CN111341872B - Gallium arsenide solar cell epitaxial structure and growth method thereof - Google Patents
Gallium arsenide solar cell epitaxial structure and growth method thereof Download PDFInfo
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Abstract
本发明涉及一种砷化镓太阳能电池外延结构及其生长方法,所述电池包括依次层叠设置的Ge底电池、GaAs中电池和GaInP顶电池,所述GaAs中电池和所述GaInP顶电池中均包括背层和发射层;所述GaAs中电池的背层包括delta掺杂的p型GaInP层,发射层包括delta掺杂的n型GaAs层;所述GaInP顶电池的背层包括delta掺杂的p型GaInP层,发射层包括delta掺杂的n型GaInP层。本发明的太阳能电池外延结构,中电池、顶电池的背层及发射层均有进行delta掺杂生长,这种delta掺杂结构能阻断晶体位错延伸、抑制晶体缺陷蔓延,提高太阳能电池外延结构的可靠性及光电转换效率。
The invention relates to an epitaxial structure of a gallium arsenide solar cell and a growth method thereof. The cell comprises a Ge bottom cell, a GaAs middle cell and a GaInP top cell that are stacked in sequence, wherein the GaAs middle cell and the GaInP top cell are both It includes a back layer and an emission layer; the back layer of the GaAs middle cell includes a delta-doped p-type GaInP layer, and the emission layer includes a delta-doped n-type GaAs layer; the back layer of the GaInP top cell includes a delta-doped The p-type GaInP layer, and the emission layer includes a delta-doped n-type GaInP layer. In the solar cell epitaxial structure of the present invention, the back layer and the emission layer of the middle cell and the top cell are all grown by delta doping. This delta doping structure can block the extension of crystal dislocations, inhibit the spread of crystal defects, and improve the epitaxy of the solar cell. Structure reliability and photoelectric conversion efficiency.
Description
技术领域technical field
本发明涉及太阳能电池技术领域,具体涉及一种砷化镓太阳能电池外延结构。The invention relates to the technical field of solar cells, in particular to an epitaxial structure of a gallium arsenide solar cell.
背景技术Background technique
三结砷化镓太阳能电池光谱响应性好,光电转换效率高,通常应用在航空航天及聚光光伏电站等领域。目前较常见的三结砷化镓太阳能电池为Ge底电池、GaAs中电池及GaInP顶电池结构,其能带从下往上依次升高,分别吸收不同波长的光,从而实现全光谱吸收。但目前的三结砷化镓电池其各底电池均采用直接掺杂生长法,即同时通生长源及掺杂源来进行生长,这种生长法会给外延结构带来一定量的缺陷,使其晶体质量受到影响,从而影响光电转换性能及其可靠性。Three-junction GaAs solar cells have good spectral responsiveness and high photoelectric conversion efficiency, and are usually used in aerospace and concentrating photovoltaic power stations. At present, the more common triple-junction GaAs solar cells are Ge bottom cell, GaAs middle cell and GaInP top cell structure, and their energy bands increase sequentially from bottom to top, respectively absorbing light of different wavelengths, thereby achieving full-spectrum absorption. However, the bottom cells of the current triple-junction gallium arsenide cells all use the direct doping growth method, that is, the growth source and the doping source are used for growth at the same time. This growth method will bring a certain amount of defects to the epitaxial structure, making the Its crystal quality is affected, thereby affecting the photoelectric conversion performance and its reliability.
发明内容SUMMARY OF THE INVENTION
本发明的目的是提供一种砷化镓太阳能电池外延结构,包括依次层叠设置的Ge底电池、GaAs中电池和GaInP顶电池,所述GaAs中电池和所述GaInP顶电池中均包括背层和发射层;The purpose of the present invention is to provide a gallium arsenide solar cell epitaxial structure, including a Ge bottom cell, a GaAs middle cell and a GaInP top cell that are stacked in sequence, wherein the GaAs middle cell and the GaInP top cell both include a back layer and a GaInP top cell. emission layer;
所述GaAs中电池的背层包括delta掺杂的p型GaInP层,发射层包括delta掺杂的n型GaAs层;所述GaInP顶电池的背层包括delta掺杂的p型GaInP层,发射层包括delta掺杂的n型GaInP层。The back layer of the GaAs middle cell includes a delta-doped p-type GaInP layer, and the emission layer includes a delta-doped n-type GaAs layer; the back layer of the GaInP top cell includes a delta-doped p-type GaInP layer, and the emission layer includes a delta-doped p-type GaInP layer. A delta-doped n-type GaInP layer is included.
对于Ge底电池、GaAs中电池和GaInP顶电池复合电池而言,可进行delta掺杂的有中电池和顶电池,而对于中电池和顶电池而言,其中一般包括背层、基区和发射层等多个结构,若想通过delta掺杂的方式来改善电池的性能,可选择的方式有多种,如可仅在中电池或顶电池中进行delta掺杂,也可对两个电池均进行delta掺杂,可仅掺杂背层、或发射层中的一部分,也可对其全部进行delta掺杂。本发明发现,对中电池和顶电池中的背层均进行掺杂,并且,基层和发射层中结构不完全是delta掺杂层时,可明显地改善电池的结构,提高电池的效率。For Ge bottom cells, GaAs mid cells and GaInP top cell composite cells, there are mid cells and top cells that can be delta-doped, and for mid cells and top cells, which generally include the back layer, base and emitter Layers and other structures, if you want to improve the performance of the battery by delta doping, there are many options, such as delta doping only in the middle battery or top battery, or you can do both batteries. For delta doping, only a part of the back layer or the emission layer can be doped, or all of them can be delta doped. It is found in the present invention that doping the back layers in both the middle cell and the top cell, and when the structures in the base layer and the emission layer are not completely delta doped layers, can significantly improve the structure of the cell and improve the efficiency of the cell.
优选的,所述GaAs中电池的背层还包括贴附于所述delta掺杂的p型GaInP层靠近所述Ge底电池的表面,通过直接掺杂生长得到的p型GaInP层,发射层中还包括贴附于所述delta掺杂的n型GaAs层靠近所述Ge底电池的表面,通过直接掺杂生长得到的n型GaAs层;Preferably, the back layer of the battery in the GaAs further includes a p-type GaInP layer that is attached to the delta-doped p-type GaInP layer close to the surface of the Ge bottom battery, and is grown by direct doping. It also includes an n-type GaAs layer that is attached to the surface of the delta-doped n-type GaAs layer close to the Ge bottom battery and grown by direct doping;
优选的,所述GaInP顶电池的背层还包括贴附于所述delta掺杂的p型GaInP层靠近所述Ge底电池的表面,通过直接掺杂生长得到的p型GaInP层,发射层还包括贴附于所述delta掺杂的n型GaInP层靠近所述Ge底电池的表面,通过直接掺杂生长得到的n型GaInP层。Preferably, the back layer of the GaInP top cell further comprises a p-type GaInP layer attached to the delta-doped p-type GaInP layer close to the surface of the Ge bottom cell and grown by direct doping, and the emission layer also It includes the n-type GaInP layer that is attached to the surface of the delta-doped n-type GaInP layer close to the Ge bottom cell and grown by direct doping.
