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Article

Decoration of Poly-3-methyl Aniline with As(III) Oxide and Hydroxide as an Effective Photoelectrode for Electroanalytical Photon Sensing with Photodiode-like Behavior

by
Mohamed Rabia
1,
Asmaa M. Elsayed
2 and
Maha Abdallah Alnuwaiser
3,*
1
Nanomaterials Science Research Laboratory, Chemistry Department, Faculty of Science, Beni-Suef University, Beni-Suef 62514, Egypt
2
TH-PPM Group, Physics Department, Faculty of Science, Beni-Suef University, Beni-Suef 62514, Egypt
3
Department of Chemistry, College of Science, Princess Nourah bint Abdulrahman University, P.O. Box 84428, Riyadh 11671, Saudi Arabia
*
Author to whom correspondence should be addressed.
Micromachines 2023, 14(8), 1573; https://doi.org/10.3390/mi14081573
Submission received: 7 June 2023 / Revised: 17 July 2023 / Accepted: 18 July 2023 / Published: 9 August 2023
(This article belongs to the Special Issue Electrochemical Capacitors and Photovoltaic Applications)
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Versions Notes

Abstract

:
This study achieved the decoration of poly-3-methyl aniline (P3MA) with As2O3–As(OH)3 using K2S2O8 and NaAsO2 on the 3-methyl aniline monomer. This resulted in a highly porous nanocomposite polymer composite with wide absorption optical behavior, an average crystalline size of 22 nm, and a 1.73 eV bandgap. The photoelectrode exhibited a great electrical response for electroanalytical applications, such as photon sensing and photodiodes, with a Jph of 0.015 mA/cm2 and Jo of 0.004 mA/cm2. The variable Jph values ranged from 0.015 to 0.010 mA/cm2 under various monochromatic filters from 340 to 730 nm, which demonstrates high sensitivity to wavelengths. Effective photon numbers were calculated to be 8.0 × 1021 and 5.6 × 1021 photons/s for these wavelength values, and the photoresponsivity (R) values were 0.16 and 0.10 mA/W, respectively. These high sensitivities make the nanocomposite material a promising candidate for use in photodetectors and photodiodes, with potential for commercial applications in highly technological systems and devices. Additionally, the material opens up possibilities for the development of photodiodes using n- and p-type materials.

1. Introduction

The relationship between energy and photon sensing is considered at its highest level under the great reduction in nonrenewable energy sources and the need for renewable resources. Under the rapid development of the industrial revolution, the demand for energy increased dramatically, the population increased, and the need for light sensing increased because of vital human activities [1,2]. The demand for friendly and renewable energy has remained a priority for industrialized countries, which has led to the development of many technologies, such as solar energy controlled through the use of photon sensors. Photon intensity and wavelength detection are applied in energy fields such as solar-powered photovoltaic scattering of water for proton (hydrogen) production and low carbon dioxide for fuel production, which has become a significant research field due to the promise of solar energy harvesting and storage in the form of chemical energy. A new alternative to photoelectrode systems inside complex technological systems for the detection and control of light in a wide range of optical regions depends on the optical properties of the nanomaterials/semiconductors [3,4]. III–V semiconductors are commonly used for efficient photovoltaic applications because of their direct beam vacuum, high absorbance of sunlight, high electron mobility, and controlled crystal evolution [5,6,7]. Under light radiation, photoinduced electrons and holes represent the sensitivity of nanomaterials to photon detection [8,9].
Another way to increase electrode efficiency is to use materials with great morphologies to capture light, in which most of nanoscale materials with porous morphologies have great capability for light sensing with high detectivity [10,11]. Moreover, one of the main reasons for using photovoltaic detection materials is to reduce the total production cost. From semiconducting inorganic compounds (groups III–V, Si, etc.), transition element oxides (BiVO4, Fe2O3, TiO2, and Cu2O), sulfides (NiS and CdS), acacinitrides (BaNbO2N), and chalcogenides that are prepared under controlled nanoscale morphologies are the most used materials for this purpose [12,13,14,15].
The preparation of photoelectrodes from polymers is less complex and more suitable for the production of large-scale devices than electrodes based on inorganic materials only. A distinctive property of polymers is that the positions of the bonds can be easily adjusted, unlike inorganic ones. Moreover, polymeric photoelectrodes have high optical absorption. Recently, metal oxide/polymer nanocomposites have demonstrated promising behavior for light detection due to its attractive photocatalytic properties, which combine the optical properties of the composite materials [16].
As2O3 is indeed a highly stable oxide that is recommended for application within various devices involved in light sensing and current control. Its exceptional stability allows it to exhibit light absorbance across a wide optical region, enabling the capture of a significant number of photons within this range [17]. This absorbance property makes As2O3 suitable for capturing and detecting energy photons, thus making it ideal for a range of optoelectronic applications and energy conversion development [18].
The high light absorbance exhibited by As2O3 when subjected to incident illumination further enhances its light-sensing capabilities. This characteristic is expected to enables the material to effectively sense and measure the number of photons in different optical regions during its application as a photoelectrode. Consequently, As2O3 demonstrates a fast response to light, allowing for quick detection and response times, which is advantageous for applications that require rapid light capture.
While As2O3 exhibits semiconducting properties, it is expected to have a small or negligible dark current (Jo) value. This implies that the ratio of the desired signal to unwanted noise, known as the signal-to-noise ratio, is highly promising in photodetectors based on As2O3. The low dark current contributes to improved sensitivity and ensures that the detected light signal stands out prominently against background noise.
Combining these advantages, including light sensitivity, stability, and cost-effectiveness, As2O3 has emerged as a highly promising material for use in optoelectronic systems [17]. Its ability to efficiently capture and sense light, coupled with its low cost and stable characteristics, positions it as a favorable candidate for a wide range of applications in optoelectronics, where precise light sensing and energy conversion are vital. Ongoing research and development continue to explore and optimize the use of As2O3 in optoelectronic systems, further expanding its potential for various applications.
Recent studies have attempted to improve the efficiency of photodetector and photodiode devices that are evaluated by electrical measurements, but the achieved Jph values still have significant drawbacks. For example, Bai et al. [19] achieved 107 µA with a ZnO/CuO nanocomposite, while Costas et al. [20] achieved only 0.1 nA. Graphene/P3HT was also investigated in previous studies [21], but the achieved Jph values were too limited for practical photodetector applications.
In this context, a new photoelectrode made of P3MA decorated with As2O3–As(OH)3 was developed and analyzed for its potential as a photodetector and photodiode. The Jph and Jo values were estimated under various monochromatic light and dark/light conditions, demonstrating the efficiency (R) and detectivity (D) of the photoelectrode. Additionally, the linear dynamic range was calculated, indicating the ability of the photoelectrode to convert photons into current. Overall, this photoelectrode shows great promise for optical applications due to its high response to incident photons.

