CN105140334B - Solar cell selective doping method based on counter diffusion - Google Patents
Solar cell selective doping method based on counter diffusion Download PDFInfo
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- 238000009792 diffusion process Methods 0.000 title claims abstract description 61
- 238000000034 method Methods 0.000 title claims abstract description 42
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 claims abstract description 56
- 229910052710 silicon Inorganic materials 0.000 claims abstract description 56
- 239000010703 silicon Substances 0.000 claims abstract description 56
- 229910021417 amorphous silicon Inorganic materials 0.000 claims abstract description 21
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 claims abstract description 12
- 229910052760 oxygen Inorganic materials 0.000 claims abstract description 12
- 239000001301 oxygen Substances 0.000 claims abstract description 12
- KRHYYFGTRYWZRS-UHFFFAOYSA-N Fluorane Chemical compound F KRHYYFGTRYWZRS-UHFFFAOYSA-N 0.000 claims description 12
- ZOXJGFHDIHLPTG-UHFFFAOYSA-N Boron Chemical compound [B] ZOXJGFHDIHLPTG-UHFFFAOYSA-N 0.000 claims description 10
- 229910052796 boron Inorganic materials 0.000 claims description 10
- 229910021421 monocrystalline silicon Inorganic materials 0.000 claims description 7
- 238000000151 deposition Methods 0.000 claims description 4
- 238000007650 screen-printing Methods 0.000 claims description 4
- 239000000872 buffer Substances 0.000 claims description 3
- 239000007853 buffer solution Substances 0.000 claims description 3
- 239000005388 borosilicate glass Substances 0.000 claims description 2
- 230000000717 retained effect Effects 0.000 claims description 2
- 239000012535 impurity Substances 0.000 abstract description 22
- 230000000694 effects Effects 0.000 abstract description 2
- 230000001568 sexual effect Effects 0.000 abstract 1
- OAICVXFJPJFONN-UHFFFAOYSA-N Phosphorus Chemical compound [P] OAICVXFJPJFONN-UHFFFAOYSA-N 0.000 description 11
- 229910052698 phosphorus Inorganic materials 0.000 description 11
- 239000011574 phosphorus Substances 0.000 description 11
- 239000005360 phosphosilicate glass Substances 0.000 description 7
- 238000004088 simulation Methods 0.000 description 7
- 238000004519 manufacturing process Methods 0.000 description 6
- 238000010586 diagram Methods 0.000 description 4
- 238000009826 distribution Methods 0.000 description 3
- 230000003647 oxidation Effects 0.000 description 3
- 238000007254 oxidation reaction Methods 0.000 description 3
- 229910019142 PO4 Inorganic materials 0.000 description 2
- 238000006243 chemical reaction Methods 0.000 description 2
- 230000007547 defect Effects 0.000 description 2
- NBIIXXVUZAFLBC-UHFFFAOYSA-K phosphate Chemical compound [O-]P([O-])([O-])=O NBIIXXVUZAFLBC-UHFFFAOYSA-K 0.000 description 2
- 239000010452 phosphate Substances 0.000 description 2
- 238000000206 photolithography Methods 0.000 description 2
- 239000002002 slurry Substances 0.000 description 2
- 230000003595 spectral effect Effects 0.000 description 2
- 150000001875 compounds Chemical class 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 230000008021 deposition Effects 0.000 description 1
- 230000007613 environmental effect Effects 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- 230000000873 masking effect Effects 0.000 description 1
- 238000003672 processing method Methods 0.000 description 1
- 238000007613 slurry method Methods 0.000 description 1
- 239000000243 solution Substances 0.000 description 1
- 239000000758 substrate Substances 0.000 description 1
- 230000009466 transformation Effects 0.000 description 1
- 238000009279 wet oxidation reaction Methods 0.000 description 1
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- H10F—INORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
