Yang
Ling‡
ab,
Tiantian
Cao‡
a,
Libin
Liu
c,
Jingli
Xu
a,
Jing
Zheng
a,
Jiaxing
Li
d and
Min
Zhang
*a
aCollege of Chemistry and Chemical Enginerring, Shanghai University of Engineering Science, Shanghai 201620, P. R. China. E-mail: zhangmin@sues.edu.cn
bInstitute for Sustainable Energy/College of Sciences, Shanghai University, No. 99, Shangda Road, Shanghai 200444, P. R. China
cSchool of Chemistry and Pharmaceutical Engineering, Qilu University of Technology (Shandong Academy of Sciences), Jinan 250353, China
dInstitute of Plasma Physics, Chinese Academy of Sciences, P. O. Box 1126, 230031 Hefei, P. R. China
First published on 20th July 2020
MoS2-based hybrids have aroused great interest for their outstanding performance in the application fields of biochemical sensing, catalysis and energy storage. Herein, we present a facile strategy to fabricate hierarchical microtubes by cultivating a MoS2 sheet-like nanostructure on polypyrrole microtubes (designated as PPy@MoS2 microtubes) using MoO3@PPy micro-cables as self-sacrificial templates. Such a dissolution–regrowth mechanism is demonstrated for the formation of hierarchical PPy@MoS2 microtubes by studying the morphology of the intermediate products in the process of the sulfidation reaction. The PPy microtubes are able to effectively improve the electrical conductivity of the hybrid architecture and greatly alleviate the agglomeration of the MoS2 nanosheets. Notably, the sheet-like MoS2 nanostructure can load more noble metal nanoparticles (NPs) owing to MoS2 released photogenerated electrons irradiated by light. Then, metal (Ag, Au, and Pd) NPs are reduced and in situ decorated on PPy@MoS2 microtubes, thus forming ternary PPy@MoS2@Ag, Au, and Pd nanohybrids, respectively. This decoration method also expands the wide range of application fields of PPy@MoS2. As a proof of application, the ternary PPy@MoS2@Au hybrids reveal excellent enzyme-like catalytic performance. Owing to the high coverage of Au NPs as well as one dimensional hierarchical MoS2-based ternary unique structures, the resultant PPy@MoS2@Au hybrid composites exhibited synergistically enhanced peroxidase-like catalytic activity relative to MoS2, MoS2@Au, and PPy@MoS2 alone, demonstrating the remarkable prospects of MoS2-based hybrids in chemical/biological molecule sensing application.
Molybdenum disulfide (MoS2), as a typical two dimensional (2D) material, has demonstrated great potential in various application fields, including sensing,11 electrocatalysis,12 and energy storage.13 To improve the poor electronic conductivity and provide other functionalities of MoS2, decoration of MoS2 materials with noble metal NPs has aroused great interest in the application of catalysis, biosensing etc. Notably, the noble metal NPs can be in situ generated on the surface of MoS2 nanosheets without using an extra reducing agent, greatly facilitating the preparation process. However, the individual MoS2 nanosheets suffered from fewer accessible active sites, and the high surface energy and interlayer van der Waals interaction caused serious aggregation of MoS2 layers. These greatly impede their decoration on noble metal NPs. To overcome these problems, many strategies have been developed to stabilize the individual MoS2 nanosheet with more exposed active sites. The most commonly used method is to decorate the 2D MoS2 nanosheets with carbonaceous materials,14,15 conductive polymers16 and metal oxides/sulfides,17–19 which could serve as supports to prevent the aggregation of MoS2. Among these backbones, the conducting polymers (CPs) are widely employed to fabricate functional CPs@MoS2 owing to their high electrical and thermal conductivity, low cost and good mechanical strength. Moreover, CPs offer a desirable matrix toward fast electron transport in the faradaic redox reaction. Therefore, hybridizing MoS2 nanosheets with CPs, especially polypyrrole (PPy), so as to improve the charge mobility and long-term stability, would be expected to obtain satisfactory overall electrochemical performance.20 For instance, Sun et al. have fabricated ultrathin MoS2/N-doped carbon nanowires with a largely expanded (002) plane of MoS2 using PPy@MoS2 as a precursor, which exhibited excellent rate capabilities and long-term durability as an anode for LIBs. However, the formation mechanism of PPy@MoS2 is not clearly explored.21 Chang et al. have deposited MoS2 nanosheets on the PPy nanotubes by a facile hydrothermal method, which showed enhanced electrochemical performance as supercapacitor electrodes, but the experimental procedures are complex and time-consuming due to the preparation of PPy nanotubes first.22,23 Thus, it is highly desired but remains challenging to develop a facile strategy for the fabrication of one dimensional hierarchical architectures with highly dispersed MoS2 immobilized on conducting polymers.
