共查询到20条相似文献,搜索用时 15 毫秒
1.
Modification of the microwave dielectric properties in Ba6−3 x Nd8+2 x Ti18 O54 ( x = 0.5) solid solutions by Bi/Sm cosubstitution for Nd was investigated. A large increase in the dielectric constant and near-zero temperature coefficient combined with high Qf values were obtained in modified Ba6−3 x Nd8+2 x Ti18 O54 solid solutions where an enlarged solid solution limit of Bi in Ba6−3 x Nd8+2 x Ti18 O54 was observed. Excellent microwave dielectric characteristics (ɛ= 105, Qf = 4110 GHz, and very low τf ) were achieved in the composition Ba6−3 x (Nd0.7 Bi0.18 Sm0.12 )8+2 x Ti18 O54 . 相似文献
2.
Ba6−3 x Nd8+2 x Ti18 O54 ceramic powders were synthesized by the modified Pechini method using ethylenediaminetetraacetic acid (EDTA) as a chelating agent. A purplish red, molecular-level, homogeneously mixed gel was prepared, and transferred into a porous resin intermediate through charring. Single-phase and well-crystallized Ba6−3 x Nd8+2 x Ti18 O54 powders were obtained from pulverized resin at a temperature of 900°C for 3 h, without formation of any intermediate phases. Meanwhile, the molar ratio of EDTA to total metal cation concentration had a significant influence on the crystallization behavior of Ba6−3 x Nd8+2 x Ti18 O54 . The Ba6−3 x Nd8+2 x Ti18 O54 ( x = 2/3) ceramics prepared via EDTA precursor have excellent microwave dielectric characteristics: ɛ= 87, Qf = 8710 GHz. 相似文献
3.
Rick Ubic Ian M. Reaney William E. Lee 《Journal of the American Ceramic Society》1999,82(5):1336-1338
The space group of the solid solution phase Ba6-3 x -RE8+2 x Ti18 O54 (RE = rare-earth cation) has been variously reported as Pba 2 (No. 32), Pbn 21 (No. 33), Pbam (No. 55), or Pbnm (No. 62). New results are presented here which indicate that its correct space group assignment may be Pb 21 m (No. 26). 相似文献
4.
Tin (Sn) substitution into the B-site and Nd/Sn cosubstitution into the A- and B-sites were investigated in a Ba 6−3 x Sm8+2 x Ti18 O54 solid solution ( x = 2/3). A small amount of tin substitution for titanium improved the temperature coefficient of resonant frequency (τf ) but led to a decrease of the relative dielectric constant (ɛ) and the quality factor ( Qf ). The Ba6−3 x Sm8+2 x (Ti1− z Snz )18 O54 -based tungsten-bronze phase became unstable for compositions with a tin content of ≥10 mol%, where BaSm2 O4 and Sm2 (Sn,Ti)2 O7 appeared, and finally, these phases became the major phases. On the other hand, Nd/Sn cosubstitution led to a good combination of high ɛ, high Qf , and near-zero τf . Excellent microwave dielectric properties were achieved in Ba6−3 x (Sm1− y Nd y )8+2 x (Ti1− z Sn z )18 O54 ceramics with y = 0.8 and z = 0.05 sintered at 1360°C for 3 h: ɛ= 82, Qf = 10 000 GHz, and calculated τf =+17 ppm/°C. The tolerance factor and electronegativity difference exhibited important effects on the microwave dielectric properties, especially the Qf value. A large tolerance factor and high electronegativity difference generally led to a higher Qf value. 相似文献
5.
Karen M. Cruickshank Xiping Jing Graeme Wood Eric E. Lachowski Anthony R. West 《Journal of the American Ceramic Society》1996,79(6):1605-1610
A solid-solution phase with the general formula Ba6-3x Nd8+2x Ti18 O54 , where 0.25(5) ≤×≤ 0.75(5), has been characterized at 1250°C; this phase has been variously described as BaNd2 Ti4 O12 and BaNd2 Ti5 O14 in the literature. Variation in its stoichiometry is accommodated via the cation substitution mechanism, 3Ba2 ⇆2Nd3+ . The location and extent of the solid solution were demonstrated by a combination of phase diagram studies and X-ray diffraction techniques, including lattice parameter measurements and electron microscopy. A combination of techniques was employed due to the insensitivity of secondary phase detection by X-ray diffraction in this system. Using this approach, a second possible solid-solution mechanism, Ba2+ 2Nd3+ ⇆2Ti4+ , is discounted. 相似文献
6.
