DOI:
10.1039/D5MA01186H
(Paper)
Mater. Adv., 2026, Advance Article
An edible microbial cellulose-based triboelectric nanogenerator: a sustainable approach for energy harvesting
Received
14th October 2025
, Accepted 5th December 2025
First published on 2nd January 2026
Abstract
The demand for sustainable energy has been increasing, driving the exploration of novel materials for sustainable energy-harvesting technologies. The present study explores a triboelectric nanogenerator (TENG) based on microbial cellulose (MC), synthesized by symbiotically cultured bacteria and yeast (SCOBY), as a positive triboelectric material, and fluorinated ethylene propylene (FEP) as a negative triboelectric material. The MC film synthesized by a simple fermentation method exhibits very high porosity and a highly rough surface, making it an excellent triboelectric material. The fabricated TENG exhibits an open-circuit voltage (Voc) of ∼620 V, a short-circuit current (Isc) of ∼40 µA, and a power density of 16.5 W m−2 at a 10 MΩ load resistance, demonstrating its superior performance compared to reported bacterial-cellulose-based TENGs. Moreover, the synthesized MC film exhibits efficient antibacterial activity against Gram-negative and Gram-positive bacteria, without the need for an additional antibacterial agent. This study fills a gap in research into clean and green energy harvesting using MC, creating an opportunity for novel, environmentally-friendly TENGs. Practical applications, such as powering a calculator, validate the potential for commercial use of innovative TENG technologies.
1. Introduction
Energy is the foundation for technological advancements, modern civilization, and the socio-economic growth of the current era. The exploitation of traditional energy resources has led to environmental pollution and global climate change. This exhausts current fossil fuel resources, and there is an urgent need to explore sustainable and renewable energy sources.1 Among the various sustainable methods of energy harvesting, Triboelectric nanogenerators (TENGs) have emerged as a promising, innovative solution due to their high efficiency, versatility, and cost-effectiveness. TENGs are based on the triboelectric effect, in which certain materials become electrically charged after coming into contact with each other and then separating.2,3 This phenomenon can be used to generate electricity from mechanical movements, such as walking, running, and vibrations, as well as from environmental motions, such as wind and waves.4–6 The TENG operates in four modes: vertical contact-separation mode, lateral sliding mode, single-electrode mode, and free-standing triboelectric-layer mode,7–9 demonstrating its adaptability across various conditions and applications.
In recent years, there has been growing interest in the use of sustainable, biocompatible materials for the fabrication of TENGs to align with eco-friendly paradigms.10,11 The integration of natural polymers into TENGs not only improves environmental sustainability but also enhances functionality and biocompatibility. Biopolymers such as natural rubber, poly(lactic) acid, chitosan, and cellulose are commonly used in the fabrication of biopolymer-based TENGs due to their biodegradability and renewable sources.12–16 Several innovative techniques are also used to optimize the functional and structural designs of biopolymers in TENGs to improve efficiency and expand application scope.13–15,17 Among naturally-derived materials, cellulose is the most abundant and renewable polymer, with great potential.18 Cellulose is a complex polysaccharide with a chain-like structure19 and the chemical formula C6H10O5.20 Cellulose exhibits excellent dielectric properties and shows superior electrical response to mechanical energy.21 Furthermore, Cellulose contains multiple oxygen atoms, which endow it with electron-donating properties—making it an excellent candidate for the positive friction material in polymer-based TENGs.22,23 Various advancements, such as structural innovations and chemical functionalization, have been implemented in cellulose-based TENGs. A multi-fluid electrospinning technique has been used to fabricate a composite of cellulose nanocrystals/cyanoethyl cellulose (CEC)/polyvinylidene fluoride (PVDF), which enhances triboelectric output performance, achieving an open-circuit voltage of 10.01 V and a short-circuit current of 3.30 µA.24 Composites of polydopamine and cellulose nanofibrils (PDA/CNF) demonstrate their potential as self-powered sensors, increasing output performance by 20 times to 205 V and 20 µA.25 Cellulose paper-based TENGs use multi-layer forming technology to achieve an open-circuit voltage of 227.1 V and operate even under harsh conditions.26
Among various types of celluloses, microbial cellulose (MC) is the most beneficial due to its natural abundance, excellent flexibility, sustainability, and biodegradability. It is mostly produced by certain bacteria.27 Microbial cellulose has a three-dimensional nanofibrillar morphology,28 providing excellent mechanical strength, moderate density, and high purity.29 It has a high water-absorption capacity, a large surface area, and moldability.30 A symbiotic culture of bacteria and yeast (SCOBY) consists of various bacteria and yeast, such as Acetobacter Aceti, Gluconobacter oxydans, Zygosaccharomyces, and Saccharomyces, which help in producing cellulose biofilm.31 The biofilm formed by bacteria consists of very fine microfibrils that bind to plant cellulose. These microfibrils have good film-forming capacity and excellent flexibility. Along with these structural advantages, the MC's antibacterial properties are also important for TENG applications. When microbes grow on the surface of wearable biomedical devices that remain in contact with human skin for an extended period, they can cause both infection and performance problems. To ensure user safety and the long-term smooth operation of the system, materials with natural or artificial antibacterial properties are crucial.
