用光学透射谱分析薄膜光学参量的一种简易方法

基于经典的色散理论建立的单振子光谱分析模型,通过理论推导,借助计算机辅助处理,提出了一种比较简捷直观的只利用垂直透射光谱对薄膜光谱进行分析的方法.利用这种方法分析了直流溅射制备的ZnO薄膜的透射光谱,计算出了薄膜在透明振荡区的折射率色散关系以及厚度等参量,并对分析方法给出了验证.     

透射光谱法测试双面薄膜的光学参数

由于普通的化学气相沉积法制作高掺Sn的二氧化硅薄膜比较容易产生结晶,而溶胶-凝胶法制备薄膜化学组成比较容易控制,可以制作出掺Sn浓度较大的材料。文章采用了溶胶-凝胶的方法制备出了66 mol%和75 mol%两种不同浓度的掺Sn的SiO₂薄膜,用浸渍法多次提拉薄膜以增加薄膜的厚度,之后用紫外-可见分光光度计测量了薄膜的透射光谱。之前基于透射光谱的方法计算玻璃基底上薄膜的光学参数都是针对单面薄膜,该文针对浸渍法产生的双面薄膜,建立了相对应的薄膜模型,并分别用包络线法计算出了两种不同薄膜样品的光学参数。计算结果表明两种不同薄膜样品的折射率随着波长的增加而增加,薄膜的厚度都为900 nm左右。     

基于反射和透射光谱的氢化非晶硅薄膜厚度及光学常量计算

采用紫外-可见透射光谱仪测量了对靶磁控溅射沉积法制备的氢化非晶硅（a-Si:H）薄膜的透射光谱和反射光谱.利用T/(1-R)方法来确定薄膜的吸收系数,进而得到薄膜的消光系数|通过拟合薄膜透射光谱干涉极大值和极小值的包络线来确定薄膜折射率和厚度的初始值,并利用干涉极值公式进一步优化薄膜的厚度值和折射率|利用柯西公式对得到的薄膜折射率进行拟合,给出了a-Si:H薄膜的色散关系曲线.为了验证该方法确定的薄膜厚度和光学常量的可靠性,将理论计算得到的透射光谱与实验数据进行了比较,结果显示两条曲线基本重合,可见这是确定a-Si:H薄膜厚度及光学常量的一种有效方法.     

Ge-Sb-Se硫系薄膜制备及光学特性研究

介绍了几种常见的硫系薄膜制备方法, 根据现有实验条件采用热蒸发法和磁控溅射法制备出Ge-Sb-Se三元体系硫系薄膜, 通过台阶仪测试薄膜的厚度和表面粗糙度, 计算出两种制备方法的成膜速率, 并通过X射线光电子能谱测试了两种制备方法所得薄膜与块体靶材组分的差别. 利用Z扫描技术和分光光度计测试了热蒸发法制备所得薄膜的三阶非线性性能和透过光谱, 计算出非线性折射率、非线性吸收系数和薄膜厚度等参数. 结果表明热蒸发法制备Ge-Sb-Se薄膜具有良好的物理结构和光学特性, 在集成光学器件方面很高的应用潜力.     

基于反射和透射光谱的氢化非晶硅薄膜厚度及光学常量计算

采用紫外-可见透射光谱仪测量了对靶磁控溅射沉积法制备的氢化非晶硅( a-Si:H)薄膜的透射光谱和反射光谱.利用T/(1-R)方法来确定薄膜的吸收系数,进而得到薄膜的消光系数;通过拟合薄膜透射光谱干涉极大值和极小值的包络线采确定薄膜折射率和厚度的初始值,并利用干涉极值公式进一步优化薄膜的厚度值和折射率;利用柯西公式对得...     

