Introduction

Continuous developments in the economy and society have led to the exhaustion of traditional non-renewable energy sources, including fossil fuels. The excessive use of non-renewable energy sources has also caused the living environment of humans to deteriorate. Therefore, the development of new green energy sources, as well as new energy storage equipment, has become a major focus of research [1,2,3,4]. As a new type of energy storage device, supercapacitors can fill the gap between traditional capacitors and chemical batteries on account of its many advantages, which include high power density, high energy density, and long cycle life [5,6,7,8].

One of the most important methods to improve the performance of supercapacitors is to develop new types of electrode materials. Various transition metal chalcogenides composed of Fe, Co, Ni, S, Se, and Te, and their composites have become a key research direction on account of their excellent specific capacitance and variable valence state. In 2007, Tao et al. [9] obtained CoS electrode materials with a specific capacitance of 475 F/g at a current density of 5 mA/cm2 via the hydrothermal reaction by using NaS·9H2O as a sulfur source and Co(CH3COO)2·4H2O as a cobalt source. In 2013, Yang et al. [10] successfully synthesized beta-NiS electrode materials with a specific capacitance of 857.76 F/g at a current density of 2 A/g via a solvothermal method. In 2013, Wang et al. [11]prepared CoSe nanotube-based electrode materials via a one-step hydrothermal method using Co(CO3)0.35Cl0.20(OH)1.10 as the cobalt source and NaHSe as the selenium source; the authors obtained a specific capacitance of 238 F/g at 1 A/g. In 2016, Guo et al. [12] applied successive cation exchange to obtain large-scale uniform Ni–Co–Se bimetallic ternary nanowires. An asymmetric supercapacitor (ASC) prepared with Ni@Ni0.8Co0.2Se and active carbon (AC) had a high specific capacitance of 86 F/g at 1 A/g. In 2015, Chen et al. [13] prepared Ni–Co sulfides as electrode materials for supercapacitors; the resultant material, Ni1.5Co1.5S4, was tested and found to have excellent performance with a maximum specific capacitance of 1093 F/g at 1 A/g. Moreover, the energy density of an ASC with Ni1.5Co1.5S4 as the anode material could reach 37.6 W·h/kg at a power density of 775 W/kg, and a high power density of 2325 W/kg could be achieved at an energy density of 17.7 W·h/kg. In 2017, Zhao et al. [14] prepared reduced graphene oxide (rGO)/FeS composite electrode materials on Fe foil via a facile one-pot hydrothermal method and obtained a specific capacitance of 300 F/g and a maximum capacity retention rate of 97.5% after 2000 charge/discharge cycles. In 2018, Ye et al. [15] reported the preparation of Se-doped NiTe electrode materials for supercapacitors via a one-step hydrothermal method; the resulting electrode had a maximum specific capacitance of 998.2 F/g at 1 A/g. In 2020, Xiao et al. [16] successfully prepared CoTe nanowires by the hydrothermal method and obtained a specific capacitance of 643.6 F/g at 1 A/g.

These previous reports mainly demonstrated the potential applications of transition metal chalcogenides as supercapacitor electrode materials. However, research on the transition metal telluride is far from sufficient. Given the variable valence state of cobalt and the excellent metallicity of tellurium, compounds combining these two elements would theoretically have good electrochemical properties. The addition of graphene to the reactants is also believed to be able to improve the performance of the resultant electrode materials remarkably [17,18,19,20,21,22]. In 2019, Chu et al. [23] proposed a scalable method to achieve highly wettable graphene-polyaniline electrodes with a maximum specific capacitance of 225 F/g at 1 A/g. In 2020, Zhang et al. [24] prepared CoNi2S4/rGO composite electrode materials by a one-step pyrolysis method and obtained a maximum specific capacitance of 1526 F/g at 2 A/g. This electrode material retained 93.7% of its original capacitance after 8000 charge/discharge cycles at 3 A/g. In 2020, Shao et al. [25] prepared MXene/RGO composite aerogels with a fusiform shape. The specific capacitance of this material at 1 A/g was 233 F/g. In 2021, Subhani et al. [26] used a graphene aerogel (GA) network impregnated on carbon fiber (CF) fabrics to prepare CF-reinforced composites. CF fabrics with 28% GA showed a specific capacitance of 92.5 F/g at 1 mV/s. Therefore, the objective of the present paper is to prepare electrode materials containing CoTe and rGO. The electric double-layer capacitance of the CoTe@rGO materials prepared in this work was provided by rGO and CoTe, while the pseudocapacitance was provided by CoTe alone. Accurate experiments proved that all of the properties of CoTe@rGO were greatly improved compared with those of pure CoTe.

