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CN104183668A - Manufacturing method of solar cell unit - Google Patents

Manufacturing method of solar cell unit Download PDF

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CN104183668A
CN104183668A CN201410162819.8A CN201410162819A CN104183668A CN 104183668 A CN104183668 A CN 104183668A CN 201410162819 A CN201410162819 A CN 201410162819A CN 104183668 A CN104183668 A CN 104183668A
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film
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solar cell
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silicon layer
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曾我知洋
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Sumitomo Heavy Industries Ltd
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    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10FINORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
    • H10F71/00Manufacture or treatment of devices covered by this subclass
    • H10F71/121The active layers comprising only Group IV materials
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L21/00Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
    • H01L21/02Manufacture or treatment of semiconductor devices or of parts thereof
    • H01L21/04Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer
    • H01L21/18Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer the devices having semiconductor bodies comprising elements of Group IV of the Periodic Table or AIIIBV compounds with or without impurities, e.g. doping materials
    • H01L21/26Bombardment with radiation
    • H01L21/263Bombardment with radiation with high-energy radiation
    • YGENERAL 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
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E10/00Energy generation through renewable energy sources
    • Y02E10/50Photovoltaic [PV] energy
    • Y02E10/547Monocrystalline silicon PV cells
    • YGENERAL 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
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02PCLIMATE CHANGE MITIGATION TECHNOLOGIES IN THE PRODUCTION OR PROCESSING OF GOODS
    • Y02P70/00Climate change mitigation technologies in the production process for final industrial or consumer products
    • Y02P70/50Manufacturing or production processes characterised by the final manufactured product

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Abstract

本发明提供一种太阳能电池单元的制造方法,其为利用了离子注入法的新的太阳能电池单元的制造方法。本发明的一方式的太阳能电池单元的制造方法包括:准备工序,准备具有第1导电型的硅层和覆盖硅层的包覆膜的太阳能电池用基板;及发射极层形成工序,经由包覆膜朝向硅层照射第2导电型的离子,在硅层的受光面侧的一部分的区域形成发射极层。发射极层形成工序中,以离子的射程成为从包覆膜的表面到包覆膜与硅层的界面的距离的能量照射该离子。

The present invention provides a method of manufacturing a solar cell, which is a new method of manufacturing a solar cell using an ion implantation method. A method of manufacturing a solar cell unit according to an aspect of the present invention includes: a preparation step of preparing a solar cell substrate having a silicon layer of the first conductivity type and a coating film covering the silicon layer; and an emitter layer forming step of The film is irradiated with ions of the second conductivity type toward the silicon layer to form an emitter layer in a part of the light-receiving surface side of the silicon layer. In the emitter layer forming step, the ions are irradiated with energy such that the range of the ions is the distance from the surface of the coating film to the interface between the coating film and the silicon layer.

Description

太阳能电池单元的制造方法Manufacturing method of solar cell

技术领域technical field

本申请主张基于2013年5月27日申请的日本专利申请第2013-110595号的优先权。该申请的全部内容通过参考援用于本说明书中。This application claims priority based on Japanese Patent Application No. 2013-110595 filed on May 27, 2013. The entire content of this application is incorporated in this specification by reference.

本发明涉及一种太阳能电池单元的制造方法。The invention relates to a method for manufacturing a solar cell unit.

背景技术Background technique

太阳能电池中,硅等半导体材料吸收光时产生的电子空穴对通过基于形成于电池内部的pn结等产生的电场,电子向n层侧移动,空穴向p层侧移动,从而作为电流向外部电路输出。形成pn结或接触层时需要局部进行使杂质的浓度或种类不同的处理。并且,为了尽可能增加吸收于太阳能电池内部的光而在硅基板的受光面侧形成防反射膜。In solar cells, electron-hole pairs generated when semiconductor materials such as silicon absorb light pass through the electric field generated by the pn junction formed inside the cell, electrons move to the n-layer side, and holes move to the p-layer side, thereby flowing as a current to the p-layer side. External circuit output. When forming a pn junction or a contact layer, it is necessary to locally perform a process of varying the concentration or type of impurities. Furthermore, an antireflection film is formed on the light-receiving surface side of the silicon substrate in order to increase the light absorbed inside the solar cell as much as possible.

具体而言,已知有太阳能电池的制造方法,所述方法中,利用离子注入法以高浓度掺杂n型杂质而在p型硅基板的表面形成n型层(发射极层)后,形成防反射膜(例如,参考专利文献1)。Specifically, there is known a solar cell manufacturing method in which an n-type layer (emitter layer) is formed on the surface of a p-type silicon substrate by doping n-type impurities at a high concentration by ion implantation, and then forming Anti-reflection film (for example, refer to Patent Document 1).

专利文献1:日本特表2010-527163号公报Patent Document 1: Japanese National Publication No. 2010-527163

然而,利用离子注入法形成发射极层时,被注入的离子的射程成为从硅基板的表面进入某一程度的位置(深度)。因此,掺杂离子的深度方向的浓度分布成为从硅基板表面在某一程度的深度具有峰值。这种杂质浓度的峰值的存在由于阻碍载流子的移动,因此成为导致发电效率下降的原因之一。However, when the emitter layer is formed by ion implantation, the range of implanted ions is a position (depth) that penetrates to a certain extent from the surface of the silicon substrate. Therefore, the concentration distribution of the dopant ions in the depth direction has a peak at a certain depth from the surface of the silicon substrate. The presence of such a peak in the impurity concentration hinders the movement of carriers, which is one of the causes of a decrease in power generation efficiency.

发明内容Contents of the invention

本发明的一方式的例示性目的之一在于提供一种利用了离子注入法的新的太阳能电池单元的制造方法。One of the exemplary objects of one aspect of the present invention is to provide a new method of manufacturing a solar cell using an ion implantation method.

