US20130247957A1 - Solar cell and solar-cell module - Google Patents

Solar cell and solar-cell module Download PDF

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US20130247957A1
US20130247957A1 US13/991,978 US201113991978A US2013247957A1 US 20130247957 A1 US20130247957 A1 US 20130247957A1 US 201113991978 A US201113991978 A US 201113991978A US 2013247957 A1 US2013247957 A1 US 2013247957A1
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electrode
solar cell
silicon
extraction
dopant
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Hiroshi Hashigami
Takenori Watabe
Mitsuhito Takahashi
Shintarou Tsukigata
Takashi Murakami
Ryo MITTA
Yoko Endo
Hiroyuki Otsuka
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Shin Etsu Chemical Co Ltd
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    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L31/00—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L31/18—Processes or apparatus specially adapted for the manufacture or treatment of these devices or of parts thereof
    • H01L31/1804—Processes or apparatus specially adapted for the manufacture or treatment of these devices or of parts thereof comprising only elements of Group IV of the Periodic Table
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L31/00—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L31/04—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof adapted as photovoltaic [PV] conversion devices
    • H01L31/042—PV modules or arrays of single PV cells
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L31/00—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L31/02—Details
    • H01L31/0216—Coatings
    • H01L31/02161—Coatings for devices characterised by at least one potential jump barrier or surface barrier
    • H01L31/02167—Coatings for devices characterised by at least one potential jump barrier or surface barrier for solar cells
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L31/00—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L31/02—Details
    • H01L31/0224—Electrodes
    • H01L31/022408—Electrodes for devices characterised by at least one potential jump barrier or surface barrier
    • H01L31/022425—Electrodes for devices characterised by at least one potential jump barrier or surface barrier for solar cells
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L31/00—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L31/04—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof adapted as photovoltaic [PV] conversion devices
    • H01L31/06—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof adapted as photovoltaic [PV] conversion devices characterised by potential barriers
    • H01L31/068—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof adapted as photovoltaic [PV] conversion devices characterised by potential barriers the potential barriers being only of the PN homojunction type, e.g. bulk silicon PN homojunction solar cells or thin film polycrystalline silicon PN homojunction solar cells
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L31/00—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L31/18—Processes or apparatus specially adapted for the manufacture or treatment of these devices or of parts thereof
    • H01L31/186—Particular post-treatment for the devices, e.g. annealing, impurity gettering, short-circuit elimination, recrystallisation
    • H01L31/1868—Passivation
    • Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E10/00—Energy generation through renewable energy sources
    • Y02E10/50—Photovoltaic [PV] energy
    • Y02E10/547—Monocrystalline silicon PV cells
    • Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02P—CLIMATE CHANGE MITIGATION TECHNOLOGIES IN THE PRODUCTION OR PROCESSING OF GOODS
    • Y02P70/00—Climate change mitigation technologies in the production process for final industrial or consumer products
    • Y02P70/50—Manufacturing or production processes characterised by the final manufactured product

Definitions

  • This invention relates to a solar cell and solar cell module having the advantages of low cost and high efficiency.
  • FIG. 1 illustrates one general solar cell of mass production model using a mono- or polycrystalline silicon substrate.
  • the solar cell includes a p-type silicon substrate 101 obtained by doping monocrystalline silicon with a dopant such as B or Ga.
  • An emitter layer 102 is formed in a light-receiving surface of silicon substrate 101 by heat treatment to diffuse a dopant for imparting n-type conductivity such as P or Sb into silicon substrate 101 in a high concentration.
  • a plurality of extraction electrodes 104 of several hundreds to several tens of microns ( ⁇ m) wide are disposed contiguous to the emitter layer 102 for extracting photogenerated electric charge from substrate 101 .
  • collector electrodes 105 of several millimeters (mm) wide are disposed for collecting the charges drawn in extraction electrodes 104 and interconnecting solar cells together. While these electrodes may be formed by various methods, one method commonly employed from the standpoint of cost is by printing a metal paste comprising fine particles of metal such as Ag and an organic binder through a screen or the like, and heat treating at a temperature of several hundreds to about 850° C. for bonding to the substrate.
