JORDAN UNIVERSITY OF SCIENCE AND TECHNOLOGY SCIENCE AND ART COLLAGE APPLIED PHYSICS DEPARTMENT Physics 791 SEMINAR SOLAR CELLS FABRICATION SUPERVISION: Dr: ADNAN SHARIAH ENAS.M.HAMASHA 20053092008 1 TABLE OF CONENT: page Abstract…………………………..…………….3 1. Introduction …………………………………4 Single-crystal wafers technology………………6 2.1 Reduction of sand to metallurgical-grade silicon………………………………..…………6 2.1.1 Arc furnace……………….………………7 2.2 Metallurgical-Grade silicon to semiconductor grade silicon …………..……....………………9 2.3 Conversion of Semiconductor-grade silicon to single-crystal silicon wafers………..……………11 2.3.1 Czocharalski process…..…………………...11 2.3.2 Czocharalski procedure..…………………...11 2.3.2.1 Crucible………………………………….12 2.3.3 Silicon wafers……………………………..14 3. Processing of single crystal wafers to solar cells…………………………….………………..16 3.1 Doping……………………….……………...16 3.2 Contact wafers with metal..............................18 3.3 Antireflection coating..............................…...20 3.4 Texturing surface ………………..………….22 4. Solar cell to solar module..........................…...24 5. Discussion and result………………………….26 6. References……………………………………..27 2 TABLE OF FIGURE: PAGE Figure 1: schematic representation of the cost distribution for solar cell and module……………………………………………………………..6 Figure 2: the schematic explain the procedure fabrication solar cell……7 Figure 3: arc furnace and the inside reaction………………………8 Figure 4: electric arc furnace……………………………………………..9 Figure 5: CZ process……………………………………………………13 Figure 6: crucible use in CZ process before use………………………..13 Figure 7: crucible during annealing……………………………………14 Figure 8: A crucible after used………………………………………….14 Figure 9: single crystal ingot……………………………………………15 Figure 10: silicon wafer a) after cutting b) after polishing…………..….16 Figure 11: phosphourus diffusion process………………………..…….18 Figure 12: distribution of phosphorus impurities………………….19 Figure 13: Solar wafer with metal contact………………………………20 Figure 14: a metal shadow mask………………………………..21 Figure 15: Major feature of solar cell…………………………………...22 Figure 16: texturing surfaces silicon by SEM…………..………………24 Figure 17: Tracked PV Array containing 16 panels……………………..25 Figure 18: Photovoltaic cells, modules, panels and arrays……………...26 3 Abstract The life cycle of single crystal solar cell start with silica or silicon dioxide SiO2 also known as quartz sand, in order to obtain 99% pure metallurgical-grade silicon (MG-Si) the oxygen must first be extracted from the silicon dioxide by carbon reduction in an arc furnace then use siemens process to produce high purity silicon (99.9999%) semiconductor-grade silicon (SeG-Si) which is used for making the silicon wafers. These SeG-Si are melted in a crucible with boron dopant and either pulled/grown as cylinder this is czocharalski process to produce single crystalline cylindrical ingots, after solidification ingots are sawn into thin slices called wafers and doping this wafers by phosphorous impurities to form p-n junction in silicon wafers and will contact with metal grid in n-type side and metal layer in p-type side to accumulate the current carriers and to pass the electrical current outside the cells. The last step is contact many wafers with series or parallel to formation solar module and encapsulation solar module with glass to protection. 4 1. Introduction Beside other renewable energy sources photovoltaic (PV) present a prime source of non polluting energy, basically it is silicon based today, in particular, silicon is used in PV for single crystalline and poly crystalline wafers production. More than 90% of the annual solar silicon production is based on single crystalline silicon wafers, [1]. Therefore the silicon wafers fabrication is the most important technology for PV today. single c-Si cells are the most common in the PV industry and has a uniform molecular structure (which is the arrangement of atom in the material) compared to non crystal materials because the entire structure is grown from the same crystal, single c-Si high uniformly result in higher energy conversion efficiency, the higher a PV cells conversion efficiency the more electricity it generates for a given area of expose to the sunlight. The average price for a single-crystal