Y3+替代Bi3+对Bi2(Zn1/3Nb2/3)2O7陶瓷显微结构和介电性能的影响

本文研究了Y3 替代Bi3 对Bi2O3-ZnO-Nb2O5系介质材料结构和性能的影响,并借助X射线、扫描电镜、LCR4284测试仪对其相结构和介电性能进行分析。研究结果表明,随着Y3 替代量的增加,Bi2O3-ZnO-Nb2O5系介质材料的晶粒尺寸、介电常数、介电损耗都有所变化,当替代量x=0.2时,介电性最佳,介电常数为79.4094,介电损耗为0.002125。     

Er3+替代Bi3+对Bi2(Zn1/3Nb2/3)2O7陶瓷烧结温度的影响

研究了Er3 替代Bi3 对Bi2(Zn1/3Nb2/3)2O7系介质材料结构和性能的影响,并借助X射线、扫描电镜、Agilent4284测试仪对其相结构和介电性能进行分析.研究结果表明:经Er3 替代的BZN陶瓷样品烧结温度升高(从960℃升高到1000℃);随着Er3 替代量的增加,Bi2(Zn1/3Nb2/3)2O7系介质材料的晶粒尺寸、介电常数、介电损耗都有所变化;当替代量x=0.1时,介电性能最佳,介电常数为78.7165,介电损耗为0.00134.     

Sm2O3掺杂的Bi2O3-ZnO-Nb2O5基陶瓷的烧结特性与介电性能

用传统的固相法合成了Sm2O3掺杂的Bi2O3-ZnO-Nb2O5(BZN)基陶瓷(Bi1.5-xSmxZn0.5)(Zn0.5Nb1.5)O7(0≤x≤0.6,BSZN),通过XRD、AV2782阻抗分析仪等测试手段对其烧结行为、相结构及介电性能进行了系统研究.结果表明纯BZN陶瓷的结构为立方焦绿石单相;当Sm2O3掺杂量较少(0＜x≤0.5)时,样品的相结构仍然保持立方焦绿石单相;随着Sm2O3掺杂量的进一步增加(x≥0.6),样品出现其它相.同时,试样的介电性能随结构的变化而呈现有规律的变化.     

铋基烧绿石陶瓷及其微波特性

介绍了低烧结温度的铋基烧绿石系介质陶瓷的结构特点和微波响应行为。以铋基烧绿石中典型的Bi2O3-ZnO-Nb2O3系及其四元系固溶体陶瓷为例，详述了这些体系的相结构、相变及其改变其微波介电性能的途径。指出低烧结温度的铋基烧绿石系介质陶瓷的基本实验制备工艺与检测技术，并讨论了进一步降低烧结温度的方法，对其今后的发展进行了展望。     

NPO型铋基焦绿石复相陶瓷的制备及介电性能

为获得温度稳定型高频高介材料,通过复相介电组成调控原理,将正温度系数型焦绿石相(Bi1.5Zn0.5)(Zr1.5Nb0.5)O7(BZZN)与负温度系数型(Bi1.5Zn0.5)(Zn0.5Nb1.5)O7(BZN)混合构成BZN-BZZN复相材料.研究了该系列陶瓷的物相组成、晶体结构及介电性能随两相组成的变化规律.晶体结构精修获得了复相结构中两相的晶格常数、A-O'键长、B--O键长、O—B—O键角的变化.复相陶瓷的介电性能可通过两相比例有规律地调制,随着BZZN含量增多,(1-x)BZN-xBZZN介电常数εr略有下降,介电常数温度系数逐渐由负值向正值变化.当x=0.7时,获得高介电常数、零温度系数陶瓷材料:εr=123.2,tanδ=7×10-4,αε=5×10-6/℃.     

W替代Bi对β-BZN介电性能的影响

采用固相反应制备(Bi2-xWx)(Zn1/3Nb2/3)2O7陶瓷。研究W6+替代Bi3+对铋锌铌基陶瓷烧结特性、相结构及介电性能的影响。结果表明:掺杂BZN烧结温度略有降低;样品相结构保持单一的单斜焦绿石相,其相结构向高角方向移动;随着W6+替代量的增加,介质材料的介电常数、介电损耗及温度系数都有所变化;当x=0.2时,样品的性能最优,εr=95.39、tanδ=3.89×10-3,αc=228.7×10-6。     

Ni替代Nb对Bi1.5ZnNb1.5O7陶瓷介电性能的影响

以分析纯级原料,按照一定比例混合,利用固相反应制备Bi1.5ZnNb1.5O7陶瓷.研究结果表明:Ni掺杂样品能够有效地降低烧结温度至960℃;样品相结构保持立方焦绿石相;随着Ni3+替代量的增加,介质材料的介电常数及介电损耗逐渐增大;在-195～150℃的温度范围内,介电常数存在明显的弛豫现象,随Ni3+的掺杂量增加,逐渐向高温方向移动,在1 MHz下其峰值温度为:-98.1℃,-97.7℃,-97.1℃,-94.2℃.     

