PZT/Si薄膜的扩散反应研究

运用XPS和AES研究了PZT薄膜／Si在热处理过程中的薄膜及界面化学反应：在热处理过程中，气氛中的氧气通过PZT的缺陷通道扩散到PZT／Si界面上，并与界面上的硅发生氧化反应形成SiO2界面层。同时基底上的硅通过PZT的缺陷扩散到样品表面形成SiO2表面层。此外，在PZT／Si界面上，Ti的氧化物和Si发生还原反应，形成了TISix金属硅化物，并残留在PZT膜层和SiO2界面层中。在PZT膜层内，有机结碳和钛的氧化物发生还原反应形成了TiCx物种，并存在于PZT膜层中。     

PZT／Si界面氧化反应机理及动力学研究

运用俄歇电子能谱深度剖析和线形分析研究了ＰＺＴ／Ｓｉ界面氧化反应的机理和动力学过程，研究结果表明，在ＰＴ／Ｓｉ样品的热处理过程中，环境气氛中的氧可以透过ＰＺＴ薄膜层扩散到ＰＴ／Ｓｉ界面，并与硅基底反庆形成ＳｉＯ２界面层，界面氧化反应由氧在ＰＴ层和ＳｉＯ２层中的扩散过程所控制。     

Pt扩散阻挡层对PZT/Si薄膜化学结构和性能的影响

运用XPS和AES研究了Pt扩散阻挡层对PZT薄膜／Si界面化学结构和性能的影响：在PZT薄膜和Si基底间增加Pt扩散阻挡层，可以抑制TiCx物种和TiSix物种的形成，促进PZT薄膜的形成反应。Pt扩散阻挡层的存在阻断了氧和Si的相互扩散反应，促进PZT物种形成钙钛矿型晶体结构，使得形成的PZT薄膜具有和体相材料相近的高介电常数和铁电性能。     

Cr/SiO_2界面还原反应研究

利用俄歇电子能谱研究了Cr／SiO2薄膜在热处理过程中的界面扩散反应机理、界面反应动力学过程及界面反应产物。研究结果表明，Cr／SiO2体系的界面还原反应主要是Cr与SiO2的反应，其还原反应产物是CrSix和Cr2O3物种。界面还原反应的速度与反应时间的平方根成正比，其界面还原反应过程受Cr向SiO2层的扩散过程所控制，界面还原反应的表观活化能为72．5kJ／mol（约0．75eV）。     

Ti/Si(100)体系界面扩散反应动力学研究

采用移动边界条件下扩散问题的处理方法，综合界面反应和扩散两个过程对界面硅化物形成的影响，建立起Ti／Si（100）界面扩散反应动力学理论模型，并拟合快速热退火处理后试样界面Auger深度分析谱，得到Ti，Si在相应界质中扩散系数和表现反应活化能。研究结果表明，Ti／Si体系界面TiSi2生成经历了一个由反应动力学控制到扩散控制的过渡。Si从其晶格中解离并扩散到Ti／TiSi2界面是制约扩散过程的关键因素。     

PZT／Si薄膜的扩散反应研究

运用ＸＰＳ和ＡＥＳ研究了ＰＺＴ膜／Ｓｉ在热处理过程中的薄膜及界面化学反应；在热处理过程中，气氛中的气通过ＰＺＴ的缺陷通道扩散到ＰＺＴ／Ｓｉ同旧，并与界面上的硅发生氧化反应形成ＳｉＯ２界面层。同时基底上的硅通过ＰＺＴ的缺陷扩散么样品表面形成ＳｉＯ２表面层。此外，在ＰＺＴ／Ｓｉ界面上，Ｔｉ的氧化物和Ｓｉ发生还原反应，形成了ＴｉＳｉｘ金属硅化物，并残留在ＰＺＴ膜层和和ＳｉＯ２界面层中。在ＰＺＴ膜层内，有     

钼网表面MoSi2涂层的制备及其1500℃高温氧化性能

钼网被广泛用作高温催化剂载体,但关于其高温防护涂层的制备及失效机制却鲜有报道.用包埋渗硅方法在钼网表面制备了MoSi2高温抗氧化涂层,并在静态大气环境中开展了1500℃恒温氧化试验.利用X射线衍射仪(XRD)、扫描电镜(SEM)、能谱分析(EDS)等对氧化前后涂层的微观形貌和组织结构进行了表征.结果表明:1500℃氧化2h,MoSi2涂层中的Si元素会发生选择性氧化,在涂层表面形成一层连续的、具有“自愈合”功能的熔融态SiO2保护膜,阻挡氧向基体一侧的扩散,展现出了良好的高温抗氧化性能;高温条件下,涂层中的Si元素会和钼基体发生界面扩散反应生成抗氧化性能差的Mo5Si3,同时MoSi2不断地和氧发生反应生成Mo5Si3和SiO2,当涂层中的MoSi2完全转化为Mo5Si3,涂层将快速氧化失效.     