2. Experimental Section

2.1. Materials and Characterization

Sodium arsenate (NaAsO2) and 3-methyl aniline were purchased from Merck Co., Ltd., Darmstadt, Germany. K2S2O8 was obtained from Pio-Chem Co., Egypt. Dimethylformamide was sourced from Sigma-Aldrich Co., Ltd., St. Louis, MO, USA.
The nanomaterials are characterized using several techniques to study their properties thoroughly. TEM (JEOL, Tokyo, Japan) was used to obtain 2D images, while SEM (ZEISS, Jena, Germany) was used to obtain 3D topography. XRD (PANalytical Pro, Waltham, MA, USA) was used to determine the peak position at 2-theta, and XPS (Kratos Aanl, London, UK) was used to determine the electron volt positions for the peaks through the photoelectron for elemental determination. FTIR (Bruker, Billerica, MA, USA) was used to confirm the functional groups, while the optical properties were observed using a Birkin Elmer spectrophotometer to measure the absorbance behavior.

2.2. P3MA Preparation

The P3MA was prepared by oxidatively polymerizing 3-methyl aniline with K2S2O8. The monomer and oxidant were present at concentrations of 0.12 and 0.15 M, respectively. An acid medium and dopant were used during the polymerization, which was achieved using 0.5 M HCl. The HCl was used to dissolve the polymer and improve its conductivity.

2.3. As2O3–As(OH)3/P3MA Optoelectronic and Photodiode Preparation

The As2O3–As(OH)3/P3MA nanocomposite was prepared by carrying out the oxidative polymerization of 3-methyl aniline with 0.07 M K2S2O8 in the presence of 0.15 M NaAsO2 at room temperature. This led to the formation of a dark green polymer film on glass, which was then purified through centrifugation to obtain the As2O3/P3MA nanocomposite.
In our photodiode preparation, we utilized a previously prepared thin film of polypyrrole (Ppy) [22]. This Ppy thin film was deposited as a p-type material. Subsequently, we deposited a thin film of the As2O3–As(OH)3/P3MA nanocomposite, which served as an n-type material in the photodiode structure. This combination of materials allowed for the formation of an efficient photodiode with complementary p–n junction characteristics, paraphrasing.

2.4. The Electrical Study

The electrical study of the As2O3–As(OH)3/P3MA nanocomposite film for electro-analytical photon detection under various light conditions or wavelengths was carried out using the CHI608E device. The current density in light (Jph) or dark (Jo) was evaluated, and the As2O3/P3MA nanocomposite film was contacted on both sides with the CHI device through silver paste. The efficacy of the prepared film to the light was evaluated using a metal halide lamp as a photon source, and the photon sensitivity was considered the main factor. The incidence light wavelengths or intensities were well controlled using an optical filter.

