不同温度下制备的CdTe薄膜对太阳电池光电性能的影响

在不同温度下用近空间升华法（CSS）制备了CdTe多晶薄膜,结合I-V,C-V特性及深能级瞬态谱研究了不同温度制备的CdTe薄膜对CdS/CdTe太阳电池性能的影响.结果表明,制备温度对电池组件的开路电压影响不大,对短路电流和填充因子有影响,CdTe薄膜的深中心对温度和频率的响应基本一致.580℃制备的样品暗饱和电流密度最小,载流子浓度较高,光电特性较好,而且空穴陷阱浓度较低,深中心复合作用较小.在此研究基础上制备出了面积为300 mm×400 mm 关键词： 制备温度 CdTe薄膜 深能级瞬态谱（DLTS） CdS/CdTe太阳电池     

化学水浴法制备大面积CdS薄膜及其光伏应用

采用化学水浴法制备了大面积CdS多晶薄膜,研究了薄膜的形貌、结构和光学性质,结果表明,大面积CdS多晶薄膜具有良好的均匀性,通过优化CdS多晶薄膜,制成了不同CdS窗口层厚度的CdTe小面积太阳电池,减薄CdS薄膜可有效提高器件的短路电流,改善器件性能.随后,在面积30cm×40cm的衬底上制备了全面积为993.6cm²的CdTe太阳电池组件,其27个集成单元的电学性质较为均匀,太阳电池组件的光电转换效率8.13%. 关键词： 化学水浴法(CBD) CdS薄膜 CdTe太阳电池 CdTe太阳电池组件     

光谱分析气体状态对近空间升华沉积CdTe多晶薄膜的影响

在CdTe多晶薄膜太阳电池制备中用近空间升华法生长了CdTe多晶薄膜,沉积工作气体的状态决定了薄膜的结构、性质。文章首先分析了近空间沉积的物理机制,测量了近空间沉积装置内的温度分布,使用氩氧混合气体为工作气体,其中重点讨论了该气体状态(包括气氛和气压)与薄膜的初期成核的关系,即择优取向程度和光能隙与气氛和气压的关系。结果表明,(1)不同气氛下沉积的CdTe薄膜均为立方相结构。随氧浓度的增加,σ增加,氧浓度为6%时,σ最大,之后随氧浓度增加,σ降低,在12%达到最小,然后随氧浓度的增加而增加, 在氧浓度为9%时沉积的结晶更完整。CdTe薄膜的光能隙为1.50～1.51 eV;(2)在氩氧气氛下氧浓度为9%,不同气压下制备的样品,均有立方相CdTe, 此外, 还有CdS和SnO₂:F衍射峰。CdTe晶粒随气压增加有减小趋势,随气压的增加,透过率呈下降趋势,相应的CdTe吸收边向短波方向移动;(3)在氩氧气氛下氧浓度为9%,采用衬底温度550 ℃,源温度620 ℃,沉积时间4 min时制备的CdTe多晶薄膜获得了转换效率优良的结构为SnO₂:F/CdS/CdTe/Au的集成电池。     

ZnS/CdS复合窗口层对CdTe太阳能电池短波光谱响应的影响

采用磁控溅射法制备了ZnS/CdS复合窗口层,并将其应用于CdTe太阳能电池。对所制备薄膜的形貌和结构等进行了研究。测试了具有不同窗口层的CdTe太阳电池的量子效率和光Ⅰ-Ⅴ特性,分析了ZnS薄膜制备条件对CdTe电池器件性能影响;研究了CdS薄膜厚度和ZnS/CdS复合窗口层对短波区透过率以及CdTe太阳电池的光谱响应的影响。着重研究了具有ZnS/CdS复合窗口层的CdTe太阳电池的短波光谱响应。结果表明,CdS窗口层厚度从100 nm减至50 nm后,其对短波区光子透过率平均提高了18.3%,CdTe太阳电池短波区光谱响应平均提高了27.6%。衬底温度250 ℃条件下制备的ZnS晶粒尺寸小于室温下制备的ZnS。具有ZnS/CdS复合窗口层的CdTe电池中,采用衬底温度250 ℃沉积ZnS薄膜来制备窗口层的电池器件,其性能要优于室温下沉积ZnS制备窗口层的电池器件。这说明晶粒尺寸的大小对电子输运有一定影响。在相同厚度CdS的前提下,具有ZnS/CdS复合窗口层的CdTe电池比具有CdS窗口层在短波的光谱响应提高了约2%。这说明ZnS/CdS复合窗口层能够做到减少对短波光子的吸收,从而使更多的光子被CdTe电池的吸收层吸收。     

