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Ferroelectric Properties of Ti-Doped and W-Doped SBT Ceramics

Ti와 W이 첨가된 SBT 세라믹스의 강유전 특성

  • 천채일 (호서대학교 신소재공학과) ;
  • 김정석 (호서대학교 신소재공학과)
  • Published : 2004.05.01

Abstract

Undoped SrB $i_2$T $a_2$O$_{9}$, donor-doped Sr$_{0.99}$B $i_2$(Ta$_{0.99}$W$_{0.01}$)$_2$O$_{9}$ and acceptor-doped SrB $i_2$(Ta$_{0.99}$Ti$_{0.01}$)$_2$O$_{8.99$ ceramics were prepared and their microstructure, ferroelectric P-E hysteresis and Curie temperature were investigated. Grain size did not influence P-E hysteresis curve in undoped SrB $i_2$T $a_2$O$_{9}$ ceramics. Donor-Doped Sr$_{0.99}$B $i_2$(Ta$_{0.99}$W$_{0.01}$)$_2$O$_{9}$ ceramics showed more saturated P-E hysteresis curve with larger remanent polarization (P$_{r}$) than undoped SrB $i_2$T $a_2$O$_{9}$ ceramics while acceptor-doped SrB $i_2$(Ta$_{0.99}$Ti$_{0.01}$)$_2$O$_{8.99}$ ceramics led to a pinched P-E hysteresis loop. Larger polarization in donor-doped Sr$_{0.99}$B $i_2$(Ta$_{0.99}$W$_{0.01}$)$_2$O$_{9}$ ceramics resulted from easier domain wall motion by Sr-vacancies.

순수한 SrB $i_2$T $a_2$$O_{9}$ 세라믹스와 도너와 억셉터가 치환된 S $r_{0.99}$B $i_2$(T $a_{0.99}$ $W_{0.01}$)$_2$$O_{9}$ 와 SrB $i_2$(T $a_{0.99}$ $Ti_{0.01}$)$_2$ $O_{8.99}$ 세라믹스를 제조하고 미세구조, 강유전 P-E 이력특성, 상전이 온도를 조사하였다. 입자크기는 SrB $i_2$T $a_2$$O_{9}$ 세라믹스의 강유전 이력곡선에는 영향을 주지 않았다. 도너를 치환한 S $r_{0.99}$B $i_2$(T $a_{0.99}$ $W_{0.01}$)$_2$$O_{9}$ 세라믹스는 순수한 SrB $i_2$T $a_2$$O_{9}$ 세라믹스보다 잔류 분극이 크고 더욱 포화된 강유전 P-E 이력곡선을 보였으며, 억셉터가 치환된 SrB $i_2$(T $a_{0.99}$ $Ti_{0.01}$)$_2$ $O_{8.99}$ 세라믹스는 잔류분극이 크게 감소하여 가운데가 잘록한 모양을 보였다. 도너가 치환된 S $r_{0.99}$B $i_2$(T $a_{0.99}$ $W_{0.01}$)$_2$$O_{9}$ 세라믹스의 강유전 분극이 순수한 SrB $i_2$T $a_2$$O_{9}$ 세라믹스보다 더 큰 것은 Sr 공공의 생성에 의하여 분역벽 이동이 용이해졌기 때문이다.동이 용이해졌기 때문이다.동이 용이해졌기 때문이다.동이 용이해졌기 때문이다.

Keywords

References

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