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23 pages, 4686 KiB  
Article
Measuring the Systemic Risk of Clean Energy Markets Based on the Dynamic Factor Copula Model
by Wensheng Wang and Rui Wang
Systems 2024, 12(12), 584; https://doi.org/10.3390/systems12120584 (registering DOI) - 21 Dec 2024
Abstract
This study is based on the stock returns of 11 subindustry markets in the international clean energy market from 2010 to 2024 and constructs a skewed t distribution dynamic factor copula model. The time-varying load factor is used to characterize the correlation between [...] Read more.
This study is based on the stock returns of 11 subindustry markets in the international clean energy market from 2010 to 2024 and constructs a skewed t distribution dynamic factor copula model. The time-varying load factor is used to characterize the correlation between a single subindustry market and the entire system, and the joint probability of distress is calculated as a measure of the overall level of systemic risk. Two indicators, Systemic Vulnerability Degree and Systemic Importance Degree, are introduced to evaluate the vulnerability of a single subindustry market in systemic risk and its contribution to systemic risk. A conditional risk-spillover index is constructed to measure the risk-spillover level between subindustry markets. This method fully considers the individual differences and inherent correlations of the international clean energy market subsectors, as well as the fat tail and asymmetry of returns, thus capturing more information and more timely information. This study found that the correlation between subindustry markets changes over time, and during the crisis, the market correlation shows a significant upward trend. In the measurement of the overall level of systemic risk, the joint probability of distress can identify the changes in systemic risk in the international clean energy market. The systemic risk of the international clean energy market presents the characteristics of rapid and multiple outbreaks, and the joint default risk probability of the whole system can exceed 0.6. The outbreak of systemic risk is closely related to a series of major international events, showing a strong correlation. In addition, the systemic vulnerability analysis found that the biofuel market has the lowest systemic vulnerability, and the advanced materials market has the highest vulnerability. The energy efficiency market is considered to be the most important market in the system. The advanced materials market and renewable energy market play a dominant role in the risk contribution to other markets, while the geothermal market, solar market, and wind energy market are net risk overflow parties in the tail risk impact, and the developer market and fuel cell market are net risk receivers. This study provides a theoretical basis for systemic risk management and ensuring the stability of the international clean energy market. Full article
30 pages, 3195 KiB  
Review
Conducting Polymers in Solar Cells: Insights, Innovations, and Challenges
by Aliya Yelshibay, Sherif Dei Bukari, Bakhytzhan Baptayev and Mannix P. Balanay
Organics 2024, 5(4), 640-669; https://doi.org/10.3390/org5040034 - 20 Dec 2024
Abstract
The pursuit of sustainable energy sources has led to significant advances in solar cell technology, with conducting polymers (CPs) emerging as key innovations. This review examines how CPs improve the performance and versatility of three important types of solar cells: dye-sensitized solar cells [...] Read more.
The pursuit of sustainable energy sources has led to significant advances in solar cell technology, with conducting polymers (CPs) emerging as key innovations. This review examines how CPs improve the performance and versatility of three important types of solar cells: dye-sensitized solar cells (DSSCs), perovskite solar cells (PSCs), and organic solar cells (OSCs). Polymers such as polyaniline, polypyrrole, and poly(3,4-ethylenedioxythiophene) have shown significant potential to increase the efficiency of solar cells. In DSSCs, conducting polymers act as counter electrodes, electrolytes, and dyes, contributing to improved efficiency and stability. In PSCs, they serve as hole transport materials and electron transport materials that improve charge separation and reduce recombination losses. In OSCs, conducting polymers act as HTMs and active layers, significantly impacting device performance and enabling advances in both binary and ternary solar cell configurations. Recent research highlights the important role of conducting polymers in improving both the efficiency and stability of solar cells under different indoor and outdoor lighting conditions. Recent advances have led to impressive energy conversion efficiencies, particularly in low-light environments. This report also highlights the environmental and economic benefits associated with these materials. At the same time, it highlights the challenges associated with optimizing the materials, scalability, and ensuring long-term stability. Future research directions are outlined to overcome these obstacles and promote the commercial viability of next-generation solar technologies. Full article
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<p>Comparison of power conversion efficiencies across different generations and types of solar cells. Data for first- and second-generation solar cells are sourced from [<a href="#B17-organics-05-00034" class="html-bibr">17</a>], while the PCE values for perovskite, dye-sensitized, and organic solar cells are obtained from references [<a href="#B14-organics-05-00034" class="html-bibr">14</a>,<a href="#B18-organics-05-00034" class="html-bibr">18</a>,<a href="#B20-organics-05-00034" class="html-bibr">20</a>], respectively.</p>
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<p>Various configurations of perovskite solar cells. (<b>a</b>) Mesoporous structure, (<b>b</b>) standard n-i-p configuration, and (<b>c</b>) p-i-n configuration. Adapted with permission from reference [<a href="#B30-organics-05-00034" class="html-bibr">30</a>]. Copyright (2022) the authors, some rights reserved; exclusive licensee MDPI. Distributed under a Creative Commons Attribution 4.0 International License (CC BY 4.0).</p>
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<p>Working principle of dye-sensitized solar cells. Adapted with permission [<a href="#B38-organics-05-00034" class="html-bibr">38</a>], copyright (2022) Springer Nature.</p>
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<p>Working principle of organic solar cell with (<b>a</b>) conventional and (<b>b</b>) inverted configurations. Adapted with permission [<a href="#B42-organics-05-00034" class="html-bibr">42</a>], copyright (2012) Royal Society of Chemistry.</p>
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<p>Chemical structures of common polymers used in solar cells.</p>
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<p>Common methods for synthesizing and fabricating conducting polymers.</p>
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<p>Chemical structures of the additives and acceptors discussed in this study.</p>
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<p>Chemical structures of PSMA and BCP5.</p>
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<p>Chemical structures of some of the conducting polymers used in dye-sensitized solar cells.</p>
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<p>Chemical structures of some of the conducting polymers used in perovskite solar cells.</p>
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<p>Chemical structures of some of the conducting polymers used in organic solar cells.</p>
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<p>Chemical structures of ProDOT-EDOT and n-PBDF.</p>
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14 pages, 26016 KiB  
Article
Electrodeposition of Nanostructured Metals on n-Silicon and Insights into Rhodium Deposition
by Giulio Pappaianni, Francesco Montanari, Marco Bonechi, Giovanni Zangari, Walter Giurlani and Massimo Innocenti
Nanomaterials 2024, 14(24), 2042; https://doi.org/10.3390/nano14242042 - 20 Dec 2024
Abstract
In this study, we investigate the electrodeposition of various metals on silicon. Mn, Co, Ni, Ru, Pd, Rh, and Pt were identified as promising candidates for controlled electrodeposition onto silicon. Electrochemical evaluations employing cyclic voltammetry, Scanning Electron Microscopy (SEM) associated with energy-dispersive X-Ray [...] Read more.
