3.1. Morphological, Elemental, and Structural Characterization
The final MnO2–CFs composite materials, synthesized via in situ redox deposition and electrochemical deposition methods prior to hydrogen exposure, were analyzed using EDS quantification to determine the manganese concentration, thereby evaluating the relative efficiency of each synthesis environment.
Theoretically, considering the redox deposition, a progressively increasing concentration of MnO
2 on the sample surface is expected as the contact time between the fibers and the reagent increases [
17]. This does not apply to the samples with reaction times of 2 h and 6 h, respectively (
Table 4), which, due to inadvertent handling errors or uncontrolled variables during the setup, may have influenced the reproducibility. The pronounced decrease in Mn% observed between the repetitions b and c during electrochemical depletion could be the result of procedural inconsistencies during sample preparation or measurement.
Further characterization was conducted on the samples with the highest manganese content from each synthesis method—specifically, the in situ redox deposition sample with a reaction duration of 24 h (MnO
2/CF #1) and the electrochemical deposition sample with a reaction time of 20 min at 28 °C (MnO
2/CF #2) (
Table 5).
Based on the comparison of SEM/EDS results, conclusions can be drawn regarding the effectiveness of the in situ redox deposition method and electrodeposition synthesis for producing the desired material.
The SEM images of sample MnO
2/CF #1 reveal dispersed bright and speckled features across the carbon fiber surface (
Figure 3), corresponding to MnO
2 deposits. The distribution appears non-uniform, with areas of higher local concentration, while untreated CFs exhibit a relatively smooth and featureless surface (
Figure 4). It may be remarked that the particulate structures observed on the surface of the carbon fibers are likely by-products from the activation process. During activation, the carbon fibers are treated with acidic solutions (such as HCl), which may cause oxidation of the fiber surface. This oxidation process can lead to the formation of small particles, which are likely residues from the oxidation treatment. These particles are not related to the final MnO
2 deposition process. The EDS results of sample MnO
2/CF #1 (
Figure 5 and
Table 6) confirm the presence of Mn on the fiber surface, along with oxygen originating from surface oxidation of the carbon fibers and Mn–O bonding of the deposited manganese oxides.
The electrochemically deposited MnO
2 layer is relatively dense and uniform, with a coating thickness in the micrometer range, approximately 8.10 μm (
Figure 6). However, certain regions show thinner coverage or partial exposure of the underlying carbon fibers, indicating some degree of non-uniformity. The corresponding EDS analysis (
Figure 5 and
Table 6) confirms the successful deposition, showing strong Mn peaks together with oxygen contributions consistent with MnO
2 formation and minimal impurities.
Raman spectroscopy reveals the characteristic D and G bands of carbon fibers at approximately 1350 cm
−1 and 1580 cm
−1, respectively, in a plain activated carbon fiber sample (CF/H
2) (
Figure 7,
Table 7) and the sample MnO
2/CF #2, composed electrochemically (
Figure 7,
Table 8). A comparative analysis between a MnO
2-free sample and a MnO
2-containing sample demonstrates the presence of a prominent phonon band at 650 cm
−1, attributed to Mn–O A
1g symmetric stretching vibrations, as well as a weaker band within the 200–500 cm
−1 range, corresponding to Mn–O bending vibrations. In general, the MnO
2-containing sample exhibits distinct peaks within the 200–800 cm
−1 region—characteristic of manganese dioxide—which are absent in the MnO
2-free sample. Taking into account the sample MnO
2/CF #2, it is estimated using the peak areas that the ratio
= 2.51, while the sample CF/H
2 exhibits
= 2.38, both showcasing structural defects in the carbon structure. The structural defects were induced by acid treatment, conducted prior to deposition, which led to the formation of functional groups within the graphite matrix of the carbon fibers (CFs) [
11,
20,
21].
The G band appears near ~1580 cm
−1 in the Raman spectra of sp
2 carbon materials and originates from the in-plane stretching of C–C bonds, specifically the E2g vibrational mode of sp2 carbon atoms within the hexagonal lattice [
22]. The D band appears around ~1350 cm
−1 and is activated by structural disorder in sp
2 carbon systems. The D band originates from a double-resonance scattering process with A
1g symmetry, in which phonons near the K point of the Brillouin zone are involved. Unlike the G band, it is forbidden in perfect crystalline graphite and only becomes Raman-active in the presence of defects, edges/curvature, finite crystallite size, or heteroatomic substitutions. Its intensity increases with the density of defects or disruption of the sp
2 network [
23]. For carbon-based materials like graphene, carbon nanotubes, or amorphous carbon, the intensity ratio of the D band to the G band is used as a quantitative metric that reflects the degree of structural order/disorder, defect density, and crystallite size in sp
2 carbon systems. Amorphous carbon phases, vacancies, and dopants cause significant increases in D-band, indicating structural disorder in carbon materials.
