Surachet
Duanghathaipornsuk
a,
Dong-Shik
Kim
a,
Tamara L.
Phares
b,
Cheng-Han
Li
c,
Joerg R.
Jinschek
c and
Ana C.
Alba-Rubio
*a
aDepartment of Chemical Engineering, The University of Toledo, Toledo, OH 43606, USA. E-mail: ana.albarubio@utoledo.edu
bDepartment of Bioengineering, The University of Toledo, Toledo, OH 43606, USA
cDepartment of Materials Science and Engineering, The Ohio State University, Columbus, OH 43210, USA
First published on 25th February 2021
It is well known that an excess of hydroxyl radicals (˙OH) in the human body is responsible for oxidative stress-related diseases. An understanding of the relationship between the concentration of ˙OH and those diseases could contribute to better diagnosis and prevention. Here we present a supersensitive nanosensor integrated with an electrochemical method to measure the concentration of ˙OH in vitro. The electrochemical sensor consists of a composite comprised of ultrasmall cerium oxide nanoclusters (<2 nm) grafted to a highly conductive carbon deposited on a screen-printed carbon electrode (SPCE). Cyclic voltammetry (CV) and electrochemical impedance spectroscopy (EIS) were used to analyze the interaction between cerium oxide nanoclusters and ˙OH. The CV results demonstrated that this electrochemical sensor had the capacity of detecting ˙OH with a high degree of accuracy and selectivity, achieving a consistent performance. Additionally, EIS results confirmed that our electrochemical sensor was able to differentiate ˙OH from hydrogen peroxide (H2O2), which is another common reactive oxygen species (ROS) found in the human body. The limit of detection (LOD) observed with this electrochemical sensor was of 0.6 μM. Furthermore, this nanosized cerium oxide-based electrochemical sensor successfully detected in vitro the presence of ˙OH in preosteoblast cells from newborn mouse bone tissue. The supersensitive electrochemical sensor is expected to be beneficially used in multiple applications, including medical diagnosis, fuel–cell technology, and food and cosmetic industries.
Various researchers have integrated sensing elements such as proteins20,21 and metal oxides nanoparticles22,23 with electrochemical techniques to develop nanosensors for the detection of chemical species of interest. The use of electrochemical techniques posseses several advantages over other methods, as the sensitivity and selectivity can be easily controlled by modifying the sensing element on the surface of the electrode.24,25 Morever, the electrochemical techniques can provide a real-time detection, which is especially important when monitoring species with short lifetime.26 Inspired by previous findings, this study reports the use of ultrasmall cerium oxide nanoclusters as the sensing element for the development of a highly sensitive and selective electrochemical sensor for ˙OH detection. According to former reports, cerium oxide nanoparticles (CeNPs) demonstrated a selective removal of ˙OH in living tissues.27,28 The scavenge of ˙OH by CeNPs is based on the dual oxidation state of cerium oxide, which can be easily switched between Ce3+ and Ce4+ by oxidizing or reducing species in the medium, respectively.29,30Fig. 1 shows the mechanism for which Ce3+ sites on CeNPs specifically reacts with ˙OH via the oxidation reaction turning into Ce4+ sites. After that, Ce4+ can be reversibly reduced to Ce3+via the reduction reaction.29,31,32 The redox reaction between CeNPs (sensing element) and ˙OH (analyte) permits the use of the electrochemical technique for the detection of ˙OH.
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| Fig. 1 Redox reaction between CeNPs and hydroxyl radicals (˙OH). Reprinted from S. Duanghathaipornsuk, F. A. O. Alateeq, S. S. Kim, D.-S. Kim and A. C. Alba-Rubio, The effects of size and content of cerium oxide nanoparticles on a composite sensor for hydroxyl radicals detection, Sens. Actuators, B, 321, 128467, Copyright (2020), with permission from Elsevier.33 | ||
As Ce3+ sites are responsible for the reaction with ˙OH, several research groups have seeked to maximize the concentration of Ce3+ sites on CeNPs to improve their ˙OH scavenging capacity.33,34 In order to minimize the size of CeNPs, and thus, maximize the amount of Ce3+ sites for ˙OH scavenging and detection, we employed Surface Organometallic Chemistry (SOMC) to obtain nanosized CeOx.35,36 We hypothesized that the size and dispersion of the CeOx nanoclusters could be adjusted by controlling the loading of the organometallic precursor. Even though the size and dispersion of the CeOx nanoclusters could be controlled, the conductivity of the electrochemical sensor is also essential to provide a high sensitivity. For this reason, we decided to anchor CeOx nanoclusters onto a highly-conductive carbon using a SOMC method.37,38 The successful development of a supersensitive composite sensor for ˙OH detection is expected to help understand the relationship between the ˙OH concentration and some oxidative stress-related diseases, which in turn would facilitate more effective prevention and treatments.
