Ag层的厚度对ZnO/Ag/ZnO多层膜性能的影响

采用射频磁控溅射ZnO陶瓷靶、直流磁控溅射Ag靶的方法制备了不同厚度Ag夹层的ZnO(60nm)/Ag/ZnO(60nm)多层膜.分别用X射线衍射仪、紫外可见分光光度计、四探针测试仪对样品的结构、光学性质、电学性质进行了研究.结果表明:随着Ag层厚度的增加,ZnO/Ag/ZnO多层膜呈现多晶结构,Ag(111)衍射峰的强度增强.Ag夹层厚度为11nm时,ZnO(60nm)/Ag/ZnO(60nm)膜在554nm处的透过率高达92.3%.随着Ag层厚度的增加,Ag膜的特征吸收峰呈现红移和宽化,ZnO/Ag/ZnO多层膜的面电阻先减小后趋于稳定.     

Ag层的厚度对ZnO/Ag/ZnO多层膜性能的影响

采用射频磁控溅射ZnO陶瓷靶、直流磁控溅射Ag靶的方法制备了不同厚度Ag夹层的ZnO(60nm)/Ag/ZnO(60nm)多层膜.分别用X射线衍射仪、紫外可见分光光度计、四探针测试仪对样品的结构、光学性质、电学性质进行了研究.结果表明:随着Ag层厚度的增加,ZnO/Ag/ZnO多层膜呈现多晶结构,Ag(111)衍射峰的强度增强.Ag夹层厚度为11nm时,ZnO(60nm)/Ag/ZnO(60nm)膜在554nm处的透过率高达92.3%.随着Ag层厚度的增加,Ag膜的特征吸收峰呈现红移和宽化,ZnO/Ag/ZnO多层膜的面电阻先减小后趋于稳定.     

室温下制备的ZnO/Ag/ZnO多层膜的性能

采用射频磁控溅射ZnO陶瓷靶、直流磁控溅射Ag靶的方法在室温下制备了不同厚度的ZnO/Ag/ZnO多层膜。对样品进行了研究。结果表明:随着Ag层厚度的增加,ZnO(002)衍射峰的强度先增加后减小,Ag(111)衍射峰的强度增强,ZnO/Ag/ZnO多层膜的面电阻先减小后趋于稳定。ZnO膜厚度增加,Ag膜易形成晶状结构,ZnO/Ag/ZnO多层膜的透射峰向长波方向移动。ZnO(60nm)/Ag(11nm)/ZnO(60nm)膜在554nm处的透过率高达92.3%,面电阻为4.2?/□,品质常数?TC最佳,约40×10–3/?。     

大面积ZnO:Al窗口层的制备与研究

采用磁控溅射方法,制备了大面积(300mm×300mm)ZnO:Al薄膜作为CIGS太阳电池的窗口层。设计以电阻率和透过率测试值的标准差乘积作为衡量大面积低阻ZnO窗口层的均匀性标准,确定4mm/s作为衬底与靶材最合适的相对行走速度,并进一步研究工作气压和溅射功率对ZnO:Al薄膜结构、电学特性和光学特性的影响,实现在400～1 200nm波长范围内平均透过率大于85%,电阻率ρ约1.0×10-3Ω.cm。试验结果表明,改善的工艺条件能得到大面积内厚度均匀、光电特性良好的低阻ZnO窗口层。     

直流磁控溅射法制备本征ZnO薄膜及光伏应用研究

采用直流磁控溅射法制备了ZnO薄膜,研究了沉积过程中变换氧分压对薄膜光电性能的影响.采用XRD、紫外可见光分光光度计及AFM等方法对薄膜的结构和光电性质进行了表征.结果表明,ZnO薄膜在可见光范围内的透过率可达88％,并且随着氧分压的增大,薄膜的透过率也增大;制备出的ZnO薄膜表面粗糙度为0.41 nm.在glass/ITO/CdS/CdTe结构的太阳电池中,将本征ZnO薄膜作为高阻层加入到ITO与CdS之间,电池的开路电压和填充因子有明显的提高,加入高阻层之后,电池的转换效率最高可达13.6％.     

