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Journal articles on the topic 'SCAPS-1D'

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Published: 4 June 2021
Last updated: 16 February 2022

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1

Kim, Kihwan, Jihye Gwak, Seung Kyu Ahn, Young-Joo Eo, Joo Hyung Park, Jun-Sik Cho, Min Gu Kang, Hee-Eun Song, and Jae Ho Yun. "Simulations of chalcopyrite/c-Si tandem cells using SCAPS-1D." Solar Energy 145 (March 2017): 52–58. http://dx.doi.org/10.1016/j.solener.2017.01.031.

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2

Sawicka-Chudy, P., Z. Starowicz, G. Wisz, R. Yavorskyi, Z. Zapukhlyak, M. Bester, Ł. Głowa, M. Sibiński, and M. Cholewa. "Simulation of TiO2/CuO solar cells with SCAPS-1D software." Materials Research Express 6, no. 8 (June 19, 2019): 085918. http://dx.doi.org/10.1088/2053-1591/ab22aa.

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3

Djinkwi Wanda, M., S. Ouédraogo, F. Tchoffo, F. Zougmoré, and J. M. B. Ndjaka. "Numerical Investigations and Analysis of Cu2ZnSnS4Based Solar Cells by SCAPS-1D." International Journal of Photoenergy 2016 (2016): 1–9. http://dx.doi.org/10.1155/2016/2152018.

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This paper reports numerical investigation, using SCAPS-1D program, of the influence of Cu2ZnSnS4(the so-called CZTS) material features such as thickness, holes, and defects densities on the performances of ZnO:Al/i-ZnO/CdS/CZTS/Mo solar cells structure. We found that the electrical parameters are seriously affected, when the absorber thickness is lower than 600 nm, mainly due to recombination at CZTS/Molybdenum interface that causes the short-circuit current density loss of 3.6 mA/cm2. An additional source of recombination, inside the absorber layer, affects the short-circuit current density and produces a loss of about 2.1 mA/cm2above this range of absorber thickness. TheJ-Vcharacteristic shows that the performance of the device is also limited by a double diode behavior. This effect is reduced when the absorber layer is skinny. Our investigations showed that, for solar cells having a CZTS absorber layer of thin thickness and high-quality materials (defects density ~1015 cm−3), doping less than 1016 cm−3is especially beneficial. Such CZTS based solar cell devices could lead to conversion efficiencies higher than 15% and to improvement of about 100 mV on the open-circuit voltage value. Our results are in conformity with experimental reports existing in the literature.
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4

Mostefaoui, M., H. Mazari, S. Khelifi, A. Bouraiou, and R. Dabou. "Simulation of High Efficiency CIGS Solar Cells with SCAPS-1D Software." Energy Procedia 74 (August 2015): 736–44. http://dx.doi.org/10.1016/j.egypro.2015.07.809.

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5

Sadanand and D. K. Dwivedi. "Numerical Simulation for Enhancement of the Output Performance of CZTS Based Thin Film Photovoltaic Cell." Advanced Science, Engineering and Medicine 12, no. 1 (January 1, 2020): 88–94. http://dx.doi.org/10.1166/asem.2020.2526.

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The performance of CZTS thin film photovoltaic cell has been simulated using SCAPS-1D (Solar cell capacitance simulator). The thickness of CZTS absorber layer, ZnO buffer layer and ZnO doped with Al window layer have been varied to optimize the overall output performance of CZTS based thin film photovoltaic cell. Simulation show the favorable result which can help to prove the feasibility of highly efficient CZTS thin film photovoltaic cell.
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Zhou, Xiangyu, and Junfeng Han. "Design and simulation of C2N based solar cell by SCAPS-1D software." Materials Research Express 7, no. 12 (December 5, 2020): 126303. http://dx.doi.org/10.1088/2053-1591/abcdd6.

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7

Mandadapu, Usha. "Simulation and Analysis of Lead based Perovskite Solar Cell using SCAPS-1D." Indian Journal of Science and Technology 10, no. 1 (January 10, 2017): 1–8. http://dx.doi.org/10.17485/ijst/2017/v11i10/110721.

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Mandadapu, Usha, S. Victor Vedanayakam, K. Thyagarajan, and B. J. Babu. "Optimisation of high efficiency tin halide perovskite solar cells using SCAPS-1D." International Journal of Simulation and Process Modelling 13, no. 3 (2018): 221. http://dx.doi.org/10.1504/ijspm.2018.093097.

