CN105428430A - Multi-junction GaAs solar cell surface grid line structure - Google Patents
Multi-junction GaAs solar cell surface grid line structure Download PDFInfo
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10F—INORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
- H10F77/00—Constructional details of devices covered by this subclass
- H10F77/20—Electrodes
- H10F77/206—Electrodes for devices having potential barriers
- H10F77/211—Electrodes for devices having potential barriers for photovoltaic cells
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10F—INORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
- H10F77/00—Constructional details of devices covered by this subclass
- H10F77/10—Semiconductor bodies
- H10F77/12—Active materials
- H10F77/124—Active materials comprising only Group III-V materials, e.g. GaAs
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- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E10/00—Energy generation through renewable energy sources
- Y02E10/50—Photovoltaic [PV] energy
- Y02E10/544—Solar cells from Group III-V materials
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Abstract
本发明公开了一种多结GaAs太阳电池表面栅线结构,包括太阳电池,所述太阳电池表面的有效受光区域呈圆形,所述太阳电池上、有效受光区域之外的部分为主栅线,在所述有效受光区域内设置有以太阳电池中点为中心呈放射状均匀分布的若干细栅线,射入到有效受光区域的光能有效倍转换为电能,光电转换的电流通过细栅线进行收集后传至主栅线上。本发明采用圆形的受光面积设计,对于光学系统如一些球形或非球形曲面光学系统所汇聚的光斑形状为近似圆形的情况,其太阳电池的有效利用率得到了提高,同时,由于放射状细栅线的设计,使得越靠近受光区域中心的细栅线的密度越大,这就增加了对中心高光强区域所产生的高电流密度的收集和载流能力,提高了太阳电池的效率。
The invention discloses a grid line structure on the surface of a multi-junction GaAs solar cell, including a solar cell, the effective light-receiving area on the surface of the solar cell is circular, and the part outside the effective light-receiving area on the solar cell is the main grid line In the effective light-receiving area, a number of fine grid lines are arranged radially and evenly distributed around the center of the solar cell. After being collected, it is transmitted to the busbar. The present invention adopts a circular light-receiving area design. For the case where the spot shape of the optical system such as some spherical or aspherical curved surface optical systems converges is approximately circular, the effective utilization rate of the solar cell has been improved. At the same time, due to the radial The design of the grid lines makes the density of the thin grid lines closer to the center of the light-receiving area greater, which increases the collection and current-carrying capacity of the high current density generated by the central high-light-intensity area, and improves the efficiency of the solar cell.
Description
技术领域 technical field
本发明属于太阳能利用技术领域,特别涉及一种多结GaAs太阳电池表面栅线结构。 The invention belongs to the technical field of solar energy utilization, and in particular relates to a grid line structure on the surface of a multi-junction GaAs solar cell.
背景技术 Background technique
太阳能具有清洁、无资源地域限制、对人类来说永无枯竭等优良特性,越来越受到人们的青睐,其中太阳能光伏利用即太阳光通过光伏器件直接转换成电能的技术尤其引人注目。 Solar energy has excellent characteristics such as cleanness, no geographical limitation of resources, and inexhaustibility for human beings. It is more and more popular among people. Among them, the technology of solar photovoltaic utilization, that is, the direct conversion of sunlight into electrical energy through photovoltaic devices, is particularly eye-catching.
传统的光伏太阳电池组件中,太阳电池使用量比较大,致使光伏发电的发电成本较常规发电成本高出数倍,因此限制了光伏发电技术的规模化应用,制约了整个行业的发展。为了节约太阳电池的使用量,降低光伏太阳电池组件的生产成本,在现有光伏太阳电池组件中多采用聚光的技术手段,使光线汇聚后再照射到高效率的多结太阳电池上,以减小太阳电池的用量。 In traditional photovoltaic solar cell modules, the use of solar cells is relatively large, resulting in the cost of photovoltaic power generation being several times higher than conventional power generation costs, thus limiting the large-scale application of photovoltaic power generation technology and restricting the development of the entire industry. In order to save the usage of solar cells and reduce the production cost of photovoltaic solar cell components, light concentrating technology is often used in existing photovoltaic solar cell components, so that the light is concentrated and then irradiated on high-efficiency multi-junction solar cells to Reduce the amount of solar cells used.
