Engineering â€ș Electrical and Electronic Engineering

Chalcogenide Semiconductor Thin Films

Description

This cluster of papers focuses on the advancements in thin-film solar cell technology, particularly on materials such as CZTS and Kesterite, aiming to improve efficiency and device characteristics. It covers topics such as semiconductor properties, materials modelling, and the use of nanocrystals in thin-film solar cells.

Keywords

Thin-Film Solar Cells; Efficiency; CZTS; Kesterite; Photovoltaics; Semiconductor; Device Characteristics; Materials Modelling; Nanocrystals; Solar Cell Efficiency

We report on a new thin-film Cu(In,Ga)Se2 (CIGS) solar cell record efficiency of 21.7%. In order to better understand this newest development, we describe the specific solar cell data as 
 We report on a new thin-film Cu(In,Ga)Se2 (CIGS) solar cell record efficiency of 21.7%. In order to better understand this newest development, we describe the specific solar cell data as obtained from I–V measurement and diode analysis, quantum efficiency and secondary neutral mass spectrometry measurements. We hope that such a description will help to exploit the potential of this promising thin-film solar technology even further. (© 2015 WILEY-VCH Verlag GmbH &Co. KGaA, Weinheim)
ABSTRACT Using vacuum process, we fabricated Cu 2 ZnSnS 4 solar cells with 8.4% efficiency, a number independently certified by an external, accredited laboratory. This is the highest efficiency reported 
 ABSTRACT Using vacuum process, we fabricated Cu 2 ZnSnS 4 solar cells with 8.4% efficiency, a number independently certified by an external, accredited laboratory. This is the highest efficiency reported for pure sulfide Cu 2 ZnSnS 4 prepared by any method. Consistent with literature, the optimal composition is Cu‐poor and Zn‐rich despite the precipitation of secondary phases (e.g., ZnS). Despite a very thin absorber thickness (~600 nm), a reasonably good short‐circuit current was obtained. Time‐resolved photoluminescence measurements suggest a minority carrier‐diffusion length on the order of several hundreds of nanometers and relatively good collection of photo‐carriers across the entire absorber thickness. Copyright © 2011 John Wiley & Sons, Ltd.
Quaternary stannite-type semiconductor films of Cu 2 CdSnS 4 and Cu 2 ZnSnS 4 with (112) orientation were deposited on heated glass substrates using atom beam sputtering. These p-type films 
 Quaternary stannite-type semiconductor films of Cu 2 CdSnS 4 and Cu 2 ZnSnS 4 with (112) orientation were deposited on heated glass substrates using atom beam sputtering. These p-type films showed resistivities which were decreasing functions of the substrate temperature up to 240°C. The films had an absorption coefficient larger than 1 × 10 4 cm -1 in the visible wavelength range. The direct optical band gaps of the (112) oriented polycrystalline films were estimated as 1.06 eV and 1.45 eV for Cu 2 CdSnS 4 and Cu 2 ZnSnS 4 , respectively.
Abstract We report the growth and characterization of record‐efficiency ZnO/CdS/CuInGaSe 2 thin‐film solar cells. Conversion efficiencies exceeding 19% have been achieved for the first time, and this result indicates that 
 Abstract We report the growth and characterization of record‐efficiency ZnO/CdS/CuInGaSe 2 thin‐film solar cells. Conversion efficiencies exceeding 19% have been achieved for the first time, and this result indicates that the 20% goal is within reach. Details of the experimental procedures are provided, and material and device characterization data are presented. Published in 2003 by John Wiley & Sons, Ltd.
A 12.6% Cu2ZnSnSxSe4–x (CZTSSe) solar cell is presented with detailed device characteristics. Both short-circuit current density (Jsc) and open circuit voltage (Voc) increase in the 12.6% champion, relative to previous 
 A 12.6% Cu2ZnSnSxSe4–x (CZTSSe) solar cell is presented with detailed device characteristics. Both short-circuit current density (Jsc) and open circuit voltage (Voc) increase in the 12.6% champion, relative to previous devices, due to better bulk CZTSSe quality and improved optical architecture. The reduction in Voc deficit shows opportunities to push CZTSSe solar cells to higher efficiency.
A comprehensive survey of the total valence-band x-ray-photoemission spectra of 14 semiconductors is reported. The x-ray photoelectron spectra of cubic GaP, GaAs, GaSb, InP, InAs, InSb, ZnS, ZnSe, ZnTe, CdTe, 
 A comprehensive survey of the total valence-band x-ray-photoemission spectra of 14 semiconductors is reported. The x-ray photoelectron spectra of cubic GaP, GaAs, GaSb, InP, InAs, InSb, ZnS, ZnSe, ZnTe, CdTe, and HgTe, and of hexagonal ZnO, CdS, and CdSe were obtained from freshly cleaved single crystals, in the 0-50-eV binding-energy range, using monochromatized $\mathrm{Al} K\ensuremath{\alpha}$ (1486.6 eV) radiation. The binding energies of the outermost $d$ shells are reported. They were determined relative both to the top of the valence bands (${E}_{B}^{V}$) and to the Fermi level of a thin layer of gold that was vapor deposited after each run (${E}_{B}^{F}$). These data also yielded accurate measures of sample charging. The Fermi level fell near the center of the gap for six samples, near the top for two, and near the bottom for three. Evidence for an apparent increase in core $d$-level spin-orbit splitting over free-atom values was interpreted as a possible spreading of a ${\ensuremath{\Gamma}}_{7}$ and a ${\ensuremath{\Gamma}}_{8}$ level from the upper $({d}_{\frac{3}{2}}) {\ensuremath{\Gamma}}_{8}$ level by a tetrahedral crystal field. The $s$, $p$ valence-band spectra showed three main peaks, with considerable structure on the "least-bound" peak. A discussion is given of the validity of comparing the valence-band (VB) spectrum ${I}^{\ensuremath{'}}(E)$ with the VB density of states, including cross-section modulation, final-state modulation, and relaxation effects. Characteristic binding energies of spectral features in ${I}^{\ensuremath{'}}(E)$ are tabulated. In addition, the energies of the characteristic symmetry points ${L}_{3}$, ${X}_{5}$, ${W}_{2}$, ${\ensuremath{\Sigma}}_{1}^{min}$, ${W}_{1}$, ${X}_{3}({L}_{1})$, ${X}_{1}$, ${L}_{1}$, and ${\ensuremath{\Gamma}}_{1}$ are given for the 11 cubic compounds. These are compared with UPS results where available and with theoretical band-structure results where available. The energies calculated using the relativistic-orthogonalized-plane-wave approach with ${X}_{\ensuremath{\alpha}\ensuremath{\beta}}$ exchange agree very well with experiment, on the whole. In particular, they predict the important "ionicity gap" ${X}_{3}\ensuremath{-}{X}_{1}$ quite accurately. The densities of states calculated using the empirical-psuedopotential method provided a useful basis for relating features in ${I}^{\ensuremath{'}}(E)$ to energies of the characteristic symmetry points. Band-structure calculations in combination with x-ray-photoemission spectra appear to provide a very powerful approach to establishing the total valence-band structure of semiconductors.
This letter describes the fabrication and characteristics of high-efficiency thin-film CdS/CdTe heterojunction solar cells. CdS films have been prepared by chemical bath deposition and p-CdTe films have been deposited by 
 This letter describes the fabrication and characteristics of high-efficiency thin-film CdS/CdTe heterojunction solar cells. CdS films have been prepared by chemical bath deposition and p-CdTe films have been deposited by close-spaced sublimation. A CdS/CdTe solar cell of greater than 1 cm2 area with an AM1.5 efficiency of 15.8% is reported.
