tailored for the detection of the SARS-CoV-2 virus, chosen as an example target species. This choice is motivated by the commercial availability of bioreceptors for this virus, including different antibodies and aptamers.
gFETs are promising biosensor candidates due to their potential for high sensitivity and ease of fabrication [13, 22, 34]. Like other FET-based biosensors, a bioreceptor-modified gFET translates the pathogen-bioreceptor interaction near the surface to a detectable electronic signal. Figure 3a shows the schematic illustration of an antibody-modified gFET. The sensor is solution-gated, where a fixed bias gate voltage (Vgs) is applied to the solution (300 mV in our experiments) using a Ag/AgCl reference electrode. A small bias voltage (Vds=50 mV) is simultaneously applied between the source and drain electrodes, generating a current flow (Ids) in the gFET, which is monitored in real time. The amplitude of Ids changes upon conjugation of target analytes (e.g., spike protein or virus) with bioreceptors, due to a change in electronic charge on the surface of the biosensor. Furthermore, the recorded Ids signal can be used to quantify the concentration of target analytes through creation of a sensitivity calibration curve, as we explain later.
However, a key experimental challenge in FET-based biosensing is the electronic screening of charges with increasing distance from the surface, characterized by the Debye length λDebye. A common approach for overcoming this limitation is to adjust the ionic strength of the buffer environment [35, 36], thereby increasing λDebye. In the experiments below, we adopt a similar strategy, modifying the buffer solution and its ionic strength based on the choice of the bioreceptor (i.e., antibody or aptamer).
Sensing using antibody-modified NanoBioFET
All electronic sensing experiments begin by employing the fabrication and biofunctionalization protocols described in Figs. 1 and 2, which involve anchoring NHS-biotin-streptavidin chains onto the thermochemically activated amine groups on the PMCC polymer, above the channel region of the gFETs. Our initial investigations focus on the use of biotinylated antibodies as a bioreceptor, which attach to the NHS-biotin-streptavidin chains. In this configuration, detecting an electronic signal induced by the antibody-analyte interaction requires λDebye of at least ~ 10 nm. To accommodate this requirement, we use a 1 mM HEPES buffer solution as the sensing environment (see Methods) [9]. Whereas a lower ionic strength enhances λDebye, the reduction of ion concentration in the sensing environment may negatively affect the efficacy of the antibody-analyte interaction.
We select biotinylated anti-SARS-CoV-2 spike RBD neutralizing antibody (see Methods) for these electronic sensing experiments. The feasibility of its binding affinity to SARS CoV-2 spike protein at 1mM HEPES buffer is confirmed by surface plasmon resonance (SPR) measurements (Fig. 3b). In these SPR experiments, the concentration of spike proteins is limited to a low nanomolar range, which is the typical sensitivity of this type of measurements [37, 38]. Following this confirmation, we proceed to perform the electronic sensing measurements with the NanoBioFET platform. In all sensing experiments, the bioreceptor-modified gFETs are placed in a microfluidic chamber (see Methods). We then perform an initial screening of a gFET sensor quality by measuring its transfer characteristics (Ids vs. Vgs) using a buffer solution gate. In Fig. 3c, we show the typical transfer characteristics of an antibody-modified gFET, obtained by sweeping the solution gate voltage, Vgs, and recording Ids at a fixed Vds of 50 mV. Vgs modulates the gFET charge carrier concentration and carrier type, from holes in the p-branch, to electrons in the n-branch, passing through the charge neutrality point (at VCNP). For simplicity the data are centered around VCNP. When an analyte is captured by the bioreceptor in the channel region, the local change in charge produces a shift of the Ids vs.Vgs characteristics and therefore a change in Ids is measured at fixed Vg.
