Photonic crystals in biology
Photonic crystals in biology
Photonic crystals in biology
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Poster Session, Tuesday, June 15<br />
Theme A1 - B702<br />
The Interaction of Electromagnetic Waves from S<strong>in</strong>gle Sheet of Spherical Nano-Elements Meshed on<br />
Spherical Shell<br />
Taner Sengor<br />
Department of Electronics and Communication Eng<strong>in</strong>eer<strong>in</strong>g, Yildiz Technical University, Istanbul 34349, Turkey<br />
Abstract—Possibilities creat<strong>in</strong>g nano-structures provid<strong>in</strong>g unnatural electromagnetic characteristics are given. Co-r<strong>in</strong>gs <strong>in</strong><br />
nano-metric dimensions ly<strong>in</strong>g on different azimuth and/or equatorial planes are def<strong>in</strong>ed as nano-element provid<strong>in</strong>g such<br />
possibilities. These nano-elements are meshed on spherical shells. The <strong>in</strong>teraction of electromagnetic wave with both of<br />
nano element and meshed spherical surface are studied. For an example, the necessary configurations for both of the<br />
electromagnetically effective cloak<strong>in</strong>g and the optically effective cloak<strong>in</strong>g (<strong>in</strong>visibility) are given for this purpose.<br />
The loops are used at meta-material applications,<br />
frequently. The us<strong>in</strong>g of circular loop comb<strong>in</strong>ations on nonplanar<br />
substrates is offered <strong>in</strong> this paper to consider <strong>in</strong> both of<br />
artificial material studies and cloak<strong>in</strong>g applications [1]. Two<br />
basic comb<strong>in</strong>ations are used: i) Parallelly located circular loop<br />
ly<strong>in</strong>g on latitude circles on a spherical core. We call this<br />
element smooth r<strong>in</strong>g ball. ii) Intersect<strong>in</strong>g circular loop ly<strong>in</strong>g<br />
on meridian circles on a spherical core. We call this element<br />
cross r<strong>in</strong>g ball. The circular loop is located on a spherical core<br />
hav<strong>in</strong>g the radius a, that is sufficiently small. The magnitudes<br />
of the currents on the circular loops must be sufficiently large.<br />
These necessary conditions give a chance to generate TM θ<br />
waves, which we call pr<strong>in</strong>cipal wave. Additionally us<strong>in</strong>g of<br />
materials hav<strong>in</strong>g time <strong>in</strong>dependent permittivity and θ-<br />
<strong>in</strong>dependent permeability br<strong>in</strong>gs the property of TE waves to<br />
the previous TM θ waves. We call the last TM θ -TE waves<br />
secondary wave. The arrangements at the circumstance of the<br />
r<strong>in</strong>g balls br<strong>in</strong>g the property of TM r waves to the waves under<br />
the discussion. The last property enforces to br<strong>in</strong>g the<br />
behavior of TE θ waves to the pr<strong>in</strong>cipal wave; therefore the<br />
pr<strong>in</strong>cipal wave ga<strong>in</strong>s the property of TEM θ waves. The last<br />
property enforces add<strong>in</strong>g the behavior of TM waves to the<br />
pr<strong>in</strong>cipal wave. So the wave under the discussion ga<strong>in</strong>s the<br />
property of TEM waves. After all, the use of suitably built up<br />
layers of almost zero epsilon material and/or perfectly<br />
conduct<strong>in</strong>g material br<strong>in</strong>gs the behavior of TE r waves to the<br />
waves under the discussion. The f<strong>in</strong>al wave is ga<strong>in</strong>ed a<br />
propagation characteristic fitt<strong>in</strong>g on the propagation<br />
characteristics of TEM θ waves and almost TEM r waves.<br />
The above said characteristic gives a way to produce<br />
suitable objects with spherical shapes <strong>in</strong> nanometer scale;<br />
those change the RCS of objects and therefore provide us to<br />
built structures demonstrat<strong>in</strong>g effective electromagnetic<br />
cloak<strong>in</strong>g property. We call this structure effective<br />
electromagnetic cloak<strong>in</strong>g device.<br />
In summary, several compositions of nano r<strong>in</strong>gs on<br />
spherical substrates are studied. The necessary conditions for<br />
both of the electromagnetically effective cloak<strong>in</strong>g and the<br />
optically effective cloak<strong>in</strong>g are generated.<br />
*Correspond<strong>in</strong>g author: sengor@yildiz.edu.tr<br />
[1] T. Sengor, " Properties of a non-planar metamaterial elements: r<strong>in</strong>g<br />
resonators on a spherical substrate, " The First International Congress on<br />
Advanced Electromagnetic Materials <strong>in</strong> Microwaves and Optics, Italy,<br />
Rome, Metamaterials 2007 Congress, 22-26 October 2007.<br />
[2] T. Sengor, Metamaterials Congress, Aug 30th-Sept 4th 2009, London, UK<br />
6th Nanoscience and Nanotechnology Conference, zmir, 2010 302