CN104091849B - Multi-junction solar cell and manufacturing method thereof - Google Patents
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Abstract
本发明提供一种多结太阳能电池,至少包括一底子电池和一位于所述底电池之上的顶子电池,所述顶子电池仅形成于所述底子电池的部分表面上以减少顶子电池的受光面积,当光线入射至该多结太阳能电池时,部分光线直接由顶子电池下面的其余子电池吸收,降低所述顶子电池的电流。
The present invention provides a multi-junction solar cell, comprising at least a bottom cell and a top sub-cell located on the bottom cell, the top sub-cell is only formed on a part of the surface of the bottom cell to reduce the number of top sub-cells When the light is incident on the multi-junction solar cell, part of the light is directly absorbed by the remaining sub-cells under the top sub-cell, reducing the current of the top sub-cell.
Description
技术领域technical field
本发明属于化合物半导体太阳能电池领域,具体涉及一种多结太阳能电池结构及其制备方法。The invention belongs to the field of compound semiconductor solar cells, and in particular relates to a multi-junction solar cell structure and a preparation method thereof.
背景技术Background technique
太阳能电池是一种利用光生伏特效应,将太阳能转化成电能的半导体器件,由一p型及n型半导体组合而成。当太阳光照射到器件时,能量大于半导体能隙的太阳光会被吸收,而使得半导体器件产生电子空穴对,接通后即形成电流。A solar cell is a semiconductor device that uses the photovoltaic effect to convert solar energy into electrical energy. It is composed of a p-type and n-type semiconductor. When sunlight irradiates the device, the sunlight with energy greater than the energy gap of the semiconductor will be absorbed, causing the semiconductor device to generate electron-hole pairs, which will form a current when it is turned on.
图1为太阳辐射光谱图,波长主要分布范围从0.3微米的紫外光到数微米的红外光,换算成光子能量,大约从0.4 eV到4 eV。为了能够更多吸收太阳光能量,多结太阳能电池被提出来,其将具有不同能隙的半导体元件堆叠在一起,如此可利用多种不同能隙的半导体材料层分别吸收不同能量的太阳光以增进光电转换效率。虽然以此种方式可增加能量吸收的带宽,但由于不同能隙的半导体材料层叠合在一起,顶层太阳能电池与底层太阳能电池各自产生的电流密度差异过大,此电流不匹配性,将导致整个元件光电转换效率减低,因此如何降低电流不匹配性是一个重要的议题。Figure 1 is a spectrum diagram of solar radiation. The main wavelength distribution ranges from ultraviolet light of 0.3 microns to infrared light of several microns. Converted into photon energy, it is approximately from 0.4 eV to 4 eV. In order to be able to absorb more sunlight energy, multi-junction solar cells have been proposed, which stack semiconductor elements with different energy gaps together, so that a variety of semiconductor material layers with different energy gaps can be used to absorb sunlight with different energies to Improve photoelectric conversion efficiency. Although the bandwidth of energy absorption can be increased in this way, due to the stacking of semiconductor material layers with different energy gaps, the current density difference between the top solar cell and the bottom solar cell is too large, and this current mismatch will cause the entire The photoelectric conversion efficiency of the device is reduced, so how to reduce the current mismatch is an important issue.
发明内容Contents of the invention
本发明的目的是提供一种可降低电流不匹配性进而提高光电转换效率的多结太阳能电池结构及其制备方法,其通过减少顶子电池的受光面积,降低顶子电池的电流,并将剩余的光留给下面的子电池来吸收,提高下面子电池的电流,最终达到多结子电池的电流匹配,从而实现多结电池效率的最优化。The purpose of the present invention is to provide a multi-junction solar cell structure and its preparation method which can reduce the current mismatch and improve the photoelectric conversion efficiency. The light is left for the lower sub-cells to absorb, increasing the current of the lower sub-cells, and finally achieving the current matching of the multi-junction sub-cells, thereby realizing the optimization of the efficiency of the multi-junction cells.
