Patent Application
20160111586
The invention relates to apparatus and methods for processing solar cell wafers, and more particularly to systems for reduction of Light Induced Degradation, herein “LID”, either before or after metallization firing, by use of High-Intensity full-spectrum Light Radiation of heated wafer surface(s), herein “HILR”, to which Boron or a Boron-containing compound or component has been applied (also known as passivating Boron applied to at least one surface of a wafer). The HILR treatment of the wafer surface may be done in a High-Intensity Light Zone, herein HILZ”, in ambient atmosphere, or preferably in a controlled atmosphere, such as a forming gas comprising from 2-90% H2 in a Nitrogen carrier gas, in either bulk (batch) processing, or in a continuous processing line. The HILR/heat treatment is effected in the HILZ at temperatures in the range of from about 100° C. to about 300° C. The HILR is applied via an Enhanced Light Source (herein “ELS”), such as a Light Emitting Plasma (LEP) or Xenon lamp source, preferably housed in a module containing at least one ELS and producing, at the wafer surface from 3-10 Sols (Suns) of full-spectrum radiation (visible, IR and UV), and may be continuous or intermittent. One or more ELS modules may be used in separate locations in a processing line system, or may be disposed adjacent each other as a series of ELS modules arrayed in a continuous zone, the HILZ, in the processing line apparatus system. The HILR/heat treatment HILZ may be followed by a controlled temperature heating zone which serves to anneal the treated wafers before discharge for further production steps to aggregate them into solar panels.
Solar panels contain a plurality of solar cells comprising electrically connected solar wafers in an array which is then sealed between glass sheets. Current high efficiency solar panels have an initial output on the order of 20-22% cell efficiency (conversion of solar energy into electricity), but after about 2 weeks, drops off by over 10% into a typical range of 17-18%. However, the common solar panels made in the US have efficiencies that peak around 13% initially, and fall off well below that after being put into service use. This efficiency fall-off phenomena is called Light-Induced Degradation (LID). While the mechanism is not precisely known, research points to the correlation of Boron content to LID, it being postulated that Boron-Oxygen Complexes (BOCs) of uncertain empirical formula(s) are formed in the wafers upon exposure to sunlight. These complexes in the silicon are generally characterized as B5O2i as a result of post-production in-service-use exposure to light.
Among the highest initial solar cell conversion efficiencies are Boron doped MCz (Magnetic Czochralski) silicon wafers. Typically the Boron is doped into the silicon surface that later becomes the back contact surface as a result of coating (Printing) it with silver compound-containing paste which is then fired in a metallization furnace to form the silver back contact layer. However, the metallization does not prevent the LID of Boron after a few days to weeks of service, resulting in efficiency fall-off. To date there has been no process for preventing Boron-Oxygen complex LID of the solar cells, nor for their permanent regeneration back to original efficiency.
Amorphous silicon, α-Si, wafers experience LID on the order of 10-15% over their first 6-months of in-use service life. Crystalline silicon, c-Si, wafers experience LID on the order of 3-7%. In α-Si LID is also known as the Staebler-Wronski effect (SWE), which can stabilize at lower Solar Conversion Efficiency (SCE) levels after about 6-months of in-use service exposure to sunlight. In mono-crystalline silicon cells, the main cause of the LID effect is a recombination-active Boron-Oxygen complex. These complexes affect the carrier lifetime (rate at which the carriers recombine). The more B—O Complexes (BOCs) there are in the wafers, the faster the carriers recombine, reducing output. Experiments have been reported on exposure of solar cell wafers with light at 1 Sol intensity for several hours in an attempt to reduce LID effects. Such light exposure experiments have not been applied to industrial in-line wafer processing furnace systems. The results have not been satisfactory to date.
Accordingly, there is an unsolved need in the solar wafer processing field to produce wafers that do not exhibit efficiency degradation (LID), or exhibit a significant reduction of the amount or rate of LID, upon mounting as solar wafers as cells in solar panels that are put in service in the field. Further, any process that can reduce or prevent LID, or treat the wafer to regenerate it after metallization back to a stable initial efficiency state, must be solved in the context of being able to be retrofit into current wafer processing furnace apparatus, at production rates and yields that are economically feasible.
