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Journal articles on the topic 'CuInGaSe'

Author: Grafiati

Published: 30 May 2022

Last updated: 31 July 2025

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1

Lee, Ah-Reum, Hun-Soo Jeon, Gang-Suok Lee, et al. "Characterizations of CuInGaSe(CIGS) mixed-source and the thin film." Journal of the Korean Crystal Growth and Crystal Technology 20, no. 1 (2010): 1–6. http://dx.doi.org/10.6111/jkcgct.2010.20.1.001.

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2

Yoshino, Kenji, Takahiro Tokuda, Akira Nagaoka, et al. "Growth of CuInGaSe₂ Films by RF Sputtering Using CuInGaSe₂ Single Phase Target." Applied Mechanics and Materials 372 (August 2013): 571–74. http://dx.doi.org/10.4028/www.scientific.net/amm.372.571.

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CuIn0.8Ga0.2Se2 thin film is grown at room temperature by RF sputtering using high quality of CuIn0.8Ga0.2Se2 single phase target. A (112) diffraction peak is dominant with no secondary phases such as selenide materials in the X-ray diffraction pattern. A flat and homogeneous surface can be obtained in the sample.

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3

Chang, Jen-Chuan, Chia-Chih Chuang, Jhe-Wei Guo, et al. "An Investigation of CuInGaSe₂ Thin Film Solar Cells by Using CuInGa Precursor." Nanoscience and Nanotechnology Letters 3, no. 2 (2011): 200–203. http://dx.doi.org/10.1166/nnl.2011.1147.

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4

SONG, H., S. KIM, H. KIM, et al. "Preparation of CuInGaSe thin films by sputtering and selenization process." Solar Energy Materials and Solar Cells 75, no. 1-2 (2003): 145–53. http://dx.doi.org/10.1016/s0927-0248(02)00125-3.

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5

Mendivil, M. I., L. V. García, B. Krishnan, D. Avellaneda, J. A. Martinez, and S. Shaji. "CuInGaSe 2 nanoparticles by pulsed laser ablation in liquid medium." Materials Research Bulletin 72 (December 2015): 106–15. http://dx.doi.org/10.1016/j.materresbull.2015.07.038.

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6

Salem, A., K. Alshehri, J. A. Mohammed Abdulwahed, and S. A. Hussein. "Examination of Thermoelectric Power of the CuInGaSe₂ Crystals." Acta Physica Polonica A 142, no. 2 (2022): 211–15. http://dx.doi.org/10.12693/aphyspola.142.211.

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7

Jeon, Hunsoo, Ahreum Lee, Gang-Seok Lee, et al. "Fabrication of the CuInGaSe Pellet and Characterization of the Thin Film." Japanese Journal of Applied Physics 50, no. 1S1 (2011): 01AG01. http://dx.doi.org/10.7567/jjap.50.01ag01.

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8

Jeon, Hunsoo, Ahreum Lee, Gang-Seok Lee, et al. "Fabrication of the CuInGaSe Pellet and Characterization of the Thin Film." Japanese Journal of Applied Physics 50 (January 20, 2011): 01AG01. http://dx.doi.org/10.1143/jjap.50.01ag01.

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9

Kim, Hong Tak, Chang Duk Kim, Maeng Jun Kim, and Young‐Soo Sohn. "AC analysis of temperature effects on conversion efficiency of CuInGaSe 2 solar cells." Electronics Letters 51, no. 1 (2015): 86–88. http://dx.doi.org/10.1049/el.2014.3257.

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10

Devaney, W. E., W. S. Chen, J. M. Stewart, and R. A. Mickelsen. "Structure and properties of high efficiency ZnO/CdZnS/CuInGaSe/sub 2/ solar cells." IEEE Transactions on Electron Devices 37, no. 2 (1990): 428–33. http://dx.doi.org/10.1109/16.46378.

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11

Mir, Irshad Ahmad, Kamla Rawat, and H. B. Bohidar. "CuInGaSe nanocrystals for detection of trace amount of water in D2O (at ppm level)." Crystal Research and Technology 51, no. 10 (2016): 561–68. http://dx.doi.org/10.1002/crat.201600054.

