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1.
湿法流延制备(Na,K)0.5Bi0.5TiO3织构陶瓷   总被引:1,自引:0,他引:1  
以NaCl-KCl熔盐法合成的片状Bi4Ti3O12微晶为模板,采用反应模板生长技术(RTGG)和湿法流延工艺制备了织构度为0.70的(Na0.84K0.16)0.5Bi0.5TiO3(NBT-KBT)织构陶瓷。研究了烧结温度对NBT-KBT织构陶瓷的相对密度、微观结构、织构度与电性能的影响。结果表明:其晶粒生长方向与电性能均表现出明显的各向异性,最佳烧结温度为1150℃,在此温度下陶瓷的d33最大为124pC/N,Pr为7.1×10–5C/cm2,Ec为3771kV/m。  相似文献   

2.
采用片状形貌的Sr3Ti2O7为模板籽晶,通过模板晶粒生长法(TGG)结合流延叠层烧结技术制备出晶粒择优取向的Sr3Ti2O7织构陶瓷,研究了还原气氛退火处理对于Sr3Ti2O7织构陶瓷微观组织结构的影响规律。结果表明,在1 500℃不同保温时间下制备的陶瓷主晶相均为Sr3Ti2O7,且有沿(00l)面择优取向晶粒形貌,其织构度随保温时间的延长呈增大趋势;将Sr3Ti2O7织构陶瓷在Ar气中退火处理后陶瓷中发生了相变,生成了新相Sr2TiO4,且Sr2TiO4含量随退火温度升高和退火时间延长而减少;退火处理后陶瓷的织构度减小;平行和垂直流延方向上介电常数存在各向异性,且退火处理后介电常数减小。  相似文献   

3.
以熔盐法制备的BaBi4Ti4O15片状粉体作为模板,流延法制备了BaBi4Ti4O15压电陶瓷,并与传统固相法制备的BaBi4Ti4O15压电陶瓷进行比较。通过XRD分析不同工艺制备的陶瓷样品相结构,SEM观察其微观形貌。结果表明:流延法制备的BaBi4Ti4O15陶瓷在(00l)方向实现了定向排列,且随着模板含量的增加,(00l)晶面的定向度f增加,模板质量分数为20%时,f=57.7%。另外,流延法制得的BaBi4Ti4O15陶瓷样品容易致密,当烧结温度从1 140℃到1 145℃时,密度由5.39 g.cm–3增大到6.64 g.cm–3,在1 150℃达到最大密度7.39 g.cm–3。  相似文献   

4.
以聚丙烯酸酯乳液为粘合剂,采用水基流延成型制备了镍电极多层陶瓷电容器(Ni-MLCC)。利用扫描电子显微镜对膜片表面形貌进行了分析,研究了该水性粘合剂对Ni-MLCC陶瓷浆料黏度、膜片拉伸强度以及所制电容器的电性能的影响。结果表明:粘合剂的用量以质量分数10%为最佳,流延成型所得膜片表面光滑,无缺陷,瓷粉分散均匀,所制备电容器的各项电性能符合EIA-Y5V规范。  相似文献   

5.
用熔盐法制备了片状 Bi4Ti3O12模板,由 Bi4Ti3O12片状前驱体制备了 Bi0.5Na0.5TiO3(BNT)模板,由模板晶粒生长法制备了织构化0.91Bi0.5Na0.5TiO3-0.06BaTiO3-0.03K0.5Na0.5NbO3陶瓷。研究了 Bi4Ti3O12以及Bi0.5Na0.5TiO3两种模板及模板含量对Bi0.5Na0.5TiO3无铅压电体系织构化的影响及织构化陶瓷的压电性能。结果表明Bi0.5Na0.5TiO3模板比Bi4Ti3O12模板更适合用于此体系的织构化,并且,在加入质量分数15%的Bi0.5Na0.5TiO3模板时 Bi0.5Na0.5TiO3陶瓷取向度达到87.3%。质量分数5%的 BNT 模板织构化的陶瓷在6×103 V/mm 电场下应变达到0.226%,相较于随机取向陶瓷提高了48.7%。  相似文献   

6.
采用流延和轧膜成型两种工艺制作了尺寸为38.1mm×38.1mm×0.15mm,介电常数为25000左右的单层微波电容用陶瓷介质基片。系统对比了两种不同成型工艺对该基片的显微结构和电阻性能的影响规律。实验结果表明.轧膜成型制备出的电容器样品的绝缘电阻偏压特性和温度特性均优于流延成型工艺制得的样品,而且在各个温度下的介电损耗低于流延成型工艺制得的样品。不同的陶瓷基片表面扫描电镜图显示,流延成型的陶瓷介质表面粗糙多孔,而轧膜成型的陶瓷介质表面致密紧实。  相似文献   

