Ba~1~-~1~.~5~yLa~ySn~xTi~1~-~xO~3固溶体的合成、结构与性能

用软化学合成方法,在100^oC以下制备了一系列Ba~1~-~1~.~5~yLa~ySn~xTi~1~-~xO~3固溶体纳米粉末,XRD物相分析和d间距-组成图证明,产品为完全互溶取代固溶体.TEM观察,粒子为均匀球形,平均粒径70nm.通过制陶实验,分别测定了该系列固溶体的室温介电常数,结果发现,用化学方法在BaTiO~3中掺入适量锡和镧,引起T~c降低,当x=0.2,y=0.08时,室温介电数高达28000,比BaTiO~3纯相提高20倍.     

低温-低压水热合成Ba1-xSrxTi1-ySnyO3纳米材料及其 结构与性能研究

采用低温-低压水热法,在150℃,0.5MPa以下合成了一系列Ba1-xSrxTi1-ySnyO3固溶体纳米粉末(0≤x≤0.5≤y≤0.4),经XRD物相分析和d-间距-组成图证明,产品为立方晶系的完全互溶取代固溶体,结果符合Vegard定律,TEM形貌观察,粒子为均匀球形,平均粒径80nm。通过制陶实验,分别测定了该系列固溶体的室温介电常数、介电损失以及介电常数随温度的变化。结果发现,用该方法在BaTiO3中掺入适量锶和锡,由于掺杂离子均匀进入母体晶格,引起Tc降低,介电性能改善显著,当x=0.1,y=0.08时,室温介电常数达17000,比BaTiO3纯相提高10倍,而介电损失却降低88%。     

微波反应合成纳米Ba1-xZnxTi1-ySnyO3介电材料及其结构、性能研究

采用微波反应技术,合成了一系列Ba1-xZnxTi1-ySnyO3固溶体纳米粉末（0≤ x≤0.3,0≤y≤0.5),XRD物相分析和d间距一组成图证明,产品为立方晶系的完全 互溶取代固溶体,结果符合Vegard定律。TEM形貌观察,粒子为均匀球形,平均粒 径40nm。通过制陶实验,分别测定了该系列固溶体的室温介电常数、介电损失以及 介电常数随温度的变化,结果发现,采用化学方法在BaTiO3中掺入适量锌和锡,由 于掺杂离子均匀进入母体晶格,引起tc降低,室温介电常数达12000以上,介电损 耗仅为0.007。纳米粉体的烧结温度为1150℃,比传统微米级粉体的烧结温度降低 200－250℃。     

室温固态反应制备纳米Ba1－xSrxTiO3固溶体及其结构与介电性能研究

采用室温固态反应合成了一系列Ba_1－xSr_xTiO₃固溶体纳米粉末(0≤x≤1.0). 经XRD物相分析和d-间距-组成图证明, 产品为立方晶系的完全互溶取代固溶体. TEM形貌观察, 粒子基本为球形, 平均粒径40 nm. 该方法具有产率高, 无需溶剂, 对环境无污染等优点. 通过制陶实验, 分别测定了该系列固溶体的室温介电常数、介电损失以及介电常数随温度的变化. 结果发现, 采用室温固态反应在BaTiO₃中掺入适量锶, 由于掺杂离子均匀进入母体晶格, 引起居里点降低, 室温介电常数达11000以上, 介电损耗由BaTiO₃纯相的0.03 (3%)降为0.008 (0.8%). 纳米粉体的烧结温度为1180 ℃, 比传统微米级粉体的烧结温度降低100～150 ℃.     

Ba1-xSrxMyTi1-yO3(M=Zr, Sn)纳米材料的软化学合成、结构与介电特性

用软化学方法,在１００℃以下合成了一系列Ｂａ_(１－ｘ)Ｓｒ_ｘＭ_ｙＴｉ_(１－ｙ)Ｏ_３固溶体纳米粉末（Ｍ＝Ｚｒ,Ｓｎ,０ ≤ｘ≤０．４,０≤ｙ≤０．３）,经ＸＲＤ物相分析和ｄ－间距－组成图证明,产品为立方晶系的完全互溶取代固溶体,结果符合Ｖｅｇａｒｄ定律．ＴＥＭ形貌观察,粒子为均匀球形,平均粒径７０ｎｍ．通过制陶实验,分别测定了该系列固溶体的室温介电常数以及介电常数随温度的变化．结果发现,用软化学方法在ＢａＴｉＯ_３中掺入适量锶和锆或锡,由于掺杂离子均匀进入母体晶格,引起Ｔｃ降低,介电性能改善显著．当ｘ＝０．２,ｙ＝０．１时,室温介电常数达 １１ ０００,比 ＢａＴｉＯ_３纯相提高 ８倍,而介电损失却下降 ３倍．     