Using self-consistent band-structure methods, we analyze the remarkable anomalies (>50%) in the energy-band gaps of the ternary $\mathrm{I}B\ensuremath{-}\mathrm{I}\mathrm{I}\mathrm{I}A\ensuremath{-}\mathrm{V}\mathrm{I}{A}_{2}$ chalcopyrite semiconductors (e.g., CuGa${\mathrm{S}}_{2}$) relative to their binary zinc-blende analogs $\mathrm{II}B\ensuremath{-}\mathrm{V}\mathrm{I}A$ (e.g., 
 Using self-consistent band-structure methods, we analyze the remarkable anomalies (>50%) in the energy-band gaps of the ternary $\mathrm{I}B\ensuremath{-}\mathrm{I}\mathrm{I}\mathrm{I}A\ensuremath{-}\mathrm{V}\mathrm{I}{A}_{2}$ chalcopyrite semiconductors (e.g., CuGa${\mathrm{S}}_{2}$) relative to their binary zinc-blende analogs $\mathrm{II}B\ensuremath{-}\mathrm{V}\mathrm{I}A$ (e.g., ZnS), in terms of a chemical factor $\ensuremath{\Delta}{E}_{g}^{\mathrm{chem}}$ and a structural factor $\ensuremath{\Delta}{E}_{g}^{S}$. We show that $\ensuremath{\Delta}{E}_{g}^{\mathrm{chem}}$ is controlled by a $p\ensuremath{-}d$ hybridization effect $\ensuremath{\Delta}{E}_{g}^{d}$ and by a cation electronegativity effect $D{E}_{g}^{\mathrm{CE}}$, whereas the structural contribution to the anomaly is controlled by the existence of bond alternation (${R}_{\mathrm{AC}}\ensuremath{\ne}{R}_{\mathrm{BC}}$) in the ternary system, manifested by nonideal anion displacements $u\ensuremath{-}\frac{1}{4}\ensuremath{\ne}0$. All contributions are calculated self-consistently from band-structure theory, and are in good agreement with experiment. We further show how the nonideal anion displacement and the cubic lattice constants of all ternary chalcopyrites can be obtained from elemental coordinates (atomic radii) without using ternary-compound experimental data. This establishes a relationship between the electronic anomalies and the atomic sizes in these systems.
ADVERTISEMENT RETURN TO ISSUEPREVArticleNEXTSemiconductor crystallites: a class of large moleculesMichael L. Steigerwald and Louis E. BrusCite this: Acc. Chem. Res. 1990, 23, 6, 183–188Publication Date (Print):June 1, 1990Publication History Published 
 ADVERTISEMENT RETURN TO ISSUEPREVArticleNEXTSemiconductor crystallites: a class of large moleculesMichael L. Steigerwald and Louis E. BrusCite this: Acc. Chem. Res. 1990, 23, 6, 183–188Publication Date (Print):June 1, 1990Publication History Published online1 May 2002Published inissue 1 June 1990https://pubs.acs.org/doi/10.1021/ar00174a003https://doi.org/10.1021/ar00174a003research-articleACS PublicationsRequest reuse permissionsArticle Views3727Altmetric-Citations848LEARN ABOUT THESE METRICSArticle Views are the COUNTER-compliant sum of full text article downloads since November 2008 (both PDF and HTML) across all institutions and individuals. These metrics are regularly updated to reflect usage leading up to the last few days.Citations are the number of other articles citing this article, calculated by Crossref and updated daily. Find more information about Crossref citation counts.The Altmetric Attention Score is a quantitative measure of the attention that a research article has received online. Clicking on the donut icon will load a page at altmetric.com with additional details about the score and the social media presence for the given article. Find more information on the Altmetric Attention Score and how the score is calculated. Share Add toView InAdd Full Text with ReferenceAdd Description ExportRISCitationCitation and abstractCitation and referencesMore Options Share onFacebookTwitterWechatLinked InRedditEmail Other access optionsGet e-Alertsclose Get e-Alerts
Chalcopyrite copper indium sulfide (CuInS2) and copper indium gallium selenide (Cu(InxGa1-x)Se2; CIGS) nanocrystals ranging from ∌5 to ∌25 nm in diameter were synthesized by arrested precipitation in solution. The In/Ga 
 Chalcopyrite copper indium sulfide (CuInS2) and copper indium gallium selenide (Cu(InxGa1-x)Se2; CIGS) nanocrystals ranging from ∌5 to ∌25 nm in diameter were synthesized by arrested precipitation in solution. The In/Ga ratio in the CIGS nanocrystals could be controlled by varying the In/Ga reactant ratio in the reaction, and the optical properties of the CuInS2 and CIGS nanocrystals correspond to those of the respective bulk materials. Using methods developed to produce uniform, crack-free micrometer-thick films, CuInSe2 nanocrystals were tested in prototype photovoltaic devices. As a proof-of-concept, the nanocrystal-based devices exhibited a reproducible photovoltaic response.
Abstract In this contribution, we present a new certified world record efficiency of 20.1 and 20.3% for Cu(In,Ga)Se 2 thin‐film solar cells. We analyse the characteristics of solar cells on 
 Abstract In this contribution, we present a new certified world record efficiency of 20.1 and 20.3% for Cu(In,Ga)Se 2 thin‐film solar cells. We analyse the characteristics of solar cells on such a performance level and demonstrate a high degree of reproducibility. Copyright © 2011 John Wiley & Sons, Ltd.
Abstract Characterization of amorphous Si, CdTe, and Cu(InGa)Se 2 ‐based thin‐film solar cells is described with focus on the deviations in device behavior from standard device models. Quantum efficiency (QE), 
 Abstract Characterization of amorphous Si, CdTe, and Cu(InGa)Se 2 ‐based thin‐film solar cells is described with focus on the deviations in device behavior from standard device models. Quantum efficiency (QE), current–voltage ( J – V ), and admittance measurements are reviewed with regard to aspects of interpretation unique to the thin‐film solar cells. In each case, methods are presented for characterizing parasitic effects common in these solar cells in order to identify loss mechanisms and reveal fundamental device properties. Differences between these thin‐film solar cells and idealized devices are largely due to a high density of defect states in the absorbing layers and to parasitic losses due to the device structure and contacts. There is also commonly a voltage‐dependent photocurrent collection which affects J – V and QE measurements. The voltage and light bias dependence of these measurements can be used to diagnose specific losses. Examples of how these losses impact the QE, J – V , and admittance characterization are shown for each type of solar cell. Copyright © 2004 John Wiley & Sons, Ltd.
This short communication reports on achieving 18·8% total-area conversion efficiency for a ZnO/CdS/Cu(In,Ga)Se2/Mo polycrystalline thin-film solar cell. We also report a 15%-efficient, Cd-free device fabricated via physical vapor deposition methods. 
 This short communication reports on achieving 18·8% total-area conversion efficiency for a ZnO/CdS/Cu(In,Ga)Se2/Mo polycrystalline thin-film solar cell. We also report a 15%-efficient, Cd-free device fabricated via physical vapor deposition methods. The Cd-free cell includes no buffer layer, and it is fabricated by direct deposition of ZnO on the Cu(In,Ga)Se2 thin-film absorber. Both results have been measured at the National Renewable Energy Laboratory under standard reporting conditions (1000 W/m2, 25°C, ASTM E 892 Global). The 18·8% conversion efficiency represents a new record for such devices (Notable Exceptions) and makes the 20% performance level by thin-film polycrystalline materials much closer to reality. We allude to the enhancement in performance of such cells as compared to previous record cells, and we discuss possible and realistic routes to enhance the performance toward the 20% efficiency level. Published in 1999 by John Wiley & Sons, Ltd. This article is a US government work and is in the public domain in the United States.