7.
以片状NaNbO3为籽晶模板,采用反应模板晶粒生长法制备了K0.48 Na0.52 NbO3-LiTa0.5 Nb0.5 O3(KNN-LTN)基无铅压电织构陶瓷,研究了保温时间对陶瓷显微组织结构、织构度和电性能的影响规律,结果表明,织构陶瓷由钙钛矿相和钨青铜结构的K3Li2Nb5O15相组成,随着保温时间的增加,陶瓷的织构度逐渐增大,保温10 h时织构度最大(0.725);织构陶瓷的介电常数随着保温时间的增加而增大,介电损耗则随之增加而减小.与传统的自由取向的KNN-LTN基陶瓷相比,织构陶瓷的压电常数d33提高,并随着保温时间的增加而增大.  相似文献   

8.
采用反应模板晶粒生长法(RTGG),制备了0.94Na0.5Bi0.5TiO3-0.06 BaTiO3无铅压电织构陶瓷,应用晶粒生长动力学唯象理论研究籽晶模板Bi2.5Na3.5Nb5O18对织构陶瓷中取向长条晶生长的影响规律,确定了长条晶生长动力学指数和激活能,探讨了籽晶含量对无铅压电织构陶瓷长条晶生长的作用机理。结果表明:籽晶含量在10%~30%(质量分数)时,随着其含量的增加,晶粒生长指数n约为2,变化不大,说明长条晶粒生长机制主要是界面反应机制。  相似文献   

9.
水基流延制备片式PTCR陶瓷的研究   总被引:1,自引:0,他引:1  
采用sol-gel法制备纳米BaTiO3基PTCR粉体,并以其为原料,采用水基流延成型工艺制备片式PTCR。研究了在sol-gel法制备BaTiO3粉体中,施受主元素含量、陶瓷的烧成温度与PTC效应、晶粒尺寸的关系以及水基流延工艺中各种添加剂对浆料和膜片性能的影响。结果表明:以纳米BaTiO3粉体为原料、水基流延的片式PTCR坯片,在1240℃下就能半导化,所得陶瓷样品的升阻比高于104,温度系数大于13%℃–1,平均晶粒尺寸小于2μm。  相似文献   

10.
以苯丙乳液为粘结剂,聚丙烯酸(PAA)为分散剂,丙三醇为增塑剂,去离子水为分散介质,对添加烧结助剂B2O3-CuO-LiCO3(BCL)的(Ca0.9375Sr0.0625)0.3(Li0.5Sm0.5)0.7TiO3(CSLST)微波介质陶瓷粉体进行了水基流延成型工艺的研究。通过研究各种添加剂含量对浆料流变性能的影响,得出了适合流延的浆料配方(质量分数)为:陶瓷粉料50%,分散剂1%,粘结剂10%,增塑剂与粘结剂质量比为1:4。该浆料呈剪切变稀特性,经流延可制备均匀无裂纹的流延膜片。膜片叠层后在900℃下烧结具有较佳的微波介电性能:εr=75.8,Q×f=1 422 GHz,τf=13.39×10–6/℃。  相似文献   

11.
12.
北京中青联迪科技发展有限公司是团中央直属单位中青高新技术产业发展中心发起组建的高新技术企业,公司是3COM公司防火墙中国区独家总代理。 1.纯硬件设备、采用专业操作系统,高安全性、高性价比,获得国际国内多种认证。 2.操作方便简单,即插即用,全部采用Web图形管理界面,可以在3分钟内完成安装配置。  相似文献   

13.
给出了一种基于2的补码的卷积运算算法及其硬件实现体系结构。该算法结构使用了一个特殊的移位累加单元代替并行补码乘法,降低了卷积系数为负数时的计算复杂度。  相似文献   

14.
采用激光诱导荧光技术对InCl分子B3П1→X1∑+荧光光谱进行了分析和归属,并对 B3П1(v′=0)→X1∑+(v″=0)的时间分辨谱进行了观测.首次得到InCl分子B3П1态(v′= 0)无碰撞辐射寿命т0≈353ns,无辐射弛豫速率常数kQ≈1.985×10-10cm3molec-1s-1及 电子跃迁矩|Re|2=0.40D2.  相似文献   

15.
Planar CH3NH3PbI3 perovskite based photodetectors are fabricated by a facile and low-cost one-step method. The devices show broad spectral photoresponse from the ultraviolet to whole visible region and the performance can be significantly improved by the introduction of a bipolar transporting MoO3 interface layer between CH3NH3PbI3 film and Au electrode. The photocurrent of the device with an optimized MoO3 layer is about twice that of the reference device without MoO3 layer, which results in a high ON/OFF current ratio of 5.9 × 103 at 5 V. Besides, slightly increased photoresponse speed is also found in the optimized device with rise time and decay time of 21.6 and 9.9 ms, respectively. The improvement can be attributed to the improved hole and electron collection efficiency and the quickly filled in or emptied trap states at the CH3NH3PbI3/Au interface due to the introduction of the bipolar transporting MoO3 layer.  相似文献   