为了解决上述课题,本发明的一方式的太阳能电池单元的制造方法包括:准备工序,准备具有第1导电型的硅层和覆盖硅层的包覆膜的太阳能电池用基板;及发射极层形成工序,经由包覆膜朝向硅层照射第2导电型的离子,在硅层的受光面侧的一部分的区域形成发射极层。发射极层形成工序中,以离子的射程成为从包覆膜的表面到包覆膜与硅层的界面为止的距离的能量照射该离子。In order to solve the above-mentioned problems, a method of manufacturing a solar cell according to an aspect of the present invention includes: a preparation step of preparing a substrate for a solar cell having a silicon layer of the first conductivity type and a coating film covering the silicon layer; and forming an emitter layer. In the step, the silicon layer is irradiated with ions of the second conductivity type through the coating film to form an emitter layer in a part of the light-receiving surface side of the silicon layer. In the emitter layer forming step, the ions are irradiated with energy such that the range of the ions is the distance from the surface of the cladding film to the interface between the cladding film and the silicon layer.

本发明的另一方式为太阳能电池单元的制造方法。该方法中,包括:准备工序,准备具有第1导电型的硅层和覆盖硅层的包覆膜的太阳能电池用基板;及发射极层形成工序,经由包覆膜朝向硅层照射第2导电型的离子,在硅层的受光面侧的一部分的区域形成发射极层。发射极层形成工序中,以如下能量照射该离子,即离子的深度方向的浓度分布的峰位置成为到包覆膜与硅层的界面为止的深度D±10nm的范围。Another aspect of the present invention is a method of manufacturing a solar battery cell. This method includes: a preparation step of preparing a substrate for a solar cell having a silicon layer of the first conductivity type and a coating film covering the silicon layer; Type ions form an emitter layer in a part of the light-receiving side of the silicon layer. In the emitter layer forming step, the ions are irradiated with energy such that the peak position of the ion concentration distribution in the depth direction falls within the range of the depth D±10 nm from the interface between the coating film and the silicon layer.

发明效果:Invention effect:

根据本发明,能够实现利用了离子注入法的新的太阳能电池单元的制造方法。According to the present invention, it is possible to realize a new method of manufacturing a solar cell using an ion implantation method.

附图说明Description of drawings

图1是表示进行标准的离子注入时的掺杂浓度分布的结果的图。FIG. 1 is a graph showing the results of doping concentration distribution when standard ion implantation is performed.

图2是表示经由屏膜对硅基板实施离子注入时的掺杂浓度分布的一例的图。FIG. 2 is a diagram showing an example of a doping concentration distribution when ion implantation is performed into a silicon substrate through a mask.

图3是表示在去除屏膜之后的硅基板内部的掺杂浓度分布的一例的图。FIG. 3 is a diagram showing an example of a doping concentration distribution inside a silicon substrate after removing a screen film.

图4是第1实施方式所涉及的太阳能电池单元的制造方法的流程图。Fig. 4 is a flowchart of a method of manufacturing a solar battery cell according to the first embodiment.

图5(a)~图5(f)是第1实施方式所涉及的太阳能电池单元的制造方法的各工序中的半导体基板的概略剖视图。5( a ) to 5 ( f ) are schematic cross-sectional views of the semiconductor substrate in each step of the method of manufacturing the solar battery cell according to the first embodiment.

图6是第2实施方式所涉及的太阳能电池单元的制造方法的流程图。6 is a flowchart of a method of manufacturing a solar battery cell according to the second embodiment.

图7(a)~图7(e)是第2实施方式所涉及的太阳能电池单元的制造方法的各工序中的半导体基板的概略剖视图。7( a ) to 7 ( e ) are schematic cross-sectional views of the semiconductor substrate in each step of the method of manufacturing a solar battery cell according to the second embodiment.

图8是第3实施方式所涉及的太阳能电池单元的制造方法的流程图。8 is a flowchart of a method of manufacturing a solar battery cell according to the third embodiment.

图9(a)~图9(e)是第3实施方式所涉及的太阳能电池单元的制造方法的各工序中的半导体基板的概略剖视图。9( a ) to 9 ( e ) are schematic cross-sectional views of the semiconductor substrate in each step of the method of manufacturing a solar battery cell according to the third embodiment.

图10(a)~图10(b)是第3实施方式所涉及的太阳能电池单元的制造方法的各工序中的半导体基板的概略剖视图。10(a) to 10(b) are schematic cross-sectional views of the semiconductor substrate in each step of the method of manufacturing a solar cell according to the third embodiment.

图中:10-硅基板,12-屏膜,14-发射极层,16-防反射膜,18-受光面电极,20-背面电极,24-掩模,26-接触区域,100、200、300-太阳能电池单元。In the figure: 10-silicon substrate, 12-screen film, 14-emitter layer, 16-anti-reflection film, 18-light-receiving surface electrode, 20-back electrode, 24-mask, 26-contact area, 100, 200, 300 - Solar cell unit.

具体实施方式Detailed ways

以下,对用于实施本发明的方式进行详细说明。另外,以下所述的结构是例示,对本发明的范围不作任何限定。并且,在附图说明中对相同的要件附加相同的符号,并适当省略重复的说明。并且,说明制造方法时所示的各剖视图中,为便于说明半导体基板和其它层的厚度、大小并不一定表示实际的尺寸和比例。Hereinafter, the form for carrying out this invention is demonstrated in detail. In addition, the structure described below is an illustration and does not limit the scope of the present invention at all. In addition, in the description of the drawings, the same reference numerals are attached to the same elements, and overlapping descriptions are appropriately omitted. In addition, in each cross-sectional view shown in the description of the manufacturing method, the thickness and size of the semiconductor substrate and other layers do not necessarily represent actual dimensions and ratios for the convenience of description.

(第1实施方式)(first embodiment)

太阳能电池被设计为多种类型。例如,结晶Si系太阳能电池由它简单的结构和制造方法、较高的转换效率等的特征确保相对于其他类型的太阳能电池的优越性。另一方面,为了在结晶Si系太阳能电池中求出更高的转换效率,找出对各工艺单位最适合的条件对进行区别非常重要。其中,认为由光电效果主导引起的表面发射极层的形成是非常重要的要素,认为优选具有以下特征。Solar cells are designed in many types. For example, a crystalline Si-based solar cell ensures superiority over other types of solar cells by its features of simple structure and manufacturing method, high conversion efficiency, and the like. On the other hand, in order to obtain higher conversion efficiency in crystalline Si-based solar cells, it is very important to find out the conditions most suitable for each process unit and to differentiate them. Among them, the formation of the surface emitter layer mainly caused by the photoelectric effect is considered to be a very important factor, and it is considered that it preferably has the following characteristics.