Advanced energy conversion and storage (ECS) devices (including fuel cells, photoelectrochemical water splitting cells, solar cells, Li-ion batteries and supercapacitors) are expected to play a major role in the development 
 Advanced energy conversion and storage (ECS) devices (including fuel cells, photoelectrochemical water splitting cells, solar cells, Li-ion batteries and supercapacitors) are expected to play a major role in the development of sustainable technologies that alleviate the energy and environmental challenges we are currently facing. The successful utilization of ECS devices depends critically on synthesizing new nanomaterials with merits of low cost, high efficiency, and outstanding properties. Recent progress has demonstrated that nanostructured metal chalcogenides (MCs) are very promising candidates for efficient ECS systems based on their unique physical and chemical properties, such as conductivity, mechanical and thermal stability and cyclability. In this review, we aim to provide a summary on the liquid-phase synthesis, modifications, and energy-related applications of nanostructured metal chalcogenide (MC) materials. The liquid-phase syntheses of various MC nanomaterials are primarily categorized with the preparation method (mainly 15 kinds of methods). To obtain optimized, enhanced or even new properties, the nanostructured MC materials can be modified by other functional nanomaterials such as carbon-based materials, noble metals, metal oxides, or MCs themselves. Thus, this review will then be focused on the recent strategies used to realize the modifications of MC nanomaterials. After that, the ECS applications of the MC/modified-MC nanomaterials have been systematically summarized based on a great number of successful cases. Moreover, remarks on the challenges and perspectives for future MC research are proposed (403 references).
Solar photovoltaics have great promise for a low-carbon future but remain expensive relative to other technologies. Greatly increased penetration of photovoltaics into global energy markets requires an expansion in attention 
 Solar photovoltaics have great promise for a low-carbon future but remain expensive relative to other technologies. Greatly increased penetration of photovoltaics into global energy markets requires an expansion in attention from designs of high-performance to those that can deliver significantly lower cost per kilowatt-hour. To evaluate a new set of technical and economic performance targets, we examine material extraction costs and supply constraints for 23 promising semiconducting materials. Twelve composite materials systems were found to have the capacity to meet or exceed the annual worldwide electricity consumption of 17 000 TWh, of which nine have the potential for a significant cost reduction over crystalline silicon. We identify a large material extraction cost (cents/watt) gap between leading thin film materials and a number of unconventional solar cell candidates including FeS2, CuO, and Zn3P2. We find that devices performing below 10% power conversion efficiencies deliver the same lifetime energy output as those above 20% when a 3/4 material reduction is achieved. Here, we develop a roadmap emphasizing low-cost alternatives that could become a dominant new approach for photovoltaics research and deployment.
A composite liquid deposition approach merging the concepts of solution and particle-based coating for multinary chalcogenide materials is demonstrated. Photovoltaic absorbers based on earth-abundant Cu–Zn–Sn–S–Se kesterites show exceptional phase purity 
 A composite liquid deposition approach merging the concepts of solution and particle-based coating for multinary chalcogenide materials is demonstrated. Photovoltaic absorbers based on earth-abundant Cu–Zn–Sn–S–Se kesterites show exceptional phase purity and are incorporated into solar cells with power conversion efficiency above 9.6%, bringing the state of the art of kesterite photovoltaic materials to a level suitable for possible commercialization.
We studied the defect physics in ${\mathrm{CuInSe}}_{2},$ a prototype chalcopyrite semiconductor. We showed that (i) it takes much less energy to form a Cu vacancy in ${\mathrm{CuInSe}}_{2}$ than to form 
 We studied the defect physics in ${\mathrm{CuInSe}}_{2},$ a prototype chalcopyrite semiconductor. We showed that (i) it takes much less energy to form a Cu vacancy in ${\mathrm{CuInSe}}_{2}$ than to form cation vacancies in II-VI compounds (ii) defect formation energies vary considerably both with the Fermi energy and with the chemical potential of the atomic species, and (iii) the defect pairs such as $({2\mathrm{V}}_{\mathrm{Cu}}^{\mathrm{\ensuremath{-}}}{+\mathrm{I}\mathrm{n}}_{\mathrm{Cu}}^{2+})$ and $({2\mathrm{C}\mathrm{u}}_{\mathrm{In}}^{2\mathrm{\ensuremath{-}}}{+\mathrm{I}\mathrm{n}}_{\mathrm{Cu}}^{2+})$ have particularly low formation energies (under certain conditions, even exothermic). Using (i)--(iii), we (a) explain the existence of unusual ordered compounds ${\mathrm{CuIn}}_{5}{\mathrm{Se}}_{8},$ ${\mathrm{CuIn}}_{3}{\mathrm{Se}}_{5},$ ${\mathrm{Cu}}_{2}{\mathrm{In}}_{4}{\mathrm{Se}}_{7},$ and ${\mathrm{Cu}}_{3}{\mathrm{In}}_{5}{\mathrm{Se}}_{9}$ as a repeat of a single unit of $({2\mathrm{V}}_{\mathrm{Cu}}^{\mathrm{\ensuremath{-}}}{+\mathrm{I}\mathrm{n}}_{\mathrm{Cu}}^{2+})$ pairs for each $n=4,$ 5, 7, and 9 units, respectively, of ${\mathrm{CuInSe}}_{2};$ (b) attribute the very efficient $p$-type self-doping ability of ${\mathrm{CuInSe}}_{2}$ to the exceptionally low formation energy of the shallow defect Cu vacancies; (c) explained in terms of an electronic passivation of the ${\mathrm{In}}_{\mathrm{Cu}}^{2+}$ by ${2\mathrm{V}}_{\mathrm{Cu}}^{\mathrm{\ensuremath{-}}}$ the electrically benign character of the large defect population in ${\mathrm{CuInSe}}_{2}.$ Our calculation leads to a set of new assignment of the observed defect transition energy levels in the band gap. The calculated level positions agree rather well with available experimental data.
Earth abundant copper-zinc-tin-chalcogenide (CZTSSe) is an important class of material for the development of low cost and sustainable thin film solar cells. The fabrication of CZTSSe solar cells by selenization 
 Earth abundant copper-zinc-tin-chalcogenide (CZTSSe) is an important class of material for the development of low cost and sustainable thin film solar cells. The fabrication of CZTSSe solar cells by selenization of CZTS nanocrystals is presented. By tuning the composition of the CZTS nanocrystals and developing a robust film coating method, a total area efficiency as high as 7.2% under AM 1.5 illumination and light soaking has been achieved.
Titanium dioxide (TiO2) doped with sulfur (S) was synthesized by oxidation annealing of titanium disulfide (TiS2). According to the x-ray diffraction patterns, TiS2 turned into anatase TiO2 when annealed at 
 Titanium dioxide (TiO2) doped with sulfur (S) was synthesized by oxidation annealing of titanium disulfide (TiS2). According to the x-ray diffraction patterns, TiS2 turned into anatase TiO2 when annealed at 600 °C. The residual S atoms occupied O-atom sites in TiO2 to form Ti–S bonds. The S doping caused the absorption edge of TiO2 to be shifted into the lower-energy region. Based on the theoretical analyses using ab initio band calculations, mixing of the S 3p states with the valence band was found to contribute to the band gap narrowing.
Femtosecond transient absorption in the visible and infrared spectral ranges has been applied to study carrier dynamics and mechanisms for resonant optical nonlinearities in CdSe nanocrystals (NCs) with a variety 
 Femtosecond transient absorption in the visible and infrared spectral ranges has been applied to study carrier dynamics and mechanisms for resonant optical nonlinearities in CdSe nanocrystals (NCs) with a variety of surface passivations. Sequential filling of the 1S, 1P, and 1D atomic-like electron orbitals, governed by Fermi statistics, is clearly observed in the NC bleaching spectra recorded at progressively higher pump intensities. We observe that electron−hole (e−h) spatial separation strongly affects electron intraband dynamics. Such dependence indicates a nonphonon energy relaxation mechanism involving e−h interactions. A strong difference in electron and hole relaxation behavior in the stage following initial intraband relaxation is observed. In contrast to electron relaxation, which is sensitive to the quality of surface passivation (i.e., is affected by trapping at surface defects), depopulation dynamics of the initially-excited hole states are identical in NCs with different surface properties, suggesting that these dynamics are due to relaxation into intrinsic NC states. In the regime of multiparticle excitation, a quantization of relaxation rates corresponding to different multiple e−h pair states is observed. This effect is explained in terms of quantum-confined Auger recombination.
