Patent Description:
Semiconductor substrates for solar cells are usually manufactured by a Czochralski method (CZ method), which can produce a single crystal with a large-diameter at relatively low cost. For example, P-type semiconductor substrates can be obtained by drawing a silicon single crystal doped with boron by a CZ method, and slicing this single crystal. Thus obtained silicon substrates doped with boron, being irradiated with strong sunlight, cause decrease in the lifetime under the influence of boron and oxygen in the substrate. As a result, the light induced degradation comes to being.

In order to solve such light induced degradation issue, <CIT> proposes the use of gallium instead of boron as P-type dopant.

As a backside structure of solar cells, a structure having a Back Surface Field (BSF) region can be illustrated. The BSF region can be applied to the almost whole surface of the backside by printing an aluminum paste to the almost whole surface of the backside of a substrate and firing thereof.

Other structures include a structure which has local contacts between the substrate and a back surface electrode and is protected by a dielectric film on the most of the back surface, which acts as a passivation layer, in order to further improve the efficiency. These solar cell structures are referred to as a Passivated Emitter and Rear Contact Solar Cell (PERC) structure and a Passivated Emitter and Rear Locally Diffused Solar Cell (PERL) structure.

The cross section of the solar cell having a previous PERL structure is schematically shown in <FIG>. As shown in <FIG>, the solar cell <NUM> is provided with the N-conductivity type layer (emitter layer) <NUM> on the side of the light-receiving surface of the P-type silicon substrate <NUM>, and the light-receiving surface electrode <NUM> on this N-conductivity type layer <NUM>. In many cases, the solar cells each have the anti-reflection film <NUM> on the light-receiving surface. The solar cell is also provided with the dielectric film <NUM>, which acts as a passivation film or a protective film, on the back surface; the back surface electrode <NUM> on the back surface; and the BSF layer <NUM> at the contact area where the back surface electrode <NUM> is in contact with the P-type silicon substrate <NUM>. <CIT> discloses a solar cell using a Ga-doped substrate.

In manufacturing of the foregoing solar cells having the PERC structure and the PERL structure, etc., the formation of a dielectric film on the backside, particularly when using a silicon substrate doped with gallium (hereinafter, referred to as a "gallium-doped substrate"), causes diffusion of the doped gallium atom(s) to the side of the dielectric film to decrease the surface concentration of gallium (P-type dopant) in the backside of the substrate.

Such decrease in the surface concentration of gallium in the backside of the substrate causes i) an increase in the contact resistance; ii) formation of the inversion layer <NUM> in the backside of the substrate as shown in <FIG> when forming a dielectric film having positive charge, thereby generating leak current near the contact (contact area) to seriously degrade the characteristics of the solar cell.

The present invention was accomplished in view of the above-described problems. It is an object of the present invention to provide a solar cell with excellent conversion efficiency provided with a gallium-doped substrate, and a method for manufacturing the same.

To achieve the above-described object, the present invention providesa solar cell (<NUM>) comprising a P-type silicon substrate (<NUM>) in which one main surface is a light-receiving surface and another main surface is a backside, a dielectric film having positive charge on the backside, and an N-conductivity type layer (<NUM>) in at least a part of the light-receiving surface of the P-type silicon substrate,.

wherein the concentration of the group III element at the diffusion surface in the backside is in a range of <NUM>×<NUM><NUM> atom/cm<NUM> or more and <NUM>×<NUM><NUM> atom/cm<NUM> or less over the whole area of the backside.

Such a solar cell, containing a group III element diffused in the backside of the substrate, has sufficient concentration of P-type dopant in the backside of the substrate even when a dielectric film is formed on the backside of a gallium-doped substrate. This can be a solar cell having high conversion efficiency that can prevent an increase in the contact resistance and generation of leak current near the contact.

In the solar cell having such a concentration of a group III element being diffused in the backside, degradation of the cell charateristics can be reduced while eliminating the decrease in the concentration of a P-type dopant in the backside.

These are particularly suitable elements contained in the backside of the substrate of the inventive solar cell.

