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The layers that the energy passes through are listed in Table 1 and are shown on the x-axis in Figure 5. e. 5% at steady state is yielded. This is shown in Figure 5 as the "Reflection Alone" trace. When the "strain response" nonlinear components are added for the BST and the NiTi, over 45% of the initial input energy is damped, as shown in Figure 5 with the "With 'Smart' Behavior" trace. This damping can be increased to almost 90%; if the BST and NiTi are deposited in such a way that a partial "phase change" occurs during transmission of the vibrational wave.

Technol. A, 22, 361-5 (2004). W. K Yun, Y. J. -T. Hsu. " Thin Solid Films, 146, 174-80(1999). K. P. Gila, J. N. D. R. Abemathy, F. J. Pearton. " J. Electrochem. Soc, 149, G128-G130 (2002). 7 V. Dimitrova, D. Manova, and E. Valcheva. " Mater. Sei. Eng. B 68,1-4(1999). J. Schulte and G. Sobe. " Thin Solid Films, 324 (1998): 19-24. N. Cheng. " Thin Solid Films, 358, 215-22 (2000). 54 Advances in Electronic and Electrochemical Ceramics K. Jagannadham, K. Sharma, Q. Wei, R. Kalyanraman, and J. Narayan.

The maximum dielectric constant, K, was approximately 250300. 4 NRL, then, conducted a further study using the same methods on the BaO-TiC>2-Al203-Si02 system, with the intent of producing BaTiCb as the crystalline phase. 10 These results indicated that a final energy density of 6 to 8 joules/cm is possible, but the one issue with BaTiCh was the energy density results at high field conditions. X)SrxTi03 and hence lower the Curie point of the ferroelectric phase. In this way, at room temperature the BST is a paraelectric phase and therefore is expected to maintain its dielectric properties at high field.

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