氧氩流量比对RF溅射ZnO:Mg薄膜结构及光学性能的影响

利用射频(RF)磁控溅射技术,采用单质Zn靶和 MgO陶瓷靶共溅射,在O₂和Ar气的混合气氛下制备了Mg掺杂ZnO(ZnO:Mg)薄膜,并通过改变O₂和Ar的流量比O ₂/Ar,研究了 对ZnO:Mg薄膜的物相结构、表面形貌及光学性能的影响。结果表明,室 温下O₂/Ar在1∶1～3∶1 范围内制备的薄膜均为单相的ZnO(002)薄膜,薄膜具有三维(3D)的结核生长模式;沉积的 ZnO:Mg薄膜在 N₂氛下200℃退火处理后,O₂/Ar为3∶1制备的薄膜在380～1200nm光谱范围内具有较高的透过率,可见光区平 均透过率约为85%、最大透过率达90%;薄膜的光学带隙 Eg为3.51eV,Mg掺杂对ZnO薄膜的光学带隙具有 较为明显的调制作用;采用极值包络线法计算表明,薄膜在589.3nm 处的折射率为1.963,膜厚约285nm。     

ITO/Ag/AgNW新型复合透明导电薄膜性能研究

采用磁控溅射和湿法涂布技术制备了一种ITO/Ag/AgNW结构的新型复合透明导电薄膜。研究其光学、电学等性能发现:ITO/Ag/AgNW薄膜在400~700nm的平均透过率高于ITO/Ag/ITO薄膜,且方块电阻远小于ITO/Ag/ITO薄膜,达到6.9Ω/□;耐弯折性能测试后,其方块电阻约增加62%,达11.2Ω/□。研究结果表明,这种新型的复合透明导电薄膜具有低阻、高透及耐弯折良好的特性,在柔性显示领域具有一定的应用潜力。     

磁控溅射法制备Ag掺杂p型ZnO薄膜的研究

采用磁控溅射法在石英玻璃基片上生长ZnO和ZnO:Ag薄膜。借助于SEM、XRD、霍尔测试、透射谱测试等方法,分析了O2气氛下退火温度对薄膜结构和电学性能的影响。霍尔测试结果表明,Ag掺杂ZnO薄膜经过600℃的O2气氛中热处理转变为p型电导。薄膜的XRD测试表明晶粒大小随退火温度升高而增大,所有薄膜样品只出现(002)衍射峰,呈现c轴取向生长。薄膜对可见光的透过率大于83%,其吸收限为378nm。     

快速热退火前后ZnO及ZnO/Al薄膜性质的研究

鉴于直流反应溅射制ZAO膜对反应条件敏感,研究发现,经快速热退火(RTA)处理能放宽对反应条件的要求。实验中ZnO及ZnO/Al薄膜用直流反应磁控溅射法制备。选用金属Zn及金属合金Zn/Al靶。经快速热退火(RTA)后,通过XRD,UV-VIS-NIR分光光度计、四探针测方电阻等,研究了经不同温度RTA后ZnO及ZnO/Al薄膜的结晶状况、方电阻、电阻率、可见光透过率等的变化。对传统热退火和RTA进行了比较:经RTA600℃后电阻率减小5~9个数量级,达1×10–3·cm。     

柔性PEN衬底ZnO：Ga薄膜的性能研究

以PEN柔性薄膜作为衬底,采用直流对靶磁控溅射的方法,在室温下制备ZnO：Ga薄膜。研究了不同溅射功率和不同溅射压强下制备出的薄膜表现出不同的光学和电学特性。经过溅射压强和溅射功率的优化,获得薄膜厚约900nm、电阻率为7．72×10^-4Ω·cm和可见光平均透过率超过75％的PEN衬底ZnO：Ga薄膜。将其应用于PE...     

反应磁控溅射直接生长绒面结构ZnO:Al-TCO薄膜及其特性研究

利用反应磁控溅射技术,在玻璃衬底上直接生长获得了"弹坑状"绒面结构的ZnO:Al-TCO薄膜。通过梯度O2生长(GOG,gradual oxygen growth)方法改善ZnO薄膜的透过率和绒度特性,并且具有较好的电学性能。通过优化实验,GOG方法生长ZnO:Al薄膜(薄膜结构:11.0sccm/10R+9.5sccm/15R)的"弹坑状"特征尺寸为300～500nm,可见光范围透过率达到90%,方块电阻约为4.0Ω/□,电子迁移率为17.4cm2/V-1.s-1。大面积镀制的ZnO:Al具有良好的绒面结构和电学均匀性,可应用于光伏(PV)产业化推广应用。     