但是,当前用作一般制造方法的热扩散法、离子注入法从其特性来看都难以同时满足以下特征。However, the thermal diffusion method and the ion implantation method currently used as general manufacturing methods are difficult to simultaneously satisfy the following characteristics from the viewpoint of their characteristics.

(1)浅接合。具体而言,使内部扩散电位进一步靠近表面。(1) Shallow joint. Specifically, the internal diffusion potential is brought closer to the surface.

(2)最佳掺杂浓度。具体而言,为了与电极的接触和通过发射极层的多数载流子的移动,发射极浓度具有某一较高的浓度。但从少数载流子的再结合减少的观点来看希望浓度不能过高。(2) Optimal doping concentration. Specifically, the emitter concentration has a certain higher concentration for contact with the electrodes and movement of majority carriers through the emitter layer. However, from the viewpoint of reducing the recombination of minority carriers, it is desirable that the concentration is not too high.

(3)在表面内侧不具有特别的浓度峰。具体而言,成为少数载流子移动的障壁程度的强电场的高低接合不存在于比表面更靠内侧。(3) There is no particular concentration peak inside the surface. Specifically, the high-low junction of a strong electric field that acts as a barrier to minority carrier movement does not exist on the inner side of the surface.

(4)在最表面具有些许的高低接合。具体而言,具有从表面向相反的一面排出少数载流子的效果。(4) There are some high and low joints on the outermost surface. Specifically, it has the effect of discharging minority carriers from the surface to the opposite surface.

由于能够控制掺杂深度、浓度,因此离子注入法相对于热扩散法的特征在前述(1)、(2)方面非常优越。另一方面,利用离子注入时,与离子的加速能量对应的深度具有掺杂浓度的峰值,且成为掺杂浓度从其峰位置朝向表面层减少的分布。Since the doping depth and concentration can be controlled, the ion implantation method is superior to the thermal diffusion method in terms of (1) and (2) above. On the other hand, when ion implantation is used, the depth corresponding to the acceleration energy of the ions has a peak of the doping concentration, and the doping concentration becomes a distribution that decreases from the peak position toward the surface layer.

图1是表示进行标准的离子注入时的掺杂浓度分布的结果的图。图1所示的离子注入中,将磷(P)用作注入离子种,以加速能量为10keV、剂量为3×1015个/cm2的条件对硅基板进行离子注入。如图1所示,根据这种条件的离子注入,掺杂浓度从表面S逐渐增加,在距表面S约0.015μm(15nm)左右的深度D处掺杂浓度成为峰值,之后掺杂浓度减少。即,该离子注入中的注入射程Rp为0.015μm(15nm)左右。FIG. 1 is a graph showing the results of doping concentration distribution when standard ion implantation is performed. In the ion implantation shown in FIG. 1 , phosphorus (P) was used as an implanted ion seed, and ions were implanted into a silicon substrate at an acceleration energy of 10 keV and a dose of 3×10 15 ions/cm 2 . As shown in FIG. 1 , according to ion implantation under such conditions, the doping concentration gradually increases from the surface S, reaches a peak at a depth D of about 0.015 μm (15 nm) from the surface S, and then decreases. That is, the implantation range Rp in this ion implantation is about 0.015 μm (15 nm).

这种分布Pr通过后面的激活退火稍微被缓和,但离子注入法在前述(3)观点上有另外改善的余地。并且,为形成浅接合,需要低能量的离子注入,但是一般越成为低能量,射束的传输效率越下降,从而生产率下降。This distribution Pr is slightly relaxed by the subsequent activation annealing, but the ion implantation method has room for improvement in the aforementioned point (3). In addition, low-energy ion implantation is required to form shallow junctions, but generally, the lower the energy, the lower the beam transmission efficiency and the lower the productivity.

本发明考虑这些方面,实现利用了离子注入法的新的太阳能电池单元的制造方法。以下方式中,对考虑离子的射程,在形成发射极层之前,先形成某一厚度的任何一个包覆膜,经由该包覆膜对半导体层进行离子注入而形成具有优选掺杂浓度分布的发射极层的方法进行说明。另外,包覆膜至少覆盖基板的一部分即可,无需完全覆盖基板。并且,整个包覆膜的厚度也无需一样,各区域的厚度也可以不同。The present invention realizes a new method of manufacturing a solar battery cell using the ion implantation method in consideration of these points. In the following method, considering the range of ions, before forming the emitter layer, any cladding film with a certain thickness is formed, and ion implantation is performed on the semiconductor layer through the cladding film to form an emitter with a preferred doping concentration distribution. The polar layer method is described. In addition, it is only necessary for the cover film to cover at least a part of the substrate, and it is not necessary to completely cover the substrate. In addition, the thickness of the entire covering film does not need to be the same, and the thickness of each region may be different.

本实施方式中,作为硅(半导体)层的包覆膜使用屏膜。作为屏膜,可以以CVD或溅射等技术、或者印刷技术或涂布技术等形成易形成于硅基板上的氧化膜或氮化膜等。另外,若考虑被生成的屏膜的厚度和所需的离子注入能量,则优选以CVD或溅射等技术形成氧化膜或氮化膜等。并且,膜的材质只要离子能够透射则并不特别限定,但优选由离子注入时产生的撞击引起的对硅基板内部的影响较小的材质。In the present embodiment, a screen film is used as the coating film of the silicon (semiconductor) layer. As the screen film, an oxide film, a nitride film, or the like that is easily formed on a silicon substrate can be formed by a technique such as CVD or sputtering, or a printing technique or a coating technique. In addition, in consideration of the thickness of the screen film to be formed and the required ion implantation energy, it is preferable to form an oxide film or a nitride film by a technique such as CVD or sputtering. In addition, the material of the film is not particularly limited as long as ions are permeable, but a material having less influence on the inside of the silicon substrate due to impacts during ion implantation is preferable.

