ANISOTROPIC METAMATERIAL GAIN-ENHANCING LENS FOR ANTENNA APPLICATIONS

• US 20120280872A1
• Filed: 05/04/2012
• Published: 11/08/2012
• Est. Priority Date: 05/04/2011
• Status: Active Grant

• Current Assignee: Penn State Research Foundation
• Original Assignee: Penn State Research Foundation
• Inventors: Werner, Douglas H., Lier, Erik, Martin, Bonnie G., Turpin, Jeremiah P., Wu, Qi
• Granted Patent: US 8,912,973 B2
• Time in Patent Office: Days
• US Class Current: 343/753
• CPC Class Codes: H01Q 15/0053 Selective devices used as spatial filter or angular sidelobe filter
• CPC Class Codes: H01Q 15/02 Refracting or diffracting devices, e.g. lens, prism
• CPC Class Codes: H01Q 19/062 for focusing

Abstract

Examples of the present invention include metamaterials, including metamaterial lenses, having material properties that approximate the behavior of a material with low (0<n<1) effective index of refraction. Metamaterials may be designed and tuned using dispersion engineering to create a relatively wide-band low-index region. A low-index metamaterial lens created highly collimated beams in the far-field from a low-directivity antenna feed.

Claims

1. An apparatus, the apparatus being a metamaterial lens having an operating frequency,

the metamaterial lens having lens faces, the lens faces being planar, parallel, and spaced apart by a lens thickness,

the metamaterial including split-ring resonators arranged in resonator arrays, the resonator arrays being parallel to the lens faces,

the metamaterial further including end-loaded dipoles arranged in end-loaded dipole arrays, the end-loaded dipole arrays being perpendicular to the lens faces.

2. The apparatus of claim 1, the split-ring resonators being dual-split ring resonators, each dual-split ring resonator having two gaps in a conducting loop structure.

3. The apparatus of claim 1, the end-loaded dipoles being configured as volumetric end-loaded dipoles,

each volumetric end-loaded dipole being formed by four end-loaded dipoles in a square arrangement, the four end-loaded dipoles consisting of two pairs of spaced apart end-loaded dipoles,

the volumetric end-loaded dipole and a pair of split-ring resonators together having a cubic arrangement.

4. The apparatus of claim 1, the split-ring resonators and end-loaded dipoles being configured so that the metamaterial lens has a permittivity ε

_z and a permeability μ

_z at the operating frequency, where

μ

_z is the permeability along a direction normal to the lens faces,

ε

_z is the permittivity along a direction normal to the lens faces, and

ε

_z and μ

_z are both positive and less than 1.

5. The apparatus of claim 1, the operating frequency being in the range 1 GHz-100 GHz.

6. The apparatus of claim 5, the operating frequency being in the range 1 GHz-20 GHz.

7. The apparatus of claim 1, the apparatus comprising a three-dimensional arrangement of dielectric substrates supporting the split-ring resonators and the end-loaded dipoles,

the split-ring resonators and the end-loaded dipoles being conducting patterns formed on the dielectric substrates,

the three-dimensional arrangement of dielectric substrates defining a plurality of hollow dielectric cubes,

a dielectric cube of the plurality of hollow dielectric cubes supporting a pair of split ring resonators, spaced apart and supported on opposed faces of the dielectric cube, the dielectric cube further supporting end-loaded dipoles supported on the other faces of the dielectric cube.

8. The apparatus of claim 1, each end-loaded dipole including a conducting track having a first end and a second end, a first sinuous end-loading arm electrically connected to the first end, and a second sinuous end-loading arm electrically connected to the second end.

9. An apparatus, the apparatus comprising a metamaterial lens having a pair of lens faces, the lens faces being planar, spaced apart, and parallel to each other, the metamaterial lens including:

a first array of dual-split ring resonators, supported by a first dielectric substrate disposed parallel to the lens faces;

a first array of end-loaded dipoles, supported by a second dielectric substrate disposed perpendicular to the lens faces; and

a second array of end-loaded dipoles, disposed on a third dielectric substrate disposed perpendicular to both the first and second dielectric substrates.

10. The apparatus of claim 9, the apparatus further including a ground plane and an antenna feed, the ground plane being spaced apart from and parallel to the metamaterial lens, the antenna feed being located between the ground plane and the metamaterial lens, the apparatus being an directional antenna,

the antenna feed having an operating frequency, the metamaterial lens being configured so that the metamaterial lens collimates radiation from the antenna feed at the operating frequency.

11. The apparatus of claim 10, the antenna feed being a dual-polarization crossed-dipole antenna feed.

12. The apparatus of claim 10, the directional antenna being a circularly polarized antenna.

13. The apparatus of claim 10, the metamaterial lens having values of ε

_z and μ

_z that are both less than 1 at the operating frequency, where

ε

_z is a permittivity along a direction normal to the lens faces,

μ

_z is a permeability along a direction normal to the lens faces.

14. The apparatus of claim 10, the metamaterial including a volumetric end-loaded dipole arrangement configured to provide the metamaterial lens with a uniaxial permittivity at the operating frequency.