2
views
0
recommends
+1 Recommend
0 collections
    0
    shares
      • Record: found
      • Abstract: found
      • Article: not found

      A comprehensive study of the optimization and comparison of cesium halide perovskite solar cells using ZnO and Cu 2FeSnS 4 as charge transport layers

      Read this article at

      ScienceOpenPublisher
      Bookmark
          There is no author summary for this article yet. Authors can add summaries to their articles on ScienceOpen to make them more accessible to a non-specialist audience.

          Abstract

          A comparative analysis along with the optimization of various parameters for 8 different Cs-halide perovskite absorber-based solar cells is performed using a SCAPS-1D simulator, where ZnO and CFTS are proposed as ETL and HTL materials, respectively.

          Abstract

          To meet the increasing demand for power sources, scientists are continuously trying to improve the efficiency of solar cells. In these circumstances, Cs-based perovskites have attracted attention due to their intriguing performance. In this paper, eight different solar cells based on Cs-halide perovskite absorbers (CsPbI 3, CsPbBr 3, CsSnI 3, CsSnCl 3, Cs 2BiAgI 6, Cs 3Bi 2I 9, CsSn 0.5Ge 0.5I 3, and Cs 3Sb 2I 9) are investigated using the SCAPS-1D simulation program. Besides, ZnO and CFTS materials are proposed as promising candidates for charge transport material application, along with gold as the back contact. Initially, the impact of the absorber and the electron transport layer (ETL) thickness on the photovoltaic performance was evaluated. In addition, various parameters, such as the thickness, the donor and acceptor densities and the defect density, are investigated to locate the final optimized Cs-based structures. From this optimization, it is evident that among all the optimizing features, absorber materials and the hole transport layer (HTL) thickness, the HTL acceptor density enhanced the performance much more than the other optimizing features. Furthermore, to evaluate the characteristics of these devices, the series resistance, shunt resistance, working temperature, current–voltage density, and quantum efficiency are also simulated. Among all eight Cs-based perovskites, the ITO/ZnO/CsPbBr 3/CFTS/Au and ITO/ZnO/Cs 3Bi 2I 9/CFTS/Au devices achieved the best performance, with a conversion efficiency of 19.28% and 19.23%, respectively. Lastly, the performance of the SCAPS-1D simulator software is verified using the wxAMPS simulation program, where both yield results that are in excellent agreement. In conclusion, this research provides useful information for optimizing solar cell architectures and understanding the effects of various device components.

          Related collections

          Most cited references83

          • Record: found
          • Abstract: found
          • Article: not found

          Organometal halide perovskites as visible-light sensitizers for photovoltaic cells.

          Two organolead halide perovskite nanocrystals, CH(3)NH(3)PbBr(3) and CH(3)NH(3)PbI(3), were found to efficiently sensitize TiO(2) for visible-light conversion in photoelectrochemical cells. When self-assembled on mesoporous TiO(2) films, the nanocrystalline perovskites exhibit strong band-gap absorptions as semiconductors. The CH(3)NH(3)PbI(3)-based photocell with spectral sensitivity of up to 800 nm yielded a solar energy conversion efficiency of 3.8%. The CH(3)NH(3)PbBr(3)-based cell showed a high photovoltage of 0.96 V with an external quantum conversion efficiency of 65%.
            Bookmark
            • Record: found
            • Abstract: found
            • Article: not found

            Efficient hybrid solar cells based on meso-superstructured organometal halide perovskites.

            The energy costs associated with separating tightly bound excitons (photoinduced electron-hole pairs) and extracting free charges from highly disordered low-mobility networks represent fundamental losses for many low-cost photovoltaic technologies. We report a low-cost, solution-processable solar cell, based on a highly crystalline perovskite absorber with intense visible to near-infrared absorptivity, that has a power conversion efficiency of 10.9% in a single-junction device under simulated full sunlight. This "meso-superstructured solar cell" exhibits exceptionally few fundamental energy losses; it can generate open-circuit photovoltages of more than 1.1 volts, despite the relatively narrow absorber band gap of 1.55 electron volts. The functionality arises from the use of mesoporous alumina as an inert scaffold that structures the absorber and forces electrons to reside in and be transported through the perovskite.
              Bookmark
              • Record: found
              • Abstract: found
              • Article: not found

              Sequential deposition as a route to high-performance perovskite-sensitized solar cells.