3. Results and Discussion

3.1. Analyses

The XRD analysis of the P3MA and As2O3–As(OH)3/P3MA nanocomposite is shown in Figure 1a. The P3MA exhibited amorphous behavior, as evidenced by the broad peaks observed. In contrast, the As2O3–As(OH)3/P3MA composite showed sharp peaks, indicating the formation of crystalline structures of both P3MA and inorganic materials (As2O3–As(OH)3). The peak observed at 21.0° for P3MA indicates that the polymer exhibited additional crystalline behavior after the composite formation. Furthermore, the peaks observed at 26.6°, 28.4°, 31.8°, 34.5°, and 45.5° in the growth directions (220), (222), (400), (311), and (440), respectively, are attributed to the As2O3 material [23]. However, the XRD analyses did not reveal much about As(OH)3, as these materials typically exhibit amorphous behavior [24,25]. The crystalline size (D) of this composite was evaluated using Scherrer’s equation (Equation (1)) by considering the highest peaks at the 331-growth direction (2-theta, Bragg angle = 34.5°) and the half maximum of the peak (W). Based on this calculation, the D value is 22 nm.
D = 0.9λ/W cosθ
The FTIR spectroscopy in Figure 1b was used to identify the materials based on their band positions in cm−1. For P3MA (black curve), the bands at 3408, 1727, 1480, and 1206 cm−1 correspond to the N–H, C–C, C=C, and C–N groups, respectively [26]. The bands at 1103 and 869 cm−1 are characteristic of C–H groups. The composite As2O3–As(OH)3/P3MA (red curve) showed similar bands to those of P3MA, but with some red shifts, indicating the interaction with As2O3–As(OH)3 [27,28,29]. Moreover, a noticeable enhancement was observed in the peak at 3410 cm−1 for O–H groups, alongside the N–H groups of the polymer.
The optical behavior of P3MA (black curve) and the As2O3–As(OH)3/P3MA composite (red curve) was analyzed, as shown in Figure 1c. The addition of As2O3–As(OH)3 to P3MA caused a significant increase in optical absorbance, which was observed in the intensities of the peaks and the coverage of the optical regions from UV to near IR spectra. This indicates that the composite has a wide photon-sensing ability that affects the electron transition in the optical regions of UV and visible light. Based on this optical behavior, the composite has potential for use in light sensing and various optical applications across a wide spectrum.
Using the theoretical Tauc equation (Equation (2)) [22,30,31], which relates the absorption coefficient of a material to the photon energy, the bandgap energy (Eg) can be demonstrated using α and ν, which is the absorption coefficient and frequency correspondingly (Figure 1d):
(αhν)0.5 = A(hν − Eg)
From this equation and figure, the estimated Eg is 2.42 and 1.73 eV for P3MA and the As2O3–As(OH)3/P3MA composite, respectively.
This reduction in the bandgap value for the composite indicates the increase in the photon absorption ability of the composite. This also suggests that the insertion of As2O3–As(OH)3 into P3MA provided a good charge transfer from the inorganic materials to the polymer matrix. The bandgap reduction also indicates the suitability of the composite for applications related to optoelectronics: Solar cells, photocatalysts, and optical sensors [32,33].
The topography of both P3MA and the As2O3–As(OH)3/P3MA nanocomposite was characterized using SEM, TEM, and theoretical roughness estimation, as shown in Figure 2. SEM analysis revealed a noticeable difference in morphology between P3MA and As2O3–As(OH)3/P3MA. P3MA exhibited nonuniform particles with an average length of 100 nm, whereas the As2O3–As(OH)3/P3MA nanocomposite displayed a well-connected network of fine particles forming a porous structure. Each particle in the nanocomposite had an average length of 20 nm, and there were instances of particle agglomeration, forming larger particles (300 nm). The TEM image in Figure 2c further confirm this observation, with the dark regions indicating the presence of the inorganic material As2O3–As(OH)3 and the faint regions representing the polymer matrix in which these particles were embedded.
The surface cross-section and roughness are evaluated theoretically with the Gwydion program. The nonuniform shape of P3MA was evident in the roughness estimation, while the highly distinct particles of the As2O3–As(OH)3/P3MA nanocomposite were clearly identified.
Chemical analysis of the As2O3–As(OH)3//P3MA nanocomposite was performed using XPS, and the results are presented in Figure 3a for the overall chemical survey and in Figure 3b specifically for the As3d spectra. The As3d spectrum showed a peak position at 45 eV, indicating the presence of As(III) in the nanocomposite. The O1s spectrum appeared at 532 eV, confirming the presence of oxygen in the composite as illustrated in Figure 3c. The C and N 1s spectra, representing the elements related to the polymer, were observed at 285 and 400 eV, respectively, as demonstrated in Figure 3d,e, respectively. Additionally, the presence of the Cl element from the HCl acid used during the synthesis was detected at 199 eV. These XPS results provide evidence for the formation of the As2O3–As(OH)3//P3MA nanocomposite, with the presence of As(III) and other relevant elements.