Experimental

Materials

Co(NO3)2·6H2O and KOH from Tianjin Kemiou Chemical Reagent Co., Ltd.; Na2TeO3, ethylene glycol, N2H4·H2O (80 wt%), and NH3·H2O from Shanghai Titan Scientific Co., Ltd.; graphene oxide (GO) from Suzhou Carbon Abundance Graphene Science and Technology Co., Ltd.; AC from Kuraray China Co., Ltd.; carbon cloth from Cetech Co., Ltd.; carbon black (super P) from Lion Corporation; and polytetrafluoroethylene (PTFE) aqueous solution (60 wt%) from Daikin Fluorochemicals (China) Co., Ltd. were used as starting materials in this work. None of these chemicals were purified prior to their use.

Synthesis of the CoTe@rGO Electrode Materials

The CoTe@rGO electrode materials were prepared by a one-step hydrothermal method. First, 0.8 mmol of Co(NO3)2·6H2O, 0.8 mmol of Na2TeO3, and different masses of GO (0, 0.2, 0.25, 0.3, and 0.35 mg) were added to 40 mL of ethylene glycol and magnetically stirred for 1 h to obtain a homogeneous solution. Then, 10 mL of N2H4·H2O and 10 mL of NH3·H2O were slowly added to the mixture as reductants. Stirring was performed for another 1 h, during which the solution changed from purple to black. Next, the solution was transferred to a 100 mL-capacity titanium alloy autoclave. The hermetic autoclave was heated in a muffle furnace at 150 °C for 12 h. During the solvothermal reaction, CoTe was synthesized and GO was reduced. The resultant materials were named CoTe@rGO-0, CoTe@rGO-0.2, CoTe@rGO-0.25, CoTe@rGO-0.3, CoTe@rGO-0.35, respectively, according to the amount of GO added to the CoTe mixture. The weight percentages of CoTe in the synthesized CoTe@rGO composites were 100 wt%, 42.73 wt%, 37.38 wt%, 33.22 wt%, and 29.89 wt%, respectively. The obtained solid material was naturally cooled, rinsed several times with deionized water and alcohol with ultrasonication and centrifugation, and then dried for 12 h in a vacuum environment at 70 °C. The final materials were prepared into working electrodes.

Preparation of Working Electrode

The working electrodes were prepared with 80 wt% CoTe@rGO as the active material, 10 wt% PTFE as an adhesive, and 10 wt% carbon black as a supporting material to improve the electrical conductivity of the electrode. These three materials were mixed in alcohol under ultrasound. The obtained mixtures were coated on clean carbon cloth (1 cm × 1 cm) and dried in a vacuum at 60 °C for 12 h to obtain the working electrodes. The mass of all active materials coated on the electrode was 1 mg.

Fabrication of the Asymmetric Supercapacitor

An AC electrode was prepared as described in last Section. Briefly, AC, PTFE, and carbon black were ultrasonically mixed at a mass ratio of 8:1:1 in alcohol and coated on 1 cm × 1 cm carbon cloth to obtain the AC electrode. The ASC was prepared by using the CoTe@rGO electrode as the positive electrode, the AC electrode as the negative electrode, and 3 M KOH as the electrolyte.

Material Characterization

The microstructures of the products were characterized by X-ray diffraction (XRD) with a Rigaku Ultima IV instrument at 40 kV and 40 mA. The scanning speed was 10°/min, and the 2θ range was 10°–70°. The microstructural and chemical properties of the materials were characterized by field-emission scanning electron microscopy (FESEM) with a ZEISS MERLIN Compact microscope and energy dispersed X-ray spectroscopy (EDS), respectively.

