室温直流反应磁控溅射制备透明导电In_2O_3∶Mo薄膜

在室温条件下采用直流反应磁控溅射法制备了新型透明导电In2O3∶Mo薄膜。研究了溅射压强中氧气百分含量[P(O2)]为8.0%~18.0%时对薄膜光电特性以及表面形貌结构的影响。结果表明,薄膜的光电性能对溅射压强中P(O2)非常敏感。分析显示P(O2)决定了薄膜中的氧空位含量和载流子浓度,从而影响了薄膜的光电特性。原子力显微镜观察表明,适量的P(O2)条件下可以获得平均粗糙度为0.3 nm、颗粒均匀、表面平整的薄膜。室温制备的IMO薄膜在可见光区域的平均透射率(含玻璃基底)高达82.1%,电阻率低至5.9×10-4Ω.cm。     

直流反应磁控溅射法制备CdIn2O4薄膜的光电性能研究

利用直流反应磁控溅射法制备了CdIn2O4(CIO)薄膜,研究了氧浓度、基片温度、溅射时间和退火处理对薄膜光电性能的影响.结果表明电阻率随着氧浓度的增加和溅射时间的减小而增加,随着基片温度的升高先减小后增加;透光率随着氧浓度、基片温度的增加和溅射时间的减小而增加.退火处理后,薄膜的电阻率降低,光吸收边发生"蓝移".点缺陷对薄膜的光电性能产生重要影响,光吸收边的移动是"Burstein-Moss"效应和多体效应共同作用的结果.综合实验结果和理论研究,推荐了直流反应磁控溅射法制备CIO薄膜的最佳条件.此条件下制备薄膜的电阻率为2.95×10-4 Ω·cm,波长为628 nm时薄膜的透光率高达91.7%.     

MOCVD方法制备In2O3薄膜的性质研究

用金属有机化学气相淀积（MOCVD）方法以三甲基铟为源材料，以O2为氧化气体，在蓝宝石衬底（0001）面上生长出了高质量的立方相In2O3薄膜。研究了In2O3薄膜的结构、表面形貌和光电性质。结果表明制备样品具有In2O3体心立方结构和（222）方向择优取向生长，电阻率～6．40×10^-3Ω·cm，在可见光区域的平均透过率达到了90％以上。     

反应溅射氧分压对In2O3薄膜光电转换性能的影响

用直流磁控溅射在不同溅射功率下制备不同厚度的In2O3薄膜。通过XRD分析薄膜结构,用紫外可见光谱分析薄膜的光吸收能力,并推导薄膜的光学带隙。结果表明,室温反应溅射条件下,直接溅射得到的薄膜都是非晶薄膜,且吸光度随制备氧分压的增大而减小,相同功率下,薄膜厚度随氧分压增大而减小,光吸收起始位置也随之蓝移。相同偏压下,薄膜的单色光转换效率(IPCE)随氧分压增大先减小后增大。在0.5 mol/L Na2SO4溶液中,0.26 Pa氧分压得到的样品IPCE为14.8%(λ=400 nm)。在1.0 V Ag/AgCl偏压下,0.26 Pa氧分压样品光电流为28μA/cm2。     

Cu/Al_2O_3复合薄膜的制备及其抗氧化性能

本文在纺织纤维基材表面采用二次溅射沉积法制备了Cu/Al_2O_3复合薄膜,利用扫描电镜(SEM)、X射线能谱仪(EDX)和矢量网络分析仪对室温环境下存放3600h的复合薄膜的表面形貌、元素含量以及屏蔽效能进行了测试,并与相同工艺条件下制备的纯Cu薄膜进行了对比分析。结果表明:与纯Cu薄膜结构的不稳定性相比,由于复合薄膜表层Al_2O_3薄膜的结构稳定性和致密性,Cu/Al_2O_3复合薄膜在保证高屏蔽性能的前提下,具有整体结构的稳定性,表现出了良好的抗氧化性能。     

纳米In_2O_3的制备与结构表征

介绍了以同纯精铟为原料,采用化学沉淀法在一定的实验条件下制备纳米级In2O3粉体的实验过程,通过XRD、TEM、BET及化学分析等多种检测及分析手段对所制得的粉体的性能进行了初步表征,结果表明:采用化学沉淀法制备的In2O3为高纯单相类球形的黄色粉末,其平均粒径小于30nm。     

Mn掺杂Ga_2O_3薄膜的结构及光吸收性能研究

采用磁控溅射法在Si(111)和玻璃衬底上制备出不同Mn掺杂含量的Ga2O3薄膜,使用扫描电子显微镜、电子能谱仪、X射线衍射仪、紫外-可见分光光度计等对Mn掺杂Ga2O3薄膜的表面形貌、结晶特性和光吸收性能进行了研究.结果表明,适量掺杂Mn可抑制薄膜的晶格膨胀,促进Ga2O3薄膜晶粒的定向生长,得到尺寸分布较均匀的多面体晶粒.Mn掺杂使Ga2O3价带项向带隙延伸,光学带隙变窄,吸收边红移,近紫外区吸收增强.     

