Home Physical Sciences Single-step fabrication of Mn(iv) oxide-Mn(ii) sulfide/poly-2-mercaptoaniline porous network nanocomposite for pseudo-supercapacitors and charge storage
Article Open Access

Single-step fabrication of Mn(iv) oxide-Mn(ii) sulfide/poly-2-mercaptoaniline porous network nanocomposite for pseudo-supercapacitors and charge storage

  • Eman Aldosari , Mohamed Rabia EMAIL logo , Qinfang Zhang and Hissah Hamad Altilasi
Published/Copyright: June 17, 2025

Abstract

The single-step fabrication of the Mn(iv) oxide-Mn(ii) sulfide/Poly-2-mercaptoaniline porous network nanocomposite (MnO2-MnS/P2MA) involves incorporating the Mn source into the P2MA polymer during polymerization. XPS analysis confirms the presence of peaks corresponding to Mn(iv) and Mn(ii), while XRD analysis highlights the formation of pronounced crystalline peaks, indicative of excellent semiconductive properties, with a crystalline size of 42 nm. The nanocomposite serves as the main electrode for electrochemically assessing its charge storage capabilities. Optimal energy density (E) values are achieved at lower current densities, with 9.7 and 7.0 W h/kg at 0.6 and 1.0 A/g, respectively. Similarly, the specific capacitance (C S) reaches peak values of 120 and 86 F/g within the same current density range. The electrochemical impedance spectroscopy (EIS) behavior is notable, with an R s value of 7.3 Ω and an impressive cycle retention of 99.2% over 1,000 cycles. The combination of simple one-pot fabrication, excellent charge storage performance, and high stability underscores the potential of these materials for charge storage applications. The MnO2-MnS/P2MA nanocomposite’s superior EIS behavior, optimal energy and capacitance values, and remarkable cycle stability make it a promising candidate for efficient and reliable charge storage solutions.

1 Introduction

The growing energy crisis and diminishing fossil fuel reserves have heightened the development of sustainable and renewable energy sources. To utilize these energy sources efficiently, various energy-harvesting technologies are required. In addition to capturing energy, it is equally important to have effective energy storage systems that can store the electricity generated from regenerative materials. One promising approach for energy storage is through electrochemical means. Devices used in electrochemical energy storage are not only more environmentally friendly but also offer a practical solution for modern energy needs [1,2,3].

Electrochemical energy storage technologies, such as batteries and supercapacitors, are gaining attention due to their high energy density and exceptional cycle efficiency. The ability to quickly charge and discharge these systems is crucial for highly technology applications such as electric vehicles and spacecraft. Among these technologies, supercapacitors stand out because they can deliver rapid energy release and have excellent charge-discharge rates, making them ideal for applications that require quick bursts of power [4,5]. Supercapacitors, in particular, have drawn significant interest due to their ability to deliver rapid acceleration in the performance of storage devices, in which the produced power density allows for quick charging and long-time discharging, which is a valuable trait for many energy applications. Furthermore, their superior cycle life means a sustainable and long-term energy storage solution [6,7].

The advancement of nanostructured materials for supercapacitors has become a significant area of focus in many research initiatives. Nanostructured metal oxides are of particular interest due to their varied crystallographic structures and the ability to undergo redox reactions, making them valuable in electrochemical energy storage devices. Their unique properties enable them to play a crucial role in enhancing the efficiency and capacity of energy storage systems [8].

Among the different materials being explored, transition metal oxides and hydroxides are prominent choices for supercapacitor electrodes. Some widely used examples include MnO2, Co(OH)2, and vanadium pentoxide (V2O5), each of which has been extensively employed to improve the specific power density and capacitance of supercapacitors. These materials’ electrochemical properties allow for more efficient energy storage and conversion, which is essential for applications requiring rapid charge and discharge cycles. One material that stands out for its energy storage capabilities is manganese oxide-sulfide, which exhibits exceptional electrical charge storage behavior [9]. This material benefits from the synergetic effect of the metal oxide and sulfide, resulting in enhanced electrical conductivity and superior electrochemical performance. The combination of manganese oxide’s high theoretical capacitance and the sulfide component’s ability to facilitate fast redox reactions significantly improves the material’s overall charge storage capacity.

The utilization of these nanostructured materials is a key factor in the development of supercapacitors with higher energy densities and longer lifespans. The morphology and nanoscale structure of the metal oxides directly influence their electrochemical performance, as smaller particle sizes and higher surface areas allow for more efficient charge transfer and storage. Researchers are continually working on optimizing these properties through various synthesis techniques and material modifications to achieve even better results.

Overall, the exploration of nanostructured metal oxides and their derivatives, such as oxides and hydroxides of transition metals, has led to substantial progress in supercapacitors progress. By leveraging the distinctive properties of materials like MnO2, Co(OH)2, V2O5, and manganese oxide-sulfide, significant improvements in power density, capacitance, and cycle stability have been realized [10,11]. As research continues, these advancements are expected to drive the development of next-generation energy storage devices for sustainable and high-performance energy solutions.

The use of metal oxides in supercapacitor applications has been validated through various studies focusing on charge storage evaluation. For instance, the C S values for ZnO and Ni(OH)2 have been estimated at 61.7 and 20.5 F/g, respectively [12,13], when applied to supercapacitors. These findings illustrate the effectiveness of metal oxides in enhancing energy storage capabilities. Alternatively, some research approaches determine charge storage by measuring discharge times, revealing that materials like nickel oxide (NiO), titanium dioxide (TiO2), and cerium oxide (CeO2) demonstrate discharge times of 10, 5, and 20 s, respectively [14,15,16]. These measurements further emphasize the potential of metal oxides in energy storage applications.

Incorporating conjugated polymers has also shown promise in supercapacitor development by facilitating charge transfer and expanding composite material formation with metal oxides. A notable example is polyaniline-co-piperazine, which achieves a C S of 126 F/g [17]. Also, It was found that a polypyrrole/polyvinyl alcohol composite yielded a C S of 13 F/g, showcasing the diverse capabilities of polymer-based materials in supercapacitor technology [18]. Similarly, a device utilizing a PEDOT/LiTFSI-PVA composite achieved a C S of 44 F/g, further underscoring the potential of combining polymers with other materials to enhance performance [19]. Despite these advancements, there is still a need for more accurate estimations of storage efficiency and discharge times, as well as the development of more cost-effective fabrication techniques. Current supercapacitor materials vary in performance, and optimizing these devices for higher efficiency remains a challenge. To address these limitations, the integration of additional composite materials is necessary to achieve greater capacitance. Thiophene-based materials, in particular, offer significant promise when used in conjunction with other oxides and sulfides. These materials could play a crucial role in further improving the charge storage properties of supercapacitors.