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12

Chen, Liang Yan, and Chao Fang. "Investigation on Stability and Optical Properties of Zn_nSe_n(n=1~13) Nanocluster in CIGS-ZnSe Heterojunction Interface." Advanced Materials Research 953-954 (June 2014): 991–94. http://dx.doi.org/10.4028/www.scientific.net/amr.953-954.991.

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ZnSe cluster is the main form of growth mechanism in CuInGaSe based solar cells as the buffer layer and the building blocks for larger bulk ZnSe materials as well. With the generalized gradient approximation in first principle all-electron calculations, a number of configurations and structural isomers of ZnnSen(n=1~13) nanoclusters has been geometrically optimized to get the lowest energy constructions of ZnnSen(n=1~13). Second-order energy difference were applied to investigate the stability of small ZnSe nanoclusters. And the nanocage Zn12Se12cluster has been identified to be in rather stab

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13

Kim, Ki Hyun, Young Gab Chun, Byung Ok Park, and Kyung Hoon Yoon. "Synthesis of CuInSe₂ and CuInGaSe₂ Nanoparticles by Solvothermal Route." Materials Science Forum 449-452 (March 2004): 273–76. http://dx.doi.org/10.4028/www.scientific.net/msf.449-452.273.

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Chalcopyrite CuInSe 2 (CIS) and CuInGaSe 2</sub(CIGS) nanoparticles were directly synthesized by a solvothemal route in an autoclave with alkylamine as a solvent. The rod-like CIS nanoparticles with widths of 5-10 nm and lengths of 10-30 nm were obtained at 180°C for 36 hour whereas spherical nanoparticles with diameter in the range of 10-80 nm were observed at 200- 250 °C for 36 hour. A morphology change from spherical to rod-like CIS nanoparticles was observed at 190 °C as reaction time increased from 36 to 60 hour. The formation of the rod-like nanoparticles in diethylamine, without doub

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14

Syabriyana, Maliya, Zeni Ulma, and Rosalia Dwi Werena. "One-Step Sputtering CuInGaSe 2 (CIGSe) Process for Thin Film Solar Cells: Progress and Challenges." Proceedings of International Conference on Multidiciplinary Research 6, no. 1 (2024): 131–39. https://doi.org/10.32672/picmr.v6i1.1162.

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The one-step sputtering for fabricating CuInGaSe2 (CIGSe) solar cells has been gaining attention due to its potential for simplifying the manufacturing process, large area uniformity, and environmentally friendly as less reliance on toxic Se precursors such as H 2 Se. Despite these advantages, several drawbacks remain. To date, devices fabricated by quaternary sputtering without additional selenization have been limited in efficiency to about 16%, and realizing bandgap grading in order to match the performance of the best evaporated devices presents a challenge. We discuss the prospects for qu

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15

Courel, Maykel, Miriam M. Nicolás, and Osvaldo Vigil-Galán. "Study on the physical properties of Cu2ZnSnS4 thin films deposited by pneumatic spray pyrolysis technique." Applied Chemical Engineering 4, no. 1 (2021): 9. http://dx.doi.org/10.24294/ace.v4i1.652.

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The acquisition of new materials for the manufacturing of high efficiency and low-cost photovoltaic devices has currently become a challenge. Thin films of CuInGaSe and CdTe have been widely used in solar cell of second generation, achieving efficiencies about 20 %; however, the low abundance of In and Te as well as the toxicity of Cd is the primary obstacles to their industrial production. Compounds such as Cu2ZnSnS4, Cu2ZnSnSe4 and Cu2ZnSn(SSe)4 have emerged as an important and less costly alternative for efficient energy conversion in the future. In addition, these compounds have the requir

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16

Selmane, Naceur, Ali Cheknane, Fakhereddine Khemloul, Mohammed H. S. Helal, and Hikmat S. Hilal. "Cost-saving and performance-enhancement of CuInGaSe solar cells by adding CuZnSnSe as a second absorber." Solar Energy 234 (March 2022): 64–80. http://dx.doi.org/10.1016/j.solener.2022.01.072.

