0.74Pb(Mg_(1/3)Nb_(2/3))O_3-0.26PbTiO_3薄膜的光学性能研究

采用磁控溅射法,选用LaNiO3(LNO)作为缓冲层和电极层,在硅基片上成功地制备出了0.74Pb(Mg1/3Nb2/3)O3-0.26PbTiO3(PMN-0.26PT)铁电薄膜.X射线衍射(XRD)分析表明薄膜具有沿(110)方向择优取向的钙钛矿结构.利用NKD光谱测试仪测试了薄膜的反射谱,并使用最小二乘法进行拟合分析得到其折射率和消光系数.在沉积温度为500℃时,薄膜具有更为均匀和致密的微观结构.在波长为633 nm时,该薄膜的折射率大小为2.41.薄膜的折射率和消光系数随着光子能量的增加而增加.薄膜的这些光学特性使其有望在低压电光转换器、光波导等器件中应用.     

Pb(Mg_(1/3)Nb_(2/3))O_3-PbTiO_3-BaTiO_3 Complex Perovskite Ferroelectric Ceramics with High Dielectric Constant and Low Firing Temperature

The effects of different firing temperatures on the stability of perovskitC phase, grain size, and die-lectric propertes were investigated by XRD, TEM, SEM and dielectric measurements. The dielectric ceramicsof Pb (Mg_(1/3)Nb_(2/3))O_3-Pb TiO_3-BaTiO_3 system were obtaine d by chemical coprecipitation in water The ceramicshave higher dielectric constan (7003-9714), lower firing temperature (950-1150℃), quite uniform micro-structrue with grain size less than 2.5 μm, and lower temperature coefficiens of capacitance. As a result, it wasconfirmed that the simple and low cost chemical route used namely coprecipitation in water is a desired meth-od for preparin high property dielectric materials applicable to multilayer capacitors.     

Pb（Cd_（1／2）Te_（1／2））O_3及三元系压电陶瓷Pb（Cd_（1／

研制了一种新的三元系统压电陶瓷材料Ｐｂ（Ｃｄ１／２Ｔｅ１／２）Ｏ３－ＰｂＺｒＯ３－ＰｂＴｉＯ３，本系统材料压电性强，时间稳定性极佳，其时间稳定性比改性的ＰＣＭ提高一个数量级，作者认为稳定性的提高原因，不是由于材料的“软化”，而在于Ｔｅ６＋离子在电畴界面的偏聚对畴壁的“钉扎”作用，确定了Ｐｂ（Ｃｄ１／２Ｔｅ１／２）Ｏ３是顺电相其含量以４～６ｍｏｌ％为宜，部分Ｃｄ２－取代，使本系统材料“硬化”．     

弛豫铁电单晶铌镁酸铅-钛酸铅的工程畴结构研究

综述了目前对铁电晶体畴结构进行观测的主要技术方法,及国内外相关研究单位对新型弛豫铁电单晶铌镁酸铅-钛酸铅[(1-x)Pb(Mg1/3Nb2/3)O3-xPbTiO3(PMN-xPT)]的工程畴结构的研究进展。以往的研究表明,该类单晶的机电性能与其工程畴结构之间存在着密不可分的关系,这些研究结果对阐明PMN-xPT单晶在不同极化方向与工程畴结构状态下,其优异机电性能的起源机制与发生规律,进而指导剪切波换能器、垂直极化方向的大应变驱动器等电机器件的设计与制作,具有重要的理论意义与实际应用价值。     

