Journal articles on the topic 'Crystalline silicon solar cells'

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1

Van Overstraeten, Roger. "Crystalline silicon solar cells." Renewable Energy 5, no. 1-4 (August 1994): 103–6. http://dx.doi.org/10.1016/0960-1481(94)90359-x.

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2

Martinelli, G. "Crystalline Silicon for Solar Cells." Solid State Phenomena 32-33 (December 1993): 21–26. http://dx.doi.org/10.4028/www.scientific.net/ssp.32-33.21.

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3

Kittler, Martin, and Wolfgang Koch. "Crystalline Silicon for Solar Cells." Solid State Phenomena 82-84 (November 2001): 695–700. http://dx.doi.org/10.4028/www.scientific.net/ssp.82-84.695.

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4

Willeke, G. P. "Thin crystalline silicon solar cells." Solar Energy Materials and Solar Cells 72, no. 1-4 (April 2002): 191–200. http://dx.doi.org/10.1016/s0927-0248(01)00164-7.

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5

Dimitrov, Dimitre Z., Ching-Hsi Lin, Chen-Hsun Du, and Chung-Wen Lan. "Nanotextured crystalline silicon solar cells." physica status solidi (a) 208, no. 12 (August 29, 2011): 2926–33. http://dx.doi.org/10.1002/pssa.201127150.

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6

Yang, Hong, He Wang, and Dingyue Cao. "Investigation of soldering for crystalline silicon solar cells." Soldering & Surface Mount Technology 28, no. 4 (September 5, 2016): 222–26. http://dx.doi.org/10.1108/ssmt-04-2015-0015.

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Purpose Tabbing and stringing are the critical process for crystalline silicon solar module production. Because of the mismatch of the thermal expansion coefficients between silicon and metal, phenomenon of cell bowing, microcracks formation or cell breakage emerge during the soldering process. The purpose of this paper is to investigate the effect of soldering on crystalline silicon solar cells and module, and reveal soldering law so as to decrease the breakage rates and improve reliability for crystalline silicon solar module. Design/methodology/approach A microscopic model of the soldering process is developed by the study of the crystalline silicon solar cell soldering process in this work. And the defects caused by soldering were analyzed systematically. Findings The defects caused by soldering are analyzed systematically. The optimal soldering conditions are derived for the crystalline silicon solar module. Originality/value The quality criterion of soldering for crystalline silicon solar module is built for the first time. The optimal soldering conditions are derived for the crystalline silicon solar module. This study provides insights into solder interconnection reliability in the photovoltaic (PV) industry.
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7

Cho, Eun-Chel, Sangwook Park, Xiaojing Hao, Dengyuan Song, Gavin Conibeer, Sang-Cheol Park, and Martin A. Green. "Silicon quantum dot/crystalline silicon solar cells." Nanotechnology 19, no. 24 (May 9, 2008): 245201. http://dx.doi.org/10.1088/0957-4484/19/24/245201.

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8

Wang, Ying Lian, and Jun Yao Ye. "Review and Development of Crystalline Silicon Solar Cell with Intelligent Materials." Advanced Materials Research 321 (August 2011): 196–99. http://dx.doi.org/10.4028/www.scientific.net/amr.321.196.

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The application of solar cell has offered human society renewable clean energy. As intelligent materials, crystalline silicon solar cells occupy absolutely dominant position in photovoltaic market, and this position will not change for a long time in the future. Thereby increasing the efficiency of crystalline silicon solar cells, reducing production costs and making crystalline silicon solar cells competitive with conventional energy sources become the subject of today's PV market. The working theory of solar cell was introduced. The developing progress and the future development of mono-crystalline silicon (c-Si), poly-crystalline silicon (p-Si) and amorphous silicon (a-Si) solar cell have also been introduced.
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9

Glunz, S. W. "High-Efficiency Crystalline Silicon Solar Cells." Advances in OptoElectronics 2007 (August 28, 2007): 1–15. http://dx.doi.org/10.1155/2007/97370.

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The current cost distribution of a crystalline silicon PV module is clearly dominated by material costs, especially by the costs of the silicon wafer. Therefore cell designs that allow the use of thinner wafers and the increase of energy conversion efficiency are of special interest to the PV industry. This article gives an overview of the most critical issues to achieve this aim and of the recent activities at Fraunhofer ISE and other institutes.
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10

Knobloch, J., and A. Eyer. "Crystalline Silicon Materials and Solar Cells." Materials Science Forum 173-174 (September 1994): 297–310. http://dx.doi.org/10.4028/www.scientific.net/msf.173-174.297.