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17

Arul, S., N. Muthukumarasamy, M. D. Kannan, and S. Jayakumar. "Preparation and Characterization of Hot Wall Deposited CuInGaSe₂ Thin Films for Solar Cell Applications." Applied Mechanics and Materials 705 (December 2014): 56–59. http://dx.doi.org/10.4028/www.scientific.net/amm.705.56.

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CuIn0.7Ga0.3Se2 (CIGS) bulk compound was prepared by direct reaction of high purity (99.99%) elemental copper, indium, gallium and selenium. Using the prepared bulk CIGS, polycrystalline CuInGaSe2 thin films were deposited onto well cleaned soda-lime glass substrates using hot wall deposition technique by optimizing process parameters such as the wall temperature, filament current and time of deposition. The x-ray diffraction studies on the as-prepared films revealed polycrystalline nature. The composition of the chemical constituents present in the prepared bulk and thin films has been determ

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18

Cheng, Xin-Yan, Zheng-Ji Zhou, Ze-Liang Hou, Wen-Hui Zhou, and Si-Xin Wu. "High Performance Dye-Sensitized Solar Cell Using CuInGaSe₂ as Counter Electrode Prepared by Sputtering." Science of Advanced Materials 5, no. 9 (2013): 1193–98. http://dx.doi.org/10.1166/sam.2013.1572.

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19

Zaidi, B., N. Mekhaznia, M. S. Ullah, and H. Al-Dmour. "Evaluating the Efficiency of CuInGaSe₂ Based Solar Cells: CuSCN Hole Transport Layer (HTL) Effect." Journal of Physics: Conference Series 2843, no. 1 (2024): 012012. http://dx.doi.org/10.1088/1742-6596/2843/1/012012.

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Abstract Copper indium gallium disulfide (CuInGaSe2) or (CIGS) based solar cells are emerging solar cell structures that have attracted significant interest in recent years. In this research, a SCAPS-1D simulator was used to investigate the performance of the proposed CIGS based solar cell under the effect of a copper (I) thiocyanate (CuSCN) hole transport layer (HTL). Different photovoltaic parameters, such as the efficiency, short circuit current density (Jsc) and open-circuit voltage (Voc), are observed with respect to the doping concentration, temperature, and thickness. A comparative stud

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20

Oliveri, Roberto Luigi, Bernardo Patella, Floriana Di Pisa, Alfonso Mangione, Giuseppe Aiello, and Rosalinda Inguanta. "Fabrication of CZTSe/CIGS Nanowire Arrays by One-Step Electrodeposition for Solar-Cell Application." Materials 14, no. 11 (2021): 2778. http://dx.doi.org/10.3390/ma14112778.

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The paper reports some preliminary results concerning the manufacturing process of CuZnSnSe (CZTSe) and CuInGaSe (CIGS) nanowire arrays obtained by one-step electrodeposition for p-n junction fabrication. CZTSe nanowires were obtained through electrodeposition in a polycarbonate membrane by applying a rectangular pulsed current, while their morphology was optimized by appropriately setting the potential and the electrolyte composition. The electrochemical parameters, including pH and composition of the solution, were optimized to obtain a mechanically stable array of nanowires. The samples wer

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21

Gour, K. S., R. Parmar, O. P. Singh, and V. N. Singh. "Optimizing CuInGaSe₂ Thin Films Grown by Selenization of Culn/CuGa Multilayers for Solar Cell Applications." Advanced Science, Engineering and Medicine 8, no. 4 (2016): 314–18. http://dx.doi.org/10.1166/asem.2016.1860.

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22

Wang, Chen, Daming Zhuang, Ming Zhao, et al. "Optimization of CuInGaSSe properties and CuInGaSSe/CdS interface quality for efficient solar cells processed with CuInGa precursors." Journal of Power Sources 479 (December 2020): 229105. http://dx.doi.org/10.1016/j.jpowsour.2020.229105.

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23

Kim, Sung Chul. "Simulation of Rough Surface of CIGS (CuInGaSe) Solar Cell by RCWA (Rigorous Coupled Wave Analysis) Considering the Incoherency of Light." Journal of the Optical Society of Korea 18, no. 2 (2014): 180–83. http://dx.doi.org/10.3807/josk.2014.18.2.180.

