Background

Quantitatively accurate and fast determination of H2O2 is extremely important in the field of food industry, pharmaceutical, clinical, industrial, and environmental analyses [1]. Among the several analytical techniques, electrochemical analysis is widely used due to the fast response, high sensitivity, and excellent selectivity [2, 3]. Although enzyme-modified electrode is always used to build H2O2 biosensor due to its high selectivity, the enzymatic biosensors still suffer from the insufficient stability which originated from the nature of enzymes [4]. Therefore, the study of nonenzymatic H2O2 sensors is aroused in this field. It is known that platinum shows excellent electroactivity because of the efficient electron transfer rate [5, 6]. Platinum with special morphologies, such as spherical [7], cubic [8], nanowires [9], nanoflowers [10], have been reported to construct biosensors. In addition, specific surface area is also a key factor affecting the performance of the biosensor. Therefore, how to increase the specific surface area is the focus in scientific research. Hollow structures have attracted extensive attentions for their special frame and composition. Large inner surface area can be obtained because of the inner void space of hollow structure. In recent years, hollow noble metals have been applied in the field of electrocatalyst due to the high electron transfer rate and large surface area [11]. However, few articles reported the applications of hollow noble metals in the field of biosensors.

In the present work, cubic PtCu NCs were fabricated using cuprous oxide (Cu2O) crystals as sacrificial templates, and their electrocatalytic activity towards H2O2 was investigated. The nonenzymatic H2O2 sensors exhibited excellent electrocatalytic performance with a high sensitivity and wide linear range for the determination of H2O2.

Methods

Reagents

Chloroplatinic acid, H2O2 (30 wt.% in H2O) and Nafion solution (5.0 wt.% in a mixture of lower aliphatic alcohols and water) were purchased from Sigma-Aldrich (St. Louis, MO, USA). All other reagents were of analytical grade and used as received without further purification (Chengdu Kelong, Chengdu, China). High-quality deionized water (resistivity > 18.0 MΩ cm-1) used for all experiments was prepared by a Water Purification System (UPT-II-10 T) provided by Chengdu YouPu, Chengdu, China.

Preparation of PtCu NCs

Cubic Cu2O template was prepared according to the previous report [12]. Ten milliliters of NaOH aqueous solution (2 M) was added dropwise into the stirred CuCl2 · 2H2O (100 mL, 0.01 M) at 55°C. After stirring for 0.5 h, 10.0 mL ascorbic acid solution (0.6 M) was added. The final products were collected by centrifugation after 3 h, followed by drying in vacuum at 40°C for 24 h.

In order to prepare PtCu NCs, 10 mg prepared Cu2O was dispersed in 10 mL distilled water by ultrasonic for 15 min and then 40 mg sodium citrate was added. After stirring for 15 min, 1 mL chloroplatinic acid (20 mM) was added. After reacting for 20 min, 1 mL of dilute HNO3 (5 mM) was injected into the above solution to etch the Cu2O cores. After 40 min, the ultimate products were separated by mild centrifugation and dried at 40°C for 24 h in an oven.

Electrochemical measurements

All electrochemical measurements were performed on a μIII Autolab electrochemical workstation in 0.1 M phosphate-buffered solution (PBS, pH = 7.0). Neutral PBS was obtained by mixing NaH2PO4 and Na2HPO4 solution (0.1 M). A conventional three-electrode system was used with Ag/AgCl (saturated with KCl) and platinum as the reference electrode and counter electrode, respectively. PtCu NC modified glassy carbon electrode (GCE, Ф = 3 mm) served as the working electrode. Typically, GCE was carefully polished with 0.05 μm alumina powders. Then, 5 μL of PtCu NC suspension (5 mg/mL) was cast onto the GCE and dried in air. Finally, 3 μL 1% Nafion solution was dipped onto the modified electrode.

Results and discussion

Characterizations

As shown in Figure 1a, no Cu2O (JCPDS 65–3288) residue remains in the final products. Compared to pure Pt (JCPDS 65–2868), all diffraction peaks shift to large angle direction. The diffraction peaks located at around 41.2°, 48.1°, and 70° can be indexed to cubic PtCu alloy (JCPDS 48–1549). The average particle size of PtCu was calculated to be 2.9 nm according to the Scherrer equation:

D = / B cos θ ,
(1)

where B is the full width at half maximum (FWHM), λ is the X-ray wavelength (1.5406 Å), and K is a shape factor (about 0.89). On account of the fact that the Cu2O/Cu redox pair value is 0.36 V, which is much lower than that of PtCl62-/Pt (0.735 V), therefore, Cu2O crystals can be used as the reducing agent and sacrificial template for the synthesis of cubic PtCu NCs. The formation process of PtCu NCs can be explained in the following equations:

2 Cu 2 O + 4 H + + PtCl 6 2 - Pt + 4 Cu 2 + + 6 Cl - + 2 H 2 O
(2)
Cu 2 O + 2 H + Cu + Cu 2 + + H 2 O
(3)
Figure 1
figure 1

XRD patterns and SEM, TEM, and HRTEM images. XRD patterns of Cu2O and PtCu NCs (a). SEM image of the Cu2O template (b) and PtCu NCs (c). TEM (d) and HRTEM (e, f) images of the PtCu NCs. The insets of (b) and (c) are the SEM images of single Cu2O crystal and PtCu NC, respectively. The inset of (d) is the TEM image of a single PtCu NC. The insets of (e) and (f) are the SAED pattern and lattice fringes of PtCu NC, respectively.