In this study, we investigate the electrodeposition of various metals on silicon. Mn, Co, Ni, Ru, Pd, Rh, and Pt were identified as promising candidates for controlled electrodeposition onto silicon. Electrochemical evaluations employing cyclic voltammetry, Scanning Electron Microscopy (SEM) associated with energy-dispersive X-Ray Spectroscopy (SEM-EDS), and X-Ray Photoelectron Spectroscopy (XPS) techniques confirmed the deposition of Pd, Rh, and Pt as nanoparticles. Multi-cycle charge-controlled depositions were subsequently performed to evaluate the possibility of achieving tunable electrodeposition of nanostructured rhodium on n-doped silicon. The procedure increased surface coverage from 9% to 84%, with the average particle size diameter ranging from 57 nm to 168 nm, and with an equivalent thickness of the deposits up to 43.9 nm, varying the number of charge-controlled deposition cycles. The electrodeposition of rhodium on silicon presents numerous opportunities across various scientific and technological domains, driving innovation and enhancing the performance of devices and materials used in catalysis, electronics, solar cells, fuel cells, and sensing. Full article
(This article belongs to the Special Issue Heterogeneous Integration Technology for More Moore)
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<p>Periodic table of elements highlighting the formation energy (eV/atom) with silicon; the metals used in this work are highlighted (nickel, ruthenium, palladium, rhodium, platinum, manganese, and cobalt).</p>
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<p>CVs performed in the potential range of −0.6 V to 0 V vs. Ag/AgCl/KCl (sat.), 10 mV/s scan rate, H<sub>2</sub>SO<sub>4</sub> 0.1 M solution (black scans), H<sub>2</sub>SO<sub>4</sub> 0.1 M, 1 mM metal solution, first metal solution scan (red), second metal solution scan (blue), and the third metal solution scans (green) relative to (<b>a</b>) Ni (NiSO<sub>4</sub>·6H<sub>2</sub>O); (<b>b</b>) Pd ([Pd(NH<sub>3</sub>)<sub>4</sub>]SO<sub>4</sub>); (<b>c</b>) Pt (K<sub>2</sub>PtCl<sub>4</sub>); (<b>d</b>) Rh (RhCl<sub>3</sub>·xH<sub>2</sub>O); and (<b>e</b>) Ru ([Ru(NH<sub>3</sub>)<sub>6</sub>]Cl<sub>3</sub>).</p>
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<p>SE-SEM images and EDS-SEM spectra of the Si working electrode after the cyclovoltammetry measurements in H<sub>2</sub>SO<sub>4</sub> 0.1 M, 1 mM metal solution relative to (<b>a</b>,<b>d</b>) 1 mM [Pd(NH<sub>3</sub>)<sub>4</sub>]SO<sub>4</sub> solution; (<b>b</b>,<b>e</b>) 1 mM K<sub>2</sub>PtCl<sub>4</sub> solution; (<b>c</b>,<b>f</b>) 1 mM RhCl<sub>3</sub> solution.</p>
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<p>SE-SEM images of the deposit obtained through charge-controlled deposition on the Si working electrode in H<sub>2</sub>SO<sub>4</sub> 0.1 M, 1 mM metal solution (<b>a</b>) 1 mM [Pd(NH<sub>3</sub>)<sub>4</sub>]SO<sub>4</sub> solution; (<b>b</b>) 1 mM K<sub>2</sub>PtCl<sub>4</sub> solution; (<b>c</b>) 1 mM RhCl<sub>3</sub> solution.</p>
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<p>XPS analysis performed on the silicon electrodes used after charge-controlled deposition on the Si working electrode in H<sub>2</sub>SO<sub>4</sub> 0.1 M, and 1 mM metal solution: (<b>a</b>) 1 mM [Pd(NH<sub>3</sub>)<sub>4</sub>]SO<sub>4</sub> solution; (<b>b</b>) 1 mM K<sub>2</sub>PtCl<sub>4</sub> solution; (<b>c</b>) 1 mM RhCl<sub>3</sub> solution.</p>
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<p>SEM images of the deposits obtained through a variable number of charge-controlled deposition cycles on the Si working electrode in H<sub>2</sub>SO<sub>4</sub> 0.1 M and RhCl<sub>3</sub> 1 mM solution: (<b>a</b>) 1 cycle; (<b>b</b>) 10 cycles; (<b>c</b>) 20 cycles; (<b>d</b>) 30 cycles; (<b>e</b>) 40 cycles; and (<b>f</b>) 50 cycles.</p>
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<p>(<b>a</b>) Surface coverage trend; (<b>b</b>) average particle diameter size trend; (<b>c</b>) equivalent thickness trend of the deposits, obtained through a variable number of charge-controlled deposition cycles (1, 10, 20, 30, 40, and 50 cycles) on the Si working electrode using H<sub>2</sub>SO<sub>4</sub> 0.1 M and RhCl<sub>3</sub> 1 mM solutions.</p>
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9 pages, 4545 KiB  
Article
Study of Thermalization Mechanisms of Hot Carriers in BABr-Added MAPbBr3 for the Top Layer of Four-Junction Solar Cells
by Yi Zhang, Huilong Chen, Junfeng Qu, Jiayu Zhang and Gavin Conibeer
Nanomaterials 2024, 14(24), 2041; https://doi.org/10.3390/nano14242041 - 19 Dec 2024
Abstract
The hot carrier multi-junction solar cell (HCMJC) is an advanced-concept solar cell with a theoretical efficiency greater than 65%. It combines the advantages of hot carrier solar cells and multi-junction solar cells with higher power conversion efficiency (PCE). The thermalization coefficient (Q [...] Read more.
The hot carrier multi-junction solar cell (HCMJC) is an advanced-concept solar cell with a theoretical efficiency greater than 65%. It combines the advantages of hot carrier solar cells and multi-junction solar cells with higher power conversion efficiency (PCE). The thermalization coefficient (Qth) has been shown to slow down by an order of magnitude in low-dimensional structures, which will significantly improve PCE. However, there have been no studies calculating the Qth of MAPbBr3 quantum dots so far. In this work, the Qth values of MAPbBr3 quantum dots and after BABr addition were calculated based on power-dependent steady-state photoluminescence (PD-SSPL). Their peak positions in PD-SSPL increased from 2.37 to 2.71 eV after adding BABr. The fitting shows that, after adding BABr, the Qth decreased from 2.64 ± 0.29 mW·K−1·cm−2 to 2.36 ± 0.25 mW·K−1·cm−2, indicating a lower relaxation rate. This is because BABr passivates surface defects, slowing down the carrier thermalization process. This work lays the foundation for the theoretical framework combining perovskite materials, which suggests that the appropriate passivation of BABr has the potential to further reduce Qth and make MAPbBr3 QDs with BABr modified more suitable as the top absorption layer of HCMJCs. Full article
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<p>XRD pattern of MAPbBr<sub>3</sub> with BABr modified.</p>
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<p>(<b>a</b>) The PL spectra for both the pristine and BABr-modified MAPbBr<sub>3</sub> samples. (<b>b</b>) The UV–vis absorption spectra curves and the Tauc plot as inset in (<b>b</b>) for both samples.</p>
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<p>PD-SSPL results in MAPbBr<sub>3</sub> QDs: (<b>a</b>) pristine and (<b>b</b>) with BABr with different power densities in mW·cm<sup>−2</sup>, where the high-energy-tail fitting region is indicated by the shaded area. Absorbed power-dependent carrier temperature for MAPbBr<sub>3</sub> QDs (<b>c</b>) pristine and (<b>d</b>) with BABr modified calculated by high-energy-tail fitting.</p>
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<p><span class="html-italic">P<sub>abs</sub></span>/<span class="html-italic">exp</span>(<span class="html-italic">−E<sub>LO</sub></span>/<span class="html-italic">k<sub>B</sub>T<sub>C</sub></span>) (mW·cm<sup>−2</sup>) as a function of Δ<span class="html-italic">T</span> (K); the gradient indicated by the blue dashed line yields the thermalization coefficient <span class="html-italic">Q<sub>th</sub></span>, with values of 2.64 ± 0.29 mW·K<sup>−1</sup>·cm<sup>−2</sup> and 2.36 ± 0.25 mW·K<sup>−1</sup>·cm<sup>−2</sup> for pristine and with BABr modified.</p>
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<p>The effects of BABr addition on thermalization and <span class="html-italic">Q<sub>th</sub></span> in MAPbBr<sub>3</sub> QDs are analyzed from different perspectives.</p>
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15 pages, 2132 KiB  
Article
Integration of Phase Change Material into PV Windows to Improve the Efficiency of Semi-Transparent Panels Based on Luminescent Solar Concentrator Technology
by Giulio Mangherini, Eleonora Baccega, Valentina Diolaiti and Donato Vincenzi
Sustainability 2024, 16(24), 11148; https://doi.org/10.3390/su162411148 - 19 Dec 2024
Abstract
This research addresses the need for enhanced thermal management in building-integrated photovoltaic systems, specifically focusing on semi-transparent PV panels based on luminescent solar concentrator (LSC) technology. In pursuit of optimal thermal regulation, the cooling effect of a paraffin PCM was investigated via finite [...] Read more.
