Biosensors based on fluorescent gels employ different approaches to analyte detection, but all of them involve the recording of changes in the fluorescent properties of the gel. Depending on the analyte detected and the design of the biosensor, the changes in the optical properties may be of two types: first, quenching of NC fluorescence due to energy transfer (e.g., via the Förster resonance energy transfer, FRET), structural degradation of the fluorescent NCs, or their aggregation due to gel structure disruption; second, changes in the fluorescence spectrum due to the activation of new fluorescent labels. The specific mechanism of the change in the optical properties often depends not only on the properties of the fluorescent NCs and the gel, but also on the characteristics of the analyte and additional sensory molecules contained in the biosensor. In some cases, specific binding of the analyte is ensured by NC functionalization with surface ligands, such as cyclodextrins [
28] or (2-hydroxyethyl) dithiocarbamate [
29]. However, this is applicable almost exclusively to relatively simple analytes, such as metal ions [
30], polyaromatic molecules [
31], and NO
2– [
32]. Specific recognition of more complex organic molecules, such as antibodies or other proteins, requires the use of affinity molecules, e.g., antibodies. The main principles of detection used in fluorescent hydrogel biosensors are shown in
Figure 2. One of the simplest detection principles (
Figure 2a) is used with analytes that disrupt the gel structure upon contact, which results in NC aggregation and decreased fluorescence intensity. This detection principle was used by Bhattacharya et al. [
33] for the detection of bacteria. They made a fluorescent gel from 6-O-(O-O′-dilauroyltharyl)-D-glucose and carbon NCs and, after its polymerization, added cultures of
Bacillus and
Staphylococcus strains. During the growth of the culture, the bacterial cells secreted esterases catalyzing the ester cleavage reaction. As a result, the fluorescence signal decreased, depending on the number of added bacteria, due to the degradation of the gel matrix and aggregation of the NCs. It should be noted that this approach entails irreversible destruction of the biosensor, which makes biosensors of this type hardly practicable. The detection principle shown in
Figure 2b is applicable to analytes that either cause specific quenching of NC fluorescence via various excitation relaxation mechanisms or fluoresce themselves (i.e., they are optically active). For example, metal ions can act as electron acceptors upon their reduction, thereby decreasing the NC fluorescence intensity [
34]. Many organic compounds can act as electron acceptors in the Förster resonance energy transfer, which also reduces the NC fluorescence intensity or leads to the formation of an additional fluorescence peak [
35]. This principle is often used for the detection of metal ions, the selectivity being ensured by functionalization of the NC surface with a ligand that selectively interacts with a specific ion, e.g., Fe
3+ [
36], Cr
6+ [
37], or Cu
2+ [
38].
Figure 2c shows the scheme for detecting optically inactive analytes. In this case, auxiliary optically active labels are used that specifically bind the analyte and either quench the optical signal or fluoresce in a different spectral region. Antibodies or oligonucleotides can be used as capture molecules [
39], and organic dyes [
40], plasmonic nanoparticles [
41], graphene [
42], or other compounds causing changes in the fluorescence of hydrogels [
43] are used as optically active labels. In the fourth detection method (
Figure 2d), two enzymes, oxidase and horseradish peroxidase, are introduced into the pores of the fluorescent gel. The former specifically oxidizes the analyte to form hydrogen peroxide, and the latter uses hydrogen peroxide as a cofactor to catalyze the formation of OH
– radicals, which weaken the hydrogel fluorescence [
44], and the oxidation of the chromogenic dye, which shifts the spectral maximum of the absorption signal, also contributing to the quenching of the gel fluorescence [
45]. For example, Cho et al. [
44] developed a glucose biosensor operating on this principle. They immobilized fluorescent carbon NCs, rhodamine 6G, glucose oxidase, and horseradish peroxidase in a hydrogel. Upon excitation at a wavelength of 360 nm, the blue fluorescence of the carbon NCs was quenched by the bienzymatic reaction with glucose and the formation of OH
– radicals, while the fluorescence of rhodamine 6G was used for calibration because it did not depend on the amount of glucose.
The miniature size of the biosensors imposes significant limitations on the area available for immobilization of sensor or affinity labels recognizing specific analytes. Switching from the 2D detection model to the 3D one by using 3D polymer matrices not only increases the capacity for binding the sensor and affinity labels, but also preserves the structure of the molecules, which could denature upon immobilization on a flat surface [
46]. This prevents the deterioration of the properties necessary for sensing, such as specificity and sensitivity [
47]. All this makes it possible to increase the detection sensitivity of microfluidic biosensors compared to their full-size counterparts. When the signal or recognition labels are immobilized in the 3D structure of the hydrogel, their orientation becomes irrelevant, because the analyte passes on all sides of them in any case, which increases the probability of the detection. For example, Gao et al. [
48] have shown that the efficiency of DNA hybridization on a surface is 20–40 times lower than in a solution. When antibodies are immobilized on a flat surface, they can also lose specificity and affinity for their antigens, which is confirmed by numerous examples reviewed by Welch et al. [
49]. Feng et al. [
50] have shown that 3D arrangement of antibodies even on a flat surface can increase the detection sensitivity by a factor of 64. In addition, the hydrogel structure itself can perform a sensory function. For example, the selectivity for the analyte size or selectivity of analyte–hydrogel interaction can be increased, or nonspecific binding of the analyte decreased, by varying the pore size of the 3D matrix or by selecting materials with different physical and chemical properties for its formation. Yuan et al. [
51] developed NC hydrogels with encapsulated tyrosinase (TYR)for biosensing of dopamine (
Figure 3). The use of a neutral phosphate-buffered saline to dissolve the precipitated CdTe NCs capped with mercaptosuccinic acid (MSA) sufficiently shortened the NC gelation time (to several days), and the sol–gel transition was also observed in the as-prepared NC gels. The resulting gels had pores ranging from 10 to 50 nm in diameter, and the enzyme could be encapsulated in the mesopores of the gel network during the gelation. The encapsulation of TYR was confirmed by atomic force microscopy and the test reaction of tyrosinase-catalyzed oxidation of catechol. The enzymatic activity of TYR in the hydrogel was preserved even after immersion in a potassium buffer solution for at least one week. Tyrosinase catalyzes the oxidation of dopamine to dopamine-o-quinone, which quenches NC fluorescence. Addition of dopamine quenched the NC fluorescence in the tyrosinase-embedded hydrogel, but it had no obvious effect on the pure NC hydrogel in the absence of tyrosinase. The detection limit for dopamine was found to be 5.0×10
−8 mol L
−1, the practicable range of detection being from 5.0×10
−5 to 1.0×10
−3 mol L
−1. This dopamine detection limit was four times lower than that determined for the CdTe NC sol [
52] and comparable with those of electrochemical assays [
53].
Thus, the use of a 3D matrix for immobilizing the labels and detecting the analytes could significantly increase the detection sensitivity due to both increased numbers of fluorescent and affinity labels and an increased efficiency of binding the analyte by the affinity labels.