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- H01L21/22—Diffusion of impurity materials, e.g. doping materials, electrode materials, into or out of a semiconductor body, or between semiconductor regions; Interactions between two or more impurities; Redistribution of impurities
- H01L21/225—Diffusion of impurity materials, e.g. doping materials, electrode materials, into or out of a semiconductor body, or between semiconductor regions; Interactions between two or more impurities; Redistribution of impurities using diffusion into or out of a solid from or into a solid phase, e.g. a doped oxide layer
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- Y02E10/50—Photovoltaic [PV] energy
- Y02E10/547—Monocrystalline silicon PV cells
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- 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
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Abstract
本发明涉及一种基于逆扩散的太阳能电池选择性掺杂方法,步骤如下:将硅片置于有氧环境下进行高温扩散形成PN结,同时硅片上表面被氧化;除去硅片顶电极区以外的氧化层;在硅片上表面淀积本征非晶硅层;将硅片置于湿氧环境中进行高温扩散,使非顶电极区的掺杂元素逆向扩散入非晶硅层,顶电极区氧化层中的掺杂元素向顶电极区扩散,同时非晶硅层及非顶电极区的硅片表面被氧化形成氧化层;去除硅片表面的氧化层,完成太阳能电池的逆扩散选择性掺杂。本发明采用逆扩散的方法,通过非晶硅吸收非顶电极区的杂质,使非顶电极区的掺杂浓度降低,同时顶电极区进行了二次掺杂,导致顶电极区与非顶电极区的掺杂浓度差进一步增大,提高了选择性掺杂的效果。
The invention relates to a method for selective doping of solar cells based on reverse diffusion. The steps are as follows: placing a silicon wafer in an oxygen environment for high-temperature diffusion to form a PN junction, while the upper surface of the silicon wafer is oxidized; removing the top electrode region of the silicon wafer Deposit an intrinsic amorphous silicon layer on the upper surface of the silicon wafer; place the silicon wafer in a wet oxygen environment for high-temperature diffusion, so that the doping elements in the non-top electrode area diffuse reversely into the amorphous silicon layer, and the top The doping element in the oxide layer of the electrode area diffuses to the top electrode area, and at the same time, the surface of the silicon wafer in the amorphous silicon layer and the non-top electrode area is oxidized to form an oxide layer; the oxide layer on the surface of the silicon wafer is removed to complete the reverse diffusion selection of the solar cell Sexual doping. The present invention adopts the method of reverse diffusion, and absorbs the impurities in the non-top electrode region through amorphous silicon, so that the doping concentration of the non-top electrode region is reduced, and at the same time, the top electrode region is doped twice, resulting in the difference between the top electrode region and the non-top electrode region. The doping concentration difference between regions is further increased, which improves the effect of selective doping.
Description
技术领域technical field
本发明涉及一种基于逆扩散的太阳能电池选择性掺杂方法,属于太阳能电池制造技术领域。The invention relates to a method for selective doping of solar cells based on reverse diffusion, and belongs to the technical field of solar cell manufacturing.
背景技术Background technique
随着人们环保意识的提高,对于清洁能源的需求日益旺盛。在人们研究的新型清洁能源中,太阳能作为一种不受地域限制的清洁能源成为了未来新能源发展的主要方向。太阳能电池是人们利用太阳的光能转换为电能的主要装置。但是,目前太阳能电池的转换效率还不能达到人们的要求。提高太阳能电池的转换效率,降低太阳能电池的制造成本成为了人们研究的热点。With the improvement of people's awareness of environmental protection, the demand for clean energy is increasing. Among the new clean energy researched by people, solar energy, as a clean energy that is not subject to geographical restrictions, has become the main direction of new energy development in the future. Solar cells are the main devices that people use the sun's light energy to convert into electrical energy. However, the conversion efficiency of solar cells cannot meet people's requirements at present. Improving the conversion efficiency of solar cells and reducing the manufacturing cost of solar cells has become a research hotspot.