solar module is 50$ in 1970 and dropped to 5$ in 1988 and 3.97$ in 1996, [2] the reason for the reduction cost is the improvement of the technology PV cell production. The cost of a module-typically (1-2) m² in size can be broken down into three main components: 35% for the solar Si material (ready for cell production) 30% for the solar cell technology (making a solar cell) 30% for module manufacture If one uses the conventional process to make single crystalline wafers as the starting material for solar cells, the cost can be broken down as follows: 30% starting material (poly-Si) 35% Crystal growth 30% sawing the crystal into wafers 5% for refining (etching, polishing, cleaning), [3] 5 One can shows this distribution of the cost in the Figure below: Starting material30% Sawing30% Crystal growth35% Refining 5% Figure 1: schematic representation of the cost distribution for solar cell and module. The objective in this project is studying the production of single-crystal wafers of silicon. 6 2-Single-crystal wafers technology The processing steps for the fabrication of a silicon wafers, which is the starting material for the fabrication of electronic devices and solar cells. Many process steps are conducted to bring Si from its native to crystalline substrate, one uses for solar cell fabrication, These steps show below: Figure 2: the schematic explain the procedure fabrication solar cell. 2.1 Reduction of sand to metallurgicalgrade silicon Silicon is the second most abundant element in the crust of the earth 27%, but it doesn't occur native element because SiO2 in the form of quartz, quartzite, and other component [4]. 7 The starting silicon for PV application is 99% pure metallurgical-grade silicon (MG-Si) obtained from reduction of SiO2 in an electric arc furnace, by carbon (in the form of a mixture of wood chips, coke and coals) [5] although the overall reaction can be considered: SiO2 + C CO2 + Si There are a complex series of reaction that take place in different temperature region of the furnace show in Figure 3: Figure 3: arc furnace and the inside reaction. 2.1.1 arc furnace The first electric arc furnace was development by Paul He'roult of furnace (1899) to make steel. An electric arc furnace is a system that heats charged material; the furnace is primarily split into three sections: 1) The shell, which consist of the sidewall and lower steel and bowel 2) The hearth, which consist of the refractory that lines the lower bowel 8 3) The roof, which may be refractory-lined or watercooled, and can be shaped as a section of a sphere or conical section[6], We can see the real arc furnace in Figure 5 below: Figure 4: electric arc furnace As shows in the Figure 3 the liquid silicon finally forming from SiC, Then the silicon liquid is periodically tapped from the furnace and typically allowed to solidify in shallow mold about 1.5× 1 m² in size, and the major impurities exist in silicon liquid is Al and Fe as table as below: Table 1: concentration impurity in M-G Si 9 So silicon liquid solidifies with impurities 99% and is subsequently broken into chunks. Characteristic of this stage is: 1 million metric tons of this MG-Si is produce globally each year (large production). Use MG-Si in the steel and aluminum industries. The total processing energy requirement is acceptable. The result the MG-Si is inexpensive (low cost) in 1997 MG-Si cost about 5$ per Kg. 99% pure with the major impurities being iron and aluminum. 2.2 Metallurgical-Grade silicon to semiconductor grade silicon In this stage one can get a semiconductor grade silicon by purification metallurgical–Grade silicon in an (a siemens process) which included multiple steps. The following refining procedures use the conversion MG-Si into volatile component such as silane (SiH4) by reaction MG-Si with HCl. The volatile component are purified by chemical method which is condensed and fractional distillation Back to the arc furnace reaction to take phase product: Solidificatio n SiO2 (s) + C (s) arc furnace CO2 (g) + Si(l) Quartzite Coke, Coal, Pebbles Wood chips MG-Si (metallurgical grade silicon) 10 The second step is: MG-Si(s) + 3HCl(g) SiHCl3 (g) + H2 (g) Condenser and multiple fractional distillations SeG-SiHCl3 (l) S Semiconductor-grade purity trichlorosilane And reaction with a hydrogen gas in a chamber containing silicon rod heated electrically to 1000-1200 °C results in deposition a fine grained poly crystalline form onto an electrically heated silicon rod. SeG-SiHCl3 (g) + H2 (g) 3HCl(g) + SeG-Si(s) Polycrystalline SemiconductorGrade Silicon [7] The net result from Siemens process to produce poly-crystalline semiconductor-grade silicon with purity is 99.9999%. Characteristics: Requirement a lot of energy. Low yield ~37% The high cost of this steps. 