This research addresses the need for enhanced thermal management in building-integrated photovoltaic systems, specifically focusing on semi-transparent PV panels based on luminescent solar concentrator (LSC) technology. In pursuit of optimal thermal regulation, the cooling effect of a paraffin PCM was investigated via finite element simulations developed with COMSOL Multiphysics. The PCM was thermally coupled with the PV cells situated in the frame of a south-facing window. Due to the seasonal difference between winter and summer, the PCM latent heat capacity and melting temperature were optimized to ensure the maximum nominal operating cell temperature (NOCT) reduction during summer months. PCM latent heat capacities equivalent to 120 kJ/kg, 180 kJ/kg, and 240 kJ/kg have been investigated, whereas for the melting temperature a range from 20 °C to 42 °C was spanned. The combination of higher latent heat and 36 °C melting point showed the most significant thermal benefits, by reducing the NOCT from 42 °C to 36 °C, which led to an 11.80% increase in power output across the whole PV window. Considering the same latent heat, the other melting temperature resulted in more moderate benefits, namely an enhancement of 7.88% and 3.94%, for 38 °C and 40 °C, respectively. The lower latent heat capacities resulted in an NOCT reduction that ranged between 2.7 °C and 5.3 °C, according to the associated melting point. These results testify that the presented solution could significantly enhance energy production in semi-transparent PV applications based on LSC panels. Full article
(This article belongs to the Section Green Building)
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<p>Schematic of LSC functioning presenting the panel used in this work. (1) Solar irradiance impinging on the semi-transparent waveguide. (2) Fluorophores absorbing the impinging radiation and re-emitting it within the waveguide. (3) Fluorescence light guided to the slab edges via total internal reflection (net of waveguide absorption). (4) Fluorescence light exiting the slab via escape cone. (5) Transmitted light.</p>
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<p>Configurations modeled. Window area 1.4 × 1 m<sup>2</sup>.</p>
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<p>Thermodynamic variables used to optimize PCM properties, including the boundary conditions imposed to the numerical models, ambient temperature and vertical radiation, and NOCT in absence of PCM in summer (<b>a</b>), and winter (<b>b</b>).</p>
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<p>PCM liquid fraction as function of the different melting temperatures, 120 kJ/kg (<b>a</b>), 180 kJ/kg (<b>b</b>), and 240 kJ/kg (<b>c</b>) (summer simulations).</p>
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<p>PCM liquid phase as a function of different melting temperatures and latent heat, considering multi-day simulations. 120 kJ/kg (<b>a</b>), 180 kJ/kg (<b>b</b>), and 240 kJ/kg (<b>c</b>).</p>
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<p>NOCT temperature at different PCM melting temperatures and different latent heat, namely 120 kJ/kg (<b>a</b>), 180 kJ/kg (<b>b</b>), and 240 kJ/kg (<b>c</b>).</p>
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<p>NOCT temperature at different PCM melting temperatures and different latent heat, namely 120 kJ/kg (<b>a</b>), 180 kJ/kg (<b>b</b>), and 240 kJ/kg (<b>c</b>).</p>
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<p>Electrical performance of a PV array depending on the NOCT temperature IV curves (<b>a</b>), and PV curves (<b>b</b>).</p>
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9 pages, 2206 KiB  
Article
Development of Model Representations of Materials with Ordered Distribution of Vacancies
by Ekaterina N. Muratova, Vyacheslav A. Moshnikov and Anton A. Zhilenkov
Crystals 2024, 14(12), 1095; https://doi.org/10.3390/cryst14121095 - 19 Dec 2024
Abstract
This paper presents an overview of research results on the physical and technological features of crystal formation with an ordered distribution of vacancies. It is noted that the composition and properties of complex chalcogenide phases are not always described by the traditional concepts [...] Read more.
This paper presents an overview of research results on the physical and technological features of crystal formation with an ordered distribution of vacancies. It is noted that the composition and properties of complex chalcogenide phases are not always described by the traditional concepts behind Kroeger’s theory. Model concepts are considered in which the carriers of properties in the crystalline state are not molecules, but an elementary crystalline element with a given arrangement of nodes with atoms and vacancies. It is established that the introduction of the term “quasi-element atom” of the zero group for a vacancy allows us to predict a number of compounds with an ordered distribution of vacancies. Examples of the analysis of peritectic multicomponent compounds and solid solutions based on them are given. Quasi-crystalline concepts are applicable to perovskite materials used in solar cells. It is shown that the photoluminescence of perovskite lead-cesium halides is determined by crystalline structural subunits i.e., the anionic octets. This is the reason for the improvement in the luminescent properties of colloidal quantum CsPbBr3 dots under radiation exposure conditions. Full article
(This article belongs to the Section Inorganic Crystalline Materials)
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<p>Triangulation of the ternary system Ag-In-S, (In<sub>2</sub>S-Ag<sub>2</sub>S<sub>3</sub> is the “four” line, In<sub>2</sub>S<sub>3</sub>-Ag<sub>2</sub>S is the “eight” line).</p>
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<p>Triangulation of the pseudo-triple system [V]-In-S, (In<sub>2</sub>S-[V]S<sub>2</sub> is the “four” line, In<sub>2</sub>S<sub>3</sub>-[V] is the “eight” line).</p>
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<p>Tetrahedration of the pseudo-quaternary system [V]-Ag-In-S. The arrow points to a known chemical compound that we have marked in <a href="#crystals-14-01095-f001" class="html-fig">Figure 1</a>.</p>
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<p>State diagram of the PbTe-Ga<sub>2</sub>Te<sub>3</sub> system.</p>
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<p>The main compounds of three-component systems of lead-cesium halides on the Gibbs triangle (underlined binary compounds do not exist for all halogens X from the series Cl, Br, I) and partial triangulation of the system using the example of CsPbCl<sub>3</sub>) [<a href="#B17-crystals-14-01095" class="html-bibr">17</a>].</p>
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<p>High-resolution transmission electron microscopy images of CsPbBr<sub>3</sub> nanocrystal [<a href="#B17-crystals-14-01095" class="html-bibr">17</a>]. (<b>a</b>) TEM images with 100 nm resolution; (<b>b</b>) TEM images with 5 nm resolution.</p>
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<p>Dynamics of changes in photoluminescence spectra during the anionic substitution of Br–I: triangles represent the time dependence of the energy corresponding to the maximum PL intensity, and dots represent the time dependence of the half-width of the PL line [<a href="#B17-crystals-14-01095" class="html-bibr">17</a>].</p>
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21 pages, 3464 KiB  
Review
Alternatives for Connecting Photovoltaic Generators to Power Systems with Three-Port and Partial Power Converters
by Donghui Ye and Sergio Martinez
Appl. Sci. 2024, 14(24), 11880; https://doi.org/10.3390/app142411880 - 19 Dec 2024
Viewed by 76
Abstract
Solar electricity has become one of the most important renewable power sources due to rapid developments in the manufacturing of photovoltaic (PV) cells and power electronic techniques as well as the consciousness of environmental protection. In general, PV panels are connected to DC-DC [...] Read more.
Solar electricity has become one of the most important renewable power sources due to rapid developments in the manufacturing of photovoltaic (PV) cells and power electronic techniques as well as the consciousness of environmental protection. In general, PV panels are connected to DC-DC converters and/or DC-AC inverters to implement the maximum power point tracking algorithm and to fulfill the load requirements. Thus, power conversion efficiency and power density need to be taken into consideration when designing PV systems. Three-port and partial power conversion technologies are proposed to improve the efficiency of a whole PV system and its power density. In this paper, three types of three-port converters (TPCs), including fully isolated, partly isolated, and non-isolated TPCs, are studied with detailed discussions of advantages, disadvantages, and comparisons. In addition, based on partial power conversion technologies, partial power two-port and three-port topologies are analyzed in detail. Their efficiency and power density can be further improved by the combination of three-port and partial power conversion technologies. Moreover, comparisons among seven different types of distributed PV systems are presented with their advantages and disadvantages. Compared to distributed PV systems without energy storage, distributed PV systems with hybridization of energy storage and with partial power regulation can use solar energy in a more efficient way. Full article
(This article belongs to the Special Issue Power Systems: Protection and Connection with Converters)
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<p>Stand-alone PV power conversion system.</p>
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<p>Hybrid PV power conversion system.</p>
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<p>Grid-connected PV power conversion system.</p>
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<p>Alternative grid-connected PV system control with power curtailment control algorithm.</p>
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<p>Traditional configuration of a PV system with two individual DC-DC converters. The red lines indicate the possible directions of power flow.</p>
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<p>Power flow scheme of traditional TPCs.</p>
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<p>Power flow scheme of traditional TPCs. Operation modes of a TPC: (<b>a</b>) SIDO; (<b>b</b>) DISO; (<b>c</b>–<b>e</b>) SISO.</p>
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<p>Full power converter. (<b>a</b>) Circuit configuration. (<b>b</b>) Power flow scheme.</p>
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<p>Partial power converter. (<b>a</b>) Circuit configuration. (<b>b</b>) Power flow scheme (red arrows indicate direct power flow).</p>
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<p>Power flow of two-port partial power converters (<b>a</b>) with step-up (<span class="html-italic">v<sub>c</sub></span> &gt; 0) or step-down (<span class="html-italic">v<sub>c</sub></span> &lt; 0) operation modes. (<b>b</b>,<b>c</b>) Two examples of circuit structure of step-up operation. (<b>d</b>,<b>e</b>) Two examples of circuit structure of step-down operation.</p>
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<p>Partial power boost DC-DC converter.</p>
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<p>Power flow scheme. (<b>a</b>) Full-power TPC; (<b>b</b>) step-down TPC with PPR; (<b>c</b>) step-up TPC with PPR.</p>
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<p>Power flow scheme of the proposed BESS-integrated PV system with PPR.</p>
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<p>Centralized PV system with a string PV panel.</p>
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<p>Centralized PV system with bypass diodes.</p>
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<p>Traditional distributed PV system with individual converters.</p>
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<p>Distributed PV system architectures. (<b>a</b>) Individual DC-DC converters connected between each PV panel and the output. (<b>b</b>) A DC-DC converter connected between PV panels and the output.</p>
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<p>Distributed PV system architecture with DC-DC converters connected between each PV panel.</p>
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<p>Distributed PV system architecture with DC-DC converters connected between each PV panel and the DC bus.</p>
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<p>Circuit configuration of a distributed PV system with a BESS and PPR.</p>
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14 pages, 7106 KiB  
Article
Numerical Investigation and Device Architecture Optimization of Sb2Se3 Thin-Film Solar Cells Using SCAPS-1D
by Chung-Kuan Lai and Yi-Cheng Lin
Materials 2024, 17(24), 6203; https://doi.org/10.3390/ma17246203 - 19 Dec 2024
Viewed by 105
Abstract
Antimony selenide (Sb2Se3) shows promise for photovoltaics due to its favorable properties and low toxicity. However, current Sb2Se3 solar cells exhibit efficiencies significantly below their theoretical limits, primarily due to interface recombination and non-optimal device architectures. [...] Read more.