The present invention also provides a method for manufacturing a solar cell (<NUM>) having a P-type silicon substrate (<NUM>) in which one main surface is a light-receiving surface and another main surface is a backside, comprising the steps of:.

Such a method for manufacturing a solar cell can introduce a P- layer in which a group III element is diffused in the backside. Accordingly, even when a dielectric film is formed on the backside of a gallium-doped substrate as a passivation film and so on, the amount of the P-type dopant is compensated, which makes it possible to prevent decrease in the P-type dopant concentration near the backside surface of the substrate in contact with the dielectric film. As a result, it is possible to avoid drop in the voltage due to leak current to keep the high efficiency.

It is also preferable that the step of diffusing a group III element and the step of forming an N-conductivity type layer be performed in one thermal treatment.

Such a method for manufacturing a solar cell can easily form a layer which contains a group III element at low cost.

The inventive solar cell contains a group III element diffused in the backside of the substrate, thereby having sufficient P-type dopant concentration in the backside of the substrate even when a dielectric film is formed on the backside of the gallium-doped substrate. The inventive method for manufacturing a solar cell introduces a group III element such as boron to the backside to compensate the amount of P-type dopant, which makes it possible to prevent decrease in the P-type dopant concentration, even when a dielectric film is formed on the backside of a gallium-doped substrate as a passivation film and so on, in the vicinity of the backside surface of the substrate in contact with the dielectric film. As a result, it is possible to avoid drop in the voltage due to leak current to keep the high efficiency.

Hereinafter, the present invention will be more specifically described.

As described above, a solar cell with excellent conversion efficiency provided with a gallium-doped substrate and a method for manufacturing the solar cell has been demanded. However, when the gallium-doped substrate is used as a substrate for a solar cell, and a dielectric film is formed on the surface of the substrate as a protective film or a passivation film, the amount of gallium, which is dopant, is decreased at an area being in contact with the dielectric film and in the vicinity thereof as described above.

The inventors have diligently investigated to solve the problems. As a result, the inventors have found that a solar cell having a gallium-doped substrate and a dielectric film on the backside, and containing a group III element diffused in the backside of this substrate can solve the foregoing problems; thereby brought the inventive solar cell and the method for manufacturing the same to completion.

Hereinafter, an embodiment of the present invention will be specifically described with reference to FIGS, but the present invention is not limited thereto.

<FIG> is a sectional view showing an example of the inventive solar cell. As shown in <FIG>, the inventive solar cell <NUM> is provided with the P-type silicon substrate <NUM> in which one of the main surface is a light-receiving surface and another main surface is a backside. This P-type silicon substrate <NUM> is a gallium-doped silicon substrate provided with the dielectric film (backside dielectric film) <NUM> on the backside. The P-type silicon substrate <NUM> also has the N-conductivity type layer <NUM> in at least a part of the light-receiving surface.

The resistivity of the gallium-doped P-type silicon substrate <NUM> is not particularly restricted, but it can be in a range of <NUM> to <NUM>Ω·cm, for example. The thickness of the P-type silicon substrate <NUM> is not particularly restricted, and can be a thickness of <NUM> to <NUM>, for example. The shape and area of the main surface of the P-type silicon substrate <NUM> is not particularly restricted.

As shown in <FIG>, the backside is generally provided with the back surface electrode <NUM> thereon. The back surface electrode <NUM> can be joined to the backside of the P-type silicon substrate <NUM> by locally opening the backside dielectric film <NUM> as shown in <FIG>. The N-conductivity type layer <NUM> is generally provided with the light-receiving surface electrode <NUM> thereon. The light-receiving surface can also be provided with the light-receiving surface dielectric film <NUM>, which acts as an anti-reflection film, etc. On the contact area where the back surface electrode <NUM> is in contact with the P-type silicon substrate <NUM>, the BSF layer <NUM> can be installed. In this case, the solar cell has a PERL structure. It is also possible to form a solar cell having a PERC structure without providing the BSF layer <NUM>.