The invention comprises apparatus for, and method of, treatment of silicon solar cell wafers, by radiation treating during controlled heating, at least the Boron-treated side or surface of such wafers with High-intensity full-spectrum Light Radiation, herein “HILR”, in the range of 3-10 Sols (Suns) continuously or intermittently (strobed) in one or more High-Intensity Light Zones, herein “HILZ”, for a time sufficient to reduce or prevent the LID effect, and as either part of an integrated wafer processing furnace system (preferred), or as a stand-alone HILZ with its own conveyor that can serve a plurality of furnaces or processing lines feeding their output to it. The inventive HILZ apparatus may also be set up for bulk processing of a plurality of wafers disposed in a static array.
By way of non-limiting examples, the inventive apparatus and process may be applied to wafers of: amorphous silicon, α-Si; crystalline silicon, c-Si; mono-crystalline silicon, mono-Si; nano-crystal silicon, n-Si; polycrystalline silicon, multi-Si; and micromorph (tandem cell) wafers using amorphous silicon interspersed with micro-crystalline silicon, α-Si/μc-Si. However, one skilled in the art will recognize that the inventive apparatus and process may be employed with any type of solar cells that experience LID effects.
The term “full-spectrum” means visible spectrum light as well as IR and UV. Preferably the HILR/heating is carried out in the HILZ in the presence of a forming gas comprising from 2-90% H2 gas with the balance being an inert carrier gas such as Nitrogen. Whether the inventive HILR/heating process passivates one or more Boron-Oxygen complexes (BOCs) that may form in the silicon of the wafers, passivates other complex(es), prevents or reduces the formation of such complex(es), or renders such complex(es) more stable, e.g., by maintaining the complex static or preventing its conversion to another state, is not fully understood or determinative of the efficacy of the inventive process. Accordingly, reference herein to reduction or elimination of LID, deactivation or “freezing” of the BOC or other complex(es), passivation of Boron, or recovery or restoration of initial cell efficiency in whole or in part, is meant to cover any of the mechanisms by which the LID reduction effect of the inventive HILR/heating process may ultimately be determined to occur.
While we do not wish to be bound by theory, on a gross chemical approach, wafer silicon typically has a content of Oxygen present in the crystalline structure. Accordingly, one aspect of the inventive HILR/heating process may result in extracting or “getting” Oxygen atoms or ions that may be in the silicon substrate, or which are chemically bound or associated-with the Boron in a BOC as a result of Boron being doped into the silicon. Typically, Boron is coated on or doped into the surface of the wafer that will form the back contact layer surface of the wafer, while Phosphorous is coated on the top surface of the wafer, onto which a fine-line collector grid will be screen printed.
The inventive process and HILR/heating apparatus is integrated into an industrial solar cell wafer processing line, including apparatus for and methods of: 1) UV pre-treatment of wafers (optional); 2) P-compound dopant coating, e.g., Phosphoric Acid, on a wafer surface that will become the emitter surface, typically the top surface; 3) optionally, coating with a B-compound on the opposite surface of the wafer, typically the bottom surface; 4) diffusion firing the wafer (in the case of P coating) or co-diffusion firing (in the case of both P and B coating) in an IR diffusion furnace; 5) application of an Anti-Reflective Coating (ARC) to the P-emitter top surface of the wafer (such as a silicon nitride PECVD coating); 6) screen printing a fine-line silver paste onto the top side (P side) of the wafer to form the collector grid, and coating the back side of the wafer with aluminum paste for the back contact layer; 7) drying the printed pastes; 8) metallization firing of the wafer, in a multi-zone IR metallization furnace, to control-melt the top surface fine lines of silver paste through the ARC layer into the P-doped Si, and fully melting the Al paste coated on the bottom surface to form a continuous back-contact layer of the wafer, followed by rapid quenching of the wafers; 9) HILR/heating treatment of the wafers in an HILZ at 3-10 Sols in the range of from about 100° C. to about 300° C. for a period of from about 10 seconds to about 5 minutes (about 300 seconds), and more preferably in the range of from about 10 seconds to about 180 seconds, the dwell time (wafer transport time through the HILZ) being a function of the light intensity at the wafer surface in the range of from about 3 to about 10 Sols, the rate of conveyor travel, and the length of the ELS array in the HILZ; and 10) an optional tempering, heat treatment zone. Typically, the metallization furnace line includes, adjacent its input end, a burn-out zone in which the organic binders of the pastes are first “burned-off”, by being heated to convert the binders to volatile gas which is drawn off. With respect to UV pre-treater and Dopers modules, exemplary ones are shown in our U.S. Pat. No. 8,742,532.