Antimony selenide (Sb2Se3) shows promise for photovoltaics due to its favorable properties and low toxicity. However, current Sb2Se3 solar cells exhibit efficiencies significantly below their theoretical limits, primarily due to interface recombination and non-optimal device architectures. This study presents a comprehensive numerical investigation of Sb2Se3 thin-film solar cells using SCAPS-1D simulation software, focusing on device architecture optimization and interface engineering. We systematically analyzed device configurations (substrate and superstrate), hole-transport layer (HTL) materials (including NiOx, CZTS, Cu2O, CuO, CuI, CuSCN, CZ-TA, and Spiro-OMeTAD), layer thicknesses, carrier densities, and resistance effects. The substrate configuration with molybdenum back contact demonstrated superior performance compared with the superstrate design, primarily due to favorable energy band alignment at the Mo/Sb2Se3 interface. Among the investigated HTL materials, Cu2O exhibited optimal performance with minimal valence-band offset, achieving maximum efficiency at 0.06 μm thickness. Device optimization revealed critical parameters: series resistance should be minimized to 0–5 Ω-cm2 while maintaining shunt resistance above 2000 Ω-cm2. The optimized Mo/Cu2O(0.06 μm)/Sb2Se3/CdS/i-ZnO/ITO/Al structure achieved a remarkable power conversion efficiency (PCE) of 21.68%, representing a significant improvement from 14.23% in conventional cells without HTL. This study provides crucial insights for the practical development of high-efficiency Sb2Se3 solar cells, demonstrating the significant impact of device architecture optimization and interface engineering on overall performance. Full article
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<p>Schematic diagram of the proposed solar-cell structure: (<b>a</b>) p-n substrate configuration, (<b>b</b>) p-n superstrate configuration, (<b>c</b>) n-p-p<sup>+</sup> substrate configuration.</p>
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<p>Energy band diagrams of different device configurations: (<b>a</b>) substrate and (<b>b</b>) superstrate structures.</p>
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<p>Performance characteristics of different device configurations: (<b>a</b>) current–voltage curves and (<b>b</b>) external quantum efficiency spectra.</p>
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<p>Energy band diagrams of various HTL materials in the device structure.</p>
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<p>PCE comparison of different HTL materials.</p>
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<p>Relationship between Cu<sub>2</sub>O HTL thickness and device performance.</p>
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<p>Relationship between Cu<sub>2</sub>O HTL shallow acceptor density and device performance.</p>
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<p>Effect of shallow acceptor density on Sb<sub>2</sub>Se<sub>3</sub> solar-cell efficiency at different Cu<sub>2</sub>O HTL thicknesses.</p>
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<p>Numerical analysis of series and parallel resistance on device performance. (<b>a</b>) Open-circuit voltage (Voc) variation, (<b>b</b>) Short-circuit current density (Jsc) response, (<b>c</b>) Fill Factor (FF) dependence, and (<b>d</b>) Device efficiency changes with respect to series and parallel resistance.</p>
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18 pages, 2363 KiB  
Article
Mixed Pt-Ni Halide Perovskites for Photovoltaic Application
by Huilong Liu, Rubaiya Murshed and Shubhra Bansal
Materials 2024, 17(24), 6196; https://doi.org/10.3390/ma17246196 - 18 Dec 2024
Viewed by 216
Abstract
Cs2PtI6 is a promising photoabsorber with a direct bandgap of 1.4 eV and a high carrier lifetime; however, the cost of Pt inhibits its commercial viability. Here, we performed a cost analysis and experimentally explored the effect of replacing Pt [...] Read more.
Cs2PtI6 is a promising photoabsorber with a direct bandgap of 1.4 eV and a high carrier lifetime; however, the cost of Pt inhibits its commercial viability. Here, we performed a cost analysis and experimentally explored the effect of replacing Pt with earth-abundant Ni in solution-processed Cs(PtxNi1−x)(I,Cl)3 thin films on the properties and stability of the perovskite material. Films fabricated with CsI and PtI2 precursors result in a perovskite phase with a bandgap of 2.13 eV which transitions into stable Cs2PtI6 with a bandgap of 1.6 eV upon annealing. The complete substitution of PtI2 in films with CsI + NiCl2 precursors results in a wider bandgap of 2.35 eV and SEM shows two phases—a rod-like structure identified as CsNi(I,Cl)3 and residual white particles of CsI, also confirmed by XRD and Raman spectra. Upon extended thermal annealing, the bandgap reduces to 1.65 eV and transforms to CsNiCl3 with a peak shift to higher 2-theta. The partial substitution of PtI2 with NiCl2 in mixed 50-50 Pt-Ni-based films produces a bandgap of 1.9 eV, exhibiting a phase of Cs(Pt,Ni)(I,Cl)3 composition. A similar bandgap of 1.85 eV and the same diffraction pattern with improved crystallinity is observed after 100 h of annealing, confirming the formation of a stable mixed Pt-Ni phase. Full article
(This article belongs to the Special Issue Advanced Energy Materials for Perovskite Solar Cells)
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<p>Atmospheric synthesis of PtI<sub>2</sub>, mixed PtI<sub>2</sub>-NiCl<sub>2</sub>, and NiCl<sub>2</sub>-based films in 50:50 DMF: DMSO via solution processing.</p>
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<p>USD/Watt (solute) of various Pb and Pb-free perovskite compositions calculated with respect to the PCE and thickness reported in the corresponding literature (blue) and the highest PCE of 25.6% and thickness of 2000 nm reported for the Pb-based FAPbI<sub>3</sub> perovskite (red). <a href="#app1-materials-17-06196" class="html-app">Figure S1</a> represents the USD/watt with the discrete effect of optimized PCE and absorber layer thickness.</p>
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<p>USD/Watt (solute + encapsulant) of various Pb and Pb-free perovskite compounds calculated with respect to the highest PCE of 25.6% and thickness of 2000 nm reported for the Pb-based FAPbI<sub>3</sub> perovskite. E1, E2, E3, and E4 represent different encapsulants: Polyolefin, Teflon, PET, and EVA, respectively. <a href="#app1-materials-17-06196" class="html-app">Figure S2</a> represents the USD/Watt (solute + encapsulant) calculated with respect to the PCE and absorber layer thickness reported in the corresponding literature. <a href="#app1-materials-17-06196" class="html-app">Figure S3</a> represents the USD/watt (solute + encapsulant) with the discrete effect of optimized PCE reported for the Pb-based FAPbI<sub>3</sub> perovskite and the corresponding absorber layer thickness from the literature. <a href="#app1-materials-17-06196" class="html-app">Figure S4</a> represents the USD/watt (solute + encapsulant) with the discrete effect of the optimized absorber layer thickness reported for the Pb-based FAPbI<sub>3</sub> perovskite and PCE from the literature.</p>
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<p>(<b>a</b>) Absorption spectrums of 2 h annealed (at −15 in Hg and 100 °C) PtI<sub>2</sub>, mixed PtI<sub>2</sub>-NiCl<sub>2</sub>, and NiCl<sub>2</sub>-based films; (<b>b</b>) Tauc plot showing the optical bandgap of the 2 h annealed (at −15 in Hg and 100 °C) PtI<sub>2</sub>, mixed PtI<sub>2</sub>-NiCl<sub>2</sub>, and NiCl<sub>2</sub>-based films; (<b>c</b>) XRD spectra of the 2 h annealed (at −15 in Hg and 100 °C) PtI<sub>2</sub>, mixed PtI<sub>2</sub>-NiCl<sub>2</sub>, and NiCl<sub>2</sub>-based films; SEM images of (<b>d</b>) PtI<sub>2</sub>, (<b>e</b>) mixed PtI<sub>2</sub>-NiCl<sub>2</sub>, and (<b>f</b>) NiCl<sub>2</sub>-based films; Raman spectra of (<b>g</b>) PtI<sub>2</sub>-based and (<b>h</b>) NiCl<sub>2</sub>-based films, respectively; (<b>i</b>) Goldschmidt and (<b>j</b>) Bartel tolerance factors for Cs(Pt,Ni)(Cl,I)<sub>3</sub>.</p>
