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用Sol—Gel法制备PZT铁电陶瓷及薄膜 总被引:3,自引:0,他引:3
用Sol-Gel法制备了Pb(Zr0.5Ti0.5)O3(PZT)铁电陶瓷与薄膜,观察了它们的结晶情况并测定了它们的电学性能。利用Sol-Gel法,可降低PZT陶瓷粉料的预烧温度约200℃,所得陶瓷致密,晶粒均匀;具有较好的介电性能。PZT陶瓷显示弥散相变特征,PZT薄膜的晶化受基底影响很大,基底晶格越完整,与PZT薄膜的晶格失配率越小,PZT薄膜的晶化就越。采用PbTiO3过渡层促进PZT薄膜在镀铂硅片上晶化。PbTiO3过渡层与PZT薄膜的串联电路,其表观电学性能与相应的PZT体材料相近。 相似文献
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利用固相反应制备的ZnO-Li_(2.2%)陶瓷靶和RF射频磁控溅射技术在Si(100)基片上制备了高度c轴择优取向的ZnO薄膜,XRD和电性能分析表明掺杂Li离子改善了ZnO靶材的结构和性能,同时研究了不同RF溅射温度对ZnO薄膜结构与取向的影响;然后采用sol-gel前驱单体薄膜制备方法,以ZnO为过渡层淀积PZT薄膜,探讨高度c轴(002)择优取向ZnO薄膜对PZT薄膜结构与性能的影响,实验发现在PZT/ZnO异质结构中,致密、均匀和高度c轴择优取向的ZnO可作为晶核,促进PZT钙钛矿结构转化、晶粒(110)择优取向生长,相应降低PZT薄膜的退火温度. 相似文献
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利用Sol-gel工艺在Pt/Ti/SiO2/Si衬底上制备了Pb(Zr0.53Ti0.47)O3(PZT)薄膜,研究了退火温度、保温时间和薄膜厚度对其晶相、微观结构和铁电性能的影响.在500℃退火处理的PZT薄膜开始形成钙钛矿相;在550℃退火处理的PZT薄膜基本形成钙钛矿相结构;升高退火温度(500~850℃)、延长保温时间(30~150min)、增加薄膜厚度(120~630nm)都有利于PZT晶粒的长大.在650~750℃退火的PZT薄膜具有较好的铁电性能,保温时间对PZT薄膜的铁电性能影响不大,PZT薄膜的厚度为200~300nm时可以得到比较好的铁电性能.在退火温度750℃、保温时间30min条件下退火处理厚310nm的PZT薄膜,其剩余极化值(2Pr)和矫顽电场(2Ec)分别是72μC/cm2、158kV/cm. 相似文献
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采用添加造孔剂的方法制备多孔锆钛酸铅(PZT95/5)铁电陶瓷, 研究了孔结构包括孔隙率、孔径及孔形状对多孔PZT95/5陶瓷机械性能和电性能的影响及机理, 并揭示多孔PZT95/5陶瓷微观结构、机械性能和铁电性能的内在联系。研究表明: 孔隙率的增加降低了多孔PZT95/5陶瓷的声阻抗, 改善了陶瓷与封装材料的声阻抗匹配. 孔隙率增加, 多孔PZT95/5陶瓷的屈服应力和剩余极化强度降低, 矫顽场强增大。孔结构对多孔PZT95/5陶瓷屈服应力的影响可由应力集中理论解释; 多孔PZT95/5陶瓷剩余极化强度随孔结构的变化可用内应力结合空间电荷理论加以解释。 相似文献
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采用溶胶-凝胶和射频磁控溅射相结合的方法制备了PZT铁电薄膜.用溶胶-凝胶法制备一层PZT薄膜作为籽晶层,在衬底PZT(seed layer)/Pt/Ti/SiO2/Si上用射频磁控溅射过量10%Pb的Pb(ZrxTi1-x)O3(x=0.3)陶瓷靶生长厚500nm的PZT铁电薄膜.采用在450℃预退火,575℃后退火的快速分级退火方法对PZT铁电薄膜进行热处理.PZT铁电薄膜获得了较好的热释电性能,热释电系数、介电常数、介电损耗和探测度优值因子分别为P=2.3×10-8C·cm-2·K-1,ε=500,tanδ=0.02,Fd=0.94×10-5Pa-0.5. 相似文献
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MgO·nAl2O3透明陶瓷的制备及其物性 总被引:4,自引:0,他引:4
制备了非化学配比(n=1~2)的透明多晶MgO·nAl2O3陶瓷,研究了光学性质和力学性质与其物相和微观结构的关系.结果表明:非配比MgO·nAl2O3陶瓷主相的晶界处有Al2O3晶粒析出,其数量随着配比n的增大而增加.n=1~1.5的非配比透明陶瓷在紫外-可见波段与化学配比透明陶瓷一样具有较高的光学透过率,而n≥1.8陶瓷的透过率由于较多的第二相物质所引起的散射而有明显的下降.由于尖晶石晶粒性能改变和Al2O3晶粒的能量耗散等因素,非配比陶瓷的硬度和抗弯强度均比化学配比的高.过多的析出相引起的弱界面和缺陷裂纹可能导致陶瓷强度的下降,表现在其抗弯强度随着n的增大呈现先提高而后下降的变化规律. 相似文献
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目前,对磁控溅射组装Cu-W均质复合膜的工艺及成膜机理研究不够深入。通过磁控溅射组装均质Cu-W薄膜,考察了溅射工艺参数对膜结构的影响。结果表明:直流磁控溅射组装均质Cu-W薄膜时,钨是以β-钨为骨架固溶进部分铜的方式存在;随铜靶功率的增加,铜的晶粒尺寸先变大后变小;随钨靶功率的增大,β-钨有向非晶态转变的趋势,且铜的晶粒尺寸会明显变小;薄膜的沉积速率主要由钨靶功率决定;工作气体氩气气压低于1.0 Pa时,随气压升高,铜的晶粒尺寸变小,高于1.0 Pa时,气压对薄膜结构没有影响。 相似文献
