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Cu‐nanowire‐doped graphene (Cu NWs/graphene) is successfully incorporated as the back contact in thin‐film CdTe solar cells. 1D, single‐crystal Cu nanowires (NWs) are prepared by a hydrothermal method at 160 °C and 3D, highly crystalline graphene is obtained by ambient‐pressure CVD at 1000 °C. The Cu NWs/graphene back contact is obtained from fully mixing the Cu nanowires and graphene with poly(vinylidene fluoride) (PVDF) and N‐methyl pyrrolidinone (NMP), and then annealing at 185 °C for solidification. The back contact possesses a high electrical conductivity of 16.7 S cm?1 and a carrier mobility of 16.2 cm2 V?1 s?1. The efficiency of solar cells with Cu NWs/graphene achieved is up to 12.1%, higher than that of cells with traditional back contacts using Cu‐particle‐doped graphite (10.5%) or Cu thin films (9.1%). This indicates that the Cu NWs/graphene back contact improves the hole collection ability of CdTe cells due to the percolating network, with the super‐high aspect ratio of the Cu nanowires offering enormous electrical transport routes to connect the individual graphene sheets. The cells with Cu NWs/graphene also exhibit an excellent thermal stability, because they can supply an active Cu diffusion source to form an stable intermediate layer of CuTe between the CdTe layer and the back contact. 相似文献
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Yixiong Ji Xiangyun Zhao Yining Pan Zhenghua Su Jinhong Lin Eser Metin Akinoglu Yang Xu Heyou Zhang Pengjun Zhao Yue Dong Xingzhan Wei Fangyang Liu Paul Mulvaney 《Advanced functional materials》2023,33(11):2211421
Optimization of the back contact interface is crucial for improving the performance of Cu2ZnSnS4 (CZTS) thin film solar cells. In this paper, self-depleted CuSCN is deployed as an intermediate layer at the Mo/CZTS interface to improve the quality of the back contact. This CuSCN layer, obtained via aqueous solution processing, reduces the thickness of Mo(S,Se)2 and eliminates multi-layer crystallization of the absorber by suppressing the undesirable reaction between Mo and Se during the selenization process. By regulating the selenium infiltration into the CZTS precursor films during the selenization process, highly crystalline, single-layer Cu2ZnSn(S,Se)4 (CZTSSe) absorber layers are realized. The single-layer CZTSSe absorber exhibits reduced carrier recombination, enhanced carrier density and increased work function. The improved back contact and absorber layer enables 11.1% power-conversion-efficiency to be achieved. 相似文献
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报道了采用局部背接触结构的激光刻槽埋栅太阳电池的研究结果.模拟分析了局部背接触结构的作用,设计了合理的电池结构.通过工艺优化,得到了转换效率达到17.28%(大气质量AM=1.5 G,VOC=650.4mV,JSC=33.15 mA/cm2,FF=0.8014,电池面积为4 cm2)的太阳电池. 相似文献
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氩氧气氛下沉积的CdTe薄膜及太阳电池的性质 总被引:7,自引:2,他引:7
研究了在氩氧气氛下近空间升华沉积CdTe的技术.发展了在表面十分平整的玻璃衬底上沉积优质CdTe薄膜的方法,对比了在玻璃衬底和CdS薄膜上CdTe薄膜的结构特征.通过研究氧分压对CdTe薄膜择优取向的影响,证实了在恰当的近空间升华沉积过程中,两种衬底上的CdTe薄膜具有相同的结构.研究了玻璃衬底上CdTe薄膜的电学与光学性质,观察了后处理对上述薄膜性质的影响,并研制出了效率达1338%的小面积CdTe 薄膜太阳电池. 相似文献
