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1.
ZrO2/SiO2多层膜由相同沉积条件下的电子束蒸发方法制备而成,通过改变多层膜中高(ZrO2)、低(SiO2)折射率材料膜厚组合周期数的方法,研究了沉积在熔石英和BK7玻璃基底上多层膜中残余应力的变化.用ZYGO光学干涉仪测量了基底镀膜前后曲率半径的变化,并确定了薄膜中的残余应力.结果发现,该多层膜中的残余应力为压应力,随着薄膜中膜厚组合周期数的增加,压应力值逐渐减小.而且在相同条件下,石英基底上所沉积多层膜中的压应力值要小于BK7玻璃基底上所沉积多层膜中的压应力值.用x射线衍射技术测量分析了膜厚组合周期数不同的ZrO2/SiO2多层膜微结构,发现随着周期数增加,多层膜的结晶程度增强.同时多层膜的微结构应变表现出了与所测应力不一致的变化趋势,这主要是由多层膜中,膜层界面之间复杂的相互作用引起的.  相似文献   

2.
以丙醇锆(ZrPr)为锆源,二乙醇胺(DEA)为络合剂,原位引入聚乙烯吡咯烷酮(PVP),在乙醇体系中成功地合成了PVP掺杂-ZrO2溶胶.采用旋涂法在K9玻璃基片上制备了PVP-ZrO2单层杂化薄膜.用不同掺杂量的PVP-ZrO2高折射率膜层与相同的SiO2低折射率膜层交替沉积四分之一波堆高反射膜.借助小角X射线散射研究胶体微结构,用红外光谱、原子力显微镜、紫外/可见/近红外透射光谱、椭圆偏振仪以及1064nm的强激光辐照实验对薄膜的结构、光学和抗激光损伤性能进行表征.研究发现,体系组成的适当配置可以在溶胶稳定的前提下实现ZrPr的充分水解,赋予薄膜良好的结构、光学和抗激光损伤性能.杂化体系中,DEA与ZPr之间强的配合作用大大降低了ZrO2颗粒表面羟基的活性,使得PVP大分子只是以微弱的氢键与颗粒的表面羟基作用而均匀分散于ZrO2颗粒的周围,对颗粒的形成和生长无显著影响.因而在实验研究范围内,随PVP含量的增大,PVP-ZrO2杂化膜层的折射率和激光损伤阈值均无显著变化.但是,薄膜中均匀分布的PVP柔性链可以有效促进膜层应力松弛,显著削弱不同膜层之间的应力不匹配程度、大大方便多层光学薄膜的制备.当高折射率膜层中PVP的质量分数达到15%—20%时,膜层之间良好的应力匹配使得多层高反射膜的沉积周期数可达到10以上.沉积10个周期的多层反射膜,在中心波长1064nm处透射率约为1.6%—2.1%,接近全反射特征,其激光损伤阈值为16.4—18.2J/cm2(脉冲宽度为1ns). 关键词: 溶胶-凝胶 2')" href="#">PVP-ZrO2 高反射膜 激光损伤  相似文献   

3.
SiO2的赝晶化及AlN/SiO2纳米多层膜的超硬效应   总被引:1,自引:0,他引:1       下载免费PDF全文
赵文济  孔明  黄碧龙  李戈扬 《物理学报》2007,56(3):1574-1580
采用反应磁控溅射法制备了一系列不同SiO2层厚度的AlN/SiO2纳米多层膜,利用X射线衍射仪、高分辨透射电子显微镜和微力学探针表征了多层膜的微结构和力学性能,研究了SiO2层在多层膜中的晶化现象及其对多层膜生长方式及力学性能的影响. 结果表明,由于受AlN六方晶体结构的模板作用,溅射条件下以非晶态存在的SiO2层在其厚度小于0.6 nm时被强制晶化为与AlN相同的六方结构赝晶体并与AlN形成共格外延生长. 由于不同模量的两调制层存在晶格错配度,多层膜中产生了拉、压交变的应力场,使得多层膜产生硬度升高的超硬效应. SiO2随层厚的进一步增加又转变为以非晶态生长,多层膜的外延生长结构受到破坏,其硬度也随之降低. 关键词: 2纳米多层膜')" href="#">AlN/SiO2纳米多层膜 赝晶化 应力场 超硬效应  相似文献   

