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1.
采用金属有机化学液相沉积法在Si衬底上制备了La0.Sr0.5CoO3(LSCO)导电金属氧化物薄膜,采用溶胶-凝胶法在LSCO导电金属氧化物薄膜上沉积了PbZr0.5Ti0.5O3(PZT)铁电薄膜,X-射线测量结果表明在700℃的退火温度下制备的PZT/LSCO铁电多层薄膜呈(110)取向的钙钛矿结构,谢乐公式估算铁电薄膜的晶粒尺寸为50-80nm,原子力显微镜观察结果显示:薄膜表面平整,均方根粗糙度(RMS)小于5nm,用拉曼光谱测量表明PZT薄膜呈拉曼活性,椭圆偏振光谱仪用来表征薄膜在400-1700nm波长范围的光学性质,用洛仑兹模型来描述PZT和LSCO薄膜的光学性质,获得PZT和LSCO薄膜的折射率,消光系数等光学常数谱。  相似文献   

2.
采用溶胶-凝胶(Sol-Gel)法在Si衬底上沉积一层La0.5Sr0.5CoO3(LSCO)薄膜底电极,并在不同的退火温度下表征薄膜的各种性质.X线衍射表明在550~750℃退火温度下制备的LSCO薄膜呈(110)取向的钙钛矿结构;谢乐公式估算薄膜的晶粒尺寸为25~50 nm.扫描电子显微镜(SEM)观察结果显示:薄膜表面平整,结构致密.运用四探针法测量薄膜的体电阻,结果表明,750℃退火温度后渗氧处理可获得电阻率较低的La0.5Sr0.5 CoO3薄膜.  相似文献   

3.
用化学溶液沉积法在Si衬底上制备了La0.5Sr0.5CoO 3(LSCO)导电薄膜.X-射线衍射结果表明退火温度600℃可以使LSCO薄膜晶化,薄膜没 有明显的择优取向并呈单一的钙钛矿相.原子力显微镜研究结果表明LSCO薄膜表面平整、无 裂纹及晶粒尺寸较大.用椭偏光谱仪测量了波长300~1700nm范围内LSCO薄膜的椭偏光谱.用适当的拟合模型进行拟合,获得了LSCO 薄膜的光学常数(包括折射率,消光系数,吸收系数等)谱.  相似文献   

4.
采用化学溶液淀积法制备了具有纯钙钛矿结构和良好导电性能的La_(0.5)Sr_(0.5)CoO_3(LSCO)薄膜。LSCO的电阻率随着退火温度的升高、退火时间的增长和厚度增加而减小。650°C退火可以得到7mΩ·cm的电阻率。分别在LSCO和Pt衬底上制备了Bi_4Ti_3O_(12)(BTO)薄膜,分析结果表明,使用LSCO衬底对BTO的析晶有影响,击穿电压、铁电特性均有较大改善。  相似文献   

5.
利用脉冲激光沉积法在STO(001)基片上外延生长了La0.5Sr0.5CoO3(LSCO)导电氧化物薄膜,研究了基片温度对LSCO薄膜结构和电性能的影响,并制备了Ni-Cr/BST/LSCO多层膜结构。XRD谱发现,沉积温度在450~700℃均能得到高度(00 l)取向的LSCO薄膜,LSCO(002)峰的半高峰宽FWHM=0.1°~0.2°;在LSCO薄膜上制备的BST介质膜具有良好的c轴取向和较高的表面平整度,其εr约为470,tgδ为0.036~0.060。  相似文献   

6.
在Si(111)衬底上利用等离子体辅助分子束外延(P-MBE)生长氧化锌(ZnO)薄膜,研究了在不同衬底生长温度下(350~750℃)制备的ZnO薄膜的结构和光学性质.随着衬底温度的升高,样品的X射线及光致发光的半高宽度都是先变小后变大,衬底温度为550℃样品的结构及光学性质都比较好,这表明550℃为在Si(111)衬底上生长ZnO薄膜的最佳衬底温度;同时,我们还通过550℃样品的变温光致发光谱(81~300K)研究了ZnO薄膜室温紫外发光峰的来源,证明其来源于自由激子发射.  相似文献   

