The present invention relates to a process for making photovoltaic modules or solar cells.
Problem
As oil prices have continued to increase and other energy sources remain limited, there is increasing pressure on global warming from the emissions of burning fossil fuel. There is a need to find and use alternative energy sources, such as solar energy because it is free and does not generate carbon dioxide gas. To that end, many nations are increasing their investment in safe and reliable long-term sources of power, particularly “green” or “clean” energy sources. Nonetheless, while the solar cell, also known as a photovoltaic cell or modules, has been developed for many years, it had very limited usage because the cost of manufacturing these cells or modules is still high, making it difficult to compete with energy generated by fossil fuel.
Presently, the single crystal silicon solar cell has the best energy conversion efficiency, but it also has the highest manufacture cost. Alternatively, thin-film silicon while it does not have the same high efficiency of a single crystal cell, it is much cheaper to produce. Therefore, it has the potential for low cost photovoltaic power generation. Other types of thin-film materials such as copper indium gallium diselenide (“CIGS”) also showed promising results with efficiencies approaching the single crystal silicon, at a lower cost, but still not low enough to compete effectively with fossil fuel.
Part of the reason for the manufacturing expense is that the deposition rates of these processes are low and time consuming. For example, the typical process of plasma glow discharge of silane in the presence of a high concentration of hydrogen gas to form the desired silicon layer achieves a deposition rate of approximately 20 A/s or 0.12 microns/minute. For another example, the typical plasma chemical vapor deposition (“CVD”) method for forming high quality i-type silicon layer achieves a reported deposition rate of approximately 15 A/s or 0.09 microns/minute. In yet another example, the typical chemical vapor transport (“CVT”) method, which uses iodine vapor as a transport medium to deposit polycrystalline silicon, achieved film growth rates up to approximately 3 microns/minute.
Similar to silicon solar cell technologies, efforts have been made to manufacture CIGS type solar cells using different techniques. In one attempt, CIGS type solar cells are manufactured in a two-stage process using various precursor structures, which is known as a the selenization technology. Attempts have been made to improve on the selenization technology. In one such attempt, a two-stage process using the magnetron sputtering technique with a conveyor system to make a thin film is known. In another attempt, a vapor-phase recrystallization process is used to make CIGS films. The recrystallization process was used as the second step of the process and it replaced the selenization process as taught by previous arts. In yet another attempt, CIGS film was manufactured using an electrochemical deposition in a solution that was followed by physical vapor deposition. This technology produced a CIGS type solar cell with an overall conversion efficiency of 13.6%.
In addition to the efforts to efficiently manufacture the types of solar cells mentioned above, additional efforts have been expended to efficiently manufacture other types of solar cells, such as multi-junction solar cells. These types of solar cells have the construction of multiple layers with different materials. The different materials have different bandgaps and they will absorb various wavelengths of the solar energy. Thus, these types of solar cells cover a broader solar spectrum and may improve the efficiency of the solar cell. Some efforts have been expended to efficiently produce these types of solar cells. In one such effort, multi-junction solar cells are manufactured with amorphous silicon and copper indium diselenide (“CIS”) and their alloys. However, this manufacturing process is very complicated and needs different kinds of equipment, thus making it expensive to produce these types of solar cells. Some examples for producing layers of CIS or CIGS include depositing these layers by way of solution growth, sputtering, or evaporation. Also, layers of silicon are deposited by way of enhanced plasma chemical vapor deposition.
As mentioned above, to make thin film solar cells requires a deposition technique to deposit the required layers, and the most effective way to lower the manufacturing cost is to increase the deposition rate. The best reported deposition rate for Plasma-Enhanced Chemical Vapor Deposition (“PECVD”) is about 5 A/sec, and the deposition rate for plasma glow-discharge of silane is 20 A/sec.