CdTe多晶薄膜沉积制备及其性能

在氩气和氧气混合气氛下,近空间升华法制备了CdTe多晶薄膜。薄膜的结构、性质决定于整个沉积过程。深入研究沉积过程中的热交换、物质输运,有助于获得结构致密具有良好光电性质的CdTe薄膜。分析了近空问沉积的物理机制,测量了近空间沉积装置内的温度分布,讨论了升温过程、气压与薄膜的初期成核的关系。结果表明,不同气压下制备的样品,均有立方相CdTe。此外,还有CdS和SnO2：F衍射峰。CdTe晶粒随气压增加有减小趋势;随气压的增加,透过率呈下降趋势,相应的CdTe吸收边向短波方向移动。采用衬底温度500℃,源温度620℃,在120℃的温差下,沉积时间4min上制备CdTe多晶薄膜,获得转换效率优良的结构为SnO2：F／CdS／CdTe／Au的集成电池。     

近空间升华法制备CdS多晶薄膜的研究

系统地研究了近空间升华法(CSS)制备CdS薄膜沉积速率的影响因素。发现CdS薄膜的沉积速率随升华源温度的升高而增大,但随衬底温度和沉积气压的上升而下降。对所制备样品的结构、表面形貌和光谱透过率特性进行了测试,结果表明：(1)不同氧分压下沉积的CdS薄膜沿(103)晶向择优生长。CdCl₂氛围下退火后,(103)晶向的优势得到进一步加强;(2)不同氧分压制备的CdS薄膜致密且粒径均匀,晶粒的大小随着衬底温度的升高而增大,但薄膜的粗糙度也随之增大;(3)随着CdS薄膜厚度的减小,可见光中短波段的透过率有所增大,有利于提高太阳电池的短波光谱响应。并将CSS制备的CdS多晶薄膜用于CdTe太阳电池的制作,获得了10.29%的光电转换效率,初步验证了该制作工艺的可行性。     

具有高阻抗本征SnO2过渡层的CdS/CdTe多晶薄膜太阳电池

采用超声喷雾热解法制备了具有高阻抗的本征SnO₂透明导电膜，将其运用在CdS层减薄了的CdS/CdTe多晶薄膜太阳电池中，对减薄后的CdS薄膜进行了XRD,AFM图谱分析，并对电池进行了光、暗I-V，光谱响应和C-V测试.结果表明，在高阻膜上沉积的减薄CdS薄膜(111)取向更明显，但易形成微孔.引入高阻层后，能消除CdS微孔形成的微小漏电通道，有效保护p-n结，改善了电池的并联电阻、填充因子和短波响应，使载流子浓度增加，暗饱和电流密度减小，从而电池性能得到改善，电池转换效率增加了14.4%. 关键词： CdTe电池 过渡层 效率     

碲化镉薄膜太阳电池中的关键科学问题研究

文章对CdTe薄膜太阳电池中的4个关键科学问题进行了讨论,并对电池器件的性能进行了研究,其中包括高质量硫化镉薄膜、背接触层、CdS/CdTe界面和CdCl2热处理性能的研究.文章作者研究了背电极接触层中Cu掺杂含量对电池性能的影响,通过改变背接触层中Cu的含量,可以改变Cu与Te反应产生的物相成分,从而发现以Cu1.4Te为主导的背接触缓冲层能有效地减少电池I—V曲线中的“翻转”(roll-over)现象,同时能有效地降低背接触势垒.此外,还研究了CdS/CdTe界面的CdCl2热处理反应,发现当热处理温度高于350℃时,CdS与CdTe之间的互扩散开始发生,此温度对应于CdS由立方相转变为六方相;而在550℃热处理后,S和Te互扩散形成的CdSxTe1-x化合物,其x值高达11％.通过优化电池制备工艺,获得了在AMl.5标准光源下高达14.6％的CdTe电池转换效率.     