:
300 wt ratio) to make a thin pellet. Moreover, the samples were characterized using a TA Instruments Q50 thermogravimetric analyzer (TGA) to determine the required temperature to remove the ligands of the CeOx precursor. To do so, 12 mg of sample was heated from 25 to 1200 °C with a heating ramp of 10 °C min−1 under 50 mL min−1 N2 flow. The size and the dispersion of the CeOx nanoclusters on the carbon surface were studied by high-angle annular dark-field scanning transmission electron microscopy (HAADF-STEM) with collection angles of 106–200 mrad using a FEI Titan3™ G2 60–300 S/TEM and by energy dispersive X-ray spectroscopy (EDS) elemental mapping using a probe-corrected Thermo Scientific Themis-Z™ STEM. For that, the composite powders were dispersed in ethanol followed by sonication for 10 min. After that, the dispersion was dropped onto 300-mesh copper TEM grids coated with lacey carbon films. The actual loading of cerium (as CeOx nanoclusters) on the carbon support was determined by inductively coupled plasma optical emission spectrometry (ICP-OES) at Galbraith Laboratories, Inc. Finally, the surface contents of Ce3+ and Ce4+ were determined from spectra obtained in a Kratos Axis Ultra XPS with a monochromatic Al X-ray source operating at 10 mA and 15 kV.
000 rpm for 15 min to separate MC3T3 from the solution. The collected MC3T3 (∼6 × 106 cells) were resuspended in 1 mL of 0.01 M phosphate-buffered saline (PBS) to detect ˙OH released from MC3T3. The signal from the sensor was analyzed using CV and EIS. For CV and EIS analyses, 200 μL of the MC3T3 suspension was dropped on the surface of the 0.64 wt% Ce/carbon-modified electrode for the first cycle. Subsequent CV and EIS cycles were performed by dropping 100 μL of 0.0003, 0.004, and 0.05 mg mL−1 lipopolysaccharides (LPS) from E. Coli solutions in PBS, respectively, in order to induce additional oxidative stress. To compare the signals obtained from the MC3T3 suspension with the ˙OH signal generated by the Fenton reaction in a PBS solution, 60 mL of a 0.01 M PBS solution containing 10 mM iron(II) sulfate was degassed by flowing argon for 2 h to dissolve FeSO4·7H2O. After that, 1 mL of a 610 mM H2O2 solution in 0.01 M PBS was injected through a septum to produce ˙OH. Then, the 0.64 wt% Ce/carbon-modified electrode was submerged into the Fenton reaction to detect the presence of ˙OH. The experimental conditions for CV were described in the previous section, and the same procedure was used to perform EIS. The impedance changes and phase angle shifts in terms of frequencies in Bode plots were used to identify the presence of ˙OH. All EIS experiments were run in a frequency range of 0.01–10
000 Hz with an alternating-current (AC) potential of Vrms = 5 mV and direct-current (DC) potential of 0.23 V.
O symmetric deformation of the carboxyl groups, respectively.39,40 Furthermore, it presents two bands at 1580 and 1735 cm−1, which can be attributed to the C
C stretching vibration and C
O symmetric stretching mode, respectively.41,42 The presence of those four bands after the acid treatment confirms an increase in the number of carboxyl groups on the surface of carbon.