ABSTRACT Consolidated tables showing an extensive listing of the highest independently confirmed efficiencies for solar cells and modules are presented. Guidelines for inclusion of results into these tables are outlined, 
 ABSTRACT Consolidated tables showing an extensive listing of the highest independently confirmed efficiencies for solar cells and modules are presented. Guidelines for inclusion of results into these tables are outlined, and new entries since July 2011 are reviewed. Copyright © 2011 John Wiley & Sons, Ltd.
Abstract Thin film solar cells (TFSC) are a promising approach for terrestrial and space photovoltaics and offer a wide variety of choices in terms of the device design and fabrication. 
 Abstract Thin film solar cells (TFSC) are a promising approach for terrestrial and space photovoltaics and offer a wide variety of choices in terms of the device design and fabrication. A variety of substrates (flexible or rigid, metal or insulator) can be used for deposition of different layers (contact, buffer, absorber, reflector, etc.) using different techniques (PVD, CVD, ECD, plasma‐based, hybrid, etc.). Such versatility allows tailoring and engineering of the layers in order to improve device performance. For large‐area devices required for realistic applications, thin‐film device fabrication becomes complex and requires proper control over the entire process sequence. Proper understanding of thin‐film deposition processes can help in achieving high‐efficiency devices over large areas, as has been demonstrated commercially for different cells. Research and development in new, exotic and simple materials and devices, and innovative, but simple manufacturing processes need to be pursued in a focussed manner. Which cell(s) and which technologies will ultimately succeed commercially continue to be anybody's guess, but it would surely be determined by the simplicity of manufacturability and the cost per reliable watt. Cheap and moderately efficient TFSC are expected to receive a due commercial place under the sun. Copyright © 2004 John Wiley & Sons, Ltd.
Two-dimensional (2D) semiconductor nanomaterials hold great promises for future electronics and optics. In this paper, a 2D nanosheets of ultrathin GaSe has been prepared by using mechanical cleavage and solvent 
 Two-dimensional (2D) semiconductor nanomaterials hold great promises for future electronics and optics. In this paper, a 2D nanosheets of ultrathin GaSe has been prepared by using mechanical cleavage and solvent exfoliation method. Single- and few-layer GaSe nanosheets are exfoliated on an SiO2/Si substrate and characterized by atomic force microscopy and Raman spectroscopy. Ultrathin GaSe-based photodetector shows a fast response of 0.02 s, high responsivity of 2.8 AW–1 and high external quantum efficiency of 1367% at 254 nm, indicating that the two-dimensional nanostructure of GaSe is a new promising material for high performance photodetectors.
Abstract We report a new record total‐area efficiency of 19·9% for CuInGaSe 2 ‐based thin‐film solar cells. Improved performance is due to higher fill factor. The device was made by 
 Abstract We report a new record total‐area efficiency of 19·9% for CuInGaSe 2 ‐based thin‐film solar cells. Improved performance is due to higher fill factor. The device was made by three‐stage co‐evaporation with a modified surface termination. Growth conditions, device analysis, and basic film characterization are presented. Published in 2008 by John Wiley & Sons, Ltd.
Consolidated tables showing an extensive listing of the highest independently confirmed efficiencies for solar cells and modules are presented. Guidelines for inclusion of results into these tables are outlined and 
 Consolidated tables showing an extensive listing of the highest independently confirmed efficiencies for solar cells and modules are presented. Guidelines for inclusion of results into these tables are outlined and new entries since July 2014 are reviewed. Copyright © 2014 John Wiley & Sons, Ltd.
A world-record CZTSSe device is reported, surpassing 11% power conversion efficiency for the first time. The results reflect not only higher efficiency, but also other improved device characteristics, such as 
 A world-record CZTSSe device is reported, surpassing 11% power conversion efficiency for the first time. The results reflect not only higher efficiency, but also other improved device characteristics, such as fill factor and short circuit current. The improvement in CZTSSe devices continues to point to significant promise for the kesterite-based absorbers.
The kesterite-structured semiconductors Cu2ZnSnS4 and Cu2ZnSnSe4 are drawing considerable attention recently as the active layers in earth-abundant low-cost thin-film solar cells. The additional number of elements in these quaternary compounds, 
 The kesterite-structured semiconductors Cu2ZnSnS4 and Cu2ZnSnSe4 are drawing considerable attention recently as the active layers in earth-abundant low-cost thin-film solar cells. The additional number of elements in these quaternary compounds, relative to binary and ternary semiconductors, results in increased flexibility in the material properties. Conversely, a large variety of intrinsic lattice defects can also be formed, which have important influence on their optical and electrical properties, and hence their photovoltaic performance. Experimental identification of these defects is currently limited due to poor sample quality. Here recent theoretical research on defect formation and ionization in kesterite materials is reviewed based on new systematic calculations, and compared with the better studied chalcopyrite materials CuGaSe2 and CuInSe2 . Four features are revealed and highlighted: (i) the strong phase-competition between the kesterites and the coexisting secondary compounds; (ii) the intrinsic p-type conductivity determined by the high population of acceptor CuZn antisites and Cu vacancies, and their dependence on the Cu/(Zn+Sn) and Zn/Sn ratio; (iii) the role of charge-compensated defect clusters such as [2CuZn +SnZn ], [VCu +ZnCu ] and [ZnSn +2ZnCu ] and their contribution to non-stoichiometry; (iv) the electron-trapping effect of the abundant [2CuZn +SnZn ] clusters, especially in Cu2ZnSnS4. The calculated properties explain the experimental observation that Cu poor and Zn rich conditions (Cu/(Zn+Sn) ≈ 0.8 and Zn/Sn ≈ 1.2) result in the highest solar cell efficiency, as well as suggesting an efficiency limitation in Cu2ZnSn(S,Se)4 cells when the S composition is high.
Abstract In this study, the Mo-electrode thin films were deposited by a two-stepped process, and the high-purity copper indium selenide-based powder (CuInSe 2 , CIS) was fabricated by hydrothermal process 
 Abstract In this study, the Mo-electrode thin films were deposited by a two-stepped process, and the high-purity copper indium selenide-based powder (CuInSe 2 , CIS) was fabricated by hydrothermal process by Nanowin Technology Co. Ltd. From the X-ray pattern of the CIS precursor, the mainly crystalline phase was CIS, and the almost undetectable CuSe phase was observed. Because the CIS powder was aggregated into micro-scale particles and the average particle sizes were approximately 3 to 8 ÎŒm, the CIS power was ground into nano-scale particles, then the 6 wt.% CIS particles were dispersed into isopropyl alcohol to get the solution for spray coating method. Then, 0.1 ml CIS solution was sprayed on the 20 mm × 10 mm Mo/glass substrates, and the heat treatment for the nano-scale CIS solution under various parameters was carried out in a selenization furnace. The annealing temperature was set at 550°C, and the annealing time was changed from 5 to 30 min, without extra Se content was added in the furnace. The influences of annealing time on the densification, crystallization, resistivity ( ρ ), hall mobility ( ÎŒ ), and carrier concentration of the CIS absorber layers were well investigated in this study.