Ti/SiO_2界面反应的研究

运用俄歇深度剖析和俄歇化学效应研究了Ti／SiO2的界面还原反应。结果表明，在薄膜样品的制备过程中，金属Ti可以和SiO2发生界面还原反应，形成TiSi和TiO2物种。薄膜样品在RTA处理时，Ti和SiO2的界面反应大幅度地增加，尤其是当RTA温度高于700℃时，界面反应增加得更快。700℃温度可能是Ti和SiO2界面反应的活化温度。随着反应时间的增加，界面反应也相应增加。当Ti层的厚度增加时，也有利于Ti和SiO2的界面反应。     

Si3N4陶瓷/Nb/Cu/Ni/Inconel 600界面反应层形成机制研究

观察分析了Si3N4陶瓷/Nb/Cu/Ni/Inconel600界面处反应层的形貌、元素分布、反应层中的相结构、界面反应以及反应层的生长规律,研究了Si3N4陶瓷/Nb/Cu/Ni/Inconel600界面处反应层的形成机制.研究结果表明:在连接过程中,Cu层首先熔化,Nb、Ni向液态Cu中扩散溶解形成Cu-Nb-Ni合金,液态合金中的Nb和Ni向Si3N4表面扩散聚集并与Si3N4反应形成反应层;Si3N4侧的反应层主要物相是NbN和Nb、Ni的硅化物,Ni基合金侧反应相主要是NbNi3和Cu-Ni合金;在连接温度为1403 K的条件下,随着连接时间的增加,界面反应层厚度先快速增加,再缓慢增加.     

溅射PZT薄膜的晶体结构和快速热处理

采用常温射频（RF）溅射法和快速热处理相结合的技术，在Pt／Ti／SiO2／Si衬底上，制备出具有铁电性的PZT薄膜。研究了快速热处理工艺条件对PZT薄膜性能的影响。通过X射线衍射法、SEM和AES等方法，分析了PZT薄膜的晶体结构、微结构、薄膜和电极间的界面效应。     

Graphene growth at the interface between Ni catalyst layer and SiO2/Si substrate

Graphene was synthesized deliberately at the interface between Ni film and SiO2/Si substrate as well as on top surface of Ni film using chemical vapor deposition (CVD) which is suitable for large-scale and low-cost synthesis of graphene. The carbon atom injected at the top surface of Ni film can penetrate and reach to the Ni/SiO2 interface for the formation of graphene. Once we have the graphene in between Ni film and SiO2/Si substrate, the substrate spontaneously provides insulating SiO2 layer and we may easily get graphene/SiO2/Si structure simply by discarding Ni film. This growth of graphene at the interface can exclude graphene transfer step for electronic application. Raman spectroscopy and optical microscopy show that graphene was successfully synthesized at the back of Ni film and the coverage of graphene varies with temperature and time of synthesis. The coverage of graphene at the interface depends on the amount of carbon atoms diffused into the back of Ni film.     

ITO用作铁电薄膜电极的研究

研究了sol-gel掺锡氧化铟（ITO溶胶在SiO2/Si衬底和光学玻璃衬底上的成膜及结晶性能,并与CVD法生长的ITO薄膜作了对比。结论是：sol-gelITO膜,虽然具有与CVD ITO膜相似的结晶性能和较高的导电性,但以sol-gel ITO膜作下电极,无法使PLT、PZT的sol-gel膜具有明显的结晶取向。因漏电太大,sol-gel ITO也无法作sol-gel铁电膜（如PLT,PZT）的上电极。但在CVD ITO膜上,sol-gel铁电膜能很好结晶,且Au/PLT/ITO电容,具有良好的电学性能。     

Magnesium metallic interlayer as an oxygen-diffusion-barrier between high-κ dielectric thin films and silicon substrate

The deposition of a thin magnesium metallic interlayer on an Si substrate prior to the deposition of an oxide thin film using rf-sputtering was investigated. The deposition of high-κ HfO₂ thin film was more particularly studied and it was demonstrated that the metallic interlayer acts as an oxygen barrier, preventing the formation of a low-κ layer at the high-κ/Si interface during the deposition. A post-deposition annealing treatment performed on the films induced the diffusion of the metal barrier into the HfO₂ film and allowed obtaining a sharp interface. However, the degree of diffusion depends not only on the interlayer thickness, but also on the thickness of the high-κ film. X-ray photoelectron spectroscopy was used to study the degree of oxidation of the Mg interlayer. High resolution transmission electron microscopy and energy filtered transmission electron microscopy were used to characterize the films and the diffusion of the Mg interlayer into the high-κ film after annealing. In this work we will stress on the engineering of the interface via the diffusion of the Mg interlayer during the growth process and on annealing.     