根据本发明的第一个方面,一种多结太阳能电池,至少包括一底子电池和一位于所述底电池之上的顶子电池,所述顶子电池仅形成于所述底子电池的部分表面上以减少顶子电池的受光面积,当光线入射至该多结太阳能电池时,部分光线直接由顶子电池下面的其余子电池吸收,降低所述顶子电池的电流。According to a first aspect of the present invention, a multi-junction solar cell includes at least a bottom cell and a top sub-cell located on the bottom cell, the top sub-cell is only formed on a part of the surface of the bottom sub-cell In order to reduce the light-receiving area of the top sub-cell, when light is incident on the multi-junction solar cell, part of the light is directly absorbed by the remaining sub-cells below the top sub-cell, reducing the current of the top sub-cell.
在一些实施例中,所述顶子电池的表面积占底子电池的70%~99%。In some embodiments, the surface area of the top sub-cell accounts for 70%-99% of that of the bottom sub-cell.
在一些实施例中,所述顶子电池具有沟槽图形,露出其下方子电池的表面,当光线入射至该沟槽图形时,由沟槽下方的子电池直接吸收。较佳的,所述沟槽图形的面积占总面积的1%~30%。较佳的,所述沟槽图形的深度不大于所述顶子电池的厚度。In some embodiments, the top sub-cell has a groove pattern exposing the surface of the sub-cell below it, and when the light is incident on the groove pattern, it is directly absorbed by the sub-cell below the groove. Preferably, the area of the groove pattern accounts for 1%-30% of the total area. Preferably, the depth of the groove pattern is not greater than the thickness of the top sub-cell.
在一些实施例中,所述的多结太阳能电池包括三结子电池,其从下到上分别为Ge第一子电池、GaAs第二子电池,GaInP第三子电池,其中所述第三子电池仅形成于第二子电池的部分表面上,所述第二子电池露出部分表面,当光线入射至该露出部分表面时直接由第二子电池吸收。较佳的,所述顶子电池的面积占中子电池的95%~99%。In some embodiments, the multi-junction solar cell includes three junction sub-cells, which are Ge first sub-cell, GaAs second sub-cell and GaInP third sub-cell respectively from bottom to top, wherein the third sub-cell It is only formed on a part of the surface of the second sub-battery, the part of the surface of the second sub-battery is exposed, and when the light is incident on the exposed part of the surface, it is directly absorbed by the second sub-battery. Preferably, the area of the top sub-cell accounts for 95%-99% of that of the neutron cell.
在一些实施例中,所述的多结太阳能电池包括四结子电池,其从下到上分别为Ge第一子电池、InGaAs第二子电池、InGaAsP或AlInGaAs第三子电池、AlInGaP第四子电池,其中所述第四子电池仅形成于第三子电池的部分表面上,所述第三子电池露出部分表面,当光线入射至该露出部分表面时直接由第三子电池吸收。In some embodiments, the multi-junction solar cell includes four-junction sub-cells, which are respectively Ge first sub-cell, InGaAs second sub-cell, InGaAsP or AlInGaAs third sub-cell, AlInGaP fourth sub-cell from bottom to top , wherein the fourth sub-cell is only formed on a part of the surface of the third sub-cell, and the exposed part of the surface of the third sub-cell is directly absorbed by the third sub-cell when light is incident on the exposed part of the surface.
根据本发明的第二个方面,一种多结太阳能电池的制备方法,包括依次沉积外延叠层,其包括一底子电池和一位于所述底电池之上的顶子电池,其特征在于:仅在所述底子电池的部分表面上形成顶子电池,以减少顶子电池的受光面积,当光线入射至该多结太阳能电池时,部分光线直接由顶子电池下面的其余子电池吸收,降低所述顶子电池的电流。According to a second aspect of the present invention, a method for preparing a multi-junction solar cell comprises sequentially depositing an epitaxial stack comprising a bottom subcell and a top subcell on top of the bottom cell, characterized in that only A top sub-cell is formed on part of the surface of the bottom sub-cell to reduce the light-receiving area of the top sub-cell. When light is incident on the multi-junction solar cell, part of the light is directly absorbed by the remaining sub-cells below the top sub-cell, reducing the light-receiving area of the top sub-cell. The current of the top sub-battery.