具有高阻抗本征SnO2过渡层的CdS/CdTe多晶薄膜太阳电池

采用超声喷雾热解法制备了具有高阻抗的本征SnO2透明导电膜,将其运用在CdS层减薄了的CdS/CdTe多晶薄膜太阳电池中,对减薄后的CdS薄膜进行了XRD,AFM图谱分析,并对电池进行了光、暗I-V,光谱响应和C-V测试.结果表明,在高阻膜上沉积的减薄CdS薄膜(111)取向更明显,但易形成微孔.引入高阻层后,能消除CdS微孔形成的微小漏电通道,有效保护p-n结,改善了电池的并联电阻、填充因子和短波响应,使载流子浓度增加,暗饱和电流密度减小,从而电池性能得到改善,电池转换效率增加了14.4%.     

近距离升华沉积CdTe掺Cd薄膜的微结构和电学、光学特性

采用近距离升华技术制备了掺杂Cd元素的CdTe多晶薄膜.利用X射线衍射仪和扫描电子显微镜表征其微结构,用霍尔效应测试仪和紫外可见分光光度计分析其电学、光学特性.结果显示,适量的掺杂Cd元素可改善CdTe薄膜晶形,显著提高薄膜的电导特性,由弱的p型电导转变为导电性能良好的n型电导,但对光能隙影响不大. 关键词： 近距离升华 CdTe薄膜 掺杂Cd 电学和光学特性     

Influence of oxygen on structural and optoelectronic properties of CdS thin film deposited by magnetron sputtering technique

In this study, CdS thin films with thicknesses of approximately 100 nm were deposited at a substrate temperature of 100 °C by a sputtering technique under two different ambient conditions—pure Ar ambient and Ar/O₂ (99:1) ambient—at deposition power densities of 1.0 and 2.0 W/cm², respectively The films were polycrystalline with a preferential orientation along the (002) crystal plane; however, the films deposited in the Ar/O₂ ambient exhibited reduced crystallinity. Furthermore, the crystallite sizes, micro-strains, and dislocation densities of the films were significantly affected by oxygen diffusion into the films’ crystal structures. The CdS films deposited in the Ar/O₂ ambient demonstrated higher optical transmittance and higher bandgaps. Morphologies observed from scanning electron microscopy images revealed that the grains of the films were also significantly affected by the oxygen present in the deposition ambient. Additionally, photoluminescence analysis revealed that the sulfur vacancies in the CdS films were partially filled by oxygen atoms, causing significant variations in the electrical properties of the films.     

Investigation of CdS and CdTe thin films and influence of CdCl2 on CdTe/CdS structure

CdTe/CdS heterojunction solar cell structure has been fabricated using simple, easy and low-cost methods. To fabricate this structure, CdS and CdTe thin films are deposited onto FTO-coated conducting glass substrates by chemical bath deposition (CBD) and electrodeposition method, respectively. The optimized growth conditions are chosen for both CdS and CdTe films by investigating the optical, structural and morphological properties of both the as-deposited and annealed films. Optical measurement showed that CdS films have higher transmittance and lower absorbance, and CdTe films have lower transmittance and higher absorbance in the near infrared region. The band gap of CdS films is estimated to lie in the range 2.29–2.41 eV and that of CdTe films is in the range 1.53–1.55 eV. X-ray diffraction (XRD) study reveals that CdS and CdTe films are polycrystalline with preferential orientation of (1 1 1) plane. Scanning electron microscopy (SEM) study reveals that both films are smooth, void-free and uniformly distributed over the surface of the substrate. Fabricated CdTe/CdS structure showed the anticipated rectifying behaviour, and the rectifying behaviour is observed to improve due to CdCl₂ treatment.     