Raman spectroscopy was used to investigate the sample with a 24 h chemical synthesis, both prior to (MnO
2/CF #1) (
Figure 7,
Table 9) and after exposure (MnO
2/CF/H
2 #1) (
Figure 7,
Table 10) to hydrogen gas. The intensity ratio I
D/I
G for MnO
2/CF #1 is 2.37, calculated using the integrated areas of the respective peaks, while sample MnO
2/CF/H
2 #1 exhibits an I
D/I
G ratio of 2.81, indicating the presence of structural defects in the carbon framework in both cases.
The peaks observed in the range 200–800 cm
−1 in both spectra can be attributed to the presence of MnO
2. More specifically, for the sample prior to hydrogen exposure (
Figure 7,
Table 9), peaks 1 (~353 cm
−1), 2 (~562 cm
−1), 3 (~626 cm
−1), and 4 (~971 cm
−1) correspond to bending and twisting modes of Mn–O bonds (arising from Mn in different polymorphic forms). The highest of these four peaks (peak 4), which is absent in the spectrum of the hydrogen-exposed sample, may be associated with more stable or rigid MnO
2 structures, such as β-MnO
2. In the spectrum of the same material after hydrogen treatment (
Figure 7,
Table 10), the number of peaks within the 200–800 cm
−1 range is reduced, their intensity increases, and a shift toward higher wavenumbers is observed. This behavior may be attributed to a phase transformation of manganese and/or its partial reduction to lower oxidation states, such as the formation of MnO [
24,
25].
The structure of the synthesized fibers was further examined using FTIR spectroscopy. Specifically,
Figure 8 presents the FTIR spectra of the following: (a) acid-treated carbon fibers; and (b) MnO
2/CF/H
2 #2, which was synthesized via electrochemical deposition for 20 min at 28 °C and subsequently exposed to H
2 treatment.
Considering the spectrum of sample #2′, the broad band at 3500–3700 cm
−1, corresponding to O–H bending vibrations, indicates the presence of hydroxyl groups, which may be attributed to either adsorbed water or the partial reduction in MnO
2. The broad band at 2220–2260 cm
−1 is assigned to C≡N stretching vibration; CFs made from polyacrylonitrile often retain small amounts of nitrile (–C≡N) groups. The band observed at 1054 cm
−1 is likely associated with C–OH bending vibrations, suggesting surface oxidation of the carbon fibers. The peak at 1525 cm
−1 corresponds to C=C bending vibrations, characteristic of the carbon fiber backbone. Alternatively, it may arise from O–H bending involving oxygen atoms coordinated to manganese [
26,
27]. Expected Mn–O bending absorptions typically occur in the region of 400–700 cm
−1. In the recorded FTIR spectrum, several low-intensity peaks are indeed observed within this range, notably at 671 cm
−1, which supports the presence of manganese oxides. Additionally, the peak at 773 cm
−1 may be attributed to a characteristic adsorption of manganese oxides with a tunnel-type structure [
28]. Regarding the spectrum of the acid-treated carbon fibers, it is evident that the peaks due to manganese vibrations are absent (671 cm
−1, 773 cm
−1).
X-ray photoelectron spectroscopy (XPS) spectra of the MnO2/CFs produced electrochemically for 20 min at 28 °C (sample #2) were used to determine the surface composition of the material prior to and after hydrogen exposure and to examine the oxidation state of Mn.
Based on the Mn 2p XPS spectra of sample MnO
2/CF #2 prior to hydrogen exposure (
Figure 9i), the surface composition is predominantly manganese in the +4 oxidation state (Mn
4+), corresponding to MnO
2. This is evidenced by the characteristic Mn 2p
3/2 and Mn 2p
1/2 peaks observed at 641.985 eV and 653.480 eV, respectively (spin-energy difference of 11,495 eV), along with the presence of shake-up satellite features typically associated with Mn
4+ [
29]. Quantitative analysis indicates that Mn
4+ accounts for approximately 96% of the total manganese signal. A minor contribution from Mn
2+ (MnO) is also detected, represented by weaker peaks at 640.303 eV (2p
3/2) and 650.476 eV (2p
1/2), comprising about 4% of the surface Mn species.
