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CN101226968A - Method for reducing series resistance of concentrating solar cell and concentrating solar cell obtained by the method - Google Patents

Method for reducing series resistance of concentrating solar cell and concentrating solar cell obtained by the method Download PDF

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CN101226968A
CN101226968A CNA2007100077003A CN200710007700A CN101226968A CN 101226968 A CN101226968 A CN 101226968A CN A2007100077003 A CNA2007100077003 A CN A2007100077003A CN 200710007700 A CN200710007700 A CN 200710007700A CN 101226968 A CN101226968 A CN 101226968A
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electrode conductor
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solar cell
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易斌宣
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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
    • H10F77/00Constructional details of devices covered by this subclass
    • H10F77/20Electrodes
    • H10F77/206Electrodes for devices having potential barriers
    • H10F77/211Electrodes for devices having potential barriers for photovoltaic cells
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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
    • H10F19/00Integrated devices, or assemblies of multiple devices, comprising at least one photovoltaic cell covered by group H10F10/00, e.g. photovoltaic modules
    • H10F19/90Structures for connecting between photovoltaic cells, e.g. interconnections or insulating spacers
    • 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
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Abstract

本发明提供一种用于降低具有掺杂半导体材料本体的聚光太阳能电池的串联电阻的方法,使用该方法制造的聚光太阳能电池,具有掺杂半导体材料本体,通过以下步骤:在半导体本体光入射面制作可焊电极导体元件,背面制作可焊电极导体元件,其位置正好为与光入射面电极导体元件错开;背面的其他位置制作铝层作为背面场;在光反射面制作减反射薄膜;电极导体元件金属化烧结;沿半导体材料光入射面、及背面电极导体元件错开位置进行划片;最终形成具有低串联电阻的聚光太阳能电池。

Figure 200710007700

The invention provides a method for reducing the series resistance of a concentrated solar cell with a doped semiconductor material body, the concentrated solar cell manufactured by the method has a doped semiconductor material body, through the following steps: Make weldable electrode conductor elements on the incident surface, and weldable electrode conductor elements on the back, whose position is just staggered from the electrode conductor elements on the light incident surface; make aluminum layers on other positions on the back as the back field; make anti-reflection films on the light reflection surface; Metallization and sintering of the electrode conductor elements; scribing along the light incident surface of the semiconductor material and staggered positions of the electrode conductor elements on the back; finally forming a concentrated solar cell with low series resistance.

Figure 200710007700

Description

降低聚光太阳能电池串联电阻阻值的方法及由该方法获得的聚光太阳能电池 Method for reducing series resistance of concentrating solar cell and concentrating solar cell obtained by the method

技术领域technical field

本发明涉及用于降低具有掺杂半导体材料本体的聚光太阳能电池串联电阻阻值的方法;另外,本发明还涉及通过使用这种方法而制造出来的聚光太阳能电池,属于太阳能光伏发电领域。The invention relates to a method for reducing the series resistance of a concentrating solar cell with a doped semiconductor material body; in addition, the invention also relates to a concentrating solar cell manufactured by using the method, which belongs to the field of solar photovoltaic power generation.

背景技术Background technique

目前,由于高纯度单、多晶硅的生产技术垄断在几个国外高技术企业中,晶体硅的价格高居不下,而太阳能光伏发电系统需要大量的单、多晶硅,直接导致太阳能发电成本过高,目前太阳能光伏发电的成本大约4-5元/KwH,是火电成本的10倍左右,因而太阳能发电项目大面积推广应用受阻。At present, because the production technology of high-purity monocrystalline and polycrystalline silicon is monopolized by several foreign high-tech enterprises, the price of crystalline silicon remains high, and solar photovoltaic power generation systems require a large amount of monocrystalline and polycrystalline silicon, which directly leads to the high cost of solar power generation. The cost of photovoltaic power generation is about 4-5 yuan/KwH, which is about 10 times the cost of thermal power, so the large-scale promotion and application of solar power generation projects is hindered.