Furthermore, in addition to slow deposition rates, another slow process step found commonly in the manufacture of solar cells involves the incorporation of p-type and n-type dopants to form the p-n junction of the semiconductor material. This step is normally done in extremely slow diffusion furnaces after the thin-film layer has already been deposited, thus further slowing down the overall process of efficiently producing solar cells.
In addition, with regard to the process of making CIGS thin films, the process usually uses two or more stages. The purpose for the additional steps of the process is to deposit or adjust these elements to achieve the desired or optimum composition ratios and phase structure of the CIGS thin films. In the first step, various techniques have been used for build-up the required thickness of film with the concentration ratios being relatively close to the designed value. The combination of these steps inhibits an efficient manufacturing process for making CIGS thin films.
Information relevant to attempts to address these problems can be found in the U.S. Pat. Nos. 5,646,050 issued 8 Jul. 1997 to Li, et al.; 5,942,049 issued 24 Aug. 1999 to Li, et al.; 6,100,466 issued 8 Aug. 2000 to Nishimoto; 6,214,706 issued 10 Apr. 2001 to Madan, et al.; 6,281,098 issued 28 Aug. 2001 to Wang, et al.; 5,141,564 issued 25 Aug. 1992 to Chen, et al.; 4,798,660 issued 17 Jan. 1989 to Ermer, et al.; 4,915,745 issued 10 Apr. 1990 to Pollock, et al.: 6,048,442 issued 11 Apr. 2000 to Kushiya, et al.; 6,258,620 issued 10 Jul. 2001 to Morel, et al.; 6,518,086 issued 11 Feb. 2003 to Beck, et al.; 5,045,409 issued 3 Sep. 1991 to Eberspacker, et al.; 5,356,839 issued 18 Oct. 1994 to Tuttle, et al.; 5,441,897 issued 15 Aug. 1995 to Noufi, et al.; 5,436,204 issued 25 Jul. 1995 to Albin, et al.; 5,730,852 issued 24 Mar. 1998 to Bhattacharya, et al.; 5,804,054 issued 8 Sep. 1998 to Bhattacharya, et al.; 5,871,630 issued 16 Feb. 1999 to Bhattacharya, et al.; 5,976,614 issued 2 Nov. 1999 to Bhattacharya, et al.; 6,121,541 issued 19 Sep. 2000 to Arya; and 6,368,892 issued 9 Apr. 2002 to Arya.
Solution
The above-described problems are solved and a technical advance achieved by the plasma deposition apparatus and method for making solar cells disclosed in this application. The novel process uses an induction coupled plasma torch to make the thin film solar cells. It has a higher deposition rate, and it can be designed as a continuous flow process such that it can dramatically lower the manufacturing cost of the thin film. By using a conveyer system for a continuous in-line process, this process can deposit the required thin film on a substrate such as glass, flexible metal, or high temperature polymer materials.
The novel induction coupled plasma deposition process provides a measurably higher deposition rate, leading to a much lower manufacturing cost. Another major aspect of the novel plasma deposition apparatus and method for making solar cells is to simultaneously incorporate such positive and/or negative dopanting material during the thin-film deposition, thus eliminating another very slow and costly process in the manufacturing steps.
One advantage of the induction coupled plasma torch is its very high deposition rate (“DR”). For additional efficiency and manufacturing cost savings, one or more induction coupled plasma torches can be grouped together to provide a set of induction coupled plasma torches to form the deposition module integrated with a conveyer system. It is an easy, yet versatile production system with high deposition and throughput rates.
In addition, the novel plasma deposition apparatus and method for making solar cells can easily inject the desired materials to the right deposition module and deposit the designed layer on one conveyer system as the substrate moves from one deposition module or deposition chamber onto another deposition module or deposition chamber. Alternatively, the novel plasma deposition apparatus and method for making solar cells provides for the solar cell to enter and reenter the same deposition modules as different chemicals are introduced in each cycle.