We next monitor the real-time electronic response of a SARS-CoV-2 antibody-modified gFET sensor to different concentrations of spike protein. The experiment involves recording Ids continuously in time at a fixed Vgs of 300 mV while injecting analytes at different times into the microfluidic chamber. The objective of this experiment is to quantify the sensitivity of this antibody-modified gFET and evaluate its limit of detection. In Fig. 3d, we show the corresponding transient response of DIds/I0, where I0 is the initial Ids (i.e., at t = 0) and DIds is evaluated by subtracting I0 from the subsequently recorded Ids. We initially perform repeated injections of the buffer solution and monitor the gFET’s DIds response. The purpose of these injections is to record possible artifacts which might contribute to a false sensor response. The sensor response due to three buffer injections are marked with yellow shading in Fig. 3d. Although each injection of the buffer solution generates a small detectable response, they are consistent among the three injections and, more critically, do not cause a permanent shift in the DIds/I0 baseline. These observations give confidence that the artifacts of the injection process are negligible and temporary, and thus do not contribute to the steady-state sensor response due to the antibody-spike protein interactions. We then monitor the transient sensor response due to injections of the spike protein (see Methods for discussion on the concentrations). Upon each spike injection, marked with red arrows in Fig. 3d, a small bump is initially observable in the transient curve of the sensor response, associated with the artifact of the injection. However, this response is accompanied with a strong decrease in DIds/I0, that follows an apparent exponential behavior (marked with dashed exponential fits). The subsequent spike injection occurs once DIds/I0 establishes a new steady-state baseline. Each of the spike protein injections generates a qualitatively similar response, with increasing magnitude, as expected for increasing concentration of spike protein in the buffer solution.
Figure 3e shows the sensitivity plot of the antibody-modified gFET, plotting the sensor response (the amplitude of the exponential decay fitting function) against its corresponding spike concentration. Since the sensor response must be null when the target analyte concentration is zero, a linear fit to the data must go through the origin and we are hence able to make a meaningful fit, obtaining a sensitivity of 0.59 ± 0.04% aM. Analysis of the electronic noise in these measurements reveals a 36 nArms input-referred noise (0.3% of I0), corresponding to an estimated limit of detection of 1.5 aM (see Supplementary Note 2). The excellent sensitivity of these gFETs, which could be further optimized in terms of electrical characteristics, reinforces the prospects of NanoBioFETs as biosensors in experiments involving ultralow concentrations of analytes.
Sensing using aptamer-modified NanoBioFET
We next examine the versatility of the NanoBioFET platform in adapting aptamers as bioreceptors for detecting spike proteins. In recent years, aptamers have become increasingly appealing as capturing probes due to their cost-effectiveness and durability [7]. More critically, modifying FET-based sensors with aptamers has proven to be an effective strategy in significantly relaxing the requirements on λDebye and, consequently, the ionic strength of the sensing environment [39]. Recent demonstrations have revealed the utility of aptamer-modified FET sensors in detecting analytes at physiological ionic strength [8], which has a λDebye of 0.7 nm. The sensing mechanism of an aptamer-modified FET-based sensor is attributed to the fact that the analyte-induced conformational changes of the aptamer alter the surface charge within λDebye, generating a detectable electronic signal. In our experiments, explained below, we demonstrate the successful electronic detection of spike proteins in buffers solutions having a λDebye of ~ 2 nm.
We implement aptamer-modified gFETs following an identical tSPL fabrication and biofunctionalization procedure as in the experiments in Figs. 1 and 2, and we use a biotinylated anti-SARS-CoV-2 aptamer as bioreceptor (see Methods for details). Before the electrical sensing experiments, we employ fluorescent microscopy to confirm the aptamer attachment in the channel region of the gFETs designated as biosensors. Indeed, the strong fluorescence in the channel region of an aptamer-modified gFET (see left panel in Fig. 4b) confirms the effectiveness of our procedure in locally attaching aptamers. In this experiment, we also demonstrate the versatility of this approach in implementing control gFETs on the same chip by leveraging the spatial-selective biofunctionalization capability of tSPL. Control devices are produced simply by skipping the tSPL step in the channel region of a few select gFETs, while subjecting these gFETs to the same subsequent surface chemistry treatments as sensor gFETs. The fluorescent microscopy results for the control gFET (see right panel in Fig. 4b) confirm the chemical inactivity of the channel region in the control gFET with minimal non-specific binding.