Following hydrogen exposure (MnO
2/CF/H
2 #2), the Mn 2p spectrum reveals significant changes in the oxidation state distribution (
Figure 9ii). New peaks appear at 639.869 eV (2p
3/2) and 651.064 eV (2p
1/2), corresponding to Mn
2+ species, now constituting approximately 7.9% of the manganese signal. Additionally, peaks at 641.400 eV (2p
3/2) and 652.824 eV (2p
1/2) are attributed to Mn
3+ species, which account for 36.1%. The proportion of Mn
4+ consequently decreases to 56%, indicating a partial surface reduction in MnO
2 upon hydrogen treatment. This suggests that not all Mn
4+ species participated in the hydrogen storage process [
10,
11,
12].
The comparison of Mn 3s XPS spectra between the two samples also confirms the partial reduction in MnO
2 to lower oxidation states (
Figure 10).
The O 1s XPS spectra of MnO
2/CFs provide information about the environment of O on the surface of the material before and after hydrogen exposure (
Figure 11). In
Figure 11, the band at 529.56 eV (33.8%) is attributed to the lattice oxygen in metal oxides, meaning Mn–O bonds within the MnO
2 structure. The band at 531.222 eV (25.2%) corresponds to carbonyl oxygen (C=O) groups, which may appear due to the previous oxidation of the carbon surface, while the band at 533.162 eV reveals the presence of C–O bonds (41%), which may occur due to air exposure. The XPS spectrum of O 1s after H conditioning showcases the same bands increased in concentration (69.4%) for the Mn–O bond at 529.784 eV, while the peaks for C=O at 531.136 eV and C–O at 533.372 eV decrease at 12.6% and 6.0%. This phenomenon suggests that the hydrogen treatment might have reacted with or removed some of these oxidized carbon species, possibly through hydrogenation reactions, forming volatile products like water or hydrocarbons. The band at 531.926 eV corresponds to –OH, meaning the formation of a hydrolyzed manganese oxide and proving the reduction in Mn [
10,
11,
12].
By integrating the data obtained from both the O 1s and Mn 2p XPS spectra, it is possible to quantify the percentage of MnO
2 present on the surface of the material before and after hydrogen conditioning, although the quantitative comparison of the two samples is not comparable due to uneven deposition of the material. Further information will be shown in
Appendix A.
3.2. Thermal Behavior Characterization
The study of TGA diagrams of the synthesized MnO
2/CFs materials under inert and oxidative atmospheres provides insight into the fiber composition and their hydrogen adsorption capacity. The thermogravimetric curve reflects various mass changes occurring during the decomposition process. The inclusion of the first derivative (DTG) in the diagram aids in detecting subtle mass changes that may not be clearly visible in the standard mass loss curve as a function of temperature [
30].
TGA studies of carbon fibers in an oxidative environment (presence of O
2) show a gradual mass loss of 1.6% up to 450 °C, followed by a sharp mass reduction between 500 and 820 °C, attributed to oxidative activity on the fiber surface. In contrast, carbon fibers in an inert atmosphere (N
2), under the same heating rate (20 °C/min), exhibit minor mass changes, with a mass loss of approximately 1.2% between 200 and 450 °C [
31]. Manganese dioxide (MnO
2) in the presence of air (O
2) exhibits a mass change at T ≈ 250–400 °C due to the following reaction:
and another mass change at 400–600 °C attributed to the following transformation [
32]:
Under inert conditions (N
2), the same transformations occur but at higher temperatures, with a mass loss of approximately 9% at T ≈ 500–600 °C, and an additional ~3% mass loss at 700–800 °C, corresponding to the same respective conversions [
33].
Both sample MnO
2/CF #1 before and sample MnO
2/CF/H
2 #1 after hydrogen exposure were studied under inert conditions (N
2 atmosphere). In the case of sample #1, a mass increase from 100% to 105% is observed up to 500 °C, followed by a 1% mass loss (
Figure 12). In contrast, the hydrogen-exposed sample (MnO
2/CF #1) shows a continuous mass decrease from 400 °C to 800 °C. In DTG curve, a negative peak appears around 500 °C, corresponding to a mass loss of approximately 7%. A contradiction seems to exist because, according to the literature, MnO and Mn
2O
3, which are manganese oxide phases, are known to gain mass under inert conditions, and these forms should be present after hydrogen exposure (i.e., in sample MnO
2/CF/H
2 #1). However, the TGA results suggest its presence in the pre-exposure sample (MnO
2/CF #1), while the post-exposure sample (MnO
2/CF/H
2 #1) exhibits mass loss, indicative of MnO
2 decomposition. This inconsistency may stem from an experimental error during sample handling, sampling procedures, or during the hydrogen exposure process.
