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Wave Manipulation by Topology Optimization - Solid Mechanics

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4.4 Effect of polarization and background material[P2] 25<br />

<br />

<br />

Figure 4.4 The cloak (a) for 1 symmetry line is near perfect at 0 o (b) whereas significant<br />

scattering is generated at 5 o (c) The dielectric layout (e) for the cloak optimized to operate<br />

in an interval from -5 o to 5 o are effective both for incident angles of 0 o (f) and 5 o (g). The<br />

robust design for small variation in the angle of incidence comes at the cost of increased<br />

scattering (d).<br />

make the cloak more versatile to various angles of incidence, more symmetry lines<br />

are added to the design domain at the cost of increased objective value.<br />

As mentioned above a slight variation in the incident angle results in a deteriorated<br />

cloaking performance. The cloak for 1 symmetry line is near perfect at<br />

0 o whereas significant scattering is generated at 5 o as shown in figures 4.4(b) and<br />

(c). A robust design for small perturbations in the angle of incidence is obtained<br />

<strong>by</strong> illuminating with uniform waves incident in an interval from -5 o to 5 o on the<br />

design domain and cylinder. The optimization is formulated as a min/max problem,<br />

i.e. the load case, which yields the highest scattering in each iteration step is<br />

minimized. The angle sweep in figure 4.4(d) and the fields patterns in figures 4.4(f)<br />

and (g) clearly shows that the cloak from figure 4.4(e) can be operated in a broader<br />

incident angle interval at the cost of increased scattering.<br />

4.4 Effect of polarization and background material[P2]<br />

Finishing the initial study we wanted to pursue a realization of an all-dielectric fully<br />

enclosing optical cloak designed <strong>by</strong> topology optimization. In a possible future experimental<br />

setup it may be easier to confine the polarized propagating wave in a<br />

material with higher index than free space and let spatial distributed areas of free<br />

space constitute the optimized design profile of the cloak. This is the ”inverse”<br />

case of the previous study, which was based on distributing material with a higher<br />

permittivity than the background material (free space). Intuitively, distributing dielectric<br />

material having a lower permittivity than the background material would<br />

result in cloaking performance on the same level or better, however, this is not the

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