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11

Zhong, Sihua, and Wenzhong Shen. "Quasi-omnidirectional crystalline silicon solar cells." Journal of Physics D: Applied Physics 53, no. 48 (September 8, 2020): 483001. http://dx.doi.org/10.1088/1361-6463/abac2d.

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12

Koynov, Svetoslav, Martin S. Brandt, and Martin Stutzmann. "Black multi-crystalline silicon solar cells." physica status solidi (RRL) – Rapid Research Letters 1, no. 2 (March 2007): R53—R55. http://dx.doi.org/10.1002/pssr.200600064.

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13

Sah, C. T. "High efficiency crystalline silicon solar cells." Solar Cells 17, no. 1 (March 1986): 1–27. http://dx.doi.org/10.1016/0379-6787(86)90056-6.

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14

Aulich, Hubert A., and Friedrich-Wilhelm Schulze. "Crystalline silicon feedstock for solar cells." Progress in Photovoltaics: Research and Applications 10, no. 2 (2002): 141–47. http://dx.doi.org/10.1002/pip.415.

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15

Kunst, M., S. von Aichberger, G. Citarella, and F. Wünsch. "Amorphous silicon/crystalline silicon heterojunctions for solar cells." Journal of Non-Crystalline Solids 299-302 (April 2002): 1198–202. http://dx.doi.org/10.1016/s0022-3093(01)01139-5.

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16

Schmidt, K. J., Y. Lin, M. Beaudoin, G. Xia, S. K. O’Leary, G. Yue, and B. Yan. "The mean crystallite size within a hydrogenated nanocrystalline silicon based photovoltaic solar cell and its role in determining the corresponding crystalline volume fraction." Canadian Journal of Physics 92, no. 7/8 (July 2014): 857–61. http://dx.doi.org/10.1139/cjp-2013-0526.

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We examine the dependence of the crystalline volume fraction on the mean crystallite size for hydrogenated nanocrystalline silicon based photovoltaic solar cells; this work builds upon an earlier study by Schmidt et al. (Mater. Res. Soc. Symp. Proc. 1536 (2013)). For each photovoltaic solar cell considered, the X-ray diffraction and Raman spectra are measured. Through the application of Scherrer’s equation, the X-ray diffraction results are used to determine the corresponding mean crystallite sizes. Through peak decomposition, the Raman results are used to estimate the corresponding crystalline volume fraction. Plotting the crystalline volume fraction as a function of the mean crystallite size, it is found that larger mean crystallite sizes tend to favor reduced crystalline volume fractions. The ability to randomly pack smaller crystallites with a greater packing fraction than their larger counterparts was suggested as a possible explanation for this observation.
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17

Yang, Hong, He Wang, and Minqiang Wang. "Investigation of the Relationship between Reverse Current of Crystalline Silicon Solar Cells and Conduction of Bypass Diode." International Journal of Photoenergy 2012 (2012): 1–5. http://dx.doi.org/10.1155/2012/357218.

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In the process of crystalline silicon solar cells production, there exist some solar cells whose reverse current is larger than 1.0 A because of silicon materials and process. If such solar cells are encapsulated into solar modules, hot-spot phenomenon will emerge in use. In this paper, the effect of reverse current on reliability of crystalline silicon solar modules was investigated. Based on the experiments, considering the different shaded rate of cells, the relation between reverse current of crystalline silicon solar cells and conduction of bypass diode was investigated for the first time. To avoid formation of hot spots and failure of solar modules, the reverse current should be smaller than 1.0 A for 125 mm × 125 mm monocrystalline silicon solar cells when the bias voltage is at −12 V.
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18

Omar, Khalid, and Khaldun A. Salman. "Effects of Electrochemical Etching Time on the Performance of Porous Silicon Solar Cells on Crystalline n-Type (100) and (111)." Journal of Nano Research 46 (March 2017): 45–56. http://dx.doi.org/10.4028/www.scientific.net/jnanor.46.45.

