脉冲激光沉积法制备钛酸锶钡薄膜及其光电性质

用脉冲激光沉积技术制备了钛酸锶钡(Ba0.5Sr0.6TiO3薄膜.用X射线光电子能谱和原子力显微镜分别分析了薄膜的化学组分和表面形貌.在交流信号为50 mV和100 kHz时测量了薄膜的介电系数和介电损耗随外加电场的变化关系,得出最高的介电可调率达到45%.利用单光束纵向Z扫描的方法研究了薄膜的非线性光学性质,得到非线性折射率为5.04×10-6cm2/kW,非线性吸收系数为3.59×10-6m/W,测量所用光源的波长为532 nm,脉宽为55 ps,表明Ba0.5Sr0.5TiO3薄膜有较快的非线性光学响应.     

Compositional and Structural Properties of TiO2-xNx Thin Films Deposited by Radio-Frequency Magnetron Sputtering

TiO2-xNx thin films are deposited onto Si（100） and quartz substrates by arf magnetron sputtering method using a titanium metal disc as a target in Ar, N2, and 02 atmospheres. The substrate temperature is kept at 300℃. The O2 and Ar gas flow rates are kept to be constants and the N gas flow rate is varied. TiO2-xNx films with different N contents are characterized by x-ray diffraction and x-ray photoelectron spectroscopy. The results indicate that the TiO2-xNx thin films can be obtained at 13% N and 15% N contents in the film, and the films with mixed TiO2 and TiN crystal can be obtained at 13% N and 15% N contents in the film. In terms of the results of x-ray photoelectron spectroscopy, N ls of β-N （396 eV） is the main component in the TiO2-xNx thin films. Because the energy level of β-N is positioned above the valence-band maximum of TiO2, an effective optical-energy gap decreases from 2.8 eV （for pure TiO2 film deposited by the same rf sputtering system） to 2.3 eV, which is verified by the optical-absorption spectra.     

直流磁控溅射氮化铁薄膜生长的动力学标度

利用直流磁控溅射方法,以Ar/N2作为放电气体,通过改变放电气体中N2的流量(N2流量比分别为5%,10%,30%,50%)及溅射时间(160,30,20,10,5min),在玻璃衬底上沉积了FexN薄膜。用X射线光电子能谱(XPS)方法确定了不同N2流量下薄膜的成分;X射线衍射(XRD)方法分析了不同N2流量下的FexN薄膜结构,当N2流量比为5%时获得了FeN0 056相,10%时为ε Fe3N相,30%和50%流量比下均得到FeN相。利用原子力显微镜(AFM)和掠入射X射线散射(GIXA)方法研究了膜表面的粗糙度和形貌,发现随着N2流量的增加,薄膜表面光滑度增加,薄膜表面呈现自仿射性质。动力学标度方法定量分析表明:薄膜表面因不同N2流量的影响而具有不同的动力学指数,当氮气流量比为5%时,静态标度指数α≈0 65,生长指数β≈0 53±0 02,薄膜生长符合基于Kolmogorov提出的能量波动概念的KPZ模型指数规律。     

磁控反应溅射SiNx薄膜的研究

用磁控反应溅射(RF)的方法制备了SiN_x薄膜. 分析了以硅为靶材, 用N₂/Ar做溅射气体条件下不同的气流比率、总气压以及沉积速率对薄膜光学常数和表面结构形态的影响, 得出较低总气压下气流比率对薄膜光学常数的影响是最关键的, 而总气压较大的时候, 水汽影响增大, 气流比率的影响反而不明显. 最后提出了合适的工艺条件来制备符合要求的SiN_x薄膜.     

Fabrication and Thickness Measurment of the Thin Films Deposited by Planar Magnetron Sputtering

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磁控溅射技术制备TiO2薄膜的研究进展

介绍了磁控溅射法镀膜的基本原理,综述了近年来关于溅射功率、工作压强、氩氧比例、沉积温度和退火等工艺参数以及掺杂对T iO2薄膜结构、形貌和光学性质影响的研究进展,并对磁控溅射技术制备T iO2薄膜的发展方向进行了展望。     

Structural Properties of Thin Films Obtained by Magnetron Sputtering of Polydiacetylene

Physics of the Solid State - Films obtained by radio-frequency sputtering of monocrystalline polydiacetylene (PDA) are under study. The structure is studied by Raman spectroscopy, transmission...     