4.
岳建岭  孔明  赵文济  李戈扬 《物理学报》2007,56(3):1568-1573
采用V和SiO2靶通过反应溅射方法制备了一系列具有不同SiO2和VN调制层厚的VN/SiO2纳米多层膜. 利用X射线衍射、X射线能量色散谱、高分辨电子显微镜和微力学探针表征了多层膜的微结构和力学性能. 结果表明:在Ar,N2混和气体中,射频反应溅射的SiO2薄膜不会渗氮. 单层膜时以非晶态存在的SiO2,当其厚度小于1nm时,在多层膜中因VN晶体层的模板效应被强制晶化,并与VN层形成共格外延生长. 相应地,多层膜的硬度得到明显提高,最高硬度达34GPa. 随SiO2层厚度的进一步增加,SiO2层逐渐转变为非晶态,破坏了与VN层的共格外延生长结构,多层膜硬度也随之降低. VN调制层的改变对多层膜的生长结构和力学性能也有影响,但并不明显. 关键词: 2纳米多层膜')" href="#">VN/SiO2纳米多层膜 共格外延生长 非晶晶化 超硬效应  相似文献   

5.
TiO2和SiO2薄膜应力的产生机理及实验探索   总被引:2,自引:0,他引:2       下载免费PDF全文
顾培夫  郑臻荣  赵永江  刘旭 《物理学报》2006,55(12):6459-6463
对最常用的TiO2和SiO2薄膜应力, 包括应力模型、应力测试方法和不同实验条件下的应力测试结果作了研究.基于曲率法模型,对TiO2和SiO2单层膜和多层膜进行了实验测试,得到了一些有价值的结果,特别是离子辅助淀积和基板温度等工艺参数对薄膜应力的影响.提出了薄膜聚集密度是应力的重要因素,低聚集密度产生张应力,而高聚集密度产生压应力.在多层膜中通过调节工艺参数,适当地控制张应力或压应力,可使累积应力趋向于零. 关键词: 薄膜应力 离子辅助淀积 聚集密度  相似文献   

6.
沈斌  张旭  熊怀  李海元  谢兴龙 《光学学报》2023,(11):291-297
采用溶胶凝胶法制备得到以正丙醇锆和正硅酸乙酯为前驱体的ZrO2和SiO2溶胶,通过TFCalc光学薄膜软件模拟了ZrO2/SiO2三层“宽M型”基频二倍频减反膜,并使用提拉法制备得到了该均匀膜层。三层减反膜在527 nm和1053 nm处的透过率约为99.5%,且透过率大于99%的波长范围均超过150 nm。经热处理后的膜层表面均方根粗糙度为1.34 nm,表面平整性良好;并运用1-on-1激光损伤阈值测试方法测得该减反膜的零几率激光损伤阈值达到36.8 J·cm-2(1064 nm,10.7 ns)。  相似文献   

7.
利用多靶磁控溅射技术制备了Au/SiO2纳米颗粒分散氧化物多层复合薄膜.研究了在保持Au单层颗粒膜沉积时间一定时薄膜厚度一定、变化SiO2的沉积时间及SiO2的沉积时间一定而改变薄膜厚度时,多层薄膜在薄膜厚度方向的微观结构对吸收光谱的影响.研究结果表明:具有纳米层状结构的Au/SiO2多层薄膜在560 nm波长附近有明显的表面等离子共振吸收峰,吸收峰的强度随Au颗粒的浓度增加而增强,在Au颗粒浓度相同的情况下,复合薄膜 关键词: 2纳米复合薄膜')" href="#">Au/SiO2纳米复合薄膜 多靶磁控溅射 吸收光谱 有效介质理论  相似文献   

8.
在SiO2玻璃衬底上用脉冲激光沉积(PLD)技术,分别沉积Ti和Ti/Al膜,经电化学阳极氧化成功制备了多孔TiO2/SiO2和TiO2/Al/SiO2纳米复合结构. 其中TiO2薄膜上的微孔阵列高度有序,分布均匀. 实验研究了Al过渡层对多孔TiO2薄膜光吸收特性的影响. 结果表明:无Al过渡层的多孔TiO2薄膜其紫外吸收峰在27 关键词: 2薄膜')" href="#">多孔TiO2薄膜 阳极氧化 紫外光吸收  相似文献   