In this study, MnO2-MnS/P2MA nanocomposite is synthesized using a one-pot approach. The material’s nanoscale crystalline framework, large-scale production capability, simple fabrication process, and porous structure contribute to its suitability for charge storage applications. To evaluate its electrochemical performance, the nanocomposite serves as the working electrode in a three-electrode cell configuration. Cyclic voltammetry and discharge curve analyses assess its charge storage behavior. The obtained values for P, E, C S, and EIS, and cyclic stability highlight its outstanding charge storage efficiency. The synergistic effects of MnO2 and MnS enhance the overall electrochemical properties of the composite, improving charge transfer kinetics and increasing active sites for ion diffusion. Additionally, the P2MA polymer matrix provides mechanical stability and facilitates ion transport, further optimizing the electrode’s performance. The porous structure enhances electrolyte penetration, ensuring efficient charge storage and retention. The material exhibits remarkable cyclic stability, retaining its performance over multiple charge–discharge cycles. This stability, combined with high specific capacitance and superior charge storage capabilities, underscores the potential of MnO₂-MnS/P2MA for next-generation energy storage devices.

2 Experimental

2.1 Materials

2-Mercptoaniline (99.9%, Merck, Germany), potassium permanganate (KMnO4, 99.8%, Pio-Chem, Egypt), hydrochloric acid (HCl, 36%, Pio-Chem), Na2SO4 (99.9%, Pio-Chem), Nafion (99.9%, Sigma Aldrich, USA), graphitic powder (99.8%, Pio-Chem), and ethanol (99.9%, Pio-Chem).

2.2 Synthesizing of MnO2-MnS/P2MA PN nanocomposite

The synthesis of the MnO2-MnS/P2MA PN nanocomposite is achieved through a one-pot technique that estimates the oxidation of 2-mercaptoaniline using KMnO4 as the oxidant. During this oxidation process, the resulting P2MA polymer is doped with the residues of oxidation, MnO2 and MnS, which become incorporated into the polymer network. This procedure begins by dissolving 0.06 M of 2-mercaptoaniline in 12 ml of HCl under vigorous stirring to ensure thorough mixing. Concurrently, KMnO4 is dissolved in distilled water to prepare the oxidant solution.

The reaction proceeds with the sudden addition of the KMnO4 solution into the 2-mercaptoaniline solution. This prompt addition triggers the oxidation process, which not only converts the monomer into the polymer but also facilitates the integration of MnO2 and MnS into the polymer matrix. These inorganic components are distributed within the polymer network, endowing the composite with enhanced chemical and electrical properties that are beneficial for charge storage applications.

The one-pot synthesis method is efficient in creating a nanocomposite where the polymer matrix is simultaneously formed and doped with the MnO2 and MnS particles. This integration is crucial as it imparts the composite with a synergistic combination of the polymer’s flexibility and the inorganic materials’ conductivity and electrochemical stability. The presence of MnO2 and MnS within the P2MA polymer enhances the overall performance of the composite, particularly in applications related to energy storage.

The resulting MnO2-MnS/P2MA PN nanocomposite exhibits improved electrical conductivity and electrochemical properties due to the distributed MnO2 and MnS particles within the polymer network. These properties are essential for efficient charge storage, making the composite an effective material for supercapacitor storage devices. The method’s simplicity and effectiveness in incorporating these inorganic materials into the polymer structure highlight its potential for large-scale production and application in advanced energy storage technologies.

2.3 The fabrication of pseudo-supercapacitor based on MnO2-MnS/P2MA PN nanocomposite and the electrochemical study

To fabricate a pseudo-supercapacitor based on the MnO2-MnS/P2MA PN nanocomposite, the composite is prepared as a paste and cast onto a carbon sheet (0.5 mm thick), which serves as the main electrode in a three-electrode cell. To create a homogeneous paste, the composite is dispersed in 5.0 mg of graphite powder, 0.1 ml Nafion, and 0.75 ml ethanol. This mixture is stirred at 1,000 rpm for 2 days at room temperature to ensure uniform distribution of materials. Once the paste is homogenous, it is cast onto the carbon sheet at a concentration of 0.003 g/cm². In setting up the three-electrode cell, the working electrode (the carbon sheet with the composite paste) is combined with two additional electrodes: a secondary electrode and a calomel electrode. The electrochemical measurements are carried out using a 1.0 M Na2SO4 electrolyte and a CHI608E electrochemical workstation. This device conducts electrochemical measurements by evaluating the current-voltage relationship to generate cyclic voltammetry over a potential range of 0.0–1.0 V. Additionally, it measures the time–voltage relationship through chronopotentiometry to determine the discharge time (Δt) and discharge voltage (ΔV). The C S of the pseudo-supercapacitor is specified using the discharge data and the mass load of the paste, as defined by Eq. (1) [2]. This calculation provides a measure of the capacitor’s ability to maintain charge.

To further assess the performance of the fabricated pseudo-supercapacitor, a Ragone plot is created. This plot illustrates the relationship between E and P, which are key indicators of a supercapacitor’s efficiency. These values are derived using Eqs. (2) and (3) [3], respectively, which take into account the maximum and minimum voltage values observed during the electrochemical tests.

Overall, the described method ensures the creation of a high-performance pseudo-supercapacitor by utilizing the MnO2-MnS/P2MA PN nanocomposite. The process includes detailed steps to achieve a homogenous paste, careful casting onto the carbon sheet, and precise setup of the three-electrode cell for accurate electrochemical measurements. This comprehensive approach guarantees that the fabricated pseudo-supercapacitor exhibits optimal charge storage capabilities and efficiency, as demonstrated by the cyclic voltammetry curves, chronopotentiometry data, and the resulting Ragone plot (Figure 1).

(1) C S = I · Δ t / Δ V · m ,

(2) E = 0.5 C S × ( V max 2 V min 2 ) ,

(3) P = E / Δ t .

Figure 1 
                  The single-step fabrication of the MnO2-MnS/P2MA PN nanocomposite and the fabrication of the pseudo-supercapacitor.
Figure 1

The single-step fabrication of the MnO2-MnS/P2MA PN nanocomposite and the fabrication of the pseudo-supercapacitor.

3 Results and discussion

3.1 Analyses

The characterization of the MnO2-MnS/P2MA PN nanocomposite was carried out using FTIR analysis, as shown in Figure 2(a). This provides and helps confirm the incorporation of MnO2-MnS into the polymer matrix by examining the functional groups present. For the pure P2MA polymer, the N–H and N–S stretching vibrations are observed at 3,373 cm⁻¹. However, in the PN nanocomposite, these peaks shift to 2,297 cm⁻¹, indicating the successful integration of MnO2-MnS within the polymer structure.

Figure 2 
                  The chemical investigation of MnO2-MnS/P2MA PN nanocomposite: (a) FTIR spectroscopy, (b) XPS Mn, (c) XPS survey, and (d) XRD pattern.
Figure 2

The chemical investigation of MnO2-MnS/P2MA PN nanocomposite: (a) FTIR spectroscopy, (b) XPS Mn, (c) XPS survey, and (d) XRD pattern.

A similar shift is observed for another vibrational mode, initially detected at 1,306 cm⁻¹ in the P2MA polymer, which appears at 1,310 cm⁻¹ in the nanocomposite. This change in the absorption band positions serves as a significant indicator of alterations in the molecular structure, specifically suggesting changes in the rotational dynamics of the ring groups due to the introduction of MnO2 and MnS. These shifts in the FTIR spectra highlight the interaction between the polymer and the inserted metal oxide and sulfide, suggesting modifications in the chemical environment and structural arrangement of the composite material. The results confirm that the presence of MnO2-MnS impacts the molecular vibrations, reflecting the successful formation of the PN nanocomposite and providing structural properties. Table 1 summarizes these groups’ investigation of the composite relative to the monomer.