在一些实施例中,所述多结太阳能电池的制备方法,包括步骤:提供一衬底,在其上依次形成各结子电池,其至少包括底子电池和位于所述底子电池之上的顶子电池;在所述顶子电池形成沟槽图形,露出其下方子电池的表面,当光线入射至该沟槽图形时,由沟槽下方的子电池直接吸收。较佳的,所述形成的沟槽图形的面积占总面积的1%~30%。In some embodiments, the method for preparing a multi-junction solar cell includes the step of: providing a substrate on which each junction cell is sequentially formed, which at least includes a bottom cell and a top cell located on the bottom cell ; A groove pattern is formed on the top sub-cell, exposing the surface of the sub-cell below it, and when light is incident on the groove pattern, it is directly absorbed by the sub-cell below the groove. Preferably, the area of the formed groove pattern accounts for 1%-30% of the total area.
附图说明Description of drawings
图1为太阳辐射光谱图。Figure 1 is a solar radiation spectrum diagram.
图2为本发明第一实施例三结太阳能电池的侧面剖视图。FIG. 2 is a side cross-sectional view of a triple-junction solar cell according to the first embodiment of the present invention.
图3为图2所示三结太阳能电池的光吸收示意图。FIG. 3 is a schematic diagram of light absorption of the triple-junction solar cell shown in FIG. 2 .
图4为图2所示三结太阳能电池的沟槽图形。FIG. 4 is a groove pattern of the triple-junction solar cell shown in FIG. 2 .
图5为GaInP子电池的光谱响应曲线图。Fig. 5 is a graph of the spectral response of the GaInP sub-cell.
图6为GaAs子电池的光谱响应曲线图。Fig. 6 is a graph of the spectral response of the GaAs sub-cell.
图7为本发明第二实施例四结太阳能电池的侧面剖视图。7 is a side cross-sectional view of a four-junction solar cell according to a second embodiment of the present invention.
图8~11显示了本发明第二实施例四结太阳能电池制作过程中的结构剖视图。8 to 11 show cross-sectional views of the structure of the four-junction solar cell in the second embodiment of the present invention during the manufacturing process.
具体实施方式detailed description
本发明之多结太阳能电池通过减少顶子电池的受光面积,降低顶子电池的电流,并将剩余的光留给下面的子电池来吸收,提高下面子电池的电流,最终达到多结子电池的电流匹配,其可适用了任意多结电池,如GaInP / GaAs 双结电池、GaInP / GaAs / Ge 晶格匹配三结电池、GaInP/ InGaAs / InGaAs 三结电池、AlGaInP / InGaAsP / InGaAs /Ge 四结电池、GaInP / InGaAs / InGaAs / InGaAs 四结电池、GaInP / InGaAs /InGaNAsSb / Ge 四结电池、AlGaInP / AlGaAs / GaAs / InGaNAs / Ge 五结电池等。一般情况下,多结太阳能电池下面子电池的限流值为5% ~ 20%,故顶电池的的受光面积可以限定为总面积的70%~97%。下面结合具体实施例对本发明的实施方式做详细说明。The multi-junction solar cell of the present invention reduces the light-receiving area of the top sub-cell, reduces the current of the top sub-cell, and leaves the remaining light for the sub-cell below to absorb, increases the current of the bottom sub-cell, and finally reaches the multi-junction cell. Current matching, which is applicable to any multi-junction cells, such as GaInP / GaAs double-junction cells, GaInP / GaAs / Ge lattice-matched triple-junction cells, GaInP/ InGaAs / InGaAs triple-junction cells, AlGaInP / InGaAsP / InGaAs /Ge quadruple-junction cells Battery, GaInP / InGaAs / InGaAs / InGaAs four-junction battery, GaInP / InGaAs /InGaNAsSb / Ge four-junction battery, AlGaInP / AlGaAs / GaAs / InGaNAs / Ge five-junction battery, etc. In general, the current limiting value of the sub-cell under the multi-junction solar cell is 5%~20%, so the light-receiving area of the top cell can be limited to 70%~97% of the total area. The implementation of the present invention will be described in detail below in conjunction with specific examples.
图2显示了本发明第一实施例GaInP / GaAs / Ge三结太阳能电池100的侧面剖视图。FIG. 2 shows a side cross-sectional view of a GaInP/GaAs/Ge triple-junction solar cell 100 according to the first embodiment of the present invention.