同时,国内外专家们已经研究发现,晶体硅光伏电池在正常的太阳光强下使用实际上是大材小用,因为晶体硅光伏电池可以承受更高的光强,发出的电流成比例增加而又不至于影响光伏电池寿命,如果通过几十倍甚至几百倍的聚光来提高光伏电池区域的光强,输出相同功率电流的光伏电池面积就能够大幅度缩小,这样一来,太阳能电池板晶体硅的使用量就能大幅度减少,太阳能光伏发电的成本就可以大幅度下降,接近风能发电或者水电的成本,达到用户能够接收的水平。At the same time, experts at home and abroad have found that the use of crystalline silicon photovoltaic cells under normal sunlight intensity is actually overkill, because crystalline silicon photovoltaic cells can withstand higher light intensity, and the emitted current increases proportionally without Affect the life of photovoltaic cells. If the light intensity of the photovoltaic cell area is increased by dozens or even hundreds of times of concentrated light, the area of the photovoltaic cell that outputs the same power current can be greatly reduced. In this way, the crystalline silicon of the solar panel The amount of usage can be greatly reduced, and the cost of solar photovoltaic power generation can be greatly reduced, approaching the cost of wind power generation or hydropower, and reaching a level that users can accept.

但是,人们通过实验发现,普通的太阳能电池在充分散热的情况下,用6倍聚光太阳光光强,可以得到4.8倍的功率输出,但是如果继续加大光强,发现其实际功率输出并没有继续成线性按比例增长。However, people have found through experiments that under the condition of sufficient heat dissipation, ordinary solar cells can obtain 4.8 times the power output with 6 times the intensity of concentrated sunlight, but if the light intensity continues to increase, it is found that the actual power output does not There is no continuing to scale linearly.

因此,研究具有高倍率聚光而功率输出能够同步增长的聚光太阳能电池成为光伏科学家的当前艰巨任务,科学家们想了不少的办法,比如刻槽埋栅技术、光刻细栅线、采用更好的半导体材料砷化镓等等。但是这些技术由于各种原因基本没有形成大规模生产,也就是说并没有比较好的经济价值。Therefore, researching concentrating solar cells with high-magnification concentrating power and synchronously increasing power output has become a difficult task for photovoltaic scientists. Better semiconductor material gallium arsenide and so on. However, due to various reasons, these technologies have basically not formed mass production, that is to say, they have no good economic value.

人们通过大量实验分析,研究得出结论:影响聚光太阳能电池的功率输出主要因素是串联电阻,即半导体的体电阻、表面方块电阻、以及电极导体电阻和电极与硅表面间的接触电阻等综合因素所组成;串联电阻越高,随着光强的升高,聚光电池的转换效率将下降越快。Through a large number of experimental analysis, the research concluded that the main factor affecting the power output of concentrating solar cells is the series resistance, that is, the volume resistance of the semiconductor, the surface square resistance, and the electrode conductor resistance and the contact resistance between the electrode and the silicon surface. The higher the series resistance, the faster the conversion efficiency of the concentrating cell will drop as the light intensity increases.

半导体的体电阻决定于半导体的材料选取,无法通过加工工艺的改善而改善;表面方块电阻也不是越低越好,表面方块电阻越低,其电子-空穴的复合速度也将呈指数倍率比例上升,不利于大量产生需要的光生电子-空穴对,因而该值也是有一定取值范围的,比如:20Ω/□-100Ω/□,常规的聚光太阳能电池产品可以做低一些,但不能够做得过低,而且这两个电阻相对于整个串联电阻的组成,占的比例比较小。The bulk resistance of a semiconductor depends on the material selection of the semiconductor, and cannot be improved by improving the processing technology; the lower the surface sheet resistance, the better, the lower the surface sheet resistance, the recombination speed of electrons and holes will also be exponentially proportional It is not conducive to a large number of photogenerated electron-hole pairs, so this value also has a certain value range, such as: 20Ω/□-100Ω/□, conventional concentrated solar cell products can be made lower, but not It can be made too low, and the proportion of these two resistors is relatively small relative to the composition of the entire series resistor.