Recent developments in photovoltaic materials have led to continual improvements in their efficiency. We review the electrical characteristics of 16 widely studied geometries of photovoltaic materials with efficiencies of 10 
 Recent developments in photovoltaic materials have led to continual improvements in their efficiency. We review the electrical characteristics of 16 widely studied geometries of photovoltaic materials with efficiencies of 10 to 29%. Comparison of these characteristics to the fundamental limits based on the Shockley-Queisser detailed-balance model provides a basis for identifying the key limiting factors, related to efficient light management and charge carrier collection, for these materials. Prospects for practical application and large-area fabrication are discussed for each material.
We report on the use and effect of the alkali elements rubidium and caesium in the place of sodium and potassium in the alkali post deposition treatment (PDT) as applied 
 We report on the use and effect of the alkali elements rubidium and caesium in the place of sodium and potassium in the alkali post deposition treatment (PDT) as applied to Cu(In,Ga)Se 2 (CIGS) solar cell absorbers. In order to study the effects of the different alkali elements, we have produced a large number of CIGS solar cells with high efficiencies resulting in a good experimental resolution to detect even small differences in performance. We examine the electrical device parameters of these fully functional devices and observe a positive trend in the I – V parameters when moving from devices without PDT to KF‐, RbF‐, and eventually to CsF‐PDT. A diode analysis reveals an improved diode quality for cells treat‐ed with heavier alkalis. Furthermore, secondary ion mass spectrometry (SIMS) measurements reveal a competitive mechanism induced within the class of alkali elements in the CIGS absorber induced by the alkali post deposition treatment. (© 2016 WILEY‐VCH Verlag GmbH &Co. KGaA, Weinheim)
Abstract Consolidated tables showing an extensive listing of the highest independently confirmed efficiencies for solar cells and modules are presented. Guidelines for inclusion of results into these tables are outlined, 
 Abstract Consolidated tables showing an extensive listing of the highest independently confirmed efficiencies for solar cells and modules are presented. Guidelines for inclusion of results into these tables are outlined, and new entries since January 2017 are reviewed.
Abstract Consolidated tables showing an extensive listing of the highest independently confirmed efficiencies for solar cells and modules are presented. Guidelines for inclusion of results into these tables are outlined, 
 Abstract Consolidated tables showing an extensive listing of the highest independently confirmed efficiencies for solar cells and modules are presented. Guidelines for inclusion of results into these tables are outlined, and new entries since January 2019 are reviewed.
In this article, the excellent properties of state-of-the-art Cd-free Cu(In,Ga)(Se,S) <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> (CIGSSe) solar cells with Zn(O,S,OH) <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">x</sub> /Zn <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">0.8</sub> Mg <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">0.2</sub> O 
 In this article, the excellent properties of state-of-the-art Cd-free Cu(In,Ga)(Se,S) <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sub> (CIGSSe) solar cells with Zn(O,S,OH) <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">x</sub> /Zn <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">0.8</sub> Mg <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">0.2</sub> O double buffer layers, deposited by a combination of chemical bath deposition and atomic layer deposition techniques, are presented. By the replacement of conventional CdS buffer layers with this double buffer layer, the open-circuit voltage (V <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">oc</sub> ) deficit of the devices could be significantly reduced, and V <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">oc</sub> increased by approximately 15 mV. In addition, the fill factor and short-circuit current were also improved, increasing the device efficiency by approximately 0.5 absolute percent compared with devices with CdS buffers. The Cd-free double buffer layer improved the device efficiency regardless of the bandgap of the CIGSSe absorber. The minority carrier lifetime (τ) measured via time-resolved photoluminescence became longer, indicating that carrier recombination is mitigated using the double buffer layer. Based on the device parameters extracted by fitting the Suns-V <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">oc</sub> characteristics to the double-diode model, the longer τ could be attributed to the decreased recombination rate in the space-charge region, rather than in the bulk and at the interface. The best performing cell was evaluated by a reliable third party, the National Institute of Advanced Industrial Science and Technology; this cell achieved a new world record efficiency of 23.35% for 1-cm <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sup> -sized thin-film polycrystalline solar cells. The device parameters of this cell are also discussed in this article.
Abstract Consolidated tables showing an extensive listing of the highest independently confirmed efficiencies for solar cells and modules are presented. Guidelines for inclusion of results into these tables are outlined, 
 Abstract Consolidated tables showing an extensive listing of the highest independently confirmed efficiencies for solar cells and modules are presented. Guidelines for inclusion of results into these tables are outlined, and new entries since June 2020 are reviewed. In this issue, charts showing efficiency improvements since 1993 are included as well as cell and module area definitions and an updated list of recognized test centres.
The direct synthesis of wafer-scale single-crystal transition metal dichalcogenides (TMDs) remains challenging, albeit with enormous potential applications as semiconductors. In this work, we demonstrate the feasibility of using single-crystal 2H-MoTe2 
 The direct synthesis of wafer-scale single-crystal transition metal dichalcogenides (TMDs) remains challenging, albeit with enormous potential applications as semiconductors. In this work, we demonstrate the feasibility of using single-crystal 2H-MoTe2 films as templates, followed by a sequential selenium substitution reaction to synthesize a variety of TMDs and their heterostructures. We also demonstrate the synthesis of a MoTe2/MoSe2 lateral heterostructure with various substitution temperatures for Se substitution in 1T' and 2H phase MoTe2. Computational results illustrate that Se substitution is likely to start at Te vacancy sites, where generated strain lowers the energy barrier for further substitution, leading to a chain reaction that propagates until the entire layer is selenized. The obtained MoSe2 shows a high hole mobility of 32 cm2 V-1 s-1, comparable to the 2.8-31.6 range from mechanically exfoliated samples. Consequently, this MoSe2-based photodetector shows a comparable responsivity of 41 mA W-1 under near-infrared (1060 nm) illumination.
Nanoparticles of transition metal dichalcogenides, including tellurides, are widely used for their dimension- and size-dependent electronic, magnetic, optical, and catalytic properties. Additional tunability can emerge from high-entropy compositions, where five 
 Nanoparticles of transition metal dichalcogenides, including tellurides, are widely used for their dimension- and size-dependent electronic, magnetic, optical, and catalytic properties. Additional tunability can emerge from high-entropy compositions, where five or more metals randomly mix on the crystalline lattice sites. Colloidal routes for synthesizing transition metal ditelluride nanoparticles can be challenging, as can achieving high-entropy mixing in colloidal nanoparticles. Here, we present three complementary strategies for synthesizing colloidal nanoparticles of high-entropy transition metal ditellurides that adopt a layered MTe2 structure. First, we react high-entropy NiPdPtRhIr alloy nanoparticles with diphenyl ditelluride, which maintains the high-entropy mixing upon transformation to (NiPdPtRhIr)Te2. However, this approach is limited in the compositional scope due to crystal structure considerations. To circumvent this limitation and to produce the high-entropy tellurides (SnPdPtRhIr)Te2 and (SnNiPtRhIr)Te2 in addition to (NiPdPtRhIr)Te2, the second strategy involves direct colloidal synthesis without first forming high-entropy alloy intermediates. Third, preformed Te particles can also transform into MTe2 high-entropy tellurides by diffusing metal reagents into them. These three strategies, which are complementary in their capabilities and limitations, provide insights for targeting the synthesis of high-entropy transition metal ditelluride nanoparticles.
Vacancies of Se and Sb are the most detrimental deep-level defects in the Sb2Se3 film. Herein, an approach is proposed to passivate the Sb vacancies using Al3+ ions. The tris(8-hydroxy-quinolinato) 
 Vacancies of Se and Sb are the most detrimental deep-level defects in the Sb2Se3 film. Herein, an approach is proposed to passivate the Sb vacancies using Al3+ ions. The tris(8-hydroxy-quinolinato) aluminum (Alq3) is employed as the Al3+ source, which is buried between indium tin oxide (ITO) and Sb2Se3. Additionally, the incorporation of the Alq3 layer not only inhibits the chemical reaction between Sb2Se3 and ITO but also lowers the contact barrier. As a result, the open-circuit voltage increases from 0.34 to 0.43 V, and the power conversion efficiency rises from 3.3% to 5.1%. Notably, our finding confirms that the grain boundary in the Sb2Se3 film with (020) preferred orientation is harmless and does not induce significant carrier recombination. The device is fabricated by conventional vacuum thermal evaporation. This study offers insights into enhancing the efficiency of Sb2Se3 solar cells.
