CdS薄膜的真空热蒸发制备及在CIGS薄膜太阳电池中的应用

采用真空热蒸发(VTE)的方法制备了CdS多晶薄膜,研究了不同衬底温度对其微观结构与光电性能的影响。结果显示,不同衬底温度下制备的CdS薄膜均属于六方相多晶结构且具有(002)择优取向;随着衬底温度的升高,(002)特征衍射峰强度增加,半高宽变小,相应薄膜结晶度增大;由CdS薄膜的透射光谱可知,在500~1 000nm波段平均透过率均超过80%,光学带隙随着衬底温度的升高而增大(2.44~2.56eV),表明真空热蒸发方法制备的CdS薄膜可以作为CIGS薄膜太阳电池的缓冲层。将真空热蒸发法制备CdS薄膜与磁控溅射法制备CIGS薄膜太阳电池相结合,在同一真空室内得到了CIGS薄膜太阳电池器件,为CIGS薄膜太阳电池的工业化推广提供了新途径。     

掺Bi热蒸发CdS光导薄膜

本文用三种方法制备了掺Bi的CdS光导薄膜。一种方法是将Bi粉和CdS粉均匀混合蒸发;第二种方法是将CdS薄膜在CdS掺杂的Bi气氛中扩散,扩散温度为400～450℃;第三种方法是在CdS膜外再镀上一层很薄的Bi膜。文中介绍了它们的制备条件和光导特性,同时讨论了制备条件与光电导特性的关系。     

不同方法及衬底类型对CdS多晶薄膜性能的影响

采用化学水浴法和磁控溅射法分别在AZO、FTO、ITO透明导电玻璃衬底上制备了CdS薄膜,利用扫描电镜、XRD以及透射光谱等测试手段,研究了两种制备方法对不同衬底生长CdS薄膜形貌、结构和光学性能的影响.研究结果表明,不同方法制备的CdS薄膜表面形貌均依赖于衬底的类型,水浴法制备的CdS薄膜晶粒度较大,表面相对粗糙.不同方法制备的CdS薄膜均为立方相和六角相的混相结构,溅射法制备的多晶薄膜衍射峰清晰、尖锐,结晶性较好.水浴法制备的CdS薄膜透过率整体低于溅射法,但在短波处优势明显.     

CdS薄膜的制备、结构和光致发光性能

CdS薄膜是一种n型半导体材料,用于CdTe多晶薄膜太阳电池的窗口层,其质量直接影响太阳电池的光电转换效率和寿命。用磁控溅射法制备了CdS薄膜,通过对薄膜进行X射线衍射(XRD)、扫描电子显微镜(SEM)、光致发光和紫外-可见光谱等测试,研究了CdS薄膜的制备工艺对薄膜结晶度、表面形貌和禁带宽度的影响关系。研究发现,随着CdS薄膜溅射功率的升高,薄膜的结晶度变好,晶粒增大,薄膜增厚,光致发光峰强度增加,禁带宽度减小;随着溅射气压减小,薄膜厚度增大,光致发光峰强度减小,禁带宽度减小。     

Cu(In,Ga)Se2太阳电池缓冲层ZnS薄膜性质及应用

在含有ZnSO4,SC(NH2)2,NH4OH的水溶液中采用CBD法沉积ZnS薄膜,XRF和热处理前后的XRD测试表明,ZnS沉积薄膜为立方相结构,薄膜含有非晶态的Zn(OH)2.光学透射谱测试表明,制备的薄膜透过率(λ＞500nm)约为90%,薄膜的禁带宽度约为3.51eV.ZnS薄膜沉积时间对Cu(In,Ga)Se2太阳电池影响显著,当薄膜沉积时间在25～35min时,电池的综合性能最好.对比了不同缓冲层的电池性能,采用CBD-CdS为缓冲层的电池转换效率、填充因子、开路电压稍高于CBD-ZnS为缓冲层的无镉电池,但无镉电池的短路电流密度高于前者,两者转换效率相差2%左右.ZnS可以作为CIGS电池的缓冲层,替代CdS,实现电池的无镉化.     

Cu(In,Ga)Se2太阳电池缓冲层ZnS薄膜性质及应用

在含有ZnSO4,SC(NH2)2,NH4OH的水溶液中采用CBD法沉积ZnS薄膜,XRF和热处理前后的XRD测试表明,ZnS沉积薄膜为立方相结构,薄膜含有非晶态的Zn(OH)2.光学透射谱测试表明,制备的薄膜透过率(λ＞500nm)约为90%,薄膜的禁带宽度约为3.51eV.ZnS薄膜沉积时间对Cu(In,Ga)Se2太阳电池影响显著,当薄膜沉积时间在25～35min时,电池的综合性能最好.对比了不同缓冲层的电池性能,采用CBD-CdS为缓冲层的电池转换效率、填充因子、开路电压稍高于CBD-ZnS为缓冲层的无镉电池,但无镉电池的短路电流密度高于前者,两者转换效率相差2%左右.ZnS可以作为CIGS电池的缓冲层,替代CdS,实现电池的无镉化.     

