Omnidirectional radiofrequency antenna with conical reflector

• US 6,084,552 A
• Filed: 07/27/1998
• Issued: 07/04/2000
• Est. Priority Date: 02/06/1996
• Status: Expired due to Fees

• Current Assignee: Qinetiq Limited (QinetiQ Group PLC)
• Original Assignee: The secretary of state for defence in her Britannic Majesty's Government of the United Kingdom of Great Britain And Northern Ireland
• Inventors: Robertson, Duncan A, May, Peter B
• Primary Examiner(s): Ho, Tan
• Application Number:
  US09/117,268
• Time in Patent Office: 708 Days
• Field of Search: 343/753, 343/754, 343/755, 343/756, 343/786, 356/247, 356/172, 356/153, 385/124, 385/127, 369/44, 250/353, 250/393
• US Class Current: 343/753
• CPC Class Codes: H01Q 19/10 using reflecting surfaces
• CPC Class Codes: H01Q 19/102 wherein the surfaces are of convex toroïdal shape biconical horns H01Q13/04

Abstract

An antenna system for providing radiation over substantially 360° in azimuth by illuminating a conical reflector with a radiation beam having a frequency distribution with a local minimum which is coincident with the point of the reflector thus avoiding scattering. Preferably the radiation intensity distribution is annular, most preferably being Laguerre-Gaussian in nature.

Claims

1. A method of transmitting radiofrequency radiation over an azimuth angle of substantially 360°

, said method comprising;

providing a substantially conical reflector;

illuminating said reflector with a beam having a Laguerre-Gaussian intensity distribution; and

locating the minimum of the Laguerre-Gaussian distribution coinciding with the apex of the reflector, wherein the arrangement of the beam and reflector being such that the radiation reflected from the reflector is divergent.

2. A radiofrequency antenna for providing transmission over substantially 360°

in azimuth, said antenna comprising;

a conical reflector;

a source of radiofrequency radiation illuminating said reflector, said radiation having a beam directed at the apex of said conical reflector and with a Laguerre-Gaussian intensity distribution, the minimum of the Laguerre-Gaussian distribution coinciding with the apex of the reflector, the beam and the reflector interrelated such that the radiation reflected from the reflector is divergent.

3. The radiofrequency antenna of claim 2 and further including a source of radiation having a Fundamental Hermite-Gaussian intensity distribution and means for converting said radiation to radiation having a Laguerre-Gaussian intensity distribution.

4. The radiofrequency antenna of claim 3 where the means for converting radiation having a Fundamental Hermite-Gaussian intensity distribution comprises a spiral phaseplate.

5. The radiofrequency antenna of claim 4 and further including means for collimating the radiation.

6. The radiofrequency antenna of claim 5 where the means for collimating the radiation having a Fundamental Hermite-Gaussian intensity distribution comprises at least one lens.

7. The radiofrequency antenna of claim 6 and further including means for controlling the angular coverage in elevation of the output radiation of the radiofrequency antenna.

8. The radiofrequency antenna of claim 7 where the means for controlling the angular coverage in elevation of the output radiation of the radiofrequency antenna comprises at least one lens.

9. The radiofrequency antenna of claim 8 where the radiation having a Fundamental Hermite-Gaussian intensity distribution is linearly polarised.

10. The radiofrequency antenna of claim 9 and further including means for converting said linearly polarised radiation to circularly polarised radiation.

11. The radiofrequency antenna of claim 10 where the means for converting said linearly polarised radiation to circularly polarised radiation comprises a quarter wave plate.