Further, when doping the thin-film by this novel plasma deposition apparatus and method for making solar cells, the direct control of the dopants distribution and a better concentration profile than the typical diffusion process is achieved. The apparatus and method can also greatly influence energy conservation efficiency and chemical and physical properties. Moreover, using a deposition process instead of diffusion process to make p-type or n-type doped thin films, not only provides better control and more uniform dopants distribution, but it also eliminates the two-step process, yielding a higher production rate.
Also, the novel plasma deposition apparatus and method for making solar cells meets the challenges of producing high quality solar cell that includes optimizing the quality i-type layer. The doped p- and n-type layers for low contact resistance, high build-in potential, and high transparency to reduce unnecessary optical losses and the present novel plasma deposition apparatus and method for making solar cells accommodates such requirements.
In one feature, the novel plasma deposition apparatus and method for making solar cells can use materials that contain the constitute elements of copper, indium, gallium, and selenium that are injected into the plasma flame to form a thin layer of CIGS. In another feature, the plasma deposition apparatus and method for making solar cells can use properly designed ratios of copper, indium, gallium, and selenium to inject into the plasma flame and form the GIGS thin film.
Conveyor 106 has a longitudinal axis that is defined as being aligned with the direction of the arrows shown in
Typically, the diameter and height or length of the outer quartz tube 108 and the inner quartz tube 110 may be any size to fit the desired application of the outer quartz tube 108 and inner quartz tube 110. Preferably, the inner quartz tube 108 has a shorter length than the outer quartz tube 108. Also, the outer quartz tube 108 preferably has a diameter in the range of from about 50 millimeters (“mm”) to about 90 mm and a height in the range of from 180 mm to about 400 mm. More preferably, the diameter for the outer quartz tube 108 is about 70 mm with a height or length of about 200 mm. Preferably, the inner quartz tube 110 has a diameter in the range of from about 50 mm to about 70 mm and a height in the range of from about 120 mm to about 180 mm. More preferably, the diameter of the inner quartz tube 110 is about 60 mm with a height of about 150 mm.
The induction coupled plasma torch 102 further includes a copper induction coil 114 that is located around the lower portion of the outer quartz tube 108. The coil 114 comprises a plurality of windings 116 having a diameter of approximately in the range of from about 56 mm to about 96 mm. Preferably, the plurality of windings 116 has a diameter of about 82 mm. Typically, the plurality of windings 116 are spaced apart from each other by a sufficient distance to provide for operation of the induction coupled plasma torch 102. Preferably, the plurality of windings 116 are spaced apart from each other by about 6 mm. In addition, a gap between the outer quartz tube 108 and the coil 114 can be in a range of from about 2 mm to about 10 mm. Also, the distance between the lowermost portion of the coil 114 and the substrate 104, is designated by “L,” which is in the range of from about 30 mm to about 55 mm.
The induction coupled plasma torch 102 further includes a pair of injection ports 118 that are connected to a precursor source chemical line (not shown) carrying the precursor source chemicals to the induction coupled plasma torch 102. With the use of the inner quartz tube 110, the plasma forming gas will have a swirl flow pattern. The source chemicals for deposition of semiconductor thin film material such as silicon will be injected through the injection ports 118, which are preferably located near the lower side of the induction coupled plasma torch 102 and aimed toward the V=0 position for the same reason as disclosed in U.S. Pat. No. 6,253,580 issued to Gouskov et al. and U.S. Pat. No. 6,536,240 issued to Gouskov et al, both of which are incorporated herein by reference. In one embodiment, the injection ports 118 are connected to the induction coupled plasma torch 102. In another embodiment, the injection ports 118 are not connected to the induction coupled plasma torch, but are connected to another structural element of the present invention as herein described. In one embodiment, the induction coupled plasma torch 102 is an inductively coupled plasma torch. The injection ports 118 comprise quartz tubing preferably having a diameter in the range of from about 3 mm to about 10 mm, more preferably of about 5 mm, although tubing diameters in other sizes may be used with the induction coupled plasma torch 102. In this embodiment, a pair of injection ports 118 is positioned diametrically across from each other. In another embodiment of the present invention, three or more ports, symmetrically arranged, may be utilized.
