氩气对直流弧光放电PCVD金刚石薄膜晶体特征的影响

本文采用自主研制的直流弧光放电等离子体CVD设备,在YG6硬质合金基体上进行了不同氩气流量下金刚石薄膜的制备研究.采用SEM对金刚石薄膜的晶体特征进行了观察.结果表明,氩气对直流弧光放电等离子体CVD金刚石薄膜的晶体特征有明显影响.在CH_4/H_2恒定时(0.8;),硬质合金基体上制备的金刚石薄膜表面形貌随Ar流量增加而变化的规律,即从以(111)八面体晶面为主→(111)和(100)立方八面体混杂晶面→以(100)立方体晶面为主→菜花状的顺序转变;当Ar流量为420～700 mL/min时,金刚石晶粒的平均尺寸由1.5 μm 逐步增大到7 μm;Ar流量为700～910 mL/min时,金刚石晶粒的平均尺寸由7 μm急剧减小到纳米尺度,约50 nm.     

Ion bombardment effect on the growth of a-Si:H films deposited from a pure silane plasma

The growth process, optical and structural properties of a-Si:H films deposited from a pure silane multipole DC discharge are analysed by real time and spectroscopic ellipsometry and I.R. absorption spectroscopy. The relative Si flux going onto the substrate under a ionized form can vary from 20% to 80%. In each extreme case the film properties are correlated with ion bombardment energy up to 300 eV. An increase of incident ion energy is found to favour the formation of high density homogeneous and isotropic films correlated with the predominance of monohydride SiH groups.     

Study of hyperfine interactions in Fe–Co nanocomposite films by Mössbauer spectroscopy and NMR

Nanogranular magnetic films were produced by the specially designed UHV plasma-jet system with DC hollow-cathode discharge. We investigated the properties of these ferromagnetic FeCo-AlN films. The samples were studied by nuclear magnetic resonance, Mössbauer spectroscopy, and transmission electron microscopy. The films are composed of nanoparticles of cubic FeCo, 2–10 nm in size, embedded in amorphous matrix containing Al, N and O. The Mössbauer spectra indicate that the orientation of local magnetic moments on the surface is random for the sample with 1:1 Fe/Co ratio, while the magnetization lays in the plane of the layer for samples with Fe/Co smaller than 1 (0.91–0.95).     

Deposition and properties of a-Si:H by cylindrical diode glow discharge

The effect of plasma parameter on the properties of a-Si:H films prepared by glow discharge process in cylindrical diode system has been studied. The glow discharge plasma is examined by measurements of the emission spectra for H, H₂, SiH and Si radicals, the mass spectra for primary decomposed and secondary polymerized ions, and the rf discharge impedance. The plasma reactions are dominated by the rf electric potential V_p and silane gas pressure p. The nucleation of SiH₂ bonding depends critically on the electron and ion bombardments and the plasma polymerization.     

直流磁控溅射陶瓷靶制备ITO薄膜及性能研究

以10%质量分数SnO2和90%质量分数In2O3烧结成的ITO氧化物陶瓷为靶材,采用直流磁控反应溅射法在玻璃基片上制备ITO透明导电薄膜,研究了基片温度和氧分压条件对ITO薄膜的物相结构和光电性能的影响。实验结果表明:ITO薄膜的方块电阻随衬底温度的升高而下降,而可见光透过率增大;ITO薄膜可见光透过率和方块电阻随氧分压的增加而增大。     

膜厚对Zr,Al共掺杂ZnO透明导电薄膜结构和光电性能的影响

采用直流磁控溅射法在玻璃衬底上制备出Zr,Al共掺杂ZnO(AZZO)透明导电薄膜.用XRD和SEM分析和观察了薄膜样品的组织结构和表面形貌.研究表明:制备的AZZO透明导电薄膜为六角纤锌矿结构的多晶薄膜,且具有c轴择优取向.另外还研究了薄膜的结构、光学和电学性质随薄膜厚度的变化关系.当薄膜厚度为843 nm时,电阻率具有最小值1.18×10~(-3) Ω·cm,在可见光区(500～800 nm)平均透过率超过93;.     

Formation kinetics and control of microcrystallite in μc-Si:H from glow discharge plasma

The formation kinetics of μc-Si:H has been investigated through the film depositions and plasma diagnoses in widely-scanned glow discharge plasma conditions; RF power density, SiH₄/H₂ ratio and substrate temperature. The roles of H and SiH_x adsorbed on the surface as well as impinging ions have been discussed in relation to volume fraction and crystallite size of μc films, and continuous control of crystallite size has been demonstrated using a triode system. Hall mobility of the deposited μc-Si:H films has also been presented as a function of the volume fraction of μc.     

