TY - CPAPER KW - Annealing KW - Heating KW - Voltage measurement KW - Polarization KW - Ferroelectric materials KW - Energy gap KW - Lead compounds KW - Crystals KW - Paramagnetic resonance KW - Barium titanate KW - Switchable polarization KW - Lead zirconate titanate (PZT) KW - Radiation effects KW - Charge carriers KW - Charge injection KW - Electrical suppression effect KW - Electronic trapping effect KW - Ionic trapping effect AU - William Warren AU - Duane Dimos AU - Bruce Tuttle AU - Gordon Pike AU - Mark Raymond AU - Robert Nasby AU - Ramamoorthy Ramesh AU - Joseph Evans Jr AB -

Switchable polarization can be significantly suppressed in ferroelectric (FE) materials by optical, thermal, and electrical processes. The thermal process can occur by either annealing the FE in a reducing environment or by heating it in air to 100 °C while impressing a bias near the switching threshold. The optical process occurs while biasing the FE near the switching threshold and illuminating with bandgap light. And the electrical suppression effect occurs by subjecting the FE to repeated polarization reversals. Using electron paramagnetic resonance, polarization-voltage measurements, and charge injection scenarios, we have been able to elucidate both electronic and ionic trapping effects that lead to a suppression in the amount of switchable polarization in FE materials. The relative roles of electronic and ionic effects in the same material can depend on the stress condition. For instance, in oxidized BaTiO3 crystals, optical and thermal suppressions occur by electronic domain pinning; electrical fatigue in the BaTiO3 crystals also appears to involve electronic charge trapping, however, it is suggested that these electronic traps are further stabilized by nearby ionic defects. In sol-gel PZT thin films with either Pt, RuO2, or La-Sr-Co-O electrodes it appears that the polarization suppression induced by electrical fatigue, a temperature/bias combination, or a light/bias combination are all primarily due to the trapping of electronic charge carriers to first order.

BT - Proceedings of the Materials Research Society Symposium - LA - eng N1 -

cited By 10

N2 -

Switchable polarization can be significantly suppressed in ferroelectric (FE) materials by optical, thermal, and electrical processes. The thermal process can occur by either annealing the FE in a reducing environment or by heating it in air to 100 °C while impressing a bias near the switching threshold. The optical process occurs while biasing the FE near the switching threshold and illuminating with bandgap light. And the electrical suppression effect occurs by subjecting the FE to repeated polarization reversals. Using electron paramagnetic resonance, polarization-voltage measurements, and charge injection scenarios, we have been able to elucidate both electronic and ionic trapping effects that lead to a suppression in the amount of switchable polarization in FE materials. The relative roles of electronic and ionic effects in the same material can depend on the stress condition. For instance, in oxidized BaTiO3 crystals, optical and thermal suppressions occur by electronic domain pinning; electrical fatigue in the BaTiO3 crystals also appears to involve electronic charge trapping, however, it is suggested that these electronic traps are further stabilized by nearby ionic defects. In sol-gel PZT thin films with either Pt, RuO2, or La-Sr-Co-O electrodes it appears that the polarization suppression induced by electrical fatigue, a temperature/bias combination, or a light/bias combination are all primarily due to the trapping of electronic charge carriers to first order.

PB - Materials Research Society, Pittsburgh, PA, United States PY - 1995 SP - 51 EP - 65 T2 - Proceedings of the Materials Research Society Symposium - T3 - Materials Research Society Symposium - TI - Mechanism(s) for the suppression of the switchable polarization in PZT and BaTiO3 VL - 361 SN - 02729172 ER -