Samples MnO
2/CF #2 and MnO
2/CF/H
2 #2, before and after hydrogen exposure, respectively, were analyzed under both inert (N
2) and oxidizing (O
2) atmospheres. In the TGA spectrum of sample MnO
2/CF #2, initial thermal stability is observed up to 500 °C, followed by a sharp mass loss of approximately 87%, reaching a plateau at 700 °C (
Figure 13). Beyond this temperature, the residual mass stabilizes at 13%. Comparing these results with known TGA profiles of pure carbon fibers suggests that the remaining mass likely corresponds to the presence of MnO
2 or other impurities. Weight loss in an oxidizing environment may be attributed to the total decomposition of carbon fibers to gas CO
2, which takes place at 400–600 °C. Similarly, in the hydrogen-treated sample (MnO
2/CF/H
2 #2), thermal stability is also maintained up to 500 °C, followed by a sharp mass loss of around 75%, resulting in a final residual mass of approximately 25% (
Figure 13). The hydrogen-treated sample consists of a higher percentage of MnO and MnOOH, which are the reduction products of MnO
2. Thus, in the hydrogen-treated sample, an increase of about 12% in residual mass is observed. This increase may be attributed to MnO
2 transformations upon reduction, leading to the formation of manganese oxides with higher thermal stability and greater residual mass.
Under inert conditions (N
2), we observe the weight change attributed mainly to the behavior of the deposited Mn oxides on the surface of CFs, as the carbon fibers do not decompose under an inert atmosphere. More specifically, MnO
2/CF #2 exhibits a slight mass loss of approximately 0.5% up to 130 °C, with a DTG minimum peak at 70 °C (
Figure 14). Between 150 and 300 °C, a gradual 0.5% mass decrease is observed, with a DTG peak at 250 °C, which is consistent with the typical TGA behavior of carbon fibers. In the range of 350–500 °C, a minor additional mass loss may be attributed to the conversion of MnO
2 to Mn
2O
3, which occurs due to high temperature exposure and releases gas O
2.
In contrast, MnO
2/CF/H
2 #2, after exposure to hydrogen, shows a gradual mass increase from 100% to 108% with rising temperature, a behavior that aligns with TGA data for MnO and Mn
2O
3 phases, which are known to undergo mass gain in inert environments due to their thermal oxidation characteristics (
Figure 14) [
31].
3.3. Electrochemical Response of CF-Electrodes Towards [Fe(CN)6]3−/4−
The electrochemical responses of bare CF and MnO
2-modified CF electrodes towards ferrocyanide/ferricyanide [Fe(CN)
6]
3−/4− standard redox system were studied by means of the cyclic voltammetry method in aqueous KCl solution (1.0 mol∙L
−1). The results obtained for all studied electrodes are presented in
Table 11. Representative CVs are illustrated in
Figure 15a. In CV-curves depicted in
Figure 15a, the redox system [Fe(CN)
6]
3−/4− exhibits a pair of reversible redox peaks on CF-based electrodes. The oxidation-reduction peak current ratio is equal to unity and independent of applied scan rate, indicating that there are no parallel chemical reactions coupled to the electrochemical process. Similarly, the oxidative and reductive peak currents are constant for numerous cycles, indicating that there are no chemical reactions coupled to the electron-transfer process and confirming that the redox system is stable in the time frame of the experiment and that the charge-transfer process occurring on MnO
2-modified CF electrodes is quite reversible. The half-wave potential estimated for [Fe(CN)
6]
3−/4− redox system on MnO
2-modified CF electrodes appears to be similar within experimental error (E
1/2 ≈ 0.275 V vs. Ag/AgCl), something that is quite expectable for reversible redox systems. Furthermore, the anodic and cathodic peak currents were found to vary linearly with the square root of scan rate in the investigated range of 0.02–0.10 V·s
−1, demonstrating that the studied redox system [Fe(CN)
6]
3−/4− is diffusion-controlled on CF-based electrodes. From the extracted electrochemical parameters presented in
Table 11, it can be clearly seen that the anodic and cathodic peak potential separation (ΔE
p) estimated for [Fe(CN)
6]
3−/4− on bare CF and MnO
2-modified CF electrodes lies in the range from 0.068 to 0.236 V (at the scan rate of 0.02 V·s
−1), demonstrating differences between charge-transfer kinetics of [Fe(CN)
6]
3−/4− on the various MnO
2-modified CF composite films studied. Namely, the large peak separation of the MnO
2/CF #2 electrode (ΔE
p = 0.086 V) indicates poorer electron-transfer kinetics of [Fe(CN)
6]
3−/4− on this particular electrode compared to the other electrodes studied. The electron-transfer kinetics of MnO
2/CF #2 become even worse after the H
2-treatment. Thus, on the MnO
2/CF/H