7.
采用直流反应磁控溅射法在Si(111)基片上制备了AIN薄膜,利用XRD、原子力显微镜(AFM)、电流-电压(I-V)测试仪等对不同衬底下制备薄膜的结构、形貌及电阻率等进行了分析表征.结果表明:随着衬底温度的升高,晶粒逐渐长大,AIN(002)择优取向明显改善,600℃达到最佳.一定范围内提高温度使晶粒均匀、致密,有利于改善表面粗糙情况和提高电阻率,550℃时表面粗糙度达到最低(2.8 nm)且有最大的电阻率(3.35×1012Ω·cm);同时薄膜应力随温度升高有增大趋势.  相似文献   

8.
刘爱云 《激光与红外》2008,38(6):566-568
采用化学溶液沉积法在Pt/TiO2/SiO2/Si衬底上制备LaxSr1-xCoO3(简称LSCO)导电薄膜,对不同的La/Sr比以及掺入Ni的情况下LSCO导电薄膜的红外光学性质进行了比较研究.结果表明:LSCO薄膜的红外吸收与La/Sr的化学计量比值有关,当La/Sr为1∶1时,LSCO薄膜的红外吸收最强;在LSCO薄膜中掺入一定量的Ni后,其红外光吸收将会增强,这说明掺Ni有利于提高基于LSCO薄膜电极的铁电探测器的红外吸收能力.  相似文献   

9.
利用化学气相淀积(CVD)的方法在AlN/Si(111)复合衬底上成功实现了4H-SiC薄膜的异质外延生长,用X射线衍射(XRD)、扫描电子显微镜(SEM)、阴极荧光(CL)等方法对所得样品的结构特征、表面形貌和光学性质进行了表征测量.XRD测量结果显示得到的SiC薄膜的晶体取向单一;室温CL结果表明所得SiC薄膜为4H-SiC,且随着生长温度的升高,SiC薄膜的CL发光效率提高.生长温度、反应气源中C/si比等工艺参数对SiC薄膜的外延生长及其性质影响的研究表明在AIN/Si(111)复合衬底上外延4H-SiC的最佳衬底温度为1230~1270℃,比通常4H-SiC同质外延所需的温度低200~300℃;较为合适的C/Si比值为1.3.  相似文献   

10.
采用磁控溅射法制备La0.5Sr0.5CoO3(LSCO)薄膜、sol-gel法制备Pb(Zr0.4Ti0.6)O3(PZT)薄膜,在玻璃和Ti-Al/Si衬底上构架了LSCO/PZT/LSCO电容器,研究了衬底对LSCO/PZT/LSCO电容器结构和铁电性能的影响。研究发现:虽然生长在两种衬底上的PZT薄膜均为钙钛矿结构多晶薄膜,但是,生长在玻璃衬底上的LSCO/PZT/LSCO电容器具有更好的铁电性能。玻璃基LSCO/PZT/LSCO电容器的剩余极化强度(Pr)为28×10–6C/cm2,矫顽电压(Vc)为0.96V;而硅基LSCO/PZT/LSCO电容器的Pr为25×10–6C/cm2,Vc为1.05V。  相似文献   

11.
在不同衬底温度下,用脉冲激光沉积法(PLD),在Al2O3(0001)平面上生长了ZnO薄膜。研究了衬底温度对其结晶质量、电学性质以及发光性质的影响。结果显示:XRD在2θ为34°处出现了唯一的ZnO(0002)衍射峰;ZnO薄膜的电阻率随衬底温度的升高而增大;在衬底温度为500℃时,出现了位于410nm附近的特殊的光致发光(PL)峰。  相似文献   

12.
在从室温到800℃的温度范围内,用脉冲激光沉积方法在Al2O3(0001)衬底上制备了ZnO薄膜。采用X射线衍射仪、原子力显微镜以及荧光光谱仪分别研究了衬底温度对ZnO薄膜表面形貌、结晶质量和光致发光特性的影响。X射线衍射仪和原子力显微镜的结果表明,当衬底温度从室温升高到400℃时,ZnO薄膜的结构及结晶质量逐渐提高,而当衬底温度超过400℃时,其结构和结晶质量变差;在400℃下生长的ZnO薄膜具有最佳的表面形貌和结晶质量。室温光致发光的测量结果表明,400℃下生长的ZnO薄膜的紫外发光强度最强,且发光波长最短(386 nm)。  相似文献   