  • a back electrode 107 of opposite polarity to the light-receiving side electrode is formed by using a metal paste comprising fine particles of metal such as Al or Ag and an organic binder, screen printing, and firing at a temperature of about 700 to 850° C.
  • an electric field layer 106 containing a dopant for imparting the same p-type conductivity as the substrate such as Al, B or Ga in a high concentration is formed for efficiently extracting charge generated on the back side to the outside.
  • a passivation film 103 is formed for optical confinement.
  • a silicon nitride film which is formed by chemical vapor deposition (CVD) or the like is commonly used as the passivation film.
  • the passivation film also has a further important function of passivating the silicon surface.
  • silicon atoms are in a stable state due to the covalent bond between adjacent atoms.
  • an unstable energy level known as “dangling bond” appears at the surface corresponding to the terminus of atom arrangement, where no adjacent atom to be bonded is available. Since the dangling bond is electrically active, it captures and extinguishes charge photogenerated within silicon, detracting from the operation of a solar cell.
  • the solar cells have been subjected to surface passivating treatment or otherwise treated to form an electric field such that photogenerated carriers may not be captured by dangling bonds.
  • a silicon nitride film formed by CVD is widely used because its optical properties are suited for silicon solar cells and because the film itself has a positive fixed charge and also has a high passivation effect due to the inclusion of much hydrogen capable of passivating dangling bonds.
  • the dopant concentration of the emitter layer should desirably be kept as low as possible or the depth of the emitter layer should desirably be shallow. However, reducing the dopant concentration, in turn, increases the contact resistance between silicon and metal electrode, giving rise to the problem of an increased resistance loss of generated power.
  • the localized doping structure or double doping structure is generally formed by forming a dielectric film of several hundreds of nanometers (nm) such as a silicon oxide or silicon nitride film on substrate surface as diffusion barrier, opening an electrode-forming portion of the dielectric film by photolithography (see, for example, J. Knobloch, A. Noel, E. Schaffer, U. Schubert, F. J. Kamerewerd, S. Klussmann, W. Wettling, Proc. the 23rd IEEE Photovoltaic Specialists Conference, p.
  • One simpler method suited for mass production is by premixing a dopant in a conductive paste as the electrode-forming material, as proposed in, for example, D. L. Meier, H. P. Davis, R. A. Garcia, J. A. Jessup, Proc. the 28th IEEE Photovoltaic Specialists Conference, p. 69, 2000.
  • P is added to Ag paste as dopant, for example, the paste is printed onto a silicon substrate, and the paste is fired at or above the eutectic point of Ag and Si.
  • the self-doping paste contains a dopant for forming a self-doped region, an additive for effectively forming a high-concentration doping layer, and the like in relatively high proportions. For this reason, while the self-doping paste provides a good electrical contact between electrode and silicon, the content of metal particles contributing to the conduction of charge extracted from the silicon substrate must be kept low. As a result, the sintered body of self-doping paste has a high interconnect resistance, giving rise to the problem that the output of the solar cell is reduced.
  • An object of the invention which is made under the aforementioned circumstances is to provide a solar cell and solar cell module having the advantages of a good electrical contact between a silicon substrate and an extraction electrode, a reduced loss by electrode interconnect resistance, and excellent cell characteristics.
  • the inventors have found that if a first electrode in the form of a sintered body of conductive paste containing a dopant for imparting conductivity to silicon is used as the extraction electrode, and a second electrode having a higher conductivity than the first electrode is used as the collector electrode, then the loss by contact resistance between silicon substrate and the extraction electrode and the loss by electrode resistance are reduced and solar cell characteristics are drastically improved.
  • the invention is predicated on this finding.
  • the invention provides a solar cell and solar cell module as defined below.