多晶Al2O3薄膜的制备及工艺研究

高能氩离子束溅射金属铝靶,沉积在SiO2基片上的非晶薄膜是Al和Al2O3的混合物.非晶薄膜在空气中800～1000℃退火后将完全氧化并晶化而成γ-Al2O3、oc-Al2O3.对溅射镀膜的工艺条件也进行了探索.     

Al掺杂ZnO薄膜的射频磁控溅射工艺与光电性能研究

用射频磁控溅射法制备Al掺杂ZnO(ZAO)薄膜,研究溅射与真空退火工艺对ZAO薄膜的显微结构及光电性能的影响.采用X射线衍射(XRD)对ZAO薄膜的显微结构进行了测试分析,用四探针测试仪、紫外-可见分光光度计对ZAO薄膜的光电性能进行了测试分析.结果表明:随溅射时间的增加,样品由非晶态向晶态转变,同时也出现(002)择优取向强弱的变化.退火提高了溅射时间较长的薄膜的结晶质量.溅射时间的增加使溅射态ZAO薄膜的光学带隙变窄,但退火处理则使光学禁带宽度增大.溅射时间的增加以及退火处理均使薄膜的透光率稍有下降,但所有ZAO薄膜的透光率均在90%.以上.薄膜的电阻率随溅射时间的增加先降低.后稍有回升.退火使薄膜的电阻率显著降低,当溅射时间为60min时退火后薄膜的电阻率达到最低值,为9.4 ×10-4Ω·cm,其方块电阻低至18.80Ωl/□.     

氧控In2O3薄膜的光电性能

对比在控氧条件下制备态和退火态In₂O₃薄膜的微观结构和光电性能,分析两种状态中不同的氧作用机制。两种控氧行为都能够有效提高In₂O₃薄膜的晶格有序度和降低氧空位浓度,使其载流子浓度下降、迁移率提高和光学带隙变窄;等离子体制备过程中氧以高活性非平衡方式注入晶格,而退火时氧以低活性平衡态扩散的方式进入晶格;不同的氧作用机制使得退火态薄膜比制备态薄膜具有更少的结构缺陷、更高的氧空位浓度和更佳的透光导电性。     

磁控溅射CrNx薄膜的制备与力学性能

采用反应磁控溅射法在不同的氮分压下制备了一系列CrNx薄膜，并利用EDS和XRD表征了薄膜的成分和相组成，采用力学探针测量了薄膜的硬度和弹性模量。研究了氮分压对薄膜成分，相组成和力学性能的影响。结果表明，随氮分压的升高，薄膜的沉积速率明显降低，薄膜中的氮含量量增加，相应地，相组成从Cr Cr2N过渡到单相Cr2N,再逐步经Cr2N CrN过渡到单相CrN,并在Cr:N原子比为1：2和1：1时，薄膜的硬度出现极值（HV27．1GPa和HV26.8GPa),而薄膜的弹性模量则在Cr2N时呈现350GPa的最高值。     

高度(002)择优取向Li+掺杂ZnO薄膜的制备和性能

制备了不同摩尔浓度Li 掺杂ZnO-Li0.022陶瓷靶、并用RF射频磁控溅射工艺在Si(100)基片上制备ZnO薄膜,研究了溅射温度、氧分压和溅射功率等对ZnO薄膜微结构、表面形貌和择优取向的影响.结果表明:Li 的最佳掺杂量(摩尔分数)为2.2%,RF溅射的最佳基片温度Ts小于300 ℃,氩氧气氛体积比为Ar:O2=20:5,溅射功率50～60 W;制备出的ZnO薄膜高度c轴(002)择优取向、均匀、致密,其绝缘电阻率ρ为4.12×108 Ω·cm,满足研制声表面波器件(SAW)的要求.     

Surface morphology and optical properties of magnetron - sputtered ultrathin Al films

Ultrathin Al films with different thicknesses were deposited on glass substrates by DC magnetron sputtering. The effects of film thickness on morphology and optical properties of the films were investigated in detail. When film thickness increases from 7.0 to 84.0 nm, the average grain size and surface roughness enlarges from 27.6 to 94.2 nm and from 0.25 to 1.87 nm, respectively. Below critical thickness of 28.0 nm, which is the thickness that Al films form continuous film, the optical properties vary significantly with thickness increasing and then tend to be stable. In the absorptance spectra, all films exhibit distinct broad peaks which can be attributed to the absorption due to the interband transition. The possible reasons for the shift in the peak position are due to the quantum size effects and internal stress in the ultrathin Al films.     