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Babu, B. J., Usha Mandadapu, S. Victor Vedanayakam, and K. Thyagarajan. "Optimisation of high efficiency tin halide perovskite solar cells using SCAPS-1D." International Journal of Simulation and Process Modelling 13, no. 3 (2018): 221. http://dx.doi.org/10.1504/ijspm.2018.10014179.

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10

Mandadapu, Usha, K. Thyagarajan, and S. Victor Vedanayakam. "Simulation and Analysis of Lead based Perovskite Solar Cell using SCAPS-1D." Indian Journal of Science and Technology 10, no. 11 (March 1, 2017): 1–8. http://dx.doi.org/10.17485/ijst/2017/v10i11/110721.

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11

Adewoyin, Adeyinka D., Muteeu A. Olopade, Olusola O. Oyebola, and Micheal A. Chendo. "Development of CZTGS/CZTS tandem thin film solar cell using SCAPS-1D." Optik 176 (January 2019): 132–42. http://dx.doi.org/10.1016/j.ijleo.2018.09.033.

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12

Mebadi, Ashkan, Mohammad Houshmand, M. Hossein Zandi, and Nima E. Gorji. "Numerical Analysis of TiO2/Cu2ZnSnS4 Nanostructured PV Using SCAPS-1D." Nano Hybrids 8 (December 2014): 27–38. http://dx.doi.org/10.4028/www.scientific.net/nh.8.27.

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A nanostructured solar cells consist of a nonporous n-type TiO2 nanoparticles and a p-type semiconductor Cu2ZnSnS4 (CZTS) thin film has been numerically simulated using SCAPS-1D tool. The performed theoretically analysis is compared with the experimental reported data. The band diagram, IV characteristics and quantum efficiency of this structure is considered. The benefit of both TiO2 and CZTS material leads to more than 10% conversion efficiency which is promising between the nanoparticle-based heterojunbctions proposed for PV applications.
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13

Mouhammed, Adnan Alwan, and Ayed N. Saleh. "Simulation Effect of Ga2O3 layer thickness on CdTe solar cell by SCAPS-1D." Tikrit Journal of Pure Science 24, no. 6 (November 3, 2019): 110. http://dx.doi.org/10.25130/j.v24i6.895.

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The effect of Ga2O3 thickness on CdTe cells was studied using the SCAPS-1D simulator. The best solar cell efficiency (14.65%) was found at the thickness of the gallium oxide layer (1-10nm) and the cell efficiency (η) decrease with an increase in the thickness of the oxide layer and the decrease of the fill factor, thus decreasing the voltage current (I-V) and decreasing the current of the short circuit (Isc). The value of the open circuit voltage (VOC) is approximately constant and at 0.76V. The optical properties of the cell of quantitative efficiency are 86% and decrease within 18nm http://dx.doi.org/10.25130/tjps.24.2019.116
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14

Ouédraogo, S., F. Zougmoré, and J. M. Ndjaka. "Numerical Analysis of Copper-Indium-Gallium-Diselenide-Based Solar Cells by SCAPS-1D." International Journal of Photoenergy 2013 (2013): 1–9. http://dx.doi.org/10.1155/2013/421076.

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We used a one-dimensional simulation program Solar Cell Capacitance Simulator in 1 Dimension (SCAPS-1D) to investigate Copper-Indium-Gallium-Diselenide- (CIGS-) based solar cells properties. Starting with a conventional ZnO-B/i-ZnO/CdS/CIGS structure, we simulated the parameters of current-voltage characteristics and showed how the absorber layer thickness, hole density, and band gap influence the short-circuit current density (Jsc), open-circuit voltage (Voc), fill factor (FF), and efficiency of solar cell. Our simulation results showed that all electrical parameters are greatly affected by the absorber thickness (w) below 1000 nm, due to the increase of back-contact recombination and very poor absorption. Increasing hole density (p) or absorber band gap (Eg) improvesVocand leads to high efficiency, which equals value of 16.1% whenp= 1016 cm−3andEg=1.2 eV. In order to reduce back-contact recombination, the effect of a very thin layer with high band gap inserted near the back contact and acting as electrons reflector, the so-called back-electron reflector (EBR), has been investigated. The performances of the solar cells are significantly improved, when ultrathin absorbers (w< 500 nm) are used; the corresponding gain ofJscdue to the EBR is 3 mA/cm2. Our results are in good agreement with those reported in the literature from experiments.
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15

Samiul Islam, Md, K. Sobayel, Ammar Al-Kahtani, M. A. Islam, Ghulam Muhammad, N. Amin, Md Shahiduzzaman, and Md Akhtaruzzaman. "Defect Study and Modelling of SnX3-Based Perovskite Solar Cells with SCAPS-1D." Nanomaterials 11, no. 5 (May 5, 2021): 1218. http://dx.doi.org/10.3390/nano11051218.