  • a solar cell comprising a crystalline silicon substrate of one conductivity type having a light-receiving surface, an emitter layer formed on the light-receiving surface side of the substrate and having a dopant of opposite conductivity type added thereto, a passivation film formed on the surface of the substrate, an extraction electrode for extracting photogenerated charge from the silicon substrate, and a collector electrode in contact with at least a portion of the extraction electrode for collecting the charge drawn in the extraction electrode, characterized in that the extraction electrode includes a first electrode in the form of a sintered conductive paste containing a dopant for imparting conductivity to silicon, at least the first electrode is formed so as to penetrate through the passivation layer, and the collector electrode includes a second electrode having a higher conductivity than the first electrode.
  • a solar cell comprising a crystalline silicon substrate having a non-light-receiving surface, a passivation film formed on the non-light-receiving surface of the substrate, an extraction electrode for extracting photogenerated charge from the silicon substrate, and a collector electrode disposed at least partially in contact with the extraction electrode for collecting the charge collected in the extraction electrode, characterized in that the extraction electrode includes a first electrode in the form of a sintered conductive paste containing a dopant for imparting conductivity to silicon, at least the first electrode is formed so as to penetrate through the passivation layer, and the collector electrode includes a second electrode having a higher conductivity than the first electrode.
  • a solar cell module comprising electrically connected solar cells according to any one of [1] to [18].
  • a self-doping electrode and a high conductivity electrode are used as the extraction electrode and collector electrode, respectively. Then the loss by silicon-electrode contact resistance and the loss by electrode resistance are reduced and at the same time, optical and electric losses in the emitter layer are reduced. Solar cell characteristics are drastically improved. Also, the process can be implemented by conventional screen printing and similar techniques, which is quite effective for cost savings.
  • FIG. 1 is a schematic perspective view of an exemplary structure of a conventional solar cell.
  • FIG. 2 is a schematic perspective view of an exemplary structure of a solar cell in one embodiment of the invention.
  • FIG. 3 is a schematic perspective view of an exemplary structure of a solar cell in another embodiment of the invention.
  • FIG. 4 is a schematic perspective view of an exemplary structure of a solar cell in a further embodiment of the invention.
  • FIG. 5 is a plan view of a printing plate for use in electrode formation according to the invention, (a) showing a pattern of extraction electrode alone, (b) showing a pattern of collector electrode alone, and (c) showing a combined pattern of extraction and collector electrodes.
  • FIG. 6 is a schematic perspective view of an exemplary structure of a solar cell in a yet further embodiment of the invention.
  • FIG. 7 is a schematic perspective view of an exemplary structure of a solar cell in a still further embodiment of the invention.
  • FIG. 8 is a diagram illustrating values of interconnect resistance and contact resistance in Example and Comparative Example.
  • FIGS. 2 to 8 several embodiments of the invention are described below.
  • Like reference characters designate like or corresponding parts throughout the several views while their description is sometimes omitted.
  • FIG. 2 illustrates a solar cell in one embodiment of the invention.
  • the solar cell includes a crystalline silicon substrate 201 of one conductivity type, an emitter layer 202 formed on the silicon substrate 201 and having a dopant of opposite conductivity type added thereto, a passivation film 203 formed on the surface of the emitter layer 202 , an extraction electrode for extracting photogenerated electric charge from the silicon substrate 201 , and a collector electrode for collecting the charge drawn in the extraction electrode, wherein the electrodes are formed by printing and firing conductive paste.
  • the extraction electrode includes a first electrode 204 in the form of a sintered body of conductive paste containing a dopant for imparting the same conductivity type as the emitter layer to silicon.
  • the first electrode 204 is formed so as to penetrate through the passivation layer 203 , and at the same time, a self-doped region 208 into which the dopant from the first electrode 204 is diffused at a high concentration is formed immediately below the first electrode 204 .
  • This enables to establish a good electrical contact between the first electrode 204 and the silicon substrate 201 and to reduce the dopant concentration or depth of the emitter layer 202 , and eventually to ameliorate any degradation of solar cell characteristics due to carrier recombination and free carrier absorption in the emitter layer.