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Electrochemical etching was carried out to produce porous silicon based on crystalline silicon n-type (100) and (111) wafers. Etching times of 10, 20, and 30 min were applied. Porous silicon layer was used as anti-reflection coating on crystalline silicon solar cells. The optimal etching time is 20 min for preparing porous silicon layers based on crystalline silicon n-type (100) and (111) wafers. Nanopores with high porosity were produced on the porous silicon layer based on crystalline silicon n-type (100) and (111) wafers with average diameters of 5.7 and 5.8 nm, respectively. Average crystallite sizes for the porous silicon layer based on crystalline silicon n-type (100) and (111) wafers were 20.57 and 17.45 nm at 20 and 30 min, respectively, due to the increase in broadening of the full width at half maximum. Photoluminescence peaks for porous silicon layers based on crystalline silicon n-type (100) and (111) wafers increased with growing porosity and a great blue shift in luminescence. The minimum effective coefficient of reflection was obtained from porous silicon layers based on the crystalline silicon n-type (100) wafer compared with n-type (111) wafer and as-grown at different etching times. Porous silicon layers based on the crystalline silicon n-type (100) wafer at 20 min etching time exhibited excellent light trapping at wavelengths ranging from 400 to 1000 nm. Thus, fabricated crystalline silicon solar cells based on porous silicon (100) anti-reflection coating layers achieved the highest efficiency at 15.50% compared to porous silicon (111) anti-reflection coating layers. The efficiency is characterized applying I-V characterization system under 100 mW/cm2 illumination conditions.
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19

Wang, He, Ao Wang, Hong Yang, and Dengyuan Song. "Analysis of the Thermal Stress for Combined Electrode of Soldered Crystalline Silicon Solar Cells under Temperature Field." International Journal of Photoenergy 2016 (2016): 1–7. http://dx.doi.org/10.1155/2016/5306925.

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Based on the theory of material mechanics and thermal stress analysis, the stress distribution of combined electrode for crystalline silicon solar module was studied for the first time. The shear stress and normal stress distribution of soldered structure for crystalline silicon solar cells under the thermal field were discussed. And the results show that the stress distribution is not simply linear relationship as some results found. But there is a stress concentration at the edge, which was considered as the true reason that caused microcracks at the edge of soldered solar cells. The conclusions we got in this paper provide a theoretical basis for deceasing the breakage rates of soldered crystalline silicon solar cells and improving the reliability of crystalline silicon solar modules.
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20

Ma, Dayan, NuoFu Chen, Quanli Tao, Jiaran Xu, Yiming Bai, and Jikun Chen. "A novel model of mono-crystalline silicon p-n homojunction." European Physical Journal Applied Physics 82, no. 1 (April 2018): 10101. http://dx.doi.org/10.1051/epjap/2018180041.

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A novel model for analyzing the conversion efficiency of mono-crystalline silicon solar cells is improved based on the detailed balance principle. The maximum theoretical conversion efficiency of the conventional planar mono-crystalline silicon solar cells has been updated to 27.94% according to the improved model. Furthermore this model is extending to cylindrical coordinates for estimating the radial p-n junction mono-crystalline silicon solar cells. A radial p-n junction mono-crystalline silicon solar cell with the highest conversion efficiency of 32.9% has been designed as that the radius of n-Si core is 1 µm, the radius of the cylinder is 40 µm, and the height of cylinder is 100 µm.
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21

NIJS, J. F., J. SZLUFCIK, J. POORTMANS, and R. P. MERTENS. "CRYSTALLINE SILICON BASED PHOTOVOLTAICS: TECHNOLOGY AND MARKET TRENDS." Modern Physics Letters B 15, no. 17n19 (August 20, 2001): 571–78. http://dx.doi.org/10.1142/s021798490100204x.

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An overview is given concerning industrial technologies, IMECS's advanced pilot line crystalline silicon solar cell technologies and medium term developments for industrial crystalline silicon terrestrial solar cell fabrication. Also IMEC's work on thin film crystalline silicon solar cells is shortly presented, all of this taking into account the existing market and technology trends.
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22

ur Rehman, Atteq, and Soo Hong Lee. "Advancements in n-Type Base Crystalline Silicon Solar Cells and Their Emergence in the Photovoltaic Industry." Scientific World Journal 2013 (2013): 1–13. http://dx.doi.org/10.1155/2013/470347.