在每层基层或发射层中,除delta掺杂层的结构外,还设置有通过直接掺杂生长得到层状结构,通过与delta的协同作用,与仅设置delta掺杂层相比,可十分有效地提高电池的效率。In each base layer or emission layer, in addition to the structure of the delta doped layer, a layered structure obtained by direct doping growth is also provided. Effectively improve the efficiency of the battery.
优选的,所述GaAs中电池的背层中,所述通过直接掺杂生长得到的p型GaInP层的厚度为20~40nm,所述p型delta掺杂的GaInP层的厚度为20~40nm;所述GaAs中电池的发射层中,所述通过直接掺杂生长得到的n型GaAs层的厚度为25~60nm,所述delta掺杂的n型GaAs发射层的厚度为25~60nm;Preferably, in the back layer of the GaAs medium cell, the thickness of the p-type GaInP layer obtained by direct doping growth is 20-40 nm, and the thickness of the p-type delta-doped GaInP layer is 20-40 nm; In the emission layer of the GaAs medium battery, the thickness of the n-type GaAs layer obtained by direct doping growth is 25-60 nm, and the thickness of the delta-doped n-type GaAs emission layer is 25-60 nm;
优选的,所述GaInP顶电池的背层中,所述通过直接掺杂生长得到的p型GaInP层的厚的为20~40nm,所述delta掺杂的p型GaInP的厚度为20~40nm;所述GaInP顶电池的发射层中,通过直接掺杂生长得到的n型GaInP层的厚的为25~60nm,所述delta掺杂的n型GaInP的厚度为25~60nm。Preferably, in the back layer of the GaInP top cell, the thickness of the p-type GaInP layer obtained by direct doping growth is 20-40 nm, and the thickness of the delta-doped p-type GaInP is 20-40 nm; In the emission layer of the GaInP top cell, the thickness of the n-type GaInP layer obtained by direct doping growth is 25-60 nm, and the thickness of the delta-doped n-type GaInP is 25-60 nm.
优选的,朝向所述Ge底电池的方向,所述GaAs中电池中包括依次层叠设置的窗口层、发射层、基区和背层;朝向所述GaAs中电池的方向,所述GaInP顶电池中包括依次层叠设置的接触层、窗口层、发射层、基区和背层。中电池的窗口层主要用来透射670nm波长以上的太阳光,中电池基区吸收670-870nm之间的太阳光后,在基区与发射层的pn结界面处产生感应电动势,背层则起到增强光子吸收达到增强效率的作用。顶电池的窗口层主要用来透射太阳全光谱,基区吸收670nm以下的波长在基区与发射层的界面产生感应电动势,背层则起到增强光子吸收达到增强效率的作用。Preferably, towards the direction of the Ge bottom cell, the GaAs middle cell includes a window layer, an emission layer, a base region and a back layer that are stacked in sequence; towards the direction of the GaAs middle cell, the GaInP top cell It includes a contact layer, a window layer, an emission layer, a base region and a back layer that are stacked in sequence. The window layer of the medium cell is mainly used to transmit sunlight with a wavelength above 670 nm. After the base region of the medium cell absorbs sunlight between 670-870 nm, an induced electromotive force is generated at the pn junction interface between the base region and the emission layer, and the back layer starts. To enhance the photon absorption to enhance the efficiency. The window layer of the top cell is mainly used to transmit the full spectrum of the sun. The base region absorbs wavelengths below 670 nm to generate an induced electromotive force at the interface between the base region and the emission layer, and the back layer enhances photon absorption to enhance efficiency.
优选的,所述Ge底电池中依次层叠设置p型Ge衬底,n型Ge发射层和n型GaInP窗口层。锗底电池主要吸收870nm以上的波长。Preferably, a p-type Ge substrate, an n-type Ge emission layer and an n-type GaInP window layer are stacked in sequence in the Ge bottom cell. The germanium bottom cell mainly absorbs wavelengths above 870nm.
优选的,所述Ge底电池与所述GaAs通过隧穿结进行连接,所述GaAs与所述GaInP通过隧穿结进行连接。Preferably, the Ge bottom cell and the GaAs are connected through a tunnel junction, and the GaAs and the GaInP are connected through a tunnel junction.
进一步优选的,所述隧穿结的材料为GaAs。这种隧穿结材料内阻较低能使各节电池更好的串起来,达到最佳的电流密度。Further preferably, the material of the tunnel junction is GaAs. The lower internal resistance of the tunneling junction material enables better stringing of cells to achieve the best current density.
本发明的另一目的是保护本发明所述太阳能电池的制备方法,包括:Another object of the present invention is to protect the preparation method of the solar cell of the present invention, including:
形成所述GaAs中电池的背层中delta掺杂的p型GaInP层,采用金属有机化合物化学气相沉淀法,先生长2~4nm的未通掺杂源的GaInP,再只通磷烷1~3秒,再通入掺杂源2~4秒,完成一个周期的生长;如此进行5~20个周期的循环生长;To form the delta-doped p-type GaInP layer in the back layer of the GaAs medium cell, adopt the metal organic compound chemical vapor deposition method, first grow 2-4 nm of GaInP without doping source, and then only pass 1-3 phosphine. seconds, and then feed the doping source for 2 to 4 seconds to complete one cycle of growth; 5 to 20 cycles of cyclic growth are thus performed;
形成所述GaAs中电池的发射层中delta掺杂的n型GaAs层,采用金属有机化合物化学气相沉淀法,先生长2~4nm未通硅烷的GaAs,再只通砷烷1~3秒,再通入硅烷2~4秒,完成一个周期的生长,如此进行6~30个周期的循环生长。To form the delta-doped n-type GaAs layer in the emission layer of the GaAs medium cell, adopt the metal organic compound chemical vapor deposition method, first grow 2-4nm GaAs without silane, and then only pass arsine for 1-3 seconds, and then The silane was passed in for 2-4 seconds to complete one cycle of growth, and 6-30 cycles of cyclic growth were thus performed.