Various studies have been conducted to analyze the antibacterial properties of cellulose derived from microbial cultures. Although microbial cellulose lacks inherent antimicrobial properties, it can serve as an effective carrier for antimicrobial agents due to its adaptable surface chemistry, porosity, and large surface area, which can inhibit microorganism growth.32 Malmir et al.33 combined bacterial cellulose with carbon quantum dots-Titanium dioxide nanoparticles, which acted as antimicrobial agents, making the film antibacterial. Similarly, Sim et al.34 integrated bacterial cellulose with silver nanoparticles to develop an antibacterial film. Moreover, the tight network of nanofibers and the low nutrient content of the microbial film create an unsupportive environment for microbial growth.35 The incorporation of antimicrobial properties into microbial cellulose significantly broadens its applicability in infection management and medical devices, while also promoting the development of biodegradable and environmentally friendly alternatives to synthetic antimicrobial materials.
The present work introduces a self-sustaining, edible, and antibacterial MC-based triboelectric nanogenerator (MC-TENG). A triboelectric nanogenerator based on microbial cellulose as the positive triboelectric material, paired with fluorinated ethylene propylene (FEP) as the negative triboelectric material, has been developed. The conducting copper tape has been used as an electrode for the cellulose and FEP film, and the real-life applications are explored. The flexible, inherently oxygen-rich, and non-fibrillar structure of MC can significantly enhance triboelectric output and exhibit intrinsic antibacterial properties without the need for external additives. The membrane surface morphology is examined by Scanning Electron Microscopy (SEM), while Fourier Transform Infrared Spectroscopy (FTIR) is used to analyse its molecular structure. The antibacterial properties of the synthesized cellulose have been investigated, and it has been found to be self-reliant in its antibacterial activity. Moreover, the synthesized microbial cellulose exhibited inherent antibacterial properties, unlike most bacterial cellulose, thereby eliminating the need for antimicrobial agents and making the biomaterial self-reliant in its antibacterial activity. The present study aims to bridge the gap between antimicrobial development and sustainable energy harvesting, demonstrating dual-functional MC-based TENGs. The proposed TENG fills a crucial gap in sustainable energy-harvesting technologies by leveraging the inherent properties of microbial cellulose and demonstrates its practical feasibility.
2. Experimental
2.1. Materials
Apple cider vinegar, SCOBY bacteria, Conductive Copper tape (3M), and Fluorinated ethylene propylene (FEP)(TESSERACT) were purchased from Amazon. Sugar and green tea were procured from the local market.
2.2. Synthesis of microbial cellulose
Two tea bags were added to 1 L of boiling water and brewed for 15 minutes. After that, 200 g of sugar was added and stirred until dissolved, and the water was allowed to reach room temperature. Then, 200 mL of apple cider vinegar was added and stirred. Finally, the SCOBY culture was added, the container was covered with air-permeable cotton cloth, and it was left for 15 days. After 15 days, a thick layer forms on top of the solution. This cellulose layer was washed with cold soapy water and then dried at 50 °C in an oven. The flowchart for the synthesis of microbial cellulose is depicted in Fig. 1.
 |
| | Fig. 1 Flow chart depicting the detailed synthesis of microbial cellulose. | |
2.3. Fabrication of the microbial cellulose-based TENG
A 2 × 2 cm2 piece of synthesized cellulose film was used as the positive triboelectric layer. A commercially available 2 × 2 cm2 film was used as a negative triboelectric counterpart to form the microbial cellulose triboelectric nanogenerator (MC-TENG) based on triboelectric pairs of cellulose and FEP. Conducting copper tape was used as an electrode for both materials, as shown in the supplementary Fig. S1. A 1-cm separation was maintained between the MC and FEP layers during all measurements.