形成屏膜后,调整离子注入的能量,以使离子的注入射程Rp成为屏膜与硅基板的界面附近,经由屏膜对硅基板实施离子注入。图2是表示经由屏膜对硅基板实施离子注入时的掺杂浓度分布的一例的图。图2所示的屏膜是厚度为约70nm的氧化膜(SiO2膜)。而且,图2所示的掺杂浓度分布中,将磷(P)用作注入离子种,以加速能量为60keV、剂量为3×1015个/cm2的条件经由屏膜对硅基板进行离子注入。After the mask is formed, the energy of ion implantation is adjusted so that the ion implantation range Rp is near the interface between the mask and the silicon substrate, and ion implantation is performed on the silicon substrate through the mask. FIG. 2 is a diagram showing an example of a doping concentration distribution when ion implantation is performed into a silicon substrate through a mask. The screen film shown in FIG. 2 is an oxide film (SiO 2 film) with a thickness of about 70 nm. Moreover, in the doping concentration distribution shown in Fig. 2, phosphorus (P) is used as implanted ion species, and the silicon substrate is ionized through the screen film under the conditions of acceleration energy of 60keV and dose of 3× 1015 / cm2 . injection.

图2所示的掺杂浓度分布Pr’为至少在硅基板的表面S’附近平缓且朝向基板内部浓度逐渐地急剧下降的理想的分布。另外,60keV左右的加速能量是作为一段加速的离子注入装置容易输出大电流的优选的能量,即使其接近一半的剂量残留在屏膜,生产率上也没有问题。因此,作为注入离子的加速能量,可调整为40keV以上,更优选为50keV以上。并且,作为注入离子的加速能量,例如可调整为80keV以下,更优选为70keV以下。另外,注入离子的加速能量并不限定于上述例,也可以根据屏膜或硅基板的各种条件适当进行改变。The doping concentration profile Pr' shown in FIG. 2 is an ideal profile in which the doping concentration profile Pr' is gentle at least near the surface S' of the silicon substrate, and the concentration gradually and sharply decreases toward the inside of the substrate. In addition, the acceleration energy of about 60keV is the preferred energy for an ion implantation device that is accelerated as a stage to easily output a large current. Even if nearly half of the dose remains on the screen film, there is no problem in productivity. Therefore, the acceleration energy of implanted ions can be adjusted to 40 keV or more, more preferably 50 keV or more. In addition, the acceleration energy of implanted ions can be adjusted to, for example, 80 keV or less, more preferably 70 keV or less. In addition, the acceleration energy of implanted ions is not limited to the above example, and may be appropriately changed according to various conditions of the screen film or the silicon substrate.

以上述条件进行了离子注入之后,以缓冲氢氟酸等蚀刻去除表面的氧化膜。图3是在去除屏膜之后的硅基板内部的掺杂浓度分布的一例的图。如图3所示,硅基板的表面S’露出,且在硅基板内形成有理想的掺杂浓度分布Pr’’。After performing ion implantation under the above-mentioned conditions, the oxide film on the surface is removed by etching with buffered hydrofluoric acid or the like. FIG. 3 is a diagram showing an example of a doping concentration distribution inside a silicon substrate after removing a screen film. As shown in FIG. 3, the surface S' of the silicon substrate is exposed, and an ideal doping concentration distribution Pr'' is formed in the silicon substrate.

图4是第1实施方式所涉及的太阳能电池单元的制造方法的流程图。图5(a)~图5(f)是第1实施方式所涉及的太阳能电池单元的制造方法的各工序中的半导体基板的概略剖视图。Fig. 4 is a flowchart of a method of manufacturing a solar battery cell according to the first embodiment. 5( a ) to 5 ( f ) are schematic cross-sectional views of the semiconductor substrate in each step of the method of manufacturing the solar battery cell according to the first embodiment.

本实施方式中,对作为半导体基板使用了p型的单晶硅基板的情况进行说明,但是使用n型的硅基板或多晶基板、其他p型或n型的化合物半导体基板时也能够适用本发明。以下,参考图4、图5对第1实施方式所涉及的太阳能电池单元的制造方法进行说明。In the present embodiment, the case where a p-type single crystal silicon substrate is used as the semiconductor substrate is described, but the present invention can also be applied when using an n-type silicon substrate or a polycrystalline substrate, or other p-type or n-type compound semiconductor substrates. invention. Hereinafter, a method of manufacturing the solar battery cell according to the first embodiment will be described with reference to FIGS. 4 and 5 .

首先,如图5(a)所示,通过将单晶硅锭用多线法进行切片来准备p型的硅基板10。接着,用碱溶液消除由基板表面的切片产生的损伤后,在受光面上形成最大高度10μm左右的微细凹凸(纹理:在图5(a)中未图示)(图4的S10)。通过由这种凹凸结构产生的散射得到陷光效果,有助于提高转换效率。First, as shown in FIG. 5( a ), a p-type silicon substrate 10 is prepared by slicing a single crystal silicon ingot by a multi-wire method. Next, after removing damage caused by slicing the substrate surface with an alkaline solution, fine unevenness (texture: not shown in FIG. 5( a )) with a maximum height of about 10 μm is formed on the light-receiving surface (S10 in FIG. 4 ). The light-trapping effect is obtained by the scattering caused by the concave-convex structure, which contributes to the improvement of the conversion efficiency.