形成所述GaInP顶电池的背层中delta掺杂的p型GaInP层,采用金属有机化合物化学气相沉淀法,先生长2~4nm的未通掺杂源的GaInP,再只通磷烷1到3秒,再通入掺杂源2~4秒,完成一个周期的生长,如此进行5到20个周期的循环生长;To form the delta-doped p-type GaInP layer in the back layer of the GaInP top cell, adopt the metal organic compound chemical vapor deposition method, first grow 2-4 nm of GaInP without doping source, and then only pass 1 to 3 of phosphine. seconds, and then pass in the doping source for 2 to 4 seconds to complete one cycle of growth, and thus carry out 5 to 20 cycles of cyclic growth;
形成所述GaInP顶电池的发射层中delta掺杂的n型GaInP层,采用金属有机化合物化学气相沉淀法,先生长2~4nm未通硅烷的GaInP,再只通磷烷1~3秒,再通入硅烷2到4秒,完成一个周期的生长,如此进行6~30个周期的循环生长。To form the delta-doped n-type GaInP layer in the emission layer of the GaInP top cell, adopt the metal organic compound chemical vapor deposition method, first grow 2-4 nm GaInP without silane, and then only pass phosphine for 1-3 seconds, and then The silane was introduced for 2 to 4 seconds to complete one cycle of growth, and 6 to 30 cycles of cyclic growth were thus performed.
优选的,所述金属有机化合物化学气相沉淀法的条件为,温度550~850℃,压强50~200托。Preferably, the conditions of the metal organic compound chemical vapor precipitation method are as follows: the temperature is 550-850° C., and the pressure is 50-200 Torr.
优选的,所述其中电池或顶电池背层掺杂源为CCl4、CBr4或二乙基锌(DEZn)中的一种。Preferably, the doping source for the back layer of the cell or top cell is one of CCl 4 , CBr 4 or diethylzinc (DEZn).
作为优选的方案,本发明所述电池的制备方法包括如下步骤:As a preferred solution, the preparation method of the battery of the present invention comprises the following steps:
1)采用金属有机化合物化学气相沉淀法(MOCVD),控制反应室温度为680℃~850℃,压力为50~200torr,在p型Ge衬底的上表面进行n型磷扩散,得n型Ge发射层,再在其上生长20到60nm厚的GaInP缓冲层,作为底电池的窗口层;1) Using the metal organic compound chemical vapor deposition method (MOCVD), the temperature of the reaction chamber is controlled to be 680 ° C to 850 ° C, and the pressure is 50 to 200 torr, and n-type phosphorus is diffused on the upper surface of the p-type Ge substrate to obtain n-type Ge. Emission layer, and then grow a 20 to 60 nm thick GaInP buffer layer on it as the window layer of the bottom cell;
2)在所述窗口层上生长5-10nm的n型GaAs和5到10nm的p型GaAs作为第一隧穿结;2) growing n-type GaAs of 5-10 nm and p-type GaAs of 5 to 10 nm on the window layer as the first tunneling junction;
3)在所述第一隧穿结上通过直接掺杂生长的方式生长厚度为20~40nm的p型GaInP背层,再采用delta掺杂方式,生长厚度为约20到40nm的delta掺杂的背层;delta掺杂具体为,先生长2到4nm的GaInP,再只通磷烷1到3秒,再通入掺杂源2到4秒;如此进行5到20个周期的循环生长;3) Grow a p-type GaInP back layer with a thickness of 20 to 40 nm on the first tunnel junction by direct doping growth, and then use a delta doping method to grow a delta doped 20 to 40 nm thick Back layer; delta doping is specifically, first grow GaInP of 2 to 4 nm, then pass only phosphine for 1 to 3 seconds, and then pass through the doping source for 2 to 4 seconds; 5 to 20 cycles of cyclic growth are performed in this way;
4)在所述delta掺杂的背层上生长厚度约2000到3000nm的p型GaAs作为中电池的基区;4) growing p-type GaAs with a thickness of about 2000 to 3000 nm on the delta-doped back layer as the base region of the medium cell;
5)通过直接掺杂生长的方式生长厚度为25到60nm的n型GaAs发射层,然后采用delta掺杂的方式,得到厚度为25~60nm的delta掺杂的n型GaAs发射层;delta掺杂具体为先生长2到4nm未通硅烷的GaAs,再只通砷烷1到3秒,再通入硅烷2到4秒,如此循环生长6到30个周期;5) Grow an n-type GaAs emission layer with a thickness of 25 to 60 nm by direct doping growth, and then use a delta doping method to obtain a delta-doped n-type GaAs emission layer with a thickness of 25 to 60 nm; delta doping Specifically, first grow 2 to 4 nm of GaAs without silane, then only pass arsine for 1 to 3 seconds, and then pass silane for 2 to 4 seconds, and this cycle grows for 6 to 30 cycles;
6)再在其上生长40到120nm厚的n型AlGaInP窗口层;6) A 40 to 120 nm thick n-type AlGaInP window layer is grown thereon;
7)再在所述窗口层上生长n型GaAs和p型GaAs作为第二隧穿结;7) growing n-type GaAs and p-type GaAs on the window layer as a second tunneling junction;
8)在所述第二隧穿结上通过直接掺杂生长的方式生长厚度为20到40nm的顶电池p型GaInP背层,再采用delta掺杂方式,厚度为20到40nm的delta掺杂背层;所述delta掺杂具体为先生长2~4nm的未通掺杂源的GaInP,再只通磷烷1~3秒,再打开掺杂源2~4秒,如此进行5到20个周期的循环生长;8) A top cell p-type GaInP back layer with a thickness of 20 to 40 nm is grown on the second tunnel junction by direct doping growth, and a delta doping back layer with a thickness of 20 to 40 nm is then grown by delta doping. layer; the delta doping is specifically the GaInP with a length of 2 to 4 nm without the doping source, then only phosphine for 1 to 3 seconds, and then the doping source is turned on for 2 to 4 seconds, and so on for 5 to 20 cycles cyclic growth;
9)在所述背层上生长厚度为300到700nm的p型GaInP作为顶电池基区;9) growing p-type GaInP with a thickness of 300 to 700 nm on the back layer as a top cell base region;
10)在所述基区上生长厚度为25到60nm的n型GaInP发射层,然后采用delta掺杂的方式,得到厚度为25~60nm的delta掺杂的n型GaInP发射层;所述delta掺杂具体为先生长2到4nm未通硅烷的GaInP,再只通磷烷1到3秒,再打开硅烷2到4秒,再生长2到4nm未通硅烷的GaInP,如此循环生长6到30个周期;10) Grow an n-type GaInP emitting layer with a thickness of 25 to 60 nm on the base region, and then adopt a delta doping method to obtain a delta-doped n-type GaInP emitting layer with a thickness of 25 to 60 nm; the delta doping The heterogeneity is to first grow 2 to 4 nm of GaInP without silane, then only pass phosphine for 1 to 3 seconds, then turn on silane for 2 to 4 seconds, and then grow 2 to 4 nm of GaInP without silane, and so on for 6 to 30 cycles. cycle;
11)生长20到60nm的n型AlGaInP窗口层;11) growing an n-type AlGaInP window layer of 20 to 60 nm;
12)降温至600到700摄氏度,生长40到100nm的n型GaAs接触层。12) The temperature is lowered to 600 to 700 degrees Celsius, and an n-type GaAs contact layer of 40 to 100 nm is grown.