Table 1

The FTIR analysis of functional groups in the MnO2-MnS/P2MA PN nanocomposite compared to the pristine P2MA polymer

Band position (cm−1) Group
MnO2-MnS/P2MA PN nanocomposite P2MA
3,397 3,373 N–H [20] and S–H [21]
1,467 and 1,624 1,514 and 1,619 Ring C–C and C═C benzene [22]
1,310 1,306 C–N [23]
1,124 and 1,209 1,126 and 1,216 C–H [3]
749 770 C–H bending out of plane ortho-disubstituted [24]

The chemical composition and oxidation states of the synthesized MnO2-MnS/P2MA PN nanocomposite are evaluated using XPS analysis. As shown in Figure 2(b), the XPS analysis of the Mn element focuses on the 2p orbital, revealing binding energies corresponding to Mn2+ and Mn4+, which are indicative of MnS and MnO2, respectively. For Mn2+, the binding energies are 641.1 and 653.2 eV for the Mn2p3/2 and Mn2p1/2 orbitals [25]. In contrast, Mn4+ exhibits binding energies at 642.5 and 654.8 eV for the same orbitals, respectively [26,28].

To further analyze the elemental structure of the MnO2-MnS/P2MA PN nanocomposite, a comprehensive XPS survey was conducted, as shown in Figure 2(c), and identifies the presence of various elements within the composite. The binding energies detected for carbon (C), nitrogen (N), and sulfur (S) are 285.3, 401, and 165.8 eV, respectively. Additionally, O for the oxide components is observed at 532 eV, and chlorine (Cl), attributed to the acidic medium, is identified at 200 eV. These findings confirm the elemental constituents of the MnO2-MnS/P2MA PN nanocomposite.

The detailed XPS analysis provides a crucial investigation into the chemical structure of the composite. The presence of Mn2+ and Mn4+ confirms the successful integration of MnS and MnO2 within the P2MA matrix. The identification of C, N, S, O, and Cl further substantiates the composite’s composition and the interactions between the organic polymer and inorganic constituents. The observed binding energies align with the expected values for these elements and their respective oxidation states, indicating a well-defined composite structure. To further assess performance, the elemental composition of the composite was analyzed using XPD. The estimated percentages of C, O, N, Cl, S, and Mn are 61.54, 16.5, 7.86, 3.9, 8.94, and 1.26%, respectively. Overall, the XPS analysis effectively characterizes the MnO2-MnS/P2MA PN nanocomposite, demonstrating the integration of the various components. The presence of Mn2+ and Mn4+ alongside other elements suggests a complex yet stable composite structure, suitable for applications in charge storage. The analysis confirms the chemical compatibility and integration of the materials, which is essential for optimizing the composite’s electrochemical performance. The detailed understanding of the elemental composition and oxidation states provided by XPS analysis is instrumental in advancing the development and application of this nanocomposite in energy storage technologies.

To complete the chemical characterization of the MnO2-MnS/P2MA PN nanocomposite, the crystalline behavior of these materials is analyzed using XRD patterns, as estimated in Figure 2(d). This analysis highlights a significant variation in the crystalline properties of the pristine polymer and the formed composite. After the formation of the composite, numerous peaks emerge, indicating a notable enhancement in the crystalline structure, which in turn suggests improved charge storage capabilities within the crystalline matrix of the composite.

For the MnO2 inside the polymer network, the XRD peaks reflect the formation of the alpha phase, in which these peaks are observed at 11.6, 17.2, 27.2, 37.9, 40.8, 42.7, 44.1, 50.4, 56.7, and 60.2° corresponding to the growth directions (110), (310), (400), (211), (111), (301), (131), (411), (600), and (521), respectively, as per the JCPDS data (024-0735) [27,28]. Additionally, the MnS material within the composite shows characteristic peaks at 2θ values of 30.8, 33.9, 47.6, 48.8, and 53.2°, corresponding to the growth directions (111), (200), (110), (220), and (112), correspondingly [29,30].

The pristine P2MA exhibits four weak peaks, which denote its semi-crystalline nature. However, after the composite formation, six peaks emerge, reflecting a significant enhancement in its crystalline structure. This improvement in crystallinity is indicative of the enhanced charge storage potential of the composite material.

For the composite, The crystalline size is determined to be 42 nm, calculated by the Scherrer equation (Eq. (4)) [31], based on the high-intensity peak at 27.2°. This small crystalline size is beneficial for charge storage applications as it provides a larger area for electrochemical reactions, thereby enhancing the performance of the supercapacitor.

(4) D = 0.9 λ / β cos θ .

The topographical and morphological behaviors of MnO2-MnS/P2MA PN nanocomposite were investigated using SEM, as estimated in Figure 3(a) and (b) at various magnifications. These images reveal the formation of a porous network, which is highly promising due to its substantial surface area and porosity, making it an excellent candidate for charge storage applications. The network is composed of small fibrous particles interconnected to form this porous structure.

Figure 3 
                  (a and b) SEM of the synthesized MnO2-MnS/P2MA PN nanocomposite at various magnifications and (d) cross section for this composite. (c) SEM of P2MA.
Figure 3

(a and b) SEM of the synthesized MnO2-MnS/P2MA PN nanocomposite at various magnifications and (d) cross section for this composite. (c) SEM of P2MA.

Figure 3(d) provides a detailed view of this structure, showing how the network extends and connects to form a cohesive structure. The varying colors in the image, ranging from dark to faint, represent the inorganic and organic components within this composite, highlighting the integration of MnO2 and MnS within the polymer matrix.

In contrast, the pristine P2MA exhibits a different morphology characterized by spherical particles. These larger particles are made up of smaller granules that aggregate to form the larger spheres. The presence of a porous structure within these spherical particles facilitates the incorporation of other materials during composite formation processes, enhancing their functionality in various applications.

So, the SEM analysis confirms that the MnO2-MnS/P2MA PN nanocomposite possesses a highly porous and interconnected structure, which is advantageous for enhancing charge storage capacity. This morphology, combined with the compositional elements of MnO2 and MnS, contributes to the improved electrochemical composite behavior.

3.2 The electrochemical testing of the synthesized MnO2-MnS/P2MA PN nanocomposite pseudo-supercapacitor

The synthesized MnO2-MnS/P2MA PN nanocomposite pseudo-supercapacitor exhibits electrochemical charge storage properties primarily through redox reactions. The charge storage process involves the reduction reaction, where the composite materials store and accumulate charges, followed by the oxidation reaction, which facilitates the de-insertion of these charges. This behavior is attributable to the redox capabilities of the materials within the composite, including MnO2, MnS, and P2MA. Specifically, manganese (Mn) undergoes reduction to Mn2+ and subsequent oxidation to Mn4+, while P2MA transitions from a benzene-like structure to a quinoid structure through similar redox processes.

Figure 4 provides a clear illustration of this phenomenon. In Figure 4(a), the electrochemical reactions of charge and discharge are depicted, showing a significant dependence on the current densities applied. As the current decreases, the discharge time notably increases, with optimal values recorded at 0.6 and 1.0 A/g, corresponding to discharge times of 80 and 34 s, respectively.

