Ba0.6Sr0.4TiO3薄膜的耐压特性研究

采用射频磁控溅射法制备了Ba0.6Sr0.4TiO3(BST)薄膜,研究了基片、退火温度及膜厚对薄膜耐压特性的影响。结果显示,铝酸镧(LaAlO3)基片上制备的BST薄膜表面较平整,有较好的耐压;随着退火温度从750℃提高到850℃,BST薄膜晶粒长大,电击穿概率有所增加,750℃是一个较合理的退火温度。在优化的工艺条件下,BST薄膜耐压可达125V/μm。     

射频磁控溅射法制备（Ba0.7Sr0.3）TiO3铁电薄膜

采用射频磁控溅射法制备了用于非致冷红外焦平面阵列的（Ba0.7Sr0.3）TiO3（BST）铁电薄膜。研究了BST铁电薄膜的制备工艺,分析了BST铁电薄膜的晶体结构和微观形貌。测试了其介电特性,测得的相对介电常数－温度曲线表明制备的（Ba0.7Sr0.3）TiO3铁电薄膜的居里温度在室温附近,约30℃处。     

基于La0.7Sr0.3FeO3的微结构乙醇气体传感器的研制

以La0.7Sr0.3FeO3为敏感材料,设计制成了一种新型的共平面结构气体传感器.基于有限元分析软件Ansys对该传感器结构进行了优化设计.实验测得该传感器对于500ppm浓度乙醇气体的灵敏度为8.0,功耗为261mW,是同种敏感材料烧结型传感器功耗的2/3,响应时间约为1.5s,恢复时间约为2.5s,是一种功耗低、灵敏度高、稳定性好的微结构乙醇气体传感器.     

Dielectric Characteristics of Ba0.65Sr0.35TiO3 Thin Films Sol-Gel Method

Ferroelectric Ba0.65Sr0.35TiO3 （BST） thin films on the Pt/Ti/SiO2/Si substrate have been successfully prepared by sol-gel. Such films have approximately 300 nm thicknesses with a remnant polarization of about 2.95 μ℃/cm^2 and a coercive field of about 21.5 kV/cm. The investigations of X-ray diffraction and atomic force microscopy show that the BST films annealed at 650 ℃ exhibit a tetragonal structure and that the films dominantly consist of large column or grains of about 89 nm in diameter. The curves of the temperature dependence of dielectric coefficient in different frequencies display the curie transition at the temperature around 23 ℃. The dielectric loss tangent of BST thin fdms at 100 kHz is less than 0.04. As a result, the BST thin films are more applicable for fabrication of infrared detector compared with the BST thin films reported previously.     

基于La0.7Sr0.3FeO3的微结构乙醇气体传感器的研制

以La0.7Sr0.3FeO3为敏感材料,设计制成了一种新型的共平面结构气体传感器.基于有限元分析软件Ansys对该传感器结构进行了优化设计.实验测得该传感器对于500ppm浓度乙醇气体的灵敏度为8.0,功耗为261mW,是同种敏感材料烧结型传感器功耗的2/3,响应时间约为1.5s,恢复时间约为2.5s,是一种功耗低、灵敏度高、稳定性好的微结构乙醇气体传感器.     

化学溶液法制备的Ba0.9Sr0.1TiO3薄膜的结构及光学特性研究

采用高度稀释的前驱体溶液在LaNiO3(LNO)薄膜上沉积了Ba0.9Sr0.1TiO3(BST)薄膜。X-射线衍射分析表明BST薄膜呈高度的（100）择优取向。原子力显微镜测量发现制备的BST薄膜具有大的晶粒尺寸80-200nm。用椭偏光谱仪测量了光子能量为0.7-3.4eV范围内BST薄膜的椭偏光谱，用Cauchy模型描述BST薄膜的光学性质，获得了BST薄膜的光学常数谱和禁带宽度Eg=3.36eV。     

La0.7Ca0.3MnO3多晶薄膜的sol-gel法制备及表征

以La、Ca、Mn的无机盐替代相应的醇盐,以冰乙酸为溶剂,乙酰丙酮(AcAc)为螯合剂,采用sol-gel法在Si(110)衬底上制备了La0.7Ca0.3MnO3(LCMO)多晶薄膜,并用FTIR、XRD、SEM、EDS和TEM等分析手段对薄膜进行了表征,通过不同磁场下电阻一温度(R-T)曲线,研究了样品的输运性质及...     

（Ba0.5Sr0.5）TiO3铁电薄膜的制备工艺及电学性质研究

采用溶胶 凝胶方法制备出纯立方钙钛矿相、介电性能和漏电流特性良好的 (Ba0 .5Sr0 .5)TiO3 铁电薄膜 .研究发现 ,随着烧结温度的升高 ,(Ba0 .5Sr0 .5)TiO3 薄膜纯度和结晶度增高 ,介电常数提高 ,漏电流密度降低 .在 75 0℃进行保温 1h热处理的薄膜性能较好且稳定 :在室温下测得薄膜介电常数为 2 5 0 ,介电损耗为 0 .0 30 ,漏电流密度为 6 .9× 10 -8A/cm2 .较高的介电常数、较低的漏电流密度可能源于良好的纯度和结晶度 .进一步研究表明 ,薄膜导电遵从空间电荷限制电流机制 .     