选择性掺杂太阳能电池是一种有效的低成本高效率的太阳能电池。选择性掺杂太阳能电池的结构特点在于在太阳能电池的上电极覆盖区域进行重掺杂降低电池的接触电阻,同时在非顶电极区进行轻掺杂,提高电池的光谱响应和降低电池中光生载流子的复合。目前进行太阳能电池选择性掺杂的方法主要有:两步扩散法、丝网印刷磷浆法、扩散掩膜法等。其中,两步扩散法是先对顶电极区重扩散,再对整个发射区轻扩散,其优点为制备工艺简单易行,但是,由于顶电极区先进行了扩散,杂质的二次分布较难控制;丝网磷浆法是用丝网在局部印刷高浓度磷浆,通过其扩散与挥发,一次扩散就能使顶电极区形成重掺杂,其他区域形成轻掺杂,但由于利用了局部的磷浆作为扩散源,必然导致表面扩散的不均匀性,这会降低电池的效率。扩散掩膜法就是先轻掺杂,再进行激光或者光刻掩膜,然后再对顶电极区进行二次重掺杂,该方法由于先进行了轻掺杂,降低了顶电极区进行选择性掺杂时与衬底的杂质浓度差,可以较好的控制电池的选择性掺杂区域,但需要用激光或光刻的方法,提高了成本,降低了生产效率。Selectively doped solar cells are an effective low-cost and high-efficiency solar cell. The structural feature of selectively doped solar cells is that heavy doping is carried out on the top electrode coverage area of the solar cell to reduce the contact resistance of the cell, while light doping is carried out on the non-top electrode area to improve the spectral response of the cell and reduce the photogenerated load in the cell. compound flow. At present, the methods for selective doping of solar cells mainly include: two-step diffusion method, screen printing phosphatization method, diffusion mask method, etc. Among them, the two-step diffusion method is to firstly diffuse the top electrode area, and then lightly diffuse the entire emission area. Control; the screen phosphate slurry method is to use a screen to print a high-concentration phosphate slurry locally. Through its diffusion and volatilization, one diffusion can make the top electrode area form a heavy doping, and other areas form a light doping. However, due to the use of local Phosphorus slurry as a diffusion source will inevitably lead to inhomogeneity of surface diffusion, which will reduce the efficiency of the cell. The diffusion mask method is to lightly dope first, then perform laser or photolithography masking, and then carry out secondary heavy doping on the top electrode area. This method reduces the selectivity of the top electrode area due to light doping first. The difference in impurity concentration between doping and the substrate can better control the selective doping area of the cell, but laser or photolithography is required, which increases the cost and reduces the production efficiency.
综上所述,目前主要的选择性掺杂的方法都存在一定的缺陷,因此,必须寻找一种新型的选择性掺杂的太阳能电池生产工艺。To sum up, the current main selective doping methods all have certain defects. Therefore, it is necessary to find a new selective doping solar cell production process.
发明内容Contents of the invention
本发明的目的在于:克服上述现有技术的缺陷,提出一种基于逆扩散的太阳能电池选择性掺杂方法,工艺实现简单,生产成本低,获得的太阳能电池性能良好。The object of the present invention is to overcome the above-mentioned defects in the prior art, and propose a method for selective doping of solar cells based on reverse diffusion, which has simple process implementation, low production cost, and good performance of the obtained solar cells.