Herein, the solar cell having a PERC structure means a solar cell provided with a surface passivation layer formed on the backside of the substrate, and having local contact areas where the P-type silicon substrate is in contact with the back surface electrode. The solar cell having a PERL structure means a solar cell where the P-type dopant concentration on the contact areas is higher than that on areas other than the contact area. In these cases, the area where the back surface electrode <NUM> is in direct contact with the P-type silicon substrate <NUM> may have a pitch of <NUM> or more and <NUM> or less, for example.

As described above, the dielectric film on the light-receiving surface can act as an anti-reflection film The dielectric film on the light-receiving surface can also act as a passivation film or a protective film. The dielectric film on the backside can act as a passivation film or a protective film. For these dielectric films, it is possible to use an SiNx film (a silicon nitride film), an SiO<NUM> film, etc., which can be formed by using a plasma CVD equipment; it is also possible to use a thermal oxide film. As the anti-reflection film, a dielectric film with the film thickness of <NUM> to <NUM> is suitable, showing the maximum effect to reduce the reflectance.

In the present invention, the P-type silicon substrate <NUM> is a silicon substrate doped with gallium. A group III element (an element of group <NUM>) is diffused on the backside of the P-type silicon substrate <NUM>. In <FIG>, the layer in which a group III element is diffused is shown by the reference number <NUM>.

Illustrative examples of the N-type dopant contained in the N-conductivity type layer <NUM> include P (phosphorus), Sb (antimony), As (arsenic), and Bi (bismuth).

The concentration of the group III element at the diffused surface in the backside is <NUM>×<NUM><NUM> atom/cm<NUM> or more and <NUM>×<NUM><NUM> atom/cm<NUM> or less. The diffusion surface concentration of <NUM>×<NUM><NUM> atom/cm<NUM> or more can sufficiently eliminate depletion of the P-type dopant concentration in the backside. The diffusion surface concentration of <NUM>×<NUM><NUM> atom/cm<NUM> or less can eliminate degradation of the cell characteristics without decrease in the voltage and the conversion efficiency. Herein, the diffused surface concentration means a concentration of the group III element on the backside which is additionally doped, and does not include a concentration of gallium that is originally contained. This condition of the diffused surface concentration may be satisfied in the prescribed thickness at the side of back surface. The prescribed thickness can be <NUM>. It is preferable to meet this prescription to the depth of <NUM>.

The diffusion depth of the group III element in the backside is not particularly restricted. The diffusion depth can be in a range of <NUM> to <NUM>, for example.

The area for diffusing the group III element is not particularly restricted. It is desirable, however, to diffuse the group III element over the whole area of the backside in order to sufficiently eliminate depletion of the P-type dopant concentration in the backside.

The concentration of N-type dopant in the N-conductivity type layer <NUM> is not particularly restricted. This concentration can be <NUM>×<NUM><NUM> atom/cm<NUM> or more and <NUM>×<NUM><NUM> atom/cm<NUM> or less, for example. The N-conductivity type layer <NUM> can be formed on the whole area of the light-receiving surface. The shape of the N-conductivity type layer <NUM> can be appropriately altered in accordance with a shape of the light-receiving surface electrode <NUM>.

Then, the inventive method for manufacturing a solar cell is described with reference to <FIG> is a flow diagram showing an example of the inventive method for manufacturing a solar cell. The method described below is a typical example, and the present invention is not restricted thereto. First, as shown in <FIG>, a silicon substrate uniformly doped with gallium is prepared for the P-type silicon substrate in which one main surface is a light-receiving surface and another main surface is a backside. It is to be noted that the silicon substrate uniformly doped with gallium means a silicon substrate that is doped with gallium of a P-type dopant uniformly over the whole region of the substrate (in the thickness direction and the length direction) such as a substrate sliced from a silicon single crystal grown by a CZ method. It may have a slight inhomogeneous concentration distribution that is not intentionally caused by segregation, etc..

The silicon single crystal from which the gallium-doped substrate is sliced can be produced by a CZ method, for example, as described above. In this case, gallium and a polycrystalline silicon may be introduced into a crucible in a lump to form a raw material melt. It is desirable to produce dopant by pulverizing a silicon single crystal doped with higher concentration of gallium, and then to adjust the concentration by introducing the dopant into melted polycrystalline silicon so as to have a desired concentration, since it is necessary to precisely adjust the concentration, particularly in mass production. The gallium-doped substrate can be obtained by slicing thus obtained gallium-doped silicon single crystal.