PbxSr1-xTiO3陶瓷及薄膜的制备和性能研究

研究了Pb的摩尔分数对PbxSr1-xTiO3(x=0.2~0.8)陶瓷微结构和介电性能的影响,当x<0.45时晶体为立方相,x≥0.45时为四方相;随着Pb的摩尔分数增大,陶瓷气孔率下降,致密度增加,晶粒尺寸逐渐增大,居里峰近似线性地向高温方向移动,并具有一致的居里外斯常数。采用射频磁控溅射法在Pt/Ti/SiO2/Si(100)上制备了Pb0.3Sr0.7TiO3(PST30)薄膜,经550℃退火后为(111)择优取向的多晶薄膜,1 kHz下的可调率为21.8%。     

倒筒式射频溅射频偏压对Ba0.65Sr0.35TiO3热释电薄膜结构及性能的影响

采用倒筒式射频溅射方法,在Pt、Ti/SiO2/Si基片上制备了Ba0.65Sr0.35TiO3(简称BST)薄膜.研究了自偏压对BST薄膜结构及电学性能的影响.在较高自偏压下制备的BST薄膜具有高度的(100)择优取向,且结晶性好,表面平整,耐压能力强.在25℃时薄膜的热释电系数高达6.73×10-7C.cM-2.K-7.研究结果表明,利用倒筒式射频溅射方法适当提高自偏压,可以制备出热释电性能优良的BST薄膜.     

Y_2O_3掺杂超细(Ba,Sr)TiO_3基电容器陶瓷的研究

通过sol-gel法制得高纯、超细的Ba0.7Sr0.3TiO3粉体。以液相法掺杂MgO、ZnO、Bi2O3,和Y2O3等物质,得到平均粒径为50nm左右的混合粉体,制备出超细晶BST电容器陶瓷。分析了掺杂Y2O3对BST电容器陶瓷介电性能和显微结构的影响。结果表明:适量的Y2O3掺杂能够明显改善陶瓷介电性能,当w(Y2O3)为0.75%,烧结温度为1200℃时,得到了εr为2538,tanδ为0.006,耐压强度为5.83×103V/mm的BST电容器陶瓷。     

磁控溅射法制备BST铁电薄膜的实验研究

采用射频磁控溅射法在Si和Pt/TiOx/SiO2/Si衬底上沉积了(Ba0.65Sr0.35)TiO3铁电薄膜,研究了BST铁电薄膜微观结构和介电性能。实验结果表明:衬底温度在550℃,工作气压为2.0 Pa的溅射条件下沉积的BST薄膜,经750℃退火处理30 min后,形成了完整的钙钛矿相;与Si衬底相比,在Pt衬底上制备的BST薄膜晶粒更均匀、表面平整无裂纹。在室温、频率为100 kHz条件下薄膜的介电常数ε=353.8,介电损耗tanδ=0.012 8。介电温谱结果表明制备的(Ba0.65Sr0.35)TiO3铁电薄膜居里温度在5.0℃左右。     

低阻钛酸锶钡基PTC材料的制备与电性能

BaTiO3正温度系数(PTC)陶瓷因其具有较高的室温电阻率而使其在低压领域中的应用受到限制,因此,有必要降低其室温电阻率.低阻化的一个途径是将金属与BaTiO3基PTC陶瓷复合来制备复合PTC材料.采用传统陶瓷工艺制备Ni/(Ba,Sr)TiO3复合PTC材料.为避免金属Ni被氧化,复合材料在弱还原气氛下烧成.为排除烧结气氛的影响而讨论金属Ni的影响,(Ba,Sr)TiO3 PTC陶瓷也在同一弱还原气氛下烧成.PbO-B2O3-ZnO-SiO2系玻璃料的加入改善了复合材料的两相分布,优化了复合材料的性能.     

La0.7Sr0.3FeO3对SnO2基CO气敏元件性能的影响

采用柠檬酸盐法合成纳米晶La0.7Sr0.3FeO3。为考察其对以SnO2为基体材料的一氧化碳气敏元件性能的影响,将一定质量分数的(1%、3%、5%)La0.7Sr0.3FeO3作为掺杂剂掺入SnO2粉体中。测试结果表明,La0.7Sr0.3FeO3的掺入改善了气敏元件的长期稳定性,同时提高了元件对CO气体的灵敏度,经10 d的老化后,80 d内元件阻值变化不超过±10%。用4A分子筛对元件进行表面修饰,改善了元件的选择性。     

