Behavior of Charged Particles do $(Sr_{0.85}{\cdot}Ca_{0.15})_mTiO_3$ Grain Boundary Layer Ceramics

$(Sr_{0.85}{\cdot}Ca_{0.15})_mTiO_3$ 입계층 세라믹의 하전입자 거동

  • 김진사 (광운대학교 전기공학과) ;
  • 정동효 (시립인천전문대학 전기과) ;
  • 김상남 (시립인천전문대학 전기과) ;
  • 박재세 (시립인천전문대학 전기과) ;
  • 최운식 (광운대학교 전기공학과) ;
  • 이준용 (광운대학교 전기공학과)
  • Published : 1995.11.01

Abstract

In this paper, the $(Sr_{0.85}{\cdot}Ca_{0.15})TiO_3$ of paraelectric grain boundary layer (GBL) ceramics were fabricated. The characteristics of electrical conduction and the thermally stimulated current(TSC) were measured respectively. The region I below 200[V/cm] shows the ohmic conduction, the region II between 200[V/cm] and 1000[V/cm] can be explained by the Pool-Frenkel emission theory, and the region III above 2000[V/cm] is dominated by the tunneling effect. As a result, The origins of these peaks are that the ${\alpha}$ peak observed at $-20[^{\circ}C]$ looks like to be ascribed to the ionization excitation from donor level in the grain, and the ${\alpha}^{\prime}$ peak observed at $-20[^{\circ}C]$ appears to show up by detrap of the trapped carrier of border between the oxidation layer and the grain, and the ${\beta}$ peak observed at $80[^{\circ}C]$ seems to be resulted from hopping conduction of existing carrier in the trap site of the border between the oxidation and second phase.

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