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The p-type crystalline silicon wafers have occupied most of the solar cell market today. However, modules made with n-type crystalline silicon wafers are actually the most efficient modules up to date. This is because the material properties offered by n-type crystalline silicon substrates are suitable for higher efficiencies. Properties such as the absence of boron-oxygen related defects and a greater tolerance to key metal impurities by n-type crystalline silicon substrates are major factors that underline the efficiency of n-type crystalline silicon wafer modules. The bi-facial design of n-type cells with good rear-side electronic and optical properties on an industrial scale can be shaped as well. Furthermore, the development in the industrialization of solar cell designs based on n-type crystalline silicon substrates also highlights its boost in the contributions to the photovoltaic industry. In this paper, a review of various solar cell structures that can be realized on n-type crystalline silicon substrates will be given. Moreover, the current standing of solar cell technology based on n-type substrates and its contribution in photovoltaic industry will also be discussed.
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23

Jagannathan, B., W. A. Anderson, and J. Coleman. "Amorphous silicon/p-type crystalline silicon heterojunction solar cells." Solar Energy Materials and Solar Cells 46, no. 4 (July 1997): 289–310. http://dx.doi.org/10.1016/s0927-0248(97)00012-3.

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24

Roca, F., G. Sinno, G. Di Francia, P. Prosini, G. Fameli, P. Grillo, A. Citarella, F. Pascarella, and D. della Sala. "Process development of amorphous silicon/crystalline silicon solar cells." Solar Energy Materials and Solar Cells 48, no. 1-4 (November 1997): 15–24. http://dx.doi.org/10.1016/s0927-0248(97)00063-9.

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25

Jeong, Myeong Sang, Yonghwan Lee, Ka-Hyun Kim, Sungjin Choi, Min Gu Kang, Soo Min Kim, and Hee-eun Song. "Numerical Simulation Analysis of Ag Crystallite Effects on Interface of Front Metal and Silicon in the PERC Solar Cell." Energies 14, no. 3 (January 25, 2021): 592. http://dx.doi.org/10.3390/en14030592.

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In the fabrication of crystalline silicon solar cells, the contact properties between the front metal electrode and silicon are one of the most important parameters for achieving high-efficiency, as it is an integral element in the formation of solar cell electrodes. This entails an increase in the surface recombination velocity and a drop in the open-circuit voltage of the solar cell; hence, controlling the recombination velocity at the metal-silicon interface becomes a critical factor in the process. In this study, the distribution of Ag crystallites formed on the silicon-metal interface, the surface recombination velocity in the silicon-metal interface and the resulting changes in the performance of the Passivated Emitter and Rear Contact (PERC) solar cells were analyzed by controlling the firing temperature. The Ag crystallite distribution gradually increased corresponding to a firing temperature increase from 850 ∘C to 950 ∘C. The surface recombination velocity at the silicon-metal interface increased from 353 to 599 cm/s and the open-circuit voltage of the PERC solar cell decreased from 659.7 to 647 mV. Technology Computer-Aided Design (TCAD) simulation was used for detailed analysis on the effect of the surface recombination velocity at the silicon-metal interface on the PERC solar cell performance. Simulations showed that the increase in the distribution of Ag crystallites and surface recombination velocity at the silicon-metal interface played an important role in the decrease of open-circuit voltage of the PERC solar cell at temperatures of 850–900 ∘C, whereas the damage caused by the emitter over fire was determined as the main cause of the voltage drop at 950 ∘C. These results are expected to serve as a steppingstone for further research on improvement in the silicon-metal interface properties of silicon-based solar cells and investigation on high-efficiency solar cells.
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26

Tanaka, Makoto. "Recent progress in crystalline silicon solar cells." IEICE Electronics Express 10, no. 16 (2013): 20132006. http://dx.doi.org/10.1587/elex.10.20132006.

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27

DING Wu-chang, 丁武昌. "Light management in crystalline silicon solar cells." Chinese Journal of Optics and Applied Optics 6, no. 5 (2013): 717–28. http://dx.doi.org/10.3788/co.20130605.0717.

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28

Wang, Weining, and E. A. Schiff. "Polyaniline on crystalline silicon heterojunction solar cells." Applied Physics Letters 91, no. 13 (September 24, 2007): 133504. http://dx.doi.org/10.1063/1.2789785.

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29

Xiong, Huaping, Chuanhai Gan, Xiaobing Yang, Zhigang Hu, Haiyan Niu, Jianfeng Li, Jianfang Si, Pengfei Xing, and Xuetao Luo. "Corrosion behavior of crystalline silicon solar cells." Microelectronics Reliability 70 (March 2017): 49–58. http://dx.doi.org/10.1016/j.microrel.2017.01.006.