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| Fig. 2 FTIR spectra of (a) carbon, (b) acid-treated carbon, and (c) CeOx nanoclusters/carbon composite (0.64 wt% Ce) after thermal treatment for ligands removal. | ||
Once confirmed the anchorage of the CeOx precursor on the carbon surface, we synthesized a series of composites with different loadings of tris(cyclopentadienyl)cerium(III), and these were labelled as X wt% Ce/Carbon, where X wt% Ce represents the theoretical Ce loading. Then, prior to the thermal treatment for ligands removal (Fig. S1†), we used TGA for further characterization of the materials. Fig. 3 compares the TGA profiles obtained with acid-treated carbon, 12.3, 18.4, and 24.6 wt% Ce/Carbon. As it can be seen in Fig. 3b, the acid-treated carbon shows two significant derivative weight losses at around 100 and 200–300 °C, which can be attributed to the loss of water and the degradation of the carboxyl groups, respectively.43 On the other hand, when the CeOx organometallic precursor is anchored to the carbon surface, there are four significant weight losses at around 100, 300–400, 400–500, and 700–1100 °C. As before, the first one corresponds to the loss of water. The derivative weight losses at 300–400 °C and 400–500 °C could be attributed to the thermal decomposition of the CeOx precursor physisorbed on the surface of the carbon support and the removal of the precursor ligands, respectively. And lastly, the derivative weight loss at 700–1100 °C could be ascribed to the decomposition of the CeOx precursor bound to the carbon surface. With the exception of the evolution of water of hydration at around 100 °C, it is noted that the area under every derivative weight loss increases with the loading of CeOx precursor added (Fig. 3b), which could be attributed to a large fraction of the CeOx precursor anchored to the carboxyl groups on carbon. Additionally, the higher evolution at 300–400 °C (physisorbed precursor) observed with 24.6 wt% Ce/Carbon could be explained as the saturation of the carboxyl groups on carbon due to efficient anchorage of the precursor, as it can be infered by the similar decomposition obtained with 18.4 and 24.6 wt% Ce/Carbon at higher temperatures (700–1100 °C). Therefore, TGA also confirmed the success of the SOMC method. It also helped us select the right temperature (400 °C) for the ligands removal from the CeOx precursor for the generation of the CeOx nanoclusters on the carbon surface (Fig. S1†).
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| Fig. 3 TGA results obtained with acid-treated carbon and 12.3, 18.4, and 24.6 wt% Ce/Carbon composites (before thermal treatment for ligands removal). | ||
ICP-OES was used to determine the actual Ce loading in the form of CeOx nanoclusters on the surface of the carbon support (Table 1). As shown in Table 1, the Ce loading increases with the amount of CeOx precursor added during the synthesis. While there was a good correlation between the theoretical and the actual Ce loadings when using diluted solutions of the CeOx precursor, a lower efficiency on the immobilization of the CeOx precursor was observed at higher loadings (Fig. S2†). For example, for a theoretical Ce loading of 38.9 wt%, the actual loading determined by ICP-OES was of 20.8 wt%, which is 54% lower than the theoretical one. This deviation is likely due to the saturation of the carboxyl groups on the carbon surface for efficient anchorage of the CeOx precursor. As a result, a fraction of the CeOx precursor is regarded weakly adsorbed on the carbon surface without chemically interacting with the support, being this easily decomposed during the thermal treatment for the removal of ligands. This is consistent with the TGA data presented in Fig. 3.
| Sample (theoretical Ce loading) | Actual Ce loading (wt%) |
|---|---|
| 0.64 wt% Ce/Carbon | 0.49 |
| 2.5 wt% Ce/Carbon | 3.34 |
| 18.4 wt% Ce/Carbon | 13.50 |
| 38.9 wt% Ce/Carbon | 20.80 |
As previously stated, it has been reported in the literature that there is a correlation between the concentrations of Ce3+ and Ce4+ species and the size of CeNPs, being the smaller ones richer in Ce3+, which are the active species for ˙OH scavenging and detection.31,44 In order to estimate the amount of active sites in our CeOx nanoclusters/carbon composites, we also characterized them by XPS. Fig. S3† shows the deconvolution of the XPS spectra obtained with the different CeOx nanoclusters/carbon composites. These spectra are composed of two multiplets (u and v) that correspond to the Ce 3d3/2 and Ce 3d5/2 spin–orbit components, respectively. While v0, v′, u0, and u′ represent the characteristic peaks of Ce3+, v, v′′, v′′′, u, u′′, and u′′′ represent those of Ce4+. Table 2 presents a summary of the results obtained from the deconvolution of these spectra, in which the abundance of Ce3+ sites was calculated as ([Ce3+]/([Ce3+] + [Ce4+])) × 100, where [Ce3+] represents the sum of the areas of the Ce3+ peaks (i.e., v0 + v′ + u0 + u′) and [Ce4+] represents the sum of the areas of the Ce4+ peaks (i.e., v + v′′ + v′′′ + u + u′′ + u′′′). As it can be seen in Table 2, there is a clear correlation between the Ce loading and the Ce3+/Ce4+ ratio, which provides additional information about the increased size of the CeOx nanoclusters at higher loadings. Likewise, the 0.64 wt% Ce/Carbon composite showed the highest content of Ce3+ sites due to the smaller size of the CeOx nanoclusters (higher dispersion). Remarkably, the SOMC method allowed us to obtain a Ce3+ content of 46.3%, the highest found in the literature when compared to previous reports that used different synthesis methods.30,45,46 Therefore, it can be concluded that the size of the CeOx nanoclusters increases with the loading of CeOx precursor, likely due to the saturation of the surface and agglomeration of the nanoclusters at higher loadings, which becomes significant on the 38.9 wt% Ce/Carbon composite.