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<p>PtI<sub>2</sub>-based films before and after the dark thermal annealing test with t representing the annealing duration: (<b>a</b>) absorption coefficient; (<b>b</b>) Tauc plot; (<b>c</b>) XRD pattern; (<b>d</b>) cross-section SEM images before annealing; (<b>e</b>) cross-section SEM images after annealing; and (<b>f</b>) EDS analysis showing the atomic % of the elemental distribution.</p>
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<p>Mixed PtI<sub>2</sub>-NiCl<sub>2</sub>-based films before and after the dark thermal annealing test with t representing the annealing duration: (<b>a</b>) absorption spectrum; (<b>b</b>) Tauc plot; (<b>c</b>) XRD pattern; (<b>d</b>) cross-section SEM image before annealing; (<b>e</b>) cross-section SEM image after annealing; and (<b>f</b>) EDS analysis showing the atomic % of the elemental distribution.</p>
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<p>NiCl<sub>2</sub>-based films before and after the dark thermal annealing test with t representing the annealing duration: (<b>a</b>) absorption spectrum; (<b>b</b>) Tauc plot; (<b>c</b>) XRD pattern; (<b>d</b>) SEM morphology before annealing; (<b>e</b>) SEM morphology after annealing; and (<b>f</b>) EDS analysis showing the atomic % of the elemental distribution.</p>
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12 pages, 7596 KiB  
Article
Finite-Difference Time-Domain Simulation of Double-Ridge Superimposed Structures for Optimizing Light-Trapping Characteristics in Ternary Organic Solar Cells
by Xiaoxiang Sun, Jinglin Song, Weijun Tan, Jing Chen, Mingxin Chen, Fen Li, Chang Li and Zhuoliang Yu
Coatings 2024, 14(12), 1583; https://doi.org/10.3390/coatings14121583 - 18 Dec 2024
Viewed by 290
Abstract
The double-ridge superimposed structures (DRSSs), formed by the superposition of a nano-ridged textured ZnO layer and a ternary organic active layer (PTB7:PC70BM:PC60BM) with self-assembled nano-ridged (SANR) structures, have been preliminarily examined experimentally for its positive effects in light-trapping for [...] Read more.
The double-ridge superimposed structures (DRSSs), formed by the superposition of a nano-ridged textured ZnO layer and a ternary organic active layer (PTB7:PC70BM:PC60BM) with self-assembled nano-ridged (SANR) structures, have been preliminarily examined experimentally for its positive effects in light-trapping for organic solar cells (OSCs). To obtain DRSSs with higher-performance light-trapping effects and enhance the light absorption of OSCs, the present work carried out prior theoretical simulations of the light-trapping characteristics of the DRSS using the finite-difference time-domain (FDTD) algorithm. The results show that the DRSS exhibits a significant light-trapping effect, with an active layer absorption peak around 530 nm due to the light-trapping effect. This helps the active layer capture more high-energy photons, significantly enhancing the photon utilization of the DRSS. Interestingly, the intensity of the light-trapping absorption peak is solely dependent on the height or width of the active layer ridges in the DRSS, while the position of the peak is jointly determined by both the ZnO and active layer ridges. By controlling the aspect ratio (W/H) of the dual ridges, the light-trapping absorption peak position can be fine-tuned, enabling precise light-trapping management for specific wavelength bands. It is certain that the outcomes of this work will provide theoretical foundations and practical guidance for the fabrication of light-trapping OSCs. Full article
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<p>(<b>a</b>) Schematic diagram of the numerical model of the DRSS. (<b>b</b>) The side view of the simulation model’s unit cell.</p>
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<p>(<b>a</b>) Schematic diagram of the different models. (<b>b</b>) Absorption spectra of the different models; the inset shows the light-trapping mechanism of the DRSS. (<b>c</b>) Corresponding transmission and reflection spectra.</p>
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<p>The normalized cross-section near-field profiles of TM-polarized light for normal-incidence monochromatic illumination at the wavelength of 520 nm in the different models. (<b>a</b>) Model A, (<b>b</b>) Model B, (<b>c</b>) Model C, and (<b>d</b>) Model D.</p>
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<p>Optical properties of the DRSS with different active layer texture morphologies; the size of the ZnO ridge structures is constant and the height of the active layer ridge structures is fixed at 50 nm. (<b>a</b>) Absorption spectra. (<b>b</b>) Transmission and reflection spectra.</p>
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<p>Optical properties of the DRSS with different active layer texture morphologies; the size of the ZnO texture structure is constant and the width of the active layer texture structure is fixed at 325 nm. (<b>a</b>) Absorption spectra. (<b>b</b>) Transmission and reflection spectra.</p>
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<p>The normalized near-field profiles of TM-polarized light for normal-incidence monochromatic illumination at a wavelength of 520 nm, observed in the DRSS with different active layer texture morphologies; the size of the ZnO texture structure is constant. (<b>a</b>) H = 10 nm and W = 325 nm; (<b>b</b>) H = 50 nm and W = 325 nm; (<b>c</b>) H = 50 nm and W = 75 nm.</p>
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<p>Optical properties of the DRSS with different ZnO and active layer texture morphologies; the width of the ZnO and active layer texture structures is fixed at 425 nm and the heights of both remain synchronized. (<b>a</b>) Absorption spectra. (<b>b</b>) Transmission and reflection spectra.</p>
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<p>Absorption spectra of the DRSS with different ZnO and active layer texture morphologies; the height of the ZnO and active layer texture structures is fixed at 50 nm and the widths of both remain synchronized.</p>
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<p>Optical properties of the DRSS with different ZnO and active layer texture morphologies; the height and width of the ZnO and active layer texture structures are kept synchronized, and the detailed aspect ratio settings are shown in <a href="#coatings-14-01583-t001" class="html-table">Table 1</a>. (<b>a</b>) Absorption spectra. (<b>b</b>) Transmission and reflection spectra.</p>
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29 pages, 10223 KiB  
Review
Advancements in Manufacturing of High-Performance Perovskite Solar Cells and Modules Using Printing Technologies
by Shohreh Soltani and Dawen Li
Energies 2024, 17(24), 6344; https://doi.org/10.3390/en17246344 - 17 Dec 2024
Viewed by 276
Abstract
Perovskite photovoltaic technology carries immense opportunity for the solar industries because of its remarkable efficiency and prospect for cost-effective production. However, the successful deployment of perovskite solar modules (PSMs) in the solar market necessitates tackling stability-based obstacles, scalability, and environmental considerations. This paper [...] Read more.