Electrochemical Measurements

An electrochemical workstation (Model: CHI760E, Shanghai Chenghua) was used for all electrochemical measurements. The performance of three-electrode systems composed of the CoTe@rGO electrodes as the working electrode, Hg/HgO as the reference electrode, platinum wire as the counter electrode was tested by cyclic voltammetry (CV), galvanostatic charge/discharge (GCD) analysis, and electrochemical impedance spectroscopy (EIS). The scanning rates of the CV tests ranged from 5 mV/s to 50 mV/s, and the potential window was 0–0.6 V. The voltage range of the GCD tests ranged from 0 V to 0.55 V, and the current densities ranged from 1 A/g to 20 A/g. The frequency range of the EIS tests ranged from 0.01 Hz to 100 kHz. The performance of the ASC, which is a two-electrode system, was evaluated on the same electrochemical workstation. Here, the scanning rates of the CV tests were changed from 5 mV/s to 100 mV/s, the potential window was 0–1.6 V, and the current densities of the GCD tests ranged from 1 A/g to 5 A/g.

Result and Discussion

Micromorphological and Structural Characterization of CoTe@rGO

Figure 1 shows the XRD patterns of CoTe@rGO-0, CoTe@rGO-0.2, CoTe@rGO-0.25, CoTe@rGO-0.3, and CoTe@rGO-0.35. The diffraction peaks of CoTe (PDF #34–0420) at 31.34°, 42.98°, 46.88°, and 58.26° were found in the spectra of all samples, thereby confirming the formation of CoTe. The diffraction peak of rGO could be observed at approximately 23°, and no GO diffraction peak was noted at 2θ = 10.9°; these results indicate that GO was completely reduced to rGO during the preparation of the electrode materials [27, 28]. The magnified diffraction intensities of peaks over the 2θ range of 21°–28° are displayed to the right of Fig. 1 to highlight the existence of rGO. Moreover, the diffraction peak intensities of CoTe@rGO-0.35 were lower than those of the three other samples, likely because excess rGO could inhibit the growth of CoTe.

Fig. 1
figure 1

X-ray diffraction patterns of CoTe@rGO with different masses of reduced graphene oxide (rGO)

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FESEM images of CoTe@rGO-0, CoTe@rGO-0.2, CoTe@rGO-0.25, CoTe@rGO-0.3, and CoTe@rGO-0.35 are shown in Fig. 2. CoTe nanowires could be observed in all photos and appeared to grow on the rGO sheets (Fig. 2b–e). The amounts of CoTe nanowires in CoTe@rGO-0.2 and CoTe@rGO-0.25 indicated in Fig. 2b,c were greater than those in other samples; moreover, some nanowires did not grow on the rGO sheets and were stacked together instead. Compared with those of other samples, the nanowires of CoTe@rGO-0.3 (Fig. 2d) demonstrated improved distribution and less agglomeration. The distribution of CoTe nanowires in CoTe@rGO-0.35 (Fig. 2e) was relatively loose, and their growth appeared to be restrained; these findings are likely due to the presence of excess rGO. These phenomena are consistent with the results shown in Fig. 1, that is, the diffraction peak intensities of CoTe@rGO-0.35 are weaker than those of the other samples. These findings confirm that excess rGO could degrade the pseudocapacitance of the resultant material. The introduction of rGO changed the micromorphology of the CoTe nanowires.

Fig. 2
figure 2

Field-emission scanning electron microscopy images of a CoTe@rGO-0, b CoTe@rGO-0.2, c CoTe@rGO-0.25, d CoTe@rGO-0.3, and e CoTe@rGO-0.35

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EDS-layered electron images of CoTe@rGO-0.3 are provided in Fig. 3 to explore the distribution of different elements in the composites. Elemental C was mainly distributed in the lamellar layer, thus confirming that the lamellar material is rGO. Co and Te were mainly distributed in the nanowires. These findings, in combination with the XRD patterns obtained earlier, indicate that the CoTe nanowires are attached to the rGO layers. A large amount of aluminum could also be detected in the images due to the presence of aluminum in the test substrate.