In Fig. 4c, we present SPR experiments confirming the binding between the anti-SARS-CoV-2 aptamer and spike protein in 0.1X PBS, corresponding to a λDebye of approximately 2 nm. The subsequent electronic sensing experiments in a microfluidic chamber demonstrate the ability of aptamer-modified gFETs in generating detectable electronic signals in response to spike protein injections in the same buffer concentrations (see Fig. 4d). The simultaneous monitoring of an adjacent control device in this experiment provides confidence about the fidelity of the electronic signals generated by the gFET biosensor. This key feature of the NanoBioFET platform in enabling differential detection and simultaneous monitoring of non-specific binding is an important step toward achieving robust analyte detection using FET-based biosensors.
A closer look at the results in Fig. 4d reveals two important observations. The first observation is the significantly weaker signal amplitude of the aptamer-modified gFET compared to its antibody-modified counterpart in Fig. 3d. Whereas the antibody-modified gFET generates a DIds/I0 of 2.5% in response to 5 aM of spike concentration, the aptamer-modified counterpart produces an order of magnitude weaker signal amplitude when exposed to 500 aM of spike protein. We attribute this characteristic primarily to the significantly smaller λDebye at 0.1X PBS. We expect that ongoing research in the field, focused on increasing the λDebye at a given ionic strength [36] and developing alternative chemical conjugation strategies beyond biotin-streptavidin will directly benefit future experiments utilizing aptamer-modified gFETs. The second observation pertains to the relationship between the signal amplitude and the spike protein concentration. The data indicate a nearly diminishing response with the subsequent spike protein injections at higher concentrations. This observation suggests that the capturing aptamers on the gFET are reaching full occupancy, wherein the captured surface proteins block the interactions of incoming proteins with the surface probes.
Evaluation of NanoBioFET platform using live human viral particles
Following the success of spike protein detection with bioreceptor-modified gFETs, we perform a final test with human live SARS-CoV-2 viral particles and the SARS-CoV-2 antibody as bioreceptor from earlier, evaluating sensitivity to low viral loads and selectivity of the response to specific viruses. Additionally, the experiments in Fig. 3 confirm the high sensitivity of antibody-modified gFETs in detecting low concentrations of spike proteins. Therefore, we employ the antibody-modified NanoBioFET platform in experiments involving live viral particle detection.
The measurement setup and procedure are nearly identical to that for the antibody–spike protein measurements earlier, with a 1 mM HEPES buffer (see Fig. 5a and Methods for details). We monitor the temporal changes in Ids during the course of the sensing experiment. The experimental sensing procedure involves injection of the blank virus medium at the beginning of the experiments, followed by a few alternating injections of SARS-CoV-2 virus and the human H1N1 influenza virus (see Methods for details on these viruses). Figure 5b shows the transient response of the antibody-modified gFET with live virus injections in 1mM HEPES. Injections of virus medium (black circle), SARS-CoV-2 virus (red diamond), and H1N1 virus (green star) are marked in Fig. 5b. The data demonstrate the sensitive and selective detection by the SARS-CoV-2 antibody-modified gFET. The SARS-CoV-2 virus (red diamond) and H1N1 virus (green star) in Fig. 5 show that the SARS-CoV-2 virus repeatedly produces an exponential-like response in the sensor, whereas the H1N1 virus (which we use as a negative control) or buffer produce no response. The first four virus injections are at a concentration of 20 TCID50/ml and the last at 200 TCID50/ml, estimated to be about 10 infectious virus particles per ml, demonstrating ultra-sensitive detection of the live virus. The insensitivity of the sensor to H1N1 injections highlights the selectivity of the platform.