请参看图2,三结太阳能电池100,包括p型Ge衬底110,Ge第一子电池120,GaAs第二子电池130,GaInP第三子电池140。一般的,第一、第二子电池之间、第二、第三子电池之间分别通过隧道结连接(图中未示出)。其中GaInP第三子电池140具有沟槽图形150,其露出其下方GaAs第二子电池130的部分表面130a。请参看附图3,当太阳能电池置于太阳光环境中,光线LA入射至第三子电池140的表面,由第三子电池吸收,光线LB入射至该沟槽图形时,直接由沟槽下方的GaAs第二子电池130吸收。Referring to FIG. 2 , the triple-junction solar cell 100 includes a p-type Ge substrate 110 , a first Ge sub-cell 120 , a second GaAs sub-cell 130 , and a third GaInP sub-cell 140 . Generally, the first and second sub-cells, and the second and third sub-cells are respectively connected through tunnel junctions (not shown in the figure). Wherein the third GaInP sub-cell 140 has a groove pattern 150, which exposes part of the surface 130a of the second GaAs sub-cell 130 below it. Please refer to accompanying drawing 3, when the solar cell is placed in the sunlight environment, the light L A is incident on the surface of the third sub-cell 140, absorbed by the third sub-cell, and when the light L B is incident on the groove pattern, it is directly absorbed by the groove pattern. The GaAs second subcell 130 below the trench absorbs.
请参看附图4,沟槽图形150可以由一系列彼此平行的沟槽组成,也可以由一系列彼此交叉的沟槽组成,还可以为一列系规则排列的圆形或方形的沟槽组成。较佳的,还可在沟槽图形150内填充透光性介电材料,如氮化硅、氧化硅等,保护第二子电池的同时保证第三子电池物理结构的完整性。Please refer to FIG. 4 , the groove pattern 150 may consist of a series of parallel grooves, or a series of intersecting grooves, or a series of regularly arranged circular or square grooves. Preferably, the trench pattern 150 can also be filled with a light-transmitting dielectric material, such as silicon nitride, silicon oxide, etc., to protect the second sub-cell while ensuring the integrity of the physical structure of the third sub-cell.
请参看附图5和6,其中图5显示了GaInP子电池的光谱响应曲线,图6显示了GaAs子电池的光谱响应曲线,从图中可看出,GaInP子电池对300nm~680nm波段光的光谱响应高于GaAs第二子电池,而一般GaInP/GaAs/Ge三结太阳能电池中第二子电池限流5%,因此沟槽图案的面积小于电池总面积的5%即可,一般为面积占比取95%~99%,较佳的取97%。Please refer to accompanying drawings 5 and 6, wherein Fig. 5 shows the spectral response curve of the GaInP sub-cell, and Fig. 6 shows the spectral response curve of the GaAs sub-cell. The spectral response is higher than that of the GaAs second sub-cell, and the current limit of the second sub-cell in a general GaInP/GaAs/Ge triple-junction solar cell is 5%, so the area of the groove pattern is less than 5% of the total area of the cell, generally the area The proportion is 95%~99%, preferably 97%.
图7显示了本发明第二实施例AlGaInP / InGaAsP / InGaAs / Ge四结太阳能电池200的侧面剖视图。FIG. 7 shows a side cross-sectional view of an AlGaInP/InGaAsP/InGaAs/Ge four-junction solar cell 200 according to the second embodiment of the present invention.
请参看附图7,四结太阳能电池200,包括p型Ge衬底210,Ge第一子电池220,p型InGaAs应力渐变层230,InGaAs第二子电池240,InGaAsP第三子电池250和AlInGaP第四子电池260,其中各结子电池之间通过一n++-GaAs/p++-GaAs隧道结连接(图中未示出)。其中AlGaInP第四子电池260具有沟槽图形270,其露出其下方InGaAsP第三子电池250的部分表面250a。下面结合制备方法对本实施例作详细说明。Please refer to accompanying drawing 7, four-junction solar cell 200, comprises p-type Ge substrate 210, Ge first sub-cell 220, p-type InGaAs stress gradient layer 230, InGaAs second sub-cell 240, InGaAsP third sub-cell 250 and AlInGaP The fourth sub-cell 260, wherein each junction sub-cell is connected through an n++-GaAs/p++-GaAs tunnel junction (not shown in the figure). Wherein the AlGaInP fourth sub-cell 260 has a groove pattern 270, which exposes part of the surface 250a of the InGaAsP third sub-cell 250 below it. The present embodiment will be described in detail below in conjunction with the preparation method.