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30

Blakers, Andrew W. "Substrates for thin crystalline silicon solar cells." Solar Energy Materials and Solar Cells 51, no. 3-4 (February 1998): 385–92. http://dx.doi.org/10.1016/s0927-0248(97)00257-2.

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31

Blakers, Andrew, Vernie Everett, Jelena Muric-Nesic, and Elizabeth Thomsen. "Thin Single Crystalline Elongate Silicon Solar Cells." Energy Procedia 15 (2012): 58–66. http://dx.doi.org/10.1016/j.egypro.2012.02.007.

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32

ZHANG Yin-bo, 张寅博, 潘淼 PAN Miao, 程翔 CHENG Xiang, and 陈朝 CHEN Chao. "Numerical Simulation for Crystalline Silicon Solar Cells." Chinese Journal of Luminescence 33, no. 6 (2012): 660–64. http://dx.doi.org/10.3788/fgxb20123306.0660.

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33

Allen, Thomas G., James Bullock, Xinbo Yang, Ali Javey, and Stefaan De Wolf. "Passivating contacts for crystalline silicon solar cells." Nature Energy 4, no. 11 (September 16, 2019): 914–28. http://dx.doi.org/10.1038/s41560-019-0463-6.

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34

Juvonen, T., J. H?rk?nen, P. Kuivalainen, and P. Kuivalainen. "High Efficiency Single Crystalline Silicon Solar Cells." Physica Scripta T101, no. 1 (2002): 96. http://dx.doi.org/10.1238/physica.topical.101a00096.

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35

Basore, Paul A. "Defining terms for crystalline silicon solar cells." Progress in Photovoltaics: Research and Applications 2, no. 2 (April 1994): 177–79. http://dx.doi.org/10.1002/pip.4670020213.

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36

Green, Martin A. "The future of crystalline silicon solar cells." Progress in Photovoltaics: Research and Applications 8, no. 1 (January 2000): 127–39. http://dx.doi.org/10.1002/(sici)1099-159x(200001/02)8:1<127::aid-pip311>3.0.co;2-d.

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37

Breitenstein, O., J. P. Rakotoniaina, M. H. Al Rifai, and M. Werner. "Shunt types in crystalline silicon solar cells." Progress in Photovoltaics: Research and Applications 12, no. 7 (2004): 529–38. http://dx.doi.org/10.1002/pip.544.

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38

Barnett, Allen M., Robert B. Hall, and James A. Rand. "Thin Polycrystalline Silicon Solar Cells." MRS Bulletin 18, no. 10 (October 1993): 33–37. http://dx.doi.org/10.1557/s0883769400038264.

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Solar cells formed with thin silicon active layers (<100 μm thick) offer advantages over thick ingot-based devices. The advantages come in two forms: the first is the potential for higher conversion efficiency than that of conventional thick devices, and the second is a reduction in material requirements. The use of thin polycrystalline silicon for solar cells offers the potential of capturing the high performance of crystalline silicon while achieving the potential low cost of thin films. Experimental and theoretical studies initially uncovered the issues of grain size and thickness as limiting factors. Subsequent work added the issue of back-surface passivation. This article addresses the conditions required for the successful development of polycrystalline silicon into a high efficiency, low-cost, terrestrial product.
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39

Schmidt, K. J., Y. Lin, M. Beaudoin, G. Xia, S. K. O'Leary, G. Yue, and B. Yan. "The dependence of the crystalline volume fraction on the crystallite size for hydrogenated nanocrystalline silicon based solar cells." MRS Proceedings 1536 (2013): 113–18. http://dx.doi.org/10.1557/opl.2013.599.

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ABSTRACTWe have performed an analysis on three hydrogenated nanocrystalline silicon (nc-Si:H) based solar cells. In order to determine the impact that impurities play in shaping the material properties, the XRD and Raman spectra corresponding to all three samples were measured. The XRD results, which displayed a number of crystalline silicon-based peaks, were used in order to approximate the mean crystallite sizes through Scherrer's equation. Through a peak decomposition process, the Raman results were used to estimate the corresponding crystalline volume fraction. It was noted that small crystallite sizes appear to favor larger crystalline volume fractions. This dependence seems to be related to the oxygen impurity concentration level within the intrinsic nc-Si:H layers.
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40

Wang, Chang Chun, and Kuang Jang Lin. "Analysis on Efficiency of Power Generation for Various Sun Tracking and Fixed Solar Cells under Different Sunshine Environment." Applied Mechanics and Materials 130-134 (October 2011): 1286–94. http://dx.doi.org/10.4028/www.scientific.net/amm.130-134.1286.

