This application claims the priority benefit of Taiwan application serial no. 98108931, filed on Mar. 19, 2009. The entirety of the above-mentioned patent application is hereby incorporated by reference herein and made a part of this specification.
1. Field of the Invention
The present invention relates to a method of fabricating a solar cell. More particularly, the present invention relates to a method of fabricating a solar cell capable of improving photoelectric conversion efficiency.
2. Description of Related Art
As the petrochemical energy source encounters the pollution and energy shortage problems, the solar energy attracts most of the attentions. Recently, it becomes a quite important research issue to directly convert a solar cell into electric energy. Solar cell is a very promising clean energy source which can generate electricity directly from sunlight, and carbon dioxide, nitride gas or pernicious gases are not generated during generating electric energy, such that the environment is not polluted.
Silicon-based solar cell is a common solar cell in the industry. The working principle of the silicon-base solar cell is that some impurities are added into a semiconductor material (silicon) with high purity, such that the semiconductor material has different features, so as to form a p-type semiconductor and an n-type semiconductor, and to joint the p-type and n-type semiconductors, thereby forming a p-n junction. The p-n junction is formed by positive donor ions and negative acceptor ions, and a built-in potential exists in a region where the positive and negative ions are located. The built-in potential may drive away movable carriers in the region, so that the region is called a depletion region. When the sunlight is irradiated onto a semiconductor with a p-n structure, the energy provided by photons excites electrons in the semiconductor, so as to generate electron-hole pairs. The electrons and holes are both affected by the built-in potential, the holes move towards a direction of the electric field, whereas the electrons move towards an opposite direction. If the solar cell is connected to a load through a wire to form a loop, the current flows through the load, which is the principle for the solar cell to generate electricity.
A backside point contact process is usually performed in the formation of the silicon-based solar cell, which forming a passivation layer on the backside of the solar cell so as to cause back surface field (BSF) effect. Thereby, the carriers collected in the solar cell are increased and the photons not absorbed can be recovered so as to improve the photoelectric conversion efficiency. However, conventionally when forming an n-type layer (n+ layer) on the front surface of the p-type semiconductor substrate with a thermal diffusion process, an n+ layer is also formed on the back surface of the p-type semiconductor substrate. The n+ layer formed on the back surface of the p-type semiconductor substrate decreases BSF effect of the backside point contact electrode. In addition, the sheet-resistance of the back surface of the p-type semiconductor substrate is not uniform because of the formation of the n+ layer thereon, such that the photoelectric conversion efficiency of the solar cell is not good.
Accordingly, the present invention is directed to a method of fabricating a solar cell capable of improving photoelectric conversion efficiency.
The present invention provides to a method of fabricating a solar cell. A semiconductor substrate having a front surface and a back surface is provided. A dopant material layer is deposited on the front surface of the semiconductor substrate, and an over-depositing dopant layer is also formed on the back surface of the semiconductor substrate. In particular, dopants of the dopant material layer diffuse into the front surface of the semiconductor substrate to form a doping layer, and dopants of the over-depositing dopant layer diffuse into the back surface of the semiconductor substrate to form a doping residual layer during depositing the dopant material layer. Next, the dopant material layer and the over-depositing dopant layer are removed. After that, an anti-reflective layer is formed on the doping layer on the semiconductor substrate. After the doping residual layer on the semiconductor substrate is removed to expose the back surface of the semiconductor substrate, a passivation layer is formed on the exposed back surface of the semiconductor substrate. Then, a first electrode is formed on the anti-reflective layer and a second electrode is formed on the passivation layer.
In light of the foregoing, the doping residual layer on the back surface of the semiconductor is removed before forming the passivation layer on the back surface of the semiconductor. Thereby, it is benefit for the second electrode to generate BSF effect, and the sheet-resistance of the back surface of the semiconductor is uniform such that the photoelectric conversion efficiency of the solar cell is improved.
In order to make the aforementioned and other features and advantages of the present invention more comprehensible, several embodiments accompanied with figures are described in detail below.
The accompanying drawings constituting a part of this specification are incorporated herein to provide a further understanding of the invention. Here, the drawings illustrate embodiments of the invention and, together with the description, serve to explain the principles of the invention.