Subsequently, slice damages on the surface of the substrate can be removed by etching with a high-concentration alkaline solution such as sodium hydroxide and potassium hydroxide in a concentration of <NUM> to <NUM>%, or mixed acid of hydrofluoric acid and nitric acid, etc. as shown in <FIG>.

Then, the substrate surface can be processed to form micro-roughness called texture as shown in <FIG>. The texture is an effective method to reduce the reflectance of a solar cell. The texture can be produced by immersing the substrate in heated alkaline solution (concentration: <NUM> to <NUM>%, temperature: <NUM> to <NUM>) such as sodium hydroxide, potassium hydroxide, potassium carbonate, sodium carbonate, and sodium hydrogencarbonate for about <NUM> minutes to <NUM> minutes. In order to form the texture uniformly over the surface, a certain amount of <NUM>-propanol (IPA: isopropyl alcohol) is commonly added to the foregoing solution.

After the damage-etching and texture formation, it is preferable to wash the substrate as shown in <FIG> The cleaning can be performed by using an aqueous acid solution of hydrochloric acid, sulfuric acid, nitric acid, hydrofluoric acid, or mixed solvent thereof; or pure water, for example.

Subsequently, a group III element is diffused to the backside of the gallium-doped substrate as shown in <FIG>. An N-conductivity type layer is also formed in the light-receiving surface of the gallium-doped substrate as shown in <FIG>. The order of the step (e) and the step (f) is not particularly restricted, and it is also possible to perform the step (e) and the step (f) simultaneously as will be described below.

The method for diffusing a group III element in the step (e) and the method for forming an N-conductivity type layer in the step (f) are not particularly restricted. For example, it is possible to use a method to thermally diffuse the dopant. This includes a vapor phase diffusion method in which POCl<NUM> (phosphoryl chloride) or BBr<NUM> (boron tribromide) is introduced into a tube furnace with carrier gas, and diffused; a coating diffusion method in which a phosphorus or boron-containing material is applied onto a substrate, and subjected to thermal treatment. The coating method in the coating diffusion method includes spin-coating method, spray-coating method, ink-jet method, and screen printing method.

In the coating diffusion method, the group III element can be diffused by coating the backside with a material which contains a group III element followed by thermal treatment. The N-conductivity type layer can be formed by coating the light-receiving surface with a material which contains N-type dopant followed by thermal treatment. The material which contains a group III element is preferably applied to the whole area of the backside to sufficiently eliminate depletion of the P-type dopant concentration in the backside.

In this case, it is preferable to perform the step (e) and the step (f) simultaneously, i.e., to perform diffusion of a group III element and forming of an N-conductivity type layer in a thermal treatment at one time Such a method can reduce the number of production steps when introducing a P-type layer into the backside, and can also reduce the cost without having trouble in the process In this way, a P-type layer having a desired surface concentration can be easily introduced into the backside by performing the step (e) and the step (f) simultaneously.

When performing the step (e) and the step (f) simultaneously, a film which contains an N-type dopant is formed at first by applying a material which contains an N-type dopant onto a light-receiving surface, and introducing the substrate into a drying furnace to dry the material. Then, a film which contains a group III element is formed on the backside in a similar manner. By performing thermal treatment subsequently, it is possible to carry out the diffusion of a group III element and the formation of an N-conductivity type layer simultaneously in one thermal treatment. It is also possible to perform one of the diffusion of a group III element and the formation of an N-conductivity type layer by using the coating diffusion method, and to perform the other process by the vapor phase diffusion method.

For the material which contains N-type dopant, it is possible to use a phosphorus diffusion source (a phosphorus diffusion source), which turns to glass by thermal treatment. This phosphorus diffusion source includes any known ones, and can be obtained by mixing P<NUM>O<NUM> pure water, polyvinyl alcohol (PVA), and tetraethyl orthosilicate (TEOS), for example.