16.
Researchers have recently revealed that hybrid lead halide perovskites exhibit ferroelectricity, which is often associated with other physical characteristics, such as a large nonlinear optical response. In this work, the nonlinear optical properties of single crystal inorganic–organic hybrid perovskite CH3NH3PbBr3 are studied. By exciting the material with a 1044 nm laser, strong two‐photon absorption‐induced photoluminescence in the green spectral region is observed. Using the transmission open‐aperture Z‐scan technique, the values of the two‐photon absorption coefficient are observed to be 8.5 cm GW?1, which is much higher than that of standard two‐photon absorbing materials that are industrially used in nonlinear optical applications, such as lithium niobate (LiNbO3), LiTaO3, KTiOPO4, and KH2PO4. Such a strong two‐photon absorption effect in CH3NH3PbBr3 can be used to modulate the spectral and spatial profiles of laser pulses, as well as to reduce noise, and can be used to strongly control the intensity of incident light. In this study, the superior optical limiting, pulse reshaping, and stabilization properties of CH3NH3PbBr3 are demonstrated, opening new applications for perovskites in nonlinear optics.  相似文献   

17.
Without adding feedback to modulate light path system, the dissymmetrical 3×3 coupled optical accelerometer reduces the complexity of the design of light path system. Experiments prove that it can attain good demodulation effects. As carrier is not needed in this system, the frequency range of input signal is diminished so as to decrease the sampling frequency of accelerometer. This makes for the system on programmable chip(SOPC) design of digital demodulating system. The upper limit of accelerometer working frequency can reach 3 500 Hz. But affected by the inherent frequency of sensitive components, its working frequency is 10 Hz~1 000 Hz, and the sensitivity is 8.718 0 V/(m·s-2). This accelerometer can detect the dynamic range of acceleration signal real-timely, steadily and accurately, solving the dissymmetrical problem of light path caused by circumstances and the complexity of process.  相似文献   

18.
采用固相反应法制备了Bi 3+ 、Eu3+ 、Tb3+ 掺杂的Lu3TaO7。测量了样品的X射线衍射谱、激发和发射光谱及荧光衰减曲线。三种离子掺杂的Lu3TaO7均呈现出强的荧光发射,其中Bi3+具有峰位在431 nm处的一强发射宽带,衰减寿命为16.8 μs,Eu 3+ 、Tb 3+ 则表现出稀土离子的特征锐发射峰,衰减寿命分别为1.26 ms和1.20 ms。因此,它们均是具有潜在应用前景的重闪烁体材料。  相似文献   

19.
Without adding feedback to modulate light path system, the dissymmetrical 3×3 coupled optical accelerometer reduces the complexity of the design of light path system. Experiments prove that it can attain good demodulation effects. As carrier is not needed in this system, the frequency range of input signal is diminished so as to decrease the sampling frequency of accelerometer. This makes for the system on programmable chip(SOPC) design of digital demodulating system. The upper limit of accelerometer working frequency can reach 3 500 Hz. But affected by the inherent frequency of sensitive components, its working frequency is 10 Hz~1 000 Hz, and the sensitivity is 8.718 0 V/(m·s-2). This accelerometer can detect the dynamic range of acceleration signal real-timely, steadily and accurately, solving the dissymmetrical problem of light path caused by circumstances and the complexity of process.  相似文献   

20.
Er3 /Yb3 共掺TeO2-WO3-Bi2O3玻璃的光谱性质   总被引:5,自引:4,他引:1  
用高温熔融法制备了Er3+/Yb3+共掺的TeO2-WO3-Bi2O3玻璃,研究了该玻璃的吸收和荧光光谱性质.应用Judd-Ofelt(JO)理论计算了Er3+的谱线强度、自发辐射跃迁几率、荧光分支比和辐射寿命等光谱参数,并拟合了相应的强度参数Ωt(t=2,4,6).Er3+在该玻璃中4I13/2→4I15/2发射的荧光半高宽(FWHM)为77nm,应用McCumber理论计算的受激发射截面为1.03×10-20cm2.其带宽特性FWHM×σpeake乘积优于掺Er3+的硅酸盐、磷酸盐和铋酸盐玻璃,说明这是一种制备宽带光纤放大器的优良基质材料.Er3+在400~850nm波长范围存在着5个上转换发射峰,分别对应Er3+的激发态4I7/2、2H11/2、4S3/2、4F9/2和4I9/2到基态4I15/2的发射,分析了其可能存在的上转换过程.  相似文献   

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