共查询到19条相似文献,搜索用时 143 毫秒
1.
2.
3.
4.
多晶Si太阳电池新型制绒工艺研究 总被引:2,自引:0,他引:2
提出一种采用二次酸腐蚀的多晶Si制绒新方法,首先在HF/HNO3的富HNO3体系中对Si片进行一次腐蚀,之后在富HF体系中进行二次腐蚀,以优化表面织构,减少光在Si表面的反射损失。制绒后,用扫描电子显微镜(SEM)对Si片进行了表面形貌分析,用Carry 5000紫外-可见-近红外分光光度计测量反射谱线,得到未镀减反射膜(ARC)的二次腐蚀制绒的最低反射率为20.34%,比一次腐蚀制绒(22.70%)低2.36%。将二次腐蚀新工艺应用于太阳电池工业制备中,对电池输出参量进行检测分析。结果表明,经过二次腐蚀工艺处理的太阳电池开路电压(VOC)、短路电流(JSC)和效率η均比采用一次腐蚀工艺的太阳电池有不同程度的提高,制成的太阳电池最高效率为14.93%。 相似文献
5.
6.
阴极材料对有机太阳电池性能的影响 总被引:1,自引:1,他引:0
分别用Al、LiF/Al和Ca/Al制备了三种不同阴极材料的体相异质结有机太阳电池。对其光电特性进行了表征,分析了不同阴极材料对电池性能的影响机制。结果表明:所制备的有机太阳电池在10–1W/cm2辐照度的光照下,开路电压分别为0.419 3,0.565 0和0.591 1 V,能量转换效率分别为1.17%、2.06%和1.91%;采用LiF/Al层状阴极制备的有机太阳电池具有更高的能量转换效率;功函数愈低的材料做阴极,有机太阳电池的能量转换效率也愈高。 相似文献
7.
8.
9.
10.
基于n型晶体硅太阳电池,分析了经光辐照后电池各性能参数的变化,探究了n型晶体硅太阳电池光诱导衰减机理.使用工业化设备在大面积(156 mm×156 mm)n型单晶硅片上制备太阳电池.利用太阳光谱模拟仪对制备的太阳电池进行光照处理,对比各阶段太阳电池电性能参数.结果表明,光照时会导致太阳电池表面减反射膜SiN:H/Si界面处积聚大量固定电荷,增大界面态密度,破坏电池表面钝化层结构,导致开路电压和短路电流产生较大衰减,35 kWh/m2光辐照后n型硅太阳电池效率衰减3.6%.在380℃低温退火处理后电池效率基本可恢复到初始状态.内量子效率测试结果表明光辐照后电池短波区域响应减弱,前表面界面效应导致电池效率发生较大衰减. 相似文献
11.
《Electron Devices, IEEE Transactions on》1965,12(9):493-496
The high reflectivity of the polished silicon surface of the newer N+/P silicon solar cells has emphasized the need for properly designed antireflection coatings to obtain improved solar cell performance. The problem is complicated by the facts that solar cells are generally tested in air, but are for their final application covered with a glass or quartz slide which is adhesive-bonded to the cell surface, and further, that solar cells operating in a nuclear particle radiation environment change their spectral response and are frequently optimized for performance at the end of design-life. Experiments have been performed to explore the antireflection characteristics of thin films of silicon monoxide which have been evaporated on the solar cell surface. The effect of the antireflection coating thickness on cell response as a function of wavelength has been determined and the improvement in cell short circuit current for Air Mass Zero space sunlight evaluated. Included in this study was the evaluation of the antireflection characteristics after the application of a coverglass with adhesive over the antireflection coating. For comparison, coverglasses were also applied to bare cells with no antireflection coating present. In all cases the various coating comparisons were based on the cell short-circuit current performance in Air Mass Zero sunlight. 相似文献
12.
13.
14.