On the basis of those mentioned above, a creative idea was proposed to fabricate3D hierarchical PPy@MoS2 microtubes which can act as both a support and a reductant for the in situ loading of noble metal (Ag, Au, and Pd) NPs, so as to improve the catalytic behaviour. The resultant noble metal NP-based PPy@MoS2 microtubes would offer the following advantages: (i) the 2D hierarchical MoS2 nanosheet decorated 1D PPy microtubes would provide confined spaces for the in situ formation of uniform noble metal NPs with high coverage, owing to the good reduction ability of the MoS2 layers; (ii) the resulting ternary PPy@MoS2@noble metal NP heterostructure provides specific metal–support interactions at the interface which would facilitate the reactivity of the noble metal NPs, further improving the mass/electron transport during the electrocatalytic reaction. Therefore, the synergy of noble metal NPs and PPy@MoS2 nanostructures can greatly influence the heterogeneous electron transfer reactions and allow rapid detection of analytes with high performances. Taking PPy@MoS2@Au as an example, the application of PPy@MoS2@Au nanocomposites toward enzyme-like catalysis is well demonstrated.
The morphology and structure of the product at each stage were characterized by SEM and TEM. Initially, the MoO3 microrods are obtained by a simple hydrothermal method, and exhibit a rod-like morphology with a smooth surface. As shown in Fig. 1(A and B), the MoO3 microrods are ∼300 nm in diameter and ∼10 μm in length. The XRD patterns of MoO3 were indexed to the orthorhombic MoO3 phase (JCPDS card no. 05-0508) as shown in Fig. 1E(a).28 Polypyrrole (PPy) has been considered as a kind of CP with π-conjugated polymeric backbones as well as a promising carbonaceous precursor, which could increase the conductivity as well as the ionic diffusion rate. Then, the MoO3 microrods were successfully coated with the PPy shell without the need for any surfactant by mixing pyrrole and ammonium persulfate in the ethanol/water suspension of MoO3 microrods at room temperature. As shown in Fig. 1(C and D), the MoO3@PPy microcables inherit a uniform microrod-like shape of the MoO3 templates, and the surface is much rougher compared to that of MoO3. The XRD pattern (Fig. 1E(b)) also showed that the peak intensity of the MoO3@PPy composite is significantly weaker than that of the virgin MoO3. This is mainly due to the semi-crystalline nature of the PPy coating.29,30
Fig. 1 SEM and TEM images of MoO3 (A and B) and MoO3@PPy (C and D), and (E) XRD patterns of MoO3 (a) and MoO3@PPy (b). Scale bars: 1 μm in (A–D). |
Subsequently, one dimensional hierarchical PPy@MoS2 composites are formed by a one-step hydrothermal process, in which MoO3@PPy as the precursor and thiourea provides the sulfur source. Owing to strong interactions between PPy and MoS2, the MoS2 nanosheets are closely decorated on the surface of PPy microtubes as a support. As shown in Fig. 2(A and B), the composite also inherits a uniform microrod-like shape from the MoO3@PPy precursor, which has a rough surface with vertically aligned layered MoS2 nanosheets. It is worth noting that the 2D MoS2 nanosheets are assembled into integrative 1D microrods, indicating the combined features of both 1D and 2D nanostructures. Indeed, XRD investigation (Fig. 2E(a)) also confirmed that the newly formed phase was MoS2 because all diffraction peaks clearly pointed to MoS2 (JCPDS number 37-1492).16 The high-resolution TEM (HRTEM) image shown in Fig. 3a provides further insight into the interior structure. The visible lattice fringes with a layer distance of 0.62 nm are consistent with the d-spacing of the (002) planes of 2H-MoS2.31 And the lattice fringes with a d-spacing of 0.2 nm correspond to the (111) plane of Au.32 The elemental mapping images in Fig. 3b–f show that the C, N, Mo, S and Au five elements were evenly distributed in the PPy@MoS2@Au microtubes.