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24

Yamaguchi, T., T. Hirao, S. Niiyama, and Y. Miyake. "Cu(In,Ga)(S,Se)2 thin films prepared by thermal crystallization from CuInGaSe/CuGaSe precursor in S/Se atmosphere." physica status solidi (c) 3, no. 8 (2006): 2555–58. http://dx.doi.org/10.1002/pssc.200669552.

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25

Dharmadasa, I. M., N. B. Chaure, G. J. Tolan, and A. P. Samantilleke. "Development of p[sup +], p, i, n, and n[sup +]-Type CuInGaSe[sub 2] Layers for Applications in Graded Bandgap Multilayer Thin-Film Solar Cells." Journal of The Electrochemical Society 154, no. 6 (2007): H466. http://dx.doi.org/10.1149/1.2718401.

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26

Kim, Hong Tak, Chang-Duk Kim, and Young-Soo Sohn. "Properties of CuInGaSe₂ (CIGS) Films Formed by a Rapid Thermal Annealing Process of CuGaSe₂/CuInSe₂ Stacked Layers." Journal of Nanoelectronics and Optoelectronics 10, no. 4 (2015): 471–74. http://dx.doi.org/10.1166/jno.2015.1784.

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27

Ru Hsu, Hung, Shu Chun Hsu, and Yung-sheng Liu. "Improvement of Voc and Jsc in CuInGaSe2 solar cells using a novel sandwiched CuGa/CuInGa/In precursor structure." Applied Physics Letters 100, no. 23 (2012): 233903. http://dx.doi.org/10.1063/1.4705297.

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28

Gour, Kuldeep S., Rahul Parmar, Rahul Kumar, and Vidya N. Singh. "Cd-Free Zn(O,S) as Alternative Buffer Layer for Chalcogenide and Kesterite Based Thin Films Solar Cells: A Review." Journal of Nanoscience and Nanotechnology 20, no. 6 (2020): 3622–35. http://dx.doi.org/10.1166/jnn.2020.17537.

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Cd is categorized as a toxic material with restricted use in electronics as there are inherent problems of treating waste and convincing consumers that it is properly sealed inside without any threat of precarious leaks. Apart from toxicity, band-gap of CdS is about 2.40–2.50 eV, which results significant photon loss in short-wavelength range which restricts the overall performance of solar cells. Thin film of Zn(O,S) is a favorable contender to substitute CdS thin film as buffer layer for CuInGaSe2 (CIGS), CuInGa(S,Se)2 (CIGSSe), Cu2ZnSn(S,Se)4 (CZTSSe) Cu2ZnSnSe4 (CZTSe), Cu2ZnSnS4 (CZTS) th

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29

Hsu, Hung-Ru, Shu-Chun Hsu, and Y. S. Liu. "Improvement of Ga distribution and enhancement of grain growth of CuInGaSe2 by incorporating a thin CuGa layer on the single CuInGa precursor." Solar Energy 86, no. 1 (2012): 48–52. http://dx.doi.org/10.1016/j.solener.2011.09.005.

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30

Deshmukh, Swapnil D., Kyle G. Weideman, Ryan G. Ellis, Kim Kisslinger, and Rakesh Agrawal. "Enabling fine-grain free 2-micron thick CISe/CIGSe film fabrication via a non-hydrazine based solution processing route." Materials Advances 3, no. 7 (2022): 3293–302. http://dx.doi.org/10.1039/d2ma00095d.

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Fine grain layer formation in solution processed CuInSe2/CuInGaSe2 (CISe/CIGSe) photovoltaic devices is controlled through surface modifications and ink manipulations to achieve improved performance and fine grain free morphologies.

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31

Perera, Sanjaya D., Haitao Zhang, Xiaoyue Ding, Andrew Nelson, and Richard D. Robinson. "Nanocluster seed-mediated synthesis of CuInS2 quantum dots, nanodisks, nanorods, and doped Zn-CuInGaS2 quantum dots." Journal of Materials Chemistry C 3, no. 5 (2015): 1044–55. http://dx.doi.org/10.1039/c4tc01887g.