Figure 4 
                  (a) Electrochemical discharge characteristics and (b) cyclic voltammetry for MnO2-MnS/P2MA PN nanocomposite pseudo-supercapacitor.
Figure 4

(a) Electrochemical discharge characteristics and (b) cyclic voltammetry for MnO2-MnS/P2MA PN nanocomposite pseudo-supercapacitor.

Additionally, Figure 4(b) presents cyclic voltammetry data, highlighting pronounced peaks in both positive and negative directions, with substantial areas under the curve. This area indicates robust charge storage capabilities, which are enhanced as the scan rate changes from 50 to 300 mV/s. The sharper peaks and larger areas under the curve correspond to increased current densities, estimating the composite’s excellent charge storage performance.

The enhanced charge storage is largely due to the inclusion and de-insertion of H+ ions from the acidic medium, which induce significant polarization in the P2MA acid. This polarization improves the conductivity and subsequently the charge storage within the porous structure of the MnO2-MnS/P2MA PN nanocomposite. The promising nature of this composite is evident in its ability to efficiently store charge, making it a potential candidate for advanced supercapacitor applications.

The charge storage capability of the fabricated MnO2-MnS/P2MA PN nanocomposite pseudo-supercapacitor is assessed through redox reactions involving charge insertion and subsequent charge de-insertion, as shown in Figure 5(a) based on C S estimation. The maximum C S values of 120 and 86 F/g are achieved at 0.6 and 1.0 A/g, respectively, illustrating the effect of current on the supercapacitor’s charge storage behavior. Lower current values facilitate a more orderly insertion of charge during the redox reactions, resulting in a longer discharge time. This behavior is described by Eq. (1), which relates the mass loaded (Δm), discharge time (Δt), and discharge voltage (ΔV). By combining these factors, the C S value is effectively determined, with the highest value corresponding to the discharge time of a longer value at a lower current density.

Figure 5 
                  The evaluated charge storage behavior through the evaluated parameters: (a) C
                     S, (b) E, (c) P, and (d) Ragone plot for MnO2-MnS/P2MA PN nanocomposite pseudo-supercapacitor.
Figure 5

The evaluated charge storage behavior through the evaluated parameters: (a) C S, (b) E, (c) P, and (d) Ragone plot for MnO2-MnS/P2MA PN nanocomposite pseudo-supercapacitor.

The estimation of the energy (E) value is demonstrated in Figure 5(b) based on Eq. (2), considering the squared values of the voltages relative to the C S values. The optimal E values are found at lower current densities, with values of 9.7 and 7.0 W h/kg at 0.6 and 1.0 A/g, respectively. These high energy values highlight the ability of the fabricated supercapacitor to store substantial energy in a compact and lightweight MnO2-MnS/P2MA PN nanocomposite.

Figure 5(c) illustrates the estimation of the output power (P) using Eq. (3), in relation to the discharge time (Δt). The optimal P values increase with the applied current, reaching approximately 960 mW/kg. This indicates the supercapacitor’s capability to deliver significant power to an external source, relative to the mass of the MnO2-MnS/P2MA PN nanocomposite. The Ragone plot [32] in Figure 5(d) is used to estimate both P and E values, showing the relationship between stored energy and produced power. According to the plot, the stored energy decreases sequentially with increasing power output. This relationship allows for an effective evaluation of the stored and discharged energies of the supercapacitor. Then, the MnO2-MnS/P2MA PN nanocomposite pseudo-supercapacitor demonstrates excellent charge storage through redox reactions, influenced by current density. With a great behavior relative to the other previous studies as shown in Table 2.

Table 2

The charge storage performance of the MnO2-MnS/P2MA PN nanocomposite relative to other literature

Supercapacitor electrode C S (F/g) Current density (A/g) Electrolyte
MnO2-Mn2O3/poly-2-methyl aniline [4] 72 0.2 1.0 M Na2SO4
Polypyrrole-Ni(OH)2 [33] 70 0.005 poly(vinyl alcohol)/H3PO4
MnO2-MnS/G-C3N4 [34] 44 0.2 1.0 M Na2SO4
Polyaniline/silver oxide/silver [35] 4.0 0.2 1 M NaOH
Gd/graphitic material [36] 16 Poly(vinyl alcohol)/H3PO4
β-Ni(OH)2/G-C3N4 [13] 20.5 1 1 M NaOH
CoO-CuO/G-C3N4 [37] 65 0.5 6 M KOH
Zn(OH)2 [38] 100 0.2 2 M KOH
MnO2-MnS/P2MA (this work) 120 0.6 1.0 M Na2SO4

The evaluation of charge storage in the fabricated MnO2-MnS/P2MA PN nanocomposite pseudo-supercapacitor can be assessed through the charge transfer between the composite paste and the electrode. The effectiveness of this charge transfer, which determines the supercapacitor’s charge storage capacity, is illustrated in the Nyquist plot shown in Figure 6(a). The solution resistance (R S), measured at 7.3 Ω, reflects the resistance encountered by the charge passing through the solution and the composite paste. Additionally, the charge transfer resistance (R CT) associated with the semicircle in the Nyquist plot is measured at 20.3 Ω. These values indicate excellent charge transfer capabilities for the supercapacitor, facilitated by the materials’ inherent properties. The impedance values, derived using the Randle circuit depicted in the figure, underscore the efficiency of the MnO2, MnS, and P2MA components, which possess significant semiconductive properties. These materials enable efficient charge transfer due to their superior semiconductivity. Figure 6(b) illustrates the cycling stability of the supercapacitor, showing an impressive retention of 99.2% after 1,000 cycles, which gradually declines to 97% after 3,000 cycles. This high stability indicates the MnO2-MnS/P2MA PN nanocomposite pseudo-supercapacitor’s potential for commercial applications, combining efficiency with cost-effectiveness and scalability for mass production.

Figure 6 
                  (a) The evaluation of the charge transfer inside the MnO2-MnS/P2MA PN nanocomposite and (b) the cycle retention.
Figure 6

(a) The evaluation of the charge transfer inside the MnO2-MnS/P2MA PN nanocomposite and (b) the cycle retention.

4 Conclusions

The MnO2-MnS/P2MA PN composite is fabricated using a single-step process. SEM analysis reveals a nanoscale network formation that merges to create an extensive surface area, while XRD analysis shows distinct crystalline peaks, indicating excellent semiconductive properties with a crystalline size of 42 nm. This nanocomposite is used as a working electrode in a three-electrode cell setup to evaluate its charge storage capabilities electrochemically. At lower current densities, the optimal E-values are achieved, with 9.7 W h/kg at 0.6 A/g and 7.0 W h/kg at 1.0 A/g. The C S also reaches its peak within this current density range, with values of 120 and 86 F/g, correspondingly. The EIS shows notable performance with an R s value of 7.3 Ω and an impressive cycle retention rate of 99.2% over 1,000 cycles.

The combination of a simple one-pot fabrication process, excellent charge storage performance, and high stability highlight the nanocomposite for charge storage applications. The MnO2-MnS/P2MA nanocomposite demonstrates superior EIS behavior, optimal energy and capacitance values, and remarkable cycle stability, reflecting its efficiency and reliability for charge storage solutions.