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碲化锌插入层对碲化镉太阳电池性能参数影响的分析 总被引:5,自引:1,他引:4
分析了有Zn Te/ Zn Te∶Cu插入层的Cd Te太阳电池在能带结构上的变化.通过对比有无插入层的Cd Te太阳电池在C- V特性、I- V特性、光谱响应上的不同,肯定了插入层对改善背接触特性的作用,发现它还可以改善器件前结Cd S/ Cd Te的二极管特性和短波光谱响应.实验结果还表明,不掺杂的Zn Te对提高器件的效率是必要的.恰当的不掺杂层厚度和退火温度能有效地改进Cd Te太阳电池的性能,而对填充因子的提高最为显著 相似文献
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Copper thiocyanate (CuSCN) has proven to be a low‐cost, efficient hole‐transporting material for the emerging organic–inorganic perovskite solar cells. Herein, we report that CuSCN can also be applied to CdTe thin‐film solar cells to achieve high open‐circuit voltages (VOCs). By optimizing the thickness of the thermally evaporated CuSCN films, CdTe cells fabricated by close space sublimation in the superstrate configuration have achieved VOCs as high as 872 mV, which is about 20–25 mV higher than the highest VOC for the reference cells using the standard Cu/Au back contacts. CuSCN is a wide bandgap p‐type conductor with a conduction band higher than that of CdTe, leading to a conduction band offset that reflects electrons in CdTe, partially explaining the improved VOCs. However, due to the low conductivity of CuSCN, CdTe cells using CuSCN/Au back contacts exhibited slightly lower fill factors than the cells using Cu/Au back contacts. With optimized CdS:O window layers, the power conversion efficiency of the best CdTe cell, using CuSCN/Au back contact, is 14.7%: slightly lower than that of the best cell (15.2%) using Cu/Au back contact. Copyright © 2015 John Wiley & Sons, Ltd. 相似文献
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利用Silvaco-TCAD仿真软件全面系统地分析了不同发射区表面浓度和结深对n型插指背接触(IBC)太阳电池短路电流、开路电压、填充因子及转换效率的影响.借鉴双极半导体器件抗二次击穿技术,详细分析了不同发射区结深、发射区边缘刻蚀技术和发射区边缘选择性掺杂技术对IBC电池热击穿特性的影响.结果表明:发射区表面浓度越大、结深越深,IBC电池效率越高.当发射区表面浓度为5× 1020 cm-3、结深为1 μm时,转换效率高达23.35%.同时,深结发射区也有助于改善IBC电池的热击穿特性.发射区边缘刻蚀结构不具有改善IBC电池热击穿特性的作用,而发射区边缘选择性掺杂结构可有效改善IBC电池的热击穿特性,从而提高IBC太阳电池组件的可靠性. 相似文献
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N型背发射极晶体硅太阳电池模拟研究 总被引:1,自引:0,他引:1
N型晶体太阳电池由于少子寿命高、光致衰减低、弱光响应好等优点,近年来在高效率低成本太阳电池领域一直备受关注。利用PC1D模拟,对N型背发射极晶体硅太阳电池进行了分析。结果表明,背发射极掺杂浓度、结深、背表面复合速率、前表面掺杂浓度及复合速率都对电池转换效率有较大影响,尤其是电池前表面与背表面复合速率对电池性能的影响最为明显,而电池前表面场掺杂深度则对电池性能影响较小。对于前表面复合来说,当前表面复合速率小于1×103cm/s时,电池性能受表面复合速率变化的影响很小;但复合速率超过1×103cm/s后,电池转换效率快速下降。背表面复合对电池效率影响则更明显,当背表面复合速率超过1×104cm/s后,电池转换效率急剧下降,在背表面复合速率增大到1×106cm/s时,电池效率下降到不足5%,而在电池背表面复合速度较小时(10~103cm/s)则可获得较高的转换效率。 相似文献
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CdS/CdTe叠层太阳电池的制备及其性能 总被引:1,自引:0,他引:1
CdS/CdTe太阳电池是薄膜太阳电池研究工作的一个重要方向.为了提高开路电压Voc、改善电池的光谱响应,进而提高电池的转换效率,在此提出CdS/CdTe叠层太阳电池结构.文中,叠层电池的顶电池由CdS/CdTe超薄层构成;底电池由CdS/CdTe薄膜层构成.经分析测试,实验制备的CdS/CdTe叠层太阳电池具有明显的叠层结构,开路电压最高达到了852mV,短路电流密度最大为13mA/cm2,填充因子最高为55.2%,这种叠层电池的效率达到了8.16%(0.071cm2).研究表明相对于传统的单层CdS/CdTe太阳电池,CdS/CdTe叠层电池的制备对研究如何提高CdS/CdTe太阳电池的光伏性能有一定的参考价值. 相似文献
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CdS/CdTe太阳电池是薄膜太阳电池研究工作的一个重要方向.为了提高开路电压Voc、改善电池的光谱响应,进而提高电池的转换效率,在此提出CdS/CdTe叠层太阳电池结构.文中,叠层电池的顶电池由CdS/CdTe超薄层构成;底电池由CdS/CdTe薄膜层构成.经分析测试,实验制备的CdS/CdTe叠层太阳电池具有明显的叠层结构,开路电压最高达到了852mV,短路电流密度最大为13mA/cm2,填充因子最高为55.2%,这种叠层电池的效率达到了8.16%(0.071cm2).研究表明相对于传统的单层CdS/CdTe太阳电池,CdS/CdTe叠层电池的制备对研究如何提高CdS/CdTe太阳电池的光伏性能有一定的参考价值. 相似文献