Next, a dopant diffusion process to the semiconductor substrate 110 is performed. In the embodiment, the dopant diffusion process to the semiconductor substrate 110 is performed by disposing the semiconductor substrate 110 in a form of standing inside a depositing chamber, and then depositing a dopant material layer on the surfaces of the semiconductor substrate 110, wherein dopants of the dopant material layer diffuse into the semiconductor substrate 110 through the thermal effect of the depositing process.
In details, as shown in
In particular, when performing said depositing process, dopants of the dopant material layer 121a diffuse into the front surface 110a of the semiconductor substrate 110 because of the high temperature of the depositing chamber, so as to form a doping layer 120a. In the embodiment, the doping layer 120a is an n-type (n+) doping layer, and thus a p-n junction is formed between the doping layer 120 and the semiconductor substrate 110. However, during said depositing process, dopants of the over-depositing dopant layer 121b also diffuse into the back surface 110b of the semiconductor substrate 110 to form a doping residual layer 120b. The doping residual layer 120b is an n+ residual layer having n-type dopants (such as phosphorous ions) therein.
After the dopant diffusion process is performed, the dopant material layer 121a and the over-depositing dopant layer 121b on the semiconductor substrate 110 are removed, as shown in
However, in the meanwhile, the non-uniform doping residual layer 120b is still on the back surface 110b of the semiconductor substrate 110.
Referring to
In the above-mentioned embodiment, the plasma treatment with hydrogen plasma is used to remove the doping residual layer 120b on the semiconductor substrate 110, but the present invention does not limit thereto. According to another embodiment, the plasma treatment with argon plasma can also be used to remove the doping residual layer 120b on the semiconductor substrate 110. In addition to the plasma treatment, a wet etching process can also be used to remove the doping residual layer 120b on the semiconductor substrate 110. The wet etching process comprises using an etchant having hydrofluoric acid, for example.
Referring to
Thereafter, a first electrode 150 and a second electrode 160 are respectively formed on the anti-reflection layer 130 and the passivation layer 140, as shown in
It is noted that the solar cell of the embodiments is formed by the backside point contact process, and thus the second electrode 160 generates back surface field (BSF) effect. Thereby, the carriers collected in the solar cell are increased and the photons not absorbed can be recovered so as to improve photoelectric conversion efficiency. However, if the doping residual layer 120b (as shown in
The method of fabricating the solar cell of the Example comprises removing the doping residual layer on the back surface of the semiconductor substrate with hydrogen treatment before the passivation layer is formed on the back surface of the semiconductor substrate. The detailed process steps are as shown in
The process steps and the materials for fabricating the solar cell in the Comparison Example are similar to the above Example, and the difference therebetween is that the back surface of the semiconductor substrate is not treated with any process before forming the passivation layer on the back surface of the semiconductor substrate, and thus a doping residual layer is remained on the back surface of the semiconductor substrate.
Electrical properties of the solar cells of the Example and the Comparison Example are measured under the same measuring condition and shown in Table 1.
As Table 1 shown, the open-circuit voltage of the solar cell in Example is 0.622V, while the open-circuit voltage of the solar cell in Comparison Example is 0.613V; and the short-circuit current density of the solar cell in Example is raised to 36.122 mA/cm2 from 35.78 mA/cm2 because of the passivation effect. In addition, the filling factor and the photoelectric conversion efficiency of the solar cell in Example are better than that of the solar cell in Comparison Example.
In the method of fabricating the solar cell of the present invention, the doping residual layer on the back surface of the semiconductor substrate is removed with plasma treatment or etching process before the passivation layer is formed. It is benefit for the solar cell to generate better BSF effect. In addition, the solar cell formed by the method comprising removing the doping residual layer on the back surface of the semiconductor substrate has uniform sheet resistance, and thus the photoelectric conversion efficiency of the solar cell is increased. In particular, if the doping residual layer is removed with hydrogen plasma, hydrogen ions are also implanted into the back surface of the semiconductor substrate at the same time. That is, the removal of the doping residual layer and the bulk passoivation effect are achieved at the same time, and thus the fabricating time and cost are reduced.
It will be apparent to those skilled in the art that various modifications and variations can be made to the structure of the present invention without departing from the scope or spirit of the invention. In view of the foregoing, it is intended that the present invention cover modifications and variations of this invention provided they fall within the scope of the following claims and their equivalents.
Number | Date | Country | Kind |
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98108931 | Mar 2009 | TW | national |