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Review

Polymer/Fullerene Nanocomposite for Optoelectronics—Moving toward Green Technology

by
Ayesha Kausar
1,2,3,*,
Ishaq Ahmad
1,2,3,
Malik Maaza
2,
M. H. Eisa
4 and
Patrizia Bocchetta
5,*
1
NPU-NCP Joint International Research Center on Advanced Nanomaterials and Defects Engineering, Northwestern Polytechnical University, Xi’an 710072, China
2
UNESCO-UNISA Africa Chair in Nanosciences/Nanotechnology, iThemba LABS, Somerset West 7129, South Africa
3
NPU-NCP Joint International Research Center on Advanced Nanomaterials and Defects Engineering, National Centre for Physics, Islamabad 44000, Pakistan
4
Department of Physics, College of Science, Imam Mohammad Ibn Saud Islamic University (IMSIU), Riyadh 13318, Saudi Arabia
5
Department of Innovation Engineering, University of Salento, Edificio La Stecca, Via per Monteroni, 73100 Lecce, Italy
*
Authors to whom correspondence should be addressed.
J. Compos. Sci. 2022, 6(12), 393; https://doi.org/10.3390/jcs6120393
Submission received: 18 October 2022 / Revised: 29 November 2022 / Accepted: 13 December 2022 / Published: 16 December 2022
(This article belongs to the Section Composites Applications)
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Abstract

:
Optoelectronic devices have been developed using the polymer/fullerene nanocomposite, as focused in this review. The polymer/fullerene nanocomposite shows significant structural, electronics, optical, and useful physical properties in optoelectronics. Non-conducting and conducting polymeric nanocomposites have been applied in optoelectronics, such as light-emitting diodes, solar cells, and sensors. Inclusion of fullerene has further broadened the methodological application of the polymer/fullerene nanocomposite. The polymeric matrices and fullerene may have covalent or physical interactions for charge or electron transportation and superior optical features. Green systems have also been explored in optoelectronic devices; however, due to limited efforts, further design innovations are desirable in green optoelectronics. Nevertheless, the advantages and challenges of the green polymer/fullerene nanocomposite in optoelectronic devices yet need to be explored.

Graphical Abstract

1. Introduction

Optoelectronic devices have outstanding optical and electronic properties [1,2,3]. Optoelectronic devices can transform electrical energy into light energy using semiconducting materials [4,5]. Important optoelectronic devices include the light-emitting diode, the photovoltaic device, and the optical sensor [5,6,7]. The use of nanocomposites and green nanomaterials in optoelectronics has been investigated [8,9]. Nanocomposites with high optical transparency and electron transfer properties are preferred for optoelectronics devices. Nanocomposites have been used in the light-emitting diode and exhibit low price, high conductivity, and fine optical properties. In photovoltaic devices, nanocomposites provide high charge transfer, high hole transport, and enhanced power conversion efficiency [10]. Optical sensors have also been developed using nanocomposites for enhanced sensing properties and applications. Polymer/fullerene nanocomposites have been applied in optical devices [11], such as the light-emitting diode [12], the photovoltaic device [13], and the optical sensor [14]. Inclusion of the fullerene nanoparticle in polymers may form physical or covalent interactions with the polymeric matrices. The polymer/nanofiller may develop an interconnecting network to facilitate electron transference and photon transfer properties [15]. For green nanocomposite technology, polymer/fullerene nanocomposites have been developed and applied. However, extensive efforts are desirable for advanced green-fullerene-based optoelectronics.
In this review, the research progress on the fullerene- and polymer/fullerene-derived nanocomposite regarding optical devices is discussed. High-performance polymer/fullerene nanocomposites have been successfully used in the light-emitting diode, photovoltaics, and the optical sensor.

