化学溶液法在LaAlO3单晶基体上制备YBa2Cu3O7-x薄膜的研究

采用三氟乙酸盐-金属有机沉积(TFA-MOD)法在LaAlO3单晶基体上成功地制备了YBa2Cu3O7-x超导薄膜(简称YBCO薄膜),并比较系统地研究了烧结温度对YBCO薄膜的影响。在烧结温度为820℃时,所制备的YBCO薄膜完全呈c-轴取向,无a-轴取向的晶粒和杂质相存在,YBCO薄膜的表面无裂纹存在,表面平整,超导转变温度Tc≈90K,转变宽度ΔTc=1K,临界电流密度(Jc)可达1.2MA.cm-2(77K,0T)。     

走带速率对Y2O3隔离层生长的影响

采用反应溅射的方法在具有立方织构的Ni基底上连续制备了 Y2O3隔离层.用X射线θ～2θ扫描, φ扫描对薄膜的取向和织构进行表征,用扫描电子显微镜(SEM)对薄膜的表面形貌进行观察.主要研究了走带速率对隔离层外延生长及表面形貌的影响.实验表明:随着走带速率的增大,Y2O3的平面内φ扫描半高宽(FWHM)增大,(400)峰的相对强度减小,晶粒更加细小;同时,制备的三层Y2O3隔离层,其面内φ扫描半高宽取决于第一层的半高宽;最终在三层Y2O3隔离层上沉积了有良好外延取向的YBCO超导层,其FWHM为8.0°.     

倾斜衬底上沉积的钙钛矿结构氧化物薄膜的电阻各向异性

用脉冲激光沉积法(PLD)分别在平的和倾角为10°、15°、20°的LaAlO3倾斜衬底上制备了La0 5Sr0 5CoO3薄膜和La0 67Ca0 33MnO3薄膜。用四探针法测量薄膜表面的电阻,发现平衬底上生长的薄膜没有电阻各向异性,而倾斜衬底上生长的薄膜存在电阻各向异性现象,并且倾角越大,电阻各向异性越明显。这是由于倾斜衬底上薄膜的自组织结构造成的。     

采用TFA-MOD技术在LaAlO3单晶基片上制备YBa2Cu3O7-x涂层导体

三氟乙酸盐-金属有机沉积技术（TFA-MOD）是制备钇钡铜氧涂层导体的有发展前景的方法之一。采用TFA-MOD技术在铝酸镧单晶基片上制备出YBa2Cu3O7-x涂层导体，并对不同烧结温度下制备的薄膜作了分析比较，找到了较为合适的烧结温度。用X射线衍射进行了物相的定性分析，由YBCO薄膜的（103）φ扫描图谱分析了薄膜的外延生长，用原子力显微镜观察了薄膜表面形貌。结果 表明制备出的YBCO薄膜表面均匀致密、无明显裂纹、有较强的（001）衍射峰。     

射频溅射法在CeO2/YSZ/Y2O3/NiW衬底上制备YBCO超导层

用射频溅射的方法在强立方织构的CeO2/YSZ/Y2O3/NiW衬底上制备了YBCO超导层. 温度、气压等因素对超导层的外延生长有重要影响. 在基片温度大于780 ℃, 气压在11～160 Pa之间, 都有NiWO4化合物生成;在退火吸氧过程中, 金属基底被氧化. 最终在温度780 ℃, 气压100 Pa的条件下, 制备出了纯（00l）取向的YBCO薄膜, 其平面内φ扫描半高宽小于10°, 超导转变温度为87.2 K, 传导电流为11 A.     

TFA-MOD法制备多层YBCO超导薄膜的特性研究

采用TFA-MOD法在LaAlO3单晶基片上制备出了五层YBa2Cu3O7-δ薄膜,膜层总厚度为1!m,临界电流密度Jc达到1.6MA/cm2,临界电流Ic为160A/cm。单层膜与三层膜的Jc值分别为3.5、1.75 MA/cm2;三层膜和五层膜截面TEM形貌中均无裂纹和明显空洞产生,各层之间的界面平滑。随着膜层厚度的增加,临界电流密度降低,主要原因可能是膜性能的劣化。     

不同生长温度对Ga掺杂ZnO透明导电薄膜性能的影响

采用磁控溅射方法在普通载玻片衬底上制备了Ga掺杂的ZnO(GZO)透明导电薄膜,并研究了不同生长温度对GZO透明导电薄膜的结构性能、电学性能及光学性能的影响.制备的GZO透明导电薄膜均沿(002)方向的择优取向生长,薄膜的表面形貌为蠕虫状,表明薄膜内存在较大的残余应力.随着生长温度的升高,GZO薄膜的电阻率先减小后增大,在生长温度为250℃时,薄膜的最低电阻率为1.91×10-3 Ωcm.不同生长温度下所制备的GZO薄膜在可见光波段的平均透过率均大于90％,薄膜具有优异的光学特性.     