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Recent achievements, based on lead (Pb) halide perovskites, have prompted comprehensive research on low-cost photovoltaics, in order to avoid the major challenges that arise in this respect: Stability and toxicity. In this study, device modelling of lead (Pb)-free perovskite solar cells has been carried out considering methyl ammonium tin bromide (CH3NH3SnBr3) as perovskite absorber layer. The perovskite structure has been justified theoretically by Goldschmidt tolerance factor and the octahedral factor. Numerical modelling tools were used to investigate the effects of amphoteric defect and interface defect states on the photovoltaic parameters of CH3NH3SnBr3-based perovskite solar cell. The study identifies the density of defect tolerance in the absorber layer, and that both the interfaces are 1015 cm−3, and 1014 cm−3, respectively. Furthermore, the simulation evaluates the influences of metal work function, uniform donor density in the electron transport layer and the impact of series resistance on the photovoltaic parameters of proposed n-TiO2/i-CH3NH3SnBr3/p-NiO solar cell. Considering all the optimization parameters, CH3NH3SnBr3-based perovskite solar cell exhibits the highest efficiency of 21.66% with the Voc of 0.80 V, Jsc of 31.88 mA/cm2 and Fill Factor of 84.89%. These results divulge the development of environmentally friendly methyl ammonium tin bromide perovskite solar cell.
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16

Benzetta, Abd Elhalim, Mahfoud Abderrezek, and Mohammed Elamine Djeghlal. "Numerical study of CZTS/CZTSSe tandem thin film solar cell using SCAPS-1D." Optik 242 (September 2021): 167320. http://dx.doi.org/10.1016/j.ijleo.2021.167320.

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17

T, Joseph Mebelson, and Elampari K. "Numerical Simulation for Optimal Thickness Combination of CdS/ZnS Dual Buffer Layer CuInGaSe2 Solar Cell Using SCAPS 1D." Indian Journal of Science and Technology 12, no. 45 (December 10, 2019): 01–06. http://dx.doi.org/10.17485/ijst/2019/v12i45/148395.

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18

Ngoupo, A. Teyou, S. Ouédraogo, F. Zougmoré, and J. M. B. Ndjaka. "Numerical analysis of ultrathin Sb2Se3-based solar cells by SCAPS-1D numerical simulator device." Chinese Journal of Physics 70 (April 2021): 1–13. http://dx.doi.org/10.1016/j.cjph.2020.12.010.

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19

AKINRINOLA, Olusola, Ayodeji AWODUGBA, Momodu JAIN, Mojoyinola AWODELE, Omowunmi AKINRINOLA, and Abideen IBIYEMI. "On the Capacitance Spectroscopy of Cu2ZnSnS4 Typed Solar Cells Anisotype Heterojunction by SCAPS-1D." International Journal of Engineering Technologies IJET 6, no. 3 (January 29, 2021): 37–44. http://dx.doi.org/10.19072/ijet.627225.

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20

Anwar, Farhana, Rafee Mahbub, Sakin Sarwar Satter, and Saeed Mahmud Ullah. "Effect of Different HTM Layers and Electrical Parameters on ZnO Nanorod-Based Lead-Free Perovskite Solar Cell for High-Efficiency Performance." International Journal of Photoenergy 2017 (2017): 1–9. http://dx.doi.org/10.1155/2017/9846310.

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Simulation has been done using SCAPS-1D to examine the efficiency of CH3NH3SnI3-based solar cells including various HTM layers such as spiro-OMeTAD, Cu2O, and CuSCN. ZnO nanorod array has been considered as an ETM layer. Device parameters such as thickness of the CH3NH3SnI3 layer, defect density of interfaces, density of states, and metal work function were studied. For optimum parameters of all three structures, efficiency of 20.21%, 20.23%, and 18.34% has been achieved for spiro-OMeTAD, Cu2O, and CuSCN, respectively. From the simulations, an alternative lead-free perovskite solar cell is introduced with the CH3NH3SnI3 absorber layer, ZnO nanorod ETM layer, and Cu2O HTM layer.
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21

Yasin, Shadi, Ziad Abu Waar, and Tariq Al Zoubi. "Development of high efficiency CZTS solar cell through buffer layer parameters optimization using SCAPS-1D." Materials Today: Proceedings 33 (2020): 1825–29. http://dx.doi.org/10.1016/j.matpr.2020.05.064.