13.
Epitaxial Ba0.6Sr0.4TiO3 (BST) thin films were deposited on LaAlO3 (LAO) substrates with the conductive metallic oxide La0.5Sr0.5CoO3 (LSCO) film as a bottom electrode by pulsed laser deposition (PLD). Xray relationship of BST/LSCO/LAO was [001] BST//[001]LSCO//[001] LAO. The atomic force microscope (AFM)revealed a smooth and crackfree surface of BST films on LSCOcoated LAO substrate with the average grain size of 120 nm and the RMS of 1.564 nm for BST films.Pt/BST/LSCO capacitor was fabricated to perform CapacitanceVoltage measurement indicating good insulating characteristics. For epitaxial BST film, the dielectric constant and dielectric loss were determined as 471 and 0.03, respectively. The tunabilty was 79.59% and the leakage current was 2.63×107 A/crm2 under an applied filed of 200 kV/cm. Furthermore, it was found that epitaxial BST (60/40) films demonstrate wellbehaved ferroelectric properties with the remnate polarization of 6.085 μC/cm2 and the coercive field of 72 kV/cm. The different electric properties from bulk BST (60/40)materials with intrinsic paraelectric characteristic are attributed to the interface effects.  相似文献   

14.
Highly crystalline SrRuO3 (SRO) and La0.5Sr0.5CoO3 (LSCO) thin films were deposited on (100) Pt/ MgO by pulsed laser deposition. The films were mainly (001) textured normal to the substrate surface with a high degree of in-plane orientation with respect to the substrate’s major axes. These films were characterized using x-ray diffraction, Rutherford backscattering, four-point probe resistivity measurement, and transmission electron microscopy. The room temperature resistivity for LSCO and SRO films on Pt/MgO was found to be ∼35 and ∼40 μΩ-cm, respectively. An ion beam minimum channeling yield of ∼43% and ∼33% was obtained for LSCO and SRO films, respectively. The interface between Pt and oxide was found to be smooth and free from any interfacial diffusion. This result showed that high-quality low resistivity oxide thin films can be deposited on Pt.  相似文献   

15.
通过飞秒脉冲激光(50 fs,800 nm,1 kHz,2 mJ)沉积技术在n型Si(100)单晶基片上制备了ZnO薄膜.详细研究了基片温度变化以及退火处理对ZnO薄膜的结构、表面形貌及光学性质的影响.X射线衍射(XRD)结果表明,不同温度下(20~350℃)生长的ZnO薄膜具有纤锌矿结构,并且呈c轴择优取向;当基片温度为80℃时,薄膜沿(002)晶面高度择优生长;当基片温度为500℃时薄膜沿(103)晶面择优生长,场发射扫描电子显微镜(FEEM)结果表明薄膜呈纳米晶结构,并观察到了ZnO的六方结构.进一步通过透射光谱的测量讨论了基片温度及退火处理对ZnO薄膜光学透射率的影响,结果表明退火后薄膜的透射率增大.  相似文献   

16.
Epitaxial Ba0.6Sr0.4TiO3 (BST) thin films were deposited on LaAlO3 (LAO) substrates with the conductive metallic oxide La0.5Sr0.5CoO3 (LSCO) film as a bottom electrode by pulsed laser deposition (PLD). X-ray diffraction ~2 and Ф scan showed that the epitaxial relationship of BST/LSCO/LAO was [001] BST//[001] LSCO//[001] LAO. The atomic force microscope (AFM) revealed a smooth and crack-free surface of BST films on LSCO-coated LAO substrate with the average grain size of 120 nm and the RMS of 1.564 nm for BST films. Pt/BST/LSCO capacitor was fabricated to perform CapacitanceVoltage measurement indicating good insulating characteristics. For epitaxial BST film, the dielectric constant and dielectric loss were determined as 471 and 0.03, respectively. The tunabilty was 79.59% and the leakage current was 2.6310-7 A/cm2 under an applied filed of 200 kV/cm. Furthermore, it was found that epitaxial BST (60/40) films demonstrate well-behaved ferroelectric properties with the remnate polarization of 6.085 C/cm2 and the coercive field of 72 kV/cm. The different electric properties from bulk BST (60/40) materials with intrinsic paraelectric characteristic are attributed to the interface effects.  相似文献   

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