Further, induction coupled plasma torch 102 includes a pair of plasma gas inlets 120 that are connected to a plasma gas supply line (not shown) carrying plasma gases to the induction coupled plasma torch 102. The plasma gas inlets 120 enter the induction coupled plasma torch 102 at substantially the same height. Preferably, these plasma gas inlets 120 comprise stainless steel tubing having a diameter of 5 mm, although a range of diameters may suffice for this purpose.
The induction coupled plasma torch 102 is also provided with a coolant inlet 122 and coolant outlet 124. During use, a coolant, such as water, passes through the coolant inlet 122, circulates within the stainless steel chamber 112, and exits through the coolant outlet 124. The coolant inlet 122 and coolant outlet 124 are preferably formed from stainless steel and have a diameter of 5 mm, for example.
The plasma gas inlets 120, the coolant inlet 122 and the coolant outlet 124 are all preferably formed in a stainless steel chamber 112. The chamber 112 is preferably a stainless steel square block 80 mm on a side, and having a height of approximately 40 mm, for example. The chamber 112 is mounted onto the support stand (not shown).
A high frequency generator (not shown) is electrically connected to the coil 114, powering it with a variable power output up to 60 kW at a frequency of 5.28+/−0.13 MHz. In an embodiment, the generator is Model No. IG 60/5000, available from Fritz Huettinger Electronic GmbH of Germany. This generator is driven with a 50 Hz, 3-phase, 380 V power supply to energize the induction coupled plasma torch 102.
In order to cover a wider deposition width, a group of induction coupled plasma torches 102 are placed together to form a deposition module 200.
In one embodiment, the induction coupled plasma torches 102 comprise one row. In another embodiment, the induction coupled plasma torches 102 comprises two or more rows and are positioned in a staggered arrangement as shown in
Deposition modules 200 may be spaced a distance apart as shown further in
The deposition chamber 302 further includes an exhaust system 312 having exhaust ports (not shown) for removing by-product gases, flumes, and particles from the deposition chamber 302. The exhaust system 312 controls the partial pressure within the deposition chamber 302 to ensure optimal deposition conditions. The control of the partial pressure within the deposition chamber 300 may further include providing a negative pressure, such as a vacuum. In another embodiment, the partial pressure may be controlled at or near atmospheric pressure. Any number of exhaust ports may be employed as desired for a specific application. Preferably, the deposition chamber 302 is made of explosive proof materials and also RF shield material to protect the workers.
Referring to
In one embodiment, a deposition module may include one row of induction coupled plasma torches 102. In another embodiment, a deposition module may include several rows of induction coupled plasma torches 102. Deposition modules 400 and 500 include two rows of induction coupled plasma torches 102 that are positioned in a staggered arrangement as shown in
In deposition module 400 as shown in
Similarly, in deposition module 500 shown in
To provide for uniform deposition coverage of a substrate 104, deposition modules 400 and 500 oscillate in a direction 408 that is substantially transverse to the longitudinal direction of movement 314 of the conveyor 106. Thus, the induction coupled plasma torches 102 of deposition modules 400 and 500 are oscillated back and forth across the substrate 104 as it is supported and moved along the longitudinal direction of movement 314 of the conveyor 106. In one aspect, the deposition modules 400 and 500 remain a fixed distance from the substrate 104 during its oscillating motion. In another aspect, the distance between the modules 400 and 500 and the substrate 104 may be variable. This oscillating deposition coverage enables fewer induction coupled plasma torches 102 to be used during a deposition operation. By utilizing fewer induction coupled plasma torches 102, the induction coupled plasma torches 102 may be spaced apart from each other at greater distances when compared to the spacing of the induction coupled plasma torches 102 of deposition module 200.