Fig. 3
figure 3

Energy-dispersive X-ray spectroscopic layered electron images of CoTe@rGO-0.3

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Electrochemical Performance of CoTe@rGO

Figure 4a shows the GCD curves of CoTe@rGO with different masses of rGO at a current density of 1 A/g. The charge/discharge time and specific capacitance of the CoTe@rGO materials increased with an increasing amount of rGO until CoTe@rGO-0.3. Further increases in the amount of rGO added to the electrode materials (i.e., CoTe@rGO-0.35) resulted in a decrease in specific capacitance compared with that of CoTe@rGO-0.3. Figure 4b clearly shows the variation of the specific capacitance of the electrode materials. The specific capacitances of CoTe@rGO-0, CoTe@rGO-0.2, CoTe@rGO-0.25, CoTe@rGO-0.3, and CoTe@rGO-0.35 at 1 A/g were 643.6, 761.9, 786.3, 810.6, and 729.5 F/g, respectively. The specific capacitances of samples added with rGO improved compared with that of pure CoTe (CoTe@rGO-0), and the best electrochemical performance was observed in CoTe@rGO-0.3. The specific capacitance of rGO is approximately 100 F/g at 1 A/g. The specific capacitance of CoTe@rGO-0.3 was greater than the combined capacitances of CoTe@rGO-0 and rGO, which indicates that the electrochemical performance of the materials could be effectively improved by the synergistic effects of CoTe nanowires and rGO [29]. These findings, in combination with the SEM results of the CoTe@rGO composite materials, reveal that increases in rGO within a certain limit enhance the growth of CoTe nanowires by providing a suitably large surface area that could avoid the stacking and agglomeration of CoTe nanowires, thereby increasing their specific capacitance. However, excess rGO (e.g., CoTe@rGO-0.35) could restrain the growth of CoTe by restricting mass transfer during the hydrothermal process, resulting in decreases in CoTe nanowire formation and pseudocapacitance. The results collectively indicate that the optimal mass of added GO is 0.3 mg; thus, all subsequent experiments were conducted using CoTe@rGO-0.3 as the electrode material.

Fig. 4
figure 4

Electrochemical properties of CoTe@rGO samples with different masses of reduced graphene oxide (rGO): a Galvanostatic charge/discharge curves and b specific capacitance curve

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Figure 5a shows the CV curves of the CoTe@rGO-0.3 electrode obtained at different scan rates in 3 M KOH. The shape of the curve and the presence of redox peaks indicate that the electrode is pseudocapacitive [30]. According to previous studies [16, 31], the curve shape is similar to that of pure CoTe nanowires, which means that the specific capacitance of the electrode may be mainly attributed to CoTe. The reaction occurring at the redox peaks can be expressed by the following equations [16, 31]:

$${\text{CoTe + OH}}^{ - } { } \leftrightarrow {\text{ CoTeOH + e}}^{ - }$$
$${\text{CoTeOH + OH}}^{ - } { } \leftrightarrow {\text{ CoTeO + H}}_{{2}} {\text{O + e}}^{ - }$$
Fig. 5
figure 5

a Cyclic voltammetry curve of the CoTe@rGO-0.3 electrode at different scan rates, b galvanostatic charge/discharge curve of the CoTe@rGO-0.3 electrode at different current densities, c changes in the specific capacitance of the CoTe@rGO-0.3 electrode as a function of the current density, and d changes in the cycling stability of the CoTe@rGO-0.3 electrode as a function of the cycle number

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The current density increased, and the redox peak of the electrode shifted with an increasing scan rate. However, the shape of the curve did not change remarkably, which indicates that the electrode has good rate performance. The GCD curves of the CoTe@rGO-0.3 electrode at different current densities are shown in Fig. 5b. The symmetrical shape of the curves shown in this figure supports the reversible charge–discharge behavior of the electrode. The specific capacitance of the electrode could be calculated using the following formula [32]:

