2.3.1. Impedance Spectra
To confirm the cycle stability of MnO
2|Li, KL|Li, MnO
2/KL+A|Li, MnO
2/KL+B|Li and MnO
2/KL+C|Li, the electrochemical impedance spectroscopy (EIS) measurements are conducted and the results are shown in
Figure 13.
The Nyquist plots (before charging-discharging) for all four electrodes are similar (excluding MnO
2—
Figure 13b), and show one semicircle in the high–middle-frequency region and an inclined line in the low-frequency region. The diameter of these circles is dependent on the interface contact and charge transfer resistance [
49]. The MnO
2/KL+C electrode has a clearly smaller diameter of the semicircle compared with MnO
2/KL+A. This difference supports the finding that lignin (KL) can facilitate electron and Li-ion transfer and improve electrical conductivity, thus resulting in significant improvement in the electrochemical performance of MnO
2 [
49]. Moreover the impedance range for pure lignin excluded that electrode from further electrochemical studies (
Figure 13c).
The EIS results also show the impedance of the anode interface. Nyquist plots for MnO
2|Li cells without activated lignin composition is shown in
Figure 13b. Typically, spectra taken immediately after cell assembly consist of two parts in the high-frequency region. On the other hand, the impedance plots consisting of two semicircles may also be attributed to the anode/electrolyte interface (the high-frequency semicircle) and to the cathode/electrolyte interface (the low-frequency semicircle). Confirmation is seen on SEM images (see
Figure 14). It is clearly observed that irregularly shaped pores are randomly located on the surface of the electrode spheres (
Figure 14a,b,d). A different structure is observed for MnO
2/KL+A and MnO
2/KL+C (
Figure 14c,e )—the change in structure is caused by the ILs used.
Low potential anodes (e.g., lithium or lithiated graphite) exhibit a tendency to spontaneously react with electrolytes. In case of metallic lithium as well as lithiated graphite it is necessary to include a protective coating, as lithium may grow dendrite crystals on its surface. As a result, it is expected that the electrolyte used for Li-ion batteries will form an SEI which will protect the anode [
67]. A similar phenomenon was observed for the presented anode materials. A solid electrolyte interface can be formed after several cycles e.g., on the MnO
2/KL+B anode. In contrast the SEI film on a graphite anode is formed during the initial cycle [
68,
69]. Impedance spectroscopy may be used in order to investigate the passivation of electrodes in a Li-ion battery (
Figure 13b,d,f,h,j). Electrochemical impedance spectra (EIS) of electrode|electrolyte|Li were measured before and after 20 cycles (at a current of 50 mA·g⁻
1). Two electrode cells were used to record the impedance spectra with the use of an Li counter. The impedance of the interface of lithium was included in the EIS results. It can be observed that the spectra obtained directly following the cell assembly included a semicircle and a linear part. The semicircle may be associated with e.g., polarization resistance or SEI layer formation, whereas the linear part may be attributed to the diffusion of Li ions (in the electrolyte, SEI or the solid electrode). The high diffusion resistance of lithium may be a rate-determining factor in the anode material. The semicircle and long line were present in the impedance spectrum obtained for 1M LiPF
6 (in EC:DMC, 1:1) during charge/discharge. However, after charging/discharging one, much smaller semicircle was present in the spectrum.
The resistance of the SEI layer,
RSEI, formed before and after charging/discharging on anode were listed in
Table 6. All value are much smaller after galvanostatic charging-discharging. A possible explanation is that at a higher temperature the thickness of the SEI layer formed was greater.
The charge transfer resistance,
Rct, of the MnO
2/KL+B|Li
+ anode was ca. 31 Ω, decreasing to ca. 18 Ω after charging/discharging (see
Table 6). The charge transfer resistance of MnO
2/KL+B electrode is 18 Ω, which is slightly lower than that of MnO
2/KL+A electrode (205 Ω), and MnO
2/KL+C (80 Ω) confirming that the electronic conductivity of MnO
2/KL+B electrode is better than that of another two electrodes. Hence, this is one of the reasons that the specific capacity of MnO
2/KL+B is higher.