9.
利用电泳法在金属基底上制备MgB2超导厚膜   总被引:2,自引:0,他引:2       下载免费PDF全文
利用电泳技术在高熔点金属基底Ta,Mo和W上制备MgB2超导厚膜.厚膜中的MgB2晶粒结合紧密,粒度小于1μm,呈随机取向生长.电阻测量表明沉积在Ta,Mo,W上的MgB2厚膜的超导起始转变温度分别为36.5K,34.8K,33.4K,对应的转变宽度为0.3K,1.5K和2.0K.三种基底上制备的MgB2厚膜的临界电流密度在不同温度下随外磁场的变化情况 基本相同,MgB2/Mo厚膜的临界电流密 关键词: 2超导厚膜')" href="#">MgB2超导厚膜 电泳 金属基底  相似文献   

10.
沉积速率和氧分压对HfO2薄膜残余应力的影响   总被引:1,自引:0,他引:1       下载免费PDF全文
岑态  章岳光  陈卫兰  顾培夫 《物理学报》2009,58(10):7025-7029
采用ZYGO MarkIII-GPI数字波面干涉仪对以K9玻璃为基底的电子束蒸发方法制备的HfO2薄膜中的残余应力进行了研究,讨论了沉积速率、氧分压这两种工艺参量对HfO2薄膜残余应力的影响.实验结果表明:在所有的工艺条件下,薄膜的残余应力均为张应力;随着沉积速率的升高,氧分压的减小,薄膜的堆积密度逐渐增大,而残余应力呈减小趋势.同时用X射线衍射技术测量分析了不同工艺条件下HfO2薄膜的晶体结构,探讨了HfO2薄膜晶体 关键词: 残余应力 2薄膜')" href="#">HfO2薄膜 沉积速率 氧分压  相似文献   

11.
Shao S  Shao J  He H  Fan Z 《Optics letters》2005,30(16):2119-2121
The effects of repeating thickness periods on stress are studied in ZrO2/SiO2 multilayers deposited by electron-beam evaporation on BK7 glass and fused-silica substrates. The results show that the residual stress is compressive and decreases with an increase of the periods of repeating thickness in the ZrO2/SiO2 multilayers. At the same time, the residual stress in multilayers deposited on BK7 glass is less than that of samples deposited on fused silica. The variation of the microstructure examined by x-ray diffraction shows that microscopic deformation does not correspond to macroscopic stress, which may be due to variation of the interface stress.  相似文献   

12.
Zirconium dioxide (ZrO2) thin films were deposited on BK7 glass substrates by the electron beam evaporation method. A continuous wave CO2 laser was used to anneal the ZrO2 thin films to investigate whether beneficial changes could be produced. After annealing at different laser scanning speeds by CO2 laser, weak absorption of the coatings was measured by the surface thermal lensing (STL) technique, and then laser-induced damage threshold (LIDT) was also determined. It was found that the weak absorption decreased first, while the laser scanning speed is below some value, then increased. The LIDT of the ZrO2 coatings decreased greatly when the laser scanning speeds were below some value. A Nomarski microscope was employed to map the damage morphology, and it was found that the damage behavior was defect-initiated both for annealed and as-deposited samples. The influences of post-deposition CO2 laser annealing on the structural and mechanical properties of the films have also been investigated by X-ray diffraction and ZYGO interferometer. It was found that the microstructure of the ZrO2 films did not change. The residual stress in ZrO2 films showed a tendency from tensile to compressive after CO2 laser annealing, and the variation quantity of the residual stress increased with decreasing laser scanning speed. The residual stress may be mitigated to some extent at proper treatment parameters.  相似文献   

13.
In this work, we report the formation of CuInS2 thin films on glass substrates by heating chemically deposited multilayers of copper sulfide (CuS) and indium sulfide (In2S3) at 300 and 350 °C in nitrogen atmosphere at 10 Torr. CIS thin films were prepared by varying the CuS layer thickness in the multilayers with indium sulfide. The XRD analysis showed that the crystallographic structure of the CuInS2 (JCPDS 27-0159) is present on the deposited films. From the optical analysis it was estimated the band gap value for the CIS film (1.49 eV). The electrical conductivity varies from 3 × 10−8 to 3 Ω−1 cm−1 depending on the thickness of the CuS film. CIS films showed p-type conductivity.  相似文献   

14.
研究了Si3N4层在ZrN/Si3N4纳米多层膜中的晶化现象及其对多层膜微结构与力学性能的影响. 一系列不同Si3N4层厚度的ZrN/Si3N4纳米多层膜通过反应磁控溅射法制备. 利用X射线衍射仪、高分辨透射电子显微镜和微力学探针表征了多层膜的微结构和力学性能. 结果表明,由于受到ZrN调制层晶体结构的模板作用,溅射条件下以非晶态存在的Si3N4层在其厚度小于0.9 nm时被强制晶化为NaCl结构的赝晶体,ZrN/Si3N4纳米多层膜形成共格外延生长的柱状晶,并相应地产生硬度升高的超硬效应. Si3N4随层厚的进一步增加又转变为非晶态,多层膜的共格生长结构因而受到破坏,其硬度也随之降低.  相似文献   