Perovskite photovoltaic technology carries immense opportunity for the solar industries because of its remarkable efficiency and prospect for cost-effective production. However, the successful deployment of perovskite solar modules (PSMs) in the solar market necessitates tackling stability-based obstacles, scalability, and environmental considerations. This paper unveils a comprehensive examination of the cutting-edge advancements in the manufacturing of perovskite solar cells (PSCs) and modules, with an emphasis on high-speed, large-area printing. The paper underscores the substantial progress achieved in printed PSCs and PSMs, demonstrating promising electrical performance and long-term device durability. This review paper categorizes printing techniques compatible with large-area high-speed manufacturing into three distinct families: blade coating, slot die coating, and screen printing, as these common printing practices offer precise control, scalability, cost-effectiveness, high resolution, and efficient material usage. Additionally, this paper presents an in-depth investigation and comparison of superior PSCs and PSMs fabricated by printing on power conversion efficiency (PCE), stability, and scalability. Full article
(This article belongs to the Section D1: Advanced Energy Materials)
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<p>(<b>a</b>) Experimental arrangement and placement using the blade coating method [<a href="#B27-energies-17-06344" class="html-bibr">27</a>], (<b>b</b>) Schematic of slot-die coating procedure [<a href="#B28-energies-17-06344" class="html-bibr">28</a>], (<b>c</b>) Illustration of R2R screen printing [<a href="#B29-energies-17-06344" class="html-bibr">29</a>], (<b>d</b>) Schematic of gravure printing on elastic substrate [<a href="#B30-energies-17-06344" class="html-bibr">30</a>], (<b>e</b>) Schematic of spray coating process [<a href="#B31-energies-17-06344" class="html-bibr">31</a>].</p>
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<p>Schematic for combined cosolvent and additive strategy to reduce coordination regulation by replacing strong coordination solvent (SCS) with weak coordination solvents (WCS), [<a href="#B36-energies-17-06344" class="html-bibr">36</a>].</p>
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<p>(<b>a</b>) J-V characteristics, (<b>b</b>) stabilized PCE over time, (<b>c</b>) EQE plot for blade coated PSCs with device area over 1 cm<sup>2</sup>, (<b>d</b>) champion Voc for WBG-based PSCs [<a href="#B37-energies-17-06344" class="html-bibr">37</a>].</p>
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<p>(<b>a</b>) Fill factor (FF) and PCE statistical distribution for blade-coated single-junction PSCs using different bottom contacts: PTAA, (MeO:Br)-2PACz, and 2PACz, (<b>b</b>) Statistical distribution of PCE and FF for blade-coating tandems with F6TCNNQ incorporation and different hole transport layer (HTL) (PTAA, (MeO:Br)-2PACz and 2PACz), (<b>c</b>) unit architecture of F6TCNNQ-doped tandems with different HTL configurations, (<b>d</b>) J-V curves of single junction (hollow circles) and tandem devices with different HTLs, (<b>e</b>) MPPT stability testing of blade-coated tandem solar cells [<a href="#B38-energies-17-06344" class="html-bibr">38</a>].</p>
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<p>(<b>A</b>) Schematic view of the tandem-structured device, (<b>B</b>) Measured reflection (1-R) and EQE of mentioned tandem solar cells, (<b>C</b>) Photovoltaic parameters of tandem solar cells with variation in thickness, (<b>D</b>) Quasi steady-state J-V characteristics [<a href="#B40-energies-17-06344" class="html-bibr">40</a>].</p>
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<p>(<b>a</b>) Structure of perovskite-silicon tandem solar cells without and with LiF layer, (<b>b</b>) Schematic of equivalent circuit of the tandem cell [<a href="#B43-energies-17-06344" class="html-bibr">43</a>].</p>
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<p>(<b>A</b>) Structure of the single-junction perovskite sub-cell for integration with commercial silicon cells, (<b>B</b>) J-V plots of champion PSCs optimized at varying annealing temperatures, (<b>C</b>) External quantum efficiency measurement and integrated short-circuit current, Jsc, (<b>D</b>) MPPT stability test of the fabricated best solar cells at 25 °C [<a href="#B44-energies-17-06344" class="html-bibr">44</a>].</p>
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<p>(<b>a</b>) Device structure and deposition approach for each layer, (<b>b</b>) J-V plots of the best PSCs based on pristine and KSCN incorporated MAPbI<sub>3</sub> films [<a href="#B45-energies-17-06344" class="html-bibr">45</a>].</p>
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<p>(<b>a</b>) Illustration of slot die coating setup, (<b>b</b>) J-V plots at various DMSO additive solvent concentrations [<a href="#B46-energies-17-06344" class="html-bibr">46</a>].</p>
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<p>(<b>a</b>) Schematic of perovskite crystallization with additive and cosolvent strategy, (<b>b</b>) J-V plots of fabricated PSCs, (<b>c</b>) EQE for both cases of with and without NH<sub>4</sub>Cl, (<b>d</b>) MPPT stability testing of PSCs with optimized NH<sub>4</sub>Cl addition [<a href="#B53-energies-17-06344" class="html-bibr">53</a>].</p>
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<p>Illustration in printing procedure and resulting structure of fully R2R printed PSMs [<a href="#B63-energies-17-06344" class="html-bibr">63</a>].</p>
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<p>(<b>a</b>) An image of a blade-coated FA<sub>0.3</sub>MA<sub>0.7</sub>PbI<sub>3</sub> perovskite layer on an ITO substrate, covering around 130 cm<sup>2</sup>, (<b>b</b>) A photograph showing enclosed minimodules with aperture areas of approximately 78 cm<sup>2</sup>, (<b>c</b>) J-V plots illustrating the characteristics of minimodules with aperture areas of 78 cm<sup>2</sup>, 84 cm<sup>2</sup>, and 108 cm<sup>2</sup>, respectively, (<b>d</b>) Performance of minimodule with various aperture areas, (<b>e</b>) Stable power output from the champion minimodules [<a href="#B71-energies-17-06344" class="html-bibr">71</a>].</p>
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<p>(<b>a</b>) Rheological characteristics of perovskite precursor inks modulated by DCB, (<b>b</b>) Visualizing PCE dependence on ink composition, (<b>c</b>) Performance characteristics of perovskite minimodule under standard testing conditions [<a href="#B82-energies-17-06344" class="html-bibr">82</a>].</p>
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<p>(<b>a</b>) Slot die coating deposition of a wide band gap perovskite absorber layer on textured silicon surface to make perovskite/silicon tandem devices, (<b>b</b>) SEM image showing cross-section of textured silicon/perovskite tandem device made by slot die coating, (<b>c</b>) PCE statistics for slot-die-coated tandems at various head speeds, (<b>d</b>) J-V plot of the best slot die coated silicon/perovskite tandem devices [<a href="#B84-energies-17-06344" class="html-bibr">84</a>].</p>
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<p>(<b>a</b>) Certified J-V plots of the top PSCs using Me-4PACz as HTL (<b>b</b>) J-V plots of a 25 cm<sup>2</sup> mini-module [<a href="#B86-energies-17-06344" class="html-bibr">86</a>].</p>
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<p>Performance development of PSMs with various unit areas, in terms of different printing methods [<a href="#B90-energies-17-06344" class="html-bibr">90</a>].</p>
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13 pages, 13568 KiB  
Article
Influence of Copper and Tin Oxidation States on the Phase Evolution of Solution-Processed Ag-Alloyed CZTS Photovoltaic Absorbers
by Abdeljalil Errafyg, Naoufal Ennouhi, Yassine Chouimi and Zouheir Sekkat
Energies 2024, 17(24), 6341; https://doi.org/10.3390/en17246341 - 17 Dec 2024
Viewed by 326
Abstract
Kesterite-based semiconductors, particularly copper–zinc–tin–sulfide (CZTS), have garnered considerable attention as potential absorber layers in thin-film solar cells because of their abundance, nontoxicity, and cost-effectiveness. In this study, we explored the synthesis of Ag-alloyed CZTS (ACZTS) materials via the sol–gel method and deposited them [...] Read more.
Kesterite-based semiconductors, particularly copper–zinc–tin–sulfide (CZTS), have garnered considerable attention as potential absorber layers in thin-film solar cells because of their abundance, nontoxicity, and cost-effectiveness. In this study, we explored the synthesis of Ag-alloyed CZTS (ACZTS) materials via the sol–gel method and deposited them on a transparent fluorine-doped tin oxide (FTO) back electrode. A key challenge is the selection and manipulation of metal–salt precursors, with a particular focus on the oxidation states of copper (Cu) and tin (Sn) ions. Two distinct protocols, varying the oxidation states of the Cu and Sn ions, were employed to synthesize the ACZTS materials. The transfer from the solution to the precursor film was analyzed, followed by annealing at different temperatures under a sulfur atmosphere to investigate the behavior and growth of these materials during the final stage of annealing. Our results show that the precursor transformation from solution to film is highly sensitive to the oxidation states of these metal ions, significantly influencing the chemical reactions during sol–gel synthesis and subsequent annealing. Furthermore, the formation pathway of the kesterite phase at elevated temperatures differs between the two protocols. Structural, morphological, and optical properties were characterized via X-ray diffraction (XRD), Raman spectroscopy, and scanning electron microscopy (SEM). Our findings highlight the critical role of the Cu and Sn oxidation states in the formation of high-quality kesterite materials. Additionally, we studied a novel approach for controlling the synthesis and phase evolution of kesterite materials via molecular inks, which could provide new opportunities for enhancing the efficiency of thin-film solar cells. Full article
(This article belongs to the Section D1: Advanced Energy Materials)
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<p>The optimized annealing profile used in this work.</p>
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<p>XRD patterns of ACZTS precursors deposited from Sol-1 or Sol-2.</p>
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<p>Raman s spectra of CZTS precursors deposited from Sol-1 or Sol-2, recorded with excitation wavelengths of 532 (<b>a</b>) and 785 nm (<b>b</b>).</p>
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<p>Transformation mechanisms from solution to precursor for the two different protocols.</p>
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<p>XRD patterns of CZTS thin-film absorbers prepared with Sol-1 (<b>a</b>) and Sol-2 (<b>b</b>) and annealed at different temperatures.</p>
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<p>Raman spectra of CZTS absorbers prepared with Sol-1 and Sol-2 and annealed at different temperatures, recorded with excitation wavelengths of 532 (<b>a</b>,<b>c</b>) and 785 nm (<b>b</b>,<b>d</b>).</p>
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<p>Surface SEM images of CZTS absorbers prepared with Sol-1 and Sol-2 and annealed at different temperatures.</p>
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<p>Transformation mechanisms from the solution to the precursor and from the precursor to the absorber for Sol-1 and Sol-2.</p>
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25 pages, 2604 KiB  
Article
Enhancing Efficiency in Hybrid Solar–Wind–Battery Systems Using an Adaptive MPPT Controller Based on Shadow Motion Prediction
by Abdorreza Alavi Gharahbagh, Vahid Hajihashemi, Nasrin Salehi, Mahyar Moradi, José J. M. Machado and João Manuel R. S. Tavares
Appl. Sci. 2024, 14(24), 11710; https://doi.org/10.3390/app142411710 - 16 Dec 2024
Viewed by 610
Abstract
Renewable energy sources are particularly significant in global energy production, with wind and solar being the most prevalent sources. Managing the simultaneous connection of wind and solar energy generators to the smart grid as distributed generators involves complex control and stabilization due to [...] Read more.