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22

Yasin, S., T. Al Zoubi, and M. Moustafa. "Design and simulation of high efficiency lead-free heterostructure perovskite solar cell using SCAPS-1D." Optik 229 (March 2021): 166258. http://dx.doi.org/10.1016/j.ijleo.2021.166258.

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23

Al-Hattab, Mohamed, L'houcine Moudou, Mohammed Khenfouch, Omar Bajjou, Younes Chrafih, and Khalid Rahmani. "Numerical simulation of a new heterostructure CIGS/GaSe solar cell system using SCAPS-1D software." Solar Energy 227 (October 2021): 13–22. http://dx.doi.org/10.1016/j.solener.2021.08.084.

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24

Ahmad, Owais, Asim Rashid, M. Waqar Ahmed, M. Farooq Nasir, and Irfan Qasim. "Performance evaluation of Au/p-CdTe/Cs2TiI6/n-TiO2/ITO solar cell using SCAPS-1D." Optical Materials 117 (July 2021): 111105. http://dx.doi.org/10.1016/j.optmat.2021.111105.

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25

Sunny, Adil, Sabrina Rahman, Most Marzia Khatun, and Sheikh Rashel Al Ahmed. "Numerical study of high performance HTL-free CH3NH3SnI3-based perovskite solar cell by SCAPS-1D." AIP Advances 11, no. 6 (June 1, 2021): 065102. http://dx.doi.org/10.1063/5.0049646.

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26

H. Najim, Alaa, and Ayed N. Saleh. "Study effect of window and BSF layers on the properties of the CZTS / CZTSe solar cell by SCAPS–1D." Tikrit Journal of Pure Science 24, no. 3 (May 8, 2019): 77. http://dx.doi.org/10.25130/j.v24i3.820.

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The solar cell CZTS / CZTSe was studied using SCAPS- computer simulator. It was noted that increasing the thickness of the absorber layer p-CZTSe from 250nm to 5μm leads to increase the IV curve. thus increasing the values ​​of Voc, Jsc, FF,
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27

Obi, U. C., D. M. Sanni, and A. Bello. "Effect of Absorber Layer Thickness on the Performance of Bismuth-Based Perovskite Solar Cells." Физика и техника полупроводников 55, no. 4 (2021): 354. http://dx.doi.org/10.21883/ftp.2021.04.50738.9386a.

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Theoretical study of methyl-ammonium bismuth halide perovskite solar cells, (CH3NH3)3Bi2I9, was carried out using a one-dimensional Solar Cell Capacitance Simulator (SCAPS-1D) software. The performance of the tested device architectures largely depends on the thickness of the absorbing layer, with the combination of electron transport, and hole transport layers. Thus, the bismuth perovskite absorber layer was optimized by varying the thickness and also, the thicknesses of the different charge-transport materials such as Spiro-OmeTAD, copper (I) oxide (Cu2O), and copper (I) iodide (CuI) as hole transport layer (HTL), and phenyl-C61-butyric acid methyl ester (PCBM), poly(3-hexylthiophene-2,5-diyl) (P3HT), zinc oxide, and titanium dioxide as electron transport layer (ETL). The best performance in terms of the power conversion efficiency (PCE) was recorded for the device with Cu2O as the HTL and ZnO as the ETL with the absorber layer thickness of 200 nm. The working temperature of the device was varied from 295 to 320 K and the effects of temperature on various device architectures were investigated. Results obtained indication that the efficiency of the bismuth perovskite solar cells can be improved by optimizing the thickness of the absorber layer and utilizing an appropriate combination of HTLs and ETLs. Keywords: methyl-ammonium bismuth perovskite, SCAPS, HTL, ETL, PCE.
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Obi, U. C., D. M. Sanni, and A. Bello. "Effect of Absorber Layer Thickness on the Performance of Bismuth-Based Perovskite Solar Cells." Физика и техника полупроводников 55, no. 4 (2021): 354. http://dx.doi.org/10.21883/ftp.2021.04.50738.9386a.