3.2. Electrical Measurements

The As2O3–As(OH)3/P3MA composite has been shown to have promising optical properties that make it suitable for use in photodetectors, particularly for detecting light intensity using electroanalytical photon intensity determination. This process involves studying the current–voltage relationship, where the current density (Jph) is observed under light or an optical filter and compared to the current density (Jo) in the dark. The difference between these values indicates the potential application of the photodiode, which involves electron transfer between n- and p-type materials. CHI608E is used for all of these electrical studies, which applies potential and registers the produced current values through the photo-generated carriers that contribute to the total current. Halide lamps serve as the photon sources for these experiments.
The results of the electrical measurements demonstrate that the As2O3–As(OH)3/P3MA composite has a high response to photons, as indicated by the significant difference between the Jph (0.015 mA.cm−2) and Jo (0.004 mA.cm−2) values under light and dark conditions, respectively (Figure 4a). This behavior is for the generated hot electrons upon photon absorption and clouded on the active sites of the material and provides a high Jph value (at a voltage bias of 2.0 V). The low Jo value reflects that the material can prevent current flow in the dark and generate electricity in the circuit in the presence of light, recommending this material as a promising candidate for photodiode applications. The on/off chopped light experiment further demonstrates the sensitivity of the material to light and the corresponding change in Jph values (Figure 4b). Therefore, the Jph value can be used to evaluate the sensitivity or efficiency of the material for photon capture and detection.
The As2O3/As(OH)3/P3MA nanocomposite film photoelectrode demonstrated high sensitivity to incident light intensity and wavelength, as shown in Figure 5a,b. The current–voltage relationship in Figure 5a shows that photosensitivity increases as the incidence light wavelengths decreased from 730 to 340 nm, which correlates to an increase in the produced Jph values. The small Jph value of 1.73 eV, calculated previously from Figure 1d, is promising and smaller than the normal visible bandgap from 1.95 to 3.26 eV. This indicates that the photodetector or photodiode device has the ability to sense light through the electron transition from the lower to the upper conducting level.
The bandgap value of the As2O3/As(OH)3/P3MA nanocomposite is considered promising for the efficient utilization of sunlight in the Vis and IR regions. The large percentage of sunlight present in these regions makes the nanocomposite well suited for capturing solar energy. Researchers in the field aim to achieve an optimal device system by carefully controlling the bandgap value of the nanocomposite.
One notable advantage of the As2O3/As(OH)3/P3MA nanocomposite is its cost-effectiveness and suitability for mass production. Its preparation on normal slide glass further contributes to its affordability. This low-cost nature of the device makes it appealing for both technical and commercial applications. It can function as a photodetector or photodiode, enabling the detection of light and control of current flow.
This dual advantage of the As2O3/As(OH)3/P3MA nanocomposite poses a significant challenge for many researchers in the field. They strive to design and optimize devices that possess both light detection capabilities and the ability to regulate current flow. Meeting this challenge opens up opportunities for various applications, ranging from renewable energy harvesting to sensing and optoelectronic systems.
The technical and commercial viability of a low-cost, high-performance device that can detect light and regulate current flow is a desirable goal. By leveraging the advantages of the As2O3/As(OH)3/P3MA nanocomposite, researchers aim to contribute to the advancement of both scientific understanding and practical applications in the field of photodetection and photodiodes.
The As2O3/As(OH)3/P3MA nanocomposite film operates through two steps, starting with the absorption of photons to generate hot electrons that transition to the upper level. These hot electrons then form clouds that collect on the surface of the inorganic materials, producing the Jph values that are measured. Equation (3) [34] estimates the number of photons absorbed under full wavelength illumination, which is 8.0 × 1021 photons/s. By analyzing the Jph values produced at various wavelengths, the effective photon number that produced the hot electrons can be estimated, which decreases from 8.0 × 1021 photons/s to 4.8 × 1021 photons/s from 340 to 540 nm. With the Jph value increasing to 0.01 at 730 nm, the estimated effective photons become 5.6 × 1021 photons/s. The results show that the As2O3/As(OH)3/P3MA nanocomposite film can electroanalytically evaluate the wavelengths or intensities of incident photons with high sensitivity across a broad optical spectra from near IR to UV. Additionally, this estimation provides a way to evaluate the photodiode’s performance at these wavelengths.
N = λ P / hc
The operation of the photodiode device involves the interaction of light with the various layers and materials within the device structure. Each wavelength of light corresponds to a specific frequency and energy, which can have different effects on the photodiode. In the case of the n-layer As2O3/As(OH)3/P3MA, the incident light interacts with this layer, causing the generation of photoelectrons. These photoelectrons are created by the absorption of light energy, which promotes the production of photoactive electrons and holes.
The generated photoelectrons are collected on the surface of the n-layer. Due to the potential difference applied within the device [35], these photoelectrons can easily migrate toward the neighboring P-type layer (Ppy), which contains a higher concentration of holes. This migration of photoelectrons is driven by the potential gradient within the device.
Similarly, the holes in the P-type layer can also migrate under the influence of the applied potentials. These holes can move toward the n-type nanocomposite layer, which typically has a higher concentration of electrons. This movement of holes is facilitated by the potential difference within the device.
All of these transitions and movements of photoelectrons and holes are primarily motivated by the effect of incident light on the photodiode. The absorption of light and the subsequent generation of electron–hole pairs initiate a series of charge carrier movements within the device, enabling the detection and conversion of light into electrical signals. It is worth noting that the specific materials and device structure (As2O3/As(OH)3/P3MA nanocomposite and Ppy) illustrate unique properties and characteristics that contribute to the overall performance of the photodiode in response to light.
The sensitivity of the As2O3/As(OH)3/P3MA nanocomposite photoelectrode was estimated using the linear dynamic range (LDR) for the photoelectrode, which was calculated using Equation (4). The LDR value of 36 dB in the UV region indicates that the photoelectrode has a high photosensitivity and can accurately detect light intensities ranging from the minimum detectable level to 36 dB above that level without saturation or distortion. This value suggests that the photoelectrode is highly responsive to incident photons in the UV region and can provide a reliable and linear response across a wide range of light intensities.
Furthermore, this LDR value is promising because it implies that the photoelectrode can be synthesized using cost-effective and readily available materials. This suggests that the development of light detection systems based on such photoelectrodes can be cost-efficient while still offering excellent sensitivity and linearity. This suggests that the photoelectrode has great potential for use in electroanalytical light estimation for photodiode applications. In other words, the LDR value is a measure of the photoelectrode’s ability to detect and respond to light, and the high value obtained in this study indicates a promising application in photodiodes.
LDR = 20 . log ( J ph   J o )
Equation (5) [36] was used to estimate the sensitivity of the prepared As2O3/As(OH)3/P3MA nanocomposite photoelectrode by taking into account the R values, which convert incident photons into an electrical signal on the surface area of the photoelectrode (S). Figure 6a shows the R values under a wide optical region, where the optimum value of 0.16 mA·W−1 was observed at 340 nm, and it decreased to 0.10 mA·W−1 in the IR region. This high R value over a wide optical spectra, combined with the high photoresponsivity, suggests that this material or device is efficient at converting photons into electrical charge, making it desirable for applications such as photodetectors and photodiodes.
  R = J ph −   J d P . S
The sensitivity of a photodetector or a photodiode to weak optical signals can be evaluated by calculating the D values at various wavelengths, as shown in Equation (6) and Figure 6b. Similarly, the fabricated As2O3/As(OH)3/P3MA nanocomposite photoelectrode exhibited high sensitivity in the UV region, with decreasing sensitivity at longer wavelengths. The optimal D value was 3.7 × 107 Jones at 340 nm, while the smallest value was 2.4 × 107 Jones at 730 nm. To further confirm the promising results of this photoelectrode and its potential for use in photodetectors and photodiodes for commercial applications in highly technological systems and devices, Table 1 compares these results with those of previous studies.
D = R   S   / 2   e   J o  

4. Conclusions

This study described the synthesis of a nanocomposite photoelectrode by decorating poly-3-methyl aniline with As2O3/As(OH)3. The resulting material had a wide bandgap of 1.73 eV, a porous structure, and an average crystalline size of 22 nm. The photoelectrode showed promising electrical properties with a high sensitivity to different wavelengths, making it suitable for electroanalytical applications as a photodetector or photodiode. The values of Jph and Jo were found to be 0.015 and 0.004 mA·cm−2, respectively, and the effective photon numbers were calculated to be 8.0 × 1021 and 5.6 × 1021 photons/s for wavelengths ranging from 340 to 730 nm. The R values were found to be 0.16 and 0.10 mA·W−1 for the same wavelength range. The high sensitivity of this nanocomposite material indicates its potential for use in highly technological systems and devices.