Renewable energy sources are particularly significant in global energy production, with wind and solar being the most prevalent sources. Managing the simultaneous connection of wind and solar energy generators to the smart grid as distributed generators involves complex control and stabilization due to their inherent uncertainties, making their management more intricate than traditional power plants. This study focuses on enhancing the speed and efficiency of the maximum power point tracking (MPPT) system in a solar power plant. A hybrid network is modeled, comprising a wind turbine with a doubly-fed induction generator (DFIG), a solar power plant with photovoltaic (PV) cells, an MPPT system, a Z-source converter, and a storage system. The proposed approach employs a motion detection-based method, utilizing image-processing techniques to optimize the MPPT of PV cells based on shadow movement patterns within the solar power plant area. This method significantly reduces the time required to reach the maximum power point (MPP), lowers the computational load of the control system by predicting shadow movements, and enhances the MPPT speed while maintaining system stability. The approach, which is suitable for relatively large solar farms, is implemented without the need for any additional sensors and relies on the system’s history. The simulation results show that the proposed approach improves the MPPT system’s efficiency and reduces the pressure on the control circuits by more than 70% in a 150,000 m2 solar farm under shaded conditions. Full article
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<p>Block diagram of the wind turbine and DFIG system studied in this work.</p>
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<p>Equivalent circuit of a DFIG.</p>
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<p>Studied 9 MW wind farm compromising a DFIG and an ANFIS controller.</p>
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<p>Equivalent circuit of a PV system.</p>
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<p>Block diagram of the studied PV and Z-source converter system.</p>
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<p>Block diagram of the proposed ANFIS controller for the studied PV system.</p>
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<p>Solar element power curve.</p>
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<p>Proposed MPPT controller.</p>
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<p>INC MPPT controller.</p>
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<p>Different aspects of the studied solar farm: (<b>a</b>) the model of the solar farm with panels represented by white dots, (<b>b</b>) a cloud and its shadow on the solar farm, and (<b>c</b>) the solar farm model with shading effects.</p>
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<p>Shade change in four-time steps on the solar farm area (cloud movement from (<b>a</b>–<b>d</b>)—the location of the shadow in the solar farm are indicated by yellow squares).</p>
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<p>Real (squares on dashed line), and predicted (circles on solid line) motion vectors.</p>
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<p>Final solution of the studied system.</p>
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<p>Output voltage (Pu) of the studied wind turbine block with a wind speed of 10 m/s.</p>
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<p>Output voltage (Pu) of the studied wind turbine block with a wind speed of 15 m/s.</p>
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<p>Output voltage (Pu) of the studied wind turbine when the wind speed changes from 10 to 15 m/s.</p>
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<p>Output power of the studied PV system, including the usual INC MPPT under different irradiance levels.</p>
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<p>Boost control signal under different conditions: (<b>a</b>) 900, (<b>b</b>) 1000, (<b>c</b>) 1100, and (<b>d</b>) 1200 W/m<sup>2</sup>.</p>
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<p>Output power of the studied PV system under two different irradiance conditions: (<b>a</b>) reduced irradiance and (<b>b</b>) increased irradiance.</p>
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<p>Output power of the studied PV system under two similar increasing and decreasing irradiation conditions: (<b>a</b>) 1250 ⇔ 750 W/m<sup>2</sup> and (<b>b</b>) 1200 ⇔ 900 W/m<sup>2</sup>.</p>
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<p>Output power of the proposed and conventional PV system under different irradiation conditions: (<b>a</b>) slightly increased irradiation and (<b>b</b>) greatly increased irradiation.</p>
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<p>Output power of the proposed and conventional PV system under different decreased irradiation conditions: (<b>a</b>) slightly decreased irradiation and (<b>b</b>) greatly decreased irradiation.</p>
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<p>Output power of the studied series of solar panels under a change in irradiation from 1200 → 900 → 1200 W/m<sup>2</sup>.</p>
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<p>Area under the curve of the output power of the proposed and conventional PV systems under increased irradiation.</p>
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<p>(<b>a</b>) Area under the curve of the output power of the proposed (line in red) and conventional (line in blue) PV systems under decreased irradiation, and (<b>b</b>) the difference between the two systems (area in black).</p>
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24 pages, 3518 KiB  
Article
A Numerical Simulation Study of the Impact of Kesterites Hole Transport Materials in Quantum Dot-Sensitized Solar Cells Using SCAPS-1D
by Sindisiwe Jakalase, Azile Nqombolo, Edson L. Meyer, Mojeed A. Agoro and Nicholas Rono
Nanomaterials 2024, 14(24), 2016; https://doi.org/10.3390/nano14242016 - 15 Dec 2024
Viewed by 374
Abstract
Energy generation and storage are critical challenges for developing economies due to rising populations and limited access to clean energy resources. Fossil fuels, commonly used for energy production, are costly and contribute to environmental pollution through greenhouse gas emissions. Quantum dot-sensitized solar cells [...] Read more.
Energy generation and storage are critical challenges for developing economies due to rising populations and limited access to clean energy resources. Fossil fuels, commonly used for energy production, are costly and contribute to environmental pollution through greenhouse gas emissions. Quantum dot-sensitized solar cells (QDSSCs) offer a promising alternative due to their stability, low cost, and high-power conversion efficiency (PCE) compared to other third-generation solar cells. Kesterite materials, known for their excellent optoelectronic properties and chemical stability, have gained attention for their potential as hole transport layer (HTL) materials in solar cells. In this study, the SCAPS-1D numerical simulator was used to analyze a solar cell with the configuration FTO/TiO2/MoS2/HTL/Ag. The electron transport layer (ETL) used was titanium dioxide (TiO2), while Cu2FeSnS4 (CFTS), Cu2ZnSnS4 (CZTSe), Cu2NiSnS4 (CNTS), and Cu2ZnSnSe4 (CZTSSe) kesterite materials were evaluated as HTLs. MoS2 quantum dot served as the absorber, with FTO as the anode and silver as the back metal contact. The CFTS material outperformed the others, yielding a PCE of 25.86%, a fill factor (FF) of 38.79%, a short-circuit current density (JSC) of 34.52 mA cm−2, and an open-circuit voltage (VOC) of 1.93 V. This study contributes to the advancement of high-performance QDSSCs. Full article
(This article belongs to the Section Solar Energy and Solar Cells)
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Figure 1
<p>(<b>a</b>) Solar cell device architecture and (<b>b</b>) the band alignment between the absorber, the proposed HTLs, and the metallic back contact (Ag).</p>
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<p>J-V curves of (<b>a</b>) CFTS-, (<b>b</b>) CZTSe-, (<b>c</b>) CNTS-, and (<b>d</b>) CZTSSe-based devices.</p>
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<p>J-V curves of (<b>a</b>) CFTS-, (<b>b</b>) CZTSe-, (<b>c</b>) CNTS-, and (<b>d</b>) CZTSSe-based devices.</p>
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<p>Quantum efficiencies of (<b>a</b>) CFTS-, (<b>b</b>) CZTSe-, (<b>c</b>) CNTS-, and (<b>d</b>) CZTSSe-based devices.</p>
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<p>MoS<sub>2</sub> thickness variation with respect to PCE, FF, J<sub>SC</sub>, and V<sub>OC</sub> in different HTL materials (<b>a</b>) CFTS-, (<b>b</b>) CZTSe-, (<b>c</b>) CNTS-, and (<b>d</b>) CZTSSe-based devices.</p>
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<p>Variation of photovoltaic parameters for devices by changing defect density of an absorber in a range of 1 × 10<sup>11</sup> to 1 × 10<sup>17</sup> for devices with different HTLs: (<b>a</b>) PCE, (<b>b</b>) FF, (<b>c</b>) V<sub>oc</sub>, and (<b>d</b>) J<sub>sc.</sub></p>
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<p>Effect of variation of ETL donor density from 1 × 10<sup>14</sup> to 1 × 10<sup>20</sup> cm<sup>−3</sup> of devices with TiO<sub>2</sub> as the ETL and different HTLs: (<b>a</b>) PCE, (<b>b</b>) FF, (<b>c</b>) V<sub>oc</sub>, and (<b>d</b>) J<sub>sc</sub>.</p>
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<p>The influence of temperature of the devices containing TiO<sub>2</sub> as ETL, MoS<sub>2</sub> as an absorber, and different HTL materials: (<b>a</b>) PCE, (<b>b</b>) FF, (<b>c</b>) V<sub>oc</sub>, and (<b>d</b>) J<sub>sc</sub>.</p>
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<p>The influence of bandgap energy of the devices containing TiO<sub>2</sub> as ETL, MoS<sub>2</sub> as an absorber, and different HTL materials: (<b>a</b>) PCE, (<b>b</b>) FF, (<b>c</b>) V<sub>oc</sub>, and (<b>d</b>) J<sub>sc.</sub></p>
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<p>The influence of bandgap energy of the devices containing TiO<sub>2</sub> as ETL, MoS<sub>2</sub> as an absorber, and different HTL materials: (<b>a</b>) PCE, (<b>b</b>) FF, (<b>c</b>) V<sub>oc</sub>, and (<b>d</b>) J<sub>sc.</sub></p>
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33 pages, 6495 KiB  
Review
A Review of Transparent Conducting Films (TCFs): Prospective ITO and AZO Deposition Methods and Applications
by Jessica Patel, Razia Khan Sharme, Manuel A. Quijada and Mukti M. Rana
Nanomaterials 2024, 14(24), 2013; https://doi.org/10.3390/nano14242013 - 14 Dec 2024
Viewed by 444
Abstract
This study offers a comprehensive summary of the current states as well as potential future directions of transparent conducting oxides (TCOs), particularly tin-doped indium oxide (ITO), the most readily accessible TCO on the market. Solar cells, flat panel displays (FPDs), liquid crystal displays [...] Read more.