For the material which contains a group III element, it is possible to use a boron diffusion source (a boron diffusion source), which turns to glass by thermal treatment. This boron diffusion source includes any known ones, and can be obtained by mixing B<NUM>O<NUM>, pure water, and PVA, for example.

By applying the phosphorus diffusion source onto the light-receiving surface of the substrate, and the boron diffusion source onto the backside, followed by performing the co-diffusion at a phosphorus diffusion temperature, it is possible to form a boron layer having a relatively low surface concentration since a boron atom has smaller diffusion coefficient compared to a phosphorus atom. This makes it possible to reduce the process cost compared to a method in which the boron layer and the phosphorus diffusion layer are formed separately. The phosphorus diffusion temperature is not particularly restricted, but generally in the range of <NUM> to <NUM>. The boron diffusion temperature is generally in the range of <NUM> to <NUM>. These thermal treatments take generally <NUM> to <NUM> minutes, approximately.

The diffusion surface concentration and the diffusion depth of the group III element can be adjusted to an appropriate value in accordance with the purpose by regulating the content of B<NUM>O<NUM> in a boron diffusion source, thermal diffusion temperature, and thermal diffusion time, for example.

Then, as shown in <FIG>, the PN junction is isolated by using a plasma etcher. In this process, samples are stacked so as not to prevent plasma and radical from getting into the light-receiving surface or the backside, and the side faces of the substrate are dry-etched by several microns under this stacked condition. This PN isolation by plasma etching may be performed before removing the boron glass and phosphorus glass or may be performed after the removal. It is also possible to form a trench with laser as an alternative method to the PN isolation.

After the step (e) and the step (f), not a little quantity of glass layer is formed on the surface of the substrate. The glass on the surface is removed by hydrofluoric acid, etc., as shown in <FIG>.

Subsequently, as shown in <FIG>, a dielectric film can be formed on the light-receiving surface of the gallium-doped substrate. For the dielectric film, it is possible to use the same ones described in the items of the solar cell.

Then, as shown in <FIG>, a dielectric film is formed on the backside of the gallium-doped substrate. For the dielectric film, it is possible to use the same ones described in the items of the solar cell. In the inventive method for manufacturing a solar cell, the group III element is diffused in the backside of the substrate in the step (e), which makes it possible to prevent induction of an inversion layer in the surface area of the backside of the substrate when forming a dielectric film that has positive charges such as a silicon nitride film. The steps (i) and (j) may be performed in the opposite order, and may be performed simultaneously.

Subsequently, as shown in <FIG>, the dielectric film on the contact area of a back surface electrode is just removed. The removal of the dielectric film can be performed by using a photo-lithography method, a laser ablation method, and an etching paste, for example. This etching paste contains at least one selected from the group consisting of phosphoric acid, hydrofluoric acid, ammonium fluoride, and ammonium hydrogen fluoride as an etching component together with water, organic solvent, and a viscosity agent, for example. The same structure can also be formed, without intentionally removing the dielectric film, by printing an electrode having a fire-through property, which will be described below, in the foregoing area by screen printing and so on, followed by penetrating the electrode to the dielectric film through firing.

Then, as shown in <FIG>, a paste for a back surface electrode is printed onto the backside of the gallium-doped substrate, followed by drying. For example, a paste in which Al powders are mixed with an organic binder is applied onto the backside of the substrate by screen printing. For the material for the back surface electrode, Ag and so on can also be used.

Subsequently, as shown in <FIG>, a paste for a light-receiving surface electrode is printed onto the light-receiving surface of the gallium-doped substrate, followed by drying. For example, an Ag paste in which Ag powders and glass frit are mixed with an organic binder is applied onto the light-receiving surface of the substrate by screen printing. The step (l) and the step (m) may be performed in the opposite order.