  • the collector electrode includes a second electrode 205 having a higher conductivity than the first electrode 204 , which enables to significantly reduce the output power loss of the solar cell by interconnect resistance.
  • an electric field layer 206 and a back electrode 207 are illustrated.
  • An as-cut monocrystalline ⁇ 100 ⁇ p-type silicon substrate in which high purity silicon is doped with a Group III element such as B or Ga so as to give a resistivity of 0.1 to 5 ⁇ -cm is etched with a conc. alkali solution of sodium hydroxide or potassium hydroxide having a concentration of 5 to 60% by weight or mixed acid of hydrofluoric acid and nitric acid for removing the work damaged surface layer.
  • the monocrystalline silicon substrate may have been prepared by either the CZ or FZ method.
  • the texture is an effective means for lowering the reflectivity of solar cells.
  • the texture may be readily provided by immersing the substrate in a hot alkaline solution of sodium hydroxide, potassium hydroxide, potassium carbonate, sodium carbonate, sodium hydrogencarbonate or tetramethylammonium hydroxide (concentration 1 to 10 wt %) at a temperature of 60 to 100° C. for about 10 to about 30 minutes. Often, a proper amount of 2-propanol is dissolved in the alkaline solution to control the reaction.
  • the texturing is followed by washing with an aqueous acidic solution such as hydrochloric acid, sulfuric acid, nitric acid or hydrofluoric acid or a mixture thereof. Washing with hydrochloric acid is preferred from the cost and property standpoints. To enhance cleanness, washing may be carried out by mixing 0.5 to 5 wt % of aqueous hydrogen peroxide with aqueous hydrochloric acid and heating at 60 to 90° C.
  • an aqueous acidic solution such as hydrochloric acid, sulfuric acid, nitric acid or hydrofluoric acid or a mixture thereof.
  • washing may be carried out by mixing 0.5 to 5 wt % of aqueous hydrogen peroxide with aqueous hydrochloric acid and heating at 60 to 90° C.
  • an emitter layer is formed by vapor phase diffusion using phosphorus oxychloride.
  • the P concentration and depth of the emitter layer are determined by a balance of resistance to current flow through the emitter layer and surface passivation effect, or the like. Typically, they are determined such that the emitter layer may have a sheet resistance of 50 to 400 ohm/square ( ⁇ / ⁇ ) as measured by the four probe method.
  • a p-n junction In common silicon solar cells, a p-n junction must be formed only on the light-receiving surface. To this end, suitable means must be taken for avoiding any p-n junction on the back surface, for example, by carrying out diffusion while two substrates are mated together, or by etching away the diffusion layer on one side in aqueous alkaline solution or the like. At the end of diffusion, the glass formed on the surface is removed using hydrofluoric acid or the like.
  • an antireflection/passivation film is formed on the light-receiving surface.
  • a silicon nitride or similar film is deposited to a thickness of 80 to 125 nm, typically about 100 nm.
  • a mixture of monosilane and ammonia (NH 3 ) is used as the reactant gas although nitrogen may be used instead of NH 3 .
  • the desired refractive index may be obtained by using H 2 gas to dilute the film-forming species, to adjust the process pressure, or to dilute the reactant gas.
  • the film is not limited to silicon nitride, and instead, silicon oxide, silicon carbide, aluminum oxide, amorphous silicon, microcrystalline silicon or titanium oxide may be used while it may be formed by heat treatment, atomic layer deposition or the like as well as chemical vapor deposition.
  • a first electrode is formed on the emitter layer.
  • a silver paste is used which is prepared by mixing silver powder, glass frit and dopant with an organic binder.
  • the dopant used herein is a Group V element such as P, In or Sb alone or a compound thereof or a combination thereof.
  • the composition of the paste must be adjusted depending on the structure and type of a solar cell. When diphosphorus pentoxide is used, for example, it is formulated in a proportion of about 0.1 to 30% by weight, preferably 2 to 15% by weight.
  • the type and amount of the organic binder are well known.
  • the paste is screen printed and fired or heat treated to establish conduction between the electrode and the silicon.