The effects of vacancy defects and biaxial strain on the magnetism of α-Te are investigated using first-principles calculations. The calculated results show that the vacancy defects induce significant magnetism in 
 The effects of vacancy defects and biaxial strain on the magnetism of α-Te are investigated using first-principles calculations. The calculated results show that the vacancy defects induce significant magnetism in α-Te: VTe1m and VTe7 defects generate magnetic moments of 3 ÎŒB and 2 ÎŒB, respectively. The density of states analysis reveals that vacancy defects introduce impurity subbands. While biaxial strain is taken into account, VTe1m exhibits a maximum magnetic moment of 3.8 ÎŒB at 4% strain and VTe7 also exhibits a maximum magnetic moment of 3.2 ÎŒB at −2% strain. Interestingly, magnetism is quenched at critical strain values (4% compression and 1% tension for VTe1m; −3% and 0% for VTe7). This study provides a theoretical foundation for designing α-Te-based spintronic devices (such as multistate magnetic memory, strain-gradient spin logic devices, and high-sensitivity magnetoelectric sensors) by regulating magnetism through vacancy defects and strain engine.
Se-doped CdTe thin films were grown employing a simple two-electrode electrochemical deposition method using glass/tin-doped indium oxide (glass/ITO). Cadmium acetate dihydrate [Cd (CH3CO2)2. 2H2O], selenium dioxide (SeO2), and tellurium dioxide 
 Se-doped CdTe thin films were grown employing a simple two-electrode electrochemical deposition method using glass/tin-doped indium oxide (glass/ITO). Cadmium acetate dihydrate [Cd (CH3CO2)2. 2H2O], selenium dioxide (SeO2), and tellurium dioxide (TeO2) were used as precursors. Instruments including X-ray diffraction for structural investigation, UV-Vis spectrophotometry for optical properties, and scanning probe microscopy for morphological properties were employed to investigate the physico-chemical characteristics of the resulting Se-doped CdTe thin-film. The films are polycrystalline with a cubic phase, according to X-ray diffraction (XRD) data. More ions are deposited on the substrate, which makes the material more crystalline and intensifies the characteristic peaks that are seen. It is observed from the acquired optical characterization that the film’s bandgap is greatly influenced by the deposition time. The bandgap dropped from 1.92 to 1.62 as the deposition period increased from 25 to 45 min, making the film more transparent and absorbing less light at shorter deposition durations. Images from scanning electron microscopy (SEM) show that the surface morphology is homogenous with closely packed grains and that the grain forms become less noticeable as the deposition time increases. This work is novel in that it investigates the influence of the deposition time on the structural, optical, and morphological properties of Se-doped CdTe thin films deposited using a cost-effective, simplified two-electrode electrochemical method—a fabrication route that remains largely unexplored for this material system.
The thermodynamic stability and mixing behavior of the MoS₂-WS₂ system were investigated using a cluster expansion model constructed from density functional theory (DFT) calculations. The alloy cluster expansion approach enabled 
 The thermodynamic stability and mixing behavior of the MoS₂-WS₂ system were investigated using a cluster expansion model constructed from density functional theory (DFT) calculations. The alloy cluster expansion approach enabled the efficient sampling of atomic configurations, overcoming the computational limitations of direct DFT calculations. The accuracy of the cluster expansion model was validated against additional DFT calculations, achieving a root-mean-squared error close to 1.0 × 10⁻⁎ eV/atom and R2 = 0.74. The mixing energy landscape was analyzed to determine the existence of ordered ground-state structures and assess the stability of solid solutions. The results indicate that MoS₂-WS₂ forms a stable solid solution across the full compositional range, with specific ordering tendencies at a broad range of intermediate atomic concentrations of tungsten, from XW = 0.33 to 0.66. The constructed convex hull suggests a multitude of ground states in this range with ordering patterns of a single solute atom residing in a hexagon of solvent atoms within a single layer. Generally small mixing energy values imply a dominant role of entropy at synthesis temperatures. The findings provide insight into the thermodynamic factors governing mixing in transition metal dichalcogenide MoS₂-WS₂ solid solutions, contributing to the rational design of materials based on them.
Abstract Due to the weak interlayer interactions, the binary III-VI chalcogenides GaSe can exist in several distinct polymorphs. Among them, the so-called ÎČ- and Δ-phase simultaneously exhibit favorable total energies 
 Abstract Due to the weak interlayer interactions, the binary III-VI chalcogenides GaSe can exist in several distinct polymorphs. Among them, the so-called ÎČ- and Δ-phase simultaneously exhibit favorable total energies and moderate band gaps, which offer a good platform to explore their thermoelectric properties. Here, we demonstrate by first-principles calculations that the two systems have very similar band structures and phonon dispersions, despite with different stacking sequences between adjacent layers. Interestingly, the lattice thermal conductivity of Δ-GaSe is obviously lower than that of the ÎČ-GaSe, which is inherently tied with stronger lattice anharmonicity caused by bonding heterogeneity. Besides, both systems exhibit higher p -type power factors due to doubly degenerate bands with weaker dispersions around the valence band maximum. As a consequence, a significantly enhanced p -type ZT of 2.1 can be realized at 700 K along the out-of-plane direction of Δ-phase.
The present work revisits the recombination velocities (sGB) of minority-charge carriers determined at grain boundaries in polycrystalline absorber materials for solar cells. The equations describing sGB as well as the 
 The present work revisits the recombination velocities (sGB) of minority-charge carriers determined at grain boundaries in polycrystalline absorber materials for solar cells. The equations describing sGB as well as the barriers for electrons and holes were derived. It is shown that for given net-doping density and absolute temperature, the experimentally determined recombination velocity of a specific grain boundary can be described by sGB=sGB,0nexp⁥[−ΩGB(NGB,charge)/(kBT)], where ΊGB is the band bending induced by the excess-charge density NGB,charge at the grain boundary, and kB as well as T are the Boltzmann constant and the absolute temperature; i.e., sGB depends only on the excess-charge density at this planar defect as well as on the prefactor sGB,0n describing the nonradiative recombination. Value ranges for these two quantities can be determined for any measured sGB value. When analyzing sGB datasets acquired on various (Ag,Cu)(In,Ga)Se2 and microcrystalline Si absorbers, it is apparent that both the excess-charge density and the prefactor sGB,0n remain within about the same orders of magnitude for all grain boundaries analyzed in a specific absorber. The broad range of the recombination velocities over several orders of magnitude indicates upward as well as downward band bending, and the band-bending values are on the order of several ±10 meV for all materials analyzed.
