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Experimental realisation of a universal inverse-design magnonic device

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arxiv 2403.17724 v2 pith:DC26VNNB submitted 2024-03-26 physics.app-ph cond-mat.mtrl-sci

classification physics.app-phcond-mat.mtrl-sci
keywords devicedatadesignexperimentalinverseinverse-designprocessingreconfigurable
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In the field of magnonics, which uses magnons, the quanta of spin waves, for energy-efficient data processing, significant progress has been made leveraging the capabilities of the inverse design concept. This approach involves defining a desired functionality and employing a feedback-loop algorithm to optimise the device design. In this study, we present the first experimental demonstration of a reconfigurable, lithography-free, and simulation-free inverse-design device capable of implementing various RF components. The device features a square array of independent direct current loops that generate a complex reconfigurable magnetic medium atop a Yttrium-Iron-Garnet (YIG) rectangular film for data processing in the gigahertz range. Showcasing its versatility, the device addresses inverse problems using two algorithms to create RF notch filters and demultiplexers. Additionally, the device holds promise for binary, reservoir, and neuromorphic computing applications.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Exchange spin-wave propagation in Ga:YIG nanowaveguides

    cond-mat.other 2025-09 conditional novelty 6.0 of 10

    Spin waves in Ga:YIG nanowaveguides propagate at up to 600 m/s nearly independent of waveguide width, with decay lengths of 7 to 10 micrometers, several times faster than in YIG.

  2. Elimination of substrate-induced FMR linewidth broadening in the epitaxial system YIG-GGG by microstructuring

    cond-mat.mes-hall 2025-02 conditional novelty 5.0 of 10

    Microstructuring YIG films so they sit only in the homogeneous region of the GGG substrate's stray field eliminates the asymmetric FMR linewidth broadening at cryogenic temperatures.

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