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Theoretical study of methyl-ammonium bismuth halide perovskite solar cells, (CH3NH3)3Bi2I9, was carried out using a one-dimensional Solar Cell Capacitance Simulator (SCAPS-1D) software. The performance of the tested device architectures largely depends on the thickness of the absorbing layer, with the combination of electron transport, and hole transport layers. Thus, the bismuth perovskite absorber layer was optimized by varying the thickness and also, the thicknesses of the different charge-transport materials such as Spiro-OmeTAD, copper (I) oxide (Cu2O), and copper (I) iodide (CuI) as hole transport layer (HTL), and phenyl-C61-butyric acid methyl ester (PCBM), poly(3-hexylthiophene-2,5-diyl) (P3HT), zinc oxide, and titanium dioxide as electron transport layer (ETL). The best performance in terms of the power conversion efficiency (PCE) was recorded for the device with Cu2O as the HTL and ZnO as the ETL with the absorber layer thickness of 200 nm. The working temperature of the device was varied from 295 to 320 K and the effects of temperature on various device architectures were investigated. Results obtained indication that the efficiency of the bismuth perovskite solar cells can be improved by optimizing the thickness of the absorber layer and utilizing an appropriate combination of HTLs and ETLs. Keywords: methyl-ammonium bismuth perovskite, SCAPS, HTL, ETL, PCE.
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29

Kata, N., D. Diouf, A. Darga, and A. Seidou Maiga. "The effect of the recombination mechanisms location on the temperature sensitivity of thin-film photovoltaic cells." EPJ Photovoltaics 10 (2019): 8. http://dx.doi.org/10.1051/epjpv/2019008.

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Thin film solar cells temperature sensitivity and impact of the main recombination mechanism location are investigated in this paper. The main mechanisms in bulk and at the heterojunction interface are discriminated. Using a 1D simulation software, “Solar Cell Capacitance Simulator” (SCAPS), we observed a higher temperature coefficient of open circuit voltage (Voc) for cells with main recombination centers at the interface than the one with main recombination centers in volume. Furthermore, an LTSpice module model is used to visualize the effects of the recombination centers' location on the performance ratios of the modules. The results show more degradation for the ratios performance of cells with the main recombination mechanisms at the interface than those in volume.
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Huang, Chia-Hua, and Wen-Jie Chuang. "Dependence of performance parameters of CdTe solar cells on semiconductor properties studied by using SCAPS-1D." Vacuum 118 (August 2015): 32–37. http://dx.doi.org/10.1016/j.vacuum.2015.03.008.

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31

Mishra, Shubham, Kshitij Bhargava, and Dipankar Deb. "Numerical simulation of potential induced degradation (PID) in different thin-film solar cells using SCAPS-1D." Solar Energy 188 (August 2019): 353–60. http://dx.doi.org/10.1016/j.solener.2019.05.077.

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32

Teyou Ngoupo, A., S. Ouédraogo, and J. M. Ndjaka. "Numerical analysis of interface properties effects in CdTe/CdS:O thin film solar cell by SCAPS-1D." Indian Journal of Physics 93, no. 7 (January 8, 2019): 869–81. http://dx.doi.org/10.1007/s12648-018-01360-z.

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33

Belarbi, F., W. Rahal, D. Rached, S. benghabrit, and M. Adnane. "A comparative study of different buffer layers for CZTS solar cell using Scaps-1D simulation program." Optik 216 (August 2020): 164743. http://dx.doi.org/10.1016/j.ijleo.2020.164743.

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Basak, Arindam, and Udai P. Singh. "Numerical modelling and analysis of earth abundant Sb2S3 and Sb2Se3 based solar cells using SCAPS-1D." Solar Energy Materials and Solar Cells 230 (September 2021): 111184. http://dx.doi.org/10.1016/j.solmat.2021.111184.

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Hussain, Syed Sajjad, Saira Riaz, Ghazi Aman Nowsherwan, Khizer Jahangir, Akram Raza, Muhammad Javaid Iqbal, Imran Sadiq, Syed Mutahir Hussain, and Shahzad Naseem. "Numerical Modeling and Optimization of Lead-Free Hybrid Double Perovskite Solar Cell by Using SCAPS-1D." Journal of Renewable Energy 2021 (July 16, 2021): 1–12. http://dx.doi.org/10.1155/2021/6668687.