Author Contributions

Writing and supervision were performed by M.R. and M.A.A.; the experiment was performed by M.R. and A.M.E. All authors have read and agreed to the published version of the manuscript.

Funding

This research was funded by the Princess Nourah bint Abdulrahman University Researchers Supporting Project (number PNURSP2023R186), Princess Nourah bint Abdulrahman University, Riyadh, Saudi Arabia.

Data Availability Statement

All data generated or analyzed during this study are included in this article.

Acknowledgments

This research was funded by the Princess Nourah bint Abdulrahman University Researchers Supporting Project (number PNURSP2023R186), Princess Nourah bint Abdulrahman University, Riyadh, Saudi Arabia.

Conflicts of Interest

The authors have no conflict of interest.

References

  1. Qin, Z.; She, Z.; Chen, C.; Wu, W.; Lau, J.K.Y.; Ip, N.Y.; Qu, J.Y. Deep Tissue Multi-Photon Imaging Using Adaptive Optics with Direct Focus Sensing and Shaping. Nat. Biotechnol. 2022, 40, 1663–1671. [Google Scholar] [CrossRef] [PubMed]
  2. Shafique, S.; Yang, S.; Wang, Y.; Woldu, Y.T.; Cheng, B.; Ji, P. High-Performance Photodetector Using Urchin-like Hollow Spheres of Vanadium Pentoxide Network Device. Sens. Actuators A Phys. 2019, 296, 38–44. [Google Scholar] [CrossRef]
  3. Proppe, A.H.; Berkinsky, D.B.; Zhu, H.; Šverko, T.; Kaplan, A.E.K.; Horowitz, J.R.; Kim, T.; Chung, H.; Jun, S.; Bawendi, M.G. Highly Stable and Pure Single-Photon Emission with 250 Ps Optical Coherence Times in InP Colloidal Quantum Dots. Nat. Nanotechnol. 2023, 2023, 1–7. [Google Scholar] [CrossRef] [PubMed]
  4. Xing, Z.; Akter, A.; Kum, H.S.; Baek, Y.; Ra, Y.H.; Yoo, G.; Lee, K.; Mi, Z.; Heo, J. Mid-Infrared Photon Sensing Using InGaN/GaN Nanodisks via Intersubband Absorption. Sci. Rep. 2022, 12, 4301. [Google Scholar] [CrossRef]
  5. Meng, Y.; Feng, J.; Han, S.; Xu, Z.; Mao, W.; Zhang, T.; Kim, J.S.; Roh, I.; Zhao, Y.; Kim, D.H.; et al. Photonic van Der Waals Integration from 2D Materials to 3D Nanomembranes. Nat. Rev. Mater. 2023, 2023, 1–20. [Google Scholar] [CrossRef]
  6. Essig, S.; Allebé, C.; Remo, T.; Geisz, J.F.; Steiner, M.A.; Horowitz, K.; Barraud, L.; Ward, J.S.; Schnabel, M.; Descoeudres, A.; et al. Raising the One-Sun Conversion Efficiency of III–V/Si Solar Cells to 32.8% for Two Junctions and 35.9% for Three Junctions. Nat. Energy 2017, 2, 17144. [Google Scholar] [CrossRef]
  7. Lin, T.N.; Santiago, S.R.M.S.; Zheng, J.A.; Chao, Y.C.; Yuan, C.T.; Shen, J.L.; Wu, C.H.; Lin, C.A.J.; Liu, W.R.; Cheng, M.C.; et al. Enhanced Conversion Efficiency of III–V Triple-Junction Solar Cells with Graphene Quantum Dots. Sci. Rep. 2016, 6, 39163. [Google Scholar] [CrossRef] [Green Version]
  8. Elsayed, A.M.; Rabia, M.; Shaban, M.; Aly, A.H.; Ahmed, A.M. Preparation of Hexagonal Nanoporous Al2O3/TiO2/TiN as a Novel Photodetector with High Efficiency. Sci. Rep. 2021, 11, 17572. [Google Scholar] [CrossRef]
  9. Hadia, N.M.A.; Shaban, M.; Mohamed, S.H.; Al-Ghamdi, A.F.; Alzaid, M.; Elsayed, A.M.; Mourad, A.H.I.; Amin, M.A.; Boukherroub, R.; Abdelazeez, A.A.A.; et al. Highly Crystalline Hexagonal PbI2 Sheets on Polyaniline/Antimony Tin Oxide Surface as a Novel and Highly Efficient Photodetector in UV, Vis, and near IR Regions. Polym. Adv. Technol. 2022, 33, 3977–3987. [Google Scholar] [CrossRef]
  10. Bakulin, A.A.; Neutzner, S.; Bakker, H.J.; Ottaviani, L.; Barakel, D.; Chen, Z. Charge Trapping Dynamics in PbS Colloidal Quantum Dot Photovoltaic Devices. ACS Nano 2013, 7, 8771–8779. [Google Scholar] [CrossRef] [Green Version]
  11. Li, Y.; An, N.; Lu, Z.; Wang, Y.; Chang, B.; Tan, T.; Guo, X.; Xu, X.; He, J.; Xia, H.; et al. Nonlinear Co-Generation of Graphene Plasmons for Optoelectronic Logic Operations. Nat. Commun. 2022, 13, 3138. [Google Scholar] [CrossRef] [PubMed]
  12. Khan, S.; Primavera, B.A.; Chiles, J.; McCaughan, A.N.; Buckley, S.M.; Tait, A.N.; Lita, A.; Biesecker, J.; Fox, A.; Olaya, D.; et al. Superconducting Optoelectronic Single-Photon Synapses. Nat. Electron. 2022, 5, 650–659. [Google Scholar] [CrossRef]
