Gyrotropic metamaterial structure
A gyrotropic metamaterial structure that include a plurality of chiral metamaterials forming one or more pairs of dipole structures. A plurality of lumped circuits are positioned between the one or more pairs of dipole structures. The lumped circuits have a plurality of subwavelengths antennas that are combined to change the polarization states of an incident polarized wave by producing Faraday-like rotation allowing for nomeciprocal propagation of the incident polarized wave.
1. A gyrotropic metamaterial structure comprising:
a plurality of chiral metamaterials forming one or more pairs of dipole structures; and
a plurality of lumped circuits positioned between the one or more pairs of dipole structures, the lumped circuits having a plurality of antennas that are combined to change the polarization states of an incident polarized wave by producing Faraday-like rotation allowing for nonreciprocal propagation of the incident polarized wave, wherein the lumped circuits comprise an amplifier structure that amplifies the power received by the incident polarized wave and provides a selected number of the one or pairs of dipole structures while isolating the remaining one or more pairs of dipole structures.
2. The gyrotropic metamaterial structure of claim 1 , wherein the chiral metamaterials are positioned on a plurality of dielectric boards to form the one or more pairs of dipole structures.
3. The gyrotropic metamaterial structure of claim 2 , wherein the one or more dipole structures comprise horizontal dipoles and vertical poles.
4. The gyrotropic metamaterial structure of claim 3 , wherein the horizontal dipoles and vertical dipoles are positioned on the dielectric boards.
5. The gyrotropic metamaterial structure of claim 4 , wherein the Faraday-like rotation comprises at least 3 degrees of rotation thru a 0.1-wavelength thick metamaterial layer.
6. The gyrotropic metamaterial structure of claim 5 , wherein the lumped circuits comprise a first inductor arrangement used for AC blocking.
7. The gyrotropic metamaterial structure of claim 6 , wherein the wherein the lumped circuits comprise a plurality of capacitors used for decoupling.
8. The gyrotropic metamaterial structure of claim 7 , wherein the lumped circuits comprise a second inductor arrangement for impedance matching with the amplifier structure.
9. A system for inducing gyrotropic properties in a metamaterial structure comprising:
a plurality of chiral metamaterials forming one or more pairs of dipole structures; and
a plurality of lumped circuits positioned between the one or more pairs of dipole structures, the lumped circuits having a plurality of antennas that are combined to change the polarization states of an incident polarized wave by producing Faraday-like rotation allowing for nonreciprocal propagation of the incident polarized wave, wherein the lumped circuits comprise an amplifier structure that amplifies the power received by the incident polarized wave and provides a selected number of the one or pairs of dipole structures while isolating the remaining one or more pairs of dipole structures.
10. The system of claim 9 , wherein the chiral metamaterials are positioned on a plurality of dielectric boards to form the one or more pairs of dipole structures.
11. The system of claim 10 , wherein the one or more dipole structures comprise horizontal dipoles and vertical poles.
12. The system of claim 11 , wherein the horizontal dipoles and vertical dipoles are positioned on the dielectric boards.
13. The system of claim 12 , wherein the Faraday-like rotation comprises 3 degrees of rotation thru a 0.1-wavelength thick metamaterial layer.
14. The system of claim 13 , wherein the lumped circuits comprise a first inductor arrangement used for AC blocking.
15. The system of claim 14 , wherein the wherein the lumped circuits comprise a plurality of capacitors used for decoupling.
16. The system of claim 15 , wherein the lumped circuits comprise a second inductor arrangement for impedance matching with the amplifier structure.
17. A method of inducing gyrotropic properties in a metamaterial structure comprising:
forming one or more pairs of dipole structures having a plurality of chiral metamaterials; and
producing Faraday-like rotation allowing for nonreciprocal propagation of an incident polarized wave by positioning a plurality of lumped circuits between the one or more pairs of dipole structures, the lumped circuits having a plurality of antennas that are combined to change the polarization states of the incident polarized wave, wherein the lumped circuits comprise an amplifier structure that amplifies the power received by the incident polarized wave and provides a selected number of the one or pairs of dipole structures while isolating the remaining one or more pairs of dipole structures.