厚度对未掺杂ZnO薄膜光谱性能的影响

X射线衍射光谱、拉曼光谱和紫外可见透射光谱技术是薄膜材料检测的重要技术手段。通过对薄膜材料光谱性能的分析,可以获得薄膜材料的物相、晶体结构和透光性能等信息。为了解厚度对未掺杂ZnO薄膜的X射线衍射光谱、拉曼光谱和紫外可见透射光谱性能的影响,利用溶胶-凝胶法在石英衬底上旋涂制备了不同厚度的未掺杂ZnO薄膜样品,并对薄膜样品进行了X射线衍射光谱、拉曼光谱和紫外可见透射光谱的检测。首先,通过X射线衍射光谱检测发现,薄膜样品呈现出（002）晶面的衍射峰,ZnO薄膜为六角纤锌矿结构,均沿着C轴择优取向生长,且随着薄膜厚度的增加,衍射峰明显增强,ZnO薄膜的晶粒尺寸随着膜厚的增加而长大。利用扫描电子显微镜对薄膜样品的表面形貌分析显示,薄膜表面致密均匀,具有纳米晶体的结构,其晶粒具有明显的六角形状。通过拉曼光谱检测发现,薄膜样品均出现了437 cm-1的拉曼峰,这是ZnO纤锌矿结构的特征峰,且随着薄膜厚度的增加,其特征拉曼峰强度也增加,进一步说明了随着ZnO薄膜厚度的增加,ZnO薄膜晶化得到了加强。最后,通过紫外可见透射光谱测试发现,随着膜厚的增加,薄膜的吸收边发生一定红移,薄膜样品在可见光区域内的透过率随着膜厚度增加而略有降低,但平均透过率都超过90%。通过对薄膜样品的紫外-可见透射光谱进一步分析,估算了薄膜样品的折射率,定量计算了薄膜样品的光学禁带宽度,计算结果表明：厚度的改变对薄膜样品的折射率影响不大,但其禁带宽度随着薄膜厚度的增加而变窄,且均大于未掺杂ZnO禁带宽度的理论值3.37 eV。进一步分析表明,ZnO薄膜厚度的变化与ZnO晶粒尺寸的变化呈正相关,本质上,吸收边或光学禁带宽度的变化是由于ZnO晶粒尺寸变化引起的。     

用分光光度法研究非晶硅薄膜的光学性质

提出了一种测量薄膜透射光谱的方法.该方法用自制的夹具改进了分光光度计,保证了在测量大小不同的样品时参考光的强度和入射到待测样品上光的强度相同.利用改进后的分光光度计测量了沉积在玻璃衬底上非晶硅薄膜的透射光谱,并对透射光谱进行了拟合和计算,确定出非晶硅薄膜的光学常量和厚度.     

金属有机分解法制备的SrTiO3薄膜的光学特性

采用金属有机分解法（MOD）在石英衬底上沉积了SrTiO3薄膜。所制备的薄膜是晶格常数为a=b=c=3.90?的多晶结构。通过测量190—1100nm波段内的透射光谱，采用包络方法计算了薄膜的光学常数（折射率n和消光系数k）。结果表明，采用MOD方法制备的薄膜的折射率大于采用射频磁控溅射、溶胶—凝胶和化学气相沉积方法制备的薄膜的折射率；薄膜的折射率色散关系满足单振子模型，其中振子强度S0为0.88′1014m-2，振子能量E0为6.40eV；薄膜的禁带宽度为3.68eV。     

椭偏透射法测量氢化非晶硅薄膜厚度和光学参数

针对多角度椭偏测量透明基片上薄膜厚度和光学参数时基片背面非相干反射光的影响问题,报道了利用椭偏透射谱测量等离子增强化学气相沉积法(PECVD)制备的a-Si:H薄膜厚度和光学参数的方法,分析了基片温度T_s和辉光放电前气体温度T_g的影响.研究表明,用椭偏透射法测量的a-Si:H薄膜厚度值与扫描电镜(SEM)测得的值相当,推导得到的光学参数与其他研究者得到的结果一致.该方法可用于生长在透明基片上的其他非晶或多晶薄膜. 关键词： 椭偏测量 透射法 光学参数 氢化非晶硅薄膜     

超薄原子蒸汽的透射与反射光谱

通过数值分析研究了超薄气体的透射与反射光谱特性与其厚度大小的树应关系。研究表明,透射光谱随薄膜厚度的增大而展宽,光谱呈现对称性,而在反射的情况下,这一对称性由薄膜厚度为1／4波长的奇数或偶数倍决定。     