Acknowledgments

Ongoing Research Funding program, (ORF-2025-845), King Saud University, Riyadh, Saudi Arabia.

  1. Funding information: Ongoing Research Funding program, (ORF-2025-845), King Saud University, Riyadh, Saudi Arabia.

  2. Author contributions: Mohamed Rabia: experimental, analysis, and writing. Eman Aldosari: writing, supervision, and project funding. Qinfang Zhang: revision and supervision. Hissah Hamad Altilasi: writing and supervision. All authors have accepted responsibility for the entire content of this manuscript and approved its submission.

  3. Conflict of interest: The authors state no conflict of interest.

  4. Data availability statement: All data generated or analyzed during this study are included in this published article.

References

[1] Pujari RB, Lokhande VC, Kumbhar VS, Chodankar NR, Lokhande CD. Hexagonal microrods architectured MoO3 thin film for supercapacitor application. J Mater Sci: Mater Electron. 2016;27:3312–7.10.1007/s10854-015-4160-3Search in Google Scholar

[2] Rabia M, Abdallah Alnuwaiser M, Hasan F, Adel A. Abdelazeez A. Highly wrinkled porous polypyrrole for the enhancement of the performance of an Fe2S3-Fe2O3/poly-O-amino benzenethiol supercapacitor from a basic medium. Inorganics. 2023;11:402.10.3390/inorganics11100402Search in Google Scholar

[3] Elsayed AM, Abdallah Alnuwaiser M, Rabia M. Effect of brain-like shape polypyrrole nanomaterial on the capacitance and stability enhancements of β-Ni(OH)2 two-symmetric electrodes supercapacitor. J Mater Sci: Mater Electron. 2023;34:1–10.10.1007/s10854-023-11014-4Search in Google Scholar

[4] Alkallas FH, Elsayed AM, Trabelsi ABG, Rabia M. Basic and acidic electrolyte mediums impact on MnO2-Mn2O3/poly-2-methylaniline hexagonal nanocomposite pseudo-supercapacitor. Phys Scr. 2024;99:065972.10.1088/1402-4896/ad3f85Search in Google Scholar

[5] Karimzadeh Z, Shokri B, Morsali A. Rapid cold plasma synthesis of cobalt metal–organic framework/reduced graphene oxide nanocomposites for use as supercapacitor electrodes. Sci Rep. 2023;13(1):1–11.10.1038/s41598-023-41816-9Search in Google Scholar PubMed PubMed Central

[6] Alshammari DA, Ahmed IA, Alahmari SD, Abdullah M, Aman S, Ahmad N, et al. Electrochemical investigation of niobium doped nickel selenide nanostructure for supercapacitor devices. J Energy Storage. 2024;75:109886.10.1016/j.est.2023.109886Search in Google Scholar

[7] Adriyani TR, Ensafi AA, Rezaei B. Flexible and sewable electrode based on Ni-Co@PANI-salphen composite-coated on textiles for wearable supercapacitor. Sci Rep. 2023;13(1):1–13.10.1038/s41598-023-47067-ySearch in Google Scholar PubMed PubMed Central

[8] Ramadoss J, Sonachalam A, Govindasamy M. Surface modification effect on V-doped Ti3C2Tx as bifunctional catalyst electrodes for symmetric supercapacitor and the hydrogen evolution reaction. Energy Fuels. 2023;37:17561–74.10.1021/acs.energyfuels.3c03411Search in Google Scholar

[9] Alshammari DA, Aman S, Ahmad N, Riyad YM, Tahir Farid HM. Development of N doped C/MnAl2O4 spinel as environmental friendly energy storage devices. Ceram Int. 2024;50:5424–33.10.1016/j.ceramint.2023.11.292Search in Google Scholar

[10] AlAnazi M, Ghrib T, Ercan F, Alsubaie M, Demirci T, Kaygili O, et al. Structural, optical, and electrical investigation of multilayered MnO2(n)/NiO(p) heterojunctions for supercapacitors applications. Surf Interfaces. 2023;42:103321.10.1016/j.surfin.2023.103321Search in Google Scholar

[11] Kulandaivalu S, Suhaimi N, Sulaiman Y. Unveiling high specific energy supercapacitor from layer-by-layer assembled polypyrrole/graphene oxide|polypyrrole/manganese oxide electrode material. Sci Rep. 2019;9(1):1–10.10.1038/s41598-019-41203-3Search in Google Scholar PubMed PubMed Central

[12] Lu T, Zhang Y, Li H, Pan L, Li Y, Sun Z. Electrochemical behaviors of graphene–ZnO and graphene–SnO2 composite films for supercapacitors. Electrochim Acta. 2010;55:4170–3.10.1016/j.electacta.2010.02.095Search in Google Scholar

[13] Roshni CP, Jithesh K, Manuraj M, Govind Raj K, Rakhi RB. β-Ni(OH)2 supported over g-C3N4: A novel catalyst for para-nitrophenol reduction and supercapacitor electrode. Results Chem. 2022;4:100498.10.1016/j.rechem.2022.100498Search in Google Scholar

[14] Avinash B, Ravikumar CR, Kumar MRA, Santosh MS, Pratapkumar C, Nagaswarupa HP, et al. NiO bio-composite materials: Photocatalytic, electrochemical and supercapacitor applications. Appl Surf Sci Adv. 2021;3:100049.10.1016/j.apsadv.2020.100049Search in Google Scholar

[15] Kumar MRA, Abebe B, Nagaswarupa HP, Murthy HCA, Ravikumar CR, Sabir FK. Enhanced photocatalytic and electrochemical performance of TiO2-Fe2O3 nanocomposite: Its applications in dye decolorization and as supercapacitors. Sci Rep. 2020;10(1):1–15.10.1038/s41598-020-58110-7Search in Google Scholar PubMed PubMed Central

[16] Afza N, Shivakumar MS, Alam MW, Kumar AN, Bhatt AS, Murthy HCA, et al. Facile hydrothermal synthesis of cerium oxide/rGO nanocomposite for photocatalytic and supercapacitor applications. Appl Surf Sci Adv. 2022;11:100307.10.1016/j.apsadv.2022.100307Search in Google Scholar

[17] Kedir CN, Salinas-Torres D, Quintero-Jaime AF, Benyoucef A, Morallon E. Hydrogels obtained from aniline and piperazine: Synthesis, characterization and their application in hybrid supercapacitors. J Mol Struct. 2022;1248:131445.10.1016/j.molstruc.2021.131445Search in Google Scholar

[18] Zang L, Liu Q, Qiu J, Yang C, Wei C, Liu C, et al. Design and fabrication of an all-solid-state polymer supercapacitor with highly mechanical flexibility based on polypyrrole hydrogel. ACS Appl Mater Interfaces. 2017;9:33941–7.10.1021/acsami.7b10321Search in Google Scholar PubMed

[19] Li J, Yan W, Zhang G, Sun R, Ho D. Natively stretchable micro-supercapacitors based on a PEDOT:PSS hydrogel. J Mater Chem C. 2021;9:1685–92.10.1039/D0TC05270ASearch in Google Scholar