2 #2 electrode, a fairly great value of peak potential separation has been estimated (ΔE
p = 0.236 V). The smallest peak potential separation has been obtained for MnO
2/CF #1 electrode (ΔE
p = 0.068 V), which is slightly smaller compared to that of the bare CF electrode (ΔE
p = 0.070 V), and it tends to increase after H
2-treatment. Consequently, on MnO
2/CF/H
2 #1, a slightly greater peak potential separation value has been obtained (ΔE
p = 0.081 V) compared to the untreated MnO
2/CF #1 electrode. Consequently, the heterogeneous electron transfer rate constants (
ks) determined for [Fe(CN)
6]
3−/4− on bare CF and MnO
2-modified CF electrodes by means of electrochemical absolute rate relation tend to increase in the following order: MnO
2/CF/H
2 #2 < MnO
2/CF #2 < MnO
2/CF/H
2 #1 < CF < MnO
2/CF #1 (
Figure 15b). The EIS measurements were carried out on MnO
2-modified CF electrodes in the presence of [Fe(CN)
6]
3−/4− redox system for the estimation of charge-transfer resistance (
Rct) (
Figure 15c). This parameter provides an estimation of the barrier to overall heterogeneous electron transfer occurring at the electrode–electrolyte interface. The estimated
Rct values are included in
Table 11 along with the other electrochemical parameters of [Fe(CN)
6]
3−/4− on various MnO
2-modified CF electrodes. The
Rct values obtained on various MnO
2-modified CF electrodes are presented graphically in
Figure 15d. It is quite interesting that the charge-transfer resistance estimated by means of EIS tends to decrease in the order: MnO
2/CF/H
2 #2 < MnO
2/CF #2 < MnO
2/CF/H
2 #1 < CF < MnO
2/CF #1 (similarly to
ks parameter), indicating that a diminishing of barrier of redox process with the simultaneous enhancement of electron-transfer kinetics takes place. For the estimation of the lower limit of detection and sensitivity of CF and MnO
2-modified CF electrodes towards [Fe(CN)
6]
3−/4−, the variation in oxidation peak current with the concentration of redox system in the concentration range of 7.0 × 10
−5–1.0 × 10
−3 mol∙L
−1 was examined. The electrochemical response of CF and MnO
2-modified CF electrodes towards [Fe(CN)
6]
3−/4−, plotted as oxidation peak current density versus concentration of electroactive compound, appears to be linear in the investigated concentration range. From the standard deviation of the electrochemical response and the slope of linear oxidation current-concentration plots, the lower limit of detections of bare CF and MnO
2-modified CF electrodes towards [Fe(CN)
6]
3−/4− were estimated and are included in
Table 11. The results exhibit that the electrochemical quality of MnO
2-modified CF electrodes can be considered quite good.
Overall, the characterization techniques employed in this study offer a thorough understanding of the composition of the functionalized materials. In particular, Raman spectroscopy validated the surface modification of pure carbon fibers by the comparison of Id/Ig ratios, which showcases the structural defects in the carbon framework. X-ray photoelectron spectroscopy (XPS) results prove that the product obtained electrochemically showcases a partial reduction in Mn on the surface of the CFs when exposed to hydrogen gas and proves the formation of an MnOOH intermediate. The presence of the MnOOH intermediate can be validated by FTIR spectroscopy, which showcases the presence of -OH groups in the prepared sample in addition to the Mn-O bonds. The possible application of fabricated carbon fiber/MnO2 composites as materials in electrochemical sensors has been studied in the presence of [Fe(CN)6]3−/4− in aqueous KCl solutions. The obtained results are rather promising and demonstrate the future potential application of carbon fiber/MnO2 composites as working electrodes in electroanalysis.
The investigation into the hydrogen storage capabilities of these materials requires further investigation regarding the release mechanism of the bonded hydrogen, but suggests that the CFs/MnO2 composite represents a promising avenue for enhancing energy storage technologies. This approach aligns with the growing demand for sustainable energy solutions. Such composite materials hold potential for a variety of industrial applications. One proposed application involves incorporating the modified fibers into textile structures capable of surface hydrogen storage, suitable for use in portable electronic devices, hybrid storage systems, and fuel cells. Additionally, these materials could function as hydrogen sensors or serve as catalysts in hydrogen production and processing reactions. Another prospective application of MnO2/CFs lies in hydrogen storage tanks for fuel-cell electric vehicles (FCEVs), either as a primary storage material or as a reinforcing component in advanced polymer composites.