接着,如图5(b)所示,在硅基板10的表面上,形成由SiO2等膜(或包覆膜)构成的屏膜12(图4的S12)。屏膜12的厚度例如为10~100nm左右。由此准备具有p型(第1导电型)的硅基板10及作为覆盖硅基板10的包覆膜的屏膜12的太阳能电池用基板。接着,如图5(c)所示,经由屏膜12朝向硅基板10照射成为与硅基板10相反的导电型的n型(第2导电型)的离子,在硅基板10的受光面侧的一部分的区域形成发射极层14(图4的S14)。Next, as shown in FIG. 5(b), on the surface of the silicon substrate 10, a screen film 12 made of a film (or coating film) such as SiO 2 is formed (S12 in FIG. 4). The thickness of the screen film 12 is, for example, about 10 to 100 nm. In this way, a solar cell substrate having a p-type (first conductivity type) silicon substrate 10 and a screen film 12 as a coating film covering the silicon substrate 10 is prepared. Next, as shown in FIG. 5(c), the silicon substrate 10 is irradiated with n-type (second conductivity type) ions of the opposite conductivity type to the silicon substrate 10 through the screen film 12, and the light-receiving surface side of the silicon substrate 10 Part of the region forms the emitter layer 14 (S14 in FIG. 4).

本实施方式所涉及的发射极层形成工序中,如图2中的说明,以离子的射程Rp成为从屏膜12的表面S到屏膜12与硅基板10的界面(硅基板10的表面S’)为止的距离的能量照射离子(参考图5(b))。In the emitter layer forming process according to the present embodiment, as described in FIG. ') to irradiate ions with the energy of the distance (refer to FIG. 5(b)).

接着,如图5(d)所示,除去屏膜12(图4的S16),为了缓和由离子注入产生的硅基板10的损伤而进行激活退火处理(图4的S18)。另外,也可以调换屏膜12的去除和激活退火处理的顺序。而且,如图5(e)所示,在发射极层14的表面上通过CVD法等形成SiN或TiO2等防反射膜16(图4的S20)。防反射膜16的厚度例如为10~100nm左右。Next, as shown in FIG. 5(d), the screen film 12 is removed (S16 in FIG. 4), and an activation annealing treatment is performed to alleviate damage to the silicon substrate 10 caused by ion implantation (S18 in FIG. 4). In addition, the order of the removal of the screen film 12 and the activation annealing treatment may be reversed. Then, as shown in FIG. 5(e), an antireflection film 16 such as SiN or TiO 2 is formed on the surface of the emitter layer 14 by CVD or the like (S20 in FIG. 4 ). The thickness of the antireflection film 16 is, for example, about 10 to 100 nm.

接着,如图5(f)所示,沿防反射膜16的图案在发射极层14的规定区域上形成直接受光面电极18(图4的S22)。受光面电极18通过例如印刷、烧成将以银(Ag)为主成分的受光面电极用浆料形成为宽度为50~100μm左右的梳状。受光面电极18的高度为10~50μm左右。Next, as shown in FIG. 5(f), the direct light-receiving surface electrode 18 is formed on a predetermined region of the emitter layer 14 along the pattern of the antireflection film 16 (S22 in FIG. 4). The light-receiving surface electrode 18 is formed into a comb shape with a width of about 50 to 100 μm by, for example, printing or firing a paste for a light-receiving surface electrode mainly composed of silver (Ag). The height of the light-receiving surface electrode 18 is about 10 to 50 μm.

并且,在该阶段,背面电极20也通过使用以铝(Al)为主成分的背面电极用浆料来进行印刷、烧成而被形成。此时,浆料所含的Al扩散到硅基板10的内部,在背面电极20附近形成p+层22。由此,能够得到BSF(Back Surface Field)效果。In addition, at this stage, the back electrode 20 is also formed by printing and firing using a paste for a back electrode whose main component is aluminum (Al). At this time, Al contained in the paste diffuses into the silicon substrate 10 to form the p+ layer 22 near the back electrode 20 . Thus, a BSF (Back Surface Field) effect can be obtained.

通过以上工序,制造太阳能电池单元100。由于该太阳能电池单元100中,被掺杂的离子的浓度分布的峰值不存在于发射极层14,因此在发电时载流子变得容易移动。即,经由屏膜12进行离子注入,由此可避免一般在离子注入中常见的掺杂浓度分布,具体而言,掺杂浓度从硅基板表面增加一次之后减少的分布。若进行详细说明,则本实施方式所涉及的太阳能电池单元100的发射极层14中,掺杂浓度分布为表面附近平缓的浓度梯度,且呈随着从表面变深而浓度梯度逐渐变大的理想的形状。其结果,得到发电效率较高的太阳能电池单元。Through the above steps, the solar cell 100 is manufactured. In this solar battery cell 100 , since the peak of the concentration distribution of ions to be doped does not exist in the emitter layer 14 , carriers can easily move during power generation. That is, ion implantation is performed through the screen film 12 , thereby avoiding a doping concentration distribution that is generally common in ion implantation, specifically, a distribution in which the doping concentration increases once from the surface of the silicon substrate and then decreases. To describe in detail, in the emitter layer 14 of the solar cell 100 according to this embodiment, the doping concentration distribution is a gentle concentration gradient near the surface, and the concentration gradient gradually increases as it goes deeper from the surface. ideal shape. As a result, a solar battery cell with high power generation efficiency is obtained.

而且,调换图4所示的步骤S16与步骤S18的处理,进行了激活退火处理后去除屏膜时,在屏膜与硅基板的界面产生的掺杂剂的高浓度层中,通过去除屏膜而被除掉一部分,因此能够减轻由高浓度层产生的载流子再结合等。Moreover, when the processes of step S16 and step S18 shown in FIG. 4 are exchanged, and when the screen film is removed after the activation annealing treatment, in the high-concentration layer of dopant generated at the interface between the screen film and the silicon substrate, by removing the screen film Since a part is removed, it is possible to reduce recombination of carriers generated in the high-concentration layer and the like.