本发明具有如下有益效果:The present invention has the following beneficial effects:
1)本发明的三结砷化镓太阳能电池外延结构中,中电池、顶电池的背层及发射层均有进行delta掺杂生长,这种delta掺杂结构能阻断晶体位错延伸、抑制晶体缺陷蔓延,使其可靠性及光电转换效率得以提升。1) In the epitaxial structure of the triple-junction gallium arsenide solar cell of the present invention, the back layer and the emission layer of the middle cell and the top cell are all grown by delta doping. This delta doping structure can block the extension of crystal dislocation and inhibit the Crystal defects spread, improving reliability and photoelectric conversion efficiency.
2)本发明所述的太阳能电池可减小电池工作时的结温,能获得更高的开路电压及短路电流。2) The solar cell of the present invention can reduce the junction temperature when the cell works, and can obtain higher open-circuit voltage and short-circuit current.
附图说明Description of drawings
图1实施例1所述电池的结构示意图。FIG. 1 is a schematic structural diagram of the battery described in Example 1.
具体实施方式Detailed ways
以下实施例用于说明本发明,但不用来限制本发明的范围。The following examples are intended to illustrate the present invention, but not to limit the scope of the present invention.
实施例1Example 1
本实施例涉及一种砷化镓太阳能电池外延结构,依次包括层叠设置的Ge底电池、GaAs中电池和GaInP顶电池;The present embodiment relates to an epitaxial structure of a gallium arsenide solar cell, which sequentially includes a Ge bottom cell, a GaAs middle cell and a GaInP top cell arranged in layers;
其具体结构为,从下至上,依次包括p-Ge衬底,锗衬底上进行n型磷扩散得到的n-Ge发射层,厚度为30nm的n-GaInP窗口层,厚度为5nm的n-GaAs隧穿结,厚度为5nm的p-GaAs隧穿结,厚度为30nm的p-GaInP背层1,厚度为32nm的delta掺杂的p-GaInP背层2,厚度为2500nm的p-GaAs基区,厚度为30nm的n-GaAs发射层1,厚度为32nm的delta掺杂的n-GaAs发射层2,厚度为80nm的n-AlGaInP窗口层,厚度为5nm的n-GaAs隧穿结,厚度为5nm的p-GaAs隧穿结,厚度为30nm的p-GaInP背层1,厚度为32nm的delta掺杂的p-GaInP背层2,厚度为500nm的p-GaInP基区,厚度为30nm的n-GaInP发射层1,厚度为32nm的delta掺杂的n-GaInP发射层2,厚度为40nm的n-AlGaInP窗口层,厚度为50nm的n-GaAs接触层。其结构示意图如图1。Its specific structure is, from bottom to top, including p-Ge substrate, n-Ge emission layer obtained by n-type phosphorus diffusion on germanium substrate, n-GaInP window layer with thickness of 30nm, n-GaInP with thickness of 5nm. GaAs tunneling junction, p-GaAs tunneling junction with a thickness of 5nm, p-GaInP back layer 1 with a thickness of 30nm, delta-doped p-GaInP back layer 2 with a thickness of 32nm, p-GaAs base with a thickness of 2500nm region, n-GaAs emitter layer 1 with a thickness of 30 nm, delta-doped n-GaAs emitter layer 2 with a thickness of 32 nm, n-AlGaInP window layer with a thickness of 80 nm, n-GaAs tunneling junction with a thickness of 5 nm, thickness 5nm p-GaAs tunnel junction, 30nm thickness p-GaInP back layer 1, 32nm thickness delta doped p-GaInP back layer 2, 500nm thickness p-GaInP base region, 30nm thickness n-GaInP emission layer 1, delta-doped n-GaInP emission layer 2 with a thickness of 32 nm, n-AlGaInP window layer with a thickness of 40 nm, and n-GaAs contact layer with a thickness of 50 nm. Its structure diagram is shown in Figure 1.
本实施例涉及本发明所述电池的制备方法,包括如下步骤:This embodiment relates to the preparation method of the battery of the present invention, which includes the following steps:
1)采用MOCVD设备进行外延层生长,设定反应室的温度为750℃,压力为150torr,在p型Ge衬底的上表面进行n型磷扩散作为底电池的发射层,再在其上生长30nm的n型GaInP缓冲层作为底电池的窗口层,此处的n型掺杂采用的硅烷。1) Use MOCVD equipment for epitaxial layer growth, set the temperature of the reaction chamber to 750°C and the pressure to 150torr, and perform n-type phosphorus diffusion on the upper surface of the p-type Ge substrate as the emission layer of the bottom cell, and then grow on it The 30nm n-type GaInP buffer layer is used as the window layer of the bottom cell, and silane is used for the n-type doping here.