为了达到上述目的,本发明提出的基于逆扩散的太阳能电池选择性掺杂方法,包括如下步骤:In order to achieve the above object, the solar cell selective doping method based on reverse diffusion proposed by the present invention comprises the following steps:
第1步、将硅片置于湿氧环境下进行高温扩散,形成PN结,同时硅片上表面生成氧化层,该氧化层中含有高浓度的掺杂元素;Step 1. Place the silicon wafer in a humid oxygen environment for high-temperature diffusion to form a PN junction, and at the same time, an oxide layer is formed on the upper surface of the silicon wafer, which contains high-concentration doping elements;
第2步、除去硅片上表面顶电极区以外的氧化层;Step 2, removing the oxide layer other than the top electrode region on the upper surface of the silicon wafer;
第3步、在硅片上表面淀积本征非晶硅层;Step 3, depositing an intrinsic amorphous silicon layer on the upper surface of the silicon wafer;
第4步、将硅片置于湿氧环境中进行高温扩散,使硅片非顶电极区的掺杂元素扩散入非晶硅层,降低硅片非顶电极区掺杂元素浓度,实现掺杂元素的逆向扩散;顶电极区氧化层中的掺杂元素向顶电极区扩散,实现顶电极区的重掺杂,同时非晶硅层及非顶电极区的硅片表面被氧化形成氧化层;Step 4, place the silicon wafer in a humid oxygen environment for high temperature diffusion, so that the doping elements in the non-top electrode area of the silicon wafer can diffuse into the amorphous silicon layer, reduce the concentration of doping elements in the non-top electrode area of the silicon wafer, and achieve doping Reverse diffusion of elements; the doping elements in the oxide layer of the top electrode area diffuse to the top electrode area to achieve heavy doping of the top electrode area, and at the same time, the surface of the amorphous silicon layer and the silicon wafer in the non-top electrode area is oxidized to form an oxide layer;
第5步、去除硅片表面的氧化层,完成太阳能电池的逆扩散选择性掺杂。In step 5, the oxide layer on the surface of the silicon wafer is removed, and the reverse diffusion selective doping of the solar cell is completed.
本发明提出了一种逆扩散的选择性掺杂方法,通过非晶硅吸收非电极区的杂质,使非电极区的掺杂浓度降低,同时电极区进行了二次掺杂,导致电极区与非电极区的掺杂浓度差进一步增大,提高了选择性掺杂的效果;并且在逆扩散工艺进行时,由于受到氧化层的保护,电极区的硅片表面氧化程度低,而非电极区的硅表面则被氧化形成氧化层,从而在去除氧化层后,电极区呈现一定程度外凸,有利于后续电极的定位。The present invention proposes a selective doping method of reverse diffusion, which absorbs impurities in the non-electrode region through amorphous silicon, so that the doping concentration of the non-electrode region is reduced, and at the same time, the electrode region is doped twice, causing the electrode region to be separated from the electrode region. The doping concentration difference in the non-electrode area is further increased, which improves the effect of selective doping; and when the reverse diffusion process is carried out, due to the protection of the oxide layer, the oxidation degree of the silicon wafer surface in the electrode area is low, and the oxidation degree of the silicon wafer in the non-electrode area is low. The silicon surface is oxidized to form an oxide layer, so that after the oxide layer is removed, the electrode area is convex to a certain extent, which is conducive to the positioning of subsequent electrodes.
本发明进一步的改进在于:The further improvement of the present invention is:
1、所述硅片为P型单晶硅,第1步中,首先将硅片置于湿氧环境下进行高温预扩散,使磷元素扩散入硅片形成PN结,同时硅片表面被氧化形成磷硅玻璃。1. The silicon wafer is P-type single crystal silicon. In the first step, the silicon wafer is first placed in a wet oxygen environment for high-temperature pre-diffusion, so that phosphorus element diffuses into the silicon wafer to form a PN junction, and the surface of the silicon wafer is oxidized at the same time Phosphosilicate glass is formed.
2、第1步中,氧化层厚度约为0.05微米,氧化层中磷元素的浓度约为1e19/cm3,高温预扩散的工艺温度为1000℃,持续时间为30分钟。2. In step 1, the thickness of the oxide layer is about 0.05 microns, the concentration of phosphorus in the oxide layer is about 1e19/cm 3 , the process temperature of high temperature pre-diffusion is 1000°C, and the duration is 30 minutes.
3、所述硅片为N型单晶硅,第1步中,首先将硅片置于有湿氧环境下进行高温预扩散,使硼元素扩散入硅片形成PN结,同时硅片表面被氧化形成硼硅玻璃。3. The silicon wafer is N-type single crystal silicon. In the first step, the silicon wafer is first placed in a humid oxygen environment for high-temperature pre-diffusion, so that boron element diffuses into the silicon wafer to form a PN junction, and at the same time, the surface of the silicon wafer is covered with Oxidation forms borosilicate glass.