采用溶胶-凝胶方法制备Tl-2212超导薄膜

研究了采用溶胶-凝胶法在(001)取向的铝酸镧(LAO)单晶衬底上制备Tl2Ba2CaCu2O8(Tl-2212)高温超导薄膜。该方法是以乙酸铊、乙酸钡、乙酸钙、乙酸铜为起始原料,其中,Tl,Cu的含量要略高于Tl-2212超导相中的比例,并以乳酸、α-甲基丙烯酸、二乙烯三胺、三乙烯四胺、甲酰胺、甲醇为络合剂及溶剂,制得粘度合适的溶胶。以旋转涂层方法制备凝胶膜,凝胶膜经过干燥、热分解及后退火等工艺处理后,可得到超导样品。X射线衍射(XRD)的θ-2θ和Φ扫描测试表明,该样品为纯c轴取向的Tl-2212高温超导薄膜,且ab面内织构;电子能谱分析(EDX)和扫描电子显微镜(SEM)测试表明,该薄膜的组分比为Tl∶Ba∶Ca∶Cu=2∶2∶1∶2,且具有平整致密的表面形貌;临界温度(Tc)测试表明,薄膜具有良好的超导特性,其Tc可达104.5 K。     

Study on Zr and Y co-doped BaCeO3 film enhencement of lightning-strike protection equipment

采用溶胶-凝胶法,在铁基底上制备了Zr和Y掺杂的BaCeO3体系涂层薄膜,利用X射线衍射（XRD）、扫描电镜（SEM）和TEM,表征了其晶体结构、表面和断面形貌。XRD分析结果表明,制备的膜层以BaCe0.8Zr0.1Y0.1O3-a相为主;膜层表面SEM表征结果表明,涂层均匀,没有大的裂纹、孔洞等缺陷;膜层与基底断面的TEM表征结果表明,界面处两者匹配较好。在干燥和湿润空气条件下测量膜层材料电导率,湿润空气中膜层材料电导率较高,且温度越高其电导率越高。这种膜层适合作为避雷线的保护层,并能起到增强避雷线性能的作用。     

热处理温度对MOD-YBCO薄膜微结构和超导电性的影响

采用TFA-MOD法在LaAlO3基体上制备YBCO薄膜,热处理温度为780-860℃。XRD结果表明,热处理温度在780-820℃之间时,随着热处理温度的提高,YBCO薄膜中BaF2逐渐减少,a轴生长的晶粒和杂质相减少,c轴生长的晶粒增加;热处理温度在820-860℃之间时,随着热处理温度的升高,薄膜中a轴生长的晶粒增加,c轴生长的晶粒减少;SEM分析发现,YBCO薄膜表面较平整,无裂纹;超导性能测试结果表明,热处理温度为820℃的YBCO薄膜的临界电流密度Jc可达1 MA.cm^-2（77 K,0 T）。     

Microstructure and Properties of La_(0.7)Sr_(0.3)MnO_3 Films Deposited on LaAlO_3 (100), (110), and (111) Substrates

Recently , doped perovskite manganite has kin-dled a renewed interest because they exhibit a varietyof unique magnetic and electronic behaviors such ascolossal magnetoresistance (CMR) ,percolative phaseseparation,and spin/charge/orbital ordering[1 ~3].Theemphasis of both theoretical and experi mental studiesof doped materials has beenthe effect of CMRbecauseit can be usedfor potential applicationin magnetic de-vices .As a member of the CMR materials ,La0 .7Sr0 .3MnO3(LSMO) possesses the …     

热丝辐射距离与甲烷浓度对CVD金刚石薄膜的影响

以H2和CH4作为反应气体,采用热丝化学气相沉积法(Hot filaments chemical vapor deposition,HFCVD),在WC-3%Co条状平板上制备金刚石薄膜,利用扫描电镜(SEM)、X射线衍射(XRD)、激光拉曼光谱(Raman)和洛氏硬度仪分析薄膜的形貌、结构、成分和附着性能,研究热丝辐...     