According to the above equations, the coexistence of Cu can be attributed to the disproportionation reaction of Cu (I). The reactions can simultaneously produce metallic Cu and Pt in the presence of H+, resulting in the formation of PtCu alloy. Figure 1b,c shows the scanning electron microscope (SEM) images of the prepared Cu2O template and the cubic PtCu NCs, respectively. The cubic Cu2O crystals have an average edge length about 200 nm, and the surface of the Cu2O crystals is smooth, uniform, and regular. However, the surface of PtCu NCs changes into rough and porous, indicating the formation of PtCu aggregates. It is clear that the PtCu NCs maintain the morphology of the Cu2O template and the interiors are hollow. The transmission electron microscope (TEM) image of PtCu NCs (Figure 1d) further provides convincing evidence of the hollow structure. For a further investigation, high-resolution transmission electron microscope (HRTEM) images were taken and displayed in Figure 1e,f. It is displayed that the shell of the PtCu NCs is porous (Figure 1e), and the porous shell is composed of amounts of PtCu nanograins. The porous structure possesses large specific surface area, which is beneficial for the electrocatalysis of H2O2. The inserted selected area electron diffraction (SAED) pattern indicates that the PtCu NCs have a polycrystalline structure. From Figure 1f, the size of the nanograins is about 2 to 4 nm, which agrees well with the value calculated from X-ray diffraction (XRD). The spacing for marked adjacent lattice fringes of PtCu NCs is about 0.22 nm, which is consistent with the standard value of PtCu (111) lattice spacing (0.219 nm).

Electrochemical performances of the PtCu NC electrode

In order to estimate the kinetics of the electrode, the cyclic voltammetries (CVs) of cubic PtCu NC electrode were measured in 0.1 M PBS containing 1.0 mM H2O2 at different scan rates. As can be seen from Figure 2a, both the anodic and cathodic peak currents are proportional to the square root of the scan rate, indicating that the electrocatalytic process is diffusion-controlled. CVs of PtCu NC electrode in 0.1 M PBS with different concentrations of H2O2 were illustrated in Figure 2b. With the increase of the concentration, both the anodic and cathodic peak currents linearly change, showing a linear dependence between the peak current and the concentration of H2O2. As can be seen from Figure 2b, peaks 1 and 2 corresponding to hydrogen adsorption are clearly investigated. Peaks 3 and 4 are the oxidation peaks of Cu and Pt in the alloy, respectively. Peak 5 corresponds to metal oxide reduction. With the reduction of Pt, more active sites are obtained, and the response current is clearly investigated.

Figure 2
figure 2

CVs of PtCu NC electrode. (a) CVs of PtCu NC electrode in 0.1 M PBS containing 1 mM H2O2 with different scan rates. The inset shows the relationship between the peak current and scan rate. (b) CVs of PtCu NC electrode in 0.1 M PBS with different concentrations of H2O2. The inset shows the dependence of the peak current on the concentration of H2O2.

Figure 3 displays the amperometric response of the cubic PtCu NC electrode at -0.45 V to successive injection of a certain amount of H2O2 into the stirred 0.1 M PBS, and the corresponding calibration curve is exhibited in the inset. After the injection of H2O2 into the 0.1 M PBS, a well-defined, stable, and fast amperometric response was observed. The linear relationship was obtained for concentration ranging from 5 μM to 22.25 mM. The linear regression equation was given as y = -20.862x - 32.157 [I (μA); x (mM)], with a correlation coefficient of R = 0.9990. The detection limit of H2O2 was found to be 5 μM (S/N = 3) with a relatively high sensitivity of 295.3 μA mM-1 cm-2. The sensitivity and linear range obtained at PtCu NC electrode are better than those for HRP immobilized at multiwalled carbon nanotube/alumina-coated silica nanocomposite modified glassy carbon electrode (157 μA mM-1 cm-2; 1 to 500 μM) [13] and nano-Au monolayer supported by carbon ceramic electrode (290 μA mM-1 cm-2; 12.2 μM to 1.1 mM) [14]. The excellent performance may be attributed to the possible synergetic effect between Pt and Cu [15] and the porous structure of the PtCu NCs, which provide a large specific surface area. In terms of the synergetic effect, Cu atom in the PtCu alloy acts both as promoting centers for the generation of the Cu-OHad species and as an electron donor to Pt in the PtCu alloy. The incorporation of Cu atom decreases the Pt 4f binding energies and consequently reduces the Pt-OHad bond strength. Therefore, the intimate contact between Pt and Cu domains in the PtCu alloy greatly promotes the regeneration of Pt sites for high electrochemical activity towards hydrogen peroxide.

Figure 3
figure 3

Current-time response of PtCu NC electrode towards H 2 O 2 . The inset shows the relationship between the catalytic current and the concentration of H2O2.

To estimate the effective surface area of the PtCu NC electrode, cyclic voltammograms on PtCu NC electrode in a solution containing 5 mM K3Fe(CN)6 and 0.1 M KCl were performed [16]. According to the Randles-Sevcik equation [17],

I p = 2.69 × 10 5 × n 3 / 2 A D 1 / 2 v 1 / 2 C ,
(4)

where A is the effective surface area (cm2), Ip is the peak current of the redox reaction of [Fe(CN)6]3-/4- (A), n is the number of electrons transferred (n = 1), D is the diffusion coefficient (0.76 × 10-5 cm2 s-1), v is the scan rate (V s-1), and C is the concentration of K3Fe(CN)6 (5 mM). The calculated value of A is 0.83 cm2 for the PtCu NC electrode, which is 11.75 times of the bare GCE.

Conclusions

Cubic PtCu NCs were successfully synthesized using Cu2O as the template. The PtCu NC electrode exhibited excellent electrocatalytic activity towards H2O2. The observed detection limit and sensitivity for PtCu NC electrode was 5 μM and 295.3 μA mM-1 cm-2, respectively, with a wide linear range from 5 μM to 22.25 mM. On the basis of our research, the PtCu NC electrode has potential applications for the design of hydrogen peroxide sensor.