（1-x）Pb（Sc1／2Ta1／2）O3-xPbTiO3陶瓷的结晶特性与介电性能研究

在钽钪酸铅中加入钛酸铅,形成具有复合钙钛矿结构的钽钪酸铅 钛酸铅固溶体(1-x)Pb(Sc1/2Ta1/2)O3 xPbTiO3(简称PSTT(x)),可有效提高钽钪酸铅材料体系的居里点、降低其制备温度,从而扩大PST体系的应用范围.用常规氧化物合成电子陶瓷方法制备了钽钪酸铅 钛酸铅弛豫铁电陶瓷,采用XRD,SEM等分析技术,研究了PSTT(x)陶瓷的结晶特性和微观形貌,测试了PSTT(x)陶瓷的介电性能.实验结果表明,利用常规氧化物合成电子陶瓷方法可以合成钙钛矿结构的PSTT(x)陶瓷,其钙钛矿相的含量可达到90%以上,最高达100%.SEM分析表明,PSTT(x)陶瓷的晶粒饱满、晶界清晰.PSTT(x)陶瓷的热滞温度随x的不同,大致在6～12℃之间变化;PSTT(x)陶瓷的居里常数C 为3.7～8.3×106K2.     

Li[Li(1/3-x/3)Mn(2/3-2x/3)Cox]O2(x=O.1)的团簇自旋玻璃态行为

采用柠檬酸盐法制备了六方层状结构的Li[Li(1/3-x/3)Mn(2/3-2x/3)Cox]O2(x=0.1)材料.体系在高温区呈现顺磁态,通过拟合Curie-Weiss定律得到Curie和Weiss常数分别为1.70(2)m3 K/mol和-22(3)K.该材料的磁化率曲线在低温区表现出不可逆转变行为,并且这种不可...     

锂离子电池正极材料Li［CoxLi 1/3-x/3Mn2/3-2x/3］O2的制备与表征

采用柠檬酸盐法合成了Li［Co_xLi _{1/3-x/3}Mn_2/3-2x/3］O₂（x=0.1,0.2,0.3,0.4,0.5）正极材料. 利用X射线衍射(XRD), Raman光谱和红外光谱(FTIR)等方法研究不同质量分数的Co对材料晶体结构的影响, 并分析了原因. 对不同组分的材料进行了电化学性能测试, 结果表明, 当x=0.5时, 样品充放电容量高, 循环性能优良.      

Optimizing the Synthetic Conditions of LiNi_(1/3)Co_(1/3)Mn_(1/3)O_2 from a Carbonate Co-precipitation Method

1 Introduction As a promising cathode material for lithium ion batteries,LiNi1/3Co1/3Mn1/3O2 attracted intensive attentions.Owing to high specific capacity,long circle life and excellent safety,it may be an alternative candidate for LiCoO2.As a complex composite,however,it is difficult to synthesize phase-pure LiNi1/3Co1/3Mn1/3O2 by a simple mixed calcination method[1].From this concern,carbonate co-precipitation method,which can prepare homogeneous LiNi1/3Co1/3Mn1/3O2 with typical layered structure,bec...     

0.05Ba(Cu_(1/2)W_(1/2))O_3-0.95PZT的性能研究

采用固相合成法制备 0 .0 5Ba(Cu1/ 2 W1/ 2 )O3 - 0 .95PZT三元体系压电陶瓷 ,研究了烧结温度对压电陶瓷压电性能的影响 ;通过XRD和SEM测试发现材料仍为钙钛矿结构 ,显微分析表明晶粒之间结合紧密 ,颗粒大小均匀 ;实验结果表明 ,压电陶瓷的压电系数d3 3 为 6 0 5pC/N ,机电耦合系数Kp为 0 .37左右 ,机械品质因数Qm 为 6 0。     

Prop铁电薄膜电容器YBCO/Pb(Ta_(0.05)Zr_( 0.48)Ti_(0.47))O_3/YBCO/Pt/TiO_2/SiO_2/Si的性质(英文)