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32

Gaillard, Nicolas, Wilman Septina, Joel Varley, et al. "Performance and limits of 2.0 eV bandgap CuInGaS2 solar absorber integrated with CdS buffer on F:SnO2 substrate for multijunction photovoltaic and photoelectrochemical water splitting devices." Materials Advances 2, no. 17 (2021): 5752–63. http://dx.doi.org/10.1039/d1ma00570g.

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Photocurrent density in excess of 10 mA cm−2 reported on 2.0 eV CuInGaS2 solar cells integrated on SnO2:F substrates, yet new wide bandgap n-type buffers required to achieve higher photoconversion efficiency.

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33

Murali, K. R., and V. Chitra. "Properties of Pulse Electrodeposited CuInGaSe2 Films." ECS Transactions 69, no. 31 (2015): 15–20. http://dx.doi.org/10.1149/06931.0015ecst.

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34

Khatri, Ishwor, Camden Kasik, and James R. Sites. "Ten-Year Performance Growth of Major Commercial Single-Junction Solar Cell Technologies." Electronics 14, no. 12 (2025): 2358. https://doi.org/10.3390/electronics14122358.

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Commercial electricity is increasingly being generated by renewable energy sources, and the photovoltaic conversion of sunlight is the fastest-growing renewable source. In addition to its rapid growth, solar electricity generation has seen very dramatic reductions in cost, as well as continuing increases in its conversion efficiency and installation lifetime. The growth between 2014 and 2024 in the record cell-level performance of four commercial technologies based on Si, CdTe, CuInGaSe2, and perovskites is compared with each other, with the highest achieved by GaAs, which is primarily used in

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35

Baan, Marzieh, Ari N. Blumer, and Tyler J. Grassman. "EBSD of Rough Native CuInGaSe2 Thin-Films." Microscopy and Microanalysis 27, S1 (2021): 3442–44. http://dx.doi.org/10.1017/s1431927621011831.

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36

Chun, Y. G., K. H. Kim, and K. H. Yoon. "Synthesis of CuInGaSe2 nanoparticles by solvothermal route." Thin Solid Films 480-481 (June 2005): 46–49. http://dx.doi.org/10.1016/j.tsf.2004.11.078.

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37

Kikuchi, Kenji, Shigeyuki Imura, Kazunori Miyakawa, Hiroshi Ohtake, Misao Kubota, and Eiji Ohta. "Photocurrent multiplication in Ga2O3/CuInGaSe2 heterojunction photosensors." Sensors and Actuators A: Physical 224 (April 2015): 24–29. http://dx.doi.org/10.1016/j.sna.2015.01.001.

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38

He, Xiaoqing, Tadas Paulauskas, Peter Ercius, et al. "Cd doping at PVD-CdS/CuInGaSe2 heterojunctions." Solar Energy Materials and Solar Cells 164 (May 2017): 128–34. http://dx.doi.org/10.1016/j.solmat.2017.01.043.

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39

Harayama, Koudai, Akira Nagaoka, Taizo Masuda, Kensuke Nishioka, and Kenji Yoshino. "Growth and Characterization of CuInGaSe2 Single Crystal." ECS Meeting Abstracts MA2020-02, no. 68 (2020): 3614. http://dx.doi.org/10.1149/ma2020-02683614mtgabs.

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40

Mandati, Sreekanth, and Bulusu V. Sarada. "Electrodeposited chalcopyrite CuInGaSe2 absorbers for solar energy harvesting." Materials Science for Energy Technologies 3 (2020): 440–45. http://dx.doi.org/10.1016/j.mset.2020.03.001.

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41

Der Wu, Jiann, Ling Ting Wang, and Chie Gau. "Synthesis of CuInGaSe2 nanoparticles by modified polyol route." Solar Energy Materials and Solar Cells 98 (March 2012): 404–8. http://dx.doi.org/10.1016/j.solmat.2011.11.044.

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42

Yanagisawa, T., T. Kojima, T. Koyanagi, K. Takahisa, and K. Nakamura. "Behaviour of CuInGaSe2 solar cells under light irradiation." Electronics Letters 36, no. 19 (2000): 1659. http://dx.doi.org/10.1049/el:20001176.