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Zhitao Rong Xiuzhen Guo Shaoshan Lian Songwei Liu Donghuan Qin Yueqi Mo Wei Xu Hongbin Wu Hong Zhao Lintao Hou 《Advanced functional materials》2019,29(42)
Low‐cost solution‐processed CdTe nanocrystal (NC) solar cells always suffer from a high interface energy barrier and unbalanced hole/electron transport as well as anisotropic atom diffusion on the CdTe surface due to the limited amount of hole/electron interface materials or the difficulty in interface processing. In this work, a novel strategy is first adopted with gradient electron transport layer (CdS/CdSe) modification in the cathode and a new crosslinkable hole transport polymer (P‐TPA) implantation in the anode. The carrier recombination at interfaces is greatly decreased and thus the carrier collection is increased. Moreover, the light harvesting is improved both in short and long wavelength regions, making Jsc and Voc increase simultaneously. A champion solar cell shows a very high power conversion efficiency of 9.2% and an outstanding Jsc of 25.31 mA cm?2, which are among the highest values for all solution‐processed CdTe NC solar cells with a superstrate structure, and the latter value is even higher than that of traditional thick CdTe thin‐film solar cells (2 µm) via the high temperature close space sublimation method. This work demonstrates that facile surface modifications in both the cathode and anode with stepped extraction and organic–inorganic hybridization are very promising in constructing next‐generation highly efficient NC photovoltaic devices. 相似文献
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Steven Hegedus Darshini Desai Chris Thompson 《Progress in Photovoltaics: Research and Applications》2007,15(7):587-602
The voltage dependence of the photocurrent JL(V) of CdTe/CdS solar cells has been characterized by separating the forward current from the photocurrent at several illumination intensities. JL(V) reduces the fill factor (FF) of typical cells by 10–15 points, the open circuit voltage (VOC) by 20–50 mV, and the efficiency by 2–4 points. Eliminating the effect of JL(V) establishes superposition between light and dark J(V) curves for some cells. Two models for voltage dependent collection give reasonable fits to the data: (1) a single carrier Hecht model developed for drift collection in p‐i‐n solar cells in which fitting yields a parameter consistent with lifetimes of 10−9 s as measured by others; or (2) the standard depletion region and bulk diffusion length model fits almost as well. The simple Hecht‐like drift collection model for photocurrent gives very good agreement to J(V) curves measured under AM1·5 light on CdTe/CdS solar cells with FF from 53% to 70%, CdTe thickness from 1·8 to 7·0 µm, in initial and stressed states. Accelerated thermal and bias stressing increases JL(V) losses as does insufficient Cu. This method provides a new metric for tracking device performance, characterizes transport in the high field depletion region, and quantifies a significant FF loss in CdTe solar cells. Copyright © 2007 John Wiley & Sons, Ltd. 相似文献