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The highest power conversion efficiency (PCE) for organic-inorganic perovskite solar cells based on lead is reported as 25.2% in 2019. Lead-based hybrid perovskite materials are used in several photovoltaics applications, but these are not highly favored due to the toxicity of lead and volatility of organic cations. On the other hand, hybrid lead-free double perovskite has no such harm. In this research study, SCAPS numerical simulation is utilized to evaluate and compare the results of perovskite solar cell based on double perovskite FA 2 BiCuI 6 and standard perovskite CH 3 NH 3 PbI 3 as an active layer. The results show that the power conversion efficiency obtained in the case of FA 2 BiCuI 6 is 24.98%, while in the case of CH 3 NH 3 PbI 3 , it is reported as 26.42%. This indicates that the hybrid organic-inorganic double perovskite FA 2 BiCuI 6 has the ability to replace hybrid organic-inorganic perovskite CH 3 NH 3 PbI 3 to expand next-generation lead-free harmless materials for solar cell applications.
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Mekky, Abdel-baset H. "Simulation and modeling of the influence of temperature on CdS/CdTe thin film solar cell." European Physical Journal Applied Physics 87, no. 3 (September 2019): 30101. http://dx.doi.org/10.1051/epjap/2019190037.

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Semiconductor materials cadmium sulfide (CdS) and cadmium telluride (CdTe) are employed in the fabrication of thin film solar cells of relatively excessive power conversion efficiency and low producing price. Simulations of thin film CdS/CdTe solar cell were carried out using SCAPS-1D. The influence of temperature field on the variation of CdTe solar cell parameters such as current–voltage, capacitance–voltage characteristics and the external quantum efficiency was investigated theoretically. For use temperatures, one obtains the external quantum efficiency has the same profiles. However, the effect of the temperature on the Mott-Schottky curves is slightly noted by variations on the characteristics. This conclusion can be used by solar cell manufacturers to improve the solar cell parameters with the biggest possible gain in device performance.
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Moustafa, Mohamed Orabi, and Tariq Alzoubi. "Numerical Simulation of Single Junction InGaN Solar Cell by SCAPS." Key Engineering Materials 821 (September 2019): 407–13. http://dx.doi.org/10.4028/www.scientific.net/kem.821.407.

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The performance of the InGaN single-junction thin film solar cells has been analyzed numerically employing the Solar Cell Capacitance Simulator (SCAPS-1D). The electrical properties and the photovoltaic performance of the InGaN solar cells were studied by changing the doping concentrations and the bandgap energy along with each layer, i.e. n-and p-InGaN layers. The results reveal an optimum efficiency of the InGaN solar cell of ~ 15.32 % at a band gap value of 1.32 eV. It has been observed that lowering the doping concentration NA leads to an improvement of the short circuit current density (Jsc) (34 mA/cm2 at NA of 1016 cm−3). This might be attributed to the increase of the carrier mobility and hence an enhancement in the minority carrier diffusion length leading to a better collection efficiency. Additionally, the results show that increasing the front layer thickness of the InGaN leads to an increase in the Jsc and to the conversion efficiency (η). This has been referred to the increase in the photogenerated current, as well as to the less surface recombination rate.
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38

Bhavsar, K., and P. B. Lapsiwala. "Numerical simulation of perovskite solar cell with different material as electron transport layer using SCAPS-1D Software." Semiconductor Physics, Quantum Electronics and Optoelectronics 24, no. 3 (August 26, 2021): 341–47. http://dx.doi.org/10.15407/spqeo24.03.341.

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Perovskite solar cells have become a hot topic in the solar energy device area due to high efficiency and low cost photovoltaic technology. However, their function is limited by expensive hole transport material (HTM) and high temperature process electron transport material (ETM) layer is common device structure. Numerical simulation is a crucial technique in deeply understanding the operational mechanisms of solar cells and structure optimization for different devices. In this paper, device modelling for different perovskite solar cell has been performed for different ETM layer, namely: TiO2, ZnO, SnO2, PCBM (phenyl-C61-butyric acid methyl ester), CdZnS, C60, IGZO (indium gallium zinc oxide), WS2 and CdS and effect of band gap upon the power conversion efficiency of device as well as effect of absorber thickness have been examined. The SCAPS 1D (Solar Cell Capacitance Simulator) has been a tool used for numerical simulation of these devices.
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Niane, Djimba, Mouhamadou M. Soce, Jean Jude Domingo, Ousmane Diagne, and Moustapha Dieng. "Influence of the Thickness of a Layer of Potassium Fluoride Incorporated in the CIGS/CdS Interface on the Macroscopic Electrical Parameters of the Solar Cell." Applied Physics Research 11, no. 1 (January 29, 2019): 1. http://dx.doi.org/10.5539/apr.v11n1p1.