如图1所示,目前市面的多结太阳电池所设计的受光面积一般为矩形,其主栅线3分布在两侧,而电池中间有许多用于收集光生电流的细栅线4,且细栅线呈均匀排布,通过主栅线与其他太阳电池进行串并联结合,得到所需的电压和电流。这种设计针对通过聚光系统后形成的方形均匀光斑比较合理,但是另外一些光学系统如一些球形或非球形曲面光学系统实际所汇聚的光斑6形状为近似圆形,且其光斑的能量分布并不均匀,一般呈现中心强,边缘弱的趋势,因此这种矩形的受光区域的设计并不能有效收集光生电流,反而会由于光斑的不均匀,中心区域栅线对电流的收集能力较差而导致电池效率的损失,如图2所示,经过聚光系统后的近圆形光斑照射到太阳电池表面时,可以看到此种情况下,太阳电池表面的受光面积利用率不高,且受光面积中心区域的光强极大,而边缘处较弱,而该种设计的细栅线是均匀分布的,因此会造成中心光强处细栅线承载的电流密度较大,从而造成效率损失。同时由于采用MOCVD工艺生产的多结太阳电池的成本非常高,而受光面积的利用率低造成了成本的升高。 As shown in Figure 1, the light-receiving area of the multi-junction solar cell currently on the market is generally rectangular, and its main grid lines 3 are distributed on both sides, and there are many thin grid lines 4 for collecting photo-generated current in the middle of the cell, and the thin The grid lines are evenly arranged, and are combined with other solar cells in series and parallel through the main grid lines to obtain the required voltage and current. This design is more reasonable for the square uniform light spot formed after passing through the light-condensing system, but the shape of the light spot 6 actually converged by some other optical systems such as some spherical or aspherical curved surface optical systems is approximately circular, and the energy distribution of the light spot is not the same. Unevenness, generally showing a trend of strong center and weak edge, so the design of this rectangular light-receiving area cannot effectively collect photo-generated current. The loss of cell efficiency, as shown in Figure 2, when the near-circular light spot after the concentrating system is irradiated on the surface of the solar cell, it can be seen that in this case, the utilization rate of the light-receiving area on the surface of the solar cell is not high, and the light-receiving area The light intensity in the central area is extremely high, while the edge is weaker, and the thin grid lines in this design are evenly distributed, so the current density carried by the thin grid lines at the center light intensity is relatively large, resulting in efficiency loss. At the same time, the cost of multi-junction solar cells produced by the MOCVD process is very high, and the low utilization rate of the light-receiving area leads to an increase in cost.
发明内容 Contents of the invention
本发明的目的在于:针对上述存在的问题,提供一种能够提高太阳电池有效利用率以及对电流收集及载流能力的多结GaAs太阳电池表面栅线结构。 The purpose of the present invention is to provide a multi-junction GaAs solar cell surface grid structure capable of improving the effective utilization rate of the solar cell and the current collection and carrying capacity in view of the above existing problems.