BaZrxTi1-xO3·yLa2O3固溶体的合成、结构与性能

在100℃以下用软化学合成方法制备了一系列BaZrxTi1-xO3·yLa2O3O(0≤x≤0.3,0≤y≤0.04)固溶体纳米粉末.XRD物相分析及d-间隔-组成图证明,产品为完全互溶取代固溶体.从TEM谱图观察,粒子为均匀球形,平均粒径60nm.通过制陶实验对该系列固溶体的介电特性进行了测试,结果表明,采用化学掺杂方法在BaTiO3中掺入适量锆和镧后,样品的室温介电常数可提高20倍.     

室温固态反应制备纳米Ba1－xSrxTiO3固溶体及其结构与介电性能研究

采用室温固态反应合成了一系列Ba_1－xSr_xTiO₃固溶体纳米粉末(0≤x≤1.0). 经XRD物相分析和d-间距-组成图证明, 产品为立方晶系的完全互溶取代固溶体. TEM形貌观察, 粒子基本为球形, 平均粒径40 nm. 该方法具有产率高, 无需溶剂, 对环境无污染等优点. 通过制陶实验, 分别测定了该系列固溶体的室温介电常数、介电损失以及介电常数随温度的变化. 结果发现, 采用室温固态反应在BaTiO₃中掺入适量锶, 由于掺杂离子均匀进入母体晶格, 引起居里点降低, 室温介电常数达11000以上, 介电损耗由BaTiO₃纯相的0.03 (3%)降为0.008 (0.8%). 纳米粉体的烧结温度为1180 ℃, 比传统微米级粉体的烧结温度降低100～150 ℃.     

低温固态反应制备纳米Ba_(1-y)Sr_yTi_(1-x)Zr_xO_3介电材料及性能研究

将TiCl4的水解产物与固体Ba(OH)2按摩尔比1∶1混合,混合物经室温研磨、100℃烘干,得到钛酸钡纳米晶;按相同工艺掺杂,合成了一系列Ba1-ySryTi1-xZrxO3(0x≤0.3,0y≤0.4)固溶体;采用X射线衍射分析了产物的晶体结构,采用透射电镜观察了其形貌;并测定了系列固溶体的室温介电常数、介电损失.结果表明,所制备的Ba1-ySryTi1-xZrxO3为完全互溶取代固溶体,由平均粒径70 nm的球形微粒组成.经低温固态反应掺入适量锆、锶后,BaTi O3的室温介电常数由3 000提高到20 000左右.     

Pb1-xTbxTi1-xMnxO3(O≤x≤0.10)固溶体的合成、结构与表征

用固相反应合成了Pb1-xTbxTi1-xMnxO3(0≤x≤0.10)固溶体,并用X射线粉末衍射进行了表征,室温下其空间群为P4mm.热分析仪测试结果显示,随着Tb和Mn掺杂量的增加,该固溶体的相变温度Tc降低.介电常数在Tc附近出现峰值,表明对应的相变是铁电相变.磁性测量显示,当x=0.08和x=0.10时,Pb1-xTbxTi1-xMnxO3分别在25和29 K附近有顺磁性向反铁磁性的转变.     

Pb_(1-x)Tb_xTi_(1-x)Mn_xO_3(0≤x≤0.10)固溶体的合成、结构与表征(英文)

用固相反应合成了Pb1-xTbxTi1-xMnxO3(0≤x≤0.10)固溶体,并用X射线粉末衍射进行了表征,室温下其空间群为P4mm.热分析仪测试结果显示,随着Tb和Mn掺杂量的增加,该固溶体的相变温度Tc降低.介电常数在Tc附近出现峰值,表明对应的相变是铁电相变.磁性测量显示,当x=0.08和x=0.10时,Pb1-xTbxTi1-xMnxO3分别在25和29 K附近有顺磁性向反铁磁性的转变.     

Synthesis, structure and dielectric properties of Ba1-xSrx My Ti1-yO3 (M = Zr, Sn)

A series of Ba1-xSrxMyTi1-yO3 (M = Zr, Sn, 0≤x≤0.4, 0≤y≤0.3) solid solutions were synthesized with the soft chemical method below 100 ℃. XRD pattern and cell parameters-composition figures of the prepared powder demonstrate that they are completely miscible solid solutions based on BaTiO3. Furthermore, TEM shows that they have a shape of uniform, substantially spherical particles with an average particle size of 70 nm in diameter. The sintered ceramics of the powder doped with Sr2 and Zr4 or Sn4 have dielectric constant eight times higher and dielectric loss thirty per cent lower than those of pure BaTiO3 phase at room temperature.     