并且,适当选择屏膜的膜厚,由此在离子注入装置中,能够以离子的传输效率较高的条件进行离子注入处理,提高生产率。即,将屏膜的厚度设为规定值以上(例如10nm以上),由此提高离子的加速能量,因此离子的注入效率变高。另一方面,将屏膜的厚度设为规定值以下(例如100nm以下),由此减少无法到达基板而停留在屏膜内部的无用的离子。In addition, by appropriately selecting the film thickness of the screen film, in the ion implantation apparatus, the ion implantation process can be performed under the condition of high ion transmission efficiency, and the productivity can be improved. That is, by setting the thickness of the screen film to a predetermined value or more (for example, 10 nm or more), the acceleration energy of ions is increased, so that ion implantation efficiency becomes high. On the other hand, by setting the thickness of the screen film to a predetermined value or less (for example, 100 nm or less), useless ions that cannot reach the substrate and stay inside the screen film are reduced.

另外,本实施方式中,仅在太阳能电池单元100的表面侧(比硅基板10更靠表面侧)形成有钝化膜(防反射膜16),但也可以在太阳能电池单元100的表面侧及背面侧这两侧形成钝化膜。并且,本实施方式中,对从硅基板10的表面侧照射离子的情况进行了说明,但在从背面侧照射离子的情况或从表面侧及背面侧这两侧照射离子的情况也能够适用本发明。In addition, in this embodiment, the passivation film (anti-reflection film 16) is formed only on the surface side of the solar battery cell 100 (the side closer to the surface side than the silicon substrate 10), but it may be formed on the surface side of the solar battery cell 100 and Passivation films are formed on both sides of the back side. In addition, in this embodiment, the case of irradiating ions from the front side of the silicon substrate 10 has been described, but this method can also be applied to the case of irradiating ions from the back side or the case of irradiating ions from both the front side and the back side. invention.

(第2实施方式)(second embodiment)

在本实施方式中,对将防反射膜用作屏膜的情况进行说明。图6是第2实施方式所涉及的太阳能电池单元的制造方法的流程图。图7(a)~图7(e)是第2实施方式所涉及的太阳能电池单元的制造方法的各工序中的半导体基板的概略剖视图。另外,对与第1实施方式相同的构成要件或工序附加相同的符号而适当省略说明。In this embodiment, a case where an antireflection film is used as a screen film will be described. 6 is a flowchart of a method of manufacturing a solar battery cell according to the second embodiment. 7( a ) to 7 ( e ) are schematic cross-sectional views of the semiconductor substrate in each step of the method of manufacturing a solar battery cell according to the second embodiment. In addition, the same code|symbol is attached|subjected to the same component or process as 1st Embodiment, and description is abbreviate|omitted suitably.

首先,如图7(a)所示,在p型的硅基板10的受光面上形成纹理(图6的S10)。接着,如图7(b)所示,在硅基板10的表面上通过CVD法等形成SiN或TiO2等防反射膜16(图6的S24)。防反射膜16的厚度例如为10~100nm左右。由此,准备具有p型(第1导电型)的硅基板10和作为覆盖硅基板10的包覆膜的防反射膜16的太阳能电池用基板。First, as shown in FIG. 7( a ), texture is formed on the light-receiving surface of the p-type silicon substrate 10 ( S10 in FIG. 6 ). Next, as shown in FIG. 7(b), an antireflection film 16 such as SiN or TiO 2 is formed on the surface of the silicon substrate 10 by CVD or the like (S24 in FIG. 6). The thickness of the antireflection film 16 is, for example, about 10 to 100 nm. Thus, a solar cell substrate having a p-type (first conductivity type) silicon substrate 10 and an antireflection film 16 as a coating film covering the silicon substrate 10 is prepared.

接着,如图7(c)所示,经由防反射膜16朝向硅基板10照射成为与硅基板10相反的导电型的n型(第2导电型)的离子,在硅基板10的受光面侧的一部分区域形成发射极层14(图6的S26)。Next, as shown in FIG. 7( c), the silicon substrate 10 is irradiated with n-type (second conductivity type) ions of the opposite conductivity type to the silicon substrate 10 through the anti-reflection film 16, and on the light-receiving surface side of the silicon substrate 10, Part of the region forms the emitter layer 14 (S26 in FIG. 6).

本实施方式所涉及的发射极层形成工序中,如图2中的说明,以离子的射程Rp成为从防反射膜16的表面S到防反射膜16与硅基板10的界面(硅基板10的表面S’)为止的距离的能量照射离子(参考图7(b))In the emitter layer forming process according to the present embodiment, as described in FIG. The energy irradiated ions at the distance to the surface S') (refer to Fig. 7(b))

接着,如图7(d)所示,为了缓和由离子注入产生的硅基板10的损伤而进行激活退火处理(图6的S28)。并且,如图7(e)所述,通过与第1实施方式相同的步骤S22的处理而形成受光面电极18和背面电极20。Next, as shown in FIG. 7( d ), activation annealing is performed in order to alleviate damage to the silicon substrate 10 caused by ion implantation ( S28 in FIG. 6 ). Then, as shown in FIG. 7( e ), the light-receiving surface electrode 18 and the rear surface electrode 20 are formed by the same process as that of the first embodiment in step S22 .

通过以上工序,制造太阳能电池单元200。该太阳能电池单元200能够得到与第1实施方式所涉及的太阳能电池单元100相同的效果。另外,作为屏膜使用防反射膜16,由此与第1实施方式所涉及的太阳能电池单元100的制造方法相比能够消减工序。并且,由于在防反射膜16内不产生光电反应,因此防反射膜16中的掺杂浓度分布不对少数载流子的移动产生影响。Through the above steps, the solar cell 200 is manufactured. This solar cell 200 can obtain the same effects as those of the solar cell 100 according to the first embodiment. In addition, by using the antireflection film 16 as the screen film, it is possible to reduce the number of steps compared with the method of manufacturing the solar battery cell 100 according to the first embodiment. Furthermore, since no photoelectric reaction occurs in the antireflection film 16 , the doping concentration distribution in the antireflection film 16 does not affect the movement of minority carriers.