首先,在MOCVD反应室沉积各结子电池的外延叠层,其包括生长第一子电池220、第二子电池240、第三子电池250及第四子电池260。具体如下:First, epitaxial stacks of each junction cell are deposited in the MOCVD chamber, which includes growing the first sub-cell 220 , the second sub-cell 240 , the third sub-cell 250 and the fourth sub-cell 260 . details as follows:
1)在p型Ge衬底210外延生长n型Ga0.5In0.5P窗口层,掺杂浓度5E18/cm3,形成Ge第一子电池220;1) An n-type Ga 0.5 In 0.5 P window layer is epitaxially grown on the p-type Ge substrate 210 with a doping concentration of 5E18/cm 3 to form the first Ge sub-cell 220 ;
2)在Ge第一子电池220上外延生长p型InGaAs应力渐变层230,保持TMGa流量不变,使In组分从0渐变到0.17,变化方式为阶梯型渐变,In组分每0.02左右为一阶梯,共9层,每一阶梯生长250nm;2) Epitaxially grow the p-type InGaAs stress gradient layer 230 on the Ge first sub-cell 220, keep the flow rate of TMGa constant, and make the In composition gradually change from 0 to 0.17, the change method is a stepwise gradient, and the In composition is about 0.02. One step, 9 layers in total, each step grows 250nm;
3)在p型InGaAs应力渐变层230上外延生长带隙为1.2eV的InGaAs第二子电池240,首先生长20nm的p型AlInGaAs背场层,再生长3µm厚,掺杂浓度为1×1017 cm-3的p型In0.17Ga0.83As基区,再生长200nm厚,掺杂浓度为2×1018cm-3的n型In0.17Ga0.83As发射层,最后生长50nm厚1×1018cm-3的n型InGaP窗口层;3) On the p-type InGaAs stress gradient layer 230, epitaxially grow the second InGaAs sub-cell 240 with a bandgap of 1.2eV, first grow a 20nm p-type AlInGaAs back field layer, and then grow a 3µm thick layer with a doping concentration of 1×10 17 cm -3 p-type In 0.17 Ga 0.83 As base region, then grow 200nm thick n-type In 0.17 Ga 0.83 As emission layer with a doping concentration of 2×10 18 cm -3 , and finally grow 50nm thick 1×10 18 cm -3 n-type InGaP window layer;
4)在InGaAs第二子电池240上外延生长带隙为1.55eV的InGaAsP第三子电池250,首先生长20nm的p型AlInGaAs背场层,再生长3µm厚,掺杂浓度为1×1017 cm-3的p型In0.27Ga0.73As0.49P0.51基区,再生长300nm厚,掺杂浓度为2×1018cm-3的n型In0.27Ga0.73As0.49P0.51发射层,最后生长50nm厚1×1018cm-3的n型AlInP窗口层;4) Epitaxially grow the third InGaAsP sub-cell 250 with a band gap of 1.55eV on the second InGaAs sub-cell 240, first grow a 20nm p-type AlInGaAs back field layer, and then grow a 3µm thick doping concentration of 1×10 17 cm -3 p-type In 0.27 Ga 0.73 As 0.49 P 0.51 base region, and then grow 300nm thick, doping concentration of 2×10 18 cm -3 n-type In 0.27 Ga 0.73 As 0.49 P 0.51 emitter layer, finally grow 50nm thick 1×10 18 cm -3 n-type AlInP window layer;
5)在InGaAsP第三子电池250上外延生长带隙为1.85eV的AlInGaP第四子电池260,首先生长100nm的p型InAlGaAs背场层,再生长600nm厚,掺杂浓度为6×1016 cm-3的p型AlInGaP基区,再生长150nm厚,掺杂浓度为5×1018cm-3的n型AlInGaP发射层,最后生长50nm厚5×1018cm-3的n型AlInP窗口层,从而在Ge衬底上完成AlGaInP /InGaAsP/ InGaAs/Ge晶格失配四结太阳能电池,其侧面剖视图如图8所示。5) Epitaxially grow the fourth AlInGaP sub-cell 260 with a bandgap of 1.85eV on the third InGaAsP sub-cell 250, first grow a 100nm p-type InAlGaAs back field layer, and then grow a 600nm thick layer with a doping concentration of 6×10 16 cm -3 p-type AlInGaP base region, then grow an n-type AlInGaP emission layer with a thickness of 150nm and a doping concentration of 5×10 18 cm -3 , and finally grow an n-type AlInP window layer with a thickness of 50nm and a thickness of 5×10 18 cm -3 , Thus, an AlGaInP/InGaAsP/InGaAs/Ge lattice-mismatched four-junction solar cell is completed on a Ge substrate, and its side cross-sectional view is shown in FIG. 8 .