  • This heat treatment is known as a fire-through phenomenon that during firing of silver paste, the silicon nitride film reacts with the glass frit and is thus decomposed, allowing the Ag particles to penetrate through the silicon nitride film to make electrical contact with the substrate.
  • the fire-through technique is widely used in the manufacture of crystalline silicon solar cells.
  • the dopant in the silver paste diffuses, in part, into the silicon substrate to achieve self-doping even on heat treatment at a temperature of about 700 to 800° C. in the electrode firing temperature range commonly employed, firing at a temperature equal to or higher than 835° C., the eutectic point of Ag and Si, is recommended in order to form a self-doped region more effectively.
  • silicon reacts with silver and melts, and then recrystallizes while taking in additive dopant. As such, high concentration doping is accomplished, making a better electrical contact between the sintered silver and silicon.
  • the electrical contact resistance between silicon and electrode is correlated to the carrier concentration, that is, dopant concentration on silicon surface and the electrode material. Where an electrical contact is made between conventional printed silver electrode and silicon, it is believed that the dopant concentration on silicon surface must be at least 1 ⁇ 10 19 cm 3 , preferably at least 5 ⁇ 10 19 cm 3 .
  • the dopant concentration may be directly measured by secondary ion mass spectroscopy (SIMS) or the like. This quantitative measurement, however, is scarcely used in the production site because preparation of a sample is cumbersome and measurement requires skill.
  • SIMS secondary ion mass spectroscopy
  • the spreading resistance method is utilized. Specifically, the method is by abutting two metal probes against a silicon substrate, conducting current flow between the two points, and measuring a voltage drop thereacross. The spreading resistance is the voltage drop divided by the current value. Since the voltage drop occurs in principle at a minute domain near the contact point of the probe, this method enables evaluation of the minute domain. If the contact area between the probe and the silicon substrate is recognized, then the resistivity relative to the dopant concentration on silicon surface may be determined.
  • the resistivity of the region at its surface should preferably be 10 m ⁇ -cm or less, more preferably 2 m ⁇ -cm or less.
  • the lower limit is usually at least 0.5 m ⁇ -cm though not critical.
  • the resistivity of the emitter layer (formed in the light-receiving area) at its surface should preferably be as high as possible from the standpoint of suppressing the aforementioned optical loss and carrier recombination loss, but should preferably be somewhat low from the standpoint of increasing the photovoltage. That is, the resistivity of the emitter layer at its surface should fall in an optimum range. The optimum range is 5 to 50 m ⁇ -cm though it varies with the structure of a solar cell. On the other hand, to take the maximum advantage of dual doping structure, the emitter layer should be designed and controlled such that the resistivity of the emitter layer at its surface may be higher than the resistivity of the self-doped region.
  • a second electrode is formed on the first electrode by screen printing and firing.
  • the second electrode should be endowed with a higher conductivity than the first electrode for the purpose of suppressing the interconnect resistance loss when the charge extracted from the silicon substrate to the first electrode flows to the collector electrode.
  • Such an electrode may be prepared using a silver paste containing a higher proportion of silver particles, for example.
  • the resistivity of the second electrode which is preferably lower should desirably be up to 5 ⁇ -cm at most, more preferably up to 3 ⁇ -cm.
  • the steps of printing and firing the first electrode and the steps of printing and firing the second electrode may be separately performed as mentioned above.
  • the second electrode is printed, and single heat treatment is effected for firing both the electrodes at the same time.
  • the extraction electrode may have a laminate structure consisting of first and second electrodes, and the collector electrode have a monolayer structure consisting of a second electrode as shown in FIG. 2 .
  • the extraction electrode may have a monolayer structure consisting of a first electrode, and the collector electrode have a monolayer structure consisting of a second electrode, as shown in FIG. 3 .
  • the extraction electrode and collector electrode each may have a laminate structure consisting of first and second electrodes as shown in FIG. 4 .