另外,本实施方式中,在硅基板10上直接形成有防反射膜16,但也可以在硅基板10与防反射膜16之间形成其他钝化膜。此时,可以在硅基板10上形成其他钝化膜,从其他钝化膜侧照射离子之后形成防反射膜16,也可以在硅基板10上形成其他钝化膜及防反射膜16之后从其他钝化膜及防反射膜16侧照射离子。In addition, in this embodiment, the antireflection film 16 is directly formed on the silicon substrate 10 , but another passivation film may be formed between the silicon substrate 10 and the antireflection film 16 . At this time, another passivation film can be formed on the silicon substrate 10, and the anti-reflection film 16 can be formed after irradiating ions from the side of the other passivation film. The passivation film and the antireflection film 16 side are irradiated with ions.

(第3实施方式)(third embodiment)

本实施方式中,作为屏膜利用防反射膜,并且对除了发射极层以外还形成接触区域的情况进行说明。图8是第3实施方式所涉及的太阳能电池单元的制造方法的流程图。图9(a)~图9(e)是第3实施方式所涉及的太阳能电池单元的制造方法的各工序中的半导体基板的概略剖视图。图10(a)~图10(b)是第3实施方式所涉及的太阳能电池单元的制造方法的各工序中的半导体基板的概略剖视图。另外,对与上述各实施方式相同的构成要件或工序附加相同符号而适当省略说明。In this embodiment mode, a case where an antireflection film is used as a screen film and a contact region is formed in addition to the emitter layer will be described. 8 is a flowchart of a method of manufacturing a solar battery cell according to the third embodiment. 9( a ) to 9 ( e ) are schematic cross-sectional views of the semiconductor substrate in each step of the method of manufacturing a solar battery cell according to the third embodiment. 10(a) to 10(b) are schematic cross-sectional views of the semiconductor substrate in each step of the method of manufacturing a solar cell according to the third embodiment. In addition, the same code|symbol is attached|subjected to the same component or process as each above-mentioned embodiment, and description is abbreviate|omitted suitably.

首先,如图9(a)所示,在p型的硅基板10的受光面形成纹理(图8的S10)。接着,如图9(b)所示,在硅基板10的表面上通过CVD法等形成SiN或TiO2等防反射膜16(图8的S24)。接着,如图9(c)所示,经由防反射膜16朝向硅基板10照射成为与硅基板10相反的导电型的n型(第2导电型)的离子,在硅基板10的受光面侧的一部分的区域形成发射极层14(图8的S26)。First, as shown in FIG. 9( a ), texture is formed on the light-receiving surface of the p-type silicon substrate 10 ( S10 in FIG. 8 ). Next, as shown in FIG. 9(b), an antireflection film 16 such as SiN or TiO 2 is formed on the surface of the silicon substrate 10 by CVD or the like (S24 in FIG. 8 ). Next, as shown in FIG. 9( c), the silicon substrate 10 is irradiated with n-type (second conductivity type) ions of the opposite conductivity type to the silicon substrate 10 through the anti-reflection film 16, and on the light-receiving surface side of the silicon substrate 10, A part of the region forms the emitter layer 14 (S26 in FIG. 8).

接着,如图9(d)所示,形成以防反射膜16的规定区域露出的方式构图的掩模24(图8的S30)。掩模24能够使用通过光刻蚀法、印刷法而形成的掩模或硬掩模。Next, as shown in FIG. 9( d ), a mask 24 patterned so that a predetermined region of the antireflection film 16 is exposed is formed ( S30 in FIG. 8 ). As the mask 24, a mask or a hard mask formed by a photolithography method or a printing method can be used.

接着,如图9(e)所示,再度对基板的受光面侧通过离子注入全面注入成为与基板相反的导电型的n型掺杂剂。此时,经由未被掩模包覆的、露出防反射膜16的规定区域16a,对处于其下部的发射极层14的一部分区域选择性地注入离子。由此,在发射极层14的规定区域形成有杂质浓度高于其他区域的接触区域26(图8的S32)。将如此对基板的一部分选择性地注入离子,并形成杂质浓度较高的接触区域的方式称为选择发射极。通过这种方式,掩盖不需要离子注入的部分后进行离子注入,由此在基板的规定区域形成与未被掩盖的部分对应的选择性离子注入图案。Next, as shown in FIG. 9( e ), an n-type dopant having a conductivity type opposite to that of the substrate is implanted into the entire surface of the light-receiving surface side of the substrate again by ion implantation. At this time, ions are selectively implanted into a part of the emitter layer 14 below the predetermined region 16 a exposed to the antireflection film 16 not covered by the mask. As a result, a contact region 26 having a higher impurity concentration than other regions is formed in a predetermined region of the emitter layer 14 (S32 in FIG. 8 ). Such a method of selectively implanting ions into a part of the substrate to form a contact region with a high impurity concentration is called a selective emitter. In this way, by masking the portion where ion implantation is not required and performing ion implantation, a selective ion implantation pattern corresponding to the unmasked portion is formed in a predetermined region of the substrate.

接着,如图10(a)所示,从硅基板10除去掩模24(图8的S34),对整个基板实施激活退火处理(图8的S36)。而且,如图10(b)所示,通过与第1实施方式同样的步骤S22的处理形成受光面电极18和背面电极20。Next, as shown in FIG. 10( a ), the mask 24 is removed from the silicon substrate 10 ( S34 in FIG. 8 ), and activation annealing is performed on the entire substrate ( S36 in FIG. 8 ). Then, as shown in FIG. 10( b ), the light-receiving surface electrode 18 and the rear surface electrode 20 are formed by the same process as that of the first embodiment in step S22 .

通过以上工序,制造太阳能电池单元300。该太阳能电池单元300能够得到与上述各实施方式所涉及的太阳能电池单元相同的效果。Through the above steps, the solar cell 300 is manufactured. This solar battery cell 300 can obtain the same effect as the solar battery cell according to each of the above-mentioned embodiments.

