Wenqi Liu*a,
Xiaochun Wub and
Xiaojin Li*a
aQingdao Institute of Bioenergy and Bioprocess Technology, Chinese Academy of Sciences, Qingdao 266101, P. R. China. E-mail: liuwq@qibebt.ac.cn
bCAS Key Laboratory of Standardization and Measurement for Nanotechnology, National Center for Nanoscience and Technology, Beijing 100190, P. R. China
First published on 24th July 2017
We developed a non-enzymatic electrochemical glucose sensor with a unique three dimensional network structure by combining Ni foam with Au nanorods (Au NRs) on its surface (Au NRs/Ni). Electrochemical measurements revealed that the Au NRs/Ni foam exhibits very high sensitivity with a linear slope of 5.27 mA mM−1 cm−2 for glucose detection, better than the Ni foam electrode and most of the reported electrodes. And its linear dynamic range is also broader than the Ni foam electrode. Moreover, upon light excitation of the localized surface plasmon resonance (SPR) of the Au NRs, light-enhanced electrochemical activities are observed from the Au NRs/Ni foam, suggesting the possibility of modifying electrochemical sensors by surface plasmon resonance. These results highlight the potentials of the Au NRs/Ni foam electrode in practical glucose monitoring and plasmonic effects in photoelectrochemical sensing.
Among numerous materials, noble metal nanoparticles (NMNPs), such as Au, Ag, Pt, Pd, exhibit high electrocatalytic activities, long-term stability and good biocompatibility11,12 and therefore have been extensively explored as electrode materials for glucose oxidation. Furthermore, NMNPs display unique optical properties, especially for Au, Ag nanoparticles, which possess strong extinctions in the visible and NIR spectral region owing to localized surface plasmon resonances (LSPR).13,14 NMNPs can act as plasmon catalysts or photosensitizers by transferring some of the absorbed plasmonic energy through either resonant energy transfer or direct hot-electron injection to the reactants, thereby improving their own catalytic activities or performances of attached substrates.15–17 This light-enhanced activity has recently attracted great attention in solar harvesting field.18
Encouraged by the achievements based on plasmon enhanced catalytic activities, we hereby propose a novel sensing platform that can utilize LSPR to enhance the glucose oxidation and thus to improve the sensitivity of the glucose sensor. The platform consists of Au nanorods (Au NRs)-modified Ni foam (Au NRs/Ni). Au NRs were employed as plasmon catalysts due to their aspect ratio-dependent LSPR responses and well-developed synthesis method.19 Ni foam was chosen as the support for the Au NRs due to its high conductivity, unique three dimensional network structure, large loading amount of active materials and low price.20,21 In addition, Ni foam can directly act as a sensing platform for glucose detection in alkaline solution, which is mediated by Ni(II)/Ni(III) redox couple.22 At first, using this nanoplatform, we investigated its electrochemical sensing of glucose in the absence of plasmon excitation by cyclic voltammetry and chronoamperometry. Significantly enhanced electro-catalytic performance has been observed using the Au NRs/Ni electrode for glucose oxidation. And it shows higher sensitivity and broader linear range than the Ni foam electrode. Upon plasmon excitation with simulated sunlight irradiation, light-enhanced electrochemical sensing of glucose is exhibited, indicating the feasibility of further improvements in sensitivity, dynamic range, and detection limit and highlighting the potential applications of plasmon effects for electrochemical sensing.
The chemical composition and crystal phase of the samples were further examined by XRD analysis. The Ni foam shows three sharp diffraction peaks at 2θ = 44.5°, 51.8°, and 76.3° (Fig. 2F, black line), which match (111), (200) and (220) planes of the face centered cubic (fcc) phase of Ni metal (JCPDS card no. 65-2865), respectively. After modification with Au NRs, new diffraction peaks appearing in the XRD pattern (Fig. 2F, red line) at 2θ = 38.2° and 64.5°, which can be well indexed to the (111) and (220) planes of fcc Au (JCPDS card no. 65-2870). In addition, the fcc Ni (111) peak almost overlaps with the fcc Au (200) peak. The above XRD results demonstrate that the Au NRs were modified on the Ni foam surface. The resulting electrode was then characterized by cyclic voltammetry (CV) in detail.
For evaluating the electrochemical properties of Au NRs modified Ni foam electrode, cyclic voltammograms of the nickel foam substrate, Au NRs/GCE and Au NRs/Ni foam electrode were carried out in 0.1 M KOH at a scan rate of 100 mV s−1 (Fig. 3). The CVs are similar to those reported in the literature for Ni and Au electrode in alkaline solution.23,24 As can be seen, four redox peaks, A/B, a/b, C/D, and c/d are present. The a/b couple is due to the Ni(II)/Ni(III) redox couple, the same to the A/B couple. While C/D and c/d process is related to gold oxide formation and subsequent reduction to Au0.25 The voltammetric profile of the modified electrode is the weighted sum of the electrochemical behaviours of Au and Ni catalyst. In addition, the Au–Ni composite electrode exhibits good stability in alkaline solutions (Fig. S2†), possibly due to the electrostatic binding between the positively charged Au NRs and negatively charged Ni foam surface.26 Moreover, the current density for the oxidation/reduction of Au NRs/Ni foam electrode is higher than that of Ni foam substrate.