11 2.3 Conversion of Semiconductor-grade silicon to single-crystal silicon wafers To make silicon in a single-crystal state, one must first melt high-purity silicon this then cause it to reform or solidify very slowly in contact with a single crystal "seed". The silicon adapts to the pattern of the single-crystal seed as it cools and gradually solidifies, not surprisingly, because one starts from a seed say that this process is growing a new rod (often called boule) of a single crystal. Several different processes can be used to grow a boule of single crystal silicon, the most established and dependable process is the czocharalski processes (CZ method). 2.3.1 Czocharalski process The czocharalski process is a technique for growing crystal in order to obtain solitary crystals of semiconductor like silicon, metal like silver and gold as well as several salts. This process is named after Jan czocharalski who first demonstrate it in 1916; he was studying the rate of crystallization of different material. The most significant applications of the czocharalski process are the growing of large use ingots of single crystal silicon [8]. 2.3.2 Czocharalski procedure High-purity, semiconductor-grade silicon is melted down in a crucible. Dopant impurities atom such as a boron can be added to the molten intrinsic silicon in precise a mount in order to dope the silicon, thus 12 changing it into p-type extrinsic silicon, this influence the electrical conductivity of the silicon. A seed crystal mounted on a rod is dipped into the molten silicon, the seed crystal rods is pulled upwards and rotates at the same time[9] as shown in the figure below: Figure 5: CZ process By precisely controlled the temperature gradient, rate of pulling and speed of rotation, its possible to extract a large single crystal cylindrical ingot from the melt, this process is normally performed in an inert atmosphere such as argon and an inert chamber such as quartz crucible. 2.3.2.1 Crucible A crucible is a cup-shaped piece of laboratory equipment used to contain chemical compound when heated them to very high temperature, the receptacle is usual made of porcelain, the crucible used in CZ molten shown below: Figure 6: crucible use in CZ process before use. 13 These crucibles are very durable and resist temperatures to over 1600 °C. A crucible is placed into a furnace and, after the melting, the liquid metal is taken out of the furnace and poured into the mold [10], Figure 7: crucible during annealing And the other case: Figure 8: A crucible after used 14 2.3.3 Silicon wafers The solidification the silicon ingots as shown in figure: Figure 9: single crystal ingot Silicon wafers are obtained from large silicon ingots by slicing and polishing to achieve a high degree of flatness. These chips, normally about 0.75 mm in thickness are thus used for the manufacture of integrated circuits. The ingots from which they are cut may range from anywhere between 1 and 2 metres in length with diameters up to 400 mm [11]. 15 Figure 10: silicon wafer a) after cutting b) after bolishing Finally, the cylindrical ingot is cut with saws (wire or diamond saws) into round waferes about 250 μm thick. Characteristics: The present wafering technology it's difficult to cut wafers from the large crystals which are any thinner than 300μm and still retain reasonable yields. More than half the silicon is wasted as kerfs or cutting loss in the process The low overall yields of single-crystal. 16 3. Processing of single crystal wafers to solar cells Wafers are clean with industrial soap and then etched using hot sodium hydroxide to remove saw damage. 