CdS薄膜的可见和近红外光谱性能研究

在康宁7059玻璃衬底上采用磁控溅射、化学水浴和近空间升华法制备CdS薄膜,在FTO、ITO、AZO衬底上采用磁控溅射法制备CdS薄膜。分别对两组CdS薄膜的形貌、结构和光学性能进行了研究,结果表明:采用不同工艺和衬底条件制备的CdS薄膜具有不同的形貌和结构,并表现出不同的光学性能。对于不同的制备技术,化学水浴法制备的CdS薄膜在520～820nm范围的光谱平均透过率最高,光学带隙最大为2.418eV,磁控溅射法制备的CdS薄膜在820～1200nm和520～1200nm范围的光谱平均透过率最高。对于不同的衬底条件,在FTO衬底上磁控溅射制备的CdS薄膜在820～1200nm和520～1200nm范围的光谱平均透过率最高。     

CdS纳米薄膜的水浴法制备与表征

CdS是一种直接能隙半导体，其带隙约为2．42eV，是一种良好的太阳能电池窗口层材料和过渡层材料。化学水浴法沉积CdS薄膜具有工艺简单，成本低廉，成膜均匀、致密以及可大面积生产等优点。本文通过对化学水浴法沉积CdS薄膜的研究，阐述了CdS膜的生成和生长过程及其机理，并不断优化此方法中的各种工艺参数，得到了适合做铜铟镓硒薄膜太阳能电池过渡层的CdS薄膜，并对该薄膜的形貌、结构和性能进行了分析。     

GaN缓冲层对生长InN薄膜的影响

采用金属有机物化学气相沉积(MOCVD)方法生长六方相InN薄膜,利用氮化镓(GaN)缓冲层技术制备了高质量薄膜,得到了其能带带隙0.7eV附近对应的光致发光光谱(PL).通过比较未采用缓冲层,同时采用低温和高温GaN缓冲层,以及低温GaN缓冲层结合高温退火三种生长过程,发现低温GaN缓冲层结合高温退火过程能够得到更优表面形貌和晶体质量的InN薄膜,同时表征了材料的电学性质和光学性质.通过对InN薄膜生长模式的讨论,解释了薄膜表面形貌和晶体结构的差异.     

GaN缓冲层对生长InN薄膜的影响

采用金属有机物化学气相沉积(MOCVD)方法生长六方相InN薄膜,利用氮化镓(GaN)缓冲层技术制备了高质量薄膜,得到了其能带带隙0.7eV附近对应的光致发光光谱(PL).通过比较未采用缓冲层,同时采用低温和高温GaN缓冲层,以及低温GaN缓冲层结合高温退火三种生长过程,发现低温GaN缓冲层结合高温退火过程能够得到更优表面形貌和晶体质量的InN薄膜,同时表征了材料的电学性质和光学性质.通过对InN薄膜生长模式的讨论,解释了薄膜表面形貌和晶体结构的差异.     

Control of the crystalline phase and morphology of CdS deposited on microstructured surfaces by chemical bath deposition

Chemical bath deposition (CBD) has been used extensively to deposit thin films of CdS for window layers in solar cells. The microtopography or roughness of the surface, however, can affect the quality of the film by influencing the morphology, uniformity, or crystal phase of the CdS film. Here, we have demonstrated that thin films of CdS can be successfully patterned on surfaces bearing micropillars as a model surface for roughness. The phase purity of CdS deposited on the micropillar surfaces is uniform and conformal with the formation of packed clusters on the micropillars at pH 10 that form flower-like structures at long deposition times. Smaller crystallites were observed on micropillar arrays at pH 8 with “network” like structures observed at long deposition times. Additionally, by controlling the pH of the chemical bath, the hexagonal and cubic crystal phases of CdS were both accessible in high purity at temperatures as low as 85 °C.     

CdS薄膜的结构特性及其对Cu(In,Ga)Se2(CIGS)薄膜太阳电池的影响

报道了CdS薄膜的CBD法沉积及其结构特性,其中的水浴溶液包括硫脲、乙酸镉、乙酸铵和氨水溶液.研究了水浴溶液的pH值、温度、各反应物溶液的浓度和滴定硫脲与倾倒硫脲等基本工艺参数对CdS薄膜结构特性的影响.其中,溶液的pH值对CdS薄膜的特性起着关键的作用.XRD图显示了随着溶液pH值的变化,薄膜的晶相由六方相向立方相转变.CdS薄膜的这两种晶相对CIGS薄膜太阳电池性能的影响不相同.c-CdS(立方相的CdS)与CIGS之间的晶格失配和界面态密度分别为1.419%和8.507×1012cm-2,而h-CdS(六方相的CdS)与CIGS之间的晶格失配和界面态密度则分别为32.297%和2.792×1012cm-2.高效CIGS薄膜太阳电池需要的是立方相CdS薄膜.     