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Solar energy directly converses light energy into DC power without fuel, no moving parts, no pollution, and no noise with long life-span more than about twenty years. Its application is extensive and the set up of solar generation can be scattered and in a small amount on demand which is the most available of all renewable energy, and is the most practical and effective energy. There are many kinds of solar cell, such first generation as Mono-crystalline Silicon, Multi-crystalline Silicon, and Amorphous Silicon, the second generation as Film Photovoltaic and the third generation as Dye-Sensitized (DSSCs) etc. The utilization of solar energy is greatly influenced by environmental change with the main reason of solar radiation. This research collects the data from the test of Mono-crystalline Silicon, Multi-crystalline Silicon, and Film Photovaltaic solar cells in different solar radiation, and then conducts the analysis and research thereby. Using the program written by Labview, collect the data of voltage, current, and the power, solar radiation, and temperature emitted by solar cells under test for analysis. And then discuss the results of the collected data by Matlab for data analysis.
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41

Binetti, S., M. Acciarri, A. Le Donne, M. Morgano, and Y. Jestin. "Key Success Factors and Future Perspective of Silicon-Based Solar Cells." International Journal of Photoenergy 2013 (2013): 1–6. http://dx.doi.org/10.1155/2013/249502.

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Today, after more than 70 years of continued progress on silicon technology, about 85% of cumulative installed photovolatic (PV) modules are based on crystalline silicon (c-Si). PV devices based on silicon are the most common solar cells currently being produced, and it is mainly due to silicon technology that the PV has grown by 40% per year over the last decade. An additional step in the silicon solar cell development is ongoing, and it is related to a further efficiency improvement through defect control, device optimization, surface modification, and nanotechnology approaches. This paper attempts to briefly review the most important advances and current technologies used to produce crystalline silicon solar devices and in the meantime the most challenging and promising strategies acting to increase the efficiency to cost/ratio of silicon solar cells. Eventually, the impact and the potentiality of using a nanotechnology approach in a silicon-based solar cell are also described.
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42

Kang, Semi, Jungkyu Kwon, Changhoon Jeong, Sung-In Mo, Joon-Ho Oh, and Sangwoo Ryu. "Polycrystalline Silicon Membranes for Solar Cells Fabricated Using Water-soluble Sacrificial Layers." Ceramist 25, no. 1 (March 31, 2022): 52–62. http://dx.doi.org/10.31613/ceramist.2022.25.1.05.

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During the fabrication of crystalline silicon solar cells, kerf-loss caused by the wire-sawing of silicon ingots to produce thin wafers inevitably limits the reduction of electricity production cost. To avoid the kerf-loss, direct growth of crystalline silicon wafers of 50-150 μm with a porous separation layer that can be mechanically broken during the exfoliation process, has been widely investigated. However, several issues including flattening of the surface after the exfoliation remain unsolved. In this work an alternative method that utilizes a water-soluble Sr3Al2O6 (SAO) sacrificial layer inserted between the mother substrate and the grown crystalline silicon layers is introduced. Polycrystalline silicon layers were grown on SAO/Si by plasma-enhanced CVD process and silicon membranes could be successfully obtained after the dissolution of SAO in the water. Same process could be applied to obtain flexible amorphous silicon membranes. Further research is being conducted to increase the size of the exfoliated wafer, which expects to reduce the production cost of crystalline silicon solar cells effectively.
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43

Jensen, N., U. Rau, R. M. Hausner, S. Uppal, L. Oberbeck, R. B. Bergmann, and J. H. Werner. "Recombination mechanisms in amorphous silicon/crystalline silicon heterojunction solar cells." Journal of Applied Physics 87, no. 5 (March 2000): 2639–45. http://dx.doi.org/10.1063/1.372230.