本发明的技术方案是这样实现的:一种多结GaAs太阳电池表面栅线结构,包括太阳电池,其特征在于:所述太阳电池表面的有效受光区域呈圆形,所述太阳电池上、有效受光区域之外的部分为主栅线,在所述有效受光区域内设置有以太阳电池中点为中心呈放射状均匀分布的若干细栅线,射入到有效受光区域的光能有效倍转换为电能,光电转换的电流通过细栅线进行收集后传至主栅线上。 The technical scheme of the present invention is achieved in the following way: a multi-junction GaAs solar cell surface grid line structure, including a solar cell, is characterized in that: the effective light-receiving area on the surface of the solar cell is circular, and on the solar cell, the effective The part outside the light-receiving area is the main grid line. In the effective light-receiving area, a number of fine grid lines are arranged radially and uniformly distributed around the center of the solar cell, and the light energy injected into the effective light-receiving area is effectively converted into Electric energy and photoelectric conversion current are collected through the thin grid lines and then transmitted to the main grid lines.
本发明所述的多结GaAs太阳电池表面栅线结构,其在所述太阳电池的中心位置设置有中心圆环细栅线,所述中心圆环细栅线内对应的太阳电池上未设置有细栅线,呈放射状的若干细栅线均与中心圆环细栅线连接。 According to the multi-junction GaAs solar cell surface grid line structure of the present invention, a central ring thin grid line is arranged at the center of the solar cell, and the corresponding solar cell in the central ring thin grid line is not provided with Thin grid lines, several thin grid lines in a radial shape are all connected with the central circular ring thin grid lines.
本发明采用圆形的受光面积设计,对于光学系统如一些球形或非球形曲面光学系统所汇聚的光斑形状为近似圆形的情况,其太阳电池的有效利用率得到了提高,同时,由于放射状细栅线的设计,使得越靠近受光区域中心的细栅线的密度越大,这就增加了对中心高光强区域所产生的高电流密度的收集和载流能力,提高了太阳电池的效率。 The present invention adopts a circular light-receiving area design. For the case where the spot shape of the optical system such as some spherical or aspherical curved surface optical systems converges is approximately circular, the effective utilization rate of the solar cell has been improved. At the same time, due to the radial The design of the grid lines makes the density of the thin grid lines closer to the center of the light-receiving area greater, which increases the collection and current-carrying capacity of the high current density generated by the central high-light-intensity area, and improves the efficiency of the solar cell.
附图说明 Description of drawings
图1是现有多结太阳电池表面栅线的结构示意图。 FIG. 1 is a schematic diagram of the structure of grid lines on the surface of an existing multi-junction solar cell.
图2是呈圆形的聚光光斑照射在现有多结太阳电池上的示意图。 Fig. 2 is a schematic diagram of a circular concentrated light spot irradiating an existing multi-junction solar cell.
图3是本发明的结构示意图。 Fig. 3 is a structural schematic diagram of the present invention.
图4是呈圆形的聚光光斑照射在本发明太阳电池上的示意图。 Fig. 4 is a schematic diagram of a circular concentrated light spot irradiating on the solar cell of the present invention.
图中标记:1为太阳电池,2为有效受光区域,3为主栅线,4为细栅线,5为中心圆环细栅线,6为光斑。 Marks in the figure: 1 is the solar cell, 2 is the effective light-receiving area, 3 is the main grid line, 4 is the thin grid line, 5 is the central ring thin grid line, and 6 is the light spot.
具体实施方式 detailed description
下面结合附图,对本发明作详细的说明。 Below in conjunction with accompanying drawing, the present invention is described in detail.
为了使本发明的目的、技术方案及优点更加清楚明白,以下结合附图及实施例,对本发明进行进一步详细说明。应当理解,此处所描述的具体实施例仅仅用以解释本发明,并不用于限定本发明。 In order to make the object, technical solution and advantages of the present invention clearer, the present invention will be further described in detail below in conjunction with the accompanying drawings and embodiments. It should be understood that the specific embodiments described here are only used to explain the present invention, not to limit the present invention.