Hui Zhang Liang Fang Heping Su Qian Yu Bolin Wu 《Journal of the American Ceramic Society》2009,92(1):238-240
Single-phase polycrystalline microwave dielectric ceramics Ba6 Ti1− x Sn x Nb4 O18 , with x changing from 0 to 1, were synthesized by the solid-state reaction method. All the solid solutions fitted well with A6 B5 O18 cation-deficient hexagonal perovskite structure. The substitution of Sn for Ti effectively enhanced the quality factor and controlled τf . With increasing Sn content, the dielectric constant decreased from ∼47 to ∼32, and the Q × f value increased significantly from 11 530 to 28 496 GHz, with τf varying from 64 to 0 ppm/°C. A zero τf was realized when Sn was fully replaced by Ti with the composition Ba6 SnNb4 O18 . 相似文献
7.
8.
Thermal expansion behaviors of Ba6−3 x Ln8+2 x Ti18 O54 (Ln=La, Nd, and Sm, x =0.5, 0.67, and 0.75) ceramics were determined by dilatometric measurement. The samples of all investigated compositions expanded nearly linearly with increasing temperature in the range of 20°–1200°C. Their thermal expansion coefficients were determined to be 10.7–11.4 ppm/°C. A discontinuous change in sample size was observed at about 1350°C for each composition, indicating the existence of a phase transition. As determined by the high-resolution X-ray diffraction analysis, the phase constitution and the lattice parameters of Ba6−3 x Sm8+2 x Ti18 O54 ceramics were maintained in the quenched samples. The origin of the phase transition was discussed thoroughly. Phase equilibrium in the BaTiO3 –Ln2/3 TiO3 system was reviewed by considering the phase transition. 相似文献
9.
Hong Xia Yuan Xiang Ming Chen Min Min Mao 《Journal of the American Ceramic Society》2009,92(10):2286-2290
CaNdAlO4 microwave dielectric ceramics were modified by Ca/Ti co-substitution, and their dielectric characteristics were evaluated along with their structure and microstructures. Ca1+ x Nd1− x Al1− x Ti x O4 ( x =0, 0.025, 0.05, 0.10, 0.15, 0.20) ceramics with the relative density of over 95% theoretical density were obtained by sintering at 1400°–1450°C in air for 3 h, where the K2 NiF4 -type solid solution single phase was determined from the compositions of x <0.20, while a small amount of CaTiO3 secondary phase was detected for x =0.20. With Ca/Ti co-substitution in CaNdAlO4 ceramics, the dielectric constant (ɛr ) increased with increasing x , and the temperature coefficient of resonant frequency (τf ) was adjusted from negative to positive, while the Q × f 0 value increased significantly at first and reached an extreme value at x =0.025 and the maximum at x =0.15. The best combination of microwave dielectric characteristics were achieved at x =0.15 (ɛr =19.5, Q × f 0 =93 400 GHz, τf =−2 ppm/°C). The improvement of the Q × f 0 value primarily originated from the reduced interlayer polarization with Ca/Ti co-substitution, while the decreased tolerance factor, the subsequent increased interlayer stress, and the appearance of CaTiO3 secondary phase brought negative effects upon the Q × f 0 value. 相似文献
10.
Ba6−3 x Sm8+2 x Ti18 O54 ( x =2/3) (BST) was prepared by the solid-state method and the effect of bismuth borate (BB)/LiF on the sinterability, microstructure, and thermal and microwave dielectric properties were studied. BST+3.5 wt% BB+0.5 wt% LiF composite sintered at 1050°C has Q × f =4500 GHz, ɛ=52, and τ f =+6 ppm/°C. Raman spectrum of the composite was compared with that of BST and the structural changes were investigated. 相似文献
11.
Om Parkash Hari Shanker Tewari Lakshman Pandey Ravindra Kumar Devendra Kumar 《Journal of the American Ceramic Society》1989,72(8):1520-1522
Attempts have been made to synthesize the compositions with x = 0.01, 0.05, 0.10, 0.20, 0.30, 0.40, and 0.50 in the valence-compensated solid-solution Ba1–x Lax Ti1–x Nix O3 by ceramic methods. Solid solutions formed in the compositions with x0.10. The structure of the composition with x = 0.01 is tetragonal, whereas samples with x = 0.05 and 0.10 are cubic. A ferroelectric-paraelectric transition is observed only in the composition with x = 0.01 at ∼ 350 K. 相似文献
12.