2.4. Antibacterial testing of microbial film
The antibacterial activities of the microbial film were investigated against Escherichia coli (E. coli), a Gram-negative model bacterium, and Bacillus subtilis, a Gram-positive model bacterium. For growth media, 2 g of Luria-Bertani (LB) and 2 g of agar were mixed in 100 mL of water and autoclaved at 121 °C for 15 minutes. After autoclaving, the growth media were poured into petri dishes and left to solidify for 15 minutes. Next, 100 µL of the bacterial culture was spread onto each agar plate. The UV-sterilized film was then placed on the agar plates. Finally, the plates were incubated at 37 °C for 24 hours, and the antibacterial activity of the film was determined by measuring the zone of inhibition.
2.5. Characterization
X-ray diffraction (XRD) data for the samples were collected on a SmartLab SE (Rigaku) instrument over a 20–90° scan range. A Field-effect scanning electron microscope (FE-SEM; Carl Zeiss Sigma 500) was used to study the morphology of the synthesized fibers. To understand the functional groups and chemical structure, Fourier-transform infrared (FTIR) spectroscopy (PerkinElmer Spectrum IT-FTIR; 500–4000 cm−1) was used. Two different materials with an active area of 2 × 2 cm2 were fixed at the two terminals of a standard linear motor-based testing system for the contact-separation process. The open-circuit voltage was measured by a digital oscilloscope (SIGLENT SDS1104X-E, impedance = 1 MΩ), and the short-circuit current of TENG was measured by an electrometer (Keithley 6517B). All the electric measurements were recorded at room temperature.
3. Results and discussion
3.1. XRD and dielectric analysis of MC film
In cellulose, the amorphousity arises from disordered chain segments, while the intra- and intermolecular hydrogen interactions of the cellulose chains contribute to a partly crystalline structure. The ratio between these amorphous and crystalline regions significantly affects the mechanical and functional properties of cellulose. Fig. 2(a) depicts the XRD analysis of the MC film recorded between 10 and 90° (2θ range). The crystallinity index (CrI) and the degree of crystallinity of the fabricated film were calculated using the Segal method36 by using eqn (1) and (2). In the case of MC, two peaks are observed at 17° and 23°, corresponding to the (101) and (002) planes of cellulose, respectively.| |
 | (1) |
| |
 | (2) |
where I002 is the maximum intensity of the diffraction peak, and Iam is the peak intensity around 20°, representing the amorphous part of cellulose. The CrI is found to be 40% and the degree of crystallinity is 2.5.36
 |
| | Fig. 2 (a) X-ray diffraction analysis, (b) dielectric constant and loss tangent, (c) AC conductivity versus frequency plots of MC film, (d) schematic diagram of dielectric-to-dielectric based TENG in contact separation mode with an equivalent circuit model of TENG. | |
The performance of the TENG has a direct relationship to the dielectric property of the triboelectric materials. The enhancement in the dielectric constant can substantially increase charge-trapping capability, reduce charge dissipation rate at the surface, and increase the surface charge density of the dielectric specimen—leading to enhanced output performance of the TENGs.37
Fig. 2(b) and (c) represent the frequency-dependent dielectric and conductivity response of the MC film measured from 100 Hz to 1 MHz at room temperature. The dielectric constant is obtained using the relation as:
| |
 | (3) |
where
C is capacitance of the sample,
d is thickness,
A is area, and
εo is permittivity of free space (8.85 × 10
−12 F m
−1). The conductivity of the materials has been obtained by using the relation:
38| |
σac = 2πfε0εr tan δ
| (4) |
where
f,
εr and tan
δ represents the angular frequency, dielectric constant, and dielectric loss tangent, respectively. The MC film shows a dielectric constant of 2.5 and a dielectric loss of 0.8 at 1 kHz, indicating the dielectric material's power loss and making it desirable for several practical applications.