Surface chemical states of barium zirconate titanate thin films prepared by chemical solution deposition

Ba(Zr_0.05Ti_0.95)O₃ (BZT) thin films grown on Pt/Ti/SiO₂/Si(1 0 0) substrates were prepared by chemical solution deposition. The structural and surface morphology of BZT thin films has been studied by X-ray diffraction (XRD) and scanning electron microscope (SEM). The results showed that the random oriented BZT thin film grown on Pt/Ti/SiO₂/Si(1 0 0) substrate with a perovskite phase. The SEM surface image showed that the BZT thin film was crack-free. And the average grain size and thickness of the BZT film are 35 and 400 nm, respectively. Furthermore, the chemical states and chemical composition of the films were determined by X-ray photoelectron spectroscopy (XPS) near the surface. The XPS results show that Ba, Ti, and Zr exist mainly in the forms of BZT perovskite structure.     

Infrared optical properties of Ba(Zr0.20Ti0.80)O3 and Ba(Zr0.30Ti0.70)O3 thin films prepared by sol-gel method

Ba(Zr_xTi_1−x)O₃ (BZT) (x = 0.20 and 0.30) thin films are deposited on Pt(1 1 1)/Ti/SiO₂/Si(1 0 0) substrate by sol-gel method. X-ray diffraction patterns show that the thin films have a good crystallinity. Optical properties of the films in the wavelength range of 2.5-12 μm are studied by infrared spectroscopic ellipsometry (IRSE). The optical constants of the BZT thin films are determined by fitting the IRSE data using a classical dispersion formula. As the wavelength increases, the refractive index decreases, while the extinction coefficients increase. The effective static ionic charges are derived, which are smaller than that in a purely ionic material for the BZT thin films.     

Effects of texture on the dielectric properties of Ba(Zr0.2Ti0.8)O3 thin films prepared by pulsed laser deposition

Ba(Zr_0.2Ti_0.8)O₃ (BZT) thin films were deposited on Pt(111)/Ti/SiO₂/Si(100) substrates by a pulsed laser deposition process. The BZT thin films directly grown on annealed and un-annealed Pt/Ti/SiO₂/Si substrates exhibited random and high (100) orientations, respectively. The dielectric constant of a 400-nm-thick BZT film with (100) orientation was 331, which was higher than that of a BZT film with random orientation (∼236). This result is attributed to the fact that the polar axis of the (100)-oriented films was more tilted away from the normal to the film surface than that of the randomly oriented films. Also, the tunabilities of BZT thin films with random and (100) orientations were ∼50% and ∼59% at an applied field of 400 kV/cm, respectively. Improved tunability has been attributed to the (100) texture of the film leading to an enhancement of the in-plane-oriented polar axis. PACS 77.22.-d; 77.55.+f; 77.80.-e; 77.84.-s     

埋藏于有机介质中金属原子团的结构研究(I)

利用双源同时蒸发和U型管热壁蒸发法制备了两种金属-有机复合薄膜Ag-7,7,8,8-tetracyanoquinodimethane和Ag-1,4-bis-(1,1-dicyanovinyl)-benze.利用透射电子显微镜和可见—紫外光谱研究了所制备的金属-有机复合薄膜的结构特性，发现它们是一种金属原子团埋藏于具有π-共轭体系的有机介质中的薄膜体系. 关键词：     

Effect of K-doping on structural and optical properties of ZnO thin films

In this work, K-doped ZnO thin films were prepared by a sol–gel method on Si(111) and glass substrates. The effect of different K-doping concentrations on structural and optical properties of the ZnO thin films was studied. The results showed that the 1 at.% K-doped ZnO thin film had the best crystallization quality and the strongest ultraviolet emission ability. When the concentration of K was above 1 at.%, the crystallization quality and ultraviolet emission ability dropped. For the K-doped ZnO thin films, there was not only ultraviolet emission, but also a blue emission signal in their photoluminescent spectra. The blue emission might be connected with K impurity or/and the intrinsic defects (Zn interstitial and Zn vacancy) of the ZnO thin films.     