Preparation and Characterization of Sol-Gel Derived Au Nanoparticle Dispersed Y2O3：Eu Films

Gold nanoparticles dispersed Y2O3 films were prepared through a sol-gel method by using yttrium acetate and Au nanoparticles colloid as precursors. The films were characterized by X-ray diffraction （XRD）, transmission electron microscopy （TEM） and UV-VIS absorption spectra. XRD patterns and TEM images of Y2O3 ＋ Au films give the same resuits on structure and particle size as that of pure Y2O3 films. The surface plasma resonance （SPR） of Au nanoparticles in Y2O3 ＋ Au film was observed around 550 nm in the absorption spectrum and its position shifts to red with increasing annealing temperature is caused by the increase of dielectric constant of Y2O3 matrix and the size of Au nanoparticles. The second and third order nonlinear optical effects of Y2O3 ＋ Au films were also observed. The photoluminescent properties of Y2O3 ： Eu ＋ Au films were investigated and results indicate that there exist an energy transfer from Eu^3 ＋ to Au nanoparticles and this energy transfer decreases the emission of Eu^3 ＋ in Y2O3 ： Eu ＋ Au film.     

锆处理低碳低合金高强度钢的杂质控制

针对传统工艺技术生产的高强度低合金钢(HSLA)中杂质较高、性能不稳定等缺陷,改进了冶炼及连铸过程中一些工艺,形成了一套自主操作技术.生产的锆处理HSLA钢杂质含量显著降低,加入合金元素锆经改进工艺生产的钢板中夹杂物的大小、形态及分布均得到了明显改善,形成颗粒细小、圆形或近圆形、呈弥散分布的夹杂物.经电子探针和能谱分析表明,夹杂物一般是由Ti2O3、Al2O3、ZrO2及MnS组成的复合夹杂物,Ti2O3、Al2O3、ZrO2位于复合夹杂物的中心部位,MnS位于外层.锆处理和新工艺联合应用有效地改善了钢中夹杂物的特性,生产的HSLA钢板质量大幅度提高,具有良好的力学性能.     

Rare earths (Ce,Y, Pr) modified Pd/La_2O_3-ZrO_2-Al_2O_3 catalysts used in lean-burn natural gas fueled vehicles

14%REO_x-2.5%La_2 O_3-33.5%ZrO_2-50%Al_2 O_3(RE = Ce, Y, Pr) composites were prepared by a coprecipitation method. The Pd catalysts were obtained by an aqueous solution of Pd(NO_3)_2 loaded on the rare earths modified composites with an initial wet impregnated method. The experiment results show that catalytic activity of the rare earths modified Pd/La_2 O_3-ZrO_2-Al_2 O_3 catalysts is better than bare sample for methane oxidation. The structural characterization results reveal that the rare earths modified Pd catalysts increase amounts of surface active oxygen species by X-ray photoelectron spectroscopy(XPS) analysis and improve the dispersion of active component from H2-temperature programmed reduction(H2-TPR) measurement compared with bare sample. Especially,Pd/14%Y_2 O_3-2.5%La_2 O_3-33.5%ZrO_2-50%Al_2 O_3 sample exhibits highly active stability, it is related to the Pd particles highly dispersion,which was observed by transmission electron microscope(TEM) images.     

Phase control of magnetron sputtering deposited Gd2O3 thin films as high-κ gate dielectrics

Gd2O3 thin films as high-κ gate dielectrics were deposited directly on Si(001) substrates by magnetron sputtering at a pressure of 1.3 Pa and different temperatures. X-ray diffraction results revealed that all the films grown from 450 to 570℃ were crystalline, and the Gd2O3 thin films consisted of a mixture of cubic and monoclinic phases. The growth temperature was a critical parameter for the phase constituents and their relative amount. Low temperature was favorable for the formation of cubic phase while higher temperature gave rise to more monoclinic phase. All the Gd2O3 thin films grown from different temperatures exhibited acceptable electrical properties, such as low leakage current density (JL) of 10-5 A/cm2 at zero bias with capacitance equivalent SiO2 thickness in the range of 6-13 nm. Through the comparison between films grown at 450 and 570℃, the existence of monoclinic phase caused an increase in JL by nearly one order of magnitude and a reduction of effective dielectric constant from 17 to 9.     