Fig. 2 SEM and TEM images of PPy@MoS2 (A and B) and PPy@MoS2@Au and (C and D) and (E) XRD patterns of PPy@MoS2 (a) and PPy@MoS2@Au (b). Scale bars: 1 μm in (A) and 500 nm in (B–D). |
Fig. 3 The HRTEM image of PPy@MoS2@Au (a and b), and the corresponding elemental mapping images of C (c), N (d), Mo (e), S (f) and Au (g). |
To demonstrate this vital role of polymer coating's strategy, polyaniline (PANI) is used as another coating polymer for the synthesis of hierarchical PANI@MoS2 microtubes. Previous work reported that PANI showed a similar property to PPy as a conducting polymer. Thus, it is expected that this strategy can be easily extended to the synthesis of the hierarchical polymer@MoS2 composites by simply alternating PPy to PANI polymers. Using the same experimental procedures, MoO3@PANI and PANI@MoS2 were easily fabricated (Fig. S1, ESI†), further proving that the organic polymer coating plays a vital role in the self-template formation of hierarchical polymer@MoS2 composites. The decoration of noble metal NPs on hierarchical PPy@MoS2 microtubes enables the formation of abundant interfaces, which generate an energy filtration effect that introduces energetic barriers to limit the transport of lower energy charge-carriers, which is greatly beneficial for the improvement of the Seebeck coefficient.23 A few methods for realizing functional decorative layered two-dimensional transition metal dichalcogenide (TMDC) materials have been reported. Unfortunately, modification processes are complicated, and the current research on decoration with noble metal NPs for PPy@MoS2 is insufficient. Herein, the PPy@MoS2@Au composites are obtained by direct reduction of HAuCl4 by PPy@MoS2. The driving force for the immobilization of the Au nanoparticles could be ascribed to MoS2 released photogenerated electrons under light irradiation, which contribute to the reduction of Au3+ to Au0. As shown in Fig. 2(C and D), high coverage of tiny Au NPs is well dispersed on the surfaces of PPy@MoS2. For the Au decorated PPy@MoS2 composites, due to the tiny Au NPs, only one characteristic peak related to Au (111) (JCPDS 04-0784) is observed in the diffraction pattern (Fig. 2E, curve b),6 and all other diffraction peaks could be indexed to PPy cores and hierarchical MoS2, revealing the coexistence of Au, PPy, and MoS2. Moreover, the density of Au NPs can be facilely adjusted by changing the amount of chloroauric acid. When the added weights of chloroauric acid were increased from 1 mg to 2 mg and 4 mg, respectively, the density of Au NPs is significantly increased while the size of Au NPs was almost kept constant (Fig. S2, ESI†).
To further validate the versatile applicability of this strategy, we have also decorated other noble metals, such as Pd and Ag, on the surface of PPy@MoS2 with a similar procedure. Fig. 4 shows the SEM and TEM images of PPy@MoS2@Pd and PPy@MoS2@Ag composites. As shown in Fig. 4(A, B, D and E), all the metal NPs are well dispersed on the PPy@MoS2 surface. The formation of a noble metal–PPy@MoS2 composite crystal structure was also verified by X-ray diffraction (XRD) and X-ray photoelectron spectroscopy (XPS). As shown in Fig. 4C, besides the diffraction peaks for MoS2, several diffraction peaks for Pd (JCPDS number 46-1043) are also found in the XRD pattern of PPy@MoS2@Pd, which proves that PPy@MoS2@Pd composites were successfully fabricated. Meanwhile, the XRD patterns of PPy@MoS2@Ag composites are almost the same as those of the PPy@MoS2 sample, indicating that the crystal structure of MoS2 does not change after surface modification (Fig. 4F). However, the XRD peaks of Ag are not observed, which were due to the tiny size of Ag NPs decorated on PPy@MoS2, which is also consistent with Sun's work.33 X-ray photoelectron spectroscopy (XPS) measurements are performed to further confirm the chemical compositions of PPy@MoS2@Pd and PPy@MoS2@Ag (Fig. S3, ESI†). The high-resolution spectra are shown in Fig. S3b (ESI†), as for the Pd 3d spectrum of PPy@MoS2@Pd nanocages, the peaks located at 341.4 and 336.3 eV are indexed to Pd 3d3/2 and Pd 3d5/2, respectively, indicative of Pd0.34 As presented in the high resolution Ag 3d spectrum (Fig. S3d, ESI†), the two main peaks at around 368.8 and 374.8 eV should be assigned to Ag0.35 To observe the distribution patterns of these supported noble metals, STEM-EDS was used. As seen from Fig. S4 and S5 (ESI†), energy-dispersive spectroscopy (EDS) mapping revealed that C, N, O, Mo, S, and Ag were doped into the PPy@MoS2@Ag composite. Similarly, elemental C, N, O, Mo, S and Pd were uniformly dispersed in the PPy@MoS2@Pd composite. The above results further illustrate that noble metals have been successfully decorated on the surface of PPy@MoS2 microtubes, consistent with SEM and TEM observations. Therefore, this strategy is a facile, efficient and general method for controlling the tailored formation of noble metal NPs decorated on one-dimensional hierarchical PPy@MoS2 nanostructures.