后面步骤中外延层n型掺杂均使用硅烷,p型掺杂均使用CBr4;In the following steps, silane is used for the n-type doping of the epitaxial layer, and CBr 4 is used for the p-type doping;
2)生长厚度为5nm的n型GaAs,厚度为5nm的p型GaAs作为第一隧穿结;2) growing n-type GaAs with a thickness of 5 nm, and p-type GaAs with a thickness of 5 nm as the first tunneling junction;
3)生长厚度为30nm的p型GaInP背层1,再采用delta掺杂方式生长p型GaInP背层2,具体为,生长2nm的GaInP(未通CBr4),再只通磷烷2秒,再打开CBr4 3秒,如此进行16个循环周期生长,得厚度为32nm的背层2;3) Grow a p-type GaInP back layer 1 with a thickness of 30 nm, and then use a delta doping method to grow a p-type GaInP back layer 2, specifically, grow 2 nm of GaInP (without CBr 4 ), and then only pass phosphine for 2 seconds, Turn on CBr 4 again for 3 seconds, and perform 16 cycles of growth in this way to obtain a back layer 2 with a thickness of 32 nm;
4)生长厚度为2500nm的p型GaAs作为中电池的基区,p型掺杂仍然采用CBr4;4) Grow p-type GaAs with a thickness of 2500 nm as the base region of the medium cell, and still use CBr 4 for p-type doping;
5)生长厚度为30nm的n型GaAs发射层1,然后采用delta掺杂的方式生长厚度为32nm的delta掺杂的n型GaAs发射层2,具体操作为,先生长2nm未通硅烷的GaAs,再只通砷烷2秒,再打开硅烷3秒,如此循环生长16个周期,得到厚度为32nm的delta掺杂的n型GaAs发射层2;5) Grow an n-type GaAs emission layer 1 with a thickness of 30 nm, and then grow a delta-doped n-type GaAs emission layer 2 with a thickness of 32 nm by delta doping. The specific operation is to grow 2 nm of GaAs without silane, Then only pass arsine for 2 seconds, then turn on silane for 3 seconds, and this cycle grows for 16 cycles to obtain a delta-doped n-type GaAs emission layer 2 with a thickness of 32 nm;
6)生长80nm厚的n型AlGaInP窗口层;6) Grow an n-type AlGaInP window layer with a thickness of 80 nm;
7)生长5nm的n型GaAs和5nm的p型GaAs作为第二隧穿结;7) growing 5nm n-type GaAs and 5nm p-type GaAs as the second tunneling junction;
8)生长厚度为30nm的顶电池p型GaInP背层1,再采用delta掺杂方式生长厚度为32nm的delta掺杂p型GaInP背层2,所述delta掺杂生长的具体操作为,先生长2nm的未通CBr4掺杂源的GaInP,再只通磷烷2秒,再打开掺杂源3秒,如此进行16个循环周期,得到厚度为32nm的delta掺杂p型GaInP背层2;8) Grow a top cell p-type GaInP back layer 1 with a thickness of 30 nm, and then use a delta doping method to grow a delta-doped p-type GaInP back layer 2 with a thickness of 32 nm. The specific operation of the delta doping growth is, first grow 2nm of GaInP without CBr 4 doping source, and then only phosphine for 2 seconds, then turn on the doping source for 3 seconds, and so on for 16 cycles to obtain a delta-doped p-type GaInP back layer 2 with a thickness of 32 nm;
9)生长厚度为500nm的p型GaInP作为顶电池基区;9) Grow p-type GaInP with a thickness of 500 nm as the base region of the top cell;
10)生长厚度为30nm的n型GaInP发射层1,然后采用delta掺杂的方式生长厚度为32nm的delta掺杂的n型GaInP发射层2,所述delta掺杂生长的具体操作为,先生长2nm未通硅烷的GaInP,再只通磷烷2秒,再打开硅烷2秒,如此循环生长,其周期为16个,得到厚度为32nm的delta掺杂的n型GaInP发射层2;10) Grow an n-type GaInP emission layer 1 with a thickness of 30 nm, and then grow a delta-doped n-type GaInP emission layer 2 with a thickness of 32 nm by delta doping. The specific operation of the delta doping growth is, first grow 2nm GaInP without silane, then only phosphine for 2 seconds, and then silane is turned on for 2 seconds, so that the cycle grows, the period is 16, and the delta-doped n-type GaInP emission layer 2 with a thickness of 32nm is obtained;
11)生长40nm的n型AlGaInP窗口层;11) Grow a 40nm n-type AlGaInP window layer;
12)降低温度至670度生长50nm的n型GaAs接触层。12) Lower the temperature to 670 degrees to grow a 50nm n-type GaAs contact layer.
实施例2Example 2
本实施例涉及一种砷化镓太阳能电池外延结构,本实施例与实施例1相比,其区别在于,delta掺杂的n-GaInP发射层2的厚度为40nm。This embodiment relates to an epitaxial structure of a gallium arsenide solar cell. Compared with Embodiment 1, the difference between this embodiment is that the thickness of the delta-doped n-GaInP emission layer 2 is 40 nm.
本实施例所述的砷化镓太阳能电池外延结构依次包括层叠设置的Ge底电池、GaAs中电池和GaInP顶电池;The epitaxial structure of the gallium arsenide solar cell described in this embodiment sequentially includes a stacked Ge bottom cell, a GaAs middle cell, and a GaInP top cell;
其具体结构为,从下至上,依次包括p-Ge衬底,锗衬底上进行n型磷扩散得到的n-Ge发射层,厚度为30nm的n-GaInP窗口层,厚度为5nm的n-GaAs隧穿结,厚度为5nm的p-GaAs隧穿结,厚度为30nm的p-GaInP背层1,厚度为32nm的delta掺杂的p-GaInP背层2,厚度为2500nm的p-GaAs基区,厚度为30nm的n-GaAs发射层1,厚度为32nm的delta掺杂的n-GaAs发射层2,厚度为80nm的n-AlGaInP窗口层,厚度为5nm的n-GaAs隧穿结,厚度为5nm的p-GaAs隧穿结,厚度为30nm的p-GaInP背层1,厚度为32nm的delta掺杂的p-GaInP背层2,厚度为500nm的p-GaInP基区,厚度为30nm的n-GaInP发射层1,厚度为40nm的delta掺杂的n-GaInP发射层2,厚度为40nm的n-AlGaInP窗口层,厚度为50nm的n-GaAs接触层。Its specific structure is, from bottom to top, including p-Ge substrate, n-Ge emission layer obtained by n-type phosphorus diffusion on germanium substrate, n-GaInP window layer with thickness of 30nm, n-GaInP with thickness of 5nm. GaAs tunneling junction, p-GaAs tunneling junction with a thickness of 5nm, p-GaInP back layer 1 with a thickness of 30nm, delta-doped p-GaInP back layer 2 with a thickness of 32nm, p-GaAs base with a thickness of 2500nm region, n-GaAs emitter layer 1 with a thickness of 30 nm, delta-doped n-GaAs emitter layer 2 with a thickness of 32 nm, n-AlGaInP window layer with a thickness of 80 nm, n-GaAs tunneling junction with a thickness of 5 nm, thickness 5nm p-GaAs tunnel junction, 30nm thickness p-GaInP back layer 1, 32nm thickness delta doped p-GaInP back layer 2, 500nm thickness p-GaInP base region, 30nm thickness An n-GaInP emission layer 1, a delta-doped n-GaInP emission layer 2 with a thickness of 40 nm, an n-AlGaInP window layer with a thickness of 40 nm, and an n-GaAs contact layer with a thickness of 50 nm.