In order to understand the role of the dielectric constant in TENGs, a schematic of a dielectric-to-dielectric-based TENG and its equivalent circuit model is depicted in Fig. 2(d). The potential difference exists across the surfaces of two dielectric layers, the two electrodes, and the dielectric-to-electrode interfaces, justifying the equivalent circuit model as three capacitors connected in series. The output performance of a TENG operating in the contact-separation mode37 can be analyzed using eqn (5).
| |
 | (5) |
where
σ is the surface charge density,
Q is the charge induced on the surface of the dielectric material,
d1 and
d2 are the thicknesses of each dielectric material;
ε1 and
ε2 represent the permittivity of the dielectric materials,
X(
t) is the separation gap between the materials,
S is the surface area of the electrode and
ε0 is the permittivity of vacuum.
Eqn (5) clarifies that the induced charge (
Q) and the surface charge density (
S) are the key parameters in the output performance of TENG, and the enhancement in dielectric constant can significantly enhance the
σ, increasing the triboelectric outputs.
3.2. Structural and morphological analysis of MC film
Fig. 3(a) shows the FTIR spectra of microbial cellulose film. The bands corresponding to the major functional groups of the cellulose can be observed in this graph. The band appearing at 1020 cm−1 is assigned to the stretching of the C–O–C bonds within a pyranose ring structure.39 The in-plane bending vibrations of the –O–H group cause the band to appear at 1240 cm−1.40 The stretching vibrations of the –C–H bond appear at 1350 cm−1.41
 |
| | Fig. 3 (a) FTIR spectra and (b) & (c) Surface micrographs of the microbial cellulose film. | |
The absorption band at 1640 cm−1 is assigned to the stretching vibrations of the carbonyl group of the cellulose.42 The band at 2910 cm−1 originates because of the –C–H stretching.43 The absorption band near 3290 cm−1 is the signature band of the stretching of the hydroxyl (O–H) group.43 In addition, a small band at ∼890 cm−1 also appears, which can be attributed to the β-1,4 bond vibrations of glucose polymers.44
The MC film synthesized by fermenting the SCOBY culture with sweetened tea was analyzed using FESEM and is shown in Fig. 3(b) and (c). The analysis includes surface morphology and porosity after drying the MC film at 50 °C. The MC film exhibits a highly irregular, rough surface, attributed to random deposition during fermentation. The image shows that the film has significant uneven features and numerous variations across its surface. Very high porosity was also observed in the MC film, with pores varying in size and shape. Due to these characteristics, it can be utilized in specific applications where the porosity and surface roughness are advantageous. That is why it is further tested as a tribopositive material in TENG, leveraging its unique morphological characteristics to enhance energy-harvesting efficacy.
3.3. Analysis of antibacterial properties of the microbial film
The bacterial inhibition diameter is used to determine the bacteriostatic ability of the microbial film. The tested samples with E. coli and Bacillus subtilis bacterial strains are shown in Fig. 4(a) and (b). The film's bacterial sensitivity is revealed by the clear zone around it. The clear area is referred to as the zone of inhibition, and it represents the area on the agar plate where microbes cannot grow due to the diffusion of the antibacterial agent into the agar, creating an unfavourable environment for the reproduction or growth of the microorganisms.45
 |
| | Fig. 4 Antibacterial activity of microbial film against (a) E. coli and (b) Bacillus. | |
The larger the inhibition zone diameter, the greater the antibacterial effectiveness of the film. MC film with E. coli bacteria shows a significant (∼10 mm) inhibition zone, whereas for Bacillus it is only 2 mm. The results suggested that the film exhibited a strong antibacterial activity against Gram-negative bacteria and mildly inhibited the growth of Gram-positive bacteria. Moreover, even though the microbial film was not incorporated with other antimicrobial agents, it still exhibited antibacterial activity, which can be due to the source of the microbial film. The symbiotic culture of bacteria and yeast (SCOBY) comprises various bacteria and yeast, including Acetobacter Aceti, Gluconobacter oxydans, Zygosaccharomyces, and Saccharomyces.31 The yeast species used, i.e., Zygosaccharomyces and Saccharomyces, exhibit antibacterial activity by releasing proteins, peptides, and killer toxins (K1, K2, K28), which disrupt cellular processes and cell membrane integrity.46 Thus, SCOBY-based cellulose film depicts a microbial cellulose film that inherently possesses antibacterial activity without the addition of other antibacterial agents. However, in the case of Bacillus, a uniform red-coloured ring formed around the film, which may be a compound released by the bacillus culture from the microbial film.