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In this work, the heterojunction composed of a n-type ZnO transparent conductive oxide (OTC) layer, a n-type CdS buffer layer and a absorber layer based Cu (In, Ga)Se2 p doped is studied under the influence of a KF layer placed in the CIGS/CdS interface. This study was done by varying the thickness of KF using thin-film simulation software named SCAPS-1D. The presence of KF for a doping of the CIGS absorber of 1016cm-3 improves strongly the electrical parameters that are the Vco, the Jcc the FF, the maximum power and the conversion efficiency of the solar cell Ƞ. However, a decrease of the FF and the Jcc is noticed when the thickness of the KF is greater than 30nm causing a deterioration of the performances of the cell.
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Mohottige, Rasika N., and Sandanuwan P. Kalawila Vithanage. "Numerical simulation of a new device architecture for CIGS-based thin-film solar cells using 1D-SCAPS simulator." Journal of Photochemistry and Photobiology A: Chemistry 407 (February 2021): 113079. http://dx.doi.org/10.1016/j.jphotochem.2020.113079.

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41

Hima, Abdelkader. "Enhancing of CH3NH3SnI3 based solar cell efficiency by ETL engineering." International Journal of Energetica 5, no. 1 (July 6, 2020): 27. http://dx.doi.org/10.47238/ijeca.v5i1.119.

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Solar cells based on organic-inorganic perovskites (PVK) are the subject of several researches in laboratories around the world. One of the most promising hybrid perovskite is the methylammonium lead tri-iodide MAPbI3 that is suitable for sun light harvesting. But the MAPbI3 is a toxic material, so in this paper is proposed another nature friendly candidate which is the methylammonium tin tri-iodide MASnI3. The proposed material is inserted into an n-i-p heterojunction solar cell which structure is electron transport layer (ETL)/PVK/hole transport layer (HTL). The used HTL is the PEDOT: PSS in combination with one of two ETLs which are the PCBM and the IGZO. Simulation efforts using 1D SCAPS was carried. It is found that IGZO ETL based solar cell yields a higher power conversion efficiency (PCE) compared with PCBM ETL based solar cell in the same thickness.
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Isoe, Wycliffe, Maxwell Mageto, Christopher Maghanga, Maurice Mwamburi, Victor Odari, and Celline Awino. "Thickness Dependence of Window Layer on CH3NH3PbI3-XClX Perovskite Solar Cell." International Journal of Photoenergy 2020 (July 28, 2020): 1–7. http://dx.doi.org/10.1155/2020/8877744.

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CH3NH3PbI3-xClx has been studied experimentally and has shown promising results for photovoltaic application. To enhance its performance, this study investigated the effect of varying thickness of FTO, TiO2, and CH3NH3PbI3-xClx for a perovskite solar cell with the structure glass/FTO/TiO2/CH3NH3PbI3-xClx/Spiro-OMeTAD/Ag studied using SCAPS-1D simulator software. The output parameters obtained from the literature for the device were 26.11 mA/cm2, 1.25 V, 69.89%, and 22.72% for Jsc, Voc, FF, and η, respectively. The optimized solar cell had a thickness of 100 nm, 50 nm, and 300 nm for FTO, TiO2, and CH3NH3PbI3-xClx layers, respectively, and the device output were 25.79 mA/cm2, 1.45 V, 78.87%, and 29.56% for Jsc, Voc, FF, and η, respectively, showing a remarkable increase in FF by 8.98% and 6.84% for solar cell efficiency. These results show the potential of fabricating an improved CH3NH3PbI3-xClx perovskite solar cell.
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Chakraborty, Kunal, Mahua Gupta Choudhury, and Samrat Paul. "Numerical study of Cs2TiX6 (X = Br−, I−, F− and Cl−) based perovskite solar cell using SCAPS-1D device simulation." Solar Energy 194 (December 2019): 886–92. http://dx.doi.org/10.1016/j.solener.2019.11.005.

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Mahammedi, Nassim Ahmed, Hamza Gueffaf, Brahim Lagoun, and Marhoun Ferhat. "Numerical simulation and optimization of a silicon clathrate-based solar cell n-Si136/p-Si2 using SCAPS-1D program." Optical Materials 107 (September 2020): 110043. http://dx.doi.org/10.1016/j.optmat.2020.110043.

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Ahmed, Saif, Farihatun Jannat, Md Abdul Kaium Khan, and Mohammad Abdul Alim. "Numerical development of eco-friendly Cs2TiBr6 based perovskite solar cell with all-inorganic charge transport materials via SCAPS-1D." Optik 225 (January 2021): 165765. http://dx.doi.org/10.1016/j.ijleo.2020.165765.