本实施例涉及本发明所述电池的制备方法,包括如下步骤:This embodiment relates to the preparation method of the battery of the present invention, which includes the following steps:
1)采用MOCVD设备来进行外延层生长,设定反应室的温度为750℃,压力为150torr,在p型Ge衬底的上表面进行n型磷扩散作为底电池的发射层。再在其上生长30nm的n型GaInP缓冲层作为底电池的窗口层,此处的n型掺杂采用的SiH4,之后的外延层n型掺杂均使用硅烷,p型掺杂均使用CBr4;1) Using MOCVD equipment to grow the epitaxial layer, set the temperature of the reaction chamber to 750°C and the pressure to 150torr, and perform n-type phosphorus diffusion on the upper surface of the p-type Ge substrate as the emission layer of the bottom cell. Then grow a 30nm n-type GaInP buffer layer on it as the window layer of the bottom cell, where SiH4 is used for n-type doping, silane is used for n-type doping in subsequent epitaxial layers, and CBr4 is used for p-type doping;
2)生长厚度为5nm的n型GaAs,厚度为5nm的p型GaAs作为第一隧穿结;2) growing n-type GaAs with a thickness of 5 nm, and p-type GaAs with a thickness of 5 nm as the first tunneling junction;
3)生长厚度为30nm的p型GaInP背层1,再采用delta掺杂方式,生长2nm的未通CBr4(掺杂源)的GaInP,再只通磷烷2秒,再打开CBr43秒,如此进行16个循环周期生长,生长厚度为32nm的delta掺杂的p型GaInP背层2;3) Grow a p-type GaInP back layer 1 with a thickness of 30nm, and then use a delta doping method to grow a 2nm GaInP without CBr4 (doping source), and then only pass phosphine for 2 seconds, then turn on CBr for 43 seconds, and so on. 16 cycles of growth to grow a delta-doped p-type GaInP back layer 2 with a thickness of 32 nm;
4)生长厚度为2500nm的p型GaAs作为中电池的基区,p型掺杂仍然采用CBr4;4) The p-type GaAs with a thickness of 2500 nm is grown as the base region of the medium battery, and CBr4 is still used for the p-type doping;
5)生长厚度为30nm的n型GaAs发射层1,然后采用delta掺杂的方式,先生长2nm未通硅烷的GaAs,再只通砷烷2秒,再打开硅烷3秒,再生长2nm未通硅烷的GaAs,如此循环生长,其周期为16个,得到厚度为32nm的delta掺杂的n型GaAs发射层2;5) Grow an n-type GaAs emission layer 1 with a thickness of 30 nm, and then use delta doping to grow 2 nm of GaAs without silane, then only pass arsine for 2 seconds, turn on silane for 3 seconds, and grow 2 nm without passing through The GaAs of silane is grown cyclically in this way, and its period is 16, and a delta-doped n-type GaAs emission layer 2 with a thickness of 32 nm is obtained;
6)生长80nm厚的n型AlGaInP窗口层;6) Grow an n-type AlGaInP window layer with a thickness of 80 nm;
7)生长5nm的n型GaAs和5nm的p型GaAs作为第二隧穿结;7) growing 5nm n-type GaAs and 5nm p-type GaAs as the second tunneling junction;
8)生长厚度为30nm的顶电池p型GaInP背层1,再采用delta掺杂方式,先生长2nm的未通CBr4掺杂源的GaInP,再只通磷烷2秒,再打开掺杂源3秒,如此进行16个循环周期,得到厚度为32nm的delta掺杂p型GaInP背层2;8) Grow the top cell p-type GaInP back layer 1 with a thickness of 30 nm, and then use the delta doping method to first grow 2 nm of GaInP without CBr4 doping source, and then only pass phosphine for 2 seconds, and then turn on the doping source 3 Second, 16 cycles are performed in this way to obtain a delta-doped p-type GaInP back layer 2 with a thickness of 32 nm;
9)生长厚度为500nm的p型GaInP作为顶电池基区;9) Grow p-type GaInP with a thickness of 500 nm as the base region of the top cell;
10)生长厚度为30nm的n型GaInP发射层1,然后采用delta掺杂的方式,生长2nm未通硅烷的GaInP,再只通磷烷2秒,再打开硅烷2秒,如此循环生长,其周期为20个,得到厚度为40nm的delta掺杂的n型GaInP发射层2;10) Grow an n-type GaInP emission layer 1 with a thickness of 30 nm, and then use delta doping to grow 2 nm of GaInP without silane, and then only pass phosphine for 2 seconds, and then turn on silane for 2 seconds. is 20 to obtain a delta-doped n-type GaInP emission layer 2 with a thickness of 40 nm;
11)生长40nm的n型AlGaInP窗口层;11) Grow a 40nm n-type AlGaInP window layer;
12)降低温度至670度生长50nm的n型GaAs接触层。12) Lower the temperature to 670 degrees to grow a 50nm n-type GaAs contact layer.
实施例3Example 3
本实施例涉及一种砷化镓太阳能电池外延结构,与实施例1相比,其区别在于,其p型delta掺杂GaInP背层2厚度为40nm。This embodiment relates to an epitaxial structure of a gallium arsenide solar cell. Compared with Embodiment 1, the difference lies in that the thickness of the p-type delta-doped GaInP back layer 2 is 40 nm.
本实施例所述的外延结构依次包括层叠设置的Ge底电池、GaAs中电池和GaInP顶电池;The epitaxial structure described in this embodiment sequentially includes a stacked Ge bottom cell, a GaAs middle cell and a GaInP top cell;
其具体结构为,从下至上,依次包括p-Ge衬底,锗衬底上进行n型磷扩散得到的n-Ge发射层,厚度为30nm的n-GaInP窗口层,厚度为5nm的n-GaAs隧穿结,厚度为5nm的p-GaAs隧穿结,厚度为30nm的p-GaInP背层1,厚度为40nm的delta掺杂的p-GaInP背层2,厚度为2500nm的p-GaAs基区,厚度为30nm的n-GaAs发射层1,厚度为32nm的delta掺杂的n-GaAs发射层2,厚度为80nm的n-AlGaInP窗口层,厚度为5nm的n-GaAs隧穿结,厚度为5nm的p-GaAs隧穿结,厚度为30nm的p-GaInP背层1,厚度为32nm的delta掺杂的p-GaInP背层2,厚度为500nm的p-GaInP基区,厚度为30nm的n-GaInP发射层1,厚度为32nm的delta掺杂的n-GaInP发射层2,厚度为40nm的n-AlGaInP窗口层,厚度为50nm的n-GaAs接触层。Its specific structure is, from bottom to top, including p-Ge substrate, n-Ge emission layer obtained by n-type phosphorus diffusion on germanium substrate, n-GaInP window layer with thickness of 30nm, n-GaInP with thickness of 5nm. GaAs tunneling junction, p-GaAs tunneling junction with a thickness of 5 nm, p-GaInP back layer 1 with a thickness of 30 nm, delta-doped p-GaInP back layer 2 with a thickness of 40 nm, p-GaAs base with a thickness of 2500 nm region, n-GaAs emitter layer 1 with a thickness of 30 nm, delta-doped n-GaAs emitter layer 2 with a thickness of 32 nm, n-AlGaInP window layer with a thickness of 80 nm, n-GaAs tunneling junction with a thickness of 5 nm, thickness 5nm p-GaAs tunnel junction, 30nm thickness p-GaInP back layer 1, 32nm thickness delta doped p-GaInP back layer 2, 500nm thickness p-GaInP base region, 30nm thickness n-GaInP emission layer 1, delta-doped n-GaInP emission layer 2 with a thickness of 32 nm, n-AlGaInP window layer with a thickness of 40 nm, and n-GaAs contact layer with a thickness of 50 nm.