Fig. 4 SEM and TEM images of PPy@MoS2@Pd (A and B) and PPy@MoS2@Ag (D and E), and (C) XRD patterns of PPy@MoS2@Pd (C) and PPy@MoS2@Ag (F). Scale bars: 1 μm in (A and D), and 500 nm in (B and E). |
The specific surface area of PPy@MoS2 was characterized by N2 adsorption/desorption experiments, as shown in Fig. 5(A and B). PPy@MoS2 shows a high Brunauer–Emmett–Teller (BET) specific surface area of 28.57 m2 g−1 and the BJH adsorption average pore diameter was about 24.81 nm. In addition, the N2 adsorption/desorption isotherm is in well accord with the IUPAC IV type, revealing the mesoporous feature of the PPy@MoS2 composites.36–41 The high specific surface area and mesoporous architecture of PPy@MoS2 could afford sufficient accessible active sites during the catalytic reaction. The chemical compositions and valence states of PPy@MoS2 and PPy@MoS2@Au were further examined by X-ray photoelectron spectroscopy (XPS). Both of them indicated similar element peaks, except for Au in PPy@MoS2@Au in Fig. 5C. The high resolution XPS spectra of Mo 3d, S 2p and Au 4f regions of PPy@MoS2@Au are shown in Fig. 5D–F. The high-resolution Mo 3d XPS spectrum (Fig. 5D) indicated that the oxidation state of the Mo ion is 4+. Meanwhile, the low binding energy peak at around 226.29 eV is ascribed to S 2s in MoS2.42Fig. 5E shows a high-resolution spectrum for S 2p, the main doublet located at 161.9 eV and 163.1 eV corresponds to S 2p3/2 and S 2p1/2, respectively. As can be seen from the Au XPS spectrum (Fig. 5F), the peaks at 87.5 and 83.8 eV are attributed to the 4f5/2 and 4f7/2 binding energies of the zero valence state of metallic Au, respectively.43 All of the above results indicate that we have successfully prepared PPy@MoS2 and PPy@MoS2@Au.