[20] Zaki SE, Basyooni MA, Shaban M, Rabia M, Eker YR, Attia GF, et al. Role of oxygen vacancies in vanadium oxide and oxygen functional groups in graphene oxide for room temperature CO2 gas sensors. Sens Actuators, A: Phys. 2019;294:17–24.10.1016/j.sna.2019.04.037Search in Google Scholar

[21] Azzam EMS, Abd El-Salam HM, Aboad RS. Kinetic preparation and antibacterial activity of nanocrystalline poly(2-aminothiophenol). Polym Bull. 2019;76:1929–47.10.1007/s00289-018-2405-zSearch in Google Scholar

[22] Alkallas FH, Elsayed AM, Trabelsi ABG, Rabia M. Porous-spherical MnO2-Mn(OH)2/polypyrrole nanocomposite thin film photodetector in a wide optical range from UV to IR. Opt Quantum Electron. 2023;55:1078.10.1007/s11082-023-05260-3Search in Google Scholar

[23] Alkallas FH, Elsayed AM, Trabelsi ABG, Rabia M. Quantum dot supernova-like-shaped arsenic (III) sulfide-oxide/polypyrrole thin film for optoelectronic applications in a wide optical range from ultraviolet to infrared. Catalysts. 2023;13:1274.10.3390/catal13091274Search in Google Scholar

[24] Elsayed AM, Alkallas FH, Trabelsi ABG, Rabia M. Highly uniform spherical MoO2-MoO3/polypyrrole core-shell nanocomposite as an optoelectronic photodetector in UV, Vis, and IR domains. Micromachines. 2023;14:1694.10.3390/mi14091694Search in Google Scholar PubMed PubMed Central

[25] Cao X, Li H, He J, Kang L, Jiang R, Shi F, et al. Preparation and formation process of α-MnS@MoS2 microcubes with hierarchical core/shell structure. J Colloid Interface Sci. 2017;507:18–26.10.1016/j.jcis.2017.07.102Search in Google Scholar PubMed

[26] Chen K, Wang M, Li G, He Q, Liu J, Li F. Spherical α-MnO2 supported on N-KB as efficient electrocatalyst for oxygen reduction in Al-air battery. Materials. 2018;11:601.10.3390/ma11040601Search in Google Scholar PubMed PubMed Central

[27] Sannasi V, Subbian K. Influence of Moringa oleifera gum on two polymorphs synthesis of MnO2 and evaluation of the pseudo-capacitance activity. J Mater Sci: Mater Electron. 2020;31:17120–32.10.1007/s10854-020-04272-zSearch in Google Scholar

[28] Shah HU, Wang F, Javed MS, Ahmad MA, Saleem M, Zhan J, et al. In-situ growth of MnO2 nanorods forest on carbon textile as efficient electrode material for supercapacitors. J Energy Storage. 2018;17:318–26.10.1016/j.est.2018.03.015Search in Google Scholar

[29] Xu D, Jiao R, Sun Y, Sun D, Zhang X, Zeng S, et al. L-cysteine-assisted synthesis of urchin-like γ-MnS and its lithium storage properties. Nanoscale Res Lett. 2016;11:444.10.1186/s11671-016-1664-6Search in Google Scholar PubMed PubMed Central

[30] Mi L, Chen Y, Zheng Z, Hou H, Chen W, Cui S. Beneficial metal ion insertion into dandelion-like MnS with enhanced catalytic performance and genetic morphology. RSC Adv. 2014;4:19257–65.10.1039/C4RA00961DSearch in Google Scholar

[31] Ahmed AM, Rabia M, Shaban M. The structure and photoelectrochemical activity of Cr-doped PbS thin films grown by chemical bath deposition. RSC Adv. 2020;10:14458–70.10.1039/C9RA11042ASearch in Google Scholar

[32] Huo P, Ni S, Hou P, Xun Z, Liu Y, Gu J. A crosslinked soybean protein isolate gel polymer electrolyte based on neutral aqueous electrolyte for a high-energy-density supercapacitor. Polymers. 2019;11(5):863.10.3390/polym11050863Search in Google Scholar PubMed PubMed Central

[33] Scarabelot LT, Muller D, de Souza LV, Hotza D, Rambo CR. Ni(OH)2 aerogels incorporated with polypyrrole as electrodes for supercapacitors. J Electron Mater. 2017;46:5232–9.10.1007/s11664-017-5526-5Search in Google Scholar

[34] Ben Gouider Trabelsi A, Elsayed AM, Alkallas FH, Rabia M. Highly uniform nanocomposite through the decoration of MnS on graphitic carbon nitride as electrodes for symmetric supercapacitor. Phys Scr. 2023;98:116005.10.1088/1402-4896/acff91Search in Google Scholar

[35] Atta A, Abdelhamied MM, Essam D, Shaban M, Alshammari AH, Rabia M. Structural and physical properties of polyaniline/silver oxide/silver nanocomposite electrode for supercapacitor applications. Int J Energy Res. 2022;46:6702–10.10.1002/er.7608Search in Google Scholar

[36] Kumar Kuila S, Ghorai A, Midya A, Sekhar Tiwary C, Kumar Kundu T. Chemisorption of gadolinium ions on 2D-graphitic carbon nitride nanosheet for enhanced solid-state supercapacitor performance. Chem Phys Lett. 2022;796:139572.10.1016/j.cplett.2022.139572Search in Google Scholar

[37] Santos RS, Suresh Babu R, Devendiran M, Haddad DB, de Barros ALF. Facile synthesis of transition metal (M = Cu, Co) oxide grafted graphitic carbon nitride nanosheets for high performance asymmetric supercapacitors. Mater Lett. 2022;308:131156.10.1016/j.matlet.2021.131156Search in Google Scholar

[38] Sasirekha C, Arumugam S. Electrochemical performance of zinchydroxide Zn(OH)2 nanosheet for supercapacitor application. AIP Conf Proc. 2017;1832:050047.10.1063/1.4980280Search in Google Scholar

Received: 2024-10-15
Revised: 2025-01-21
Accepted: 2025-02-24
Published Online: 2025-06-17

© 2025 the author(s), published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