| Sample (theoretical Ce loading) | % Ce3+ | % Ce4+ | Ce3+/Ce4+ |
|---|---|---|---|
| 0.64 wt% Ce/Carbon | 46.3 | 53.7 | 0.86 |
| 2.5 wt% Ce/Carbon | 43.4 | 56.6 | 0.77 |
| 18.4 wt% Ce/Carbon | 42.5 | 57.5 | 0.74 |
| 38.9 wt% Ce/Carbon | 29.0 | 71.0 | 0.41 |
Fig. 4 shows some STEM images of the 0.64 wt% Ce/Carbon (Fig. 4a) and 18.4 wt% Ce/Carbon (Fig. 4b) composites. Even when there is an uniform distribution of CeOx nanoclusters on carbon in both samples, it is evident the high degree of agglomeration and lower dispersion on the 18.4 wt% Ce/Carbon sample (Fig. 4b). This is in agreement with the lower content of Ce3+ observed on the composites with higher CeOx loadings (Table 2). In contrast, we found ultrasmall well-dispersed CeOx nanoclusters on the 0.64 wt% Ce/Carbon sample (Fig. 4a). The high dispersion of the CeOx nanoclusters on that sample was also confirmed by EDS mapping (Fig. S4†).
ΔA obtained with the different CeOx nanoclusters/carbon samples have also been plotted in Fig. 6a for easier comparison. As it can be seen, the electrode modified with the highest CeOx loading (38.9 wt% Ce/Carbon) demonstrated a four times lower response (4 × 10−5 A) than the 18.4 wt% Ce/Carbon composite. As previously stated, the lower redox response can be attributed to the high degree of agglomeration and lower content of Ce3+ sites, as shown in Table 2.
It should be noted that even though the 2.5 and 18.4 wt% Ce/Carbon composites present similar Ce3+ contents, 43.4 and 42.5%, respectively, the latter resulted in a much higher redox response (1.6 × 10−4 A) compared to that obtained with the 2.5 wt% Ce/Carbon composite (1.1 × 10−4 A). This is due to the higher loading of CeOx nanoclusters that provide a larger number of Ce3+ active sites to interact with ˙OH. In order to compare the efficiency of the different composites for the detection of ˙OH, ΔAs in Fig. 6a were normalized per mass of Ce on the composite, and plotted in Fig. 6b. Even when the highest sensor response was obtained with the 18.4 wt% Ce/Carbon composite (Fig. 6a), the 0.64 wt% Ce/Carbon showed to be the most efficient, as it provided the highest reactivity per gram of Ce used (Fig. 6b), which is beneficial from an economic point of view. As shown in Fig. 6b, the ΔA per gram of Ce was of 20 mA g−1 with the 0.64 wt% Ce/Carbon composite, while it was of 0.15 mA g−1 with the 38.9 wt% Ce/Carbon sample, so that means that 1 g of Ce as CeOx nanoclusters on 0.64 wt% Ce/Carbon is 133 times more reactive towards ˙OH than the 38.9 wt% Ce/Carbon composite due to the small size of the CeOx nanoclusters, the higher content of active sites (Ce3+), and the lower degree of agglomeration. As the 0.64 wt% Ce/Carbon composite showed the highest efficiency (ΔA per gram of Ce), we used this material to further investigate the sensor response towards different concentrations of ˙OH generated from the Fenton reaction (Fig. S5†). As it can be seen in Fig. S5,† there are two distinctive regions: a linear relationship at low ˙OH concentrations (0–1 mM) and another that deviates from the linearity at high ˙OH concentrations, likely due to the lack of enough Ce3+ sites (due to the low CeOx loading) for complete ˙OH scavenging and detection. By using the linear relationship at low ˙OH concentrations, we obtained a limit of detection (LOD) as low as 0.6 μM, which is regarded as highly sensitive compared to others reported in the literature, as shown in Table 3.