  13. Asahi, S.; Teranishi, H.; Kusaki, K.; Kaizu, T.; Kita, T. Two-Step Photon up-Conversion Solar Cells. Nat. Commun. 2017, 8, 14962. [Google Scholar] [CrossRef] [Green Version]
  14. Fu, J.; Fan, Z.; Nakabayashi, M.; Ju, H.; Pastukhova, N.; Xiao, Y.; Feng, C.; Shibata, N.; Domen, K.; Li, Y. Interface Engineering of Ta3N5 Thin Film Photoanode for Highly Efficient Photoelectrochemical Water Splitting. Nat. Commun. 2022, 13, 729. [Google Scholar] [CrossRef]
  15. Shaban, M.; Rabia, M.; El-Sayed, A.M.A.; Ahmed, A.; Sayed, S. Photocatalytic Properties of PbS/Graphene Oxide/Polyaniline Electrode for Hydrogen Generation. Sci. Rep. 2017, 7, 14100. [Google Scholar] [CrossRef] [PubMed] [Green Version]
  16. Chen, H.; Yu, P.; Zhang, Z.; Teng, F.; Zheng, L.; Hu, K.; Fang, X.; Chen, H.Y.; Yu, P.P.; Teng, F.; et al. Ultrasensitive Self-Powered Solar-Blind Deep-Ultraviolet Photodetector Based on All-Solid-State Polyaniline/MgZnO Bilayer. Small 2016, 12, 5809–5816. [Google Scholar] [CrossRef] [PubMed]
  17. Acikgoz, S.; Yungevis, H. Controlled Electrochemical Growth of Micro-Scaled As2O3 and Ga2O3 Oxide Structures on p-Type Gallium Arsenide. Appl. Phys. A Mater. Sci. Process. 2022, 128, 824. [Google Scholar] [CrossRef]
  18. Abdullahi, Y.Z.; Caglayan, R.; Mogulkoc, A.; Mogulkoc, Y.; Ersan, F. New Stable Ultrawide Bandgap As2O3 Semiconductor Materials. J. Phys. Mater. 2023, 6, 025003. [Google Scholar] [CrossRef]
  19. Bai, Z.; Zhang, Y. Self-Powered UV–Visible Photodetectors Based on ZnO/Cu2O Nanowire/Electrolyte Heterojunctions. J. Alloys Compd. 2016, 675, 325–330. [Google Scholar] [CrossRef]
  20. Costas, A.; Florica, C.; Preda, N.; Apostol, N.; Kuncser, A.; Nitescu, A.; Enculescu, I. Radial Heterojunction Based on Single ZnO-CuxO Core-Shell Nanowire for Photodetector Applications. Sci. Rep. 2019, 9, 5553. [Google Scholar] [CrossRef] [Green Version]
  21. Tan, W.C.; Shih, W.H.; Chen, Y.F. A Highly Sensitive Graphene-Organic Hybrid Photodetector with a Piezoelectric Substrate. Adv. Funct. Mater. 2014, 24, 6818–6825. [Google Scholar] [CrossRef]
  22. Hamid, M.M.A.; Alruqi, M.; Elsayed, A.M.; Atta, M.M.; Hanafi, H.A.; Rabia, M. Testing the Photo-Electrocatalytic Hydrogen Production of Polypyrrole Quantum Dot by Combining with Graphene Oxide Sheets on Glass Slide. J. Mater. Sci. Mater. Electron. 2023, 34, 831. [Google Scholar] [CrossRef]
  23. Bioud, Y.A.; Boucherif, A.; Belarouci, A.; Paradis, E.; Drouin, D.; Arès, R. Chemical Composition of Nanoporous Layer Formed by Electrochemical Etching of P-Type GaAs. Nanoscale Res. Lett. 2016, 11, 446. [Google Scholar] [CrossRef] [PubMed] [Green Version]
  24. Balayeva, O.O.; Azizov, A.A.; Muradov, M.B.; Alosmanov, R.M.; Eyvazova, G.M.; Mammadyarova, S.J. Cobalt Chromium-Layered Double Hydroxide, α- and β- Co(OH)2 and Amorphous Cr(OH)3: Synthesis, Modification and Characterization. Heliyon 2019, 5, e02725. [Google Scholar] [CrossRef]
  25. Zhang, W.; Yang, Y.; Li, F.; Song, G.; Shao, Y.; Ouyang, R.; Xu, L.; Li, W.; Miao, Y. A Newly Prepared Ni(OH)2@Cr(OH)3 Nanohybrid for Its Bioelectrocatalysis. Sens. Actuators B Chem. 2014, 198, 350–359. [Google Scholar] [CrossRef]
  26. Linganathan, P.; Sundararajan, J.; Samuel, J.M. Synthesis, Characterization, and Photoconductivity Studies on Poly(2-Chloroaniline) and Poly(2-Chloroaniline)/CuO Nanocomposites. J. Compos. 2014, 2014, 838975. [Google Scholar] [CrossRef]
  27. Trabelsi, A.B.G.; Essam, D.H.; Alkallas, F.M.; Ahmed, A.; Rabia, M. Petal-like NiS-NiO/G-C3N4 Nanocomposite for High-Performance Symmetric Supercapacitor. Micromachines 2022, 13, 2134. [Google Scholar] [CrossRef]
  28. Ben Gouider Trabelsi, A.; MElsayed, A.; HAlkallas, F.; Al-Noaimi, M.; Kusmartsev, F.V.; Rabia, M. A Fractal, Flower Petal-like CuS-CuO/G-C3N4 Nanocomposite for High Efficiency Supercapacitors. Coatings 2022, 12, 1834. [Google Scholar] [CrossRef]
