铌酸盐 Ba5YTi3 Nb7 O30的结构与介电性能

在BaO-TiO2-Mb2O5体系中通过掺Y3－合成了铌酸盐Ba5YTi3Nb7O30 ,采用粉晶X射线衍射（XRD）对其结构进行了分析,并测试了其烧结体的介电特性,结果表明,在室温下Ba4YT3 Nb7O30属于填满型四方钨青铜结构,晶胞参数,a=1.24332(2)nm,c=0.39453(1)nm,α=β=γ＝90度,Ba5TYi3Nb7O30在100度从铁电相转变为顺电相。     

类钙钛矿新铌酸盐Ba5NdTi2Nb3O18的合成、结构与介电特性

为满足现代通信技术的小型化、集成化与高可靠性的迫切要求,探索具有高介电常数、低介电损耗与低温度系数的微波介电材料引起了材料科学、化学、物理、电子等领域科学工作者的广泛关注,并已开发出复合钙钛矿结构Ba(Zn_(1/3)Ta_(2/3))O_3、钨青铜结     

钽酸盐Ba5YTi3Ta7O30的X射线衍射分析及其介电特性

在BaO -TiO2-Ta2O5 体系中通过掺Y3 +合成了钽酸盐Ba5YTi3Ta7O30,采用粉晶X射线衍射 (XRD)对其结构进行了分析 ,并测试了其陶瓷体的介电特性;结果表明 ,Ba5YTi3Ta7O30 在室温下属于填满型四方钨青铜结构顺电相,晶胞参数为a=1.24387(2)nm,c=0.39178(1)nm ,α= β=γ=90° ;频率为1MHz时Ba5YTi3Ta7O30 陶瓷的室温相对介电常数为155 ;而且介电损耗低至0.0009。     

新铌酸盐Ba5NdTi3Nb7O30的合成与介电性能

The New Niobate Ba₅NdTi₃Nb₇O₃₀ was synthesized by solid state reaction at 1250℃ for 48h. The crystal structure and dielectric properties of Ba₅NdTi₃Nb₇O₃₀ were determined by X-ray powder diffraction and dielectric measurements. The results show that Ba₅NdTi₃Nb₇O₃₀ belongs to ferroelectric phase of tetragonal tungsten bronze structure at room temperature with unit cell parameters: a=1.24424(4)nm, c=0.39476(2)nm, calculated density 5.719g·cm^-3. Ba₅NdTi₃Nb₇O₃₀ belongs to relaxor ferroelectrics. The phase transition temperature (T_c) of Ba₅NdTi₃Nb₇O₃₀ from ferroelectric to paraelectric is found to shift toward higher temperature side at higher fre-quency, and T_c is 90℃ at 1kHz. At room temperature, the dielectric constant (ε_r) and dielectric loss of Ba₅NdTi₃Nb₇O₃₀ decrease with the increase of frequency, and Ba₅NdTi₃Nb₇O₃₀ ceramic have high dielectric constant 489 at 1kHz.     

铌酸盐Ba3NaBiNb10O30的结构与介电特性

一些铁电铌酸盐具有优良的电光性能和非线性光学性能,因此该类化合物的人工合成,结果与性能的研究受到了人们的重视,其中钨青铜结构的系列晶体（例如SBN,KNSBN,SCNN）在材料制备和器件设计方面都取得了很大进展,它们在实时全息存储,集成光学与光信号处理等领域具有广泛的应用前景[1-4],Ba2NaNb5O145(BNN)是目前认为最好的一种倍频晶体,Geusic[5,6]等人报导了在BNN晶体能实现最优位相匹配,可将1．06um红外光以100％的效率转换为0．53um绿光,我们在BaO-Na2O-Nb2O5体系中通过掺杂Bi3 合成了铌酸盐Ba3NaBiNb10O30,并采用粉晶X射线衍射（XRD）对其结构进行了分析,测试了其烧结体的介电特性。     

新铌酸盐Sr5LnTi3Nb7O30的结构与介电性能

在SrO-Ln2O3-TiO2-Nb2O5(Ln=La, Y)体系中,通过固相反应法，合成了填满型钨青铜结构新铌酸盐Sr5LaTi3Nb7O30与Sr5YTi3Nb7O30.分别采用X射线衍射分析、扫描电镜进行了结构分析,并进行了介电性能测试.结果表明, Sr5LaTi3Nb7O30室温时为四方钨青铜结构顺电相,晶胞参数a=1.233 60(4) nm, c=0.388 01(2) nm;频率为1 MHz时,其陶瓷的室温相对介电常数为466,介电损耗约为5×10－3.Sr5YTi3Nb7O30为弛豫性铁电体, 10 kHz时居里温度为260 ℃;室温时为四方钨青铜结构铁电相,晶胞参数a=1.228 80(4) nm, c=0.387 05(2) nm; 1 MHz时,陶瓷体的室温相对介电常数为290.     