衬底温度对直流磁控溅射法制备掺锆氧化锌透明导电薄膜性能的影响

利用直流磁控溅射法在石英衬底上制备出了高透明导电的掺锆氧化锌(ZnO:Zr)薄膜.研究了衬底温度对ZnO:Zr薄膜结构、形貌及光电性能的影响.XRD表明实验中制备的ZnO:Zr为六方纤锌矿结构的多晶薄膜,具有垂直于衬底方向的c轴择优取向.实验所制备ZnO:Zr薄膜的晶化程度和导电性能对衬底温度有很强的依赖性.当衬底温度为300 ℃时, ZnO:Zr薄膜具有最小电阻率7.58×10-4 Ω·cm,其可见光平均透过率超过了91;.     

TiO2 thin films as sensing gas materials

TiO₂ thin films were prepared by DC reactive magnetron sputtering on heated Si, quartz and glass substrates using O₂ and water vapor as reactive gases. The percentage of anatase and rutile as well as the grain size strongly depend on the deposition conditions, as revealed by X-ray diffraction patterns. The films deposited on Si substrates are pure rutile, while a mixed anatase/rutile structure occurs in the films deposited on glass and quartz substrates. Smaller grain rutile and anatase films were prepared in a water vapor atmosphere, in contrast to the films grown in oxygen. The former choice considerably increases the sensing properties of titanium dioxide films. The gas sensitivity was investigated for some reducing gases (methane, acetone, ethanol and liquefied petroleum gas) and the optimum operating temperatures were found.     

基底温度对ZnO/Cu/ZnO透明导电膜性能的影响

采用射频磁控溅射ZnO陶瓷靶、直流磁控溅射Cu靶的方法在不同基底温度下制备了ZnO/Cu/ZnO多层膜.用X射线衍射仪、原子力显微镜、紫外可见分光光度计和四探针测试仪对样品的性能进行了表征.结果表明,随着基底温度的升高,ZnO层c轴择优取向明显,结晶程度变好,Cu层的结晶性先变好后逐渐变差;多层膜表面均方根粗糙度随基底温度的升高而增加;光学透过率随基底温度的升高逐渐增大,基底温度为300 ℃时最大透过率接近90;;面电阻随基底温度的升高逐渐增加,最小面电阻为12.4 Ω/□.     

WO3薄膜的电致变色与响应时间机理研究

采用直流反应磁控溅射方法制备了纳米WO3薄膜,研究了溅射气压对WO3薄膜的表面形貌和微结构的影响.利用X射线衍射仪和扫描电子显微镜对WO3的微结构进行了表征.采用紫外-可见分光光度计和循环伏安测试系统对样品的电致变色及响应时间性能进行了研究.结果表明,纳米WO3薄膜的微孔结构特征具有较大的比表面积,有利于改善其电致变色性能.当溅射气压为4Pa时,WO3薄膜在可见光区的电致变色平均调色范围达到了71.6;,并且其着色响应时间为5 s,漂白响应时间为16 s.     

直流反应磁控溅射法制备ZnO: Zr透明导电薄膜

以Zn∶ Zr为靶材,利用直流反应磁控溅射法制备了ZnO∶ Zr透明导电薄薄膜.研究了沉积压强对ZnO∶ Zr薄膜形貌、结构、光学及电学性能的影响.实验结果表明所制备的ZnO∶ Zr为六方纤锌矿结构的多晶薄膜,具有垂直于衬底方向的c轴择优取向.沉积压强对ZnO∶ Zr薄膜的晶化程度、形貌、生长速率和电阻率影响很大,而对其光学性能如透光率、光学带隙及折射率影响不大.当沉积压强为2Pa时,ZnO∶ Zr薄膜的电阻率达到最小值2.0×10-3Ω ·cm,其可见光平均透过率和平均折射率分别为83.2％和1.97.     

热处理工艺对室温制备ZnO:Al薄膜结构与光电性能的影响

采用室温溅射加后续退火工艺制备了ZnO∶ Al透明导电薄膜.研究了热处理工艺对薄膜微观结构和光电性能的影响.研究表明:退火有助于减小Al~(3+)对Zn~(2+)的取代造成的晶格畸变,消除应力,促进晶粒长大,有效提高电子浓度和迁移率,降低电阻率;当溅射功率为80 W、退火温度为320 ℃时,薄膜的电阻率可低至8.6×10~(-4) Ω·cm;退火气氛对薄膜的导电性能有较大影响,真空退火可使吸附氧脱附,大大降低薄膜的方块电阻.而退火温度和退火气氛均对ZnO∶ Al薄膜的透光率没有明显影响,薄膜的透光率在86;以上.     

