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By K. M. Nair, Shashank Priya

Prior to now many years, knowing of the technology and expertise powering digital fabrics has performed an important function in enjoyable social wishes via constructing digital units for car, telecommunications, army, and scientific functions. This quantity incorporates a selection of chosen papers from the foreign symposia on complicated Dielectric fabrics and digital units and Ferroelectrics and Multiferroics awarded throughout the fabric technology and expertise convention held in Pittsburgh in October 2009. it's a one-stop source for lecturers at the most vital concerns in advances in electroceramic materials.Content:

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Ceram. S o c , 42 (1959) 438 4) R. Wang, R-J. Xie, K. Hanada, K. Matsusaki, H. Bando, M. Itoh, Phys. Stat. , (a) 2002,6 (2005) R57 5) E. Li, R. Suzuki, T. Hoshina, H. Takada, T. Tsurumi, Appl. Phys. Lett. 94 (2009) 132903 6) J . F u . R . Z u o . X . , Mater. Res. Bull. 44 (2009) 1188 7) M. Matsubara, K. Kikuta, S. Hirano, J. Appl. , 97(11) (2005) 114105 8) M. Matsubara, T. Yamaguchi, W. Sakamoto, K. Kikuta, T. Yogo, and S. Hirano, J. Am. Ceram. S o c , 88 (2005) 1190 9) Y. Watanabe, K. Sumida, S.

A) 2002,6 (2005) R57 5) E. Li, R. Suzuki, T. Hoshina, H. Takada, T. Tsurumi, Appl. Phys. Lett. 94 (2009) 132903 6) J . F u . R . Z u o . X . , Mater. Res. Bull. 44 (2009) 1188 7) M. Matsubara, K. Kikuta, S. Hirano, J. Appl. , 97(11) (2005) 114105 8) M. Matsubara, T. Yamaguchi, W. Sakamoto, K. Kikuta, T. Yogo, and S. Hirano, J. Am. Ceram. S o c , 88 (2005) 1190 9) Y. Watanabe, K. Sumida, S. Yamada, S. Sago, S. Hirano, K. Kikuta, Jpn. J. Appl. , 47(5) (2008) 3556 Table 1 Electric properties of KNN based ceramics kp £r Qm d}3 (pC/N ) KNN-KCN 40.

SBiojTi03 samples sintered at 1030°C for 5 and 20 h were 92 and 96%, respectively, of the theoretical density of KBT. Like with the pure KBT sample, the XRD patterns of the NBT-KBT samples after both calcinations showed a predominant perovskite matrix phase and wide peaks of low intensities, suggesting a pseudocubic structure and smaller crystallites. No secondary-phase peaks could be observed from the XRD spectra. After the sintering of the pellets the peaks in the XRD patterns became narrow and sharp, with the appearance of peak splitting due to a lowering of the symmetry after cooling down to room temperature (Figure 3).

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