钨青铜结构Ba6Zn0.67M9.33O30(M=Nb,Ta)的合成与介电特性

Two compounds Ba₆Zn_0.67M_9.33O₃ and Ba₆Zn_0.67M_9.33O₃₀ with tungsten bronze structure were synthesized in the BaO-ZnO-Nb₂O₅/Ta₂O₅ systems by the conventional high temperature solid-state reaction.The structure and dielectric properties of Ba₆Zn_0.67M_9.33O₃ and Ba₆Zn_0.67M_9.33O₃₀ were determined by X-ray powder diffraction,scanning electron microscope and dielectric measurements.The results show that Ba₆Zn_0.67M_9.33O₃₀ belongs to paraelectric phase of fully filled tetragonal tungsten bronze structure at room temperature with unit cell parameters a:1.26256(4) nm, c:0.39698(2) nm. The room temperature dielectric constant (ε) of Ba₆Zn_0.67M_9.33O₃₀ ceramic reached 108 combined with a low dielectric loss of 0.005 at 1 MHz. While Ba₆Zn_0.67M_9.33O₃ belongs to fully filled tetragonal tungsten bronze structure at room temperature with the unit cell parameters a:1.25940 (3) nm, c=0.40008(2) nm. Ba₆Zn_0.67M_9.33O₃₀ ceramic shows significant relaxor behaviors, and the phase transition from ferroelectric to paraelectric occurred at 55℃ (at 1 MHz). The room temperature dielectric constant (ε) of ceramic reached 570 at 1 MHz.     

铌酸盐Ba_3NaBiNb_(10)O_(30)的结构与介电特性

A niobate was synthesized by doping Bi3＋ in the ternary system BaO Na2O Nb2O5. The crystal structure was determined by X ray powder diffraction,and it belongs to tetragonal tungsten bronze structure at room temperature with unit cell parameters a=1.24777 (2) nm,c=0.39266(1) nm,α =β =γ =90° .Measurements of dielectric properties indicate that phase transitions of Ba3NaBiNb10O30 from paraelectric to ferroelectric occurs at 400℃ ,which is lower than that of Ba2NaNb5O30.     

新铌酸盐Ba3Ni0.33Nb4.67O15的合成与X射线衍射分析

在BaO-Ni2O3-Nb2O5三元系统中,用固相反应法合成了新铌酸盐Ba3Ni0.33Nb4.67O15。以BaCl2和B2O3为主要助熔剂制备了Ba3Ni0.33Nb4.67O15的单晶体。利用四圆单晶衍射仪测定晶胞参数,然后采用X射线粉晶衍射法进行了物相分析,对该化合物的粉晶衍射数据进行了指标化,并报道了其X射线衍射数据。分析结果表明,该化合物属于填满型四方钨青铜结构,空间群P4bm(100),晶胞参数为a=1.26092(5)nm,c=0.40096(4)nm,α=β=γ=90°,Z=2。     

新钽酸盐Ba3TiTa4O15的结构与介电性能

在BaO Ta2O5系统通过掺Ti4＋合成了新钽酸盐Ba3TiTa4O15,用粉晶XRD对其结构进行了分析,并测试了其烧结体的介电特性.结果表明:Ba3TiTa4O15在室温下属于填满型四方钨青铜结构,晶胞参数a=1.256 27(6)nm, c=0.395 86(4)nm; Ba3TiTa4O15在－35 ℃从铁电相转变为顺电相.     

类钙钛矿新铌酸盐Ba6LaTi3Nb3O21的合成、结构与介电特性

A New Niobate Ba₆LaTi₃Nb₃O₂₁ was synthesized by high temperature solid state reaction in the BaO-La₂O₃-TiO₂-Nb₂O₅ system. The chemical compositions, crystal structure, microstructure, density and melting point of the new compound were characterized by EPMA, XRD, DTA and so on. Ba₆LaTi₃Nb₃O₂₁ crystallizes the rhombohedral system with unit cell parameters a=0.57388(2) nm, c=4.928 3(3) nm, and space group R3m, Z=3. The structure may be described as six (Nb,Ti)O₆ octahedra corner-sharing along c-axis to form perovskite layer connected by Ba atoms. The Ba₆LaTi₃Nb₃O₂₁ ceramics exhibits high dielectric of 74.1, low dielectric loss of 4.7×10^-4 and small temperature coefficient of dielectric constant of -69 ppm·K^-1 at 1 MHz due to its close structure and relative high dielectric polarizabilities of Ba²⁺, La³⁺, Ti⁴⁺ and Nb⁴⁺. Ba₆LaTi₃Nb₃O₂₁ might be a suitable candidate of high ε_r microwave dielectric ceramics.     

类钙钛矿新铌酸盐Ba5LaTi2Nb3O18的合成、结构与介电特性

为满足现代通信技术小型化、集成化与高可靠性的迫切要求,探索具有高介电常数、低介电损耗与低温度系数的微波介电材料引起了材料科学、化学、物理和电子科学等领域科学工作者的广泛关注,并已开发出复合钙钛矿结构的Ba(Mg1/3Ta2/3)O3、Ba(Zn1/3Ta2/3)O3和钨青铜结构的Ba6-3xLn8+2x·Ti18O54及Ba2Ti9O20等实用化的高性能材料[1～7].这类材料均由氧八面体共顶连接,而且氧八面体内(B位)、外(A位)阳离子比例等于或略大于1,由此,我们推测在B位与A位阳离子比例略小于1的类钙钛矿结构中也极有可能存在具有优良介电性能的新材料,因此对通式为AnBn-1O3n(n=5,6,7,8)的系列新化合物进行了系统的合成、结构与介电性能研究[8,9].本文报道在BaO-La2O3-TiO2-Nb2O5体系中合成的具有5层类钙钛矿结构的新铌酸盐Ba5LaTi2Nb3O18,发现该材料具有较好的介电性能.