其次,在AlInGaP第四子电池260上形成沟图形270,露出其下方InGaAsP第三子电池250的部分表面250a。具体如下:请参看附图9,使用光刻工艺,在AlInGaP第四子电池260表面制作光刻图形280;然后采用化学蚀刻去除没有光刻胶保护的AlGaInP第四子电池260,形成沟槽270,如图10所示;去除四结电池上的光刻胶280,最终获得沟槽式AlGaInP/InGaAsP/ InGaAs/Ge晶格失配四结电池,如图11所示。Next, a groove pattern 270 is formed on the AlInGaP fourth sub-cell 260, exposing part of the surface 250a of the InGaAsP third sub-cell 250 below it. The details are as follows: please refer to accompanying drawing 9, use photolithography process, make photolithography pattern 280 on the surface of AlInGaP fourth sub-cell 260; then use chemical etching to remove AlGaInP fourth sub-cell 260 without photoresist protection, and form groove 270 , as shown in FIG. 10 ; remove the photoresist 280 on the four-junction cell, and finally obtain a trench AlGaInP/InGaAsP/InGaAs/Ge lattice-mismatched four-junction cell, as shown in FIG. 11 .
在本实施例中,分别制作了两种样品,对两样品的外量子效率进行测试,两样品均为AlGaInP/InGaAsP/ InGaAs/Ge四结太阳能电池,其中样品1的第四子电池260完全覆盖第三子电池250,即没有沟槽图案,样品2的第四子电池260仅覆盖第三子电池250的部分表面,即设有沟槽图案(面积约20%),露出部分第三子电池250的部分表面。测试结果如下表:In this embodiment, two samples were produced respectively, and the external quantum efficiencies of the two samples were tested. Both samples were AlGaInP/InGaAsP/InGaAs/Ge four-junction solar cells, and the fourth sub-cell 260 of sample 1 completely covered The third sub-cell 250 has no groove pattern, and the fourth sub-cell 260 of sample 2 only covers part of the surface of the third sub-cell 250, that is, it has a groove pattern (about 20% of the area), exposing part of the third sub-cell 250 part surface. The test results are as follows:
从上表可看出,样品1的InGaAsP第三结子电池限流严重,其主要原因为AlGaInP第四子电池带隙较低导致的,而样品2(即本实施例之四结太阳能电池)在保证电池其它性能参数不变的情况下实现了子电池间电流匹配,其在1000倍聚光测试条件下的转换效率达到44.1%。It can be seen from the above table that the current limitation of the InGaAsP third-junction sub-cell of sample 1 is serious, which is mainly caused by the lower band gap of the AlGaInP fourth sub-cell, while sample 2 (that is, the four-junction solar cell of this embodiment) is in The current matching between the sub-cells was realized while keeping other performance parameters of the battery unchanged, and the conversion efficiency reached 44.1% under the test conditions of 1000 times concentrated light.
惟以上所述者,仅为本发明之较佳实施例而已,当不能以此限定本发明实施之范围,即大凡依本发明申请专利范围及专利说明书内容所作之简单的等效变化与修饰,皆仍属本发明专利涵盖之范围内。But the above-mentioned ones are only preferred embodiments of the present invention, and should not limit the scope of implementation of the present invention with this, that is, all simple equivalent changes and modifications made according to the patent scope of the present invention and the content of the patent specification, All still belong to the scope covered by the patent of the present invention.
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