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环保型BaTiO3基陶瓷介质的掺杂与介电性能的研究

Study of Doping and Dielectric Properties in Lead-Free BaTiO3-based Ceramics

【作者】 李远亮

【导师】 曲远方;

【作者基本信息】 天津大学 , 材料学, 2009, 博士

【摘要】 本文以具有钙钛矿结构的BaTiO3基陶瓷作为研究对象,分别研究了Sm2O3掺杂对(BaxSr1-x)TiO3、Ba(SnxTi1-x)O3和Ba(ZrxTi1-x)O3陶瓷微观结构与介电性能的影响,以及Y2O3和NiO掺杂对(BaxSr1-x)TiO3陶瓷微观结构与介电性能的影响。通过对试样微观结构和介电特性的研究,揭示了Sm2O3、Y2O3和NiO在BaTiO3基陶瓷中的掺杂机理。研究结果发现:Sm2O3和Y2O3在(BaxSr1-x)TiO3陶瓷中,随着掺杂量的增加,Sm3+和Y3+有一个优先取代位置,也就是在它们掺杂的起始阶段,Sm3+和Y3+主要进入晶格A位位置,而在其掺杂量超过某个量之后,则以进入晶格B位位置为主,这种优先取代结果导致试样晶胞参数a随掺杂量的增加先减小后增大,试样介电常数先增大后减小。两者都能使试样介电损耗得到改善,尤其是当Y3+掺杂量为1.0 mol%时,试样介电损耗降低到0.0015。两者掺杂结果的显著不同在于Y3+掺杂使试样表现出了弥散相变特性,而Sm3+掺杂却没有。当NiO被添加到(BaxSr1-x)TiO3陶瓷中时,只有一少部分Ni2+离子进入晶格的B位取代Ti4+离子,导致试样晶格参数轻微增加,之后NiO主要在晶界附近聚集,形成BST/NiO复合材料。试样介电常数随NiO掺杂量的增加而下降,介电温谱显示含Ni试样具有弥散相变特性,且随掺杂量的增加,效果越明显,这也使试样介电温谱得到了很大改善。Sm2O3的加入并不改变BTS10和BZT20陶瓷的主晶相结构,与空白试样相比,掺杂微量Sm3+会使晶粒尺寸下降。随着Sm2O3掺杂量的增加,BTS10和BZT20陶瓷试样介电常数先增大后减小,当试样介电常数最大时,其介电损耗也最高。BTS10和BZT20陶瓷试样Tm和Sm2O3掺杂量之间的变化规律大致相似,不同点在于BTS10陶瓷的Tm在Sm2O3掺杂起始阶段并不改变。掺杂Sm2O3的BTS10和BZT20陶瓷试样均具有弥散相变特性,但二者有两点明显不同,其一,BTS10空白试样本身并不具有弥散相变特性,而BZT20空白试样即具有弥散相变特性。其二,随Sm2O3掺杂量的增加,BTS10陶瓷试样弥散特性一致增强,而BZT20陶瓷试样弥散特性却是先变弱后增强。这种差别说明,在Sm2O3掺杂起始阶段,一部分Sm3+进入了BTS10陶瓷晶格B位位置,而在BZT20陶瓷中却没有,而两者试样Tm在Sm2O3掺杂起始阶段变化的差异性也说明了这一点。

【Abstract】 The effects of Sm2O3, Y2O3 and NiO on microstructure and dielectric properties in BaTiO3-based ceramics are investigated, respectively. Based on the effects of Sm3+, Y3+, and Ni2+ on the microstructure and dielectric properties, the substitution mechanism of Sm3+, Y3+, and Ni2+ in BaTiO3-based ceramics is also investigated and discussed, respectively. The research achievements are as follows:There is an alternation of substitution preference of Sm3+ and Y3+ for the host cations in perovskite lattice, that is, Sm3+ and Y3+ enter the A site in perovskite lattice at first, then they enter the B site when the additive amount of Sm3+ and Y3+ exceed some value. Owing to the substitution preference, the crystal cell a and dielectric constant rise at first, if the amount continues increasing, they will decrease. Both Sm3+ and Y3+ can improve the dissipation factor, especially, the optimized dissipation factor is 0.0015 for 1.0 mol%-Y3+-doped samples, making it a superior candidate material for applications. There is an obvious distinction for the effects on dielectric properties between Sm3+ and Y3+, that is, the Y3+, not Sm3+, makes the BST ceramics exhibit the diffuse phase transition.It is also found that Ni2+ can enter the B site in ABO3 perovskite at first, making the crystal cell a rise, whereafter, Ni2+ ions most segregate on the grain boundaries to inhabit the grain growth, forming the BST/NiO composites. Due to the decrease of grain size and the impurity, the dielectric constants are decreased. It is concluded that the diffuse phase transition is linked to the adulteration of Ni2+, and the diffuse phase transition increases with the doping level increasing, leading to that the peaks of dielectric constants become slower and flatter.The results indicate that the crystal structures are perovskite phase for all of the examined samples in BTS10 and BZT20 ceramics, however, contrasting to the blank sample, the grain size of the sample with Sm2O3 addition is decreased. Owing to the substitution of Sm3+, the dielectric constant rises at first, if the amount continues increasing, it will decrease, in the mean time, the dissipation factor also comes to its maximum when the dielectric constant is the highest. The relation between Tm and the concentration of Sm2O3 has some similarity except that Tm does not move in BTS10 ceramics at first, resulting from a handful of Sm3+ entering into the B site. All of the samples exhibit the diffuse phase transition with Sm2O3 addition, however, there are two obvious distinction among BTS10 and BZT20 ceramics. First, the blank sample of BTS10 has no diffuse phase transition in nature, the samples of BTS10 can exhibit diffuse phase transition only when the Sm3+ ions are added, on the contrary, the blank sample of BZT20 possesses the diffuse phase transition in nature. Second, the diffuse phase transition congruously increases with the level of the Sm3+ doping increasing in BTS10 ceramics, however, the diffuse phase transition lowers in the beginning in BZT20 ceramics, if the amount continues increasing, it will increase, which demonstrated that a handful of Sm3+ ions have entered into the B site in BTS10 ceramics but not in BZT20 ceramics in the beginning, proved by the distinction of the relation between Tm and the concentration of Sm2O3 at first.

【关键词】 陶瓷掺杂介电性能弥散相变
【Key words】 CeramicsDielectric propertiesDopingDiffuse phase transition
  • 【网络出版投稿人】 天津大学
  • 【网络出版年期】2010年 12期
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