如图3和4所示,一种多结GaAs太阳电池表面栅线结构,包括太阳电池1,所述太阳电池1表面的有效受光区域2呈圆形,对于光学系统如一些球形或非球形曲面光学系统所汇聚的光斑6形状为近似圆形的情况,能够使太阳电池的有效利用率得到提高;所述太阳电池1上、有效受光区域2之外的部分为主栅线3,在所述有效受光区域2内设置有以太阳电池1中点为中心呈放射状均匀分布的若干细栅线4,射入到有效受光区域2的光能有效倍转换为电能,光电转换的电流通过细栅线4进行收集后传至主栅线3上,由于放射状细栅线的布置方式,使得越靠近受光区域中心,细栅线的密度越大,对于光斑的能量分布呈现中心强而边缘弱的趋势情况,这样增加了太阳电池表面细栅线对中心高光强区域所产生的高电流密度的收集和载流能力,从而提高了太阳电池的效率。 As shown in Figures 3 and 4, a grid line structure on the surface of a multi-junction GaAs solar cell includes a solar cell 1, and the effective light-receiving area 2 on the surface of the solar cell 1 is circular, for optical systems such as some spherical or aspherical curved surfaces When the shape of the light spot 6 converged by the optical system is approximately circular, the effective utilization rate of the solar cell can be improved; The effective light-receiving area 2 is provided with a number of thin grid lines 4 that are evenly distributed radially around the center of the solar cell 1. The light energy incident on the effective light-receiving area 2 is effectively converted into electrical energy, and the photoelectrically converted current passes through the thin grid lines. 4 After collecting, it is transmitted to the main grid line 3. Due to the arrangement of the radial thin grid lines, the closer to the center of the light-receiving area, the greater the density of the thin grid lines, and the energy distribution of the spot shows a tendency that the center is strong and the edge is weak. , which increases the collection and carrying capacity of the high current density generated by the thin grid lines on the surface of the solar cell to the high light intensity area in the center, thereby improving the efficiency of the solar cell.
其中,在所述太阳电池1的中心位置设置有中心圆环细栅线5,所述中心圆环细栅线5内对应的太阳电池1上未设置有细栅线,呈放射状的若干细栅线4均与中心圆环细栅线5连接。因为汇聚后的光斑中心光强极高,而细栅线在中心区域形成交叉结合点,由于细栅线对入射到太阳电池表面的汇聚光具有反射作用,而中心的光强又极高,这样就会导致细栅线在受光面积中心的交叉结合点对高强度的入射光有较明显的反射作用。通过将太阳电池的中心区域设计成空白区域,即中心圆环细栅线内未设置细栅线,有利于减少细栅线对入射光的反射效果,同时由于中心圆环细栅线的环绕,也能保证对中心区域所产生的光生电流的收集,从而可以进一步提高太阳电池的效率。 Wherein, at the central position of the solar cell 1, a central ring thin grid line 5 is arranged, and the corresponding solar cell 1 in the central ring ring thin grid line 5 is not provided with a thin grid line, and several thin grid lines in a radial shape The wires 4 are all connected with the thin grid wires 5 of the central ring. Because the light intensity in the center of the converged light spot is extremely high, and the thin grid lines form a cross junction in the central area, because the thin grid lines reflect the concentrated light incident on the surface of the solar cell, and the light intensity in the center is extremely high, so It will cause the cross joint point of the fine grid lines in the center of the light-receiving area to have a more obvious reflection effect on high-intensity incident light. By designing the central area of the solar cell as a blank area, that is, there is no thin grid line in the central ring thin grid line, it is beneficial to reduce the reflection effect of the thin grid line on incident light, and because the central ring thin grid line surrounds, It can also ensure the collection of the photo-generated current generated in the central area, so that the efficiency of the solar cell can be further improved.
以上所述仅为本发明的较佳实施例而已,并不用以限制本发明,凡在本发明的精神和原则之内所作的任何修改、等同替换和改进等,均应包含在本发明的保护范围之内。 The above descriptions are only preferred embodiments of the present invention, and are not intended to limit the present invention. Any modifications, equivalent replacements and improvements made within the spirit and principles of the present invention should be included in the protection of the present invention. within range.
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