Microwave dielectric properties of Ba[Ti0.4Ga0.3Nb0.3(l-x)Sb0.3x]O3 perovskite ceramics

被引:3
作者
Tian, Cailan [1 ]
Yue, Zhenxing [1 ]
Zhou, Yuanyuan [1 ]
机构
[1] Tsinghua Univ, Dept Mat Sci & Engn, State Key Lab New Ceram & Fine Proc, Beijing 100084, Peoples R China
关键词
Ceramics; X-ray diffraction; Crystal structure; Dielectric properties; ELECTRICAL-PROPERTIES; COMPLEX PERMITTIVITY;
D O I
10.1016/j.materresbull.2012.11.001
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The perovskite Ba[Ti0.4Ga0.3Nb0.3((1-x))Sb-0.3x]O-3 (x = 0-1.00) solid solutions were synthesized by the conventional solid-state reaction method. The structures and microwave dielectric properties were investigated by X-ray and dielectric measurements. Their crystal structures transferred from the cubic to hexagonal one with increasing x. The oxygen octahedra distortions were described from the refinement data. It revealed that the negative and positive charge centers coincided at the origin in the cornersharing octahedra, but they did not coincide with each other in the face-sharing ones. Two pairs of dipoles canceled in the face-sharing oxygen octahedra, which had an effect on lowering the dielectric constant (epsilon(r)). The temperature coefficient of resonant frequency (tau(f)) of ceramic at x = 0.50 was -1.1 ppm/degrees C. The hexagonal perovskite had much higher quality factor (Q x f), nearer-zero tau(f), and lower sr than the cubic one. This was ascribed to the canceled dipoles and more shared oxygen ions in the face-sharing oxygen octahedra. (c) 2012 Elsevier Ltd. All rights reserved.
引用
收藏
页码:455 / 460
页数:6
相关论文
共 22 条
[1]   Synthesis and structural study of the new perovskite series CaLn2ZnTi2O9 (=(Ca1/3Ln2/3)A(Zn1/3Ti2/3)BO3) (Ln=La, Pr, Nd, Eu) [J].
Aatiq, A ;
Boukhari, A .
MATERIALS LETTERS, 2004, 58 (19) :2406-2411
[2]   REFINEMENT OF HEXAGONAL BATIO3 [J].
AKIMOTO, J ;
GOTOH, Y ;
OOSAWA, Y .
ACTA CRYSTALLOGRAPHICA SECTION C-CRYSTAL STRUCTURE COMMUNICATIONS, 1994, 50 :160-161
[3]   Low-Loss Microwave Ceramics Based on Non-Stoichiometric Perovskites Ba(Co1/3Nb2/3)O3 and Ba(Zn1/3Nb2/3)O3 [J].
Belous, A. G. ;
Ovchar, O. V. ;
Kramarenko, O. V. ;
Bezjak, J. ;
Jancar, B. ;
Suvorov, D. ;
Annino, G. .
FERROELECTRICS, 2008, 367 :149-162
[5]   Dielectric relaxation and electronic structure of BaAl1/2Nb1/2O3: x-ray photoemission and nuclear magnetic resonance studies [J].
Dutta, Alo ;
Sinha, T. P. ;
Pahari, B. ;
Sarkar, R. ;
Ghoshray, K. ;
Shannigrahi, Santiranjan .
JOURNAL OF PHYSICS-CONDENSED MATTER, 2008, 20 (44)
[6]  
Hakki BW., 1960, IEEE. Trans. MTT, DOI DOI 10.1109/TMTT.1960.1124749
[7]   Ba3MIIITiMVO9 (MIII = Fe, Ga, Y, Lu, MV = Nb, Ta, Sb) perovskite oxides Synthesis, structure and dielectric properties [J].
Joy, Joby E. ;
Atamanik, Eric ;
Mani, Rohini ;
Nag, Abanti ;
Tiwari, R. M. ;
Thangadurai, V. ;
Gopalakrishnan, J. .
SOLID STATE SCIENCES, 2010, 12 (12) :1970-1976
[8]   A dielectric resonator for measurements of complex permittivity of low loss dielectric materials as a function of temperature [J].
Krupka, J ;
Derzakowski, K ;
Riddle, B ;
Baker-Jarvis, J .
MEASUREMENT SCIENCE AND TECHNOLOGY, 1998, 9 (10) :1751-1756
[9]   Crystal chemistry and microwave dielectric properties of Ba3MNb2-xSbxO9 (M = Mg, Ni, Zn) [J].
Lufaso, MW ;
Hopkins, E ;
Bell, SM ;
Llobet, A .
CHEMISTRY OF MATERIALS, 2005, 17 (16) :4250-4255
[10]   Study of Ba3MIIMIVWO9 (MII = Ca, Zn; MIV = Ti, Zr) perovskite oxides:: Competition between 3C and 6H perovskite structures [J].
Mani, Rohini ;
Selvamani, P. ;
Joy, Joby E. ;
Gopalakrishnan, J. .
INORGANIC CHEMISTRY, 2007, 46 (16) :6661-6667