3.4. Working mechanism and overlapped electron cloud model of Microbial Cellulose-based MC-TENG device
The working mechanism of the microbial cellulose-based triboelectric nanogenerator (MC-TENG) is shown in Fig. 5(a) and (b). When an external force is applied to the nanogenerator, the upper and lower layers come into contact. The transfer of surface charge will occur due to contact electrification. Cellulose is tribopositive, and FEP is tribonegative in the triboelectric series. It can be concluded that microbial cellulose is more likely to lose electrons while FEP gains electrons. Due to contact electrification, the positive charges gather on the surface of the cellulose film, while the negative charges are on the FEP polymer sheet (Fig. 5(b)(i)). As soon as both layers start separating due to external force, a potential difference is generated, as shown in Fig. 5(b)(ii). The potential difference keeps increasing with an increase in the separation gap until equilibrium (Fig. 5(b)(iii)) is attained. When the direction of the external force changes, the potential difference decreases with increasing separation distance between the two layers. Because of the electric potential difference, the electrons are compelled to move between the two layers, as the electrodes form a closed circuit. Due to electrostatic induction, the electrons will move in opposite directions from the source (Fig. 5(b)(iv)). Wang et al.47 have explained these atomic interactions using an electron-cloud model. The possible physical process of electron transfer in contact electrification is shown in Fig. 5(c). Initially, as the MC and FEP are separated, the H atoms of MC and the F atoms of FEP are isolated, showing that no electron clouds are overlapping (Fig. 5(c)(i)). The atoms hold their electrons within the potential wells, and the interfacial potential barrier (Ei) prevents electron transfer between the electron clouds.
 |
| | Fig. 5 (a) and (b) Working mechanism and (c)(i)–(iii) electron cloud model describing contact-electrification in MC-FEP for MC-TENG. | |
As soon as MC and FEP come into contact with each other, the H and F atoms of the interface enter into the repulsive area with the overlapping of clouds, reducing the interfacial potential barrier (Fig. 5(c)(ii)). At this stage, the contact electrification between the MC and FEP will occur because the electrons transfer easily into the potential well of the F atom at the interface of the polymer films. After this, when the layers get separated again, the H atom MC loses electrons, and the F atoms of FEP gain electrons. As a result of this, the contact surface of MC becomes positively charged while the contact surface of FEP becomes negatively charged (Fig. 5(c)(iii)). This continuous contact-and-separation mechanism on the MC generates a potential difference between the copper electrodes of both films, causing the external circuit to conduct current as charge flows.
3.5. Testing of an effective output power density of CS/PVA-TENG
An MC film of size 2 × 2 cm2 has been tested in MC-TENG for current (I) and Voltage (V) measurements. The electrical output of MC-TENG has been measured at three different frequencies: 3 Hz, 4 Hz, and 5 Hz by applying a compressive force of 1.5 N. Fig. 6(a) and (b) represents the measured open circuit voltage (Voc) and short-circuit current (Isc).
 |
| | Fig. 6 (a) Voc and (b) Isc of fabricated TENGs using a linear-motor-based contact-separation mechanism. The measured (c) Voc and Isc, (d) power density on the external load resistance in the range of 10 KΩ to 100 MΩ of MC-TENG, (e) Stability measurement test of MC-TENG for more than 10 000 cycles. | |
The MC-TENG exhibits a maximum voltage of ∼620 V (peak-to-peak) at approximately 4 Hz and a current of ∼40 µA (peak-to-peak) at approximately 5 Hz. Fig. 6(c) depicts the Isc and Voc values of MC-TENG measured at different load resistance values. As the load resistance increases, the current decreases, while the voltage increases. The short-circuit and open-circuit conditions affect the output power density of any TENG. So, the power density is obtained by dividing the current and voltage values at different load resistances by the contact area, as depicted in Fig. 6(d). As expected, the MC-TENG exhibits lower power density at both lower and higher resistances. The MC-TENG achieved a maximum power density of 16.5 W m−2 at a load resistance of 10 MΩ. The increased output can be attributed to the film's high roughness and very high porosity. There are no reports available on such microbial cellulose-based TENG. The durability test was performed using a repetitive contact-separation test with more than 10
000 cycles, as shown in Fig. 6(e). On the other hand, very few reports are available on bacterial cellulose-based TENG. Table 1 represents triboelectric outputs of bacterial-cellulose-based TENGs reported to date.