$$C_{m} = \frac{I \times \Delta t}{{m \times \Delta V}}$$

where \(C_{m}\) (F/g) is the mass specific capacitance; \(I\) (A) and \(\Delta {t}\) (s) are the discharge current and time, respectively; \(m\) (g) is the mass of the active substance loaded onto the electrode; and \(\Delta V\) (V) is the voltage window of the active substance. Calculations indicated that the \(C_{m}\) of the CoTe@rGO-0.3 electrode at 1 A/g is 810.6 F/g and decreases with increasing current density, as shown in Fig. 5c. An increase in current density could lead to higher reaction rates, which may affect the entry of ions into the deeper layers of the electrode materials, resulting in a decrease in the utilization rate of the electrode and, ultimately, a decline in its energy storage performance [33]. Moreover, even at a high current density of 20 A/g, the composite electrode retained 79.0% of its specific capacitance at 1 A/g, thus confirming its excellent rate performance. Figure 5d shows the cycling stability of the CoTe@rGO-0.3 electrode at a high current density of 5 A/g and 5000 charge/discharge cycles. As shown in Fig. 5d, the specific capacitance of the electrode initially declined slowly over the first 500 cycles and then began to decline at a faster rate because of the destruction of the microstructure of the material. The electrode retained approximately 77.2% of its initial specific capacitance after 5000 charge/discharge cycles, which means it has good cycling stability. The comparative advantages of CoTe@rGO over other CoTe materials are detailed in Table 1, which lists various performance indicators of previously reported CoTe materials for supercapacitors, including specific capacitance, cycling stability, and surface mass loading. Table 1 reveals that the specific capacitance of the sample prepared in this work is greater than those of all previously reported CoTe materials. This finding could be mainly attributed to the introduction of rGO, which enhances the microscale effects of the CoTe nanowires. After cycling 5000 times at a high current density of 5 A/g, the specific capacitance of the electrode remained fairly stable, thus confirming its advantageous properties.

Table 1 Comparison of the specific capacitance, cycling stability, and surface mass loading of CoTe materials reported in previous and present studies
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Figure 6 shows the Nyquist diagrams of the CoTe@rGO-0.3 electrode obtained before and after 5000 charge/discharge cycles at 5 A/g over the frequency range of 10−2–105 Hz. The intercepts between the curve and Z’-axis represent the internal resistance (Rs) of the system, which includes the internal resistance of the electrolyte and electrode materials. The semicircles near the origin of the coordinates represent the Faradaic charge-transfer resistance (Rct), and the straight lines extending outward from the semicircles represent the Warburg impedance [36]. Prior to charge/discharge cycling, Rs and Rct of the electrode were 1.367 and 0.947 Ω, respectively. After 5000 charge/discharge cycles, Rs and Rct increased to 1.647 and 1.469 Ω, respectively. This finding demonstrates good recombination between the CoTe nanowires and rGO. The observed increase in resistance may be attributed to the irreversible damage to the microstructure of the materials caused by multiple redox reactions. The angles between the straight lines and the Z’-axis were fairly large before and after cycling, which means the electrode material has abundant ion diffusion paths and low interfacial charge-transfer resistance between the electrode and electrolyte [37].

Fig. 6
figure 6

Nyquist diagrams of the CoTe@rGO-0.3 electrode before and after 5000 charge/discharge cycles with an equivalent circuit

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Electrochemical Performance of the Asymmetrical Supercapacitor

An ASC was successfully prepared using the CoTe@rGO-0.3 electrode as the positive electrode, an AC electrode as the negative electrode, and 3 M KOH as the electrolyte. Figure 7 shows the CV curves of the CoTe@rGO-0.3 and AC electrodes in a three-electrode system at a scanning rate of 50 mV/s. The potential windows of the AC and CoTe@rGO-0.3 electrodes ranged from − 1.0 V to 0 V and from 0 V to 0.6 V, respectively. The potential window of the ASC, which is composed of these two electrodes, could theoretically be expanded to 1.6 V. However, prior to the fabrication of the ASC, the masses of the positive and negative electrodes must be balanced to ensure that the electrochemical reaction occurs equally on both electrodes and improve the performance of the ASC. The specific calculation method is as follows [38, 39]:

$$q = C_{m} \times \Delta V \times m$$
$$q^{ + } = q^{ - }$$
$$\frac{{m^{ + } }}{{m^{ - } }} = \frac{{C_{{m^{ - } }} \times \Delta V^{ - } }}{{C_{{m^{ + } }} \times \Delta V^{ + } }}$$
Fig. 7
figure 7

Cyclic voltammetry curves of CoTe@rGO-0.3 and active carbon electrodes in a three-electrode system at a scan rate of 50 mV/s

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where \(q\) is the charge stored in the electrode. At 1 A/g, the specific capacitances of the CoTe@rGO-0.3 and AC electrodes were 810.6 and 257.4 F/g, respectively. Therefore, under the premise that the active substance load of the CoTe@rGO-0.3 composite electrode is 1 mg, the active substance load of the AC electrode should be 1.89 mg.