The oscillating or reciprocating motion is set to provide the optimal deposition of reaction product on a substrate 104. This oscillating or reciprocating motion has an amplitude and a speed that is variable or fixed to provide the desired deposition results. The amplitude of the oscillating motion of the deposition modules 400 and 500 is generally defined as the distance it oscillates or reciprocates from side to side in the transverse direction 408 relative to the conveyor 106 or substrate 104. Preferably, deposition module 400 will oscillate or reciprocate with an amplitude equal to the distance 402 or 404 depending on which one is larger. Regarding deposition module 500, it will oscillate or reciprocate with an amplitude equal to the distance 502. These are exemplary amplitudes and other amplitudes may be used to achieve a desired deposition result.
Further, deposition modules 400 and 500 will oscillate or reciprocate at a desired frequency. The frequency is typically defined as the number of times the deposition modules 400 and 500 oscillate back and forth across a substrate 104 or conveyor 106 in a given time. In addition, due to the oscillating or reciprocating motion, deposition modules 400 and 500 will travel back and forth across a substrate 104 or conveyor 106 at a desired speed.
Further, the speed and frequency of the oscillating motion may be further determined by the speed of the conveyor 106. For example, if the speed of the conveyor 106 is slower, then the speed and frequency of the oscillating motion may also be slower. Conversely, if the speed of the conveyor 106 is fast, then the speed and frequency of the oscillating motion may also be faster. Moreover, if the speed of the conveyor 106 is varied while the speed and frequency of the oscillating motion remains fixed, then different thicknesses of the reaction product will be achieved on the substrate 104. Also, if fewer induction coupled plasma torches 102 are employed on a particular deposition module, then its amplitude of the transverse direction 408 may be greater. Conversely, if more induction coupled plasma torches 102 are employed on a particular deposition module, then its amplitude of the transverse direction 408 may be less.
Combined, these characteristics of the oscillating motion along the transverse direction 408 provide a desirable deposition result of a reaction product on a substrate 104. These characteristics are set or adjusted prior or during the deposition process to achieve the desired deposition results. For example, deposition module 400 includes fewer induction coupled plasma torches 102 than deposition module 500, thus the spacing of the distances 502 and 504 may be greater than the distances 402, 404, 406 of deposition module 400. Because of these greater distances and fewer induction coupled plasma torches 102, the oscillating motion of deposition module 500 may have a greater speed and frequency than deposition module 400. All of these characteristics of the oscillating motion may be optimized for a particular application to provide an optimal deposition thickness of a reaction product on a particular substrate 104. Typically, the amplitude equals the distance that the deposition modules 400 and 500 travel as herein described, and the frequency time equals the time for a complete oscillation cycle. Thus, an oscillation speed may be calculated by dividing the amplitude by the frequency time.
The distances 402, 404, and 406 may be the same or different depending on several factors, including desired deposition rate and coverage, deposition thickness, uniformity of deposition, speed of the conveyor 106, number of induction coupled plasma torches 102 used, orientation of the induction coupled plasma torches 102, and the like. Likewise, the distances 502 and 504 may be the same or different depending on these factors.
Deposition modules 400 and 500 may be spaced a distance apart similarly to deposition modules 200 as shown in
In yet another embodiment of the present invention the rows of each deposition module may oscillate or reciprocate relative to each other. For example, referring to
Likewise, referring to
In yet another embodiment of the present invention, one induction coupled plasma torch 102 may be oscillated like that described above. In this embodiment, the conveyor 106 will move in a step-wise motion and not a continuous motion. For example, the conveyor 106 will move the substrate 104 a distance relative to the deposition module and then the deposition module would oscillate or reciprocate across the substrate 104 beginning on one side and traversing to the other side of the substrate 104. Then the conveyor 106 would move the substrate 104 another distance and stop for another traverse of the substrate surface by the deposition module. The distance of each step is dependent upon the diameter of the induction coupled plasma torch 102. In another aspect of the present invention, a single or plurality of induction coupled plasma torches 102 may make several oscillations or reciprocations across a substrate 104 while depositing a particular reaction product on each pass while the conveyor is moving continuously or step-wise.