  29. Rabia, M.; Essam, D.; Alkallas, F.H.; Shaban, M.; Elaissi, S.; Ben Gouider Trabelsi, A. Flower-Shaped CoS-Co2O3/G-C3N4 Nanocomposite for Two-Symmetric-Electrodes Supercapacitor of High Capacitance Efficiency Examined in Basic and Acidic Mediums. Micromachines 2022, 13, 2234. [Google Scholar] [CrossRef]
  30. Khalafalla, M.A.H.; Hadia, N.M.A.; Elsayed, A.M.; Alruqi, M.; El Malti, W.; Shaban, M.; Rabia, M. ATO/Polyaniline/PbS Nanocomposite as Highly Efficient Photoelectrode for Hydrogen Production from Wastewater with Theoretical Study for the Water Splitting. Adsorpt. Sci. Technol. 2022, 2022, 5628032. [Google Scholar] [CrossRef]
  31. Elsayed, A.M.; Alkallas, F.H.; Trabelsi, A.B.G.; AlFaify, S.; Shkir, M.; Alrebdi, T.A.; Almugren, K.S.; Kusmatsev, F.V.; Rabia, M. Photodetection Enhancement via Graphene Oxide Deposition on Poly 3-Methyl Aniline. Micromachines 2023, 14, 606. [Google Scholar] [CrossRef] [PubMed]
  32. Hwang, D.K.; Lee, Y.T.; Lee, H.S.; Lee, Y.J.; Shokouh, S.H.; Kyhm, J.H.; Lee, J.; Kim, H.H.; Yoo, T.H.; Nam, S.H.; et al. Ultrasensitive PbS Quantum-Dot-Sensitized InGaZnO Hybrid Photoinverter for near-Infrared Detection and Imaging with High Photogain. NPG Asia Mater. 2016, 8, e233. [Google Scholar] [CrossRef]
  33. Ding, H.; Lv, G.; Cai, X.; Chen, J.; Cheng, Z.; Peng, Y.; Tang, G.; Shi, Z.; Xie, Y.; Fu, X.; et al. An Optoelectronic Thermometer Based on Microscale Infrared-to-Visible Conversion Devices. Light Sci. Appl. 2022, 11, 130. [Google Scholar] [CrossRef] [PubMed]
  34. Shaban, M.; Ahmed, A.M.; Abdel-Rahman, E.; Hamdy, H. Tunability and Sensing Properties of Plasmonic/1D Photonic Crystal. Sci. Rep. 2017, 7, 41983. [Google Scholar] [CrossRef] [Green Version]
  35. Sulaman, M.; Yang, S.; Imran, A.; Zhang, Z.; Bukhtiar, A.; Ge, Z.; Song, Y.; Sun, F.; Jiang, Y.; Tang, L.; et al. Two Bulk-Heterojunctions Made of Blended Hybrid Nanocomposites for High-Performance Broadband, Self-Driven Photodetectors. ACS Appl. Mater. Interfaces 2023, 15, 25671–25683. [Google Scholar] [CrossRef]
  36. Noothongkaew, S.; Thumthan, O.; An, K.S. Minimal Layer Graphene/TiO2 Nanotube Membranes Used for Enhancement of UV Photodetectors. Mater. Lett. 2018, 218, 274–279. [Google Scholar] [CrossRef]
  37. Hong, Q.; Cao, Y.; Xu, J.; Lu, H.; He, J.; Sun, J.L. Self-Powered Ultrafast Broadband Photodetector Based on p-n Heterojunctions of CuO/Si Nanowire Array. ACS Appl. Mater. Interfaces 2014, 6, 20887–20894. [Google Scholar] [CrossRef]
  38. Chen, Z.; Ci, H.; Tan, Z.; Dou, Z.; Chen, X.-D.; Liu, B.; Liu, R.; Lin, L.; Cui, L.; Gao, P.; et al. Growth of 12-Inch Uniform Monolayer Graphene Film on Molten Glass and Its Application in PbI 2-Based Photodetector. Nano Res. 2019, 12, 1888–1893. [Google Scholar] [CrossRef]
  39. Ismail, R.A.; Mousa, A.M.; Shaker, S.S. Visible-Enhanced Silver-Doped PbI2 Nanostructure/Si Heterojunction Photodetector: Effect of Doping Concentration on Photodetector Parameters. Opt. Quantum Electron. 2019, 51, 362. [Google Scholar] [CrossRef]
  40. Lan, T.; Fallatah, A.; Suiter, E.; Padalkar, S. Size Controlled Copper (I) Oxide Nanoparticles Influence Sensitivity of Glucose Biosensor. Sensors 2017, 17, 1944. [Google Scholar] [CrossRef] [Green Version]
  41. Liu, K.; Sakurai, M.; Liao, M.; Aono, M. Giant Improvement of the Performance of ZnO Nanowire Photodetectors by Au Nanoparticles. J. Phys. Chem. C 2010, 114, 19835–19839. [Google Scholar] [CrossRef]
  42. Naldoni, A.; Guler, U.; Wang, Z.; Marelli, M.; Malara, F.; Meng, X.; Besteiro, L.V.; Govorov, A.O.; Kildishev, A.V.; Boltasseva, A.; et al. Broadband Hot-Electron Collection for Solar Water Splitting with Plasmonic Titanium Nitride. Adv. Opt. Mater. 2017, 5, 1601031. [Google Scholar] [CrossRef] [Green Version]
  43. Wang, S.B.; Hsiao, C.H.; Chang, S.J.; Lam, K.T.; Wen, K.H.; Hung, S.C.; Young, S.J.; Huang, B.R. A CuO Nanowire Infrared Photodetector. Sens. Actuators A Phys. 2011, 171, 207–211. [Google Scholar] [CrossRef]
Micromachines 14 01573 g001
Figure 1. The characterization analyses of P3MA (black curve) and the As2O3–As(OH)3/P3MA composite (red curve) through (a) XRD, (b) FTIR, (c) optical absorbance, and (d) the calculated band gap.