氢水平衡法制备二氧化钒薄膜及XPS能谱分析

采用溶胶－凝胶法，结合氢水平衡还原处理得到了二氧化钒薄膜，对薄膜的XPS能谱分析及对反应体系的热力学分析表明，氢水 平衡还原处理是制备二氧化钒薄膜的一种可行方法。     

Comparison of ZnO thin films grown on a polycrystalline 3C-SiC buffer layer by RF magnetron sputtering and a sol-gel method

Zinc oxide (ZnO) thin films were deposited on a polycrystalline (poly) 3C-SiC buffer layer using RF magnetron sputtering and a sol-gel method. The post-deposition annealing was performed on ZnO thin films prepared using both methods. The formation of ZnO piezoelectric thin films with less residual stress was due to a close lattice mismatch of the ZnO and SiC layers as obtained by the sputtering method. Nanocrystalline, porous ZnO film prepared using the sol-gel method showed strong ultraviolet UV emission at a wavelength of 380 nm. The 3C-SiC buffer layer improved the optical and piezoelectric properties of the ZnO film produced by the two deposition methods. Moreover, the different structures of the ZnO films on the 3C-SiC intermediate layer caused by the different deposition techniques were also considered and discussed.     

Structural and optical properties of Ba(Zn1/3Ta2/3)O3 thin films deposited by pulsed laser deposition

Ba(Zn_1/3Ta_2/3)O₃, (BZT), is a high-k and low loss dielectric resonator material which finds applications in the area of microwave communication and related areas. While there are reports on its bulk properties, there is hardly any report on its thin films. We report here preparation of thin films of BZT deposited on to borosilicate and quartz substrates using the pulsed laser deposition (PLD) technique under different oxygen mixing percentage (OMP) and preliminary studies on their structural and optical properties. The EDAX spectra show that the deposited films exhibit the composition of the target. As-deposited films, whether on a glass or quartz substrate, were found to be amorphous. The refractive index and energy bandgap of the films were found to be around 1.5 in the dispersion free region (500–1500 nm) and 5.2–5.5 eV, respectively. The Dynamic Force Microscopy (DFM) study of the BZT films exhibited columnar growth and films deposited at higher OMPs showed the smaller grain size.     

用锌金属有机源和二氧化碳等离子体增强化学气相沉积的方法制备高质量氧化锌薄膜

报道了用金属锌有机源和二氧化碳混合气源等离子体增强化学气相沉积(PECVD)的方法成功地制备高质量择优取向(0002)的ZnO薄膜。通过X-ray衍射谱进行了结构分析得到六方结构,择优取向,晶粒尺寸大约在220nn.并通过原子力显微镜分析更进一步验证了晶粒的尺寸。通过透射谱分析观察到了典型的激子吸收线。这种方法的特点是可以在低温条件下在任何衬底上生长大面积均匀性好、结晶度高的ZnO薄膜。     

Influence of MgO and ZrO2 buffer layers on dielectric properties of Ba(Zr0.20Ti0.80)O3 thin films prepared by sol-gel processing

Ba(Zr_0.20Ti_0.80)O₃ (BZT) thin films are deposited on Pt(1 1 1)/Ti/SiO₂/Si, MgO and ZrO₂ buffered Pt(1 1 1)/Ti/SiO₂/Si substrates by a sol-gel process. The BZT thin films directly grown on Pt(1 1 1)/Ti/SiO₂/Si substrates exhibit highly (1 1 1) preferred orientation, while the films deposited on Pt(1 1 1)/Ti/SiO₂/Si substrates with MgO and ZrO₂ buffer layers show highly (1 1 0) preferred orientation. At 100 kHz, dielectric constants are 417, 311 and 321 for the BZT thin films grown on Pt(1 1 1)/Ti/SiO₂/Si, MgO and ZrO₂ buffered Pt(1 1 1)/Ti/SiO₂/Si substrates, respectively. The difference in dielectric properties of three BZT films can be attributed to the series capacitance effect, interface conditions and their orientations.