Fig. 3 Cyclic voltammograms of the nickel foam substrate, the Au NRs/Ni foam electrode, and the Au NRs/GCE measured in 0.1 M KOH at a scan rate of 100 mV s−1. |
The electrochemical behaviors of glucose oxidation were investigated by CV. Fig. 4A and B and S3† display the CVs over a voltage range from −0.2 to 0.7 V for the nickel foam substrate, Au NRs/Ni foam electrode, and Au NRs/GCE in 0.1 M KOH solution with different glucose concentrations at a sweep rate of 100 mV s−1. As Fig. 4A shows, one redox peak is observed at the Ni foam due to the glucose oxidation and reduction mediated by Ni(II)/Ni(III) redox couple. The oxidation currents at 0.4–0.6 V increase gradually with the introduction of glucose from 0 to 1 mM, indicating the electrochemical oxidation of glucose, but the currents gradually become saturated from 1 to 5 mM. Fig. S3† and 4B shows the CVs for Au NRs/GCE and Au NRs/Ni foam electrode with different glucose concentrations. They exhibit some common properties. In the positive potential scan two oxidation peaks appear both in Fig. S3† and 4B at about +0.45 V (peak A) and +0.65 V (peak B), peak A is due to the direct electrochemical oxidation of glucose by the electroactive species of Au(OH)ads and peak B is attributed to the further oxidation of gluconolactone generated from glucose oxidation (peak A). While during the reverse scan a single oxidation peak at about 0 V (peak C) is also observed both in Fig. S3† and 4B. As Fig. S3† and 4B show, the rate of oxidation increases greatly and a well-defined peak (peak C) is soon developed. The formation of peak C is due to the re-oxidation of glucose for it's in the same potential region as soon as the Au oxides are reduced.27 So peak C reflects the oxidation of glucose by Au oxides. In addition, the difference between Fig. S3† and 4B is that no glucose oxidation and reduction peaks mediated by Ni(II)/Ni(III) redox couple are found in Fig. S3.† Furthermore, the peak current for Au NRs/Ni foam electrode is higher than that of Ni foam substrate, and proportional to the glucose concentration up to 5 mM, since more electrons could be provided with a high content of reaction reagents during electrochemical oxidation for Au NRs/Ni foam electrode.
Fig. 4 CV curves of (A) the nickel foam substrate and (B) the Au NRs/Ni foam electrode in a series of glucose concentration measured in 0.1 M KOH at a scan rate of 100 mV s−1. |
To further evaluate the sensitivity of the NEG sensor based on Au NRs/Ni foam electrocatalyst, the chronoamperometry is performed. Fig. 5A depicts the amperometric response curves of the nickel foam substrate and Au NRs/Ni foam electrode upon the successive addition of glucose at 0.6 V vs. Ag/AgCl electrode. The currents increase immediately with the increase of glucose concentrations, indicating the sensitive and rapid responses as a glucose monitor. And the Au NRs/Ni foam electrode shows larger current response toward glucose sensing than the nickel foam. Fig. 5B displays the linear relationship between the current density and the glucose concentrations. The sensitivity of the sensors could be calculated from the linear regression equations. The sensitivity of Au NRs/Ni foam is 5.27 mA mM−1 cm−2 for glucose detection, which is 2.62 times as high as the nickel foam (2.01 mA mM−1 cm−2). Table S2† summarizes the sensitivity of several typical NEG sensors with different electrodes reported previously. It should be noted that the Au NRs/Ni foam electrode possesses excellent sensitivity toward glucose detection among these electrodes. And the limit of detection can be calculated to be 14 μM for the Au NRs/Ni foam electrode based on the signal-to-noise ratio of 3 (S/N = 3). The excellent sensitivity of Au NRs/Ni foam can be attributed to the high electrocatalytic activity of Au NRs. Moreover, the well-distributed Au NRs on the surface of Ni foam favor the full access of single Au NR to glucose, which significantly enhances the electrochemical response toward glucose oxidation. The amperometric response curve of the Au NRs/GCE as control is shown in Fig. S4,† which indicates that no Ni foam as the substrate significantly decreased the sensitivity.
The photoelectrochemical properties of Au NRs/Ni foam electrode were studied under simulated sunlight irradiation at room temperature in 0.1 M KOH solution. Fig. 6A shows the CVs over a voltage range from −0.2 to 0.7 V for the Au NRs/Ni foam electrode with light on/off. The CV curves were measured upon successive addition of 0.1 mM glucose between every two scans. Light was turned on or off just before adding glucose. As can be seen, a clear increase in current change between two scans is observed when the light is switched on, and the current change immediately returned to its initial state after the light is turned off, suggesting the enhanced redox reactions on the sensor surface under sun light illumination. By statistics, the current change with light on is 1.77 times of the current change with light off, and the percentage of the photo-enhanced effect is about 44% in the total signal. The UV-vis-NIR spectra were measured to prove light absorption by Au NRs/Ni foam electrode. As Fig. 6B shows, Ni foam presents an absorption band at about 350 nm, which is ascribed to the absorption of NiO.28 In contrast, two additional broad absorption bands are found for the Au NRs/Ni foam between 500 and 700 nm, which correspond to the transverse and longitudinal SPR bands of the Au NRs, respectively. Band shifting and broadening are caused by the assembly of Au NRs on Ni foam. As the ultraviolet part of simulated sunlight irradiation is low, the effect of NiO absorption on light-enhanced electrochemical responses can be ignored. In contrast, plasmonic photocatalysis of the Au NRs is the main cause of improved photoelectrochemical responses for glucose. In addition, whether the Au NRs act as the photosensitizers and lead to extra photocurrent increase through transferring plasmonic energy to underneath Ni foam need further investigations. In all, our results show that the plasmonic effect has a great application potential in photoelectric sensors.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c7ra06909j |
This journal is © The Royal Society of Chemistry 2017 |