CdTe太阳电池前电极SnO2:F/SnO2复合薄膜性能分析

减薄CdS窗口层是提高CdS/CdTe太阳电池转换效率的有效途径之一,减薄窗口层会对器件造成不利的影响,因此在减薄了的窗口层与前电极之间引入过渡层非常必要.利用反应磁控溅射法在前电极SnO₂:F薄膜衬底上制备未掺杂的SnO₂薄膜形成过渡层,并将其在N₂/O₂=4 ∶1,550 ℃环境进行了30 min热处理,利用原子力显微镜、X射线衍射仪、紫外分光光度计对复合薄膜热处理前后的形貌、结构、光学性能进行了表征,同时分析了复     

CdSyTe1-y多晶薄膜的制备及光谱表征

采用真空共蒸发法制备了CdSyTe1-y(0≤y≤1)多晶薄膜,并用X射线衍射谱(XRD)、能量色散谱(EDS)研究了CdSyTe1-y多晶薄膜的结构、组分。实验结果表明:石英振荡法监控的组分与EDS谱结果较为一致;当y<0·3时,CdSyTe1-y多晶薄膜为立方结构,当y≥0·3时,CdSyTe1-y多晶薄膜为六方结构。采用XRD线形分析法可计算出CdSyTe1-y多晶薄膜晶粒大小约20～50nm。最后,用紫外-可见-近红外谱(UV-Vis-NIR),测得300～2500nmCdSyTe1-y多晶薄膜的透过率曲线,并结合一阶Sellmeier模型的折射率色散关系,表征了CdSyTe1-y多晶薄膜的光学性质,获得了CdS0·22Te0·78多晶薄膜的光学厚度d～535nm,光能隙Eg～1·41eV,以及吸收系数α(λ)、折射率n(λ)等光学量。结果也表明,采用真空共蒸发法可以制备需要组分的CdSyTe1-y多晶薄膜,对CdSyTe1-y多晶薄膜光学性质的表征方法可推广到其他的半导体薄膜材料。     

Growth, structural and optical transport properties of nanocrystal Zn1−xCdS thin films deposited by solution growth technique (SGT) for photosensor applications

Solution Growth Technique (SGT) has been used for deposition of Zn_1−xCdS nanocrystalline thin films. Various parameters such as solution pH (10.4), deposition time, concentration of ions, composition and deposition and annealing temperatures have been optimized for the development of device grade thin film. In order to achieve uniformity and adhesiveness of thin film on glass substrate, 5 ml triethanolamine (TEA) have been added in deposition solution. The as-deposited films have been annealed in Rapid Thermal Annealing (RTA) system at various temperature ranges from 100 to 500 °C in air. The changes in structural formation and optical transport phenomena have been studied with annealing temperatures and composition value (x). As-deposited films have two phases of ZnS and CdS, which were confirmed by X-ray diffraction studies; further the X-ray analysis of annealed (380 °C) films indicates that the films have nanocrystalline size (150 nm) and crystal structure depends on the films stoichiometry and annealing temperatures. The Zn_0.4CdS films annealed at 380 °C in air for 5 min have hexagonal structure where as films annealed at 500 °C have represented the oxide phase with hexagonal structure. Optical properties of the films were studied in the wavelength range 350-1000 nm. The optical band gap (E_g=2.94-2.30 eV) decreases with the composition (x) value. The effect of air rapid annealing on the photoresponse has also been observed on Zn_1−xCdS nanocrystal thin films. The Zn_1−xCdS thin film has higher photosensitivity at higher annealing temperatures (380-500 °C), and films also have mixed Zn_1−xCdS/Zn_1−xCdSO phase with larger grain size than the as-deposited and films annealed up to 380 °C. The present results are well agreed with the results of other studies.     