铁电薄膜有望被应用于“不挥发随机存储器 (NvRAM )” ,在这其中 ,Pb(Zr,Ti)O3(PZT)铁电薄膜由于有较大的剩余极化 ,较小的矫顽场 ,高居里点 ,以及与硅集成的可能性而得到了广泛的研究 .但是 ,由于铁电薄膜与金属电极之间的界面不理想 ,以及铁电薄膜中的晶界角度过高 ,而大大降低了铁电电容器的性能 .最近的研究表明 ,通过用导氧化物作电极 ,可部分的改善电薄膜的疲劳和保持性能 .用脉冲激光沉积法 (PLD) ,以YBa2 Cu3O7(YBCO)为隔离层 ,在Pt/TiO2 /Si(10 0 )衬底上制备Pb(Ta0 .0 5Zr0 .48Ti0 .47)O3(PTZT)铁电薄膜 ;并以YBCO为上下电极做成铁电电容器 .X衍射发现以YBCO为电极的PTZT结晶成完全钙钛矿相 .SEM结果表明PTZT晶粒大约在 180nm左右 ,YBCO/Pt ,Pt/TiO2 界面非常清晰 ,没有发现任何扩散 .在RT6 0 0 0HVS环境下 ,发现在 91kV/cm的外场下反转 1× 10 1 1 次后 ,此电容器的极化P 和P^分别只减少了 2 0 %和 6 % ;在 145kV/cm的读写外场下经过 1× 10 5s后 ,此电容器的极化基本保持不变 ;在过大的外场下 ,此电容器的疲劳特性明显变差 .由于引入YBCO过渡层 ,改善了界面 ,减少了薄膜中氧空位的聚集程度 ,铁电薄膜的疲劳及保持性能得到了极大的改善     

Voltage-controlled Kerr response in Ni/Pb（Zr0.52Ti0.48）O3 heterostructures

Voltage-modified magneto-optical Kerr effect（MOKE） is widely used to describe the converse magnetoelectric（ME） effect in the ferroelectric/ferromagnetic（FE/FM） heterostructures. However, the applied voltage can possibly give rise to electro-optical effect of the FE layer, which would also affect the Kerr signals in the MOKE system. Here, we used an AC voltage to modulate the magnetization in the Ni/Pb（Zr0.52Ti0.48）O3（PZT） heterostructures with different pre-polarization states of the PZT layers to investigate the complexity of the Kerr signals. The results suggested that the voltage control of Kerr signal contained several origins; however, the straininduced ME effect dominated in the ME effect in the heterostructures.     

Microstructure,crystalline phase and electrical properties of Li_(0.06)(Na_(0.5)K_(0.5))_(0.94)Nb_(1-2x/5)Mg_xO_3 lead-free piezoelectric ceramics

MgO-modified Li0.06(Na0.5K0.5)0.94NbO3(L6NKN) lead-free piezoelectric ceramics were synthesized by normal sintering at a relatively low temperature of 1000°C.The crystalline phase,microstructure,and electrical properties of the ceramics were investigated with a special emphasis on the influence of MgO content.The addition of MgO effectively improves the sinterability of the L6NKN ceramics.X-ray diffraction analysis indicates that the morphotropic phase boundary(MPB) separating orthorhombic and tetragonal phases for the ceramics lies in the range of Mg doping content(x) from 0.3at% to 0.7at%.High electrical properties of the piezoelectric constant(d33=238 pC/N),planar electromechanical coupling coefficient(kp=41.5%),relative dielectric constant(εr=905),and remanent polarization(Pr=38.3 μC/cm2) are obtained from the specimen with x=0.5at%,which suggests that the Li0.06(Na0.5K0.5)0.94Nb(1-2x/5)MgxO3(x=0.5at%) ceramic is a promising lead-free piezoelectric material.     

包含式完全正则(T*3(1/2))是相对可乘的

本文讨论包含式完全正则空间（T31/2^＊）关于相对积拓扑的可乘性问题．     

Cd_(0.03)Sr_(0.485)Ba_(0.485)Nb_2O_6单晶的介电和铁电性能

在500Hz 至13MHz 的频率范围内,测量了Cd_(0.03)Sr_(0.485) Ba_(0.485)Nb_2O_6晶体的新鲜试样以及经过强交流电场处理的试样的介电谱。结果表明,新鲜晶体试样中存在低频弛豫机构,经过强的交流电场处理后这一弛豫机构消失,而且晶体的交流电导率也降低一个数量级。我们还研究了偏置电场对介电常数温度依赖性的影响,发现偏置电场使介电常数呈现极大渔的温度Tm向高温方向移动,而且使Tm附近介电常数的值减小。前者可由扬致相变加以解释,后者表示此晶体的铁电-顺电相变可能是二级的。另外,实验结果表明,在本工作的测试范围内,偏置电场对本晶体相变的弥散性没有影响。     