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He, Yizhou, Liyifei Xu, Cheng Yang, Xiaowei Guo, and Shaorong Li. "Design and Numerical Investigation of a Lead-Free Inorganic Layered Double Perovskite Cs4CuSb2Cl12 Nanocrystal Solar Cell by SCAPS-1D." Nanomaterials 11, no. 9 (September 7, 2021): 2321. http://dx.doi.org/10.3390/nano11092321.

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In the last decade, perovskite solar cells have made a quantum leap in performance with the efficiency increasing from 3.8% to 25%. However, commercial perovskite solar cells have faced a major impediment due to toxicity and stability issues. Therefore, lead-free inorganic perovskites have been investigated in order to find substitute perovskites which can provide a high efficiency similar to lead-based perovskites. In recent studies, as a kind of lead-free inorganic perovskite material, Cs4CuSb2Cl12 has been demonstrated to possess impressive photoelectric properties and excellent environmental stability. Moreover, Cs4CuSb2Cl12 nanocrystals have smaller effective photo-generated carrier masses than bulk Cs4CuSb2Cl12, which provides excellent carrier mobility. To date, there have been no reports about Cs4CuSb2Cl12 nanocrystals used for making solar cells. To explore the potential of Cs4CuSb2Cl12 nanocrystal solar cells, we propose a lead-free perovskite solar cell with the configuration of FTO/ETL/Cs4CuSb2Cl12 nanocrystals/HTL/Au using a solar cell capacitance simulator. Moreover, we numerically investigate the factors that affect the performance of the Cs4CuSb2Cl12 nanocrystal solar cell with the aim of enhancing its performance. By selecting the appropriate hole transport material, electron transport material, thickness of the absorber layer, doping density, defect density in the absorber, interface defect density, and working temperature point, we predict that the Cs4CuSb2Cl12 nanocrystal solar cell with the FTO/TiO2/Cs4CuSb2Cl12 nanocrystals/Cu2O/Au structure can attain a power conversion efficiency of 23.07% at 300 K. Our analysis indicates that Cs4CuSb2Cl12 nanocrystals have great potential as an absorbing layer towards highly efficient lead-free all-inorganic perovskite solar cells.
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Karthick, S., J. Bouclé, and S. Velumani. "Effect of bismuth iodide (BiI3) interfacial layer with different HTL’s in FAPI based perovskite solar cell – SCAPS – 1D study." Solar Energy 218 (April 2021): 157–68. http://dx.doi.org/10.1016/j.solener.2021.02.041.

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Tara, Ayush, Vishal Bharti, Susheel Sharma, and Rockey Gupta. "Device simulation of FASnI3 based perovskite solar cell with Zn(O0.3, S0.7) as electron transport layer using SCAPS-1D." Optical Materials 119 (September 2021): 111362. http://dx.doi.org/10.1016/j.optmat.2021.111362.

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Houimi, Amina, Serap Yiğit Gezgin, Bedrettin Mercimek, and Hamdi Şükür Kılıç. "Numerical analysis of CZTS/n-Si solar cells using SCAPS-1D. A comparative study between experimental and calculated outputs." Optical Materials 121 (November 2021): 111544. http://dx.doi.org/10.1016/j.optmat.2021.111544.

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Mohammed, Tariq A., and Ayed N. Saleh. "Study the effect of thickness and reflectivity on (n-ZnSe / p-MASnI3 / p-CuSCN) solar cell properties using SCAPS-1D." Tikrit Journal of Pure Science 24, no. 7 (December 22, 2019): 93. http://dx.doi.org/10.25130/j.v24i7.917.

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The effect of the absorption layer (MASnI3) within the range (200nm-900nm) was studied with the thickness of each layer HTM and ETM (10nm) for each. After completion of the study we found that the best thickness of the absorption plate is at (400nm), note that the cells used in the program is not perfect it contain defects, to be closer to the practical reality, after completing this study In the framework of this study was added a filter mirrors (95% mirro) from the library of the program (Scaps) and that the studied solar cells (n-ZnSe / p-MASnI3 / p-CuSCN) Reflectivity (R) ranged between 0.11-0.99 and the best reflective range at 0.99 was (η) 20.98 filler (FF) 68.55% short circuit current (Jsc) 34.040 mA/cm2 and volt circuit (Voc) 0.894 V. The default illumination spectrum has been set to the AM1.5 global standard http://dx.doi.org/10.25130/tjps.24.2019.134
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