如果需要有效地降低串联电阻的阻值,只有对“电极导体电阻”和“电极与硅表面间的接触电阻”进行改善,比如:①、使用更好的电极导电材料;②、加宽电极导体的宽度;③、采用刻槽埋栅技术;都能够有效减少电极导体电阻的阻值,从而达到减少串联电阻的目的;然而,1、使用更好的导电材料,将使制造成本迅速上升,而且降低的电阻阻值有限;2、对于目前常见的太阳能电池,基本的要求是电极导体元件应当尽可能窄,以便使光入射面部分受光面积最大化,被电极导体元件掩蔽的光入射面的比率越小,则电池的性能越好,一般电极导体元件的面积不超过太阳能电池总面积的10%;3、使用刻槽埋栅技术,即通过减少电极导体宽度,加大电极导体纵深,可以减少一些串联电阻,但同样增加了制造成本,而且目前的生产技术不足以支持大规模批量生产。If it is necessary to effectively reduce the resistance value of the series resistance, only the "electrode conductor resistance" and "contact resistance between the electrode and the silicon surface" can be improved, such as: ①, use better electrode conductive materials; ②, widen the electrode conductor ③. Adopting groove-buried gate technology; can effectively reduce the resistance value of the electrode conductor resistance, thereby achieving the purpose of reducing the series resistance; however, 1. Using better conductive materials will increase the manufacturing cost rapidly, and The reduced resistance resistance is limited; 2. For the current common solar cells, the basic requirement is that the electrode conductor element should be as narrow as possible, so as to maximize the light-receiving area of the light incident surface, and the ratio of the light incident surface covered by the electrode conductor element The smaller the battery, the better the performance of the battery. Generally, the area of the electrode conductor element does not exceed 10% of the total area of the solar cell; Some series resistors, but also increased manufacturing costs, and the current production technology is not enough to support large-scale batch production.

现在已经发现,使用简单的加宽电极导体元件宽度等技术,可以得到串联电阻比较小的聚光太阳能电池,但是电极元件加宽了,同时由电极遮盖的电池面积也增大了,并没有获得好的效果。It has now been found that using simple technologies such as widening the width of the electrode conductor element can obtain a concentrator solar cell with a relatively small series resistance, but the electrode element is widened, and the area of the cell covered by the electrode is also increased, which has not been obtained. Good results.

发明内容Contents of the invention

本发明涉及一种用于降低具有掺杂半导体材料本体的聚光太阳能电池的串联电阻阻值的方法,该本体具有两个主要相对面,该两个相对面形成具有一个可焊电极导体元件的光入射面和一个可焊电极导体元件的背面,其中,聚光太阳能电池的光入射面和背面都分别安装有可焊电极导体元件,光入射面以及背面的可焊电极导体元件刚好安置在聚光电池相对应的相对较长的两侧;该方法包括步骤:The invention relates to a method for reducing the resistance value of the series resistance of a concentrator solar cell having a body of doped semiconducting material, the body having two main opposing faces forming a solderable electrode conductor element The light incident surface and the back of a weldable electrode conductor element, wherein, the light incident surface and the back of the concentrator solar cell are respectively equipped with weldable electrode conductor elements, and the light incident surface and the back weldable electrode conductor element are just arranged on the concentrating solar cell. corresponding relatively long sides of the photocell; the method comprising the steps of:

a)提供具有p/n节的掺杂半导体本体;a) providing a doped semiconductor body having p/n junctions;

b)在半导体本体光入射面制作可焊电极导体元件,其规格为:可焊电极导体元件宽度0.2mm-0.8mm,电极导体元件长度为与半导体本体的宽度等同,相邻两条可焊电极导体元件之间间隔1.0mm-4mm,相邻两条可焊电极导体元件之间无导体连接;b) Make weldable electrode conductor elements on the light incident surface of the semiconductor body. The specifications are: the width of the weldable electrode conductor elements is 0.2mm-0.8mm, the length of the electrode conductor elements is equal to the width of the semiconductor body, and two adjacent weldable electrodes The distance between conductor elements is 1.0mm-4mm, and there is no conductor connection between two adjacent weldable electrode conductor elements;