15.
In this study, SnO2/TiO2 thin films are fabricated on SiO2/Si and Corning glass 1737 substrates using a R.F. magnetron sputtering process. The gas sensing properties of these films under an oxygen atmosphere with and without UV irradiation are carefully examined. The surface structure, morphology, optical transmission characteristics, and chemical compositions of the films are analyzed by atomic force microscopy, scanning electron microscopy and PL spectrometry. It is found that the oxygen sensitivity of the films deposited on Corning glass 1737 substrates is significantly lower than that of the films grown on SiO2/Si substrates. Therefore, the results suggest that SiO2/Si is an appropriate substrate material for oxygen gas sensors fabricated using thin SnO2/TiO2 films.  相似文献   

16.
李微  赵彦民  刘兴江  敖建平  孙云 《中国物理 B》2011,20(6):68102-068102
Mo thin films are deposited on soda lime glass (SLG) substrates using DC magnetron sputtering. The Mo film thicknesses are varied from 0.08 μm to 1.5 μm to gain a better understanding of the growth process of the film. The residual stresses and the structural properties of these films are investigated, with attention paid particularly to the film thickness dependence of these properties. Residual stress decreases and yields a typical tensile-to-compressive stress transition with the increase of film thickness at the first stages of film growth. The stress tends to be stable with the further increase of film thickness. Using the Mo film with an optimum thickness of 1 μm as the back contact, the Cu(InGa)Se2 solar cell can reach a conversion efficiency of 13.15%.  相似文献   

17.
We describe the structural properties and electrical characteristics of thin thulium oxide (Tm2O3) and thulium titanium oxide (Tm2Ti2O7) as gate dielectrics deposited on silicon substrates through reactive sputtering. The structural and morphological features of these films were explored by X-ray diffraction, X-ray photoelectron spectroscopy, secondary ion mass spectrometry, and atomic force microscopy, measurements. It is found that the Tm2Ti2O7 film annealed at 800 °C exhibited a thinner capacitance equivalent thickness of 19.8 Å, a lower interface trap density of 8.37 × 1011 eV−1 cm−2, and a smaller hysteresis voltage of ∼4 mV than the other conditions. We attribute this behavior to the Ti incorporated into the Tm2O3 film improving the interfacial layer and the surface roughness. This film also shows negligible degrees of charge trapping at high electric field stress.  相似文献   

18.
Y.J. Guo  X.T. Zu  B.Y. Wang  X.D. Jiang  X.D. Yuan  H.B. Lv  S.Z. Xu 《Optik》2009,120(18):1012-1015
Two-layer ZrO2/SiO2 and SiO2/ZrO2 films were deposited on K9 glass substrates by sol–gel dip coating method. X-ray photoelectron spectroscopy (XPS) technique was used to investigate the diffusion of ZrO2/SiO2 and SiO2/ZrO2 films. To explain the difference of diffusion between ZrO2/SiO2 and SiO2/ZrO2 films, porous ratio and surface morphology of monolayer SiO2 and ZrO2 films were analyzed by using ellipsometry and atomic force microscopy (AFM). We found that for the ZrO2/SiO2 films there was a diffusion layer with a certain thickness and the atomic concentrations of Si and Zr changed rapidly; for the SiO2/ZrO2 films, the atomic concentrations of Si and Zr changed relatively slowly, and the ZrO2 layer had diffused through the entire SiO2 layer. The difference of diffusion between ZrO2/SiO2 and SiO2/ZrO2 films was influenced by the microstructure of SiO2 and ZrO2.  相似文献   

19.
在SiO2玻璃衬底上用脉冲激光沉积(PLD)技术,分别沉积Ti和Ti/Al膜,经电化学阳极氧化成功制备了多孔TiO2/SiO2和TiO2/Al/SiO2纳米复合结构. 其中TiO2薄膜上的微孔阵列高度有序,分布均匀. 实验研究了Al过渡层对多孔TiO2薄膜光吸收特性的影响. 结果表明:无Al过渡层的多孔TiO2薄膜其紫外吸收峰在27  相似文献   

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