2. Optoelectronics

Polymer/nanocarbon nanocomposites have been applied in optical and electronic industries [16,17]. Accordingly, polymer/nanocarbon nanocomposites have been used in light-emitting diodes, sensors, and electronic devices [18,19,20,21]. Among nanocarbons, graphene, carbon nanotubes, nanodiamond, etc., have been found useful in next-generation devices [22,23,24,25]. Nanocomposites have been fabricated through in situ, solution, melt-processing, spin-coating, printing, and other chemical and physical methodologies [26,27,28]. Fullerene is an important type of hollow cage-like nanocarbon nanostructure. Fullerene is composed of sp2-hybridized carbon atoms with a π-conjugation system [29,30]. The fullerene molecule is constructed by polygons, i.e., five- to seven-membered rings in the structure. Fullerene with 60 carbon atoms is named the C60 fullerene molecule, also referred to as Buckminster fullerene. It was first discovered as a polygon with 60 vertices and 32 faces [31]. This object is like a football or a soccer ball. Hence, C60 is the most symmetrical form of fullerene, with superior optical, electrical, magnetic, and pharmaceutical properties, in addition to the properties of encapsulating small molecules for various industrial applications. The optical properties of fullerenes have been widely examined in different solvents through spectroscopic techniques. Furthermore, according to the laws of quantum mechanics, the nonlinear optical polarizability of fullerene molecules was calculated and found to be higher than that of the carbon nanotube [31]. An electrical property study of zero-dimensional fullerene showed that fullerenes have semiconducting-metallic transitions in the large electric field, similar to the one-dimensional carbon nanotube and two-dimensional graphene. The magnetic properties of fullerene have been studied using density functional theory. In the presence of a magnetic field, fullerene exhibits diamagnetism independent of a metallic or semiconducting nature, similar to the carbon nanotube. Among pharmaceutical properties, fullerenes have the ability to inhibit the access of toxins to the catalytic site of enzymes. Moreover, fullerenes may act as radical scavengers and antioxidants, like other nanocarbons. Similarly, C70 is a higher fullerene analogue having 70 carbon atoms. C70 has excellent catalytic and photovoltaic properties for relevant applications [32]. The important forms of fullerene include C60 and C70 molecules (Figure 1) [33]. The higher fullerene analogues have also been reported with large cage sizes and a higher number of carbon atoms [34]. Fullerenes have been prepared using numerous methods, such as arc discharge, laser irradiation, plasma technique, microwave synthesis, CO2 reduction with metallic lithium, and chemical methods [35]. Among these techniques, the arc discharge method is a successful, advantageous, and widely used method to generate high-quality fullerene in high yield. The fullerene production time and method parameters are also easily controllable. The plasma technique and microwave synthesis also produce good-quality fullerene. However, the plasma and microwave techniques have lower yield, high cost, and complicated parameters involved, relative to the arc discharge method. The use of a chemical method usually yields byproducts and has lower fullerene quality compared to the other methods. Kroto et al. [36] synthesized fullerene via carbon source vaporization using the laser irradiation method. The resulting fullerene consisted of clusters of 60 carbon atoms. The plasma technique was used to form good-quality fullerenes [37]. Xie et al. [38] used the microwave plasma synthesis method to attain fullerenes from chloroform plasma in a low-pressure and high-temperature argon atmosphere. Chen and Lou [39] developed fullerene C60 by reduction of CO2 using metallic lithium at 700 °C and 100 MPa. Scott et al. [40] adopted multi-step chemical conditions to convert the carbon precursor to fullerene C60. Henceforth, several methods were used to synthesize fullerene structures, although all the techniques have relative advantages and disadvantages involved. Fullerene molecules have fine structural, electronic, optoelectronic, fluorescence, and photochemical properties [41,42,43,44]. Substituted fullerene nanostructures have also been used to develop optoelectronics [45,46,47].
Fullerene and derived fullerene molecules have been used in various technical areas, as shown in Figure 2 [48]. The applications of fullerene include solar cells, fuel cells, capacitors, sensors, catalysis, and adsorption. In optical devices, electron affinity, charge transference, optoelectronic features, band gap, and other tunable properties have been studied. The compatibility between the polymer and fullerene has been improved through using modified fullerene molecules and an appropriate polymer. Mostly, conjugated polymers have been found well matched with fullerenes. Especially, the π-conjugated structure of polythiophene has been found compatible with the fullerene sp2-hybridized nanocarbon structure [49]. Similarly, polythiophene derivatives have been found to be quite compatible with the fullerene molecule. Other conjugated polymers, such as polyaniline and polypyrrole, may also develop π–π stacking interactions with fullerene.