Structure and properties of amorphous thin film for optical data storage

In this paper the magnetic and magneto-optical properties of amorphous rare earth-transition metal (RE-TM) alloys as well as the magnetic coupling in the multi-layer thin films for high density optical data storage are presented. Using magnetic effect in scanning tunneling microscopy the clusters structure of amorphous RE-TM thin films has been observed and the perpendicular magnetic anisotropy in amorphous RE-TM thin films has been interpreted. Experimental results of quick phase transformation under short pulse laser irradiation of amorphous semiconductor and metallic alloy thin films for phase change optical recording are reported. A step-by-step phase transformation process through metastable states has been observed. The waveform of crystallization propagation in micro-size spot during laser recording in amorphous semiconductor thin films is characterized and quick recording and erasing mechanism for optical data storage with high performance are discussed. The nonlinear optical effects in amorphous alloy thin films have been studied. By photo-thermal effect or third order optical nonlinearity, the optical self-focusing is observed in amorphous mask thin films. The application of amorphous thin films with super-resolution near field structure for high-density optical data storage is performed.     

Preferential segregation of dopants in μc-Si:H

Electronic and structural properties of heavily B-doped μc-Si:H films prepared by rf glow discharge technique have been studied by Raman scattering, IR absorption, SIMS and conductivity measurements. It is found that boron atoms in μc-Si:H tend to segregate in the amorphous tissue. The remarkable difference in doping efficiency between B- and P-doped μc-Si:H was interpreted in terms of the different degree of dopant segregation in the amorphous phase.     

Preparation and analysis of reactively evaporated a-Si:H

a-Si:H formed by the method of reactive evaporation of silicon with supplying hydrogen ion has much the same properties as films prepared by silane grow discharge (GD) decomposition. Growth kinetics in this method is described. Hydrogen ion suppresses the oxidation of silicon and it is incorporated as mono-hydride, whose content is proportional to hydrogen ion current. Adsorption energy of hydrogen ion is some 130 meV. Dark conductivity of a-Si:H depends mainly on energy gap associated with hydrogen content. Spin density is determined by the collision phenomenon between Si-H and spin in depositing.     

Effect of calcination on the crystallinity of sputtered TiO2 thin films as studied by Raman scattering

Titanium dioxide films have been deposited using DC magnetron sputtering technique onto silicon substrates at an ambient temperature and at an oxygen partial pressure of 7 × 10 ^–5 mbar and sputtering pressure (Ar + O₂) of 1 × 10 ^–3 mbar. The deposited films were calcinated at 673 and 773 K. The composition of the films as analyzed using Auger Electron Spectroscopy (AES) revealed the stoichiometry with an O and Ti ratio of 2.08. The influence of post‐deposition calcination on the Raman scattering of the films was studied. The existence of Raman active modes A_1g, B_1g and E_g corresponding to the Raman shifts are reported in this paper. The improvement of crystallinity of the TiO₂ films as shown by the Raman scattering studies has also been reported. (© 2005 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)     

Pb过量对以Ti-Al为阻挡层的硅基铁电电容器极化翻转性能的影响

以射频磁控溅射法生长的La0.5Sr0.5CoO3( LSCO)为电极,采用溶胶-凝胶法在以Ti-Al为导电阻挡层的Si基片上生长了用不同Pb过量前驱体溶液(溶胶)制备的LSCO/Pb( Zro4Ti0.6)O3(PZT)/LSCO电容器,以此构造了Pt/LSCO/PZT/LSCO/Ti-Al/Si异质结.Pb过量对LSCO/PZT/LSCO电容器极化翻转性能的影响表明:不同Pb过量溶胶对电容器的极化翻转性能影响很大,其中Pb过量15;的溶胶制备的样品在550℃常规退火1h后相对具有较好的翻转性能.在5V的外加电场下,LSCO/PZT/LSCO电容器的矫顽电压和剩余极化强度分别为1.25V和24.6μC/cm2.疲劳和电阻率测试分析表明:在经过109翻转后,不同样品的抗疲劳性能均很好,而电阻率随前驱体溶液Pb过量的增加呈现下降的趋势.     

双靶磁控溅射聚焦共沉积AlN薄膜生长速率研究

采用直流双靶磁控溅射聚焦共沉积技术在Fe衬底上高速率生长A lN薄膜,结果表明,双靶共沉积技术有效地提高了A lN薄膜生长速率,相同工作气压或低N2浓度时双靶磁控溅射沉积速率约为单靶沉积速率的2倍;随着溅射系统内工作气压或N2浓度的升高,薄膜生长速率不断减小;薄膜择优取向与薄膜生长速率相互影响,随着工作气压的升高,(100)晶面的择优生长减缓了薄膜生长速率的降低,随着N2浓度的升高,(002)晶面的择优生长加剧了薄膜生长速率的降低,而相对较低的溅射沉积速率有利于(002)晶面择优取向生长。     

Effect of AC and DC voltage on dielectric properties of CeO2 films

The capacitance-voltage characteristics have been studied for both AC and DC fields of Al/Cerium Oxide/Al thin film capacitor structures. Compared to DC fields, these structures can withstand higher AC fields. Capacitance increases with increase in AC and DC fields. The former behaviour is explained on the basis of presence of oxygen vacancies and the latter one is attributed for the Joule heating phenomena. The presence of oxygen vacancies were confirmed from the thermoluminescence studies on these films.