It is particularly important for transport of the wafers through the line during metallization firing to have a short dwell time, on the order of 1-2 seconds, in the peak firing zone of the IR metallization furnace. During the time of transport through the peak firing zone, also known as “the dwell time”, the temperature peaks very rapidly to the preselected maximum temperature for the selected wafer/paste(s) composition. The wafers are immediately thereafter cooled rapidly in a quench zone, which is the zone next downstream of the peak zone. Again, while we do not wish to be bound by theory, we find that the short dwell time in the peak zone helps to prevent or reduce BOC formation.
It is preferable, but not absolutely necessary, that the wafers are fired in at least the IR peak firing zone of the metallization furnace in the presence of the forming gas described above. In this firing embodiment, it is convenient to use a metallization furnace employing an isolation IR lamp module, in which quartz window(s) separate(s) the processing zone, through which the wafers are transported, from the lamps. An exemplary furnace employing one or more isolation lamp module(s) in the peak firing zone is set forth in our U.S. Pat. No. 7,805,064. Where a forming gas is not used, an exemplary furnace is shown in our U.S. Pat. No. 8,571,396, or in US published Application 2014/0017848 A1.
With respect to wafer transport systems, wire mesh belts such as shown in our U.S. Pat. No. 7,805,064 may be used. However, an ultra-low mass transport system such as shown in our U.S. Pat. Nos. 8,039,289, 8,236,596 and 8,828,776 may be employed. As to transports, single or dual- and multi-lane wide transport belts, ultra-low mass, or zero mass shadowless finger drive systems may be employed in the furnace system. The transport systems are driven synchronously by a single drive system (motor and associated gears, jack shafts, chains and the like), or by separate, independently controllable drive systems, such as shown in our U.S. Pat. No. 8,816,253.
The preferred transport system, as used in the exemplary embodiments herein, is a “Zero Mass”, “Shadowless” finger drive system, as described in detail in our U.S. Pat. No. 8,829,396. This finger drive system permits high speed operation on the order of 200-400 inches/minute, very short dwell times in (transport through) the peak firing zone on the order of 1-2 seconds. This Shadowless finger drive system may be used in an IR furnace configured with an isolation lamp module so that forming gas may be used in the peak firing zone followed by a compressed gases quench zone (forming gas may be used in the quench jets). Another advantage of the Shadowless finger drive system is that it permits exposure on both sides of the wafer simultaneously or sequentially, with no belt structure shadowing the underside of the wafers. Thus, in the ELS module of the inventive HILZ, the forming gas accesses both the top and bottom sides of the wafers so that this gas can permeate the Silicon of the wafers more efficiently to assist in passivation or LID reduction. It should be understood that individual ELS modules, or the HILZ, may include isolation windows so that the forming gas may be kept separate from the lamps of the ELS modules.