4、第1步中,氧化层厚度约为0.05微米,硅薄层中硼元素的浓度约为1e19/cm3,高温预扩散的工艺温度为1000℃,持续时间为30分钟。4. In step 1, the thickness of the oxide layer is about 0.05 microns, the concentration of boron in the silicon thin layer is about 1e19/cm 3 , the process temperature of high temperature pre-diffusion is 1000°C, and the duration is 30 minutes.
5、所述第2步中,采用丝网印刷的方法保留顶电极区的氧化层,将硅片上其它区域的氧化层利用氢氟酸缓冲液去除掉。5. In the second step, the oxide layer in the top electrode area is retained by screen printing, and the oxide layer in other areas on the silicon wafer is removed by hydrofluoric acid buffer.
6、所述第3步中,淀积的本征非晶硅层厚度约为40-50nm。6. In the third step, the thickness of the deposited intrinsic amorphous silicon layer is about 40-50 nm.
7、所述第4步中,高温扩散的工艺温度为900℃-1100℃,持续时间为30-2分钟。7. In the fourth step, the process temperature of high-temperature diffusion is 900°C-1100°C, and the duration is 30-2 minutes.
8、所述第5步中,采用氢氟酸缓冲液去除硅片表面的氧化层。8. In the fifth step, a hydrofluoric acid buffer solution is used to remove the oxide layer on the surface of the silicon wafer.
本发明该工艺方法的特点在于:The feature of this processing method of the present invention is:
1、不同于传统的选择性掺杂工艺,采用的是先全片重掺杂,后逆向扩散受光面杂质,降低受光面的杂质掺杂浓度的方法。1. Different from the traditional selective doping process, the whole chip is heavily doped first, and then the impurities on the light-receiving surface are diffused backwards to reduce the doping concentration of impurities on the light-receiving surface.
2、应用本征非晶硅薄膜吸收电池表面已掺杂区域的杂质,使得电池表面不会被其他不同元素污染。2. The intrinsic amorphous silicon film is used to absorb the impurities in the doped area on the surface of the battery, so that the surface of the battery will not be polluted by other different elements.
3、保留电极区的磷硅玻璃作为高温杂质逆向扩散工艺的电极杂质保护层,保证了电极区的重掺杂。3. The phosphosilicate glass in the electrode area is reserved as the electrode impurity protection layer in the high-temperature impurity reverse diffusion process, which ensures the heavy doping of the electrode area.
4、在杂质逆向扩散过程中采用湿法氧化的方法,使非晶硅层氧化,减少了去除非晶硅薄膜的步骤,提高了生产效率。4. The method of wet oxidation is adopted in the impurity reverse diffusion process to oxidize the amorphous silicon layer, which reduces the steps of removing the amorphous silicon film and improves the production efficiency.
附图说明Description of drawings
下面结合附图对本发明作进一步的说明。The present invention will be further described below in conjunction with the accompanying drawings.
图1是本发明方法的工艺流程示意图。Fig. 1 is a schematic process flow diagram of the method of the present invention.
图2是本发明实施例一方法所得到的硅片杂质分布仿真示意图。FIG. 2 is a schematic diagram of a simulation of impurity distribution on a silicon wafer obtained by a method according to Embodiment 1 of the present invention.
图3是本发明实施例二方法所得到的硅片杂质分布仿真示意图。FIG. 3 is a schematic diagram of a simulation of impurity distribution on a silicon wafer obtained by the method in Embodiment 2 of the present invention.
图4是本发明实施例三方法所得到的硅片杂质分布仿真示意图。FIG. 4 is a schematic diagram of a simulation of impurity distribution on a silicon wafer obtained by the method of Embodiment 3 of the present invention.
具体实施方式detailed description
下面结合附图和具体实施例对本发明做进一步说明。The present invention will be further described below in conjunction with the accompanying drawings and specific embodiments.
