Wave Manipulation by Topology Optimization - Solid Mechanics
Wave Manipulation by Topology Optimization - Solid Mechanics
Wave Manipulation by Topology Optimization - Solid Mechanics
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4.1 Transformations Optics 21<br />
a spoon) is manipulated to generate a scattering pattern of a completely different<br />
object (e.g. a cup) and there<strong>by</strong> give the illusion of being that object. Unfortunately<br />
no materials in nature posses extreme properties (zero or negative), which makes<br />
realizations challenging. A possible remedy to achieve extreme material properties<br />
is to use metamaterials.<br />
4.1.1 Metamaterials<br />
The concept of metamaterials is to tailor micro structures with a periodicity much<br />
smaller than the wavelength of the incoming wave. The incoming wave does not<br />
”see” the inhomogeneity of the individual micro structure due to the structure being<br />
sub-wavelength. In stead the wave react as if the material is homogenous with<br />
effective material parameters given <strong>by</strong> the micro structure. This way it is possible to<br />
mix natural occurring materials in a clever way to obtain certain properties which<br />
were otherwise not possible. The idea of metamaterials originates from Veselago<br />
who theoretically studied the effect of both permittivity and permeability being<br />
negative simultaneously[71]. Many years later Pendry proposed the designs of artificial<br />
structured materials which would have effectively negative permittivity and<br />
permeability[72, 73] and not long after the first metamaterial with negative index<br />
of refraction was demonstrated[74]. Shortly after the initial papers on transformation<br />
optics a cloak with approximated extreme anisotropic material properties was<br />
realized in the micro-wave regime using a structured metamaterial[75]. However, realizations<br />
at optical frequencies of the extreme properties even with metamaterials<br />
still remain challenging due to bandwidth-limitations, material absorption and not<br />
to mention fabrication difficulties of sub-wavelength artificial structures.<br />
At a first glance the problem of systematic designing metamaterials using topology<br />
optimization to mitigate some of the challenges seems equivalent to designing<br />
materials with negative Poisson’s ratio[76] and negative thermal expansion[20].<br />
However, obtaining the effective parameters in a systematic and automated way,<br />
which is needed for the topology optimization method to be effective, has proven to<br />
be very challenging. The problem arises from branch ambiguities and that the parameters<br />
vary in a non-trivial way with the angle of incidence[77]. Several methods for<br />
extracting the effective parameters have been reported in the literature[78, 79, 80, 81]<br />
and based on such extraction methods metamaterials with negative permeability<br />
have been designed using topology optimization[82]. However, based on the study<br />
in [82] we do not find it worthwhile at the moment to proceed with double negative<br />
materials. In stead, we take a different path <strong>by</strong> designing the entire cloaking<br />
structure and there<strong>by</strong> <strong>by</strong>passing homogenization issues.<br />
4.1.2 All-dielectric cloaking<br />
Several alternative approaches to cloaking have emerged due to all the challenging<br />
problems that arises from extreme material parameters. The most prominent is the