SiO_2层对金刚石膜初期生长影响的研究

用俄歇子能谱（AES）研究了热丝法生长金刚石膜中未经划痕处理的单晶硅衬底在不同沉积时间下的表面结构及Si，C，O元素浓度的深度分布。结果表明：在沉积过程中，随沉积时间增加时，基材表面C浓度增加，O浓度下降，但SiC过渡层的生长缓慢。700℃沉积4h时仍无结构完整的SiC层生成，这是表面SiO2层阻碍了SiC的形成。分析了不经划痕处理的基材形核率低的原因。用高分辨电镜（HREM）观察了生长良好的金刚石膜的膜—基界面，发现没有SiO2层存在。     

Lead zirconate titanate thin films on GaAs substrates

Thin films of the piezoceramic lead zirconate titanate (PZT) of composition Pb(Zr0.53Ti0.47)O3 have been prepared on a platinized GaAs substrate system using a propanediol based sol-gel technique. A Si3N4 buffer layer was deposited onto the GaAs by plasma-enhanced chemical vapour deposition so as to minimize Ga and As diffusion during film fabrication. Rapid thermal processing (RTP) techniques were used to thermally decompose the sol-gel layer to PZT in a further effort to avoid problems of Ga and As diffusion. Adhesion between the electrode and substrate was found to improve when an intermediate Ti layer deposited between the Pt and Si3N4 was oxidized prior to depositing the Pt layer. A crystalline PZT film was produced on the Pt/TiO2/Si3N4/GaAs by firing the sol-gel coating at 350°C for 1 min and then at 650°C for 10 s using RTP. A single deposition of precursor sol resulted in a film 0.5 μm thick. Measured average values of remanant polarization and coercive field were 14 μC cm-2 and 47 kV cm-1, respectively. The polarization value is rather low, as conventionally fired films on silicon have remanent polarization values of 20–30 μC cm-2; the lower values may be due to incomplete crystallization during RTP, but a degradation of properties due to Ga-As diffusion, despite the precautions, cannot be ruled out at this stage. This revised version was published online in November 2006 with corrections to the Cover Date.     

Characteristics of SiO2/Si3N4/SiO2 stacked-gate dielectrics obtained via atomic-layer deposition

An interpoly-stacked dielectric film with a SiO2/Si3N4/SiO2/Si (ONO) structure was prepared via the atomic-layer deposition method. The multilayer structure of the ONO film with triple interfaces was investigated via medium-energy ion scattering (MEIS). A few defects in the interface layer of the ONO structure were detected. From the X-ray photoelectron spectroscopy (XPS) results, it was presumed that the interface layer with defects in the MEIS result is due to the formation of an oxynitride layer on the unstable and rougher Si3N4 layer via. By measuring the I-V characteristics, the leakage current density and breakdown field of the ONO film were determined to be 3.4 x 10(-9) A/cm2 and 10.86 MV/cm, respectively. By estimation the C-V curve, the flat band (V(FB)) of the ONO film shifted to a negative voltage (-1.14 V), the dielectric constant (K(ONO)) of the ONO film was 5.79, and the effective interface-trapped charge density of the ONO film was about 4.96 x 10(11)/cm2.     

Interfacial layer growth of ZrO2 films on silicon

In this work, the interfacial layer growth for both as-deposited and annealed ZrO₂ thin films on silicon is analyzed in detail by the high-resolution cross-sectional transmission electron microscope and spectroscopic ellipsometry. For as-deposited ZrO₂/SiO₂/Si, the thickness of a SiO₂-like layer at the silicon interface was found to depend on the oxygen partial pressure during deposition. At oxygen partial pressure ratio of above 50% the interfacial silicon oxide thickness increased through oxygen diffusion through the ZrO₂ film and silicon consumption at the interface. At oxygen partial pressure ratio in the range 7-50%, the visible growth of interfacial silicon oxide layer was not present. The interfacial layer for ZrO₂/Si with optimal partial pressure (15%) during annealing at 600 °C was found to be the two-layer structure composed of the ZrSi_xO_y overlayer and the SiO_x downlayer. The formation of the interfacial layer is well accounted for diffusion mechanisms involving Si indiffusion and grain-boundary diffusion.