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44

Moon, Inyong, Kyunghae Kim, M. Thamilselvan, Youngkuk Kim, Kyumin Han, Doheon Kyeong, Taeyoung Kwon, Dao Vinh Ai, Jeongchul Lee, and Minkyu Ju. "Selective emitter using porous silicon for crystalline silicon solar cells." Solar Energy Materials and Solar Cells 93, no. 6-7 (June 2009): 846–50. http://dx.doi.org/10.1016/j.solmat.2008.09.042.

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45

Scherff, M., R. Drzymalla, R. Gösse, W. R. Fahrner, M. Ferrara, H. Neitzert, J. Opitz-Coutureau, et al. "Proton Damage in Amorphous Silicon/Crystalline Silicon Heterojunction Solar Cells." Journal of The Electrochemical Society 153, no. 12 (2006): G1117. http://dx.doi.org/10.1149/1.2360771.

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46

Mews, Mathias, Caspar Leendertz, Michael Algasinger, Svetoslav Koynov, and Lars Korte. "Amorphous/crystalline silicon heterojunction solar cells with black silicon texture." physica status solidi (RRL) - Rapid Research Letters 8, no. 10 (July 30, 2014): 831–35. http://dx.doi.org/10.1002/pssr.201409327.

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47

Xue, Chun Rong. "Research on Nanocrystalline Silicon Film Solar Cells." Advanced Materials Research 347-353 (October 2011): 870–73. http://dx.doi.org/10.4028/www.scientific.net/amr.347-353.870.

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Nanocrystalline silicon film has become the research hit of today’ s P-V solar technology. It’s optical band gap was controlled through changing the grain size and crystalline volume fraction for the quanta dimension effect. The crystalline volume fraction in nc-Si:H is modulated by varying the hydrogen concentration in the silane plasma. Also, the crystallinity of the material increases with increasing hydrogen dilution ratio, the band tail energy width of the nc-Si:H concurrently decreases. Two sets of nc-Si:H solar cells were made with different layer thicknesss, their electronic and photonic bandgap, absorption coefficient, optical band gap, nanocrystalline grain size(D), and etc have been stuied. In addition, we discussed the relationship between the stress of nc-Si thin films and H2 ratio. At last nc-Si:H solar cells have been designed and prepared successfully in the optimized processing parameters.
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48

Chen, Yusi, Yangsen Kang, Jieyang Jia, Yijie Huo, Muyu Xue, Zheng Lyu, Dong Liang, Li Zhao, and James S. Harris. "Nanostructured Dielectric Layer for Ultrathin Crystalline Silicon Solar Cells." International Journal of Photoenergy 2017 (2017): 1–6. http://dx.doi.org/10.1155/2017/7153640.

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Nanostructures have been widely used in solar cells due to their extraordinary photon management properties. However, due to poor pn junction quality and high surface recombination velocity, typical nanostructured solar cells are not efficient compared with the traditional commercial solar cells. Here, we demonstrate a new approach to design, simulate, and fabricate whole-wafer nanostructures on dielectric layer on thin c-Si for solar cell light trapping. The optical simulation results show that the periodic nanostructure arrays on dielectric materials could suppress the reflection loss over a wide spectral range. In addition, by applying the nanostructured dielectric layer on 40 μm thin c-Si, the reflection loss is suppressed to below 5% over a wide spectra and angular range. Moreover, a c-Si solar cell with 2.9 μm ultrathin absorber layer demonstrates 32% improvement in short circuit current and 44% relative improvement in energy conversion efficiency. Our results suggest that nanostructured dielectric layer has the potential to significantly improve solar cell performance and avoid typical problems of defects and surface recombination for nanostructured solar cells, thus providing a new pathway towards realizing high-efficiency and low-cost c-Si solar cells.
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49

Liang, Z. C., D. M. Chen, X. Q. Liang, Z. J. Yang, H. Shen, and J. Shi. "Crystalline Si solar cells based on solar grade silicon materials." Renewable Energy 35, no. 10 (October 2010): 2297–300. http://dx.doi.org/10.1016/j.renene.2010.02.027.

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50

MacQueen, Rowan W., Martin Liebhaber, Jens Niederhausen, Mathias Mews, Clemens Gersmann, Sara Jäckle, Klaus Jäger, et al. "Crystalline silicon solar cells with tetracene interlayers: the path to silicon-singlet fission heterojunction devices." Materials Horizons 5, no. 6 (2018): 1065–75. http://dx.doi.org/10.1039/c8mh00853a.

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