Abstract The electrodeposition procedure was carried out utilizing a two-electrode system on fluorine-doped tin oxide (FTO) glass substrates, with the as-prepared thin film and various annealing temperatures for cadmium zirconium 
 Abstract The electrodeposition procedure was carried out utilizing a two-electrode system on fluorine-doped tin oxide (FTO) glass substrates, with the as-prepared thin film and various annealing temperatures for cadmium zirconium sulfide (CdZrS) thin films. On the synthesized thin films, the structural, surface morphology, elemental composition, surface roughness, and optical properties of the resulting films were studied by characterization techniques such as X-ray diffraction (XRD), scanning electron microscopy (SEM), energy dispersive spectrometry (EDS), scanning probe microscopy (SPM), and ultraviolet-visible spectroscopy (UV-vis) techniques. The XRD results revealed that CdZrS thin films exhibit the cubic phase. The crystallite size of the films fluctuated with an increase in annealing temperature. The SEM images show the hexagonal shape and white rod-like structures on the surface of the films. The EDS results confirmed the presence of all the expected elements for Cd, Zr, and S forming the desired compound of CdZrS. The surface roughness of the films decreased with an increase in annealing temperature from 250 - 550 ÂșC in the range of 36.67-21.81 nm compared to the as-prepared film. The UV-vis measurements show that the absorbance decreases with an increase in annealing temperature, and the energy bandgap increased from 2.22 - 2.31 eV at 250 - 450 ÂșC and suddenly decreased to 2.25 eV at 550 ÂșC. To maximize charge transport, light transmission, and solar device efficiency, the optimal window layer material for n-type thin films should have small, compatible crystallite sizes, low surface roughness, minimal absorbance, and a carefully chosen energy bandgap.&amp;#xD;
A simple electrochemical method called electrolysis was used in this research to create zinc oxide (ZnO) nanoparticles from zinc and gold electrodes in diluted hydrochloric acid solution. The process of 
 A simple electrochemical method called electrolysis was used in this research to create zinc oxide (ZnO) nanoparticles from zinc and gold electrodes in diluted hydrochloric acid solution. The process of electrolysis was performed with a constant voltage of 5 V over 30 minutes in a mixture of HCl and water 12.5 % . The nanoparticles of ZnO were characterized by examining them with XRD, SEM, AFM and UV-Visible spectroscopy. Analysis of the particles showed that hexagonal wurtzite-phase ZnO nanoparticles have an average size between 30 and 50 nm. Approximately 3.3 band gap was estimated for ZnO and the given spectroscopic data revealed another band gap of 4.2 eV which is likely because the sample contained ultra-small particles of ZnO. The procedure uses electrolysis which provides benefits such as low temperatures, friendliness to the environment and scalability, so it has potential for use in photocatalysis, gas sensing and optoelectronics.
The present work reports on microscopic analyses of recombination at grain boundaries (GBs) in polycrystalline Li‐doped (Ag,Cu) 2 ZnSn(S,Se) 4 (Li‐ACZTSSe) and Cu 2 ZnSnS 4 (CZTS) absorber layers in 
 The present work reports on microscopic analyses of recombination at grain boundaries (GBs) in polycrystalline Li‐doped (Ag,Cu) 2 ZnSn(S,Se) 4 (Li‐ACZTSSe) and Cu 2 ZnSnS 4 (CZTS) absorber layers in high‐efficiency solar cells (conversion efficiencies of 14.4% and 10.8%). Recombination velocities s GB were determined at a large number of GBs by evaluating profiles extracted from cathodoluminescence intensity distributions across GBs in these polycrystalline layers. In both Li‐ACZTSSe and CZTS absorber layers, the s GB values exhibited wide ranges over several orders of magnitude with a median values of 680 and 1100 cm s −1 for the Li‐ACZTSSe and CZTS absorbers. A model that provides a comprehensive explanation for this finding is presented and discussed in detail. Correspondingly, wide ranges for s GB can be explained by different positive or negative excess charge densities present at different GBs, leading to different downward or upward band bending on the order of several ±10 meV, provided that the net‐doping density of the absorber layers is sufficiently large. As a result of the evaluation of the s GB , input parameters for multidimensional device simulations are obtained. It is revealed that the grain boundary lifetime closely matches the overall effective lifetime, indicating that grain boundary recombination is a key factor limiting the effective carrier lifetime of both Li‐ACZTSSe and CZTS absorbers. The estimated V OC losses due to GBs reach up to 126 mV for Li‐ACZTSSe and 88 mV for CZTS. This work highlights that reducing grain boundary recombination via improved passivation and increasing grain size is an effective strategy for achieving further efficiency improvements.
Layered α-In2Se3 has been studied using a combined in situ synchrotron angle-dispersive powder x-ray diffraction and Raman spectroscopy study in a diamond anvil cell up to 60+ GPa, at room 
 Layered α-In2Se3 has been studied using a combined in situ synchrotron angle-dispersive powder x-ray diffraction and Raman spectroscopy study in a diamond anvil cell up to 60+ GPa, at room temperature. Helium, which remains fairly hydrostatic up to the highest pressure in this study, was used as the pressure-transmitting medium. The results from both experimental methods reveal a pressure-induced structural phase transition from α-In2Se3 to a monoclinic ÎČâ€Č-In2Se3 structure at ≈1 GPa, in agreement with previous studies. Based on our detailed measurements using both experimental techniques and the F–f formalism, the ÎČâ€Č-In2Se3 structure remains stable up to 45 GPa, without a clear indication of a phase transition toward the previously reported ÎČ-In2Se3 phase. Above this pressure, In2Se3 adopts a disordered solid-solution-like orthorhombic structure, phase IV. The results are discussed in comparison with the relevant previous studies of α-In2Se3 under pressure.
Abstract The resilience of chalcogenide-based solar cells (SCs) in space environment is crucial for their applications in satellite power systems. In this experimental study, we investigate the effects of 1 
 Abstract The resilience of chalcogenide-based solar cells (SCs) in space environment is crucial for their applications in satellite power systems. In this experimental study, we investigate the effects of 1 MeV proton irradiation at fluences ranging from 3×10^10 to 10^14 H^+/cm^2 on the optoelectronic properties of Cu(In,Ga)Se2 (CIGS) based SCs. In situ and ex situ electrical characterization revealed that irradiation causes degradation of the diode parameters and the electrical performance of the device, in particular the open-circuit voltage (VOC), fill factor (FF) and power conversion efficiency (η). Fluences above 10^13 H^+/cm^2 caused significant degradation of the solar cells. Keeping the SCs at room temperature, ambient atmosphere and in the dark did not contribute significantly to the SC recovery. The photoluminescence (PL) analysis revealed an increase in the defect density leading to the formation of deeper radiative recombination channels as well as non-radiative ones and an increase on the magnitude of the fluctuating potentials. In order to revert this degradation, we explored a heat light soaking (HLS) treatment that consisted in exposing the SCs to light incidence at temperature slightly above 90ÂșC. This treatment significantly restored the device’s electrical performance and the luminescence properties, demonstrating partial defect annihilation and restoration of the CIGS electronic structure. Interestingly, a non-irradiated SC subjected to the same HLS treatment showed no significant beneficial effect on the performance of the SC, which confirms the link between the observed recovery of the irradiated SCs and the annihilation of irradiation-induced defects. The findings of this work suggest that HLS is an effective, space-compatible self-healing mechanism that mitigates radiation damage in CIGS SCs, potentially enabling satellite SCs to be designed without cover glass.&amp;#xD;
Abstract This study investigates the crystallization process of amorphous Cu(In,Ga)Se 2 (CIGSe) through in-situ characterization techniques, specifically Raman spectroscopy, X-ray diffraction (XRD), and transmission electron microscopy (TEM). Amorphous CIGSe was 
 Abstract This study investigates the crystallization process of amorphous Cu(In,Ga)Se 2 (CIGSe) through in-situ characterization techniques, specifically Raman spectroscopy, X-ray diffraction (XRD), and transmission electron microscopy (TEM). Amorphous CIGSe was deposited through sputtering of a ternary target with simultaneous supply of selenium by evaporation. A Se capping layer revealed to enhance crystallization at lower temperatures, yielding larger crystallites at 400 °C and larger crystal grains after the crystallization process. The A 1 Raman mode of CIGSe appears at a lower temperature and with higher intensity in samples with Se capping compared to those without capping layer. The effect of temperature on the Raman spectra was considered by fitting post-crystallization data with a three-phonon coupling model, allowing for deconvolution of the thermal and material crystallization effects. In-situ XRD data corroborate the Raman data and revealed the formation of MoSe2 and Cu2Se secondary phases at 250 °C and 400 °C, respectively. Moreover, in-situ TEM allowed to further assess crystal growth during the crystallization process.