Studies on the properties of sputter-deposited Ag-doped ZnO films

Ag-doped ZnO films were prepared by simultaneous rf magnetron sputtering of ZnO and dc magnetron sputtering of Ag on glass substrate. The influences of dopant content and substrate temperature on the properties of the as-grown films were investigated. Several analytical tools such as X-ray diffraction, spectrophotometer, atomic force microscopy, scanning electron microscopy and four-point probe were used to explore the possible changes in electrical and optical properties. The as-grown film has a preferred orientation in the (0 0 2) direction. As the amounts of the Ag dopant were increased, the crystallinity as well as the transmittance and optical band gap were decreased while the electrical resistivity increased. However, as the substrate temperature was increased, the crystallinity and the transmittance were increased. A small amount of Ag (<1 at%) lowered the resistivity by 30% with only a slight decrease in the visible transparency.     

表面等离子体共振增强ZnO/Ag薄膜发光特性研究

为了提高氧化锌光致发光强度,以磁控溅射氧化锌/银复合薄膜为研究对象,系统地研究了氧化锌薄膜的光学性质。实验中首先在硅衬底上用射频磁控溅射的方法沉积氧化锌/银复合薄膜,作为对比,同时沉积了一层氧化锌薄膜。通过扫描电子显微镜和原子力显微镜对样品的形貌及成份进行表征,并且在室温下测试样品在300~800 nm波长范围内的光致发光光谱。实验结果表明:所制得样品为均匀分布的氧化锌纳米薄膜,纯氧化锌光致发光光谱结果显示有波长位于378 nm左右的紫光、470 nm左右的蓝色发光峰存在,加入银薄膜后,氧化锌可见光区和紫外光区的光致发光光谱强度均有所增强,而且紫外光峰位出现了红移。实验结果结合样品吸收谱对光致发光机理的分析作了进一步的分析。     

同质缓冲层厚度对掺铝氧化锌薄膜性能的影响

室温下,采用射频磁控溅射法在玻璃衬底上制备具有同质缓冲层的ZnO∶Al(AZO)薄膜。用X射线衍射仪、紫外-可见分光光度计、四探针探测仪等对薄膜的结构和光电性能进行了研究。结果表明:当薄膜总厚度为400 nm时,制备具有66 nm同质缓冲层的AZO薄膜的方块电阻为26Ω.□–1,与单层AZO(400 nm)薄膜的方块电阻(63Ω.□–1)相比,下降了59%,其在可见光范围内的平均透过率为91%。     

Low resistive transparent and flexible ZnO/Ag/ZnO/Ag/WO3 electrode for organic light-emitting diodes

Transparent electrodes cannot easily be created with high transmittance and low sheet resistance simultaneously, although some optoelectronic devices, such as large organic light-emitting diode (OLED) displays and lightings, require very low resistive transparent electrodes. Here, we propose a very low resistive transparent electrode (～1.6 Ω/sq) with a high transmittance (～75%) for OLED devices, the transmittance level of which represents the highest reported value to date given such a low sheet resistance level. It consists of a stacked silver (Ag)/zinc oxide (ZnO)/Ag multilayer covered by high refractive index dielectric layers. The proposed multilayer electrode with optimal layer thicknesses has a high and wide spectral transmittance peak due to interference. The low sheet resistance is a result of two Ag layers connected via the sandwiched ZnO layer. In addition to its low sheet resistance coupled with high transmittance, the proposed multilayer electrode has good flexibility. An OLED with an anode of the stacked Ag/ZnO/Ag multilayer shows performance comparable to that of an anode of indium tin oxide.     

Electrical and optical properties of deep ultraviolet transparent conductive Ga2O3/ITO films by magnetron sputtering

Ga2O3/ITO films were prepared by magnetron sputtering on quartz glass substrates. The transmittance and sheet resistance of ITO films and Ga2O3/ITO films were measured by using a double beam spectrophotometer and four point probes. The effect of the ITO layer and Ga2O3 layer thickness on the electrical and optical properties of Ga2O3/ITO bi-layer films were investigated in detail. Ga2O3 (50 nm)/ITO (23 nm) films exhibited a low sheet resistance of 323 Ω/□ and high deep ultraviolet transmittance of 77.6% at a wavelength of 280 nm. The ITO layer controls the ultraviolet transmittance and sheet resistance of Ga2O3/ITO films. The Ga2O3 layer thickness has a marked effect on the transmission spectral shape of Ga2O3/ITO films in the violet spectral region.