              Following pioneering work, solution-processable organic-inorganic hybrid perovskites-such as CH3NH3PbX3 (X = Cl, Br, I)-have attracted attention as light-harvesting materials for mesoscopic solar cells. So far, the perovskite pigment has been deposited in a single step onto mesoporous metal oxide films using a mixture of PbX2 and CH3NH3X in a common solvent. However, the uncontrolled precipitation of the perovskite produces large morphological variations, resulting in a wide spread of photovoltaic performance in the resulting devices, which hampers the prospects for practical applications. Here we describe a sequential deposition method for the formation of the perovskite pigment within the porous metal oxide film. PbI2 is first introduced from solution into a nanoporous titanium dioxide film and subsequently transformed into the perovskite by exposing it to a solution of CH3NH3I. We find that the conversion occurs within the nanoporous host as soon as the two components come into contact, permitting much better control over the perovskite morphology than is possible with the previously employed route. Using this technique for the fabrication of solid-state mesoscopic solar cells greatly increases the reproducibility of their performance and allows us to achieve a power conversion efficiency of approximately 15 per cent (measured under standard AM1.5G test conditions on solar zenith angle, solar light intensity and cell temperature). This two-step method should provide new opportunities for the fabrication of solution-processed photovoltaic cells with unprecedented power conversion efficiencies and high stability equal to or even greater than those of today's best thin-film photovoltaic devices.
                Bookmark

                Author and article information

                Contributors
                (View ORCID Profile)
                (View ORCID Profile)
                (View ORCID Profile)
                (View ORCID Profile)
                (View ORCID Profile)
                (View ORCID Profile)
                (View ORCID Profile)
                Journal
                NJCHE5
                New Journal of Chemistry
                New J. Chem.
                Royal Society of Chemistry (RSC)
                1144-0546
                1369-9261
                May 09 2023
                2023
                : 47
                : 18
                : 8602-8624
                Affiliations
                [1 ]Institute of Electronics, Atomic Energy Research Establishment, Bangladesh Atomic Energy Commission, Dhaka 1349, Bangladesh
                [2 ]Department of Advanced Energy Engineering Science, Interdisciplinary Graduate School of Engineering Sciences, Kyushu University, Fukuoka 816-8580, Japan
                [3 ]College of Materials Science and Engineering, Donghua University, Shanghai 201620, China
                [4 ]VLSI Centre of Excellence, Chitkara University Institute of Engineering and Technology, Chitkara University, Punjab 140401, India
                [5 ]LEREESI, Higher National School of Renewable Energies, Environment and Sustainable Development, Batna 05078, Algeria
                [6 ]Radiological Techniques Department, Al-Mustaqbal University College, 51001 Hillah, Babylon, Iraq
                [7 ]Department of Electrical and Electronic Engineering, Bangamata Sheikh Fojilatunnesa Mujib Science & Technology University, Jamalpur 2012, Bangladesh
                [8 ]Department of Materials Science and Engineering, University of Rajshahi, Rajshahi 6205, Bangladesh
                [9 ]Advanced Energy Materials and Solar Cell Research Laboratory, Department of Electrical and Electronic Engineering, Begum Rokeya University, Rangpur 5400, Bangladesh
                [10 ]Department of Physics, Arunachal University of Studies, Namsai, 792103, Arunachal Pradesh, India
                [11 ]Dept. of ECE, Indian Institute of Information Technology, Design & Manufacturing, Madhya Pradesh 482005, India
                Article
                10.1039/D3NJ00320E
                b6340fdb-d2b8-4503-b6d6-87a6fb344067
                © 2023

                http://rsc.li/journals-terms-of-use

                History

                Comments

                Comment on this article