3. Polymer/Fullerene Nanocomposite for LEDs: Insertion of Green Technology

The term “green technology” means the use of eco-friendly, renewable, and biodegradable materials for desired applications, i.e., optoelectronic devices [50]. In this regard, on the one hand, green polymers (naturally derived biodegradable) and green nanofillers have been used to construct these devices. On the other hand, green synthesis methodologies have been applied to develop desired biodegradable nanomaterials. The ecofriendly nanocomposites developed for optoelectronics have low cost, light weight, fine processability, and electrical and optical properties [51,52]. The green-nanomaterial-derived donor–acceptor structures possess fine photo-energy conversion for LED devices. Fullerene-based organic light-emitting diodes (OLEDs) have been focused on in the literature [53,54]. OLEDs with fullerene nanoparticles have been fabricated due to inexpensiveness and high efficiency for next-generation optoelectronics [55]. OLEDs have been designed using the polythiophene/fullerene nanocomposite (Figure 3) [56]. In this attempt, the promising solution-processing approach was used to form low-cost, flexible, and compact sensor arrays of polythiophene/fullerene. The novelty of the OLED sensing system relies on its workability in two operating modes, i.e., photoluminescence intensity and decay time detection modes. The dye-embedded polythiophene/fullerene-derived OLED had a fast photo-response toward red-emitting dye-based oxygen and glucose sensors. Another successful design for the LED is poly(3,4-ethylenedioxythiophene):polystyrene sulfonate (PEDOT:PSS) [57]. In another attempt [58], an OLED based on tetracene, indium tin oxide/poly(3,4-ethylenedioxythiophene):polystyrene sulfonate (ITO/PEDOT:PSS), polycyclopentadithiophene-benzothiadiazole (PCPDTBT), phenyl-C70-butyric acid methyl ester (PC70BM), and phenyl-C71-butyric acid methyl ester (PC71BM) has been reported. Figure 4 shows the chemical structures and energy-level diagrams of solar cell devices [58]. It has been observed that the HOMO-LUMO was 5.4 and 3.0 eV for tetracene. PCPDTBT revealed a HOMO-LUMO of 5.1 and 3.7 eV. Tetracene/PCPDTBT exhibited an energetic barrier of 0.3 eV for hole extraction. The results suggested that the presence of a conjugated system promotes electron transport and hole extraction processes. Kang et al. [59] proposed LED devices with a high power conversion efficiency of 3.1% (AM 1.5 irradiation) and luminance of 8000 cd/m2 [60]. For green OLED technology, Herrera et al. [61] developed a nanocomposite system using a green design and fabrication route. Inclusion of a small amount of polymer/fullerene may modify the optical response of the LED or OLED. Nevertheless, more focused research efforts may be needed to develop green polymer/fullerene systems to be applied in diode-based devices. In this regard, novel solution-processable polymer/fullerene-based flexible conductors can be developed to replace the ITO/glass electrode in these devices. The main advantages of using polymer/fullerene-based materials in LEDs (relative to ITO or glass materials) include design flexibility, light weight, low cost, and high efficiency. In this regard, the development of new green polymer/fullerene systems and ecofriendly processing routes must be focused on to form next-generation efficient, green OLED devices.