In accord with the inventive HILZ system, the full-spectrum high radiation intensity of the ELS modules is maintained in the range of 3-10 Sols, preferably on the order of greater than 4 Sols. While we do not wish to be bound by theory, under this level of full-spectrum radiation, a portion of the H2 of the forming gas dissociates, forming a proton component (e.g., a “protium”, hydrogen-1, 1H, isotope or ion), which is 1/64,000th the size of the hydrogen atom and thus more permeable into the silicon crystalline structure of the wafer. It is believed that the protium isotope is “injected” into the wafers by the radiant energy. With respect to the term “Sols” used herein, the solar power density at the equator on a bright day at noon is about 1000 watts per square meter (103 W/m2) which is equivalent to 105 Lux. This value is called a “standard sun” or “Sol”, thus the range used herein is 3×103-104 watts/m2. The higher the intensity, in Sols, the shorter the exposure time that is required to reduce the detrimental LID effect on wafers used in solar cell panel arrays. This translates into shorter HILZ zone with fewer ELS modules. We also have found that intermittent exposure, an ON/OFF strobing effect exposure, is effective in reducing the LID. While we do not wish to be bound by theory, it is presently thought that the alternating intervals of HILR exposure (ON) compared to dark (OFF) prevents BsO2i-type BOC formation, or the uncoupling of such complexes. The light initiates the BOC breakdown, which then proceeds during the dark interval. The ON/OFF intervals are on the order of less than 1 second. We have found that a shadow mask produces effective strobing for ELP lamps, and Xenon, Halogen and LED lamps may be electronically controlled for the ON/OFF strobing effect.
In a first apparatus embodiment, a high-intensity full-spectrum (as defined above) Enhanced Light Source (“ELS”) is provided in one or more module(s) that is/are installed in-line in a wafer processing line so that the LID treatment is effected as part of a continuous wafer firing operation. The ELS module(s) may be placed at any suitable place in the processing line, two alternative locations being described herein by way of example. In these examples the ELS module(s) are shown above the line, that is, above the top surface of the wafer as it is transported along the processing line for treatment, but it should be understood that the invention includes disposing the ELS modules above and/or below the wafer transport path, depending on the wafer surfaces to be treated with high-intensity radiation. Several embodiment configurations of the ELS modules are disclosed by way of example: Example I) single, solid state electrode-less lamp, employing a solid-state device to generate RF energy that powers a plasma emitter, with water cooled plasma generator engine and air-cooled parabolic reflector as shown in detail in
Other high-intensity discharge lamps may be used for the ELS to produce the necessary range of light radiation (3-10 Sols), but the LEP module lamps of Example II, as used herein have the advantage of reliability, an order of magnitude higher lumen density from each lamp device, a full color spectrum having a color-rendering index up to about 95, and the ability to be controlled for light intensity down to 20% full brightness (dimming or “turn-down”). LEP lamps are available commercially, being used as grow lamps, for area and high mast lighting, such as parking lots, roadways, in high-bay industrial and commercial facilities (e.g., membership warehouse stores, and super-centers), and in entertainment and architectural lighting installations. The Example II LEP lamps are also available commercially being principally used in agricultural hydroponic and aeroponic grow facilities, and in industrial and commercial facilities. Similarly, high-intensity Zenon and Halogen ELS lamps have suitable full spectral output and can produce the radiation intensity required for the inventive high speed, in-line LID treatment.
In one embodiment, one or more of the wafer surface(s), e.g., top surface, is/are continuously exposed to the ELS full-spectrum high-intensity light in the HILZ. In an alternate embodiment, one or more of the wafer surface(s) is/are exposed intermittently to the light, e.g.: 1) by ON-OFF electronic switching of the ELS lamp sources, e.g., LED, Zenon or Halogen; 2) by use of a slotted mask between the ELS lamps and the wafers, e.g., LEP lamp; or 3) by use of a rotating, slotted disk, also for an LEP lamp. The mask or rotating disk projects alternating bands of full-spectrum high-intensity radiation, HILR, (ON) and reduced intensity shadow (OFF) onto the wafer top surface as the wafer is transported along the treatment path, creating an intermittent ON/OFF, strobing effect. In the latter two embodiments, the reduced intensity (shadow) band functions as the OFF mode for the ELS lamp even though the ELS is still continuously ON. The use of the mask or rotating slotted disk lengthens the ELS service life, which is otherwise shortened by frequent ON-OFF cycling. The widths of the mask slots and solid “lands” are selected in relation to the rate of wafer transport to provide reduced intensity shadow (“OFF”) during a selected percentage of the dwell time of the wafer traversing under an ELS while in the HILZ. While we do not wish to be bound by theory, the intermittent ON/OFF high-intensity full-spectrum radiation exposure assists in the decoupling of BOCs in the wafer body, thereby improving LID reduction.