本实施例涉及本发明所述电池的制备方法,包括如下步骤:This embodiment relates to the preparation method of the battery of the present invention, which includes the following steps:
1)采用MOCVD设备来进行外延层生长,设定反应室的温度为750℃,压力为150torr,在p型Ge衬底的上表面进行n型磷扩散作为底电池的发射层。再在其上生长30nm的n型GaInP缓冲层作为底电池的窗口层,此处的n型掺杂采用的SiH4,之后的外延层n型掺杂均使用硅烷,p型掺杂均使用CBr4;1) Using MOCVD equipment to grow the epitaxial layer, set the temperature of the reaction chamber to 750°C and the pressure to 150torr, and perform n-type phosphorus diffusion on the upper surface of the p-type Ge substrate as the emission layer of the bottom cell. Then grow a 30nm n-type GaInP buffer layer on it as the window layer of the bottom cell, where SiH4 is used for n-type doping, silane is used for n-type doping in subsequent epitaxial layers, and CBr4 is used for p-type doping;
2)生长厚度为5nm的n型GaAs,厚度为5nm的p型GaAs作为第一隧穿结;2) growing n-type GaAs with a thickness of 5 nm, and p-type GaAs with a thickness of 5 nm as the first tunneling junction;
3)生长厚度为30nm的p型GaInP背层1,再采用delta掺杂方式,生长2nm的未通CBr4(掺杂源)的GaInP,再只通磷烷2秒,再打开CBr43秒,再生长2nm的未通CBr4的GaInP,如此进行20个循环周期生长,生长厚度为40nm的delta掺杂的p型GaInP背层2;3) Grow the p-type GaInP back layer 1 with a thickness of 30nm, and then use the delta doping method to grow 2nm GaInP without CBr4 (doping source), and then only pass phosphine for 2 seconds, then turn on CBr for 43 seconds, and grow again 2nm of GaInP without CBr4 was grown in this way for 20 cycles to grow a delta-doped p-type GaInP back layer 2 with a thickness of 40nm;
4)生长厚度为2500nm的p型GaAs作为中电池的基区,p型掺杂仍然采用CBr4;4) The p-type GaAs with a thickness of 2500 nm is grown as the base region of the medium battery, and CBr4 is still used for the p-type doping;
5)生长厚度为30nm的n型GaAs发射层1,然后采用delta掺杂的方式,先生长2nm未通硅烷的GaAs,再只通砷烷2秒,再打开硅烷3秒,再生长2nm未通硅烷的GaAs,如此循环生长,其周期为16个,得到厚度为32nm的delta掺杂的n型GaAs发射层2;5) Grow an n-type GaAs emission layer 1 with a thickness of 30 nm, and then use delta doping to grow 2 nm of GaAs without silane, then only pass arsine for 2 seconds, turn on silane for 3 seconds, and grow 2 nm without passing through The GaAs of silane is grown cyclically in this way, and its period is 16, and a delta-doped n-type GaAs emission layer 2 with a thickness of 32 nm is obtained;
6)生长80nm厚的n型AlGaInP窗口层;6) Grow an n-type AlGaInP window layer with a thickness of 80 nm;
7)生长5nm的n型GaAs和5nm的p型GaAs作为第二隧穿结;7) growing 5nm n-type GaAs and 5nm p-type GaAs as the second tunneling junction;
8)生长厚度为30nm的顶电池p型GaInP背层1,再采用delta掺杂方式,先生长2nm的未通CBr4掺杂源的GaInP,再只通磷烷2秒,再打开掺杂源3秒,再生长2nm的未通掺杂源的GaInP,如此进行16个循环周期,得到厚度为32nm的delta掺杂p型GaInP背层2;8) Grow the top cell p-type GaInP back layer 1 with a thickness of 30 nm, and then use the delta doping method to first grow 2 nm of GaInP without CBr4 doping source, and then only pass phosphine for 2 seconds, and then turn on the doping source 3 Second, re-grow 2 nm of GaInP without doping source, and perform 16 cycles in this way to obtain a delta-doped p-type GaInP back layer 2 with a thickness of 32 nm;
9)生长厚度为500nm的p型GaInP作为顶电池基区;9) Grow p-type GaInP with a thickness of 500 nm as the base region of the top cell;
10)生长厚度为30nm的n型GaInP发射层1,然后采用delta掺杂的方式,生长2nm未通硅烷的GaInP,再只通磷烷2秒,再打开硅烷2秒,再生长2nm未通硅烷的GaInP,如此循环生长,其周期为16个,得到厚度为32nm的delta掺杂的n型GaInP发射层2;10) Grow an n-type GaInP emission layer 1 with a thickness of 30 nm, and then use delta doping to grow 2 nm of GaInP without silane, then only pass phosphine for 2 seconds, turn on silane for 2 seconds, and grow 2 nm without silane The GaInP is grown in such a cycle, and its period is 16 to obtain a delta-doped n-type GaInP emission layer 2 with a thickness of 32 nm;
11)生长40nm的n型AlGaInP窗口层;11) Grow a 40nm n-type AlGaInP window layer;
12)降低温度至670度生长50nm的n型GaAs接触层。12) Lower the temperature to 670 degrees to grow a 50nm n-type GaAs contact layer.
对比例1Comparative Example 1
与实施例1相比,本对比例的区别在于,所述GaAs中电池的中不设置p-GaInP背层1和n-GaAs发射层1。Compared with Example 1, the difference of this comparative example is that the p-GaInP back layer 1 and the n-GaAs emission layer 1 are not provided in the GaAs mid-cell.