c)在半导体本体背面制作可焊电极导体元件,其规格为:可焊电极导体元件宽度0.2mm-0.8mm,可焊电极导体元件长度为与半导体本体的宽度等同,相邻两条电极导体元件之间间隔1.0mm-4mm,其位置正好为与光入射面电极导体元件错开,并且保证所有可焊电极导体元件的错开位置均一致;c) Make weldable electrode conductor elements on the back of the semiconductor body, the specifications are: the width of the weldable electrode conductor elements is 0.2mm-0.8mm, the length of the weldable electrode conductor elements is equal to the width of the semiconductor body, and two adjacent electrode conductor elements The distance between them is 1.0mm-4mm, and its position is exactly staggered from the electrode conductor elements on the light incident surface, and the staggered positions of all weldable electrode conductor elements are guaranteed to be consistent;

d)在半导体本体背面的其他位置制作铝层作为背面场;d) making an aluminum layer at other positions on the back of the semiconductor body as a back field;

e)在光入射面制作减反射薄膜;e) making an anti-reflection film on the light incident surface;

f)电极导体元件金属化烧结;f) Metallization and sintering of electrode conductor elements;

g)使用激光划片机沿上、下可焊电极导体元件错开位置进行划片,形成独立的具有低串联电阻的聚光太阳能电池。g) Using a laser scribing machine to scribe along the staggered positions of the upper and lower weldable electrode conductor elements to form an independent concentrator solar cell with low series resistance.

当然,上述步骤(b、c、d、e)的制作顺序可以相对调整而不影响聚光太阳能电池最后的效果。Of course, the production sequence of the above steps (b, c, d, e) can be relatively adjusted without affecting the final effect of the concentrating solar cell.

另外,本发明涉及聚光太阳能电池,该电池包括掺杂半导体本体,该本体具有两个主要的相对面,该两个相对面形成具有一个可焊电极导体元件的光入射面和一个可焊电极导体元件的背面,其中,聚光太阳能电池的光入射面和背面都分别安装有可焊电极导体元件,可焊电极导体元件的宽度是0.2mm-0.8mm,可焊电极导体元件长度为与半导体本体的宽度等同,光入射面以及背面的电极导体元件刚好安置在聚光电池相对应的相对较长的两侧,整个聚光电池的宽度范围是1.2mm-4.8mm,最大长度则与制作聚光太阳能电池的半导体材料的宽度等同,实际的使用长度则根据实际需要来裁定。Furthermore, the invention relates to concentrator solar cells comprising a doped semiconductor body having two main opposing faces forming a light entrance face with a solderable electrode conductor element and a solderable electrode The back side of the conductor element, wherein, the light incident surface and the back side of the concentrator solar cell are respectively equipped with weldable electrode conductor elements, the width of the weldable electrode conductor element is 0.2mm-0.8mm, and the length of the weldable electrode conductor element is equal to that of the semiconductor The width of the main body is the same, and the light incident surface and the electrode conductor elements on the back are just placed on the relatively long sides of the concentrator cell. The width of the semiconductor material of the battery is the same, and the actual use length is determined according to the actual needs.