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长时高温作用会显著加速压电陶瓷元件电学性能的退化,极大地影响压电元件使用寿命。本工作在85、125和150℃下对PZT压电陶瓷元件进行长时老化处理,研究并分析了高温老化过程中PZT陶瓷元件电学性能退化规律及其微观机制。压电常数与介电常数随老化周期延长均退化明显,初期退化速率较慢,后期退化加快并逐渐趋于稳定,介电常数和压电常数退化均符合Boltzmann变化规律。85℃和125℃下老化49 d时,元件介电常数退化率达到最大,分别为31.01%和36.48%;压电常数退化率达到最大,分别为11.57%和19.02%。PZT压电元件介电性能退化主要由表面Ag电极内结构退化、Ag/PZT界面弱化及PZT陶瓷退极化三方面所贡献,其中界面弱化和陶瓷退极化占主导。长时高温作用促使Ag电极逐渐缓慢氧化生成Ag2S,晶粒收缩产生大量孔洞,导致Ag电极致密度下降和Ag/PZT界面分层,降低了Ag/PZT的电容率;此外,长时高温作用加速了PZT陶瓷电畴转向无序状态,促进氧空位位移钉扎电畴壁,导致了PZT压电元件介电性能退化。 相似文献
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潜艇目标尺度模拟研究是水中目标特性研究的一个重要课题。本文结合潜艇目标回波特性及探(反)潜设备目标尺度识别方法,提出了潜艇目标尺度模拟特征模型,并建立硬件系统予以实现取得了满意的湖上试验结果。 相似文献
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A. Yoshida Y. YanagisawaT. Kubo 《Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment》2011,655(1):10-16
Since 2007, a water-cooled high-power rotating disk target has been in operation at the in-flight radioactive-isotope beam separator (BigRIPS), RIKEN. The target should withstand a goal beam intensity of 1 particle μA (pμA) 238U-beam at 350 AMeV with a spot size of 1 mm in diameter, resulting in a heat deposit of 22 kW in the target.A beam-spot temperature monitoring system using infrared devices in high-radiation environment was elaborately developed. The beam-spot temperature on a beryllium (Be) fixed target and on a rotating Be and tungsten (W) disk target was measured with the most intense beams presently available at our facility. The heat deposit achieved was 0.6 kW, that is 1/37 of the goal value. At the present beam intensity, the result supports our estimation that a water-cooled rotating disk target of 30 cm diameter can withstand an approximately tenfold beam intensity compared to a water-cooled fixed target. 相似文献
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A. Yoshida T. Suda T. Ohtsuki H. Yuki T. Kubo 《Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment》2008,590(1-3):204
A water-cooled high-power rotating disk target is employed at the in-flight radioactive-isotope (RI) beam separator (BigRIPS), RIKEN. For a 238U primary beam with energy of 350 A MeV and an intensity of 1 particle μA bombarding a beryllium or carbon target disk with a 1 g/cm2 thickness, a total heat loss of 28 GW/m2 on the target surface is estimated for a beam-spot size of 1 mm in diameter.For the development of a suitable target assembly, a test bench was constructed and has been used for the present RI beam separator (RIPS). A beam spot temperature monitor using an infrared thermo-viewer with telescope lens was developed. The measured temperature for some high-power beam experiments corresponded to results of computer simulations. A radiation hardness test of the magnetic fluid used for a vacuum-tight rotating actuator was performed by irradiating with intense γ-ray converted from an electron beam. No significant change of viscosity was observed up to the total dose of 0.7–1.8 MGy.Based on these studies, a practical target system for the BigRIPS separator was designed. To facilitate the maintenance of the target system in a high-radiation environment, a remote-handling maintenance cart system is considered. 相似文献