Hydrotherrnal synthesis, structure and property of nano-BaTiO3-based dielectric materials

A series of Ba1-xSrxTi1-yZryO3 (0≤x≤0.5, 0≤y≤0.4) and Ba1-xZnxTi1-ySnyO3 (0≤x≤0.3, 0≤y≤0.3) solid solutions were synthesized by Iow-temperature/Iow-pressure hydrothermal method below 170℃, 0.8 MPa. XRD pattern and cell parameters-composition figures of these prepared powders demonstrated that they are completely miscible solid solutions based on BaTiO3. Furthermore, TEM showed that they have a shape of uniform, substantially spherical particles with an average particle size of 70 nm in diameter. The sintered ceramics of those powders doped by Sr2+ and Zr4+ or Zn2+ and Sn4+ have dielectric constant twelve times higher than and dielectric loss 1/6 those of pure BaTiO3 phase at room temperature.     

Hydrothermal synthesis, structure and property of nano-BaTiO3-based dielectric materials

A series of Ba_1-xSr_xTi_1-yZr_yO₃ (0≤x≤0.5, 0≤y≤0.4) and BA_1?xZn_xTi_1?ySn_yO₃ (0≤x≤0.3, 0≤y≤0.3) solid solutions were synthesized by low-temperature/low-pressure hydrothermal method below 170°C, 0.8 MPa. XRD pattern and cell parameters-composition figures of these prepared powders demonstrated that they are completely miscible solid solutions based on BaTiO₃. Furthermore, TEM showed that they have a shape of uniform, substantially spherical particles with an average particle size of 70 nm in diameter. The sintered ceramics of those powders doped by Sr²⁺ and Zr⁴⁺ or Zn²⁺ and Sn⁴⁺ have dielectric constant twelve times higher than and dielectric loss 1/6 those of pure BaTiO₃ phase at room temperature.     

Synthesis, structure and dielectric properties of Ba1-xSrxMyTi1-yO3 (M = Zr, Sn)

A series of Ba_1-xSr_xM_yTi_1-yO₃ (M = Zr, Sn, 0?x?0.4, 0?y?0.3) solid solutions were synthesized with the soft chemical method below 100 °C. XRD pattern and cell parameters-composition figures of the prepared powder demonstrate that they are completely miscible solid solutions based on BaTiO₃. Furthermore, TEM shows that they have a shape of uniform, substantially spherical particles with an average particle size of 70 nm in diameter. The sintered ceramics of the powder doped with Sr²+and Zr⁴⁺ or Sn⁴⁺ have dielectric constant eight times higher and dielectric loss thirty per cent lower than those of pure BaTiO₃ phase at room temperature.     

La~2~-~xSr~xNiO~4~-~λ系列催化剂结构与氨氧化活性的关系

本文报道了La~2~-~xSr~xNiO~4~-~λ(0≤x≤1)系列复合氧化物的固体结构性质和用于氨的氧化制硝酸的催化性能。La~2~-~xSr~xNiO~4~-~λ的晶胞体积V随x的增大而逐渐减小;c轴在x≤0.5前逐渐增大,在x≥0.5后逐渐减小。α轴在x≤0.5前逐渐减小,在x≥0.5后基本保持恒定。在x≤0.5前,La~2~-~xSr~xNiO~4~-~λ中存在氧过剩,在x≥0.5后存在氧缺陷。TPD表明,α氧(吸附在氧缺陷上的氧)在x=0.6时出现极大,β氧(晶格氧)随x增大而逐渐增大。La~2~-~xSr~xNiO~4~-~λ的氧化还原能力,Ni^3^+的量,氨氧化的NO选择性都随x增大而增加。由此得出,Ni^3^+是催化剂的活性离子,β氧是氨的氧化的活性氧种,在La~2~-~xSr~xNiO~4~-~λ上的氨的氧化遵循氧化还原(Redox)机理。     

Synthesis, structure and dielectric properties of Ba1-xSrxMyTi1-yO3 (M = Zr, Sn)

A series of Ba_1-xSr_xM_yTi_1-yO₃ (M = Zr, Sn, 0⩽x⩽0.4, 0⩽y⩽0.3) solid solutions were synthesized with the soft chemical method below 100 °C. XRD pattern and cell parameters-composition figures of the prepared powder demonstrate that they are completely miscible solid solutions based on BaTiO₃. Furthermore, TEM shows that they have a shape of uniform, substantially spherical particles with an average particle size of 70 nm in diameter. The sintered ceramics of the powder doped with Sr²+and Zr⁴⁺ or Sn⁴⁺ have dielectric constant eight times higher and dielectric loss thirty per cent lower than those of pure BaTiO₃ phase at room temperature.