金属Ag微网格修饰ITO薄膜的制备及光电性能

利用聚苯乙烯(PS)微球模板技术和直流磁控溅射技术在ITO(In2O3∶Sn)薄膜表面进行Ag的微网格修饰,得到具有良好周期性的表面结构。研究了PS微球直径和直流磁控溅射Ag时间对ITO薄膜表面形貌、可见光区透过率、漫反射率和导电性能的影响。实验及分析证明,对ITO表面进行Ag微网格修饰,当微球直径为2μm,溅射时间为30s时,最大可提高薄膜的导电性能19.5%,其漫反射性能可提高200%,同时在可见光区透过率的降低控制在10%以下,这将有助于提高ITO薄膜作为太阳能电池透明电极的陷光性能。     

磁控溅射制备ITO薄膜光电性能的研究

采用直流磁控溅射方法在玻璃基底上制备了ITO薄膜.分别用分光光度计和四探针仪测试了所制备ITO薄膜在可见光区域内的透过率和电阻率,研究了溅射气压、氧氩流量比和溅射功率三个工艺参数对ITO薄膜光电性能的影响.研究结果表明,制备ITO薄膜的最佳工艺参数为:溅射气压0.6 Pa,氧氩流量比1:40,溅射功率108 W.采用此工艺参数制备的ITO薄膜在可见光区平均透过率为81.18％,薄膜电阻率为8.9197×10-3Ω·cm.     

Effect of aluminum and indium co-doping on zinc oxide films prepared by dc magnetron sputtering

Aluminum and indium co-doped zinc oxide (AIZO) thin films were prepared by direct current (dc) magnetron sputtering on glass substrate in pure argon atmosphere. Three inches of zinc oxide ceramic with 0.5 wt.% of aluminum and indium doping was used as a target in static mode. The influence of sputtering conditions i.e. substrate-target distance, pressure and power on AIZO films was studied. The electrical resistivity and microstructure of thin films were investigated by the four point probe technique and the scanning electron microscope, respectively. The optical transmittance of AIZO films was measured by UV visible spectrophotometer in the wavelength of 300-1100 nm. Depending on the deposited conditions, highly transparent films up to 80% with low resistivities in the range of 2.6-7.9 × 10^− 4 Ω cm were achieved at room temperature. Possible mechanism in the processing which, ultimately, determines the physical properties of AIZO films will be discussed.     

Polycrystalline films of tungsten-doped indium oxide prepared by d.c. magnetron sputtering

Electrical and optical properties of polycrystalline films of W-doped indium oxide (IWO) were investigated. These films were deposited on glass substrate at 300 °C by d.c. magnetron sputtering using ceramic targets. The W-doping in the sputter-deposited indium oxide film effectively increased the carrier density and the mobility and decreased the resistivity. A minimum resistivity of 1.8 × 10^− 4 Ω cm was obtained at 3.3 at.% W-doping using the In₂O₃ ceramic targets containing 7.0 wt.% WO₃. The 2.2 at.% W-doped films obtained from the targets containing 5.0 wt.% WO₃, showed the high Hall mobility of 73 cm² V^− 1 s^− 1 and relatively low carrier density of 2.9 × 10²⁰ cm^− 3. Such properties resulted in novel characteristics of both low resistivity (3.0 × 10^− 4 Ω cm) and high transmittance in the near-infrared region.     

氨化Si基Ga2O3/In2O3制备GaN薄膜

研究了Ga2O3/In2O3 膜反应自组装制备GaN薄膜,再将Ga2O3/In2O3膜在高纯氨气气氛中氨化反应得到GaN薄膜,用X射线衍射 (XRD),傅里叶红外吸收(FTIR),扫描电镜(SEM)和透射电镜(TEM)对样品进行结构、形貌的分析.测试结果表明,用此方法得到了六方纤锌矿结构的GaN多晶膜,且900℃时成膜的质量最好.     

HfO2薄膜的制备与光学性能

采用射频磁控反应溅射法，以高纯热压HfO2陶瓷为靶材，在Si衬底上成功制备出HfO2薄膜。系统研究了工艺参数对薄膜沉积速率的影响规律，并对薄膜的光学性能进行了研究。结果表明，射频功率对薄膜沉积速率的影响最为明显，O2／Ar流量比和衬底温度对沉积速率的作用不明显，所制备薄膜的折射率较高在近红外波段趋于1．95，在500-1650nm波段范围内薄膜几乎无吸收，透过率较高。     

On the structural and electrical characteristics of zinc oxide thin films

ZnO thin films with thickness d = 100 nm were deposited by radio frequency magnetron sputtering onto glass substrate from different targets. The structural analyses of the films indicate they are polycrystalline and have a wurtzite (hexagonal) structure. Crystallites are preferentially oriented with (002) plane parallel to the substrate surface and the samples have low values for surface roughness, between 1.7 nm and 2.7 nm. The mechanism of electrical conduction in the studied films is strongly influenced by this polycrystalline structure and we used Van der Pauw method to analyze these properties. Electrical studies indicate that the ZnO thin films are n-type. For the cooling process, thermal activation energy of electrical conduction of the samples can vary from 1.22 eV to 1.07 eV (for the ZnO layer obtained from for metallic Zn target) and from 0.90 eV to 0.63 eV (for the ZnO layer obtained from ZnO target), respectively. The influence of deposition arrangement and oxidation conditions on the structural and electrical properties of the ZnO films was investigated in detail.