4. Polymer/Fullerene Nanocomposite in Solar Cells via the Green Approach

Advanced nanocomposites have always been of interest for application in solar cells [62,63,64]. Nanocomposites have good crystallinity, good contact between layers, good electrical conductivity, and promising light absorption properties, resulting in an improvement in the net efficiency of solar cells [65,66,67]. The design combination of a conducting polymer and nanocarbon nanofillers has resulted in enhanced solar cell efficiency [68]. Conjugated polymer/nanocarbon nanocomposites mostly act as electron donors, whereas the nanocarbon performs as the electron acceptor [69,70]. Generally, low-band-gap nanocomposites and blends have been found valuable in solar cell application [71]. Initially, various non-green polymeric nanocomposite systems were used in solar cell devices. PEDOT:PSS has been applied as an essential solar cell material [72]. PEDOT:PSS possesses fast electron and hole transportation features. The PEDOT:PSS-based nanocomposite was coated on the indium tin oxide (ITO) electrode using the spin-casting technique [73]. Consequently, the morphological, electron-conducting, and solar cell properties of PEDOT:PSS have been examined [74,75]. In this case, a solar cell efficiency of ~9% was obtained, which was high enough to obtain a high-performance solar cell device. Another successful system identified for the solar cell was poly(3-hexylthiophene-2,5-diyl):[6,6]-penyl-C61-butyric-acid-methyl-ester (P3HT:PCBM) [76]. For bulk heterojunction solar cell application, P3HT:PCBM film was developed through the spin-casting technique. The power conversion efficiency was found to be ~3.5%. For the P3HT:PCBM system [77], solvent methods, annealing, and drying approaches have been found useful. The microstructure analysis and optical micrographs have been obtained (Figure 5). Both micrometer-size crystalline domains and small domains (<200 nm) have been detected in the micrographs of P3HT:PCBM films [77]. It has been observed that the presence of impurities may produce inhomogeneities in the samples. The spin-coated and slow-dried nanocomposite showed homogeneous dispersion; however, impurities were still present in the sample. An important solar cell system was reported by Roy et al. [78]. Poly(methyl methacrylate) (PMMA), fullerene, quantum dots, single-walled carbon nanotubes, and reduced graphene oxide were used (Figure 6). Here, fullerene addition affected the charge carrier ability of the nanocomposites. With fullerene addition, the power conversion efficiency improved up to 1.15% (Table 1) [78]. PMMA and fullerene and other nanocarbons have the ability to develop interconnecting pathways for electron conduction [79,80]. Later research shifted toward the use of green designed materials and green synthesis approaches in solar cells.
For green nanocomposite technology, polymer/fullerene systems have been designed and studied in the literature [81]. However, limited reports have focused on the use of green polymers and green fabrication routes for solar cells. Amb et al. [82] designed conjugated polymer/fullerene-based blue-green solar cells using the thin-film deposition technique, i.e., spin coating. They reported a blue-green-colored low-bandgap polymer (PGREEN)-based nanocomposite (Figure 7) [82]. The poly(3-hexylthiophene):(6,6)-phenyl-C61-butyric acid methyl ester (PCBM)-based nanocomposite was used as a light-absorbing layer. The spin-coated PCBM-based PGREEN revealed fine solar cell performance. The donor–acceptor bulk heterojunction solar cell design is given in Figure 8 [82]. The J–V features of the devices with the PGREEN nanocomposite are also give in Figure 8. With fullerene inclusion, the solar cell system had a power conversion efficiency of up to 1.92%. The results were observed due to the high electron mobility of fullerenes effectively promoting charge dissociation and transportation in solar cell devices. Khlyabich et al. [83] reviewed the use of polymer/fullerene designs using non-halogenated solvent systems, such as toluene and tetrahydrofuran. Recent efforts have focused on the replacement of non-halogenated organic solvents with green solvent systems, such as water and ionic liquid [84]. The green-solvent-based methods have been successful in the fabrication of photoactive fullerene solar cells. Lee et al. [85] also proposed routes to develop polymer solar cells with a power conversion efficiency of >17%. Such solar cells have been developed using the green solvent and green fabrication route (Figure 9) [85]. The appropriate material design, choice of processing technique, and choice of solvent may lead to the formation of green solar cells on a large scale. Thus, green polymer/fullerene systems provide a roadmap to design efficient green future solar cell materials. The latest advances in perovskite solar cells have also pointed out the use of fullerene molecules [86]. Thus, fullerene-based high-efficiency perovskite solar cells have been reported. The inclusion of fullerene molecules in interfacial selective electron extraction layers in perovskite have remarkably improved the solar cell efficiency and device stability [87]. In this regard, facile processing methods have been used to form perovskite films. In conclusion, fullerene-based perovskite solar cells have been produced for large-scale and commercial applications [88].