In a first example: HILZ Location A, Examples I, II or III ELS module(s) are placed downstream of a diffusion furnace, e.g., between an ARC (Anti-Reflective Coating) module and the printing module. Where the Boron is coated on or doped into the silicon wafer surface upstream of the diffusion furnace, the inventive ELS module immediately follows the diffusion furnace or the ARC module before the paste is applied to the back contact Boron-treated surface.
In a second exemplary location: HILZ Location B, Examples I, II or III ELS module(s) are disposed downstream of the quench zone of a metallization furnace, just downstream of the furnace firing zone, and upstream of the annealing zone.
The ELS module radiation treatment may be applied to one or both sides of the wafers, and preferably to the Boron-treated side. The amount of radiation is measured in Sols, meaning the light flux of sunlight at noon at the equator on a clear day. The inventive modules are configured with ELS sources to provide from 3-10 Sols of radiation. The dwell time of the wafers transiting through the HILZ under ELS radiation is inversely proportional to the speed of transport of the wafers and will typically range from about 10 seconds to about 5 minutes, more preferably from about 10-180 seconds. To increase the radiation flux in the 3-10 Sol range the number of ELS lamps, the number of ELS modules in series (each having one or more ELS lamp(s), or the lamp output may be increased for a given dwell time. Lamp output is controlled and adjusted by means of a controller that controls voltage and/or amperage to the lamps. The full-spectrum light source for the high-intensity radiation ELS modules is preferably a Light Emitting Plasma source, but may also include a high-intensity LED source, or Xenon or Metal Halide high intensity discharge source.
The wafer transport may include current wire mesh belts. However, where the underside of the wafer is to be treated in a diffusion furnace or a metallization furnace, a zero-mass finger drive of the type disclosed in our U.S. Pat. No. 8,829,396 is preferred. In the detailed examples below, a finger drive is used and shown in the drawings. The finger drive has the advantage of being essentially zero mass, and the wafers cool much more quickly, as there is no heated belt mass to retain residual heat that slows cooling. Thus, using a finger drive, the wafer upon reaching the peak temperature in the peak firing zone can be immediately cooled in the quench zone to the temperature required for the full-spectrum radiation treatment of the instant process invention.
In accord with the principles of the invention, it will be evident to those skilled in the art that the visible spectrum radiation may be supplied by any high-intensity full-spectrum light source, and the ELS modules may be integrated with any type of metallization furnace having an annealing section. The light sources (lamps) output is controlled by any suitable controller to provide the light intensity within the preferred 3-10 Sols range, and to provide selected output and turn-down as needed during processing. The ELS modules may be also used as separate modules inserted at any suitable point in the wafer processing line, such as upstream of the metallization firing furnace, or both downstream and upstream of that firing furnace. ELS modules may be used with or without a forming gas, and with or without wafer heating during the radiation treatment. The wafer heating during radiation may be accomplished by a wide variety of means, including platen, open resistance wire coils, or lamp heating. Any type of wafer transport may be used, including standard wire mesh belts, ultra-low mass drives, ceramic roller drives, and zero-mass finger drive systems. The transport system may be single or multiple lane, either driven synchronously off a single jack shaft or independent side-by-side drives. In the case of side-by-side drives, a single furnace width may be longitudinally divided to provide two or more wafer transport and processing lanes, which dividers permit isolation of each lane for independent control therein. One skilled in this art of wafer treatment will easily recognize that in accord with the teaching of this application, the particular schedule of diffusion, metallization firing, and HILZ LID reduction treatment (BOC passivation, deactivation, wafer energy conversion back to near initial state, or conversion efficiency restoration) may be controlled and modified for particular types and sizes of wafers, and may be tailored to the doping components and paste compositions.
It should be understood that “shadowless” and “shadow mask” as used herein are not the same and are not to be confused. Shadowless refers to a type of transport system in which the underside (bottom surface) of the wafers are not occluded (shadowed) by furnace mechanisms, such as conveyor transport members of conventional furnaces. In contrast, shadow mask refers to a physical element interposed between the ELS bulb and the wafer to produce a strobing of the HILR (intermittent ON/OFF of the HILR) as the wafers are transported through the HILZ.