To investigate the possible formation process of MoO3@PPy converting to PPy@MoS2, we carried out a series of control experiments by varying the solvothermal time. As shown in Fig. 6a and b, almost no MoS2 nanosheets were found on the final products, and the PPy hollow microtubes with smooth surfaces were obtained when the reaction time was 3 h. This indicates that MoO3 microrod cores start to transform to MoO42− when the reaction time increases to 3 h. As the solvothermal time reaches 6 h, some MoS2 nanosheets were covered on the PPy microtubes (Fig. 6(c and d)). When the solvothermal time was further prolonged to 12 hours, the density of the MoS2 nanosheet on the PPy surface was further increased (Fig. 6(e and f)). After reacting for 24 h, the morphology of PPy@MoS2 did not obviously change (Fig. 6(g and h)). Based on the all above results, the formation of the one dimensional hierarchical structures of PPy@MoS2 probably involved an interesting dissolution–regrowth process in which MoO3@PPy and thiourea were involved (Fig. 7). At first, thiourea was decomposed to CS2 and NH3 in solution, which can dissolve the MoO3 cores to form (NH4)2MoO4, and the hollow PPy microtubes were easily obtained. This was confirmed by the SEM and TEM results of intermediate products after 3 hours. Subsequently, MoS2 began to form gradually resulting from the reaction between MoO42− and CS2, which can slowly cover the surface of PPy microtubes. When the reaction time reached up to 12 and 24 hours, there is no obvious difference in the morphology of PPy@MoS2 synthesized at 12 h and 24 h, indicating that the inner MoO3 cores were totally converted to MoS2 covering the surface of PPy microtubes. To gain further insight into the formation process of MoO3@PPy converting to PPy@MoS2, X-ray photoelectron spectroscopy (XPS) measurements of the samples at different reaction times were performed and Mo 3d spectra were deconvoluted. The summary of XPS analysis of the valence states, peak position and relative content in these composites are listed in Table S1 (ESI†). As can been seen in Fig. S6 (ESI†), when the reaction time reached 3 h, the Mo 3d XPS spectrum is fitted to the doublet peaks at 232.6 and 235.8 eV, corresponding to Mo6+ peaks with ca. 3.2 eV spin–orbit splitting, which reveals that only Mo6+ ions are present in the composites (shown in Fig. S6 and Table S1, ESI†).44 When the reaction time increased to 6 h, there are five peaks at 226.1, 229.0, 232.2, 233.3 and 236.1 eV of Mo 3d, which belong to S 2s, Mo4+ 3d5/2, Mo4+ 3d3/2, Mo6+ 3d5/2, and Mo6+ 3d3/2, revealing that there are two molybdenum oxidation states, 67.01% Mo4+ and 32.99% Mo6+ in the composites (shown in Fig. S6 and Table S1, ESI†).44 With the reaction time increasing from 6 h to 12 h, the content of MoS2 increases from 67.01 to 72.98%. With a further increase in reaction time to 24 h, as shown in Fig. S6d (ESI†), only Mo4+ is present in the composites, which indicates that the inner MoO3 cores were totally converted to MoS2. The XPS results verify the conversion of MoO3 into (NH4)2MoO4, and then formation of MoS2 nanosheets, which is also in accordance with the SEM and TEM results. In fact, similar growth processes have also been exemplified in many other materials with the development of many unique structures.45–47 Notably, the in situ interfacial construction of PPy nanolayers plays a vital role in maintaining the one-dimensional (1D) hybrid structure. As a comparison, we tried to prepare MoS2 composites without the participation of PPy. As seen from Fig. S7 (ESI†), without the coating of an organic polypyrrole layer, the MoO3 microrods completely collapsed, resulting in the formation of aggregated MoS2 flowers.
Fig. 6 SEM and TEM images of PPy@MoS2, 3 h (a and b), 6 h (c and d), 12 h (e and f) and 24 h (g and h). Scale bars: 1 μm in (a, c, e and g), and 500 nm in (b, d, f and h). |
In particular, Zhu's group reported a similar route to synthesize a composite with ultrathin MoS2 nanosheets on Mo2C-embedded N-doped carbon nanotubes.42 In their report, the growth of MoS2 nanosheets on Mo2C-embedded NCNTs is based on in situ solids and subsequent hydrothermal reactions. The difference in them is that the synthetic strategy we employed does not require a high temperature carbonization process. As a comparison, we also applied their method to synthesize one dimensional hierarchical C@MoS2 (MoO2@C was obtained by calcination of MoO3@PPy at 500 °C under an N2 atmosphere). Initially, the S2− ions decomposed from thiourea react with Mo4+ of MoO2@C microcables, forming thin MoS2 nanosheets on the surface of MoO2@C. These MoS2 nanosheets act as physical barriers, which will hinder the further inward diffusion of