Abstract
In this chapter, we describe the development and properties of the first experimental dynamic magnonic crystal devices and highlight certain aspects of the intriguing new physics that they have to offer us. We discuss the significance of the dynamic magnonic crystal both in the context of the furtherance and technological application of magnonics, and in the understanding of general wave dynamics in metamaterial systems.
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Notes
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Approximately two orders of magnitude lower than all other practical experimental materials.
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Note that backward volume magnetostatic spin waves (BVMSWs) are called so because their dispersion relation ω(k) has a negative slope, implying that the group and phase velocities of the waves are in opposite directions. We stress, however, that none of the results we describe later in this chapter hinge on this unusual physics; all may be generalized to any waves having a symmetric dispersion function ω(k)=ω(−k) propagating in a dynamic artificial crystal structure.
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Acknowledgements
Financial support from the Deutsche Forschungsgemeinschaft (Grant No. SE 1771/1-2). Dynamic magnonic crystals were fabricated with the technical assistance of the Nano-Structuring Center, TU Kaiserslautern. A.D.K. is grateful for the support of Magdalen College, Oxford.
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Chumak, A.V., Karenowska, A.D., Serga, A.A., Hillebrands, B. (2013). The Dynamic Magnonic Crystal: New Horizons in Artificial Crystal Based Signal Processing. In: Demokritov, S., Slavin, A. (eds) Magnonics. Topics in Applied Physics, vol 125. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-30247-3_17
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