Table 1 Literature summary of the bacterial cellulose-based TENGs
| Tribopositive layer |
Tribonegative layer |
Voc (V) |
Isc (μA) |
Output power (W m−2) |
Ref. |
| Bacterial cellulose (BC)/sodium alginate |
FEP |
300 |
27 |
1.81 × 10−3 |
29 |
| BC and barium titanate (BT) |
PDMS |
57.6 |
5.78 |
0.042 |
27 |
| BC and BT |
Copper tape |
181 |
21 |
4.8 |
48 |
| BC and carbon black grains |
Ecoflex |
102.3 |
2 |
— |
49 |
| MC |
FEP |
620 |
40 |
16.5 |
Present work |
3.6. Practical and real-time applications of the MC-TENG device
The electrical output o any TENG is an alternating signal, which is unsuitable for powering various portable and wearable electronic devices. Thus, a full-bridge rectifier has been connected to TENG to convert the alternating signal generated by TENG into a direct signal to charge capacitors. The electrical energy stored in the capacitor is then used to power the calculator.
The circuit diagram of the MC-TENG charging different capacitors is shown in Fig. 7(a). Different capacitors with capacitances of 1, 10, 22, and 47 µF were charged with the rectified voltage from the MC-TENG, and the accumulated voltages across the capacitors are shown in Fig. 7(b). As shown in Fig. 7(b), the 1-µF capacitor was charged to more than 35 V in 150 s. Finally, Fig. 7(c) shows the practical application of MC-TENG, using the electrical energy stored in the capacitor to power the calculator. Also, several red LEDs connected in series, spelt as “TIET”, are turned on by contact separation of the MC-TENG without using any components such as rectifiers or capacitors, as shown in Fig. 7(d) and in supplementary video V1. As a result, these practical applications demonstrate the excellent efficiency of MC-TENG, which is synthesized and fabricated in a simple, cost-effective approach and can be easily used to power low-power, portable electronic equipment for commercial use.
 |
| | Fig. 7 (a) Equivalent circuit of the full-wave bridge rectifier for converting the alternating current signals of MC-TENG into the direct current signal to power up the electronic equipment by charging capacitors, (b) voltage accumulated across the capacitors having a capacitance of 1, 10, 22, and 47 µF. Photographic image of (c) (i) Calculator without any battery, (ii) calculator in switch off mode, (iii) calculator in switch on mode, (iv) charging and discharging of 22 µF capacitors for powering the calculator, (d) (i, ii) 55 red commercial LEDs connected in series spelt as ‘TIET’ was directly turned on by MC-TENG device. | |
4. Conclusion
This study effectively demonstrates the potential of MC as a tribopositive material in the fabrication of an environmentally friendly MC-TENG. Synthesized via a simple fermentation process, the fundamental characteristics of MC film, such as rough surface morphology and high porosity, improve the electrical outputs of TENG. The advantages of MC film, such as edibility, non-toxicity, and biodegradability, make it an exceptional material for sustainable energy applications. The MC-TENG exhibits an open-circuit voltage (Voc) of ∼620 V, a short-circuit current (Isc) of ∼40 µA, and a power density of 16.5 W m−2 at a 10 MΩ load resistance. Moreover, the biomaterial demonstrated remarkable inherent antibacterial activity against Gram-negative and Gram-positive bacteria with a zone of inhibition of 10 mm and 2 mm, respectively. In addition, the device's ability to charge the capacitor and power the calculator demonstrates its practical application.
Author contributions
Raj Ankit: conceptualization, visualization, synthesis, methodology, characterization, analysis, validation, writing – original draft, review, and editing. Simranjeet Kaur: synthesis, methodology, analysis, characterization writing – original draft. Shinar Athwal: conceptualization, methodology, analysis, validation, writing – original draft. Taranveer Kaur: characterization, analysis, validation, writing – original draft. Jayant Kolte: conceptualization, supervision, investigation, methodology, validation, writing – review and editing.
Conflicts of interest
The authors declare that they have no known competing financial interests or personal relationships that could have influenced the work reported in this paper.
Data availability
The data included in this article are available on request via the corresponding author. Supplementary information (SI) is available. See DOI: https://doi.org/10.1039/d5ma01186h.
Acknowledgements
The authors thank DST FIST (grant no. SR/FST/PS-II/2018/53) for providing characterization facilities.
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