ZnO对铋锌硼系电子封接玻璃烧结性能的影响研究

利用X射线衍射分析、SEM对Bi2O3-ZnO-B2O3系统低熔点玻璃的烧结性能、玻璃的结晶、烧结后玻璃试样的结构进行了研究.研究结果表明:随着ZnO含量的增加,玻璃试样的烧结收缩率有所增加,烧结变得相对容易,玻璃颗粒液相出现所需要的温度-有所降低.Bi2O3-ZnO-B2O3系统低熔点玻璃粉末的烧结是在有粘性液相参与下的烧结过程,使得玻璃试样的致密化更加有效,效率更高.B组试样中都析出了a-Bi2O3晶相.当温度继续升高时,试样的烧结收缩出现了"滞缓"的现象,试样中有大量的液相出现,试样在表面张力的作用下出现了流散.     

掺钇铌酸锌铋陶瓷的介电性能

通过X射线衍射、扫描电镜、精密阻抗分析仪等对A位Y3 取代的Bi(1.5-x)YxZnNb1.5O7介质陶瓷样品的结构和介电性能进行了研究.结果表明:当Y3 取代量较少时(x≤0.2),样品保持立方焦绿石结构;当Y3 取代较多时(x≥0.4),样品出现第二相.随着取代量的增加,样品的致密化温度升高,表观密度减小,晶粒尺寸减小,介电常数减小,介电损耗增加.Y3 取代后(x≤0.8),样品的温度系数得到优化,且具有良好的高频稳定性.低温的介电弛豫现象随着Y3 取代的增加发生有规律的变化,表现为介电常数下降,介电常数峰宽化和平坦.     

烧结温度对LaCrO3陶瓷介电性能的影响

采用La_2O_3和Cr_2O_3为原料,固相法制备了LaCrO_3陶瓷粉末,并在不同烧结温度下得到LaCrO_3陶瓷,通过X射线衍射分析仪、扫描电镜及介电频谱仪对其物相、微结构及介电性能进行了研究。结果表明:1 200℃烧结4 h,LaCrO_3陶瓷的致密度最佳,其颗粒尺寸约为1μm～2μm。随着烧结温度增加,LaCrO_3陶瓷的介电常数和介电损耗随频率增大而减小,这可能归因于纯LaCrO_3陶瓷中的氧空位难以形成,氧空位数非常少。     

Ferroelectric to Relaxor Transition in BaTiO3–Bi(Zn2/3Nb1/3)O3 Ceramics

The (1?x)BaTiO₃–xBi(Zn_2/3Nb_1/3)O₃ (x = 0.01–0.30) ceramics were synthesized by solid‐state reactions. The solubility limit was determined to be x = 0.20. A systematic structural transition from a tetragonal phase (x ≤ 0.034), to a mixture of tetragonal and rhombohedral phases (0.038 ≤ x ≤ 0.20), and finally to a pseudocubic phase (x ≥ 0.22) at room temperature was identified. Dielectric measurement revealed a ferroelectric (x ≤ 0.04) to relaxor (x ≥ 0.06) transition with permittivity peak broadening and flattening, which was further verified by Raman spectroscopy and differential scanning calorimetry (DSC). Activation energies obtained from the Vogel–Fulcher model displayed an increasing trend from ~0.03 eV for x ~ 0.05, to unusually high values (>0.20 eV) for the compositions with x ≥ 0.15. With the increase in Bi(Zn_2/3Nb_1/3)O₃ content, the polarization hysteresis demonstrated a tendency from high nonlinearity to sublinearity coupled with the reduction in remnant polarization and coervice field. The deconvolution of the irreversible/reversible polarization contribution was enabled by first‐order reversal curve distributions, which indicates that the decreasing polarization nonlinearity with the increase in Bi(Zn_2/3Nb_1/3)O₃ concentration could be related with the change from the ferroelectric domain and domain wall contributions to the weakly coupled relaxor behaviors.     