中频孪生磁控溅射WO3薄膜及变色性能研究

采用先进的中频孪生非平衡磁控溅射技术,以金属钨为靶材,制备非晶态WO3电致变色薄膜。用X射线衍射(XRD)、X射线光电子能谱(XPS)、紫外分光光度计等测试手段分析薄膜的结构、表面形貌、成分以及透射光谱特性。研究了氧气流量比及热处理温度对WO3薄膜变色性能的影响。结果表明,中频孪生非平衡磁控溅射技术是制备WO3变色薄膜的一种有效方法;室温条件下沉积获得的原始态薄膜为非晶态WO3;提高氧气流量比和适当热处理温度能有效改善薄膜的电致变色性能。实验中在较高氧气流量比,200℃热处理条件下制备的薄膜在380~780 nm的可见光范围内着色态和褪色态平均透光率差值高达50%以上,表现出较好的电致变色性能。     

High Ferroelectricities and High Curie Temperature of BiInO3PbTiO3Thin Films Deposited by RF Magnetron Sputtering Method

Properties of ferroelectric xBiInO_3-(1-x)PbTiO_3(xBI-(1-x)PT) thin films deposited on(101) SrRuO_3/(200)Pt/(200) MgO substrates by rf magnetron sputtering method and effects of deposition conditions are investigated.The structures of the xBI-(1-x)PT films are characterized by x-ray diffraction and scanning electron microscopy.The results indicate that the thin films are grown with mainly(001) orientation. The chemical compositions of the films are analyzed by scanning electron probe and the results indicate that the loss phenomena of Pb and Bi elements depend on the pressure and temperature during the sputtering process.The sputtering parameters including target composition, substrate temperature, and gas pressure are adjusted to obtain optimum sputtering conditions. To decrease leakage currents,2 mol% La_2 O_3 is doped in the targets. The P-E hysteresis loops show that the optimized xBI-(1-x)PT(x = 0.24) film has high ferroelectricities with remnant polarization2 P_r = 80μC/cm~2 and coercive electric field 2 E_C = 300 kV/cm. The Curie temperature is about 640℃. The results show that the films have optimum performance and will have wide applications.     

Structural and Electric Characteristics of Two-Layer Bi4Ti3O12/(Ba,Sr)TiO3 Thin Films Deposited on a Silicon Substrate by Radio-Frequency Sputtering at Increased Oxygen Pressures

Physics of the Solid State - The 400–450-nm-thick Bi4Ti3O12 thin films with various orientations of crystallites with respect to a normal to the (100)Si substrate plane have been studied. It...     

化学浴沉积法制备CdS多晶薄膜

利用化学浴沉积法制备适合于铜铟镓硒薄膜太阳能电池缓冲层材料的CdS多晶薄膜,研究了在不同温度和不同时间下沉积薄膜的性质．薄膜生长开始由ion-by-ion机制控制,随着时间的进行,cluster-by-cluster机制占据主导．薄膜的生长速度随着沉积温度的升高而快速增加,直到达到饱和厚度．并且饱和厚度随温度升高而相应降低．SEM表明随沉积时间增加以及温度升高,薄膜表面形貌从多孔到粗糙的不均匀转变．XRD结果显示,薄膜由立方和六方两相结构组成,控制沉积时间对薄膜的主要晶相结构很关键．所有温度下沉积的CdS     

Optical-Energy Properties of CdS Thin Films Obtained by the Method of High-Frequency Magnetron Sputtering

Optics and Spectroscopy - The results of experimental and theoretical studies of the optical-energy properties of CdS thin films are reported. The synthesis procedure and the results of structural...     

磁控溅射制备铬薄膜的结构和光电学性质

用直流磁控溅射技术在石英基片上制备不同厚度(5 nm~114 nm之间)的铬膜.使用X射线衍射仪和分光光度计分别检测薄膜的结构和光学性质,利用德鲁特模型和薄膜的透射、反射光谱计算铬膜的厚度和光学常量,并采用Van der Pauw方法测量薄膜电学性质.结果表明:制备的铬薄膜为体心立方的多晶态,随着膜厚的增加,薄膜的结晶性能提高,晶粒尺寸增大;在可见光区域,当膜厚小于32 nm时,随着膜厚的增加,折射率快速减小,消光系数快速增大,当膜厚大于32 nm时,折射率和消光系数均缓慢减小并逐渐趋于稳定;薄膜电阻率随膜厚的增加为一次指数衰减.     