5. Polymer/Fullerene for Optical Sensors: On the Road to Green Nanocomposites

Optical or electronic sensors have been reported using various relevant materials [89,90,91]. Conducting polymers have notable electron donor or acceptor properties valuable for sensor applications [92]. Consequently, conducting polymers have been used for optical, electrical, and sensing properties. The conducting polymer/nanocarbon nanocomposite has also been prepared and analyzed [93,94]. Nanocarbon nanostructures, such as graphene and carbon nanotubes, have been applied in sensing applications [95]. Among conducting polymers, polyaniline has been frequently chosen for optical sensing [96,97,98]. The sensing mechanism of the nanocomposite has been found dependent on the matrix–nanofiller interactions and interface development [99,100,101]. Similarly, the conducting polymer/fullerene nanocomposite has been fabricated using appropriate techniques [102,103,104]. In this regard, organic thin-film photodiode (OPD) devices have been developed for optical sensors [105]. Optical sensors have been formed through advanced techniques, such as printing, spraying, and spin casting [106]. Analytes have been detected using the fluorescence/luminescence detection technique with the OPD device [107]. Various conducting polymers, such as P3HT, PCBM, PEDOT:PSS, and PEDOT:PSS, have been applied in optical sensors. In optical sensors, fullerene molecules, such as C60 and C70, have been applied [108,109,110]. Amao et al. [111] fabricated an optical temperature sensor using a PMMA- and C60-derived nanocomposite. The fluorescence intensity was explored in the range of 260–373 K. However, initial efforts on optical sensors have focused on the use of non-green materials and methods. Similar to solar cells, the technology for optical sensors has also been upgraded toward the use of green nanocomposite or green synthesis routes. For green nanocomposite technology, Rather et al. [112] developed a green polymer/fullerene optical sensor. The sensor was used for sensing bisphenol A in the concentration range of 74 nM to 0.23 M. A detection limit of 3.7 nM was observed. Zhang et al. [113] formed a porphyrin–diazocine–porphyrin–fullerene (PDP–C60)- and porphyrin–diazocine–porphyrin–fullerene/glassy carbon electrode (PDP–C60/GCE)-based optical sensor. The fine dopamine detection of the PDP–C60/GCE nanocomposite electrode was analyzed. Figure 10 shows the cyclic voltammetry (CV) curves of the PDP–C60/GCE nanocomposite [113]. The linear relationship between the peak currents and scan rates of the nanocomposite revealed fine sensing performance toward dopamine. The sensor shows a detection limit of 0.015 μM. Here again, the development and analysis of better polymer/fullerene-based green nanocomposite systems have been found essential to obtain high-performance advanced optical sensors.

6. Future and Conclusions

Polymer/fullerene nanocomposites have fine optical, electronic, electrical, thermal, mechanical, sensing, and other valuable properties for technical applications. Fullerene and fullerene-derived nanomaterials have led to high-performance optoelectronics, such as the light-emitting diodes, photovoltaic devices, and optical sensors (Table 2).
In such devices, mostly conducting polymers, such as polyaniline, polypyrrole, polythiophene, and poly(3,4-ethylenedioxythiophene), have been used [114,115,116]. To further enhance properties, nanocarbon nanoparticles are incorporated in conjugated polymers. The optoelectronic performance of polymer/fullerene nanomaterials is dependent on the fullerene dispersion and matrix–fullerene interactions. However, non-conjugated polymers have also been applied in optoelectronics devices. The future of polymer/fullerene nanocomposite-derived optoelectronics depends on the design novelties and fullerene dispersion and functionality in the conjugated polymers. For all types of optoelectronic devices, facile fabrication techniques, modified polymers, and functional fullerene nanoparticles need to be incorporated. The systems developed for green polymer/fullerene nanocomposite technology show fine performance; however, further efforts must be made to develop green LEDs, OLEDs, solar cells, and optical sensors. Thus, in recent years, great advancements have been made in fabrication skills and integration of optoelectronic nanomaterials to improve performance and the final device architecture. For next-generation optoelectronics, fullerene-based green nanocomposites can be studied as promising candidates for creating miscellaneous flexible and miniature devices. The recent advances in optoelectronics, in material selection and fabrication approaches, have proposed the use of thiophene-derived green polymers and green synthesized/functionalized fullerenes. These materials are considered ideal to obtain eco-friendly energy conversion, sensing, and diode devices. In this regard, green nanocomposites processed through the eco-friendly solution route can lead to the best results. However, the challenges and future research direction in this area need to be analyzed.
In short, this review summarizes the critical properties and performance of the polymer/fullerene nanocomposite in optoelectronic devices. Numerous facile fabrication and design approaches have been used to fabricate these technical devices. The versatility of the polymer/fullerene nanocomposite for optoelectronic devices relies on processing, fullerene dispersal, matrix–nanofiller compatibility, and essential properties. Future advancements in the field of the polymer/fullerene nanocomposite may develop advanced next-generation green optoelectronic devices.

Author Contributions

Conceptualization, A.K.; data curation, A.K.; writing of original draft preparation, A.K.; Review and editing, A.K.; I.A.; M.M.; M.H.E.; P.B. All authors have read and agreed to the published version of the manuscript.

Funding

This research received no external funding.

Conflicts of Interest

The authors declare no conflict of interest.