对比例2Comparative Example 2
与实施例1相比,本对比例的区别在于,所述GaInP顶电池中不设置p-GaInP背层1和n-GaInP发射层1Compared with Example 1, the difference of this comparative example is that the GaInP top cell is not provided with the p-GaInP back layer 1 and the n-GaInP emission layer 1
对比例3Comparative Example 3
与实施例1相比,本对比例的区别在于,所述GaAs中电池的delta掺杂的背层的制备方法为先生长1nm的未通CBr4(掺杂源)的GaInP,再只通磷烷2秒,再打开CBr4 3秒,如此进行32个循环周期生长,生长厚度为32nm的delta掺杂的p型GaInP背层2;delta掺杂的发射层的制备方法为先生长1nm未通硅烷的GaAs,再只通砷烷2秒,再打开硅烷3秒,如此循环生长,其周期为32个,得到厚度为32nm的delta掺杂的n型GaAs发射层2。Compared with Example 1, the difference of this comparative example is that the preparation method of the delta-doped back layer of the battery in the GaAs is to first grow 1 nm of GaInP without CBr 4 (doping source), and then only pass phosphorus. Alkane for 2 seconds, then turn on CBr 4 for 3 seconds, and thus carry out 32 cycles of growth to grow a delta-doped p-type GaInP back layer 2 with a thickness of 32 nm; the preparation method of the delta-doped emission layer is to grow 1 nm first without passing through For GaAs of silane, only pass arsine for 2 seconds, then turn on silane for 3 seconds, and so on, the cycle is 32, and a delta-doped n-type GaAs emission layer 2 with a thickness of 32 nm is obtained.
对比例4Comparative Example 4
与实施例1相比,本对比例的区别在于,所述GaAs顶电池的delta掺杂的背层生长方法为先生长6nmm的未通CBr4掺杂源的GaInP,再只通磷烷4秒,再打开掺杂源6秒,如此进行5个循环周期,得到厚度为30nm的delta掺杂p型GaInP背层2;其delta掺杂的发射层的制备方法为生长6nm未通硅烷的GaInP,再只通磷烷4秒,再打开硅烷6秒,再生如此循环生长,其周期为5个,得到厚度为30nm的delta掺杂的n型GaInP发射层。Compared with Example 1, the difference of this comparative example is that the delta-doped back layer growth method of the GaAs top cell is to first grow 6 nm of GaInP without CBr4 doping source, and then only pass phosphine for 4 seconds. Then turn on the doping source for 6 seconds, and perform 5 cycles in this way to obtain a delta-doped p-type GaInP back layer 2 with a thickness of 30 nm; the preparation method of the delta-doped emission layer is to grow 6 nm of GaInP without silane, and then The phosphine was only passed through for 4 seconds, and the silane was turned on for 6 seconds. The regeneration cycle was performed in 5 cycles, and a delta-doped n-type GaInP emitting layer with a thickness of 30 nm was obtained.
对比例5Comparative Example 5
本对比例涉及市面上常见的复合电池,包括层叠设置的Ge底电池、GaAs中电池和GaInP顶电池,其具体结构为:This comparative example involves common composite cells on the market, including stacked Ge bottom cells, GaAs middle cells, and GaInP top cells. The specific structures are:
常见电池的具体结构为,从下至上,依次包括p-Ge衬底,锗衬底上进行n型磷扩散的n-Ge发射层,再生长厚度为30nm的n-GaInP窗口层,厚度为5nm的n-GaAs隧穿结,厚度为5nm的p-GaAs隧穿结,厚度为60nm的p-GaInP背层1,厚度为2500nm的p-GaAs基区,厚度为70nm的n-GaAs发射层1,厚度为80nm的n-AlGaInP窗口层,厚度为5nm的n-GaAs隧穿结,厚度为5nm的p-GaAs隧穿结,厚度为60nm的p-GaInP背层1,厚度为500nm的p-GaInP基区,厚度为60nm的n-GaInP发射层1,厚度为40nm的n-AlGaInP窗口层,厚度为50nm的n-GaAs接触层。The specific structure of a common battery is, from bottom to top, including a p-Ge substrate, an n-Ge emitter layer with n-type phosphorus diffusion on a germanium substrate, and an n-GaInP window layer with a thickness of 30nm and a thickness of 5nm. n-GaAs tunnel junction, p-GaAs tunnel junction with thickness of 5nm, p-GaInP back layer with thickness of 60nm 1, p-GaAs base with thickness of 2500nm, n-GaAs emitter layer with thickness of 70nm 1 , an n-AlGaInP window layer with a thickness of 80 nm, an n-GaAs tunnel junction with a thickness of 5 nm, a p-GaAs tunnel junction with a thickness of 5 nm, a p-GaInP back layer with a thickness of 60 nm, and a p-GaInP with a thickness of 500 nm. GaInP base region, n-GaInP emission layer 1 with thickness of 60nm, n-AlGaInP window layer with thickness of 40nm, n-GaAs contact layer with thickness of 50nm.
实验例Experimental example
对实施例和对比例的太阳能外延结构的光电转换效率进行测定,其测定方法为在AM1.5D,500倍聚光测试条件下,其光电转换效率分别为:The photoelectric conversion efficiency of the solar epitaxial structure of embodiment and comparative example is measured, and its measuring method is under AM1.5D, 500 times of concentrating test conditions, and its photoelectric conversion efficiency is respectively:
由以上数据可以看出,仅对中电池和顶电池进行掺杂生长,其对效果的改善上远不如在中电池和顶电池中均进行掺杂生长的效果,而且采用本申请所述的delta掺杂生长的方式效果更为理想。It can be seen from the above data that only the doping growth of the middle cell and the top cell is far less effective than the effect of doping growth in both the middle cell and the top cell, and the delta described in this application is used. The effect of doping growth is more ideal.
本发明在研究的过程中还尝试过仅对背层和发射层仅进行delta掺杂,即背层和发射层中仅含有一层的delta掺杂层,不含有普通的掺杂层,结果发现与采用普通的掺杂方式相比,效果没有明显的改善。也尝试仅在中电池和顶电池的背层进行delta掺杂,不对发射层进行delta掺杂,其效果也没有采用本发明的方式理想。In the process of research, the present invention also tried to perform only delta doping on the back layer and the emissive layer, that is, the back layer and the emissive layer only contain one delta doped layer and no ordinary doped layer. It was found that Compared with the common doping method, the effect is not significantly improved. An attempt was also made to perform delta doping only on the back layer of the middle cell and the top cell, without performing delta doping on the emissive layer, and the effect was not as ideal as the method of the present invention.
虽然,上文中已经用一般性说明、具体实施方式及试验,对本发明作了详尽的描述,但在本发明基础上,可以对之作一些修改或改进,这对本领域技术人员而言是显而易见的。因此,在不偏离本发明精神的基础上所做的这些修改或改进,均属于本发明要求保护的范围。Although the present invention has been described in detail above with general description, specific embodiments and tests, some modifications or improvements can be made on the basis of the present invention, which is obvious to those skilled in the art . Therefore, these modifications or improvements made without departing from the spirit of the present invention fall within the scope of the claimed protection of the present invention.
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