The invention is described in more detail with reference to the drawings, in which:
The following detailed description illustrates the invention by way of example, not by way of limitation of the scope, equivalents or principles of the invention. This description will clearly enable one skilled in the art to make and use the invention, and describes several embodiments, adaptations, variations, alternatives and uses of the invention.
In this regard, the invention is illustrated in the several figures, and is of sufficient complexity that the many parts, interrelationships, and sub-combinations thereof simply cannot be fully illustrated in a single patent-type drawing. For clarity and conciseness, several of the drawings show in schematic, or omit, parts that are not essential in that drawing to a description of a particular feature, aspect or principle of the invention being disclosed. Thus, details of one embodiment of one feature may be shown in one drawing, and the details of another feature will be called out in another drawing.
Following the diffusion firing zone 18 is an ARC coating apparatus 20, which coats an anti-reflective coating onto the P-doped upper surface of the wafers. Optionally, following ARC coating in zone 20, the wafers can be flipped-over and the bottom side doped with a B-compound in zone 22 and dried. In that case, the wafers are then flipped again for introduction into ELS-containing HILZ apparatus 24A (ELS/HILZ Zone A) wherein the top or/and bottom surface(s) are exposed to high-intensity full visible spectrum radiation, HILR, by ELS lamps (disclosed above, and in more detail below). The number of ELS lamps in zone 24A will be selected for the desired exposure dwell time at the selected, controlled transport conveyor rate of the furnace, and the light intensity within the range of from about 3 Sols to about 10 Sols. Exemplary lamps are LEP, Xenon, Halogen or LED type lamps to provide the high-intensity full-spectrum light radiation, HILR. The HILR exposure treatment in ELS/HILZ zone 24A may also be accompanied by exposure to a forming gas having from 2-90% H2 and the balance N2. The wafers may be heated to within the range of from about 100° C. to about 300° C., e.g., by a platen heater or resistance coils, 50, disposed beneath the wafers and located in the gap between the transport fingers. Optionally, the wafers may be heated from below or/and from above by use of suitably located high-intensity IR lamps of the type used in the diffusion or metallization furnaces of this line.
The irradiated wafers exit ELS/HILZ Zone A, 24A, into printer 26 which applies a fine grid of Ag-based paste to the top (P-doped) surface of the wafers and a full surface area, Al-based paste to the bottom (B-doped) surface of the wafers, and dried. The doped, diffusion-fired, ARC-coated and printed wafers (and optionally irradiated) are then fed into a multi-zone, high-intensity, IR-Lamp heated metallization furnace 28, which includes a burn-out and pre-heat zones 28a, a peak firing zone 28b, and a quench zone 28c containing air knives to quickly cool the wafers from peak firing of in the range of from about 800° to about 1050° C. The high-intensity IR lamps in the metallization furnace 28 are designated IRL in
In this example a metallization furnace having one or more isolation lamp module(s) forming the peak firing zone 28b includes a quartz window separating the wafer processing zone through which the transport drive moves the wafers from the high-intensity IR lamp zone. This isolation configuration permits supply of the forming gas to the wafers in the peak firing zone, and in the adjacent downstream ELS/HILZ Zone B, 30. In
The left end of
Continuing with the embodiment in which LEP-type ELS lamps are used in the HILR treatment zone, HILZ-B,
Alternately,
In the embodiment calling for intermittent light exposure treatment of the wafers,
The mask slots also assist in collimating the light, so that as the wafer passes underneath it, see
As an option to using a shadow mask, a horizontal, rotating thin plate having one or more slots therein at the output aperture of the ELS lamp module may be used. In another alternative, the ELS lamp modules may be spaced apart with suitable vertical shielding extending downwardly to close to the wafer top surface 90 so that the wafers traverse a dark zone between the longitudinally spaced-apart lamps. As an alternative to the use of a slotted metal shadow mask 78, the shadow mask may be a glass plate having dark lines formed on its surface, e.g., by vapor deposition or sputtering thereon a metal layer or opaque oxide layer. The glass may be Vycor, quartz or a high-temperature borosilicate glass. In this alternative embodiment, the shadow mask plate can thus double as the isolation window, permitting use of a forming gas in the wafer-travel processing space, WPZ (see
In the preferred shadow mask embodiment, the width and number of the mask shadowing lines are selected with respect to the light output aperture of the ELS module (e.g., 210 mm width) for a standard 6″ wafer being transported along the processing line and the conveyor transport speed (by way of example, 230 inches/minute), to provide rapid strobing (ON) effect on the top surface of the wafer on the order of less than 1 second light radiation exposure between shadow (OFF) modes. The ON/OFF intervals may be equal or unequal as noted above.