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铝掺杂氧化锌(AZO)废弃靶材回收再利用的研究 总被引:1,自引:1,他引:0
将AZO原料粉末和AZO残靶研磨后的粉末混合,采用注浆成型和常压大气烧结工艺制备靶材,实验主要测试了相对密度、吸水率、线收缩率和电阻率等性能,并通过XRD和SEM表征AZO靶材的晶体形态和微观结构,与新靶材进行性能对比,研究残靶粉末回收利用对靶材性能的影响。残靶粉末的加入对AZO靶材有轻微影响,测试结果显示烧结温度1450℃、保温5h、AZO残靶加入量为10%时有较好的性能:相对密度高达99.24%,吸水率和收缩率分别为17.96%和15.70%,电阻率为2.12×10-3Ω·cm。含有残靶的AZO靶材稍差的性能可能归结于AZO粉末和残靶粉末的兼容性。 相似文献
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A. Vascon Ch.E. Düllmann K. EberhardtB. Kindler B. LommelJ. Runke 《Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment》2011,655(1):72-79
TRAKULA (Transmutationsrelevante kernphysikalische Untersuchungen langlebiger Aktinide, i.e., nuclear physical investigations of long-lived actinides with relevance to transmutation) is a joint research project of the German Federal Ministry of Science and Education (BMBF) on nuclear physics investigations with modern scientific, technological and numerical methods. Experiments concerning the transmutation of radioactive waste are a central topic of the project. For this, large-area samples (≥40 cm2) of 235,238U and 239,242Pu compounds are required for the calibration of fission chambers and for fission yield measurements. Another topic within the project requires large-area targets for precise measurements of the half-life, t1/2, of very long-lived α-particle emitters like 144Nd (t1/2≈2×1015 y). Here, we report on electrodeposition tests with Gd and Nd (used as chemical homologs of the actinides), which were performed to find optimal deposition conditions for small-area targets that should be applicable to future large-area targets.The layers were produced by molecular plating. A new stirring technique, ultrasonic stirring, was adopted and found to be suitable for producing large-area targets. Moreover, two different current densities (namely 0.7 and 1.4 mA/cm2) were studied and found appropriate for target preparation. Characterization of the layers with different analytical techniques played a major role in these studies to gain a deeper understanding of the deposition process itself: neutron activation analysis and γ-spectroscopy were used for yield measurements, radiographic imaging for homogeneity studies, scanning electron microscopy for morphology studies, and atomic force microscopy for roughness studies. According to the obtained results, a new electrochemical cell for the production of large-area targets was designed. 相似文献