通过上述方法制造的聚光太阳能电池,半导体本体的光入射面的一侧和背面的另一侧将分别形成一条宽度与聚光太阳能电池长度相等的可焊电极导体元件,而可焊电极导体元件的长度最大值为仅0.8mm,即可焊电极导体元件的导电横截面积=半导体本体材料的宽度×电极导体元件的高度,因而其电阻值远远小于普通太阳能电池的电极导体元件的电阻值,电极导体元件的电阻几乎可以忽略不计,有效降低了聚光太阳能电池的整体串联电阻阻值;而且,由于聚光太阳能电池光入射面的可焊电极导体元件与另一块聚光太阳能电池的背面可焊电极导体元件焊接在一起,属于串联连接方式,即另一块聚光太阳能电池盖住了上一块聚光太阳能电池的电极导体元件,从表面上看,太阳光照射在聚光太阳能电池上的光入射面,无任何物体阻挡,全部被聚光太阳能电池所吸收,更加充分利用了太阳光资源,提高了聚光太阳能电池的发电效率。In the concentrating solar cell manufactured by the above method, one side of the light incident surface of the semiconductor body and the other side of the back will respectively form a weldable electrode conductor element with a width equal to the length of the concentrator solar cell, and the weldable electrode conductor element The maximum length is only 0.8mm, that is, the conductive cross-sectional area of the weldable electrode conductor element = the width of the semiconductor body material × the height of the electrode conductor element, so its resistance value is much smaller than that of the electrode conductor element of ordinary solar cells. , the resistance of the electrode conductor element is almost negligible, which effectively reduces the overall series resistance of the concentrating solar cell; The weldable electrode conductor components are welded together, which belongs to the series connection mode, that is, another concentrating solar cell covers the electrode conductor component of the previous concentrating solar cell. From the surface, the sunlight shining on the concentrating solar cell The incident surface of light is not blocked by any object, and all of it is absorbed by the concentrating solar cell, which makes full use of sunlight resources and improves the power generation efficiency of the concentrating solar cell.

附图说明:Description of drawings:

图1聚光太阳能电池各种投影面图;Fig. 1 Various projection plane diagrams of concentrating solar cells;

图1(a)是聚光太阳能电池的光入射正面图,光入射面4和正面可焊电极导体元件3;图1(b)是聚光太阳能电池的背面图,背面2和背面可焊电极导体元件1,其中背面2已经被蒸镀上一层绝缘薄膜材料;图1(c)是划片前两片聚光太阳能电池联结在一起的侧面状态,正面可焊电极导体元件3和背面可焊电极导体元件1刚好在5处被错开,激光划片机就在错开处5将聚光太阳能电池片划开,形成两个独立的聚光太阳能电池片;图1(d)是划片后两片聚光太阳能电池串联在一起的侧面状态,第一片聚光太阳能电池的正面可焊电极导体元件3和第二片聚光太阳能电池的背面可焊电极导体元件1已经牢牢地焊接在一起,由于可焊电极导电元件的宽度非常宽,等同于半导体材料的宽度,而且长度非常短,长度0.2mm-0.8mm,因而其可焊电极导体电阻可以忽略不计,同时第一块聚光太阳能电池光入射面的可焊电极导电元件3被第二块聚光太阳能电池所覆盖,图1(e)是10块聚光太阳能电池串联连接的平面图,从表面上看,只有聚光太阳能电池光入射面4暴露在太阳光下,没有任何电极导体元件覆盖,太阳光资源被100%的利用,提高了聚光太阳能电池的发电效率。Fig. 1 (a) is the light incident front view of concentrator solar cell, light incident surface 4 and front weldable electrode conductor element 3; Fig. 1 (b) is the back view of concentrator solar cell, back 2 and back weldable electrode Conductor element 1, wherein the back side 2 has been vapor-deposited with a layer of insulating film material; Figure 1 (c) is the side state of two concentrator solar cells connected together before scribing, and the front side can be soldered. The electrode conductor element 3 and the back side can be The welding electrode conductor element 1 is just staggered at position 5, and the laser scribing machine cuts the concentrating solar cell at the staggered position 5 to form two independent concentrating solar cells; Figure 1(d) is after scribing In the side state where two concentrating solar cells are connected in series, the front weldable electrode conductor element 3 of the first concentrating solar cell and the back weldable electrode conductor element 1 of the second concentrating solar cell have been firmly welded on the At the same time, since the width of the conductive element of the weldable electrode is very wide, which is equivalent to the width of the semiconductor material, and the length is very short, the length is 0.2mm-0.8mm, so the resistance of the weldable electrode conductor is negligible, and the first concentrated solar energy The weldable electrode conductive element 3 on the light incident surface of the battery is covered by the second concentrating solar cell. Fig. 1 (e) is a plan view of 10 concentrating solar cells connected in series. Seen from the surface, only the concentrating solar cell light The incident surface 4 is exposed to sunlight without any electrode conductor element covering, and the sunlight resource is utilized 100%, which improves the power generation efficiency of the concentrating solar cell.

