19 research outputs found

    Lead-free piezoceramics - Where to move on?

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    Lead-free piezoceramics aiming at replacing the market-dominant lead-based ones have been extensively searched for more than a decade worldwide. Some noteworthy outcomes such as the advent of commercial products for certain applications have been reported, but the goal, i.e., the invention of a lead-free piezocermic, the performance of which is equivalent or even superior to that of PZT-based piezoceramics, does not seem to be fulfilled yet. Nevertheless, the academic effort already seems to be culminated, waiting for a guideline to a future research direction. We believe that a driving force for a restoration of this research field needs to be found elsewhere, for example, intimate collaborations with related industries. For this to be effectively realized, it would be helpful for academic side to understand the interests and demands of the industry side as well as to provide the industry with new scientific insights that would eventually lead to new applications. Therefore, this review covers some of the issues that are to be studied further and deeper, so-to-speak, lessons from the history of piezoceramics, and some technical issues that could be useful in better understanding the industry demands. As well, the efforts made in the industry side will be briefly introduced for the academic people to catch up with the recent trends and to be guided for setting up their future research direction effectively.ope

    Temperature-Dependent Phase Transitions in the Lead-Free Piezoceramics (1 – x – y)(Bi<sub>1/2</sub>Na<sub>1/2</sub>)TiO<sub>3</sub>–xBaTiO<sub>3</sub>–y(K<sub>0.5</sub>Na<sub>0.5</sub>)NbO<sub>3</sub> Observed by in situ Transmission Electron Microscopy and Dielectric Measurements

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    Lead-free piezoelectric (1-x-y)(Bi1/2Na1/2)TiO3-xBaTiO(3)-y(K0.5Na0.5)NbO3 (BNT-BT-KNN) ceramics were examined in situ under increasing temperature in the transmission electron microscope. Changing superstructure reflections indicate a transition from rhombohedral to tetragonal to cubic phase with broad coexistence regions. The additional evolution of the microstructure in combination with dielectric measurements leads to a model of two relaxor-type phase evolutions with temperature.close5
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