3.1 Doping The objective is to create planer region having different concentration of impurities so as to form a p-n junction, thus in n-on p silicon cells. One may start with a p-type wafers containing boron as its chief impurity, and produce a very thin n-type layer near its surface by introducing phosphorous impurity into the wafers. Impurity may be added intentionally to a molten semiconductor before solidification. The traditional method of forming a layer of different conductivity on the surface of such of a wafer has been thermal diffusion of dopant atoms present in a gaseous molecule in a high temperature furnace in which the carefully cleaned wafers. Usually two-steps diffusion process is employed, in the predepostion step the desired impurity, transport by carriers gas to the hot semiconductor surface, and is diffused to a depth of a few tenths of a micron. To dope Si with P, one may bubble nitrogen gas through liquid POCl3 into a furnace held at from 800 to 1100°C for anywhere from minutes to an hour or so. Alternatively, a solid oxide such as P2O5 might be heated for producing gaseous P2O5 which will react at the hot Si surface to form P and solid SiO2. In drive-in step, the semiconductor is simply heated and the predeposited dopant atoms diffuse into the semiconductor to a 17 greater depth, up to about 1μm as and formation oxide layer on the surface shown in the Figure below [12]: a) Figure 11:phosphourus diffusion process: a) Schematic b) Real In asubsequence processing the oxide layer is removed as are the junction at the side and back of the cell to give the structure below: 18 Figure 12: distribution of phosphorus impurities: a) Immediately after diffusion process. b) After etching of back and side of wafers [13]. 3.2 Contact wafers with metal In a p-n junction solar cells ohmic contact are typically made with a uniform metallic electrode over the back surface and fingerlike front electrode. They should be highly conducting and should bond well by soldering to contact wires or conducting supports. So the contacts contain three separate layers of metal: 1. Titanium 2. Silver, Al or copper. 3. Palladium. A thin layer of titanium is used as the button layer for good adherence to silicon; the top layer is silver for low resistance and solder ability, sandwiches between these two is layer of palladium which prevent an undesirable reaction between Ti and Ag layer in the presence of moisture. 19 Figure 13: Solar wafer with metal contact [14]. Metal contacts are then attached to both the n-type and the ptype region. In the standard technology, the process used is known as vacuum evaporation. The metal to be deposited is heated in a vacuum to a high-enough temperature to cause it to melt and vaporize. It will then condense on any cooler part of the vacuum system in direct line of sight, including the solar cells. The back contact is normally deposited over the entire back surface, while the top contact is required in the form of a grid two techniques are available for defining such pattern, one is to use a metal shadow mask shown in Figure 14. Alternatively, the metal can be deposited over the entire front surface of the cell and subsequently etched a way from unwanted region using a photographic technique known as photolithography. 20 Figure 14: a metal shadow mask [15]. 3.3 Antireflection coating The one type of the losses in solar cells of an optical nature that bare silicon is quite reflective. The antireflection losses to about 10%. Antireflection coating consisting of layers indices of refraction between that of the semiconductor and air, the simplest AR is a single layer whose thickness is one-quarter wavelength of light in the coating and whose index of refraction nc is the geometrical mean of the indices of the two media containing it so nc =1.84 for silicon. 