The diffusion of electro-active species may be attributed to the line visible in the low-frequency region. In general, the Warburg model based on a symmetrical constant phase element is applied by all software responsible for the deconvolution of the EIS curve. Therefore the approximation of the diffusion process is based on the Zw (the Warburg element). In case of the linear parts, the slopes were not at 45° in contrast to the preductions of the Warburg model. Furthermore, an increase of the diffusion impedance with the increase of temperature was observed in case of the MnO2/activated lignin|Li+ anode, however the explanation of this phenomenon is difficult. On the other hand, a considerable decrease of the diffusion impedance with the increase of temperature was observed in case of the MnO2/activated lignin anode.
Moreover, it is considered that the semicircle in the low frequency region may be attributed to ohmic resistance, which corresponds to the electrolyte R
el in the equivalent circuit. The resistance associated with the charge transfer occurring on the electrode/electrolyte interface, which is related to a parallel circuit element, may correspond to the semicircle in the medium frequency region. This corresponds to the capacitance of the double layer C
dl as well as the resistance of charge transfer
Rct in the equivalent circuit. The linear part, associated with the diffusion of Li ions in the electrode, may correspond to Z
w (the Warburg element) in the equivalent circuit [
70]. Further explanations may be found in corresponding literature reports [
71,
72,
73]. The obtained data was analysed by fitting equivalent circuit [
70].
The transition metal oxides (TMOs) are another group of studied anode materials, which are mostly characterized by a specific mechanism of lithium storage in comparison to the two previous types of metal oxides. The resulting forward displacement redox reaction involving MO and Li
+ is favourable in terms of thermodynamics. Usually multiple-electron transfers per a single metal atom are required for the conversion of metal oxides to their metallic state, which results in a high theoretical storage capacity of lithium [
74,
75].
However, it seems that the reversed reaction of extracting Li+ from Li2O cannot be achieved thermodynamically under normal conditions. The formation of metal nanoparticles (M) upon first discharge may facilitate the reversible formation and decomposition of the Li2O matrix, and the use of nanostructured materials possessing large surface area, high surface energy and enhanced electrochemical reactivity can also facilitate the backward reaction. The nanoscale facilitates the conversion reaction and improves its reversibility. Aside from the abovementioned potential thermodynamic and kinetic limitations associated with lithium diffusion, it has also been established that the reorganization of structure and variation of volume resulting from the charge/discharge may also lead to the cracking of active materials and rapid decrease of their capacity. It may possible to overcome such restrictions of TMO-based materials by preparation of specific nanostructures which would sustain structural disintegration and facilitate reactions associated with lithium storage.
2.3.2. Cyclic Voltammetry
Figure 15 shows the cyclic voltammograms of MnO
2, MnO
2/KL+A, MnO
2/KL+B and MnO
2/KL+C electrodes in the potential range from 1 to 3 V (versus Li/Li
+) at a scan rate of 0.2 mV s
−1 for the first cycle. Notably, the redox curves of the first two samples intersect at a low potential.
It can be seen that the shapes of the CV curves for the four samples are similar, indicating that the reduction and oxidation process of the prepared MnO
2/KL+IL samples are consistent (with the exception of
Figure 15c). As seen in
Figure 15b–d, the three peaks at 2.35 V; 1.90 V and 1.01 V in the cathodic scan, which may arise from the formation of a solid electrolyte interface (SEI) layer and can be assigned to the electrochemical reduction of MnO
2 with Li, respectively [
76]. The shifts may be associated with the presence of activated lignin. The oxidation peaks centered at 1.23 V in the anodic scan are characteristic for the oxidation reaction. Significant flattening of the peaks in oxidation and reduction can indicate that the MnO
2/KL+A and MnO
2/KL+C have an immense polarization effect.
Although acceptable performances were not yet reached for the majority of applications due to low output voltage, this first attempt presents some advantages of MnO
2 and activated lignin that react with Li through two-step processes, separated by a potential. Since each ΔV depends on the potential values of each respective process, they can be modified using chemical methods (e.g., by changing the nature of active species, substitution of functional groups, or addition of a modifier), in order to either separate or merge the two redox processes. Of course, this requires further analysis of quinone groups and their potential impact on electrochemical processes [
77].