  • the structure of these electrodes may be prepared, for example, by screen printing an electrode paste to form, in case of the first electrode, a pattern consisting solely of extraction electrodes as shown in FIG. 5( a ), or a pattern of both extraction and collector electrodes as shown in FIG. 5( c ), and in case of the second electrode, a pattern as shown in FIG. 5( c ) or a pattern consisting solely of collector electrodes as shown in FIG. 5( b ).
  • the electrode forming method is not limited to screen printing and may be performed by inkjet printing, dispenser, intaglio printing, aerosol spraying or the like.
  • An electrode having a structure as shown in FIG. 4 may be prepared by effecting metallization, with the first electrode serving as seed, to form the second electrode.
  • electroplating, electroless plating or photo-plating is applicable.
  • the second electrode may penetrate through the passivation layer 203 , for example, by fire-through capability, until it contacts the emitter layer 202 , as shown in FIGS. 2 and 3 , or may not penetrate through the passivation layer 203 as shown in FIG. 6 .
  • the embodiment of FIG. 6 wherein the passivation film immediately below the collector electrode is left intact inhibits recombination of carriers at the silicon surface in this portion, thus improving solar cell characteristics.
  • the fire-through capability of electrode paste to penetrate through the passivation film is tailored by the amount of low-softening-point glass frit added.
  • the second electrode may be formed using a high-temperature firing paste containing a relatively small amount of glass frit or free of glass frit, or a low-temperature cure resin paste.
  • the back electrode is formed by mixing aluminum powder with an organic binder and screen printing the resulting paste. Printing is followed by firing at a temperature of 700 to 900° C. for 5 to 30 minutes to form the back electrode and an electric field layer.
  • the electric field layer may also be formed by vapor phase diffusion of boron bromide, for example. In this case, it is preferred from the standpoint of suppressing interconnect resistance to use silver paste to form the back electrode.
  • Firing of the back electrode and the light-receiving surface electrode may be performed at a time. Also, the order of forming electrodes on opposite surfaces may be reversed.
  • FIG. 7 illustrates an embodiment wherein the electrode of the invention is applied to both the light-receiving surface and the non-light-receiving surface.
  • the p-type silicon solar cell uses the silicon substrate 401 of p-type conductivity
  • this embodiment is such that the self-doped region 407 b formed immediately below the non-light-receiving side first electrode 404 b is of p-type conductivity and the self-doped region 407 a on the light-receiving side is of n-type conductivity.
  • a self-doping paste containing a Group V element is used for the light-receiving side first electrode 404 a and a self-doping paste containing a Group III element is used for the non-light-receiving side first electrode 404 b .
  • an emitter layer 402 is also illustrated.
  • a passivation layer 403 a is also illustrated.
  • collector electrodes 405 a and 405 b are also illustrated.
  • Such a structure on the non-light-receiving side allows the non-electrode-forming surface to be covered with the electric field layer 406 and passivation film 403 b , enhancing the collection efficiency of photogenerated carriers. It is noted that the electric field layer 406 may not be formed where the passivation film has a fully high passivation effect.
  • first and second electrodes 404 b and 405 b on the non-light-receiving side may be the same as the electrodes on the light-receiving side in FIGS. 2 to 6 .
  • the extraction electrode on the non-light-receiving side may have a laminate structure consisting of first and second electrodes
  • the collector electrode have a monolayer structure consisting of a second electrode
  • the extraction or collector electrode may have a monolayer structure consisting of a first or second electrode
  • the extraction electrode and collector electrode each may have a laminate structure consisting of first and second electrodes.
  • the second electrode 405 b may penetrate through the passivation layer 403 b until it contacts the field effect layer 406 or silicon substrate 401 , as shown in FIG. 7 , or may not penetrate through the passivation layer.
  • a reflector (not shown) is preferably provided for taking in again the light transmitted by the substrate.
  • the reflector may be a film of aluminum or silver formed by vacuum evaporation or the like, a sufficient reflector effect is obtainable simply by using a white backsheet or the like on the solar cell module without any additional treatment. Absent the reflector, electricity generation is yet possible by causing scattering light to enter from the back surface or by placing the solar cell such that the non-light-receiving surface may become a light-receiving side.