Y3+取代对(Bi1.5Zn0.5)(Nb0.5Ti1.5)O7陶瓷显微结构与介电性能的影响

研究了Y3 取代的(Bi1.5Zn0.5)(Nb0.5Ti0.5)O7(BZNT)基陶瓷(Bi1.5-xYx Zn0.5)(Nb0.5Ti1.5)O7(0≤x≤1.5,BYZNT)的显微结构和介电性能。采用传统的固相反应法制备陶瓷样品,XRD分析样品的相结构。结果表明:BZNT陶瓷的相结构中主相为立方焦绿石相;在整个取代范围内,BYZNT陶瓷的结构仍然保持主相为立方焦绿石的相结构。同时,随着Y3 取代的增加,晶胞体积减小,介电性能随结构的变化而呈现有规律的变化。其介电性能为:εr≈73-180,tanδ≈1.6％-0.4％,αε≈(-583-89)× 10-6／℃(1MHz)。     

Conduction Mechanisms in BaTiO3–Bi(Zn1/2Ti1/2)O3 Ceramics

Polycrystalline BaTiO₃–Bi(Zn_1/2Ti_1/2)O₃ (BT–BZT) ceramics have superior dielectric properties for high‐temperature and high‐energy density applications as compared to the existing materials. While it has been shown that the addition of BZT to BT leads to an improvement in resistivity by two orders of magnitude, in this study impedance spectroscopy is used to demonstrate a novel change in conduction mechanism. While nominally undoped BT exhibits extrinsic‐like p‐type conduction, it is reported that BT–BZT ceramics exhibit intrinsic n‐type conduction using atmosphere‐dependent conductivity measurements. Annealing studies and Seebeck measurements were performed and confirmed this result. For BT, resistivity values were higher for samples annealed in nitrogen as compared to oxygen, whereas the opposite responses were observed for BZT‐containing solid solutions. This suggests a fundamental change in the defect equilibrium conditions upon the addition of BZT to the solid solution that lowered the carrier concentration and changed the sign of the majority charge carrier. This is then also linked to the observed improvement in resistivity in BT–BZT ceramics as compared to undoped BT.     

Ferroelectric Ceramics in the PbMg1/3Nb2/3O3-PbCd1/3Nb2/3O3 System

Solid solutions (1-x)PbMg_1/3Nb_2/3O₃ + xPbCd_1/3Nb_2/3O₃ with x = 0-0.30 are investigated with purpose to work out a capacitor ceramics with good dielectric properties and low sintering temperature. It is found that the perovskite phase forms at sintering near to 980°C and begins to decompose at higher temperatures. When x grows from 0 to 0.30, the Curie temperature linearly grows from -10°C to +25°C, the dielectric permittivity ε_m in the Curie point T_C decreases from 18000 to 6800 and the phase transition becomes more diffused. The dielectric permittivity at room temperature is rather high and the temperature stability is improved. The system is of interest, because it can serve as a base for working out some ceramic materials for capacitors with low sintering temperature, which needs of no special atmosphere at burning.     

Re‐entrant relaxor behavior in BaTiO3‐Bi(Zn2/3Nb1/3)O3 ceramics

The (1?x)BaTiO₃?xBi(Zn_2/3Nb_1/3)O₃ (x=0.10‐0.25) ceramics were fabricated via solid‐state reactions. Temperature‐dependent polarization measurement reveals that with the temperature lowering, the remnant polarization increases till a maximum value before it decreases, showing a reentrant phenomenon. Absence of apparent switching current peaks in the current density as a function of electric field should indicate the lack of a ferroelectric transition, which is further verified by the consistent macroscopic phase structure from the Raman spectra. An anomalous peak in the full width at half maximum of a deconvoluted mode at ~515 cm^?1 suggests the entering of a more disordered state of dipolar dynamics, which may be originated from the competition between the freezing of polar nanoregions and the random interacting fields.     

V2O5掺杂对(Bi1.5Zn1.0Nb1.5)O7介质陶瓷性能的影响

采用传统的固相反应法制备陶瓷试样,借助XRD,SEM和LCR测试仪,研究了V2O5掺杂对(Bi1.5Zn1.0Nb1.5)O7介质陶瓷的烧结特性和介电性能的影响.结果表明,掺杂适量V2O5后试样的烧结温度明显降低,相结构仍为立方焦绿石单相,且具有良好的介电性能:介电常数(εr)为135～154,介电损耗(tan δ)为0.0033～0.0007,频率温度系数(τf)为-442～-387(2MHz).     

Bi2O_3－Fe_2O_3系陶瓷材料的气－湿－温多功能特性

利用Ｘ射线衍射（ＸＲＤ）分析了烧结温度及Ｂｉ／Ｆｅ比对Ｂｉ２Ｏ３－Ｆｅ２Ｏ３系物相组成的影响。初步探讨了材料的导电类型、气敏性能及阻－湿特性，结果表明Ｂｉ２Ｏ３－Ｆｅ２Ｏ３系有可能作为一种气－湿－温多功能敏感材料体系