Other studies report the use of polymers [
78,
79,
80] and radical polymers [
81,
82,
83] or organic radicals as possible electro-active materials in Li-ion batteries. Working with such systems is associated with many issues therefore researchers are looking for new solutions. Authors demonstrated the principle by grafting a quinine derivative of calix[4]arene onto the surface of two different substrates: (a) nanosized silica particles and (b) selected carbon black samples. Although this approach has several limitations, it can in principle be enhanced by the use of appropriate novel solutions. The energy density lost as a result of grafting on inactive substrate may be efficiently restored by the use of organic compounds with lower molecular mass or substrates which exhibit very high surface area. In addition, high loading of redox active molecules may be alternatively achieved by construction of electrode composites similar to those proposed recently in Li–S batteries [
84]. Recent literature reports confirm that strong interactions between organic compounds and the surface of carbon may be achieved during their electrochemical treatment [
85,
86]. As a result, effective grafting of specific compounds onto a substrate may potentially be obtained by employing electrochemically assisted covalent modification of substrates.
The authors observed more pronounced peaks of oxidation and reduction processes only in
Figure 15c. This property has shifted to a higher stiffness of this electrode during the charging/discharging process.
2.3.3. Charging/Discharging
Figure 16a displays the rate performance of MnO
2, MnO
2/KL+A, MnO
2/KL+B and MnO
2/KL+C electrodes at 50 mA·g⁻
1, 100 mA·g⁻
1, 200 mA·g⁻
1, 500 mA·g⁻
1 and 1000 mA·g⁻
1 for 20 cycles each. The results show that the specific capacity decreases with increasing current density, since high current density causes a low rate of the Li-ion diffusion [
87].
The MnO
2/KL+B delivers specific capacities of 760, 605 and 587 mAh·g⁻
1 at current densities of 50, 100 and 200 mA·g⁻
1, respectively. Even at a current density of 1000 mA·g⁻
1, the MnO
2/KL+B electrode still maintains a specific capacity as high as 520 mAh·g⁻
1. Remarkably, all of these values are much higher than for MnO
2/KL+A, MnO
2/KL+C and MnO
2, suggesting that the rate capability of the MnO
2/KL+B electrode is superior in comparison with the other three electrodes. The excellent electrochemical performance of the MnO
2/KL+B composite may be attributed to the unique porous structure, which provides many large electrochemical sites and a short pathway for Li-ion diffusion, and limits the volume change, as well as the synergistic effect of activated lignin (with ionic liquid–triethylammonium hydrogen sulfate) and MnO
2 [
51,
88,
89].
Numerous studies have been carried out on the characterization of the SEI (solid electrolyte interphase) on the negative electrode in Li-ion batteries. The chemical composition at a detailed level is dependent on the type of salt present in the electrolyte, temperature, type and surface chemistry of the anode, among other parameters [
90].
Firstly, the activated lignin coating most likely prevents the direct exposure of MnO2 to the electrolyte, and thus maintains the structural and interfacial stabilization. Secondly, the activated lignin coating favors formation of a stable SEI layer owing to the improved surface chemistry state of MnO2. Thirdly, the activated lignin can accommodate the large volume change of MnO2 and thus improve the electrochemical activity. Fourthly, the activated lignin provides abundant electroactive sites for Li-ion storage. In addition, the components in the MnO2/activated lignin have a synergistic effect on the cycling stability. It should be noted that all of the electrodes (MnO2/activated lignin) had stable capacities and no significant drop in stability was observed as in the case of pure MnO2.