Articles in the same Issue

  1. Research Articles
  2. Single-step fabrication of Ag2S/poly-2-mercaptoaniline nanoribbon photocathodes for green hydrogen generation from artificial and natural red-sea water
  3. Abundant new interaction solutions and nonlinear dynamics for the (3+1)-dimensional Hirota–Satsuma–Ito-like equation
  4. A novel gold and SiO2 material based planar 5-element high HPBW end-fire antenna array for 300 GHz applications
  5. Explicit exact solutions and bifurcation analysis for the mZK equation with truncated M-fractional derivatives utilizing two reliable methods
  6. Optical and laser damage resistance: Role of periodic cylindrical surfaces
  7. Numerical study of flow and heat transfer in the air-side metal foam partially filled channels of panel-type radiator under forced convection
  8. Water-based hybrid nanofluid flow containing CNT nanoparticles over an extending surface with velocity slips, thermal convective, and zero-mass flux conditions
  9. Dynamical wave structures for some diffusion--reaction equations with quadratic and quartic nonlinearities
  10. Solving an isotropic grey matter tumour model via a heat transfer equation
  11. Study on the penetration protection of a fiber-reinforced composite structure with CNTs/GFP clip STF/3DKevlar
  12. Influence of Hall current and acoustic pressure on nanostructured DPL thermoelastic plates under ramp heating in a double-temperature model
  13. Applications of the Belousov–Zhabotinsky reaction–diffusion system: Analytical and numerical approaches
  14. AC electroosmotic flow of Maxwell fluid in a pH-regulated parallel-plate silica nanochannel
  15. Interpreting optical effects with relativistic transformations adopting one-way synchronization to conserve simultaneity and space–time continuity
  16. Modeling and analysis of quantum communication channel in airborne platforms with boundary layer effects
  17. Theoretical and numerical investigation of a memristor system with a piecewise memductance under fractal–fractional derivatives
  18. Tuning the structure and electro-optical properties of α-Cr2O3 films by heat treatment/La doping for optoelectronic applications
  19. High-speed multi-spectral explosion temperature measurement using golden-section accelerated Pearson correlation algorithm
  20. Dynamic behavior and modulation instability of the generalized coupled fractional nonlinear Helmholtz equation with cubic–quintic term
  21. Study on the duration of laser-induced air plasma flash near thin film surface
  22. Exploring the dynamics of fractional-order nonlinear dispersive wave system through homotopy technique
  23. The mechanism of carbon monoxide fluorescence inside a femtosecond laser-induced plasma
  24. Numerical solution of a nonconstant coefficient advection diffusion equation in an irregular domain and analyses of numerical dispersion and dissipation
  25. Numerical examination of the chemically reactive MHD flow of hybrid nanofluids over a two-dimensional stretching surface with the Cattaneo–Christov model and slip conditions
  26. Impacts of sinusoidal heat flux and embraced heated rectangular cavity on natural convection within a square enclosure partially filled with porous medium and Casson-hybrid nanofluid
  27. Stability analysis of unsteady ternary nanofluid flow past a stretching/shrinking wedge
  28. Solitonic wave solutions of a Hamiltonian nonlinear atom chain model through the Hirota bilinear transformation method
  29. Bilinear form and soltion solutions for (3+1)-dimensional negative-order KdV-CBS equation
  30. Solitary chirp pulses and soliton control for variable coefficients cubic–quintic nonlinear Schrödinger equation in nonuniform management system
  31. Influence of decaying heat source and temperature-dependent thermal conductivity on photo-hydro-elasto semiconductor media
  32. Dissipative disorder optimization in the radiative thin film flow of partially ionized non-Newtonian hybrid nanofluid with second-order slip condition
  33. Bifurcation, chaotic behavior, and traveling wave solutions for the fractional (4+1)-dimensional Davey–Stewartson–Kadomtsev–Petviashvili model
  34. New investigation on soliton solutions of two nonlinear PDEs in mathematical physics with a dynamical property: Bifurcation analysis
  35. Mathematical analysis of nanoparticle type and volume fraction on heat transfer efficiency of nanofluids
  36. Creation of single-wing Lorenz-like attractors via a ten-ninths-degree term
  37. Optical soliton solutions, bifurcation analysis, chaotic behaviors of nonlinear Schrödinger equation and modulation instability in optical fiber
  38. Chaotic dynamics and some solutions for the (n + 1)-dimensional modified Zakharov–Kuznetsov equation in plasma physics
  39. Fractal formation and chaotic soliton phenomena in nonlinear conformable Heisenberg ferromagnetic spin chain equation
  40. Single-step fabrication of Mn(iv) oxide-Mn(ii) sulfide/poly-2-mercaptoaniline porous network nanocomposite for pseudo-supercapacitors and charge storage
  41. Novel constructed dynamical analytical solutions and conserved quantities of the new (2+1)-dimensional KdV model describing acoustic wave propagation
  42. Tavis–Cummings model in the presence of a deformed field and time-dependent coupling
  43. Spinning dynamics of stress-dependent viscosity of generalized Cross-nonlinear materials affected by gravitationally swirling disk
  44. Design and prediction of high optical density photovoltaic polymers using machine learning-DFT studies
  45. Robust control and preservation of quantum steering, nonlocality, and coherence in open atomic systems
  46. Coating thickness and process efficiency of reverse roll coating using a magnetized hybrid nanomaterial flow
  47. Dynamic analysis, circuit realization, and its synchronization of a new chaotic hyperjerk system
  48. Decoherence of steerability and coherence dynamics induced by nonlinear qubit–cavity interactions
  49. Finite element analysis of turbulent thermal enhancement in grooved channels with flat- and plus-shaped fins
  50. Modulational instability and associated ion-acoustic modulated envelope solitons in a quantum plasma having ion beams
  51. Statistical inference of constant-stress partially accelerated life tests under type II generalized hybrid censored data from Burr III distribution
  52. On solutions of the Dirac equation for 1D hydrogenic atoms or ions
  53. Entropy optimization for chemically reactive magnetized unsteady thin film hybrid nanofluid flow on inclined surface subject to nonlinear mixed convection and variable temperature
  54. Stability analysis, circuit simulation, and color image encryption of a novel four-dimensional hyperchaotic model with hidden and self-excited attractors
  55. A high-accuracy exponential time integration scheme for the Darcy–Forchheimer Williamson fluid flow with temperature-dependent conductivity
  56. Novel analysis of fractional regularized long-wave equation in plasma dynamics
  57. Development of a photoelectrode based on a bismuth(iii) oxyiodide/intercalated iodide-poly(1H-pyrrole) rough spherical nanocomposite for green hydrogen generation
  58. Investigation of solar radiation effects on the energy performance of the (Al2O3–CuO–Cu)/H2O ternary nanofluidic system through a convectively heated cylinder
  59. Quantum resources for a system of two atoms interacting with a deformed field in the presence of intensity-dependent coupling
  60. Studying bifurcations and chaotic dynamics in the generalized hyperelastic-rod wave equation through Hamiltonian mechanics
  61. A new numerical technique for the solution of time-fractional nonlinear Klein–Gordon equation involving Atangana–Baleanu derivative using cubic B-spline functions
  62. Interaction solutions of high-order breathers and lumps for a (3+1)-dimensional conformable fractional potential-YTSF-like model
  63. Hydraulic fracturing radioactive source tracing technology based on hydraulic fracturing tracing mechanics model
  64. Numerical solution and stability analysis of non-Newtonian hybrid nanofluid flow subject to exponential heat source/sink over a Riga sheet
  65. Numerical investigation of mixed convection and viscous dissipation in couple stress nanofluid flow: A merged Adomian decomposition method and Mohand transform
  66. Effectual quintic B-spline functions for solving the time fractional coupled Boussinesq–Burgers equation arising in shallow water waves