Effect of metal doping into Ce0.5Zr0.5O2 on catalytic activity of MnOx/Ce0.5-xZr0.5-xM0.2xOy/Al2O3 for benzene combustion

The research investigated the effect of doping two metals separately or together into Ce0.5Zr0.5O2 on the catalytic activity of MnOx/Ce0.5–xZr0.5–xM0.2xOy/Al2O3 (M=Y, Mn, Y and Mn) for catalytic combustion of benzene. The prepared catalysts were characterized by X-ray diffraction (XRD), surface area analysis, oxygen storage capacity (OSC), and H2-temperature programmed reduction (H2-TPR). Cata-lytic test was performed on a conventional fixed bed flow reactor. The characterization results revealed that Y and Mn ions entered into the ceria-zirconia mixed oxides framework, which improved the textural properties and greatly promoted the MnOx dispersion on the support surface. The complete conversion temperature of benzene on MnOx/Ce0.4Zr0.4Y0.1Mn0.1Oy /Al2O3 was 563 K, and the selectivity of carbon dioxides was 99%. This catalyst could be applied in a wide range of GHSV and wide concentration condition, showing great potential for application.     

Band gap and structure characterization of Tm2O3 films

Single crystalline Tm2O3 films were grown on Si (001) substrates by molecular beam epitaxy using metallic Tm source and atomic oxygen source. X-ray photoelectron spectroscopy, atomic force microscopy and high-resolution transmission electron microscopy were employed to investigate the compositions, surface morphology and microstructure of the sample. A very flat surface with a root mean square roughness of 0.3 nm could be reached, and a sharp interface between the film and the Si substrate was achieved. The result of optical spectrum at ultraviolet and visible wavelengths showed that the band gap of the Tm2O3 film was 5.76 eV.     

Microstructure and Properties of Lao.7 Sr0.3 MnO3 Films Deposited on LaAlO3 （100）, （110）, and （111） Substrates

A comparative study of the crystalline structure, magnetic properties, and transport properties of LSMO films grown on （100）-, （110）-, and （111） LaAlO3（LAO） substrates was carried out. Using atomic force microscopy, round, rectangle, and dot surface morphologies were observed in （ 100）-, （ 110）-, and （ 111 ）-oriented LSMO films, respectively. Electrical and magnetic characterizations were performed on LSMO films of different orientation to provide evidence for the effect of strain on the magnetotransport properties. The （ 111 ）-oriented LSMO film has higher saturation magnetization and lower resistance compared with the （100）- and （110）-oriented LSMO films, which results from the smaller elastic deformation due to the larger elastic modulus along the 〈 111 〉 crystallographic direction.     

Rare Earth Doping Effects on Properties of Ceria-Zirconia Solid Solution

Ce0.6Zr0.3RE0.1O2(RE=Y, La, Pr, Tb)solid solutions were prepared by co-precipitation technique and characterized by a series of methods. XRD and FT-Raman results show that Ce0.6Zr0.3RE0.1O2 has cubic fluorite structure. The different dopant ion radii bring different effect on the cell parameter of Ce0.6Zr0.3RE0.1O2. The X-ray photoelectron spectroscopy (XPS) results show that the binding energy of Ce3d, Zr3d and O1s for Ce0.6Zr0.3RE0.1O2 rises compared with that for Ce0.6Zr0.4O2, indicating that dopant elements change chemistry environment of solid solutions which is available to improve redox performance. Compared with Pd/Ce0.6Zr0.4O2, doping Y and La does not change air/fuel (A/F) characteristic of TWCs, but doping Pr and Tb widens A/F operating window and makes HC, CO and NO have higher conversion. The light-off temperature of Pd/Ce0.6Zr0.3La0.1O2 is corresponding to that of Pd/Ce0.6Zr0.4O2. However, the light-off temperatures of Pd/Ce0.6Zr0.3M0.1O2 (M=Y, Pr, Tb) are lower than that of Pd/Ce0.6Zr0.4O2, which keep much lower after high temperature treatments. Among Pd/Ce0.6Zr0.3RE0.1O2, Pd/Ce0.6Zr0.3Tb0.1O2 represents wider A/F operating window, higher conversion, lower light-off temperature and better high-temperature resistance.