| Sensor | Linear range (M) | LOD (M) | Ref. |
|---|---|---|---|
| CeNPs/GO-GCE | 1 × 10−5 to 1 × 10−3 | 8.5 × 10−5 | 33 |
| N–C/AuNPs/DNA/MCH/GCC | 5 × 10−5 to 5 × 10−4 | 2.5 × 10−5 | 47 |
| NPCN/PGE | 1 × 10−6 to 1 × 10−5 | 1.0 × 10−6 | 48 |
| Graphene/Au/Cys-PP-Zn2+ | 1 × 10−7 to 1 × 10−4 | 1.0 × 10−10 | 49 |
| Ce/carbon/GCE | 1 × 10−5 to 1 × 10−3 | 6.0 × 10−7 | This work |
In terms of the sensor selectivity, the 0.64 wt% Ce/Carbon-modified electrode also showed a distinctive response toward ˙OH when compared to a similar oxidizing chemical as H2O2. As shown in Fig. 7, the pattern of the phase angle change for ˙OH generated from the Fenton reaction is significantly different than that for H2O2. It is concluded that our composite sensor is not only highly sensitive, but it is also able to distinguish ˙OH from another similar oxidizing chemical such as H2O2. It is noted that MC3T3 + LPS shows a similar pattern of phase angle shift as ˙OH generated from the Fenton reaction, which confirms the detection of ˙OH released from the cells. For ˙OH, phase angle shifts occur at 0.06 and 0.3 Hz (Fenton reaction) and 0.16 and 0.6 Hz (cell + LPS), whereas only a shift was observed at 0.5 Hz for H2O2.
In order to further study the induced oxidative stress in MC3T3 by the addition of LPS, CV was performed in the presence of different concentrations of LPS: 0.0001, 0.001, and 0.01 mg mL−1. These low concentrations were chosen to promote the oxidative stress and the generation of ˙OH without significant cells death.50 As previously stated, these experiments were carried out sequentially by the addition of further volumes of LPS solutions in PBS. Thus, the first CV curve was recorded after dropping 200 μL of MC3T3 in PBS onto the electrode. For the second one, 100 μL of a 0.0003 mg mL−1 LPS solution in PBS was added onto the previous droplet (200 μL) to reach an overall concentration of 0.0001 mg mL−1 LPS. Likewise, for the third cycle, 100 μL of a 0.004 mg mL−1 LPS solution in PBS was added onto the previous droplet (300 μL) to achieve a concentration of 0.001 mg mL−1 LPS. Finally, for the fourth cycle, 100 μL of a 0.05 mg mL−1 LPS solution in PBS was added onto the previous droplet (400 μL) to make a final concentration of 0.01 mg mL−1 LPS. As expected, the current response increased with the addition of LPS (Fig. 8a) as a result of the increased generation of ˙OH due to the additional induced oxidative stress of MC3T3. In order to account for the dilution effect on the second, third, and fourth cycles, Fig. 8b shows the current response normalized by the concentration of MC3T3, which was calculated in terms of the number of cells per droplet volume in every cycle. As it can be seen in Fig. 8b, the 0.64 wt% Ce/Carbon-modified electrode was able to detect the increased concentration of ˙OH in MC3T3 by the addition of LPS. It is noted that the sensor produced a proportional redox response to the increase of LPS, rising by 1.9 × 10−9 A per count per μL every time that the LPS concentration was increased in an order of magnitude. These results demonstrate the high sensitivity and selectivity of the sensor for the in vitro detection of ˙OH in biological systems.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/d1nr00015b |
| This journal is © The Royal Society of Chemistry 2021 |