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Figure 1. Comparison of C60 and C70 nanostructures.
Figure 1. Comparison of C60 and C70 nanostructures.
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Figure 2. Synthesis, functionalization, and application of fullerene [48]. Reproduced with permission from Wiley.
Figure 2. Synthesis, functionalization, and application of fullerene [48]. Reproduced with permission from Wiley.
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Figure 3. Organic light-emitting diode setup [56]. Reproduced with permission from Wiley.
Figure 3. Organic light-emitting diode setup [56]. Reproduced with permission from Wiley.
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Figure 4. (a) Chemical structure of fullerene materials and (b) energy-level diagram of a bulk heterojunction device [58]. ITO/PEDOT:PSS = indium tin oxide/poly(3,4-ethylenedioxythiophene):polystyrene sulfonate; PCPDTBT = polycyclopentadithiophene-benzothiadiazole; PC70BM = phenyl-C70-butyric acid methyl ester; PC71BM = phenyl-C71-butyric acid methyl ester. Reproduced with permission from Wiley.
Figure 4. (a) Chemical structure of fullerene materials and (b) energy-level diagram of a bulk heterojunction device [58]. ITO/PEDOT:PSS = indium tin oxide/poly(3,4-ethylenedioxythiophene):polystyrene sulfonate; PCPDTBT = polycyclopentadithiophene-benzothiadiazole; PC70BM = phenyl-C70-butyric acid methyl ester; PC71BM = phenyl-C71-butyric acid methyl ester. Reproduced with permission from Wiley.
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Figure 5. Optical microscope images for P3HT:PCBM film: (a) untreated (i.e., fast spin coated), (b) thermally annealed, (c) vapor annealed, and (d) slow dried. Inhomogeneities produced by impurities in (d) (upper-right corner of image) can often be seen in spin-coated P3HT:PCBM films [77]. P3HT:PCBM = poly(3-hexylthiophene):[6,6]-phenyl C61-butyric acid methyl ester. Reproduced with permission from Nature.
Figure 5. Optical microscope images for P3HT:PCBM film: (a) untreated (i.e., fast spin coated), (b) thermally annealed, (c) vapor annealed, and (d) slow dried. Inhomogeneities produced by impurities in (d) (upper-right corner of image) can often be seen in spin-coated P3HT:PCBM films [77]. P3HT:PCBM = poly(3-hexylthiophene):[6,6]-phenyl C61-butyric acid methyl ester. Reproduced with permission from Nature.
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Figure 6. Schematic diagram of (a) sequential fabrication of solar cells using different allotropes of carbon and (b) probable arrangement of different allotropes used during sequential fabrication of carbon solar cells [78]. PMMA = poly(methyl methacrylate); QD = quantum dot; SWCNT = single-walled carbon nanotube; r-GO = reduced graphene oxide. Reproduced with permission from ACS.
Figure 6. Schematic diagram of (a) sequential fabrication of solar cells using different allotropes of carbon and (b) probable arrangement of different allotropes used during sequential fabrication of carbon solar cells [78]. PMMA = poly(methyl methacrylate); QD = quantum dot; SWCNT = single-walled carbon nanotube; r-GO = reduced graphene oxide. Reproduced with permission from ACS.
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Figure 7. A green polymer/fullerene solar cell [82]. Reproduced with permission from ACS.
Figure 7. A green polymer/fullerene solar cell [82]. Reproduced with permission from ACS.
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Figure 8. Schematic diagram of PGREEN polymer solar cells with (a) conventional and (b) inverted geometry. (c) Current–voltage plots for illuminated conventional geometry cells (0.04 cm2) for each of the three polymer batches produced under identical processing conditions. [82]. Reproduced with permission from ACS.
Figure 8. Schematic diagram of PGREEN polymer solar cells with (a) conventional and (b) inverted geometry. (c) Current–voltage plots for illuminated conventional geometry cells (0.04 cm2) for each of the three polymer batches produced under identical processing conditions. [82]. Reproduced with permission from ACS.
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Figure 9. Design of eco-friendly polymer solar cells [85]. Reproduced with permission from ACS.