The reaction product is produced by the reaction of the precursor gas sources in the presence of the induction coupled plasma torch 102. The induction coupled plasma torch 102 preferably uses an inert plasma source gas to form the plasma where the reaction takes place between the precursor gas source and the induction coupled plasma torch 102 for depositing the reaction product on the substrate 104. Some exemplary plasma source gases include silane, hydrogen, methane, diborane, trimethylborone, phosphine, and mixtures thereof. The precursor gas source may include or be additional forms of matter such as gases, vapors, aerosols, small particles, or powders. For example, it is possible to deposit thin film of a few microns in thickness by oscillating or reciprocating the induction coupled plasma torches 102 to cover a width of 1 meter or wider and continuing to move the conveyor to achieve any desired deposition length.
The reaction product is preferably a single element, compound, or mixture of elements or compounds and includes elements and compounds as copper, indium, gallium, selenium, silicon, intrinsic I-type layers, p-type doped silicon layers, and n-type doped silicon. In one embodiment, the reaction product is a copper indium gallium diselenide (“CIGS”) layer that is found in solar cells.
The typical solar cell will have p-i-n or n-i-p layer structures. Further, an individual layer for the silicon solar cell can be formed with the following chemicals.
For intrinsic silicon (i-type layer), silane (SiH4) is the most common material used for these silicon layers. In addition, hydrogen (H2) gas is also added to the gas stream for making the desired Si: H i-type layer. For p-type doped silicon, either a SiH4, CH4, and B2H6 gas mixture or a SiH4, H2, and Trimethylboron B(CH3)3 gas mixture may be used, for example. For n-type doped silicon, either a SiH4 and PH3 gas mixture or a SiH4, H2, and PH3 gas mixture may be used, for example.
The substrate 104 may be any desired size including those sizes commonly known in the art of solar cells. Preferably, the substrate is made from a tin oxide coated glass, such as from Asahi or a molybdenum coated glass, such as Corning 1737, for example.
In addition to the aforementioned aspects and embodiments of the present plasma deposition apparatus, the present invention further includes methods for manufacturing these solar cells.
In step 608, the induction coupled plasma torch 102 is initiated. This step can include initiating the flow of the plasma gas supply to the plasma gas inlets 120 and then plasma ignition by supplying electricity to the induction coil 114. In addition, step 608 may also include selecting the precursor gas source to be used to produce the desired reaction product during deposition on the substrate 104 or plurality of substrates 104. Step 608 may also include initiating all the other induction coupled plasma torches 102 if a plurality of them are used such as in deposition modules 200.
In step 610, the induction coupled plasma torch 102 deposits the reaction product onto the substrate 104. In step 612, an inquiry is made as to whether another layer of a reaction product is to be deposited by the induction coupled plasma torch 102. If the response in step 612 is “no,” then the process terminates. If the response to this inquiry is “yes,” then another inquiry is made in step 613. If the response to the inquiry in step 613 is “no,” then the process proceeds to step 616 where the distance between the induction coupled plasma torch 102 and the substrate 104 can be adjusted prior to depositing another thin film layer of reaction product. Preferably, this step is then followed by a return to step 610. As described above, step 610 may include uniformly depositing the thin film reaction product layer with one or more induction coupled plasma torches 102 concurrently. If the response to the inquiry in step 613 is “yes,” then in step 614, the conveyor 106 moves the substrate 104 or plurality of substrates 104 along to the next induction coupled plasma torch 102 or plurality of induction coupled plasma torches 102 of deposition module 200 and the next layer of reaction product is deposited on the substrate 104 or plurality of substrates 104. Preferably, the process then proceeds back to step 612 where another inquiry is made regarding whether another layer of reaction product is to be deposited onto the substrate 104 or plurality of substrates 104. This process is repeated until the desired number and types and thicknesses of reaction products have been deposited onto the substrate 104 or plurality of substrates 104.