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43

Hameed, Talaat A., I. M. El Radaf, and Hani E. Elsayed-Ali. "Characterization of CuInGeSe4 thin films and Al/n–Si/p–CuInGeSe4/Au heterojunction device." Journal of Materials Science: Materials in Electronics 29, no. 15 (2018): 12584–94. http://dx.doi.org/10.1007/s10854-018-9375-7.

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44

Hsieh, Tung-Po, Chia-Chih Chuang, Chung-Shin Wu, Jen-Chuan Chang, Jhe-Wei Guo, and Wei-Chien Chen. "Effects of residual copper selenide on CuInGaSe2 solar cells." Solid-State Electronics 56, no. 1 (2011): 175–78. http://dx.doi.org/10.1016/j.sse.2010.11.019.

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45

Ramanathan, K., G. Teeter, J. C. Keane, and R. Noufi. "Properties of high-efficiency CuInGaSe2 thin film solar cells." Thin Solid Films 480-481 (June 2005): 499–502. http://dx.doi.org/10.1016/j.tsf.2004.11.050.

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46

Kim, Ki-Hyun, Young-Gab Chun, Kyung-Hoon Yoon, and Byung-Ok Park. "Synthesis of CuInGaSe2 nanoparticles by low temperature colloidal route." Journal of Mechanical Science and Technology 19, no. 11 (2005): 2085–90. http://dx.doi.org/10.1007/bf02916502.

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47

Choi, In-Hwan, Chul-Hwan Choi, and Joo-Won Lee. "Deep centers in a CuInGaSe2 /CdS/ZnO:B solar cell." physica status solidi (a) 209, no. 6 (2012): 1192–97. http://dx.doi.org/10.1002/pssa.201127596.

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48

Hsiao, Yu-Jen, Chung-Hsin Lu, and Te-Hua Fang. "To Enhance Performance of Light Soaking Process on ZnS/CuIn1-xGaxSe2Solar Cell." International Journal of Photoenergy 2013 (2013): 1–5. http://dx.doi.org/10.1155/2013/561948.

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The ZnS/CuInGaSe2heterojunction solar cell fabricated on Mo coated glass is studied. The crystallinity of the CIGS absorber layer is prepared by coevaporated method and the ZnS buffer layer with a band gap of 3.21 eV. The MoS2phase was also found in the CuInGaSe2/Mo system form HRTEM. The light soaking effect of photoactive film for 10 min results in an increase in F.F. from 55.8 to 64%, but series resistivity from 7.4 to 3.8 Ω. The efficiency of the devices improved from 8.12 to 9.50%.

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49

Rzheutski, Mikalai, Vasilii Cherkesov, Dzmitry Kabanau, Evgenii Lutsenko, and Liliya Bui. "A Benchtop X-Ray Diffractometer as a Tool for Thin Film Characterization." Materials Science Forum 1141 (December 20, 2024): 111–17. https://doi.org/10.4028/p-1dvv4m.

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An application of compact benchtop X-ray diffractometer for investigation of thin film semiconductor structures was demonstrated. A depth-dependent qualitative phase analysis of multilayer polycrystalline CuInGaSe2-based solar cell structure was performed. The independent goniometer allowed determination of residual stress values in the molybdenum layer of the solar cell. Grazing-incidence X-ray diffractometry was used to estimate polycrystallinity degree of AlN layers grown by molecular beam epitaxy and correlate it with the growth temperature. X-ray reflectometry measurement were also perfor

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50

Hsieh, Li Zen, Xi Ming Duan, and Ming Jer Jeng. "The Study of CIGS Absorption Layer Grown by Two-Step Growth Method for Thin-Film Solar Cell." Applied Mechanics and Materials 418 (September 2013): 238–41. http://dx.doi.org/10.4028/www.scientific.net/amm.418.238.

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Two-step growth method was used for CuInGaSe2,(CIGS) absorption layer in this study. The layer was first deposited by thermal evaporator to use indium and gallium sauces at a vacuum of 5 × 10-6 torr and secondly, the deposited thin film was enclosed in a quartz cartridge for the first selenization. The second selenization process was coated by copper and then annealed again in a furnace. Finding best precursor for thin film solar cells was analyzed by scanning electron microscope (SEM), X-ray diffraction analyzer (XRD) and energy dispersive spectrometer (EDS).

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