Pechini法制备超细BST粉体及其陶瓷的研究

采用Pechini法制备了约100nm的（Ba0.79Sr0.21）TiO3超细粉体,并在其中掺杂超细Bi4Ti3O12粉体制备了BST混合粉体．并用其制备了平均粒径为0．5μm、ετ为1740和tanδ为0．0038的BST陶瓷．研究了热处理温度和分散剂的量对粉体性能的影响,烧结温度对BST陶瓷介电性能和显微结构的影响。得到了较优的工艺参数,即热处理温度800℃、分散剂的量2．25mL和烧结温度1150℃．     

Strain‐Mediated Inverse Photoresistivity in SrRuO3/La0.7Sr0.3MnO3 Superlattices

In the pursuit of novel functionalities by utilizing the lattice degree of freedom in complex oxide heterostructure, the control mechanism through direct strain manipulation across the interfaces is still under development, especially with various stimuli, such as electric field, magnetic field, light, etc. In this study, the superlattices consisting of colossal‐magnetoresistive manganites La_0.7Sr_0.3MnO₃ (LSMO) and photostrictive SrRuO₃ (SRO) have been designed to investigate the light‐dependent controllability of lattice order in the corresponding functionalities and rich interface physics. Two substrates, SrTiO₃ (STO) and LaAlO₃ (LAO), have been employed to provide the different strain environments to the superlattice system, in which the LSMO sublayers exhibit different orbital occupations. Subsequently, by introducing light, we can modulate the strain state and orbital preference of LSMO sublayers through light‐induced expansion of SRO sublayers, leading to surprisingly opposite changes in photoresistivity. The observed photoresistivity decreases in the superlattice grown on STO substrate while increases in the superlattice grown on LAO substrate under light illumination. This work has presented a model system that demonstrates the manipulation of orbital–lattice coupling and the resultant functionalities in artificial oxide superlattices via light stimulus.     

Large,Temperature‐Tunable Low‐Field Magnetoresistance in La0.7Sr0.3MnO3:NiO Nanocomposite Films Modulated by Microstructures

Magnetic properties and low‐field magnetoresistance (LFMR) in La_0.7Sr_0.3MnO₃ (LSMO):NiO nanocomposite films grown on SrTiO₃ (001) substrates, which are shown to be tunable with different microstructures, are investigated. The LSMO:NiO nanocomposite films with NiO volume ratio of 50% have a checkerboard‐like structure and show a large LFMR in a temperature range from 200 to 300 K (≈17% at 250 K with a magnetic field of 1 T). As the NiO volume ratio is increased to 70%, a nano‐columnar structure formed in the films. Their LFMR is significantly enhanced at a wide temperature range of 10–210 K. The highest value of LFMR with 41% is achieved at 10 K in a magnetic field of 1 T. The enhanced LFMR can be considered to result from the electron scattering at the ferromagnetic LSMO/NiO interfaces and magnetic tunnel junctions (MTJs) of LSMO/NiO/LSMO at the nanometer scale. These results demonstrate that large and tunable LFMR from low temperature to room temperature can be realized by controlling the microstructures in the epitaxial La_0.7Sr_0.3MnO₃:NiO nano­composite thin films, which will be expected to be applied in the devices using for a wide temperature range.     

凝胶固相反应法合成亚微米级钛酸锶钡陶瓷粉体

以TiO2和BaCO2,SrCO3粉体为原料,采用凝胶固相反应法合成了亚微米级Ba—Sr0.4TiO3陶瓷粉体。对凝胶固相反应过程进行了DSC热分析,并观察和测定了合成粉体的微观形貌、相结构和粒度分布。结果表明：Ba0.6Sr0.4TiO3粉体合成温度对应于857℃,在900～1000℃温度范围煅烧均可获得颗粒尺寸约0．5μm、粒径分布均匀的Ba0.6Sr0.6TiO3粉体。试验结果表明,凝胶固相合成Ba0.6Sr0.4TiO3的粉体粒径取决于原料粉体尺寸,经高温煅烧后因各组元元素的互扩散导致粉体粒径有所长大,要获得更细的合成粉体应采用更细的粉体原料。     

BST铁电薄膜非制冷红外探测器热成像应用

报道了基于Bao.8Sr0.2TiO3薄膜的红外探测器列阵原型器件,并通过将探测器器件与光学机械扫描器、红外图象采集卡、信号处理电路、热像仪系统软件和热像记录装置等组合形成整机系统,采用单元扫描方式,获得了目标物体的热图像.制作器件的Bao.8Sr0.2 TiO3薄膜是使用浓度为0.05 M的前躯体溶液、采用溶胶-凝胶法制备的.对Bao.8Sr0.2 TiO3薄膜材料的测试结果表明,在5～30℃的温度范围内,a0.8 Sr0.2TiO3薄膜的热释电系数大于20 nC/cm2K,在16℃处达到最大值41. 3 nC/cm2K.在23℃的环境温度下,使用1000 K的标准黑体和35 Hz的调制频率,测得探测器列阵探测单元的探测率D*为2.3×108cmHz1/2W-1,已经能够满足红外热像仪应用的要求.