In step 708, the induction coupled plasma torch 102 or plurality of induction coupled plasma torches 102 are initiated. This step can include initiating the flow of the plasma gas supply to the plasma gas inlets 120 and then plasma ignition by supplying electricity to the induction coil 114. In addition, step 708 may also include selecting the precursor gas source to be used to produce the desired reaction product during deposition on the substrate 104 or plurality of substrates 104.
In step 710, the precursor gas source is injected into the induction coupled plasma torch 102 or plurality of induction coupled plasma torches 102. In one embodiment, the flow of the precursor gas source may be set or optimized by measuring off-line the thicknesses, composition, and/or performance of substrates 104 that have already been deposited with a reaction product layer. If the thicknesses, composition, and/or performance is not within design standards, then the precursor gas source and/or the flow rate of the precursor gas source can be adjusted accordingly. In step 712, the plasma flame of the induction coupled plasma torch 102 or plurality of induction coupled plasma torches 102 is stabilized.
In step 714, an inquiry is made as to whether additional induction coupled plasma torch 102 or plurality of induction coupled plasma torches 102 are to be initiated and stabilized. If so, then the process preferably returns to step 708 to initiate the induction coupled plasma torch 102 or plurality of induction coupled plasma torches 102 or deposition modules 200. If the answer to the inquiry in step 714 is “no,” then another inquiry is made in step 716. In this inquiry, additional deposition modules 200 may be initiated and stabilized. If the answer to this inquiry is “no,” then the process preferably proceeds to step 718 where the substrates 104 are loaded onto the conveyor 106. This is followed by step 720, where the distance between the induction coupled plasma torch 102 or plurality of induction coupled plasma torches 102 and the substrates 104 may be adjusted.
In step 722, the induction coupled plasma torch 102 or plurality of induction coupled plasma torches 102 of the deposition modules 200 deposit the reaction product onto the substrate 104. In step 724, an inquiry is made as to whether another layer of a reaction product is to be deposited by the induction coupled plasma torch 102 or plurality of induction coupled plasma torches 102. If the response in step 724 is “no,” then the process preferably terminates. If the response in step 724 is “yes,” then another inquiry is made in step 726. In step 726, an inquiry is made as to whether a different thin film layer of reaction product is to be deposited on substrate 104. If the response to this inquiry is “no,” then preferably the process returns to step 720 to adjust distance between the induction coupled plasma torch 102 or plurality of induction coupled plasma torches 102 and the substrate 104 or plurality of substrates 104, followed by deposition of another reaction product layer in step 722. If the response to the inquiry in step 726 is “yes,” then in step 728 the conveyor 106 preferably moves the substrate 104 or plurality of substrates 104 along to the next induction coupled plasma torch 102 or plurality of induction coupled plasma torches 102 or deposition module 200. Then in step 730, the induction coupled plasma torch 102 or plurality of induction coupled plasma torches 102 deposit or deposition module 200 deposits the next layer of reaction product on the substrate 104 or plurality of substrates 104.
In step 732, another inquiry is made as to whether another thin film layer of reaction product is to be deposited. If the response to this inquiry is “yes,” then the process preferably returns to step 726. If the response to this inquiry is “no,” then the process preferably terminates and the substrates 104 or plurality of substrates 104 are removed from the conveyor 106.
In another aspect of the present methods for manufacturing solar cells, the substrates 104 may be removed from the process at other times than described above to measure the thicknesses, compositions, and/or performance of the deposition process to determine whether to adjust any of the process parameters described above, such as conveyor temperature, deposition chamber pressure, composition of the precursor gas source, and/or the flow rate of the precursor gas source to one or more of the induction coupled plasma torch 102 or plurality of induction coupled plasma torches 102 or deposition modules 200.