实施方式:Implementation method:

本发明涉及对聚光太阳能电池的改进,这种聚光太阳能电池基于掺杂的半导体材料的本体如单晶硅片。本发明还涉及对准备这种聚光太阳能电池的可焊电极导体元件方法的改进。The present invention relates to improvements in concentrator solar cells based on bodies of doped semiconductor material, such as monocrystalline silicon wafers. The invention also relates to improvements in the method of preparing the solderable electrode-conductor elements of such concentrator solar cells.

根据优选实施案例,聚光太阳能电池是用掺杂的硅用作有源半导体设备制成的,取125mm×125mm的方形、厚度为220μm的常规直拉单晶硅片,这种晶片可以在市场上获得。According to a preferred embodiment, the concentrating solar cell is made of doped silicon as an active semiconductor device, and a conventional Czochralski monocrystalline silicon wafer with a square shape of 125 mm x 125 mm and a thickness of 220 μm is used. This wafer can be purchased in the market obtained on

通过蚀刻、构造以及清洗晶片等常规工艺,然后将该硅晶片的光入射面在800-900℃通过使用磷化合物,如POCl3掺杂,进行重扩散,将其制成n型并形成作为聚光太阳能电池的有源组分的基本p/n节,表面电阻的值为30Ω/□左右。Through conventional processes such as etching, structuring, and cleaning the wafer, and then the light incident surface of the silicon wafer is re-diffused at 800-900°C by doping with a phosphorus compound, such as POCl 3 , to make it n-type and form a poly The basic p/n node of the active component of the solar cell has a surface resistance value of about 30Ω/□.

通过掩膜,将可焊的银浆应用在掺杂半导体本体的光入射表面,形成若干条宽度为0.5mm,任意两条焊电极导体元件之间的净空为2mm,长度为125mm的可焊电极导体元件,而且相邻两条可焊电极导体元件之间没有任何导体连接。Apply the solderable silver paste on the light incident surface of the doped semiconductor body through a mask to form several solderable electrodes with a width of 0.5mm, a clearance of 2mm between any two soldering electrode conductor elements, and a length of 125mm. conductor elements, and there is no conductor connection between two adjacent weldable electrode conductor elements.

同样,通过掩膜,将可焊的银浆应用在掺杂半导体本体的背面,形成若干条宽度为0.5mm,两条之间的间隔为2mm,长度为125mm的可焊电极导体元件,掺杂半导体本体的背面可焊电极导体元件的位置刚好与光入射表面的可焊电极导体元件错开,并且所有可焊电极导体元件的错开位置均一致。Similarly, through a mask, solderable silver paste is applied to the back of the doped semiconductor body to form several solderable electrode conductor elements with a width of 0.5mm, an interval of 2mm between the two, and a length of 125mm. The positions of the solderable electrode conductor elements on the back surface of the semiconductor body are just staggered from those on the light incident surface, and the staggered positions of all the weldable electrode conductor elements are consistent.

在掺杂半导体本体的背面没有应用银浆的位置,蒸镀一层铝,用于生成背电场。On the back side of the doped semiconductor body where no silver paste is applied, a layer of aluminum is evaporated to generate a back electric field.

通常使用的高温烧结工艺方法等措施,应用于以上材料,使银浆牢固可靠连接在硅表面,并在背面形成背电场。The commonly used high-temperature sintering process and other measures are applied to the above materials, so that the silver paste is firmly and reliably connected to the silicon surface, and a back electric field is formed on the back.

采用常规的工艺方法在聚光太阳能电池的光入射表面沉积一层减反射薄膜。A layer of anti-reflection film is deposited on the light incident surface of the concentrating solar cell by using a conventional process method.

应用激光划片机,沿光入射面可焊电极导体元件和背面可焊电极导体元件的错开处划开,形成独立的长度为125mm,宽度为2.5mm的具有低串联电阻的聚光太阳能电池。Use a laser scribing machine to slit along the staggered part of the weldable electrode conductor element on the light incident surface and the back weldable electrode conductor element to form an independent concentrating solar cell with a length of 125mm and a width of 2.5mm with low series resistance.