实施例一Embodiment one
如图1所示为本发明基于逆扩散的太阳能电池选择性掺杂方法的流程示意图,具体包括如下步骤:As shown in Figure 1, it is a schematic flow chart of the method for selective doping of solar cells based on reverse diffusion in the present invention, which specifically includes the following steps:
1a、将P型单晶硅片置于湿氧环境下进行高温预扩散,使磷元素扩散入硅片形成PN结,同时硅片表面形成厚度约为0.05微米的磷硅玻璃层1,磷硅玻璃层1中磷元素的浓度约为1e19/cm3;高温预扩散的工艺温度为1000℃,持续时间为30分钟;1a. Place the P-type monocrystalline silicon wafer in a humid oxygen environment for high-temperature pre-diffusion, so that phosphorus element diffuses into the silicon wafer to form a PN junction. At the same time, a phosphosilicate glass layer 1 with a thickness of about 0.05 microns is formed on the silicon wafer surface. The concentration of phosphorus in the glass layer 1 is about 1e19/cm 3 ; the process temperature of high temperature pre-diffusion is 1000°C, and the duration is 30 minutes;
2a、采用丝网印刷的方法保留顶电极区的磷硅玻璃,将硅片上其它区域的磷硅玻璃利用氢氟酸缓冲液去除掉;2a. Retain the phosphosilicate glass in the top electrode area by screen printing, and remove the phosphosilicate glass in other areas on the silicon wafer with hydrofluoric acid buffer;
3a、在硅片上表面淀积厚度约为40nm的本征非晶硅层2;3a. Depositing an intrinsic amorphous silicon layer 2 with a thickness of about 40 nm on the upper surface of the silicon wafer;
4a、将硅片置于湿氧的环境中进行高温扩散,使硅片非顶电极区的掺杂元素(磷)扩散入非晶硅层,降低硅片非顶电极区掺杂元素浓度,实现掺杂元素逆向扩散;顶电极区氧化层中的掺杂元素(磷)向顶电极区扩散,实现顶电极区的重掺杂,同时非晶硅层及非顶电极区的硅片表面被氧化形成磷硅玻璃层1;高温扩散的工艺温度为900℃,持续时间为30分钟;4a. Place the silicon wafer in a humid oxygen environment for high-temperature diffusion, so that the doping elements (phosphorus) in the non-top electrode area of the silicon wafer can diffuse into the amorphous silicon layer, reducing the concentration of doping elements in the non-top electrode area of the silicon wafer, and realizing Reverse diffusion of doping elements; the doping element (phosphorus) in the oxide layer of the top electrode area diffuses to the top electrode area to achieve heavy doping of the top electrode area, and at the same time, the surface of the amorphous silicon layer and the silicon wafer in the non-top electrode area is oxidized Forming the phosphosilicate glass layer 1; the process temperature of high-temperature diffusion is 900° C., and the duration is 30 minutes;
5a、采用氢氟酸缓冲液去除硅片表面的磷硅玻璃,完成太阳能电池的逆扩散选择性掺杂。5a. Using a hydrofluoric acid buffer solution to remove the phosphosilicate glass on the surface of the silicon wafer to complete the reverse diffusion selective doping of the solar cell.
利用仿真软件对本实施例一方法进行仿真后,硅片内杂质分见图2。仿真结果图中的曲线分别表示掺杂元素(磷)的浓度、以及PN结的位置。After using the simulation software to simulate the method of the first embodiment, the impurities in the silicon wafer are shown in FIG. 2 . The curves in the simulation result graph respectively represent the concentration of the doping element (phosphorus) and the position of the PN junction.
实施例二Embodiment two
本实施例的步骤与实施例一相同,区别在于步骤4a(第四步)中干氧环境下高温扩散的工艺参数,本实施例中,高温扩散的工艺温度为1000℃,持续时间为5分钟。利用仿真软件对本实施例二方法进行仿真后,硅片内杂质分见图3。仿真结果图中的曲线分别表示掺杂元素(磷)的浓度、以及PN结的位置。The steps of this example are the same as those of Example 1, the difference lies in the process parameters of high-temperature diffusion in dry oxygen environment in step 4a (the fourth step). In this example, the process temperature of high-temperature diffusion is 1000°C, and the duration is 5 minutes . After using the simulation software to simulate the method of the second embodiment, the impurities in the silicon wafer are shown in FIG. 3 . The curves in the simulation result graph respectively represent the concentration of the doping element (phosphorus) and the position of the PN junction.