  67. Analysis of MHD hybrid nanofluid flow over cone and wedge with exponential and thermal heat source and activation energy
  68. Solitons and travelling waves structure for M-fractional Kairat-II equation using three explicit methods
  69. Impact of nanoparticle shapes on the heat transfer properties of Cu and CuO nanofluids flowing over a stretching surface with slip effects: A computational study
  70. Computational simulation of heat transfer and nanofluid flow for two-sided lid-driven square cavity under the influence of magnetic field
  71. Irreversibility analysis of a bioconvective two-phase nanofluid in a Maxwell (non-Newtonian) flow induced by a rotating disk with thermal radiation
  72. Hydrodynamic and sensitivity analysis of a polymeric calendering process for non-Newtonian fluids with temperature-dependent viscosity
  73. Exploring the peakon solitons molecules and solitary wave structure to the nonlinear damped Kortewege–de Vries equation through efficient technique
  74. Modeling and heat transfer analysis of magnetized hybrid micropolar blood-based nanofluid flow in Darcy–Forchheimer porous stenosis narrow arteries
  75. Activation energy and cross-diffusion effects on 3D rotating nanofluid flow in a Darcy–Forchheimer porous medium with radiation and convective heating
  76. Insights into chemical reactions occurring in generalized nanomaterials due to spinning surface with melting constraints
  77. Influence of a magnetic field on double-porosity photo-thermoelastic materials under Lord–Shulman theory
  78. Soliton-like solutions for a nonlinear doubly dispersive equation in an elastic Murnaghan's rod via Hirota's bilinear method
  79. Analytical and numerical investigation of exact wave patterns and chaotic dynamics in the extended improved Boussinesq equation
  80. Nonclassical correlation dynamics of Heisenberg XYZ states with (x, y)-spin--orbit interaction, x-magnetic field, and intrinsic decoherence effects
  81. Exact traveling wave and soliton solutions for chemotaxis model and (3+1)-dimensional Boiti–Leon–Manna–Pempinelli equation
  82. Unveiling the transformative role of samarium in ZnO: Exploring structural and optical modifications for advanced functional applications
  83. On the derivation of solitary wave solutions for the time-fractional Rosenau equation through two analytical techniques
  84. Analyzing the role of length and radius of MWCNTs in a nanofluid flow influenced by variable thermal conductivity and viscosity considering Marangoni convection
  85. Advanced mathematical analysis of heat and mass transfer in oscillatory micropolar bio-nanofluid flows via peristaltic waves and electroosmotic effects
  86. Exact bound state solutions of the radial Schrödinger equation for the Coulomb potential by conformable Nikiforov–Uvarov approach
  87. Some anisotropic and perfect fluid plane symmetric solutions of Einstein's field equations using killing symmetries
  88. Nonlinear dynamics of the dissipative ion-acoustic solitary waves in anisotropic rotating magnetoplasmas
  89. Curves in multiplicative equiaffine plane
  90. Exact solution of the three-dimensional (3D) Z2 lattice gauge theory
  91. Propagation properties of Airyprime pulses in relaxing nonlinear media
  92. Symbolic computation: Analytical solutions and dynamics of a shallow water wave equation in coastal engineering
  93. Wave propagation in nonlocal piezo-photo-hygrothermoelastic semiconductors subjected to heat and moisture flux
  94. Comparative reaction dynamics in rotating nanofluid systems: Quartic and cubic kinetics under MHD influence
  95. Laplace transform technique and probabilistic analysis-based hypothesis testing in medical and engineering applications
  96. Physical properties of ternary chloro-perovskites KTCl3 (T = Ge, Al) for optoelectronic applications
  97. Gravitational length stretching: Curvature-induced modulation of quantum probability densities
  98. The search for the cosmological cold dark matter axion – A new refined narrow mass window and detection scheme
  99. A comparative study of quantum resources in bipartite Lipkin–Meshkov–Glick model under DM interaction and Zeeman splitting
  100. PbO-doped K2O–BaO–Al2O3–B2O3–TeO2-glasses: Mechanical and shielding efficacy
  101. Nanospherical arsenic(iii) oxoiodide/iodide-intercalated poly(N-methylpyrrole) composite synthesis for broad-spectrum optical detection
  102. Sine power Burr X distribution with estimation and applications in physics and other fields
  103. Numerical modeling of enhanced reactive oxygen plasma in pulsed laser deposition of metal oxide thin films
  104. Dynamical analyses and dispersive soliton solutions to the nonlinear fractional model in stratified fluids
  105. Computation of exact analytical soliton solutions and their dynamics in advanced optical system
  106. An innovative approximation concerning the diffusion and electrical conductivity tensor at critical altitudes within the F-region of ionospheric plasma at low latitudes
  107. An analytical investigation to the (3+1)-dimensional Yu–Toda–Sassa–Fukuyama equation with dynamical analysis: Bifurcation
  108. Swirling-annular-flow-induced instability of a micro shell considering Knudsen number and viscosity effects
  109. Numerical analysis of non-similar convection flows of a two-phase nanofluid past a semi-infinite vertical plate with thermal radiation
  110. MgO NPs reinforced PCL/PVC nanocomposite films with enhanced UV shielding and thermal stability for packaging applications
  111. Optimal conditions for indoor air purification using non-thermal Corona discharge electrostatic precipitator
  112. Investigation of thermal conductivity and Raman spectra for HfAlB, TaAlB, and WAlB based on first-principles calculations
  113. Tunable double plasmon-induced transparency based on monolayer patterned graphene metamaterial
  114. DSC: depth data quality optimization framework for RGBD camouflaged object detection
  115. A new family of Poisson-exponential distributions with applications to cancer data and glass fiber reliability
  116. Numerical investigation of couple stress under slip conditions via modified Adomian decomposition method
  117. Monitoring plateau lake area changes in Yunnan province, southwestern China using medium-resolution remote sensing imagery: applicability of water indices and environmental dependencies
  118. Heterodyne interferometric fiber-optic gyroscope
  119. Exact solutions of Einstein’s field equations via homothetic symmetries of non-static plane symmetric spacetime
  120. A widespread study of discrete entropic model and its distribution along with fluctuations of energy
  121. Empirical model integration for accurate charge carrier mobility simulation in silicon MOSFETs
  122. The influence of scattering correction effect based on optical path distribution on CO2 retrieval
  123. Anisotropic dissociation and spectral response of 1-Bromo-4-chlorobenzene under static directional electric fields
  124. Role of tungsten oxide (WO3) on thermal and optical properties of smart polymer composites
  125. Analysis of iterative deblurring: no explicit noise
  126. Review Article
  127. Examination of the gamma radiation shielding properties of different clay and sand materials in the Adrar region
  128. Erratum
  129. Erratum to “On Soliton structures in optical fiber communications with Kundu–Mukherjee–Naskar model (Open Physics 2021;19:679–682)”
  130. Special Issue on Fundamental Physics from Atoms to Cosmos - Part II
  131. Possible explanation for the neutron lifetime puzzle
  132. Special Issue on Nanomaterial utilization and structural optimization - Part III
  133. Numerical investigation on fluid-thermal-electric performance of a thermoelectric-integrated helically coiled tube heat exchanger for coal mine air cooling
  134. Special Issue on Nonlinear Dynamics and Chaos in Physical Systems
  135. Analysis of the fractional relativistic isothermal gas sphere with application to neutron stars
  136. Abundant wave symmetries in the (3+1)-dimensional Chafee–Infante equation through the Hirota bilinear transformation technique
  137. Successive midpoint method for fractional differential equations with nonlocal kernels: Error analysis, stability, and applications
  138. Novel exact solitons to the fractional modified mixed-Korteweg--de Vries model with a stability analysis
Downloaded on 31.12.2025 from https://www.degruyterbrill.com/document/doi/10.1515/phys-2025-0132/html
Scroll to top button