共查询到19条相似文献,搜索用时 78 毫秒
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报道了转换效率为14.6%~15.8%的多晶薄膜CdS/CdTe太阳电池的研制。用MOCVD法,在玻璃衬底上制备SnO_2和SnO_2:F薄膜,水溶液化学淀积法获得80~100nm厚的CdS薄膜和密堆积升华法制备5μm厚CdTe薄膜,CdS/CdTe太阳电池的短路电流密度高达24~25mA/cm ̄2。同时,对各层薄膜晶形和微观结构进行了分析研究。 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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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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核壳半导体量子点材料因其在修复单量子点表面缺陷方面的特殊性能,极大地提高了量子点的光学性能而受到人们的研究。改进了CdTe核心的制作方法,使用小型三口瓶替代传统的小烧瓶作为反应容器,制备碲氢化钠,合成了不同核心尺寸、不同壳层厚度与不同壳层材料的10种CdTe/CdS、CdTe/ZnS核壳结构半导体量子点。对10种核壳结构半导体量子点材料进行紫外可见吸收光谱及荧光光谱测试,并分析其荧光特性。量子点在紫外可见波段的吸收光谱表明随着量子点尺寸的增大,吸收峰发生红移。通过实验结果与分析可推断出CdTe/CdS量子点荧光寿命和强度的不同是由于核心和壳层尺寸的不同量子点在I型和II型中相互转换;CdTe/ZnS的壳层厚度增加时,由于ZnS的壳层降低了核心外表的悬空键和表面缺陷态的数量,使电子空穴对复合机率加大,使得荧光峰位产生了红移。 相似文献
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在玻璃衬底上依次采用化学水浴法(CBD)和真空蒸发工艺沉积CdS和CdTe薄膜,并在不同条件下进行热处理,制备了CdTe/CdS异质结复合薄膜。利用XRD、SEM、AFM和UV-VIS透射光谱对薄膜的结构、表面形貌、剖面及光学性能进行了研究。结果表明:以玻璃衬底和CdS薄膜作为衬底沉积的CdTe多晶薄膜结构相似,均具有(1l1)面择优取向;不同条件下制备的薄膜致密且粒径均匀,随着热处理温度的升高,薄膜晶粒增大明显,并出现CdS层减薄的现象,但薄膜的粗糙度也随之增大;CdCl2氛围下热处理后,薄膜粒径增大,粗糙度明显降低,其(111)晶面的择优取向进一步增强,且透过率下降,这对于提高太阳电池的光谱响应是非常有利的。 相似文献
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An attempt is made to understand, quantify, and reduce the reflectance and photocurrent loss in CdTe solar cells. Model calculations are performed to determine the optimum thicknesses of CdS and SnO2 films and anti-reflection (AR) coating on glass that can minimize the reflectance and enhance the performance of CdTe/CdS/SnO2/glass solar cells. Photocurrent loss due to absorption in CdS films is also calculated as a function of CdS thickness. It was found that the current loss due to reflectance ando absorption is more sensitive to the CdS film when its thickness falls below 1500Å. Model calculations show that reducing the CdS thickness from 1500 to 600Å increases short-circuit current density ( Jsc) by 3 mA/cm2 because of reduced reflectance as well as absorption. Further decrease in CdS thickness below 600Å increases reflectance but results in higher Jsc, because current gain due to reduced absorption in thin CdS offsets the current loss due to higher reflectance. Model calculations also indicate that Jsc is not sensitive to SnO2 thickness above 4000Å. Finally, an optimum thickness for single layer MgF2 AR coating on glass was calculated to be 1100Å, which should provide an additional increase of 0.7 mA/cm2 in Jsc. Some of these results are also experimentally validated in this paper. 相似文献
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CAIDao-lin ZHENGJia-gui WULi-li FENGLiang-huan ZHANGJing-quan CAIYa-Ping CAIWei LIWei XIAGeng-pei YANQiang 《半导体光子学与技术》2003,9(2):95-98
ZnTe/ZnTe:Cu layer is used as a complex back contact.The parmeters of CdTe solar cells with and without the complex back contacts are compared.The effects of un-doped layer thickness,doped concentration and post-deposition annealing temperature of the complex layer on solar cells preformance are investigated.The results show that ZnTe/ZnTe:Cu layer can improve back contacts and largely increase the conversion efficiency of CdTe solar cells.Un-doped layer and post-deposition annealing of high temperature can increase open voltage.Using the complex back contact,a small CdTe cell with fill factor of 73.14% and conversion efficiency of 12.93% is obtained. 相似文献