聚光太阳能电池使用的半导体材料本体不但包含掺杂硅,还可以包含其它任何半导体材料,其他半导体材料的例子是砷化镓、磷化铟、硒化铜铟、锗以及氧化锌。The semiconductor material body used in concentrating solar cells not only contains doped silicon, but also any other semiconductor materials. Examples of other semiconductor materials are gallium arsenide, indium phosphide, copper indium selenide, germanium and zinc oxide.

可焊电极导体元件是自由电子流动的媒体,而且是聚光太阳能电池串联连接方式中一块聚光太阳能电池上表面与另一块聚光太阳能电池的下表面焊接之处,必须保证该元件的高导电性能和高可焊接性能,所用金属材料主要有铝、银、钛、镍等,或是这些金属的综合应用。The weldable electrode conductor component is the medium for free electron flow, and it is the place where the upper surface of one concentrating solar cell is welded to the lower surface of another concentrating solar cell in the series connection mode of concentrating solar cells, and the high conductivity of the component must be ensured Performance and high weldability, the metal materials used are mainly aluminum, silver, titanium, nickel, etc., or the comprehensive application of these metals.

Claims (9)

1.一种用于降低具有掺杂半导体材料本体的聚光太阳能电池的串联电阻阻值的方法,该本体具有两个主要相对面,该两个相对面形成具有一个可焊电极导体元件的光入射面和一个可焊电极导体元件的背面,其中,聚光太阳能电池的光入射面和背面都分别安装有可焊电极导体元件,光入射面以及背面的可焊电极导体元件刚好安置在聚光电池相对应的两侧;该方法包括步骤:1. A method for reducing the resistance value of the series resistance of a concentrator solar cell having a body of doped semiconductor material, the body having two main opposing faces forming a solar cell having a solderable electrode conductor element The incident surface and the back of a weldable electrode conductor element, wherein the light incident surface and the back of the concentrator solar cell are respectively equipped with weldable electrode conductor elements, and the light incident surface and the back weldable electrode conductor element are just placed on the concentrator cell. corresponding sides; the method comprises the steps of: a)提供具有p/n节的掺杂半导体本体;a) providing a doped semiconductor body having p/n junctions; b)在掺杂半导体本体光入射面制作可焊电极导体元件,其规格为:可焊电b) Make weldable electrode conductor components on the light incident surface of the doped semiconductor body, and its specifications are: weldable electric 极导体元件宽度0.2mm-0.8mm,可焊电极导体元件长度为与半导体本体的宽度等同,相邻两条可焊电极导体元件之间间隔1.0mm-4mm,相邻两条可焊电极导体元件之间无导体连接;The width of the pole conductor element is 0.2mm-0.8mm, the length of the weldable electrode conductor element is equal to the width of the semiconductor body, the distance between two adjacent weldable electrode conductor elements is 1.0mm-4mm, and the distance between two adjacent weldable electrode conductor elements There is no conductor connection between them; c)在掺杂半导体本体背面制作可焊电极导体元件,其规格为:可焊电极导体元件宽度0.2mm-0.8mm,可焊电极导体元件长度为与半导体本体的宽度等同,相邻两条可焊电极导体元件之间间隔1.0mm-4mm,其位置正好为与光入射面电极导体元件错开,并且保证所有可焊电极导体元件的错开位置均一致;c) Weldable electrode conductor elements are made on the back of the doped semiconductor body. The distance between the welding electrode conductor elements is 1.0mm-4mm, and its position is just staggered from the electrode conductor elements on the light incident surface, and the staggered positions of all weldable electrode conductor elements are guaranteed to be consistent; d)在掺杂半导体本体背面的其他位置制作铝层作为背面场;d) forming an aluminum layer at other positions on the backside of the doped semiconductor body as a backside field; e)在光入射面制作减反射薄膜;e) making an anti-reflection film on the light incident surface; f)电极导体元件金属化烧结;f) Metallization and sintering of electrode conductor elements; g)应用激光划片机沿掺杂半导体材料光入射面可焊电极导体元件及背面可焊电极导体元件错开位置进行划片,最终形成独立的具有低串联电阻的聚光太阳能电池;g) Use a laser scribing machine to scribe along the staggered positions of the weldable electrode conductor elements on the light incident surface of the doped semiconductor material and the weldable electrode conductor elements on the back side, and finally form an independent concentrator solar cell with low series resistance; 2.