S2− ions. With the increase of reaction time, more Mo4+ ions diffuse to the surface and then react with S2− ions, leading to the sustained growth of MoS2 nanosheets.48 Interestingly, we found that this synthesis method is affected by the thickness of PPy. When we also used the same MoO3@PPy-100 μL as the precursor, followed by high-temperature calcination, and then the hydrothermal reaction to synthesize MoS2-based composites. The test results indicate that the MoS2 nanosheets were almost not found on the surface of MoO2@C (Fig. S8(a and b), ESI†). We suspect that the coated carbon layer is too thick, so that Mo4+ cannot diffuse out and react with S2− to form MoS2 nanosheets. In order to prove this assumption, we reduced the pyrrole to 50 μL while keeping other conditions unchanged. The SEM and XRD results of C@MoO2@MoS2-50 showed that the MoS2 nanosheets grew on the surface of the one-dimensional structure (Fig. S8(c, d) and Fig. S9, ESI†). It is worth noting that our method is not affected by the thickness of PPy. We reduced the amount of pyrrole to 50 μL and increased the amount to 150 μL respectively, to obtain MoO3@PPy-50 and MoO3@PPy-150. Under the same experimental conditions, PPy@MoS2 with one dimensional hierarchical morphology could also be obtained (Fig. S10A, ESI†). The corresponding XRD results also proved that the hierarchical PPy@MoS2 can be easily obtained, which is not related to the thickness of PPy (Fig. S10B, ESI†). The reason may be attributed to the different formation mechanisms of MoS2. In Zhu's work, the mechanism of forming MoS2 is mainly that during the heating process, O2− ions in MoO2/Mo2C–NCNTs were replaced with S2− ions, leading to the transformation of MoO2 to MoS2. However, in our work, the formation of PPy@MoS2 is demonstrated to involve the dissolution–regrowth process.
Recently, MoS2 nanosheets have also been demonstrated to exhibit inherent enzyme-like activity, which have been used for sensing and antibacterial applications.49,50 Nevertheless, owing to the aggregated MoS2, the peroxidase-like activity of individual MoS2 is not high, which greatly limits its practical applications. To further enhance the peroxidase-like activity of MoS2 nanosheets, coupling MoS2 nanosheets with one or two kinds of nanomaterials to produce binary or ternary components of MoS2 based nanozymes have been designed and fabricated for synergistic enhanced enzyme-like catalysis.51,52 As a proof of application, the as-prepared PPy@MoS2@Au (the mass ratio of PPy@MoS2 to HAuCl4 is 10:2) was employed to evaluate the enzyme-like activity using the TMB–H2O2 reaction as a model reaction system because the colourless TMB can be oxidized to a blue product in the presence of a catalyst. As shown in Fig. 8A(I), there is an obvious absorption peak at 652 nm originating from the oxidation of TMB in the presence of H2O2. Compared with no PPy@MoS2@Au, the response rate is 595%, indicating that the nanocomposites do have excellent catalytic properties. Meanwhile, the TMB–H2O2 reaction systems in the presence of PPy@MoS2@Au produced a deep blue colour, while no obvious reactions occurred in the control systems (Fig. 8B). This again proves the important role of the empty tube and layered structure PPy@MoS2@Au nanozymes as the case with horseradish peroxidase (HRP). To investigate the ternary compound advantages of PPy@MoS2@Au, the catalytic activities with MoS2, MoS2@Au and PPy@MoS2 were tested for comparison. Fig. 8A indicates that the UV-Vis spectrum of PPy@MoS2@Au has the largest absorption peak at 652 nm. Meanwhile, the absorption peaks of PPy@MoS2, MoS2@Au, and MoS2 nanoflowers are all inferior to that of PPy@MoS2@Au (the corresponding SEM images of MoS2 and MoS2@Au are shown in Fig. S7 and S11, ESI†). As shown in Fig. 8C and D, it was found that PPy@MoS2@Au composite showed remarkably higher catalytic activity than the controlled samples and other nanomaterials, which could be owing to the synergistic effect from the strong interfacial interactions between MoS2 nanosheets and PPy microtubes, as well as Au nanoparticles. In addition, the TMB–H2O2 reaction solutions catalyzed by different nanomaterials can be visually observed through the inset photograph, which are in accordance with the foregoing results. First, the substrate can access the inner surface of the PPy microtubes through the holes and form a local concentration effect, speeding up the catalytic reaction rate. Secondly, the MoS2 nanosheets dispersed on PPy microtubes can provide more exposed active sites. After being decorated with high coverage of gold NPs, the catalytic effect on the oxidation of TMB was greatly enhanced owing to multiple synergistic catalytic effects among PPy, MoS2 and Au.