After the foregoing printing of the electrodes, the paste for a light-receiving surface electrode and the paste for a back surface electrode are fired as shown in <FIG>. In this way, the light-receiving surface electrode and the back surface electrode are formed by printing the pastes followed by firing. The firing is generally performed by thermal treatment at a temperature of <NUM> to <NUM> for <NUM> to <NUM> minutes. This thermal treatment makes the Ag powders penetrate to the dielectric film (fire through) on the light-receiving surface side to electrically conduct the light-receiving surface electrode and the gallium-doped substrate. It is also possible to fire back surface electrode and the light-receiving surface electrode separately.

In such a way, the solar cell shown in <FIG> can be manufactured. The inventive method for manufacturing a solar cell mainly features to use a gallium-doped substrate and to diffuse a group III element onto the backside before forming a dielectric film, and can be applied to various methods for manufacturing solar cells.

Hereinafter, the present invention will be specifically described by showing Examples and Comparative Example, but the present invention is not limited these Examples.

First, as-sliced CZ substrate in a <NUM> square with the thickness of <NUM> and substrate resistivity of <NUM>Ω·cm was prepared for a silicon substrate uniformly doped with gallium (<FIG>).

Then, this gallium-doped substrate was subjected to damage etching by immersing into a solution of hydrofluoric acid and nitric acid for <NUM> seconds (<FIG>). This was also subjected to chemical etching for <NUM> minutes by using an aqueous solution with the temperature of <NUM> containing <NUM>% of KOH and <NUM>% of IPA (<FIG>). Subsequently, this was cleaned with deionized water and dried to form texture structures onto the light-receiving surface of the gallium-doped substrate (<FIG>).

Next, a boron-containing film was formed on the whole area of the backside by applying a boron diffusion source which contained boric acid onto the backside by spin-coating method, followed by drying in a drying furnace at <NUM> for about <NUM> minute. Then, the gallium-doped substrate having the boron-containing film formed thereon was introduced into a tube furnace, and subjected to thermal treatment at the temperature of <NUM> for the thermal treatment time of <NUM> minutes to diffuse the group III element to the backside of the gallium-doped substrate (<FIG>). At this process, two pieces of the substrates were set on a slot of a quarts boat with the boron-coated surfaces facing outward so as not to grow boron-diffusion layers on the non-boron-coated faces as possible.

Subsequently, the gallium-doped substrate was subjected to thermal treatment under the atmosphere of phosphoryl chloride at <NUM> for <NUM> minutes to form an N-conductivity type layer in the light-receiving surface (<FIG>). At this process, the diffusion was performed by superposing the boron-diffusion surfaces with each other, which was introduced to a slot of a quartz boat, to prevent phosphorus from diffusing into the boron-diffusion layers as possible.

Then, the PN junction was isolated by using a plasma etcher (<FIG>). Subsequently, diffusion glass remained on the surface of the substrate was removed by immersion in a <NUM>% aqueous hydrofluoric acid solution over <NUM> minutes, followed by rinsing with pure water over <NUM> minutes (<FIG>).

This gallium-doped substrate subjected to diffusion was introduced into an oxidation furnace, and subjected to thermal treatment under an oxygen atmosphere at <NUM> for <NUM> minutes to form oxide layer with each layer thickness of <NUM> on the both surfaces of the substrate as dielectric films. On the light-receiving surface and the backside of the gallium-doped substrate, silicon nitride layers were formed respectively as dielectric films by using a plasma CVD equipment (<FIG>). The dielectric film on the light-receiving surface was set to have a film thickness of <NUM>. The dielectric film on the backside was also set to have a film thickness of <NUM>. At this step, the oxide films were etched with hydrofluoric acid, and the sheet resistivity was measured to be <NUM>Ω/□. The surface concentration was assumed from this value to be about <NUM>×<NUM><NUM> atom/cm<NUM>.

Subsequently, the dielectric film was removed just on the contact area for the electrodes on the backside by using an etching paste (<FIG>).

Then, on the backside of the gallium-doped substrate, an electric conductive paste mainly composed of silver was printed by a screen-printing method, and dried at <NUM> (<FIG> (<NUM>)).

The electric conductive paste mainly composed of silver was also printed onto the light-receiving surface of the gallium-doped substrate by a screen-printing method, and dried at <NUM> (<FIG>).