By way of example of the HILR processing method of this invention, mono-Si solar cell wafers treated with full-spectrum HILR employing an ELS of the apparatus disclosed herein were tested for LID reduction in two series of tests: Test I Series, at 5 Sols intensity with heating at between 150° C.-230° C. for a continuous illumination period in the range of 60-180 seconds; and Test II Series, at >5 Sols intensity with heating at between 230° C.-300° C. for a continuous illumination period in the range of 10-60 seconds. Both Test Series subjected the treated wafers to sunlight exposure (one week) to simulate in-use service to demonstrate LID; both Test Series exhibited unexpectedly improved LID reduction, as follows:
Test I series results show that longer ELS high-intensity full-spectrum exposure of the wafer top surface produces greater LID reduction, with doubling of time cutting the LID effect (reduction in SCE) by half or more. In addition, that doubling of exposure time effect holds true at all temperatures in the range, but the greater reduction of LID occurs at hotter temperatures in the range.
Test Series II shows that at higher temperature and higher intensity of the HILR, the treatment time can be reduced to under 1 minute with unexpected reduction in LID, 50% in these exemplary tests.
It will be understood by one of ordinary skill in this art that the one-week sunlight exposure to simulate in-use operation is relatively short, and that the LID is known to increase over time. Indeed, test Wafer # C, Series I, exhibited not only no LID, but an improvement over its initial SCE as a result of HILR treatment. That is, the 136.9% reduction in LID may be interpreted as not only no LID effect during use, but indeed, improvement in SCE during operation. Thus, with longer sunlight exposure, the reduction in LID as a result of the inventive HILR method of wafer treatment will have an even greater impact with a more substantial improvement in SCE over the useful life of the wafers in a solar cell array. The Test Series II shows that the inventive process can be integrated into a wafer processing line, such as a metallization furnace, and treat wafers at a rate matching the rate of exit of the wafers from the furnace firing/quench zones.
It is clear that the inventive HILR treatment apparatus and methods of this application has wide applicability to the solar cell processing industry, namely to LID reduction, whether through BOC formation prevention, BOC deactivation, or BOC passivation, and to restoration of the solar energy conversion efficiency of solar cell wafers back or close to original values, and that the rate of HILR treatment can match wafer firing furnace output. Thus, the inventive system has the clear potential of becoming adopted as the new standard for apparatus and methods of LID reduction in the solar cell wafer processing industry.
It should be understood that various modifications within the scope of this invention can be made by one of ordinary skill in the art without departing from the spirit thereof and without undue experimentation. For example, the ELS high-intensity light modules can have a wide range of types, designs and locations in the integrated processing line to provide the full-spectrum functionalities at in the range of intensity (3-10 Sols) disclosed herein. This invention is therefore to be defined by the scope of the appended claims as broadly as the prior art will permit, and in view of the specification if need be, including a full range of current and future equivalents thereof.
Parts List
(This Parts List is provided as an aid to Examination and may be canceled upon allowance)
This is the Regular US patent application corresponding to, and claiming priority of, U.S. Provisional Application 62/065,441 filed Oct. 17, 2014 of the same inventors under the title Solar Cell Boron Passivation System, the benefit of the filing date of which is claimed under 35 USC §§119 and 120.
| Number | Date | Country | |
|---|---|---|---|
| 62065441 | Oct 2014 | US |