Fig. S13A and B (ESI†) depict typical Michaelis–Menten curves by fixing concentrations of H2O2 (10 mM) and TMB (10 mM), respectively. A reciprocal relationship between the initial velocity and the substrate concentration was obtained (Fig. S13C and D, ESI†). Furthermore, the Michaelis–Menten curves can be fitted to Lineweaver–Burk plots, which are shown in Fig. S13C and D (ESI†). From the Lineweaver–Burk diagram, the key enzyme kinetic parameters such as the maximum initial velocity (Vm) and the Michaelis–Menten constant (Km) were obtained by the Lineweaver–Burk equation (Table S2, ESI†).55 It is well known that Km is generally considered to be an indicator of the affinity of an enzyme for a substrate. The lower the Km, the higher the affinity of the enzyme and vice versa. The results indicate that PPy@MoS2@Au composites possess a much higher binding affinity of nanocomposites towards H2O2, suggesting that H2O2 could be detected at a lower concentration. It can be seen from Table S2 (ESI†) that the Km value of PPy@MoS2@Au to the substrate H2O2 is 247 times smaller than that of horseradish peroxidase (HRP). These data indicate that the prepared PPy@MoS2@Au microtubes are efficient peroxidase mimics, suggesting that H2O2 can be detected at lower concentrations.
Fig. 9 (A) The dose–response curve and (B) calibration curves of the analytical approach for the colorimetric detection of H2O2. The inset shows the linear response plot of absorbance to the concentration of H2O2. The absorbance changes of the system consisting of NaAc–HAc (0.2 M, pH 3.0), TMB (0.25 mM), and PPy@MoS2@Au catalyst suspension (0.025 mg mL−1) in the presence of various concentrations of H2O2 (1.0–6000 μM) (Fig. 9A). Error bars show the standard deviations of three repeated measurements. |
Analytical method (material) | Linear range (μM) | Detection limit (μM) | Ref. |
---|---|---|---|
a PrTu (1-benzoyl-3-(pyrrolidine) thiourea). | |||
Spectrophotometry | 1.0–100.0 | 1.0 | 61 |
Electrochemistry (PrTu)a | 10–500 | 3.0 | 62 |
Spectrophotometry | 40–147 | 10 | 63 |
Fluorescence | 0.8–4.8 | 0.24 | 64 |
Chemiluminescence | 0.07–10.0 | 0.6 | 65 |
Colorimetric method | 0.1–10.0 | 0.048 | 58 |
Colorimetry (Mn3O4) | 0.05–1.4 | 0.019 | 66 |
Colorimetric detection | 1.0–100.0 | 0.87 | This work |
Samples | Detected (μM) | Added (μM) | Found (μM) | Recovery (%) | RSD (n = 3, %) |
---|---|---|---|---|---|
Black tea | 28.93 | 25.0 | 51.25 | 89.26 | 1.8 |
30.0 | 56.64 | 92.04 | 2.5 | ||
35.0 | 62.47 | 95.83 | 3.0 | ||
35.0 | 76.49 | 92.60 | 2.1 | ||
Green tea | 44.08 | 45.0 | 84.73 | 90.34 | 1.4 |
50.0 | 95.49 | 102.82 | 3.2 |
Footnotes |
† Electronic supplementary information (ESI) available: Fig. S1 showing SEM and TEM images of MoO3@PAIN (a and b) and PAIN@MoS2 (c and d). Scale bars: 1 μm in (a and b) and 500 nm in (c and d); Fig. S2 showing SEM and TEM images of PPy@MoS2@Au, 2 mg (a and b) and 4 mg (c and d). Scale bars: 1 μm in (a and c) and 200 nm in (b and d); Fig. S3 showing the XPS full spectrum of PPy@MoS2@Pd (a) and PPy@MoS2@Ag (c), (b) XPS spectra of Pd 3d of PPy@MoS2@Pd and (d) XPS spectra of Ag 3d of PPy@MoS2@Ag; etc. See DOI: 10.1039/d0tb01387k |
‡ These authors contributed equally to this work. |
This journal is © The Royal Society of Chemistry 2020 |