实施例三Embodiment Three
本实施例的步骤与实施例一相同,区别在于步骤4a(第四步)中干氧环境下高温扩散的工艺参数,本实施例中,高温扩散的工艺温度为1100℃,持续时间为2分钟。利用仿真软件对本实施例三方法进行仿真后,硅片内杂质分见图4。仿真结果图中的曲线分别表示掺杂元素(磷)的浓度、以及PN结的位置。The steps of this example are the same as those of Example 1, the difference lies in the process parameters of high-temperature diffusion in dry oxygen environment in step 4a (the fourth step). In this example, the process temperature of high-temperature diffusion is 1100°C, and the duration is 2 minutes . After using the simulation software to simulate the method of the third embodiment, the impurities in the silicon wafer are shown in FIG. 4 . The curves in the simulation result graph respectively represent the concentration of the doping element (phosphorus) and the position of the PN junction.
对比本发明三个实施例,从仿真结果图中可以看出,随着逆向扩散工艺的高温扩散温度的升高,电池的PN结在不断的加深。电池的表面的杂质浓度先增加后减小,但顶电极区的杂质浓度随着温度的增加而逐步增加。顶电极区的重掺杂杂质主要向电池体内进行扩散,横向扩散较小,这与在电池表面淀积本征非晶硅层有关,过多的横向扩散杂质被非晶硅层吸收。这说明应用非晶硅层作为电池的逆扩散层,可以起到限制重掺杂区杂质横向扩散作用。轻掺杂区域的杂质浓度比较接近,较低的扩散温度可以有效地形成浅结,提高电池短波光谱响应,综合比较之后,可知步骤4a(第四步)中采用扩散温度900℃、扩散持续时间30分钟是较好的杂质逆扩散工艺条件。Comparing the three embodiments of the present invention, it can be seen from the simulation results that the PN junction of the battery is continuously deepened with the increase of the high-temperature diffusion temperature of the reverse diffusion process. The impurity concentration on the surface of the battery first increases and then decreases, but the impurity concentration in the top electrode region gradually increases with the increase of temperature. The heavily doped impurities in the top electrode region mainly diffuse into the battery body, and the lateral diffusion is small. This is related to the deposition of the intrinsic amorphous silicon layer on the surface of the battery. Excessive lateral diffusion impurities are absorbed by the amorphous silicon layer. This shows that using the amorphous silicon layer as the reverse diffusion layer of the battery can limit the lateral diffusion of impurities in the heavily doped region. The impurity concentration in the lightly doped region is relatively close, and the lower diffusion temperature can effectively form a shallow junction and improve the short-wave spectral response of the battery. After a comprehensive comparison, it can be seen that in step 4a (the fourth step), the diffusion temperature of 900°C and the diffusion duration 30 minutes is a better impurity reverse diffusion process condition.
本发明实施例部分以P型单晶硅为例对本发明工艺进行了详细说明,对N型单晶硅进行选择性掺杂的工艺及条件与之类似,区别仅在于掺杂元素由磷换成了硼,本领域技术人员完全可以通过了解本实施例部分,举一反三来实现对N型单晶硅的逆扩散选择性掺杂。因此本文不再赘述。The embodiment part of the present invention takes P-type single crystal silicon as an example to describe the process of the present invention in detail. The process and conditions for selective doping of N-type single crystal silicon are similar to it, the only difference is that the doping element is replaced by phosphorus In addition to boron, those skilled in the art can fully realize the reverse diffusion selective doping of N-type single crystal silicon by understanding the part of this embodiment and drawing inferences from facts. Therefore, this article will not repeat them.
除上述实施例外,本发明还可以有其他实施方式。凡采用等同替换或等效变换形成的技术方案,均落在本发明要求的保护范围。In addition to the above-mentioned embodiments, the present invention can also have other implementations. All technical solutions formed by equivalent replacement or equivalent transformation fall within the scope of protection required by the present invention.
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