This study offers a comprehensive summary of the current states as well as potential future directions of transparent conducting oxides (TCOs), particularly tin-doped indium oxide (ITO), the most readily accessible TCO on the market. Solar cells, flat panel displays (FPDs), liquid crystal displays (LCDs), antireflection (AR) coatings for airbus windows, photovoltaic and optoelectronic devices, transparent p–n junction diodes, etc. are a few of the best uses for this material. Other conductive metals that show a lot of promise as substitutes for traditional conductive materials include copper, zinc oxide, aluminum, silver, gold, and tin. These metals are also utilized in AR coatings. The optimal deposition techniques for creating ITO films under the current conditions have been determined to be DC (direct current) and RF (radio frequency) MS (magnetron sputtering) deposition, both with and without the introduction of Ar gas. When producing most types of AR coatings, it is necessary to obtain thicknesses of at least 100 nm and minimum resistivities on the order of 10−4 Ω cm. For AR coatings, issues related to less-conductive materials than ITO have been considered. Full article
(This article belongs to the Section Nanophotonics Materials and Devices)
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Figure 1
<p>Schematic diagram of the e-beam evaporation system used to deposit ITO films. Reproduced from with permission from the copyright clearance center.</p>
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<p>The XRD patterns for the phase analysis of the ITO on Si films (<b>A</b>) as deposited and post-annealed at (<b>B</b>) 500 °C, (<b>C</b>) 600 °C, and (<b>D</b>) 700 °C. Reproduced from [<a href="#B37-nanomaterials-14-02013" class="html-bibr">37</a>] with permission from the copyright clearance center.</p>
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<p>Transmittance spectra for the ITO thin films as deposited and after annealing are displayed. Reproduced from [<a href="#B37-nanomaterials-14-02013" class="html-bibr">37</a>] with permission from the copyright clearance center.</p>
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<p>ITO’s electrical resistivity was measured, and its relationship to the post-annealing temperature was determined. Reproduced from [<a href="#B37-nanomaterials-14-02013" class="html-bibr">37</a>] with permission from the copyright clearance center.</p>
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<p>At three distinct post-annealing temperatures, surface roughness was measured for ITO thin films on Si using 3D AFM: (<b>a</b>) as deposited, (<b>b</b>) 500 °C, (<b>c</b>) 600 °C, and (<b>d</b>) 700 °C. Reproduced from [<a href="#B37-nanomaterials-14-02013" class="html-bibr">37</a>] with permission from the copyright clearance center.</p>
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<p>At three distinct post-annealing temperatures, surface roughness was measured for ITO thin films on Si using 3D AFM: (<b>a</b>) as deposited, (<b>b</b>) 500 °C, (<b>c</b>) 600 °C, and (<b>d</b>) 700 °C. Reproduced from [<a href="#B37-nanomaterials-14-02013" class="html-bibr">37</a>] with permission from the copyright clearance center.</p>
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<p>ITO films’ XRD patterns after being deposited and heated to various temperatures (<b>a</b>) in air and (<b>b</b>) under vacuum. Reproduced from [<a href="#B2-nanomaterials-14-02013" class="html-bibr">2</a>] with permission from the copyright clearance center.</p>
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<p>The transmittance spectra of the ITO thin films under diverse environmental conditions, including (<b>a</b>) in air and (<b>b</b>) under vacuum, at different temperatures during deposition and annealing. Reproduced from [<a href="#B2-nanomaterials-14-02013" class="html-bibr">2</a>] with permission from the copyright clearance center.</p>
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<p>Transmittances (%T) and resistivities (%R) of (<b>a</b>) Asahi ITO film and (<b>b</b>) conventional sol–gel ITO film (were measured and fitted. Reproduced from [<a href="#B45-nanomaterials-14-02013" class="html-bibr">45</a>] with permission from the copyright clearance center.</p>
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<p>Electrical resistivity and mobility (μ) spectra were calculated from the fit of the optical data in <a href="#nanomaterials-14-02013-f010" class="html-fig">Figure 10</a>b. Reproduced from [<a href="#B45-nanomaterials-14-02013" class="html-bibr">45</a>] with permission from the copyright clearance center.</p>
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<p>The heated ITO films’ XRD patterns, which were made from an aqueous solution with r = 0.030–0.15, are as follows: (<b>a</b>) from 20 to 60° and (<b>b</b>) from 28 to 33°. Reproduced from [<a href="#B44-nanomaterials-14-02013" class="html-bibr">44</a>] with permission from the copyright clearance center.</p>
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<p>Optical transmittance (%T) spectra (<b>a</b>) and annealing-temperature-dependent optical transmittance and bandgap (<b>b</b>,<b>c</b>) of inkjet-printed ITO thin films annealed at various temperatures. Reproduced from [<a href="#B47-nanomaterials-14-02013" class="html-bibr">47</a>] with permission from the copyright clearance center.</p>
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<p>XRD patterns of glass, ITO/NP–glass samples, and ITO/glass. Reproduced from [<a href="#B48-nanomaterials-14-02013" class="html-bibr">48</a>] with permission from the copyright clearance center.</p>
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<p>Variations in resistivity with substrate temperature for ITO films. Reproduced from [<a href="#B43-nanomaterials-14-02013" class="html-bibr">43</a>] with permission from copyright clearance center.</p>
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<p>XRD patterns of the AZO/Ag/AZO multilayer stacks on mica sheets at different annealing temperatures. Reproduced from [<a href="#B38-nanomaterials-14-02013" class="html-bibr">38</a>] with permission from the copyright clearance center.</p>
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<p>The AZO/Ag/AZO films’ optical transmittance (%T) spectra recorded at various annealing temperatures and for the as-deposited sample. Reproduced from [<a href="#B55-nanomaterials-14-02013" class="html-bibr">55</a>] with permission from the copyright clearance center.</p>
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<p>Resistivity and FOM values of AZO/Ag/AZO films for the as-deposited sample and different annealing temperatures. Reproduced from [<a href="#B55-nanomaterials-14-02013" class="html-bibr">55</a>] with permission from the copyright clearance center.</p>
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<p>Resistivity spatial distribution as a function of the film thickness for AZO thin films produced by RF-DC with H2 injection. Reproduced from [<a href="#B49-nanomaterials-14-02013" class="html-bibr">49</a>] with permission from the copyright clearance center.</p>
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<p>Resistivities of AZO films, made with different thicknesses via PLD, as a function of the exposure duration. Reproduced from [<a href="#B49-nanomaterials-14-02013" class="html-bibr">49</a>] with permission from the copyright clearance center.</p>
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