Figure 9. Design of eco-friendly polymer solar cells [85]. Reproduced with permission from ACS.
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Figure 10. (a) CV curves of PDP–C60/GCE nanocomposite (pH 7.4) containing 400 μM of DA at different scan rates (v) ranging from 0.1 to 1.0 V s−1 and (b) linear relationship between the peak currents and scan rates [113]. CV = cyclic voltammetry; PDP–C60/GCE = porphyrin–diazocine–porphyrin–fullerene/glassy carbon electrode; DA = dopamine. Reproduced with permission from Elsevier.
Figure 10. (a) CV curves of PDP–C60/GCE nanocomposite (pH 7.4) containing 400 μM of DA at different scan rates (v) ranging from 0.1 to 1.0 V s−1 and (b) linear relationship between the peak currents and scan rates [113]. CV = cyclic voltammetry; PDP–C60/GCE = porphyrin–diazocine–porphyrin–fullerene/glassy carbon electrode; DA = dopamine. Reproduced with permission from Elsevier.
Jcs 06 00393 g010
Table
Table 1. Solar cell parameters of nanocarbon-based solar cells [78]. PMMA/C60 = poly(methyl methacrylate)/fullerene C60; PCE = photo-conversion efficiency; Jsc = short-circuit current density; Voc = open-circuit voltage; FF = fill factor. Reproduced with permission from ACS.
Table 1. Solar cell parameters of nanocarbon-based solar cells [78]. PMMA/C60 = poly(methyl methacrylate)/fullerene C60; PCE = photo-conversion efficiency; Jsc = short-circuit current density; Voc = open-circuit voltage; FF = fill factor. Reproduced with permission from ACS.
CellVoc (mV)Jsc (mA·cm−2)FFPCE (%)
No PMMA/C605001.540.560.56
PMMA/C605063.930.591.15
Table
Table 2. Stipulations of the polymer/fullerene nanocomposite in optoelectronic applications.
Table 2. Stipulations of the polymer/fullerene nanocomposite in optoelectronic applications.
PolymerNanofillerProperty/ApplicationRef.
PolythiopheneFullereneOLED device,
photoluminescence,
oxygen sensitivity		[56]
Poly(3,4-ethylenedioxythiophene):polystyrene sulfonateFullereneOLED device,
energetic barrier,
hole extraction		[57]
Polycyclopenta-dithiophene-benzothiadiazoleFullereneOLED device,
energetic barrier,
hole extraction		[58]
Poly(3,4-ethylenedioxythiophene):polystyrene sulfonateFullereneLED,
power conversion efficiency 3.1% (AM 1.5 irradiation),
luminance of 8000 cd/m2		[59]
Poly(3-hexylthiophene-2,5-diyl):[6,6]-penyl-C61-butyric-acid-methyl-esterFullereneBulk heterojunction solar cell,
power conversion efficiency,
solar cell efficiency ~3.5%,
electron transport,
interface formation		[76]
Poly(3-hexylthiophene):[6,6]-phenyl C61-butyric acid methyl esterFullereneOptical micrographs,
PCBM domains <200		[77]
Poly(methyl methacrylate)FullerenePhotovoltaic device,
power conversion efficiency 1.15%,
short-circuit current density
3.93 mA/cm2
open-circuit voltage 506 mV,
fill factor 0.59		[78]
Poly(3-hexylthiophene):(6,6)-phenyl-C61-butyric acid methyl esterFullerenePower conversion efficiency 1.92%[82]
PolymerFullerenePower conversion efficiency >17%[85]
Poly(methyl methacrylate)FullereneOptical sensor,
fluorescence intensity 260–373 K		[111]
PolymerFullereneBisphenol A detection limit 3.7 nM[112]
Porphyrin–diazocine–porphyrinFullereneOptical sensor,
dopamine,
detection limit 0.015 μM		[113]
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Kausar, A.; Ahmad, I.; Maaza, M.; Eisa, M.H.; Bocchetta, P. Polymer/Fullerene Nanocomposite for Optoelectronics—Moving toward Green Technology. J. Compos. Sci. 2022, 6, 393. https://doi.org/10.3390/jcs6120393

AMA Style

Kausar A, Ahmad I, Maaza M, Eisa MH, Bocchetta P. Polymer/Fullerene Nanocomposite for Optoelectronics—Moving toward Green Technology. Journal of Composites Science. 2022; 6(12):393. https://doi.org/10.3390/jcs6120393

Chicago/Turabian Style

Kausar, Ayesha, Ishaq Ahmad, Malik Maaza, M. H. Eisa, and Patrizia Bocchetta. 2022. "Polymer/Fullerene Nanocomposite for Optoelectronics—Moving toward Green Technology" Journal of Composites Science 6, no. 12: 393. https://doi.org/10.3390/jcs6120393

APA Style

Kausar, A., Ahmad, I., Maaza, M., Eisa, M. H., & Bocchetta, P. (2022). Polymer/Fullerene Nanocomposite for Optoelectronics—Moving toward Green Technology. Journal of Composites Science, 6(12), 393. https://doi.org/10.3390/jcs6120393

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