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<table>Inverse temperature-dependent variation of ln (real part of complex ac conductivity) for <svg height="15.0875" id="M238" style="vertical-align:-2.3205pt" version="1.1" viewbox="0 0 47.087502 15.0875" width="47.087502" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink">
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</svg>BNT-<svg height="7.9499998" id="M239" style="vertical-align:-0.1638pt" version="1.1" viewbox="0 0 9.625 7.9499998" width="9.625" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink">
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</svg>BT (<svg height="11.125" id="M240" style="vertical-align:-0.1638pt" version="1.1" viewbox="0 0 37.212502 11.125" width="37.212502" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink">
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</svg>, 0.02, 0.04, 0.05, 0.06, 0.08, and 1) ceramics at 10 kHz.</table>

International Scholarly Research Notices

fig7

Figure 7

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International Scholarly Research Notices

Electrical Conduction in Ceramic by Complex Impedance/Modulus Spectroscopy

Figure 7