21 Figure 15: Major feature of solar cell But no material having exactly this index is known, some oxide and fluorides approximating it do exist see table below: Table 2: Indices of refraction of material [16]. Material Al2O3 Glasses MgO SiO SiO2 Ta2O5 TiO2 Index of refraction 1.77 1.5-1.7 1.74 1.5-1.6 1.46 2.2 2.5-2.6 90% of light is transmitted through 600Å coating of Ta2O5 on silicon. Antireflection coating are applied primarily by vacuum evaporation is deposited on the top of the cell. 22 The AR material to be deposited is heated in a vacuum to a high – enough temperature to cause it to melt and vaporize if will condense on cell cooler parts of vacuum system in direct line of sight. Characteristics: • Yield of about 90% from starting wafers to completed terrestrial cells can be obtained • This make the processing very labor-intensive • The vacuum evaporation equipment is expensive compared to its throughput • the material expensive such Ag. 3.4 Texturing surface The other technique to reduce reflection from the surface is texturing. To minimize reflection from the flat surface solar cell wafers are textured, this means a creating a roughened surface, so that incident light will have a larger probability of being absorbed into the solar cell. This is performed by etching in a week alkaline solution such as Hf. 23 Figure 16: texturing surfaces silicon by SEM [17]. The textured surface results when a single –crystal semiconductor is treated with an orientation –dependent etch that attack some crystal planes faster than it does other. For etching a Si wafers whose normal orientation is in the (100) or equivalent direction in heated (90 to 95°C) hydrazine (36 percent N2H4) produces small pyramid whose faces are (111) planes shown in figure 16. Light incident on these pyramids is partially transmitted and partially reflected at each contact with their surface as the light bounces its way down toward the bottom of the pyramids. As with a properly designed AR coating, the surface of a textured cell appear dark when viewed in white light. 24 4. solar cell to solar module After the three steps to obtain solar wafers prepared to contact together to formation a solar module by metal wire with high conductivity to accumulate the electric current from every cell. After interconnecting between cells solar cells require encapsulation by glass to: 1. Mechanical protection 2. Electrical isolation 3. Chemical protection 4. Mechanical rigidity to support the prattle cells and their flexible interconnection Figure 17: Tracked PV Array containing 16 panels [18]. The most common material for the structural back has been anodized Aluminum, porcelainized steel, epoxy board or window glass. The structural front configuration glass is the obvious choice for the structural layer, it combine excellent weather ability with low cost and good self- cleaning properties. So we will connect many cells to make module and connect more than two modules to make panel and the many panel to make array show below: 25 Figure 18: Photovoltaic cells, modules, panels and arrays. 26 5. Discussion and result The result show that dedicated process of solar cell module from the sand in nature to solar cell system can produce a new a renewable energy sources. And open wide field to improvement the fabrication solar cell by modern technique to reduction the time and the money. 27 REFERENCES: [1] a.müller, M.Ghosh, R.Sonneushein, P.Woditsch, Material science and Engineering B 134,257-262,(2006). [2]Department of Energy, Renewable energy annual,Vol 1,Chapter 2, Table 28, 1997. [3] http://WWW.SILICON.COM [4] J.Gee, J.Van Den Avyle, J.slepanek, B.L.Sopori, 520552,(1998). [5] T.Wang, F.Ciszek, Journal. Crystal Growth 174, 176,(1997). [6] http://en.Wikipedia.org/Wiki/Electric arc furnace [7] C.Hu, R.M.White, Solar Cell from basic to advance system, First Edition,MC Grow Hill, (1983). [8] http://en .Wiki/Czocharalski process [9]http://WWW.article world.org/index.php/czocharalski process [10] http://WWW.en.Wikipedia.org/Wiki/Crucible [11] http://WWW.article world.org/index.php/Monokrristallines_Silizium [12] M.Green, Solar Cell operation principal Technology and system Application, Prentice-Hall.Inc,firstedition,(1982). [13] http://WWW. Solar Photovoltic Cells.com [14] M.Green, Solar Cell operation principal Technology and system Application, Prentice-Hall.Inc,firstedition,(1982). [15] H.Möller,Semiconductor for Solar Cells,Artech House,first edition,(1993). [16] http://WWW. IMEC/Crystal Growth, Crystalline Si Solar Cells.htm [17] Bp Solar web page "An Introduce to BpSolar in Australia" (online),http://WWW.bp.com.au/Solar/Default.asp Accessed on 16 Feb 2007. [18] http://WWW.Wikipedia.org/Wiki/panel 28