Figure 8 illustrates the CV and GCD curves of the ASC. Figure 8a shows the CV curves of the ASC at different potential windows ranging from 0.8 V to 1.6 V at a scan rate of 100 mV/s. Redox peaks gradually appeared as the potential window increased. The shape of the CV curve remained symmetric and stable when the maximum potential window was reached, thus indicating that the ASC potential window could reach the theoretical maximum value. Figure 8b shows the GCD curves of the ASC at different potential windows ranging from 0.8 V to 1.6 V at 1 A/g. The shapes of the GCD curves obtained were virtually identical and highly symmetrical with increasing potential windows. This finding confirms that the ASC can perform well at a potential window ranging from 0 V to 1.6 V [40].

Fig. 8
figure 8

a Cyclic voltammetry curves of the asymmetric supercapacitor (ASC) at different potential windows under a scan rate of 100 mV/s. b Galvanostatic charge/discharge curves of the ASC at different potential windows at 1 A/g

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Figure 9a shows the CV curve of the ASC at different scan rates ranging from 5 mV/s to 100 mV/s, and a redox peak could clearly be seen. The shapes of the CV curves were maintained despite increases in scan rate. Figure 9b shows the GCD curves of the ASC at different current densities ranging from 1 A/g to 5 A/g. The curves in the figure demonstrated the excellent reversibility of the ASC, which had a specific capacitance of 112.6 F/g at 1 A/g.

Fig. 9
figure 9

a Cyclic voltammetry curves of the asymmetrical supercapacitor (ASC) at different scan rates, b galvanostatic charge/discharge curves of the ASC at different current densities, c changes in the specific capacitance of the ASC as a function of the current density, and d changes in the cycling stability of the ASC as a function of the cycle number

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As the current density increases, the ions in the electrolyte become more difficult to bind to the electrode material, thereby resulting in a decrease in specific capacitance. Although the specific capacitance of the ASC decreased with increasing current density, 83.4% of the specific capacitance obtained at 1 A/g was preserved even at a high current density of 5 A/g, as shown in Fig. 9c. After 5000 charge/discharge cycles at a current density of 5 A/g (Fig. 9d), the specific capacitance of the ASC was still greater than 87.1% of the original value, revealing the excellent cycling stability of this system.

The Ragone plot in Fig. 10 shows the relationship between the energy densities and power densities of CoTe@rGO-0.3||AC ASC. The energy and power densities of the ASC were calculated as follows [31, 41]:

$$E = \frac{{C_{m} \left( {\Delta V} \right)^{2} }}{2}$$
$$P = \frac{E \times 3600}{{\Delta t}}$$
Fig. 10
figure 10

Ragone plot of the CoTe@rGO-0.3||AC asymmetric supercapacitor

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where \(E\) (Wh/kg) is the energy density; \(P\) (W/kg) is the power density. The ASC revealed a high energy density of 40.04 W·h/kg at a power density of 799.91 W/kg and a high power density of 4004.93 W/kg at an energy density of 33.43 W·h/kg. These results are better than those obtained from pure CoTe nanowires||AC ASCs reported in Refs. [16, 31]. The findings confirm that the energy storage performance of CoTe@rGO is greatly improved compared with that of CoTe nanowires, thus, the synthesized material is a potential electrode material for supercapacitors.

Conclusion

CoTe@rGO composite materials were successfully synthesized by adding GO to the reaction materials. The addition of 0.3 mg GO to 0.8 mmol of Co(NO3)2·6H2O and 0.8 mmol Na2TeO3 yielded a composite material with a highly uniform distribution and optimal electrochemical performance. The specific capacitance of the electrode prepared with CoTe@rGO could reach 810.6 F/g at 1 A/g; such capacitance is much higher than that of pure CoTe nanowires. At the current density of 20 A/g, the composite electrode retained 79.0% of its specific capacitance at 1 A/g, indicating the excellent rate performance. An ASC in which the CoTe@rGO composite material and AC were used as electrodes was fabricated, and the specific capacitance of this system was 112.6 F/g at 1 A/g. After 5000 charge/discharge cycles at a current density of 5 A/g, the specific capacitance of the ASC remained as high as 87.1%, indicating the excellent cycling stability. The maximum energy density of the ASC was 40.04 W·h/kg, and its power density was as high as 4004.93 W/kg at an energy density of 33.43 W·h/kg. These results collectively confirm that the preparation of CoTe@rGO is an effective means to improve the properties of CoTe electrode materials. The electrode materials prepared in this work demonstrate broad application prospects.