Lead zinc niobate pyrochlore: Structure and dielectric properties |
| |
Authors: | H C Ling M F Yan W W Rhodes |
| |
Affiliation: | (1) AT&T Bell Laboratories, 08540 Princeton, New Jersey, USA;(2) AT&T Bell Laboratories, 07974 Murray Hill, New Jersey, USA |
| |
Abstract: | In Pb(B
x
B1–x
)O3 ceramic compositions, it is customary to find a mixture of cubic pyrochlore and perovskite phases after calcination. Based on X-ray diffraction analysis, we concluded that both phases are made up of the same structural unit of BO6 octahedra. The B and B ions occupy the B sites randomly to the extent that local charge equilibrium is maintained. Thus a general formula for the pyrochlore phase can be expressed as Pb(B
x
B1–x
)O3 · Op where O p 0.5. An extensive study of the Pb(Zn
x
Nb1–x
)O3.5–1.5x
pyrochlore system was made by varying the zinc concentration. We interpret changes in the X-ray diffraction pattern and the lattice constant as indicative of the changing occupancy of the seventh oxygen sites in order to maintain local charge balance. The best combination of the dielectric properties, with a dielectric constant of130 and a factor greater than 1000 at10 MHz, is achieved at a composition of 0.3 x 0.4 and a sintering temperature of 980° C. The temperature coefficient of the dielectric constant measures –0.75 × 10–3° C–1. It decreases to –0.54 × 10–3° C–1 when5 mol% of PbTiO3 was mixed with the nominal pyrochlore compositions and sintered. Thus, it may be possible to effect a larger change in the temperature coefficient by judiciously including selective amounts of a second phase which has the best compensating temperature coefficient. |
| |
Keywords: | |
本文献已被 SpringerLink 等数据库收录! |
|