J. K. PLOURDE D. F. LINN H. M. O'BRYAN Jr .JOHN THOMSON Jr . 《Journal of the American Ceramic Society》1975,58(9-10):418-420
Microwave measurements of Ba2 Ti9 O20 show that this ceramic is uniquely suited for dielectric resonators. (Suitable ceramics should have a high dielectric constant K , a low dielectric loss (high Q ), and a low temperature coefficient of resonant frequency, τ.) At 4 GHz, Ba2 Ti9 O20 resonators have Q >8000, K = 39.8, and τ=2 ppm/°C. Measurements of Q and τ were made on unmetallized ceramic resonator disks positioned in a waveguide; K was measured using a dielectric post resonator technique. From 4 to 10 GHz, Q approaches that for a copper waveguide cavity, whereas the temperature coefficient is typically 8 times lower. 相似文献
13.
Sandeep Butee Ajit Kulkarni Om Prakash Ramnath P.R.C. Aiyar Sumesh George Mailadi Sebastian 《Journal of the American Ceramic Society》2009,92(5):1047-1053
(Ni1− x Zn x )Nb2 O6 , 0≤ x ≤1.0, ceramics with >97% density were prepared by a conventional solid-state reaction, followed by sintering at 1200°–1300°C (depending on the value of x ). The XRD patterns of the sintered samples (0≤ x ≤1.0) revealed single-phase formation with a columbite ( Pbcn ) structure. The unit cell volume slightly increased with increasing Zn content ( x ). All the compositions showed high electrical resistivity (ρdc =1.6±0.3 × 1011 Ω·cm). The microwave (4–5 GHz) dielectric properties of (Ni1− x Zn x )Nb2 O6 ceramics exhibited a significant dependence on the Zn content and to some extent on the morphology of the grains. As x was increased from 0 to 1, the average grain size monotonically increased from 7.6 to 21.2 μm and the microwave dielectric constant (ɛ'r ) increased from 23.6 to 26.1, while the quality factors ( Q u × f ) increased from 18 900 to 103 730 GHz and the temperature coefficient of resonant frequency (τf ) increased from −62 to −73 ppm/°C. In the present work, we report the highest observed values of Q u × f =103 730 GHz, and ɛ'r =26.1 for the ZnNb2 O6 -sintered ceramics. 相似文献
14.
Ni Qin Marjeta Maek Krmanc Danilo Suvorov 《Journal of the American Ceramic Society》2008,91(8):2593-2600
K x Ba1− x Ga2− x Ge2+ x O8 (0.6≤ x ≤1) polycrystalline ceramics are potential materials for glass-free low-temperature cofired ceramics (LTCC) substrates. We have made a comprehensive study of the kinetics of the monoclinic-to-monoclinic P 21 / a ⇔ C 2/ m phase transition. The low-temperature-stable P 21 / a phase with a high Q × f value was synthesized using a subsolidus method and was well sintered at the LTCC temperature with a H3 BO3 additive. A good combination of low sintering temperature (910°–920°C), high Q × f values (96 700–104 500 GHz), low permittivities (5.6–6.0), and a small temperature coefficient of resonant frequency (∼−20 ppm/°C) was obtained for ceramics with x =0.67 and 0.9 and with 0.1 wt% of H3 BO3 . 相似文献
15.
Hiroaki Takeda Masataka Ohgaki Takashi Kizuki Kazuaki Hashimoto Yoshitomo Toda Shigekazu Udagawa Kimihiro Yamashita 《Journal of the American Ceramic Society》2000,83(11):2884-2886
The formation process of Ba2 La8 (SiO4 )6 O2 was clarified using thermogravimetry–differential thermal analysis (TG-DTA) and a high-temperature powder X-ray diffraction (HT-XRD) method. Phase changes identified from the HT-XRD data surprisingly corresponded to the weight loss and/or endothermic peaks observed in the TG-DTA curves. Raw material with the composition Ba2 La8 (SiO4 )6 O2 was completely reacted at 1400°C and produced only an apatite-type compound without a secondary phase. Moreover, the synthesis of Ba2+ x La8− x (SiO4 )6 O2−δ crystals with x = 0–2 was attempted using a solid-state reaction. 相似文献
16.
EKKEHART TILLMANNS WOLFGANG HOFMEISTER WERNER H. BAUR 《Journal of the American Ceramic Society》1983,66(4):268-271
A single-crystal X-ray study of dibarium nonatitanate, Ba2 Ti9 O20 , yielded the triclinic space group P 1 with a =0.7471(1), b= 1.4081(2), c= 1.4344(2) nm, α=89.94(2)°, β= 79.43(2)°, γ= 84.45(2)°, V = 1.476 nm3 Z = 4, and Dx = 4.61 Mg/m3 . A refinement of atomic coordinates and isotropic thermal parameters led to a residual of 0.03. The structure consists of hexagonally closest-packed layers of Ba and O atoms in the sequence (hch)3 . All Ti atoms reside in octahedral interstices of this closest packing. The various Ti coordination octahedra share only edges and corners with each other. One-half of the Ba atoms is twelve-coordinated by oxygen atoms, the other half is eleven-coordinated. 相似文献
17.