Abstract As a highly energy-efficient and sensitive radiation source, narrowband thermal emitters provide an ideal solution for non-contact gas detection, enabling the widespread application of mid-infrared "molecular fingerprint" technology. However, 
 Abstract As a highly energy-efficient and sensitive radiation source, narrowband thermal emitters provide an ideal solution for non-contact gas detection, enabling the widespread application of mid-infrared "molecular fingerprint" technology. However, most narrowband thermal emitters lack reconfigurability, limiting their adaptability in practical applications. In this study, we propose a novel dual-band switchable narrowband thermal emitter in the mid-infrared region. The emitter consists of an aperiodic Ge/SiO 2 /Ge/SiO 2 (GSGS) structure and a phase change material In 3 SbTe 2 (IST). When IST is in the crystalline state, the emitter achieves narrowband emission peaks at wavelengths of 3.79 ”m and 6.12 ”m, corresponding to the "on" state. However, when IST transitions to the amorphous state, the dual-band high emission disappears and it features angle- and polarization-independent behavior, representing the "off" state. Furthermore, we verify the physical mechanism behind the high emission through phase and amplitude calculations as well as electric field distribution analysis. Notably, the introduction of the IST provides an additional degree of freedom for tunability. Furthermore, by adjusting the thickness of the spacer layer, the emitter can be precisely tuned to match the characteristic absorption peaks of various mid-infrared gases, such as CH 4 , CO 2 , CO, and NO, enabling multi-gas detection in mixed gas environments. The proposed thermal emitter serves as an effective and low-cost alternative for dualband narrowband mid-infrared light sources, contributing to the advancement of multigas detection strategies.
Kesterite (CZTS/CZTSSe) thin-film solar cells are considered an eco-friendly, earth-abundant, and low-cost photovoltaic technology that can fulfill our future energy needs. Due to its outstanding properties including tunable bandgap and 
 Kesterite (CZTS/CZTSSe) thin-film solar cells are considered an eco-friendly, earth-abundant, and low-cost photovoltaic technology that can fulfill our future energy needs. Due to its outstanding properties including tunable bandgap and high absorption coefficient, the power conversion efficiency (PCE) has reached over 14%. However, toxic cadmium sulfide (CdS) is commonly used as an n-type buffer layer in kesterite thin-film solar cells (KTFSCs) to form a better p–n junction with the p-type CZTS/CZTSSe absorber. In addition to its toxicity, the CdS buffer layer shows parasitic absorption at low wavelengths (400–500 nm) owing to its low bandgap (2.4 eV). For the last few years, several efforts have been made to substitute CdS with an eco-friendly, Cd-free, cost-effective buffer layer with alternative large-bandgap materials such as ZnSnO, Zn (O, S), In2Se3, ZnS, ZnMgO, and TiO2, which showed significant advances. Herein, we summarize the key findings of the research community using a Cd-free buffer layer in KTFSCs to provide a current scenario for future work motivating researchers to design new materials and strategies to achieve higher performance.
Abstract Selenium (Se), the oldest material used in photovoltaic devices, initiated the development of modern solar technology. Trigonal Se ( t ‐Se), the most thermodynamically stable and photoactive phase, exhibits 
 Abstract Selenium (Se), the oldest material used in photovoltaic devices, initiated the development of modern solar technology. Trigonal Se ( t ‐Se), the most thermodynamically stable and photoactive phase, exhibits remarkable photoelectric properties. However, achieving high‐quality, pure‐phase, and well‐oriented t ‐Se films remains a significant challenge due to the high energy barrier for phase transformation and its inherent anisotropy. Here, an oxygen‐assisted high‐temperature deposition strategy is reported, wherein films are grown at temperatures exceeding the selenium re‐sublimation point and under elevated selenium vapor pressure. This approach effectively overcomes the intrinsic thermodynamic limitations, enabling the one‐step fabrication of single‐phase, highly crystalline, and vertically oriented polycrystalline t ‐Se absorber layers. The resulting t ‐Se absorbers exhibit improved carrier transport, reduced deep‐level defects, minimized surface potential fluctuations, and enhanced grain boundary properties. These advances significantly reduce electrical losses in t ‐Se thin film solar cells, leading to a certified efficiency of 7.55%, the highest certified efficiency so far. This work provides a thermodynamically viable route to the growth and application of trigonal Se and other low‐dimensional materials.
Simon Steinberg | Journal of Physics Condensed Matter
Abstract Future problems request the development of materials, which serve as components in technologies addressing these challenges. In this context, tellurides are of great interest since many members of that 
 Abstract Future problems request the development of materials, which serve as components in technologies addressing these challenges. In this context, tellurides are of great interest since many members of that remarkable family of solids are at the frontline of fundamental research and technological applications. The tailored design of novel tellurides showing task-specific features also demands a proper understanding of their electronic structures, as the knowledge of them provides invaluable insights into the materials characteristics. Therefore, it will be quite helpful if there is a fundamental design principle that allows us to plan electronic peculiarities in tellurides in a straightforward manner. Eventually, the Zintl−Klemm−Busmann idea is a recipe that can guide us through electronic structures based on the corresponding crystal structures and it has been applied to several tellurides to date; yet, how helpful is that approach with regard to the prediction of electronic peculiarities for tellurides in general? In the framework of this review, it will be the overall goal to answer that question.&amp;#xD;
Understanding the physical mechanism of interface transport properties that affect hydrogen production is key for improving the performance of photocatalytic hydrogen generation reaction in two-dimensional (2D) van der Waals ferroelectric 
 Understanding the physical mechanism of interface transport properties that affect hydrogen production is key for improving the performance of photocatalytic hydrogen generation reaction in two-dimensional (2D) van der Waals ferroelectric heterostructures with various band arrangements. Herein, four CuInP2S6 (CIPS)/MoTe2 heterostructures with three band alignment transitions are obtained by controlling polarization direction and interface mismatch. To study the influence of polarization reversal and the different band alignments on transport properties, an analytical model is established to clarify the interface charge separation and recombination induced by built-in electric fields in type-II and Z-scheme heterostructures. The results show that polarization reversal can enhance the interface electron mobility by more than two orders of magnitude, and interface Auger recombination can greatly enhance the lifetime of photogenerated carriers at relatively higher bands. Moreover, by involving the energy loss induced by the interface electric field scattering rate and Auger recombination rate, we find that the solar-to-hydrogen efficiency of CIPS/MoTe2 with Z-scheme heterostructure is much larger than that of type-II heterostructures. Our prediction provides a quantitative approach to deal with the photocatalytic properties from interface transport under various band alignments and may offer guidance to pursue multifunctional applications in 2D ferroelectric materials.
Abstract Tandem solar cells are anticipated to possess higher efficiencies than single-junction counterparts originating from the broader absorption spectra. In recent years, machine learning methods have demonstrated to be efficient 
 Abstract Tandem solar cells are anticipated to possess higher efficiencies than single-junction counterparts originating from the broader absorption spectra. In recent years, machine learning methods have demonstrated to be efficient tools for the design and optimization of photoelectric devices. Herein, we proposed a tandem solar cell based on absorber layers of MAPbI3 and Sb2Se3 and employed three different machine learning models to predict its photovoltaic response. Additionally, a co-simulation model of metaheuristic algorithm (GA, PSO, SA) and machine learning model (LR, RR, MLP, DT, RF) is constructed to optimize the bandgap of the absorption materials, as well as the thicknesses of the ETL, HTL, and absorber layers. Through the proposed inverse design, the optimized power conversion efficiency (PCE) of the concerned cell is demonstrated to reach ~39.86%. The current work is believed to be insightful for the design and boosting the efficiency of tandem solar cells.