Low temperature ferromagnetic properties of CdS and CdTe thin films

The magnetic property in a material is induced by the unpaired electrons. This can occur due to defect states which can enhance the magnetic moment and the spin polarization. In this report, CdS and CdTe thin films are grown on FTO glass substrates by chemical bath deposition and close-spaced sublimation, respectively. The magnetic properties, which are introduced from oxygen states, are found in CdS and CdTe thin films. From the hysteresis loop of magnetic moment it is revealed that CdS and CdTe thin films have different kinds of magnetic moments at different temperatures. The M–H curves indicate that from 100 K to 350 K, CdS and CdTe thin films show paramagnetism and diamagnetism, respectively.A superparamagnetic or a weakly ferromagnetic response is found at 5 K. It is also observed from ZFC/FC curves that magnetic moments decrease with temperature increasing. Spin polarized density functional calculation for spin magnetic moment is also carried out.     

Structure and properties of zirconium oxide thin films prepared by filtered cathodic vacuum arc

Zirconium oxide (ZrO₂) thin films deposited at room temperature by the filtered cathodic vacuum arc (FCVA) technique are detailed in terms of the film structure, composition, morphology, and optical and mechanical properties, which are tailored by the oxygen (O₂) flow rate during deposition. The relationships between the film structure, composition, morphology, and properties are emphasized. With an increasing O₂ flow rate, the film evolves in structure from amorphous, through a pure monoclinic phase with varying preferential orientation, to amorphous again, accompanied by an increase in the O/Zr atomic ratio and a conversion of Zr ions from low oxidation states into Zr⁴⁺. Such a structural trend arises from the change in composition, and influences the film morphology and mechanical properties so that the amorphous films exhibit small clusters on the surface and smoother morphology as well as lower hardness compared with the polycrystalline films. The film composition rather than the density dominates the optical properties, where the transmittance and the optical band gap increase with increasing O/Zr values, while the refractive index and extinction coefficients behave conversely with the lowest refractive index (2.16 at 550 nm) approaching the bulk value (2.2) . PACS  68.55.Jk; 78.66.Nk; 68.37.Ps     

Process-parameter optimization of Sb2O3 films in the ultraviolet and visible region for interferometric applications

The influence of different evaporation process parameters on the optical properties and constants of thin Sb₂O₃ films in the ultraviolet and visible region from 250 to 800 nm has been investigated. The most dominant parameters, namely the substrate temperature, rate of evaporation, and ambient oxygen pressure used during the deposition process and the post-annealing temperatures were optimised which resulted in low loss, dense and homogeneous Sb₂O₃ films. The optical constants and band gaps of these films were evaluated using their interference modulated transmittance spectra in case of both homogeneous and inhomogeneous conditions. Optimized films have been successfully used in developing multilayer high reflecting coatings for Fabry-Perot etalons along with the cryolite (Na₃AlF₆) films.     

Optical and structural properties of CdS thin films grown by chemical bath deposition doped with Ag by ion exchange

In this work thin CdS films using glycine as a complexing agent were fabricated by chemical bath deposition and then doped with silver (Ag), by an ion exchange process with different concentrations of AgNO₃ solutions. The CdS films were immersed in silver solutions using different concentrations during 1 min for doping and after that the films were annealed at 200 °C during 20 min for dopant diffusion after the immersion on the AgNO₃ solutions. The aim of this research was to know the effects of different concentrations of Ag on the optical and structural properties of CdS thin films. The optical band gap of the doped films was determined by transmittance measurements, with the results of transmittance varying between 35% and 70% up to 450 nm in the electromagnetic spectra and the band gap varying between 2.31 and 2.51 eV depending of the silver content. X-ray photoelectron spectroscopy was used to study the influence of silver on the CdS:Ag films, as a function of the AgNO₃ solution concentration. The crystal structure of the thin CdS:Ag films was studied by the X-ray diffraction method and the film surface morphology was studied by atomic force microscopy. Using the ion exchange process, the CdS films’ structural, optical and electric characteristics were modified according to silver nitrate concentration used.