The EDS maps in Fig. 1 show that sulfur is efficiently and uniformly incorporated into carbon nanotubes.
The XRD characteristic peaks of the carbon nanotubes are (002) and (100) peaks with 2-Theta angles around 26° and 42.9°, as shown in Fig. 2, which we can observe in all samples. Compared to the original samples (CNTs), S-droped CNTs have no significant deviation in peak intensity and peak position, indicating that the doping sites of sulfur atoms are mainly concentrated on the surface layer of carbon nanotubes.
Figure 2b shows the Full Spectrum XPS spectrum of all samples,it can be seen that CNTs are primarily composed of two elements, i.e., C and O. In the XPS spectra of S-droped CNTs the S2p hybrid characteristic peak is observed at ~ 160 eV. The sulfur contents of CNTs@S-1, CNTs@S-2, and CNTs@S-3 are 0.78%, 0.98%, and 1.07%, respectively, consistent with EDS results, further proving the successful sulfur doping of CNTs. The S2p peak fitting (Figs. 2(c–e)) reveals that the S2p peaks observed in the XPS spectra of samples obtained at different temperatures[600,700,800℃] appear at approximately 163.9 and 165.1 eV correspond to the C–S bond (C–S) and C = S bond (165.5 eV), respectively, and the peak of the carbon–sulfur oxide bond of C–SOX (x = 2–4); 168.9 eV) is not observed in the XPS spectrum of S-droped CNTs, indicating that under the experimental conditions, the temperature affects the sulfur doping amount of CNTs, but not the carbon and sulfur binding mode.
, CNTs@S-1, CNTs@S-2 and CNTs@S-3, (b) XPS XPS Full Spectrum of CNTs
, CNTs@S-1, CNTs@S-2 and CNTs@S-3, (c) S2p of CNTs@S-1, (d) S2p of CNTs@S-2, (e) S2p of CNTs@S-3.
Raman spectroscopy is an efficient technique to identify electronic or structural rearrangements and the atomic properties of defects in carbon nanotubes. In the Raman spectrum, the D peak at ~ 1310 cm− 1 represents the C atom lattice defect or disorder site, and the G peak at ~ 1600 cm− 1 is the characteristic peak of sp2 carbon atoms. The intensity of the D peak to the G peak (called the ID/IG ratio) is usually used to represent the degree of defects in carbon nanotubes or graphene. The Raman spectra of CNTs, CNTs@S-1, CNTs@S-2, and CNTs@S-3 are shown in Fig. 3a. The ID/IG ratios of CNTs, CNTs@S-1, CNTs@S-2, and CNTs@S-3 are 0.62, 0.63, 0.64, and 0.57, respectively.
Figures 3(b–d) show the TEM images of CNTs, CNTs@S-1, CNTs@S-2, and CNTs@S-3, it can be seen that there is no significant change in the structure and morphology of the carbon nanotubes before and after doping, indicating that sulfur doping does not damage the structure of carbon nanotubes.
The pore structures of CNTs and S-droped CNTs were studied via N2 adsorption–desorption isotherms. Figure 4 shows that specific surface areas of CNTs, CNTs@S-1, CNTs@S-2, and CNTs@S-3 are 285.69, 295.77, 308.52, and 354.51 m2·g− 1, respectively. This means that as the sulfur doping amount in carbon nanotubes increases, the specific surface area of the S-droped CNTs considerably increases. This is because the atomic radius of sulfur is much greater than that of carbon, and the C–S bond is longer than the C–C bond; hence, the combination of sulfur and carbon distorts the six-ring structure of carbon nanotubes in the same plane. Such changes are beneficial to the diffusion of lithium ions.
CV was performed in the range of 0.1–1 mV. The potential difference between the oxidation/reduction peaks is usually used to indicate the degree of polarization of a cell. As shown in Fig. 5, the battery (C-1) manufactured using untreated carbon nanotubes as conductive agents (carbon nanotubes) exhibits the most severe polarization, compared with C-1, the polarization of batteries (C-2, C-3, C-4) made with sulfur doped carbon nanotubes as conductive agents has significantly decreased, with C1, C4, C3, C2 in descending order from high to low. Polarization decreases the battery output power and energy utilization and affects the service life and safety of the battery. Reduced polarization can increase the effective current and improve the rate performance of the cells.This indicates that sulfur doping can effectively improve the rate, cycling, and safety of batteries
Chart 1.ΔE of C-1, C-2, C-3 and C-4 in different scan rates
Scan rate/mV·s− 1 | Materials |
CNTs | CNTs@S-1 | CNTs@S-2 | CNTs@S-3 |
0.1 | 0.317 | 0.145 | 0.172 | 0.171 |
0.2 | 0.332 | 0.152 | 0.248 | 0.268 |
0.3 | 0.425 | 0.272 | 0.327 | 0.315 |
0.4 | 0.534 | 0.325 | 0.392 | 0.367 |
0.5 | 0.576 | 0.378 | 0.446 | 0.426 |
0.6 | 0.642 | 0.441 | 0.495 | 0.472 |
0.7 | 0.696 | 0.45 | 0.547 | 0.516 |
0.8 | 0.759 | 0.488 | 0.589 | 0.56 |
0.9 | 0.812 | 0.521 | 0.632 | 0.591 |
1 | 0.855 | 0.553 | 0.672 | 0.637 |
EIS results in the frequency range of 0.1–100 kHz are shown in Fig. 6a. The high-frequency region is controlled by the electrode reaction dynamics (charge transfer process), and the low-frequency region is controlled by the diffusion of reactants or products produced at the electrode. From the perspective of the semicircle diameter in the high-frequency region, as conductive agents, sulfur-doped carbon nanotubes considerably reduce the charge transfer resistance (Rct) of the battery, which further decreases with an increase in the doping amount. Furthermore, the oblique line in the low-frequency region in the EIS plots of CNTs also significantly deviates from 45°, indicating that sulfur doping is conducive to the diffusion of lithium ions.
Figure 6(b) shows taht the first charge and discharge performance of the battery, which was studied at 25°C and 0.2 C. The first discharge capacities of C-1, C-2,C-3 and C-4 are 156.3, 157.0, 160.5, and 162.9 mAh·g− 1, respectively, and the first coulombic efficiencies are 84.4%, 85.0%, 87.0%, and 89.2%, respectively, both of which increase as the S doping amount increases, consistent with EIS results.
Figure 6(d) shows that rate performance shows a different regularity from EIS and first discharge specific capacity. Firstly, at a low rate (< 1 C), there is almost no difference in the discharge specific capacity of C-1, C-2, C-3, and C-4. However, as the discharge rate increases(2 C, 3 C, 5 C ), the influence of polarization on the battery performance increases, the discharge specific capacity and stability of batteries (C-2, C-3, C-4) using S-droped CNTs as conductive agents is significantly higher than that of original sample(C-1).
The cycle performance of cells was tested at 3 C. Figure 6(d) shows that the initial discharge specific capacity of batteries (C-2, C-3, C-4) using S-droped CNTs as conductive agents is significantly higher than that of original sample(C-1). The capacity retention rates of C-1, C-2, C-3, and C-43 are 71.3%, 83.1%, 84.7%, and 81.8%, respectively. The cycle performance of cells is affected by battery internal resistance and polarization.
Fiugre 6. Electrochemical properties.(a)EIS, (b)First charge and discharge, (c)Rate performance, (d)Cyclic performance at 3 C