另外,本实施方式中,在硅基板10上直接形成防反射膜16,但也可以在硅基板10与防反射膜16之间形成其他钝化膜。此时,可以在硅基板10上形成其他钝化膜,从其他钝化膜侧照射离子之后形成防反射膜16,也可以在硅基板10上形成其他钝化膜及防反射膜16之后从其他钝化膜及防反射膜16侧照射离子。In addition, in this embodiment, the antireflection film 16 is directly formed on the silicon substrate 10 , but another passivation film may be formed between the silicon substrate 10 and the antireflection film 16 . At this time, another passivation film can be formed on the silicon substrate 10, and the anti-reflection film 16 can be formed after irradiating ions from the side of the other passivation film. The passivation film and the antireflection film 16 side are irradiated with ions.

上述各实施方式所涉及的太阳能电池单元经由屏膜12或防反射膜16将离子照射(注入)到基板,由此无需过于降低能量就能够实现在基板表层上的浅接合。并且,由于不过于降低离子注入时的能量而完成,因此避免射束的传输效率的降低,且提高生产率。In the solar cell according to each of the above-mentioned embodiments, ions are irradiated (implanted) to the substrate via the screen film 12 or the antireflection film 16 , thereby enabling shallow junctions on the surface of the substrate without reducing energy too much. In addition, since ion implantation is completed without reducing the energy too much, reduction in beam transmission efficiency is avoided, and productivity is improved.

另外,掺杂浓度分布的峰位置并不一定在屏膜12或防反射膜16的内部。例如,发射极层形成工序中,也可以以如下能量照射离子,即离子的深度方向的浓度分布的峰位置成为直至屏膜12或防反射膜16与硅基板10的界面为止的深度D±10nm的范围。由此,被掺杂的离子的浓度分布的峰值存在于屏膜或防反射膜16与硅基板10之间的界面的附近,因此发电时载流子变得容易移动。In addition, the peak position of the doping concentration distribution is not necessarily inside the screen film 12 or the antireflection film 16 . For example, in the emitter layer forming step, ions may be irradiated with energy such that the peak position of the concentration distribution of the ions in the depth direction becomes the depth D±10 nm up to the interface between the screen film 12 or the antireflection film 16 and the silicon substrate 10. range. As a result, the peak of the concentration distribution of the doped ions exists near the interface between the screen film or the anti-reflection film 16 and the silicon substrate 10 , so that carriers can easily move during power generation.

以上,参考上述各实施方式对本发明进行了说明,但本发明并不限于上述实施方式,关于适当组合或替换各实施方式的结构的方式也包括在本发明中。并且,根据本领域的技术人员的知识,能够在各实施方式中的离子注入装置、传送容器等中将各种设计变更等变形追加到实施方式中,这种追加有变形的实施方式也包括在本发明的范围内。As mentioned above, although this invention was demonstrated with reference to said each embodiment, this invention is not limited to the above-mentioned embodiment, About the form which suitably combines or replaces the structure of each embodiment, it is also included in this invention. In addition, according to the knowledge of those skilled in the art, various modifications such as design changes can be added to the embodiments in the ion implantation apparatus, transfer container, etc. in each embodiment, and such embodiments with added modifications are also included in within the scope of the present invention.

上述各实施方式中,对硅基板上形成新的包覆膜的情况进行了说明,但也可以处理硅基板的表面而使表层部分变质为硅氧化膜,并以此作为包覆膜进行离子注入。In each of the above-mentioned embodiments, the case where a new coating film is formed on the silicon substrate has been described, but it is also possible to process the surface of the silicon substrate to modify the surface layer into a silicon oxide film, and perform ion implantation using this as a coating film. .

Claims (4)

1.一种太阳能电池单元的制造方法,其特征在于,包括:1. A method for manufacturing a solar cell unit, comprising: 准备工序,准备具有第1导电型的硅层和覆盖所述硅层的包覆膜的太阳能电池用基板;及a preparation step of preparing a solar cell substrate having a silicon layer of the first conductivity type and a coating film covering the silicon layer; and 发射极层形成工序,经由所述包覆膜朝向所述硅层照射第2导电型的离子,在所述硅层的受光面侧的一部分的区域形成发射极层,an emitter layer forming step of irradiating the silicon layer with ions of the second conductivity type through the coating film to form an emitter layer in a part of the light-receiving surface side of the silicon layer, 所述发射极层形成工序中,以所述离子的射程成为从所述包覆膜的表面到所述包覆膜与所述硅层的界面为止的距离的能量照射该离子。In the emitter layer forming step, the ions are irradiated with energy such that the range of the ions is the distance from the surface of the coating film to the interface between the coating film and the silicon layer. 2.根据权利要求1所述的太阳能电池单元的制造方法,其特征在于,2. The method of manufacturing a solar cell unit according to claim 1, wherein 所述包覆膜为防反射膜。The coating film is an anti-reflection film. 3.根据权利要求1所述的太阳能电池单元的制造方法,其特征在于,还包括:3. The method for manufacturing a solar cell unit according to claim 1, further comprising: 去除工序,在形成所述发射极层后去除所述包覆膜;及a removing step of removing the cover film after forming the emitter layer; and 防反射膜形成工序,在所述去除工序之后,在所述发射极层上形成防反射膜。An antireflection film forming step is to form an antireflection film on the emitter layer after the removal step. 4.一种太阳能电池单元的制造方法,其特征在于,包括:4. A method for manufacturing a solar cell unit, comprising: 准备工序,准备具有第1导电型的硅层和覆盖所述硅层的包覆膜的太阳能电池用基板;及a preparation step of preparing a solar cell substrate having a silicon layer of the first conductivity type and a coating film covering the silicon layer; and 发射极层形成工序,经由所述包覆膜朝向所述硅层照射第2导电型的离子,在所述硅层的受光面侧的一部分的区域形成发射极层,an emitter layer forming step of irradiating the silicon layer with ions of the second conductivity type through the coating film to form an emitter layer in a part of the light-receiving surface side of the silicon layer, 所述发射极层形成工序中,以如下能量照射该离子,即所述离子的深度方向的浓度分布的峰位置成为到所述包覆膜与所述硅层的界面为止的深度D±10nm的范围。In the emitter layer forming step, the ions are irradiated with energy such that the peak position of the concentration distribution of the ions in the depth direction becomes a depth D±10 nm from the interface between the coating film and the silicon layer. scope.
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