Figure 1. The characterization analyses of P3MA (black curve) and the As2O3–As(OH)3/P3MA composite (red curve) through (a) XRD, (b) FTIR, (c) optical absorbance, and (d) the calculated band gap.
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Figure 2. The SEM morphology of (a) P3MA and (b) the As2O3–As(OH)3/P3MA nanocomposite (with inserted magnified image). (c) TEM of the As2O3–As(OH)3/P3MA composite. Cross-section and roughness of (d) P3MA and (e) the As2O3–As(OH)3/P3MA nanocomposite.
Figure 2. The SEM morphology of (a) P3MA and (b) the As2O3–As(OH)3/P3MA nanocomposite (with inserted magnified image). (c) TEM of the As2O3–As(OH)3/P3MA composite. Cross-section and roughness of (d) P3MA and (e) the As2O3–As(OH)3/P3MA nanocomposite.
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Figure 3. The XPS survey of (a) the As2O3–As(OH)3/P3MA nanocomposite. The XPS of the individual elements (b) As (c) O, (d) C, and (e) N spectra.
Figure 3. The XPS survey of (a) the As2O3–As(OH)3/P3MA nanocomposite. The XPS of the individual elements (b) As (c) O, (d) C, and (e) N spectra.
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Figure 4. (a) The electrical study of the As2O3/As(OH)3/P3MA nanocomposite film through current–voltage under dark and light conditions and (b) the Jph value at 2.0 V.
Figure 4. (a) The electrical study of the As2O3/As(OH)3/P3MA nanocomposite film through current–voltage under dark and light conditions and (b) the Jph value at 2.0 V.
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Figure 5. (a) The electrical study of the As2O3/As(OH)3/P3MA nanocomposite photoelectrode through current–voltage under various monochromatic light conditions (340–730 nm) and (b) the Jph value at 2.0 V.
Figure 5. (a) The electrical study of the As2O3/As(OH)3/P3MA nanocomposite photoelectrode through current–voltage under various monochromatic light conditions (340–730 nm) and (b) the Jph value at 2.0 V.
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Figure 6. The study of the efficiency of the As2O3/As(OH)3/P3MA nanocomposite film through estimation of the (a) R and (b) D values under λ (340–730 nm).
Figure 6. The study of the efficiency of the As2O3/As(OH)3/P3MA nanocomposite film through estimation of the (a) R and (b) D values under λ (340–730 nm).
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Table 1. The study of the efficiency of the As2O3/As(OH)3/P3MA nanocomposite film through estimation of the definite wavelength R values.
Table 1. The study of the efficiency of the As2O3/As(OH)3/P3MA nanocomposite film through estimation of the definite wavelength R values.
StructureWavelength
(nm)		Bais (V)R
(mA·W−1)
Graphene/P3HT [21]3251NA
Polyaniline/MgZnO [16]25050.1
ZnO-CuO [20]40513 × 10−3
CuO/Si Nanowire [37]4050.23.8 × 10−3
PbI2-graphene [38]5502NA
PbI2-5%Ag [39]5326NA
GO/Cu2O [40]30020.5 × 10−3
ZnO/RGO [41]35051.3 × 10−3
ZnO/Cu2O [19]35024 × 10−3
TiN/TiO2 [42]5505-
CuO nanowires [43]3905-
ZnO/RGO [41]35051.3 × 10−3
As2O3/As(OH)3/P3MA (this work)44020.16
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Rabia, M.; Elsayed, A.M.; Alnuwaiser, M.A. Decoration of Poly-3-methyl Aniline with As(III) Oxide and Hydroxide as an Effective Photoelectrode for Electroanalytical Photon Sensing with Photodiode-like Behavior. Micromachines 2023, 14, 1573. https://doi.org/10.3390/mi14081573

AMA Style

Rabia M, Elsayed AM, Alnuwaiser MA. Decoration of Poly-3-methyl Aniline with As(III) Oxide and Hydroxide as an Effective Photoelectrode for Electroanalytical Photon Sensing with Photodiode-like Behavior. Micromachines. 2023; 14(8):1573. https://doi.org/10.3390/mi14081573

Chicago/Turabian Style

Rabia, Mohamed, Asmaa M. Elsayed, and Maha Abdallah Alnuwaiser. 2023. "Decoration of Poly-3-methyl Aniline with As(III) Oxide and Hydroxide as an Effective Photoelectrode for Electroanalytical Photon Sensing with Photodiode-like Behavior" Micromachines 14, no. 8: 1573. https://doi.org/10.3390/mi14081573

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