The dielectric properties, including the DC breakdown strength, of 1 mol% Nb5+ -doped BaTiO3 ceramics with different quantities of excess TiO2 have been investigated. The breakdown strength was found to decrease with increasing TiO2 content, but could not be readily explained by relative density and grain size effects. The decrease in the breakdown strength from a stoichiometric BaTiO3 composition to samples with excess TiO2 is believed to be due to the field enhancement effect (up to a factor of 1.40) at the BaTiO3 matrix because of the presence of a Ba6 Ti17 O40 second phase. The thermal expansion coefficient mismatch between the BaTiO3 matrix phase and the Ba6 Ti17 O40 phase may also result in a low breakdown strength. The dielectric properties of the pure Ba6 Ti17 O40 phase were also investigated and are reported herein. 相似文献
18.
Wen-Yi Lin Robert F. Speyer Wesley S. Hackenberger Thomas R. Shrout 《Journal of the American Ceramic Society》1999,82(5):1207-1211
The effects of solid-solution additives, their concentration, and the thermal processing schedule on the microstructure evolution and microwave properties of Ba2 Ti9 O20 were studied. The solubility of tin in Ba2 Ti9 O20 was higher than that of zirconium. Both elements facilitated the formation of phase-pure Ba2 Ti9 O20 resonators. Ba2 Ti9 O20 formed most easily with low dopant concentrations (0.82 mol%) (most impressively for ZrO2 substitutions). Extended heat treatment (16 h versus 6 h at a temperature of 1390°C) resulted in volatilization of the grain-boundary liquid phase, which leads to more-porous resonators that have correspondingly lower permittivities. Increasing the dopant concentration resulted in minor increases in the quality factor; doping with zirconium led to slightly higher values (a maximum of 13900 at a frequency of 3 GHz). Increasing the measurement temperature degraded the quality factor (most precipitously for BaTi4 O9 ). The temperature coefficient decreased as the ZrO2 substitution increased but was largely unaffected by the SnO2 concentration. Excess TiO2 in a batch with no other dopants demonstrated degraded microwave properties. 相似文献
19.
Jing Pei Zhenxing Yue Fei Zhao Zhilun Gui Longtu Li 《Journal of the American Ceramic Society》2007,90(10):3131-3137
Tungstenbronze-type Ba4 (Nd0.7 Sm0.3 )9.33 Ti18 O54 (BNST) microwave dielectric ceramics doped with 0–10 wt% silver (Ag) particles were successfully fabricated by a citrate sol–gel method. The influence of Ag doping on the sinterability, microstructure, bulk conductivity, and dielectric properties of BNST was investigated. The desired tungstenbronze-type phase was obtained at 900°–950°C. The sintering temperature of BNST decreased to 1100°C with the aid of a small amount of Ag addition (1 wt%). No chemical reaction between the tungsenbronze phase and Ag was detected. The particle size of the powders decreased with increasing Ag content up to 1 wt% and it then increased with a further increase in the Ag content. The dense fine-grained ceramics with submicrometer grains (∼300 nm) were obtained with 1 wt% Ag addition. The submicrometer-grained ceramics had excellent dielectric properties of ɛr ∼81 and Q × f ∼11 000 GHz. Both the dielectric constant and dielectric loss significantly increased with large additions (>3 wt%) of Ag due to the percolation effect. 相似文献
20.
Chang Wei Zheng Shu Ya Wu Xiang Ming Chen Kai Xin Song 《Journal of the American Ceramic Society》2007,90(5):1483-1486
MgAl2 O4 microwave dielectric ceramics were modified by Zn substitution for Mg, and their dielectric characteristics were evaluated, along with their structures. Dense (Mg1− x Zn x )Al2 O4 ceramics were obtained by sintering at 1550°–1650°C in air for 3 h, and the (Mg1− x Zn x )Al2 O4 solid solution was determined in the entire composition range. With Zn substitution for Mg, the dielectric constant ɛ of MgAl2 O4 just varied from 7.90 to 8.56, while the Q × f value had significantly improved up to a maximal value of 106 000 GHz at x =1.0. Moreover, the τf of MgAl2 O4 ceramics had declined from −73 to −63 ppm/°C. 相似文献