The charging/discharging profiles for the electrodes of MnO
2 and MnO
2/KL+B at a current of 50 mA·g⁻
1 are shown in
Figure 16c,d. It can be clearly observed that the MnO
2/KL+B electrode has a much better capacity performance and cycling stability. After 20 discharging and charging cycles, it delivers a discharge capacity of 750 mAh·g⁻
1, whereas that of the MnO
2 electrode is only 250 mAh·g⁻
1. Moreover, after the initial cycles, the Coulombic efficiency (
Figure 16b) can reach up to 98.5%, which further indicates that the MnO
2/KL+B electrode has good reversibility. The lowest value is observed for pure MnO
2 (Coulombic efficiency: 86%), which is due to significant decrease in capacitance during charging and discharging and poor electrode reversibility. For other electrodes, the Coulombic efficiency is similar: MnO
2/KL+A = 89% and MnO
2/KL+C = 91%, respectively.
There was one plateau at approx. 1.1 V in the charge process and one plateau at approx. 0.47 V in the discharge process (
Figure 16c–d). The shape of the charge-discharge curves is typical for the conversion reactions of transition metal oxide anode materials. It has been found that the reaction leads to formation of nano metal clusters embedded in Li
2O matrix, accompanied by enormous structural change [
91,
92].
The gradual increase of capacity in case of nanosize metal oxide anodes, may potentially result from a mechanism associated with interfacial storage of metal oxides nano domains due to the amorphization process which occurs during cycling [
93,
94,
95]. Both the rate capability and cycle stability of the composite were similar in comparison to other reports regarding manganese dioxide anode materials [
51,
96,
97,
98].
Moreover the practical capacity provided by the transition metal oxide and phosphate anodes has reached its maximum intrinsic limit (140–170 mAh·g⁻
1). In this respect, there is an increasing demand for the development of cathode and anode materials which have higher capacity [
99,
100]. Organic electrodes offer high theoretical capacity (300–800 mAh·g⁻
1) due to possible low molecular weight structure and multiple electron redox reaction [
101]. Their electrochemical properties could be finely tuned by structural modification. Although properties of organic compounds are desirable, critical issues such as dissolution of electrodes in liquid electrolytes, low electronic conductivity, irreversibility and low cyclability, should be addressed. Recently organic electrode materials are revisited by many research groups [
101,
102].
One of the main challenge in the development of organic electrode material is the capacity loss due to dissolution of the material in liquid electrolytes. Attempts have been made to tackle this problem by optimization of molecular structure, polymerization, using higher content of carbon, low solubility electrolyte etc. But one of them completely eliminates the problem of dissolution and gives higher capacity [
78,
80,
103,
104,
105]. Therefore the fundamental solution to dissolution of electrode material is solid state battery. Solid state batteries are gathering increasing attention compared to the liquid electrolyte based battery due to their potential advantages over the latter [
106,
107]. In this regard, it is highly important to study the organic electrodes in conjunction with the electrolytes.
It has been reported that materials based on metal oxides exhibit increased lithium storage performance as a result of their efficient traits in terms of Li
+ ion insertion and buffering of volume during the charge-discharge process [
108,
109]. Additionally, the hybrid core/shell structures exhibited improved electrochemical properties compared to those based on a single component as a result of higher surface areas and integral configurations [
110,
111].
In the table 7 are listed the new composite-electrode materials for comparison with the anode presented in this paper.
Moreover many efforts have been done in the investigation of both carbon and non-carbon materials for high performances and high capacity anode in LIBs. A short list must include: carbon nanotubes (1100 mAh·g⁻
1) [
112], carbon nanofibers (450 mAh·g⁻
1) [
113], porous carbon (800–1100 mAh·g⁻
1) [
114], SiO
x-based anodes (1600 mAh·g⁻
1) [
115], germanium (1600 mAh·g⁻
1) [
116], tin (994 mAh·g⁻
1) [
117] and transition metal oxides (500–1000 mAh·g⁻
1) [
118,
119,
120]. Furthermore, metal sulphides, phosphides and nitrides [
121,
122,
123] might be also considered for anodes purposes, in fact they possess specific capacity higher ca. 500 mAh·g⁻
1. However, high volume expansion, poor electron transport, capacity fading, and low coulombic efficiency as well, are the main limitations that have to be overcame before they can be used as effective anodes. Compared to the literature (
Table 7), the presented material, in particular its capacity, falls within the confines of other scientists.