High-gain, hemi-spherical coverage, multi-sided flattened Luneburg lens antenna
A multiple flat sided modified Luneburg Lens antenna to provide a broadband and hemi-spherical coverage. The Modified Luneburg Lens antenna has a flat surface at the bottom and quadrilateral/hexagonal/octagonal/decagon/dodecagon flat surfaces at the sides (e.g., “cupcake shaped”) to manipulate the signal directivity of a radio frequency transmission or reception of interest in a plurality of octaves of bandwidth. The antenna may be configured with a Planar Ultra-Wideband Modular Array (PUMA) Antenna array structure with a broadband anti-reflective layer added between the two devices. The anti-reflective layer marries the two devices (lens and PUMA) and creates a broadband impedance matching between the new modified Luneburg lens antenna and dipoles of the PUMA array while maintaining the capability of the system to transmit and receive signals in a plurality of octaves of bandwidth.
1. A Luneburg lens antenna comprising a Luneburg lens having flattened side surfaces and a flat bottom,
wherein the flattened side surfaces are configured with Planar Ultrawideband Modular Arrays (PUMA) or
wherein the flattened side surfaces are configured with ultra-wideband (UWB) antenna structure.
2. The Luneburg lens antenna of claim 1 , wherein the lens has 4, 6, 8, 10, or 12 flattened side surfaces.
3. The Luneburg lens antenna of claim 1 , wherein the flattened side surfaces are in a lower hemisphere of the lens.
4. The Luneburg lens antenna of claim 1 , wherein the flattened side surfaces are configured with a broadband anti-reflective (AR) layer.
5. The Luneburg lens antenna of claim 4 , wherein the anti-reflective layer has an inhomogeneous graded dielectric permittivity profile.
6. The Luneburg lens antenna of claim 5 , wherein the inhomogeneous graded dielectric permittivity profile is Klopfenstein, Exponential, Gaussian, or Triangular.
7. The Luneburg lens antenna of claim 1 , wherein the Luneberg lens can achieve multiple simultaneous beams on a 180° elevation plane and 360° azimuthal plane.
8. The Luneburg lens antenna of claim 1 , wherein the Luneburg lens has an increased aperture efficiency of more than 80%.
9. The Luneburg lens antenna of claim 1 , wherein the intersection of adjacent scanned beams can be designed to be about 1 dB-3 dB below to peak gain value.
10. The Luneburg lens antenna of claim 1 , wherein the Luneburg lens has a wideband frequency coverage allowing for operation in multiple frequency bands simultaneously.
11. The Luneburg lens antenna of claim 1 , wherein the Luneburg lens is configured for multiple simultaneous beams.
12. The Luneburg lens antenna of claim 1 , wherein the Luneburg lens is configured to provide up to +/−90 degrees of sky coverage in a semi-hemispherical pattern.
13. The Luneburg lens antenna of claim 1 , wherein the UWB antenna structure is matched to the lens via an anti-reflective layer.
14. The Luneburg lens antenna of claim 13 , wherein the anti-reflective layer has an inhomogeneous graded dielectric permittivity profile.
15. The Luneburg lens antenna of claim 14 , wherein the inhomogeneous graded dielectric permittivity profile is Klopfenstein, Exponential, Gaussian, or Triangular.
16. The Luneburg lens antenna of claim 1 , wherein individual elements of the UWB antenna function as individual feeds for individual beams aimed in separate directions through the lens.
17. The Luneburg lens antenna of claim 7 , wherein the Luneburg lens can achieve multiple simultaneous beams on a 180° elevation plane and 360° azimuthal plane, with high gain and low side-lobes.
18. The Luneburg lens antenna of claim 10 , wherein the Luneburg lens has a 6:1 bandwidth ratio.
19. A method for manufacturing a Luneburg lens antenna comprising connecting a multi-sided flattened Luneburg lens to a PUMA antenna comprising removing a top dielectric layer of the PUMA antenna and using the multi-sided flattened Luneburg Lens to match the impedance of dipole elements of the PUMA to the Luneburg lens antenna.
20. The method of claim 19 , wherein the method does not comprise matching the impedance to free space.