TY - JOUR
T1 - Origins of thermally stimulated current in polyethersulfone
AU - Kim, E. J.
AU - Takeda, T.
AU - Ohki, Y.
N1 - Funding Information:
This work was partly supported by Shinsei Foundation, Nagoya
PY - 1996
Y1 - 1996
N2 - In order to understand the dominant carrier species in electrical conduction in polyethersulfone (PES), thermally stimulated current (TSC) measurements were carried out under various conditions. It was found that PES has two TSC peaks in the temperature range from 20 to 220°C, consisting of an α peak at ∼ 210°C and a β peak whose peak temperature moves towards a higher temperature with an increasing poling temperature. Even when the sample was not poled, PES shows a spontaneous current with its peak at ∼ 210°C. Both the spontaneous current peak and the α peak were found to disappear when the sample had been heated to 230°C, keeping the external circuit closed. From such similarity of appearance and disappearance between the two peaks, it is concluded that they have the same origin. From the change in the spatial distribution of space charges inside the sample measured simultaneously with the TSC measurements, positive charges, probably due to K+ ions, existed nonuniformly in the sample from the beginning, and are thought to be responsible for the two peaks. From a similar study, the βpeak is considered to be due to polarization of ionic space charges during the poling process.
AB - In order to understand the dominant carrier species in electrical conduction in polyethersulfone (PES), thermally stimulated current (TSC) measurements were carried out under various conditions. It was found that PES has two TSC peaks in the temperature range from 20 to 220°C, consisting of an α peak at ∼ 210°C and a β peak whose peak temperature moves towards a higher temperature with an increasing poling temperature. Even when the sample was not poled, PES shows a spontaneous current with its peak at ∼ 210°C. Both the spontaneous current peak and the α peak were found to disappear when the sample had been heated to 230°C, keeping the external circuit closed. From such similarity of appearance and disappearance between the two peaks, it is concluded that they have the same origin. From the change in the spatial distribution of space charges inside the sample measured simultaneously with the TSC measurements, positive charges, probably due to K+ ions, existed nonuniformly in the sample from the beginning, and are thought to be responsible for the two peaks. From a similar study, the βpeak is considered to be due to polarization of ionic space charges during the poling process.
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U2 - 10.1109/94.506211
DO - 10.1109/94.506211
M3 - Article
AN - SCOPUS:0030165820
SN - 1070-9878
VL - 3
SP - 386
EP - 391
JO - IEEE Transactions on Dielectrics and Electrical Insulation
JF - IEEE Transactions on Dielectrics and Electrical Insulation
IS - 3
ER -