Guoping Du Yu Zhang Wang Li Nan Chen Bingfa Liu Jie Sun 《Progress in Photovoltaics: Research and Applications》2015,23(12):1806-1814
Silicon nitride coating deposited by the plasma‐enhanced chemical vapor deposition method is the most widely used antireflection coating for crystalline silicon solar cells. In this work, we employed double‐layered silicon nitride coating consisting of a top layer with a lower refractive index and a bottom layer (contacting the silicon wafer) with a higher refractive index for multicrystalline silicon solar cells. An optimization procedure was presented for maximizing the photovoltaic performance of the encapsulated solar cells or modules. The dependence of their photovoltaic properties on the thickness of silicon nitride coatings was carefully analyzed. Desirable thicknesses of the individual silicon nitride layers for the double‐layered coatings were calculated. In order to get statistical conclusions, we fabricated a large number of multicrystalline silicon solar cells using the standard production line for both the double‐layered and single‐layered antireflection coating types. On the cell level, the double‐layered silicon nitride antireflection coating resulted in an increase of 0.21%, absolute for the average conversion efficiency, and 1.8 mV and 0.11 mA/cm2 for the average open‐circuit voltage and short‐circuit current density, respectively. On the module level, the cell to module power transfer factor was analyzed, and it was demonstrated that the double‐layered silicon nitride antireflection coating provided a consistent enhancement in the photovoltaic performance for multicrystalline silicon solar cell modules than the single‐layered silicon nitride coating. Copyright © 2015 John Wiley & Sons, Ltd. 相似文献
15.
《Electron Device Letters, IEEE》1983,4(5):138-139
The potential of tin oxide as an inexpensive antireflection (AR) coating for polycrystalline silicon solar cells has been investigated. Undoped tin oxide films of a desired thickness were deposited over p on n polycrystalline silicon solar cells by spray pyrolysis of an alcoholic solution of hydrated stannic chloride at 500°C. Evaluation of cell performance before and after this AR coating showed that the AR coating is highly compatible with the polycrystalline silicon solar cells. About 40-50 percent improvement in the short-circuit current of p on n polycrystalline cells has been measured. The coating may be highly suited to large-scale production of low-cost polycrystalline silicon solar cells for terrestrial application. 相似文献
16.
Recent high-efficiency silicon solar cells employ high-quality oxides both for surface passivation and as a rudimentary antireflection coating. This gives over 3% reflection at the cell front surface, even though the surface is microstructured. A double layer antireflection coating applied to cells with reduced SiO2 thickness reduces the cell reflection. However, although reflection is minimized by reducing the oxide thickness to values below 100 Å, a rapid falloff in both open-circuit voltage and short-circuit current is observed experimentally once this thickness is reduced below 200 Å. The best compromise is found when oxide thickness is 250 Å which allows improved short-circuit current density without appreciable loss in open-circuit voltage 相似文献
17.
The electromagnetic fields for an extended-cavity laser are described precisely and in detail. The extended-cavity laser consists of a semiconductor laser diode with a partially reflecting coating on one facet and an antireflection coating on the other coupled by radiation through a lensed-fiber, single-mode guide to another partially reflecting coating terminating a narrow-wavelength filter. The formulation is based on the Lorentz reciprocity theorem, the fields are described by angular plane-wave spectra, and the equivalent transmission line representation is used to determine the fields reflected and transmitted by partially reflecting and antireflection coatings. The design of antireflection coatings is considered in detail, and a formula which gives the optimum distance from the diode antireflection coating to an inline lensed fiber is derived 相似文献
18.
The polarization photosensitivity of two types of GaAlAs/GaAs heterophotoelements has been investigated. It has been shown
that in heterophotoelements without an antireflection coating the induced photopleochroism is governed by optical processes
at the air-GaAlAs surface boundary, and the angular dependence of the short-circuit photocurrents is described by the Fresnel
relations. It was found that the angular dependence of the photocurrents for s and p polarizations are similar in heterophotoelements with an antireflection coating and exhibits growth with increase of the
angle of incidence. In the cleared region the induced photopleochroism is observed to fall to zero. It has been shown that
heterophotoelements without an antireflection coating can be used as wideband photoanalyzers with a maximum azimuthal photosensitivity
of up to 0.1 A/W·deg for an angle of incidence of 75°, while polarization photosensitivity spectroscopy makes it possible
to carry out express diagnostics of the clearing effect in thin-film solar cells.
Fiz. Tekh. Poluprovodn. 33, 747–751 (June 1999) 相似文献