Inverse grating problem: Efficient design of anomalous flexural wave reflectors and refractors
We present an extensive formulation of the inverse grating problem for flexural waves in
which the energy of each diffracted mode is selected and the grating configuration is then
obtained by our solving a linear system of equations. The grating is designed as a lineal
periodic repetition of a unit cell comprising a cluster of resonators attached at points whose
physical properties are directly derived by inversion of a given matrix. Although both active
and passive attachments can be required in the most-general case, it is possible to find …
which the energy of each diffracted mode is selected and the grating configuration is then
obtained by our solving a linear system of equations. The grating is designed as a lineal
periodic repetition of a unit cell comprising a cluster of resonators attached at points whose
physical properties are directly derived by inversion of a given matrix. Although both active
and passive attachments can be required in the most-general case, it is possible to find …
We present an extensive formulation of the inverse grating problem for flexural waves in which the energy of each diffracted mode is selected and the grating configuration is then obtained by our solving a linear system of equations. The grating is designed as a lineal periodic repetition of a unit cell comprising a cluster of resonators attached at points whose physical properties are directly derived by inversion of a given matrix. Although both active and passive attachments can be required in the most-general case, it is possible to find configurations with only passive (i.e., damped) solutions. This inverse design approach is an alternative to the design of metasurfaces for flexural waves, overcoming the limitations of gradient phase metasurfaces, which require a continuous variation of the surface’s impedance. When the grating is designed in such a way that all the energy is channeled into a single diffracted mode, it behaves as an anomalous refractor or reflector. The negative refractor is analyzed in depth, and it is shown that with only three scatterers per unit cell is it possible to build such a device with unitary efficiency.
American Physical Society
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