In step 808, the induction coupled plasma torch 102 or plurality of induction coupled plasma torches 102 are initiated. This step can include initiating the flow of the plasma gas supply to the plasma gas inlets 120 and then plasma ignition by supplying electricity to the induction coil 114. In addition, step 808 may also include selecting the precursor gas source to be used to produce the desired reaction product during deposition on the substrate 104 or plurality of substrates 104.
In step 810, one or more of the deposition modules 400 and 500 are oscillated or reciprocated in a transverse to provide an amplitude, speed, and frequency sufficient to provide desired deposition coverage across the substrate 104 or plurality of substrates 104. In step 812, the precursor gas source is injected into the induction coupled plasma torch 102 or plurality of induction coupled plasma torches 102. In one embodiment, the flow of the precursor gas source may be set or optimized by measuring off-line the thicknesses, composition, and/or performance of substrates 104 that have already been deposited with a reaction product layer. If the thicknesses, composition, and/or performance is not within design standards, then the precursor gas source and/or the flow rate of the precursor gas source can be adjusted accordingly. The plasma flame of the induction coupled plasma torch 102 or plurality of induction coupled plasma torches 102 is stabilized.
In step 814, an inquiry is made as to whether another layer of a reaction product is to be deposited by the induction coupled plasma torch 102 or plurality of induction coupled plasma torches 102. If the response in step 814 is “no,” then the process preferably terminates. If the response in step 814 is “yes,” then another inquiry is made in step 815. In step 815, an inquiry is made as to whether a different thin film layer of reaction product is to be deposited on substrate 104. If the response to this inquiry is “no,” then preferably the process returns to step 818 to adjust distance between the induction coupled plasma torch 102 or plurality of induction coupled plasma torches 102 and the substrate 104 or plurality of substrates 104, followed by deposition of another reaction product layer in step 812. If the response to the inquiry in step 815 is “yes,” then in step 816 the conveyor 106 preferably moves the substrate 104 or plurality of substrates 104 along to the next induction coupled plasma torch 102 or plurality of induction coupled plasma torches 102 of deposition module 400 and 500. Then in steps 814, 815, 818, and 812 the induction coupled plasma torch 102 or plurality of induction coupled plasma torches 102 deposit or deposition module 400 and 500 deposits the next layer of reaction product on the substrate 104 or plurality of substrates 104.
In another aspect of the present methods for manufacturing solar cells, the substrates 104 may be removed from the process at other times than described above to measure the thicknesses, compositions, and/or performance of the deposition process to determine whether to adjust any of the process parameters described above, such as conveyor temperature, deposition chamber pressure, composition of the precursor gas source, and/or the flow rate of the precursor gas source to one or more of the induction coupled plasma torch 102 or plurality of induction coupled plasma torches 102 or deposition modules 400 and 500.
Although there has been described what is at present considered to be the preferred embodiments of the plasma deposition apparatus and methods for making solar cells, it will be understood that the present plasma deposition apparatus can be embodied in other specific forms without departing from the spirit or essential characteristics thereof. For example, additional plasma torches or different combinations of deposition modules, other than those described herein could be used without departing from the spirit or essential characteristics of the present plasma deposition apparatus and methods for making solar cells. The present embodiments are, therefore, to be considered in all aspects as illustrative and not restrictive. The scope of the invention is indicated by the appended claims rather than the foregoing description.
This application claims the benefit of U.S. Provisional Application No. 60/791,883, filed 14 Apr. 2006 and U.S. Provisional Application No. 60/815,575, filed 22 Jun. 2006. The entireties of these applications are incorporated herein by reference.
Number | Date | Country | |
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60791883 | Apr 2006 | US | |
60815575 | Jun 2006 | US |