磁控溅射制备铬薄膜的结构和光电学性质(英文)

用直流磁控溅射技术在石英基片上制备不同厚度(5nm～114nm之间)的铬膜.使用X射线衍射仪和分光光度计分别检测薄膜的结构和光学性质,利用德鲁特模型和薄膜的透射、反射光谱计算铬膜的厚度和光学常量,并采用Van der Pauw方法测量薄膜电学性质.结果表明:制备的铬薄膜为体心立方的多晶态,随着膜厚的增加,薄膜的结晶性能提高,晶粒尺寸增大;在可见光区域,当膜厚小于32nm时,随着膜厚的增加,折射率快速减小,消光系数快速增大,当膜厚大于32nm时,折射率和消光系数均缓慢减小并逐渐趋于稳定;薄膜电阻率随膜厚的增加为一次指数衰减.     

RF溅射钕掺杂ZnO薄膜的结构与发光特性

通过射频磁控溅射技术在Si(111)衬底上制备了未掺杂ZnO薄膜和Nd掺杂ZnO薄膜。应用XRD分析了ZnO:Nd薄膜的晶格结构,通过AFM观察了ZnO:Nd薄膜的表面形貌。结果表明,Nd掺入了ZnO晶格中,由于Nd原子半径大于Zn原子半径,Nd以替位原子的形式存在于ZnO晶格中。ZnO:Nd薄膜为纳米多晶薄膜,表面形貌粗糙。ZnO:Nd薄膜的室温光致发光谱表明,相同条件下制备的未掺杂ZnO薄膜和Nd掺杂ZnO薄膜都出现了395nm的强紫光带和495nm的弱绿光带。我们认为,紫光发射峰窄而锐且强度远大于绿光峰,源于薄膜中激子复合;绿光峰强度较弱,源于薄膜中的氧空位(VO)及氧反位锌缺陷(OZn)。Nd掺杂没有影响ZnO:Nd薄膜的PL谱的发射峰的峰位。由于Nd3 离子电荷数与Zn2 离子电荷数不相等,为了保持ZnO薄膜的电中性,间隙锌(VZn)可以作为Nd替位补偿性的受主杂质而存在,影响ZnO薄膜的激子浓度。同时,Nd掺入使ZnO的晶格畸变缺陷浓度改变增强,因而发射峰的强度随Nd掺杂浓度不同而变化。     

射频磁控溅射ZnO薄膜的结构和光学特性

采用射频（RF）反应磁控溅射法在n-Si(001)衬底上外延生长ZnO薄膜。XRD谱测量显示出较强的（002）衍射峰，表明ZnO薄膜为c轴择优取向生长的。室温PL谱测量观察到了较强的紫外光发射和深能级发射。     

射频磁控溅射法制备的Eu掺杂ZnO薄膜的结构及其发光性质

用射频磁控溅射法在石英衬底上制备了ZnO:Eu3+薄膜,通过X射线衍射仪、扫描电子显微镜和荧光光谱仪测试了薄膜结构、形貌以及发光性能,重点考察了溅射功率和退火工艺对其组织结构和发光性能的影响.结果表明:样品均呈现ZnO的六角纤锌矿结构,增大溅射功率有利于形成ZnO的c轴择优取向;增大溅射功率以及高温退火会使晶粒尺寸增大...     

The Influence of Au-Doping on Morphology and Visible-Light Reflectivity of TiN Thin Films Deposited by Direct-Current Reactive Magnetron Sputtering

Ti, TiN and Au-TiN （Au content： from 0.5%to 7.7%） thin films were deposited on stainless steel substrates by dc reactive magnetron sputtering with a metal Ti target. The crystal structure, surface morphology and visiblelight reflectivity of the films for different film compositions are studied in detail. Distinctly different surface morphologies appear for the Ti, TiN and Au-TiN thin films. It can be observed that the surface morphology of the TiN film is affected by the Au-doping, when the Au content increases from 0% to 7.7%, surface roughness enlarges from 62.4 to 82.8 nm. Moreover, visible-light reflectivity varies significantly with increasing A u contents in the TiN films. However, the rettectivity of the TiN thin film at 550-800 nm is higher than that of the Au-TiN thin film. The present work illustrates the dependence of metal elements on the surface morphology and on the reflectivity of Au-TiN thin films. It is speculated that the addition of Au can suppress the formation and growth of TiN grains so that it changes the surface morphology and the Au-TiN thin film has potential applications in spectral selective coating.