根据权利要求1所述的方法,其中步骤(b、c、d、e)的制作顺序可以作相对调整而不影响聚光太阳能电池最后的效果。2. The method according to claim 1, wherein the production sequence of steps (b, c, d, e) can be adjusted relatively without affecting the final effect of the concentrated solar cell. 3.根据权利要求1、2所述的方法,其中半导体材料本体包含硅、砷化镓、磷化铟、硒化铜铟、锗以及氧化锌构成的组中的一种。3. The method according to claim 1, 2, wherein the body of semiconductor material comprises one of the group consisting of silicon, gallium arsenide, indium phosphide, copper indium selenide, germanium and zinc oxide. 4.根据权利要求1、2、3所述的方法,其中可焊电极导体元件所用金属材料主要有铝、银、钛、镍等,或是这些金属的综合应用。4. The method according to claim 1, 2, 3, wherein the metal materials used for the weldable electrode conductor components mainly include aluminum, silver, titanium, nickel, etc., or a comprehensive application of these metals. 5.一种聚光太阳能电池,包括掺杂半导体本体,该本体具有两个主要的相对面,该两个相对面形成具有一个可焊电极导体元件的光入射面和一个可焊电极导体元件的背面,以及该掺杂半导体材料本体还在主要相对面之间具有多个侧面,其中,聚光太阳能电池的光入射面和背面都分别安装有可焊电极导体元件,可焊电极导体元件的宽度是0.2mm-0.8mm,可焊电极导体元件长度为与半导体本体的宽度等同,光入射面以及背面的可焊电极导体元件刚好安置在聚光电池相对应的较长的两侧,整个聚光电池的宽度是1.2mm-4.8mm,最大长度则与半导体材料的宽度等同,实际的使用长度则根据实际需要来裁定。5. A concentrator solar cell comprising a doped semiconductor body having two main opposing faces forming a light entrance face with a solderable electrode conductor element and a solderable electrode conductor element The back side, and the doped semiconductor material body also has a plurality of side faces between the main opposite sides, wherein the light incident side and the back side of the concentrator solar cell are respectively equipped with weldable electrode conductor elements, and the width of the weldable electrode conductor element is It is 0.2mm-0.8mm. The length of the weldable electrode conductor element is equal to the width of the semiconductor body. The weldable electrode conductor element on the light incident surface and the back is just placed on the corresponding longer sides of the concentrator cell. The entire concentrator cell The width is 1.2mm-4.8mm, and the maximum length is equal to the width of the semiconductor material. The actual length is determined according to actual needs. 6.根据权利要求5所述的聚光太阳能电池,其中半导体材料本体包含硅、砷化镓、磷化铟、硒化铜铟、锗以及氧化锌构成的组中的一种。6. The concentrated solar cell according to claim 5, wherein the semiconductor material body comprises one of the group consisting of silicon, gallium arsenide, indium phosphide, copper indium selenide, germanium and zinc oxide. 7.根据权利要求5、6所述的聚光太阳能电池,其中可焊电极导体元件所用金属材料主要有铝、银、钛、镍等,或是这些金属的综合应用。7. The concentrated solar cell according to claims 5 and 6, wherein the metal materials used for the weldable electrode conductor elements mainly include aluminum, silver, titanium, nickel, etc., or a comprehensive application of these metals. 8.根据权利要求5、6、7所述的聚光太阳能电池,其中半导体材料体是掺杂晶片。8. Concentrating solar cell according to claim 5, 6, 7, wherein the body of semiconductor material is a doped wafer. 9.用在权利要求1、2、3、4中任何一个所述的方法获得的聚光太阳能电池。9. Concentrating solar cells obtained by the method of any one of claims 1, 2, 3, and 4.
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