This substrate coated with the electric conductive paste was introduced into a firing furnace, and the electric conductive paste was fired at the maximum temperature of <NUM> for <NUM> seconds to form a back surface electrode and a light-receiving surface electrode to fabricate the solar cell shown in <FIG>).

The solar cell shown in <FIG> was fabricated by the same processes as in Example <NUM> except for processing the steps shown in (e) and (f) of <FIG> simultaneously. That is, in this process, a boron-containing film was formed on the whole area of the backside by applying a boron diffusing source containing boric acid onto the back surface by a spin-coating method, followed by drying on a hot plate at <NUM> for about <NUM> minute. Subsequently, a phosphorus-containing film was formed on the whole area of the front surface by applying a phosphorus diffusing source containing phosphoric acid by a spin-coating method, followed by drying on a hot plate at <NUM> for about <NUM> minute. This substrate was introduced into a tube furnace, and subjected to thermal treatment at <NUM> for <NUM> minutes to form an N-conductivity type layer on the front side and a P-conductivity type layer on the backside simultaneously At this process, the diffusion was performed by superposing the boron-diffusion surfaces with each other or the phosphorus-diffusion surfaces with each other, which was introduced to a slot of a quartz boat, to prevent mutual diffusion of boron and phosphorus as possible.

The diffusion profile of Example <NUM> by secondary ion mass spectrometry (SIMS) is shown in <FIG>. This was measured on the substrate after the step (h). As revealed from <FIG>, boron was diffused in the backside, and phosphorus was diffused in the light-receiving surface of the gallium-doped substrate as had been intended.

The solar cell shown in <FIG> was fabricated by the same processing as in Examples except for skipping the step (e) in <FIG> (the step for diffusing a group III element by forming a boron-containing film on the backside of a gallium-doped substrate).

On <NUM> pieces of solar cells thus fabricated (Example <NUM>: <NUM> pieces, Example <NUM>: <NUM> pieces, Comparative Example: <NUM> pieces), evaluations (inspections of current-voltage characteristics) were performed with a solar simulator (in an atmosphere of <NUM>, irradiation intensity: <NUM> kW/m<NUM>, spectrum: AM <NUM> global). The results of Examples <NUM> and <NUM> and Comparative Example were shown in Table <NUM>. The conversion efficiencies and so on in Table <NUM> are average values of each <NUM> pieces of solar cells of Examples <NUM> and <NUM> and Comparative Example.

As shown in Table <NUM>, Examples <NUM> and <NUM>, in which a group III element was diffused in the backside of each gallium-doped substrate, showed good results of the short-circuit current density, open circuit voltage, fill factor, and conversion efficiency. On the other hand, Comparative Example, in which a group III element was not diffused in the backside of the substrate, formed the inversion layer <NUM> in the backside of the substrate as shown in <FIG>, and degrade the results of the short-circuit current density, etc..

The internal quantum efficiencies of Example <NUM> and Comparative Example are shown in <FIG>. The internal quantum efficiencies in <FIG> were measured by spectral response measurement equipment. As shown in <FIG>, Example <NUM> showed better internal quantum efficiencies compared to Comparative Example, particularly at wavelengths in the range of <NUM> to <NUM>. It is to be noted that the internal quantum efficiencies in Example <NUM> were almost the same as the internal quantum efficiencies in Example <NUM>.

Claim 1:
A solar cell (<NUM>) comprising a P-type silicon substrate (<NUM>) in which one main surface is a light-receiving surface and another main surface is a backside, a dielectric film having positive charge on the backside, and an N-conductivity type layer (<NUM>) in at least a part of the light-receiving surface of the P-type silicon substrate,
wherein the P-type silicon substrate (<NUM>) is a silicon substrate doped with gallium,
characterized in that
the backside of the P-type silicon substrate contains diffused boron as a diffused group III element over the whole area of the backside,
wherein the concentration of the group III element at the diffusion surface in the backside is in a range of <NUM>×<NUM><NUM> atom/cm<NUM> or more and <NUM>×<NUM><NUM> atom/cm<NUM> or less over the whole area of the backside.