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CdTe solar cells were fabricated by depositing CdTe films on CdS/SnO2/glass substrates in various metalorganic chemical vapor deposition growth ambient with varying Te/Cd mole ratio in the range
of 0.02 to 15. The short-circuit current density (Jsc) showed a minimum at a Te/Cd ratio of 0.1 and increased on both sides of this minimum. The open-circuit voltage (Voc) was found to be the highest for the Te-rich growth ambient (Te/Cd∼6)and was appreciably lower (600 mV as opposed to 720
mV) for the stoichiometric and the Cd-rich growth conditions. This pattern resulted in highest cell efficiency (12%) on Te-rich
CdTe films. Auger electron spectroscopy revealed a high degree of atomic interdiffusion at the CdS/CdTe interface when the
CdTe films were grown in the Te-rich conditions. It was found that the current transport in the cells grown in the Cd-rich
ambient was controlled by the tunneling/interface recombination mechanism, but the depletion region recombination became dominant
in the Te-rich cells. These observations suggest that the enhanced interdiffusion reduces interface states due to stress reduction
or to the gradual transition from CdS to CdTe. The hypothesis of reduced defect density in the CdTe cells grown in the Te-rich
conditions is further supported by the high effective lifetime, measured by time-resolved photoluminescence, and the reduced
sensitivity of quantum efficiency to forward/light bias. 相似文献
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通过应用Scharfetter-Gummel解法数值求解Poisson方程,对热平衡态p(ZnTe)/i(CdTe)/n(CdS)薄膜太阳能电池进行计算机数值模拟。结果表明,p(ZnTe)/i(CdTe)/n(CdS)的能带结构有利于光生载流子传输与收集,CdTe中高内建场提高了光生载流子通过有源区的输运能力,对CdTe进行适量P型掺杂还能提高其电池的短波收集效率。 相似文献
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E. Colegrove R. Banai C. Blissett C. Buurma J. Ellsworth M. Morley S. Barnes C. Gilmore J. D. Bergeson R. Dhere M. Scott T. Gessert Siva Sivananthan 《Journal of Electronic Materials》2012,41(10):2833-2837
Multiple polycrystalline CdS/CdTe solar cells with efficiencies greater than 15% were produced on buffered, commercially available Pilkington TEC Glass at EPIR Technologies, Inc. (EPIR, Bolingbrook, IL) and verified by the National Renewable Energy Laboratory (NREL). n-CdS and p-CdTe were grown by chemical bath deposition (CBD) and close space sublimation, respectively. Samples with sputter-deposited CdS were also investigated. Initial results indicate that this is a viable dry-process alternative to CBD for production-scale processing. Published results for polycrystalline CdS/CdTe solar cells with high efficiencies are typically based on cells using research-grade transparent conducting oxides (TCOs) requiring high-temperature processing inconducive to low-cost manufacturing. EPIR’s results for cells on commercial glass were obtained by implementing a high-resistivity SnO2 buffer layer and by optimizing the CdS window layer thickness. The high-resistivity buffer layer prevents the formation of CdTe-TCO junctions, thereby maintaining a high open-circuit voltage and fill factor, whereas using a thin CdS layer reduces absorption losses and improves the short-circuit current density. EPIR’s best device demonstrated an NREL-verified efficiency of 15.3%. The mean efficiency of hundreds of cells produced with a buffer layer between December 2010 and June 2011 is 14.4%. Quantum efficiency results are presented to demonstrate EPIR’s progress toward NREL’s best-published results. 相似文献