Preparation and radar-absorbing properties of Al_2O_3/TiO_2/Fe_2O_3/Yb_2O_3 composite powder

Al_2O_3/Ti O_2/Fe_2O_3/Yb_2O_3 composite powder was synthesized via the sol–gel method. The structure,morphology,and radar-absorption properties of the composite powder were characterized by transmission electron microscopy,X-ray diffraction analysis and RF impedance analysis. The results show that two types of particles exist in the composite powder. One is irregular flakes(100–200 nm) and the other is spherical Al_2O_3 particles(smaller than 80 nm). Electromagnetic wave attenuation is mostly achieved by dielectric loss. The maximum value of the dissipation factor reaches 0.76(at 15.68 GHz) in the frequency range of 2–18 GHz. The electromagnetic absorption of waves covers 2–18 GHz with the matching thicknesses of 1.5–4.5 mm. The absorption peak shifts to the lower-frequency area with increasing matching thickness. The effective absorption band covers the frequency range of 2.16–9.76 GHz,and the maximum absorption peak reaches-20.18 d B with a matching thickness of 3.5 mm at a frequency of 3.52 GHz.     

钨青铜陶瓷Sr_(0.5)Ba_(0.5)N_2O_6的制备结构与介电性能研究

采用固相反应法合成Sr0.5Ba0.5Nb2O6陶瓷,并对其结构、介电性能进行表征.研究结果表明,Sr0.5Ba0.5Nb2O6陶瓷为四方钨青铜结构单相,其在100℃附近存在一个明显的弥散介电峰,峰值随测试频率增加而减小,为典型的弛豫铁电相变.室温时,10kHz频率下,其介电常数约为450,介电损耗为0.121.     

电脱氧Nb2O5制取金属铌

以Nb2O5粉末烧结片为阴极,以石墨为阳极,在CaC12-NaCl熔盐电解质中对Nb2O5进行电脱氧,获得金属铌.对不同密度的Nb2O5粉末烧结阴极的制取以及烧结阴极密度对电脱氧Nb2O5的影响进行研究.结果表明,阴极片的烧结密度对Nb2O5在CaC12-NaCl熔盐中的电脱氧有着极其重要的影响,烧结密度越低,电解起始电流越大,并且在电脱氧过程中电流也越大;在相同电解时间内,阴极产物中残余氧化物化合价随阴极片密度的降低而降低;Nb2 O5粉末在8 MPa压力下成型,1 150℃下烧结8 h,所得的阴极片具有较好的电化学活性;在850℃下电解150 min,Nb2 O5可完全被还原;电脱氧反应速度会随电解时间的延长而逐渐减慢.实验结果表明,电脱氧是氧化物粉末颗粒与熔盐电解质接触、反应和电离的过程,Nb2O5的电脱氧过程是分步进行的,其中间产物是铌的一系列低价氧化物,即Nb5+→Nb4+→Nb2+→Nb.     

Cd_(0.03)Sr_(0.485)Ba_(0.485)Nb_2O_6单晶及其介电谱

本文报告了f=1KHz到1GHz范围内Cd_(0.03)Sr_(0.485)Ba_(0.485)Nb_2O_6(CdSBN)单晶的新鲜样品,和经交变电场处理后样品的介电谱.实验表明,低频介电弛豫经强交变电场处理后而消失,同时交流电导率也降低.在施加偏置电场后,其介电常数出现极大值的温度T_m向高温方向移动,这可用场致相变加以解释.同时也说明该晶体属于二级相变的特性.又在实验所加的偏置电场范围内,晶体相变的弥散性不产生影响.