Cadmium sulfide thin films growth by chemical bath deposition

Cadmium sulfide (CdS) thin films have been prepared by a simple technique such as chemical bath deposition (CBD).A set of samples CdS were deposited on glass substrates by varying the bath temperature from 55 to 75 ℃ at fixed deposition time (25 min) in order to investigate the effect of deposition temperature on CdS films physical properties.The determination of growth activation energy suggests that at low temperature CdS film growth is governed by the release of Cd2+ ions in the solution.The structural characterization indicated that the CdS films structure is cubic or hexagonal with preferential orientation along the direction (111) or (002),respectively.The optical characterization indicated that the films have a fairly high transparency,which varies between 55％ and 80％ in the visible range of the optical spectrum,the refractive index varies from 1.85 to 2.5 and the optical gap value of which can reach 2.2 eV.It can be suggested that these properties make these films perfectly suitable for their use as window film in thin films based solar cells.     

Observation of Meyer–Neldel rule in CdS thin films

A study of electrical transport in CdS thin films is reported. We have observed, for the first time, that CdS thin film conductivity obeys the Meyer–Neldel rule (MNR). This was deduced from linking the conductivity pre-exponential factor to the activation energy variation. CdS films were deposited by chemical bath deposition at different solution temperatures in order to vary the electrical activation energy of the films. A correlation between the MNR rule and the disorder in the film network is highlighted. The multi-trapping process in the band tail-localized states governs the conductivity in CdS films. This explains the MNR observation in CdS films. The variation of the electrical conductivity pre-exponential factor and activation energy are correlated to the disorder in the film network; this was explained in terms of polaron formation and phonon–electron coupling with disorder.     

用化学热解沉积法制备硫化镉薄膜的微结构

在载玻片或ITO涂覆的玻璃上采用化学热解法沉积CdS固体薄膜,沉积温度在350-540℃之间,部分制备的CdS薄膜进行200-600℃的退火热处理,由SEM,AFMT和XRD分析测量退火热处理前后的CdS薄膜的微观结构,结果表明,沉积温度低于540℃以下制备的CdS薄膜具有类六方结构相当于540℃沉积的CdS薄膜的晶料尺寸依赖于沉积温度及不同基体的情况也在本文中进行了讨论。     

High Performance PbS Colloidal Quantum Dot Solar Cells by Employing Solution‐Processed CdS Thin Films from a Single‐Source Precursor as the Electron Transport Layer

CdS thin films are a promising electron transport layer in PbS colloidal quantum dot (CQD) photovoltaic devices. Some traditional deposition techniques, such as chemical bath deposition and RF (radio frequency) magnetron sputtering, have been employed to fabricate CdS films and CdS/PbS CQD heterojunction photovoltaic devices. However, their power conversion efficiencies (PCEs) are moderate compared with ZnO/PbS and TiO₂/PbS heterojunction CQD solar cells. Here, efficiencies have been improved substantially by employing solution‐processed CdS thin films from a single‐source precursor. The CdS film is deposited by a straightforward spin‐coating and annealing process, which is a simple, low‐cost, and high‐material‐usage fabrication process compared to chemical bath deposition and RF magnetron sputtering. The best CdS/PbS CQD heterojunction solar cell is fabricated using an optimized deposition and air‐annealing process achieved over 8% PCE, demonstrating the great potential of CdS thin films fabricated by the single‐source precursor for PbS CQDs solar cells.     

Comparative study between CBD and SILAR methods for deposited TiO2, CdS,and TiO2/CdS core-shell structure

TiO₂, CdS, and TiO₂/CdS core–shell structures were deposited on fluorine-doped tin oxide (FTO)-coated glass substrate using chemical methods. TiO₂ thin films were prepared by chemical bath deposition (CBD) and successive ionic layer adsorption and reaction (SILAR). SILAR was also utilized to deposit CdS film on TiO₂ thin film. The structural, surface morphology, and optical characteristics of FTO/TiO₂, FTO/CdS, and FTO/TiO₂/CdS core- shell structures were evaluated. The FTO/TiO₂ films produced by both methods conformed to anatase and rutile phase structures. Corresponding XRD pattern of the FTO/TiO₂/CdS sample exhibited one peak corresponding to hexagonal (101) for CdS. Scanning electron micrographs showed nanorod structures for the TiO₂ thin films deposited by CBD, contrary to the nanograin structure formed by SILAR. Optical results showed highly extended absorption edge to the visible region for the FTO/TiO₂/CdS structure deposited by the two methods. The TiO₂ thin films deposited by CBD exhibited higher absorption in the visible region than nanograined TiO₂ thin films deposited by SILAR because of the high surface area of the TiO₂ nanorod. Photoelectrochemical (PEC) properties of FTO/TiO₂, and FTO/TiO₂/CdS system were also examined. PEC behavior of FTO/TiO₂/CdS was compared with that of FTO/TiO₂ deposited by CBD and SILAR. The TiO₂ nanorod thin films deposited by CBD showed evidently enhanced PEC performance compared with nanograined TiO₂ thin films deposited by SILAR.     

太阳电池中CdS薄膜的制备及其性能的研究

分别采用化学池沉积(CBD)和真空蒸发法,在三种衬底(玻片、ITO玻片、SnO2玻片)上沉积CdS薄膜,并利用扫描电镜(SEM)、透射光谱、X射线衍射(XRD)等方法对沉积膜进行了测试分析,同时阐述了两种不同方法下CdS膜的生长沉积机制。