  • the solar cell of the invention is described by referring to the embodiments using p-type silicon substrates, the invention is equally applicable to a solar cell using an n-type silicon substrate.
  • silicon substrate 401 , electric field layer 406 and self-doped region 407 b on the non-light-receiving side are of n type and the emitter layer 402 and self-doped region 407 a on the light-receiving side are of p type.
  • the silicon substrate 401 is a n-type crystalline silicon substrate which is prepared by doping high-purity silicon with a Group V element such as P or Sb to give a resistivity of 0.1 to 5 ⁇ -cm.
  • the emitter layer 402 may be formed when the silicon substrate is doped with boron by vapor phase diffusion using boron bromide, for example.
  • the electric field layer may be formed by vapor phase diffusion using phosphorus oxychloride, for example.
  • the self-doped layer 407 a on the light-receiving side is formed using a self-doping paste containing a Group III element such as B, Al, Ga or In alone or a compound thereof or a combination thereof.
  • the self-doped layer 407 b on the non-light-receiving side is formed using a self-doping paste containing a Group V element such as P, As or Sb alone or a compound thereof or a combination thereof.
  • a plurality of solar cells according to the invention may be electrically connected and used as a solar cell module.
  • the connection may be made by any well-known methods.
  • a solar cell having a conventional electrode structure and a solar cell having an electrode structure according to the invention are compared for electricity generating ability.
  • a silicon nitride film was formed over the sample surface on the light-receiving side as a passivation film.
  • the substrates were divided into three groups (1), (2) and (3), each consisting of 30 substrates.
  • Each of different silver pastes (see below) was printed on the substrates as a light-receiving side electrode using a printing screen having a pattern of extraction and collector electrodes on a common screen as shown in FIG. 5( c ).
  • printing conditions such as printing pressure and squeeze angle were controlled such that an equivalent line width and cross-sectional area were obtained at the end of firing.
  • Group (1) is a comparative example by the prior art technique.
  • first electrode ordinary fire-through type high-temperature firing paste (paste A) was screen printed and dried.
  • paste B high-conductivity silver paste
  • firing at 830° C. or optimum condition was carried out in the ambient (air) atmosphere.
  • Group (2) is another comparative example by the prior art technique.
  • fire-through type self-doping silver paste (paste C) having a phosphorus compound added so that the self-doped region might have a resistivity of 2 m ⁇ -cm was screen printed and dried.
  • paste C was again screen printed as the second electrode so that the first electrode was completely overlaid therewith. Thereafter, firing at 880° C. or optimum condition was carried out in the ambient atmosphere.
  • Group (3) is an example of the invention.
  • Paste C was screen printed and dried as the first electrode, and paste B was screen printed as the second electrode so that the first electrode was completely overlaid therewith. Thereafter, firing at 880° C. or optimum condition was carried out in the ambient atmosphere.
  • the shape of light-receiving side electrode was examined by selecting 5 samples from each group, and measuring the line width and cross-sectional area of the electrode at nine (9) positions within the sample surface under a laser microscope.
  • Table 1 reports an average of measurements for each group, demonstrating that electrodes of equivalent shape were obtained for all the groups.
  • Determination of contact resistance was by the ladder method.
  • Determination of interconnect resistance was carried out by cutting out an extraction electrode portion from the solar cell sample, placing probes at opposite ends of the electrode and measuring current-voltage values.
  • FIG. 8 illustrates relative values of the two resistances for each group, provided that the average value of samples of group (1) is 1. It is seen that the samples of group (3) having the electrode structure according to the invention have a low contact resistance. It is thus concluded that the samples of group (3) show the highest fill factor in Table 2 as a result of the contact resistance and interconnect resistance being suppressed.

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EP2650923B1 (fr) 2021-06-02
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EP2650923A4 (fr) 2017-11-22
CA2820002A1 (fr) 2012-06-14

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