Reflector array antenna with crossed polarization compensation and method for producing such an antenna

• US 9,112,281 B2
• Filed: 02/11/2011
• Issued: 08/18/2015
• Est. Priority Date: 03/19/2010
• Status: Active Grant

• Current Assignee: Thales SA
• Original Assignee: Thales SA
• Inventors: Bresciani, Daniele, Legay, Herv, Caille, Grard, Labiole, Eric
• Primary Examiner(s): SMITH, GRAHAM P
• Application Number:
  US13/636,252
• Publication Number:
  US 20130099990A1
• Time in Patent Office: 1,649 Days
• US Class Current: 1/1
• CPC Class Codes: H01Q 15/00 Devices for reflection, refraction, diffraction or polarisation of waves radiated from an antenna, e.g. quasi-optical devices variable for purpose of altering directivity H01Q3/00; arrangements of such devices for guiding waves H01P3/20; variable for purpose of modulation H03C7/02
• CPC Class Codes: H01Q 15/006 Selective devices having photonic band gap materials or materials of which the material properties are frequency dependent, e.g. perforated substrates, high-impedance surfaces
• CPC Class Codes: H01Q 15/12 functioning also as polarisation filter polarisation converters H01Q15/242
• CPC Class Codes: H01Q 15/141 Apparatus or processes specially adapted for manufacturing reflecting surfaces
• CPC Class Codes: H01Q 15/24 Polarising devices; Polarisation filters H01Q15/12, H01Q15/22 take precedence
• CPC Class Codes: H01Q 19/10 using reflecting surfaces
• CPC Class Codes: H01Q 3/46 Active lenses or reflecting arrays
• CPC Class Codes: Y10T 29/49016 Antenna or wave energy "plumbing" making

Abstract

A reflector array antenna with cross-polarization compensation including at least one radiating element having an etched pattern dissymmetric with respect to at least one direction X and/or Y of the plane XY of the radiating element, the dissymmetry of the pattern of the radiating element being calculated individually on the basis of a radiating element of the same symmetric pattern along the two directions X and Y, so as to engender a reflected wave having a controlled depolarization which opposes a depolarization, engendered in a plane normal to a direction of propagation, by the reflector array illuminated by a primary source.

Claims

1. A reflector array antenna with cross-polarization compensation comprising

a reflector array consisting of a plurality of elementary radiating elements regularly distributed and forming a reflecting surface;

and

a primary source intended to illuminate the reflector array;

wherein

the reflector array having a radiation diagram according to two orthogonal principal polarizations in a chosen direction of propagation with a chosen phase law;

each elementary radiating element has been produced in planar technology and comprises an etched pattern consisting of at least one metallic patch and/or of at least one radiating slot,

the metallic patch comprising, in a symmetric configuration, at least four sides that are pairwise opposite with respect to a center of the etched pattern and are disposed parallel to two directions X, Y of the plane XY of the radiating element, and

the radiating slot comprising, in a symmetric configuration of the radiating element, at least two branches that are diametrically opposite with respect to the center of the etched pattern and are disposed parallel to at least one of the directions X and/or Y of the radiating element; and

at least one radiating element of the reflector array comprises an etched pattern having a dissymmetric geometric shape with respect to at least one of the directions X and/or Y of the plane XY of the radiating element, the dissymmetry of the etched pattern of the radiating element consisting of an angular inclination of at least one side, respectively of at least one branch, of the geometric shape of the etched pattern with respect to the directions X and/or Y of the plane of the radiating element.

2. The antenna as claimed in claim 1, wherein an etched pattern comprises a metallic patch and at least two slots etched in the metallic patch, the slots forming at least four principal branches oriented respectively, pairwise, parallel to the directions X and Y in a symmetric configuration of the radiating element, the angular dissymmetries consist of angular rotations of the four principal branches of the slots, around the center of the etched pattern, in the plane XY.

3. The antenna as claimed in claim 1, wherein an etched pattern comprises, in a symmetric configuration, a metallic patch having a square geometric shape, the angular dissymmetries consist of an angular inclination of at least two opposite sides of the metallic patch of the radiating elements in one and the same sense or in opposite senses so as to transform the square shape respectively into a trapezium or into a parallelogram.

4. The antenna as claimed in claim 1, wherein several adjacent radiating elements of the reflector array comprise an etched pattern having a dissymmetric geometric shape with respect to at least one direction X and/or Y of the plane XY of each of said radiating elements, the angular inclinations of the side or of the branch of the geometric shape of the etched pattern of each of said radiating elements forming an angle of continuously progressive value from one radiating element to another adjacent radiating element on the reflecting surface.

5. The antenna as claimed in claim 1, wherein

the reflector array comprises several plane facets oriented according to different planes, each plane facet comprising a plurality of elementary radiating elements, and

at least one radiating element of each plane facet of the reflector array comprises an etched pattern having a dissymmetric geometric shape with respect to at least one direction X and/or Y of the plane XY of the facet to which the corresponding radiating element belongs.

6. A method for producing a reflector array antenna with cross-polarization compensation comprising:

producing a reflector array consisting of a plurality of elementary radiating elements regularly distributed and forming a reflecting surface;

illuminating the reflector array by a primary source;

producing each elementary radiating element in planar technology and comprising an etched pattern having a geometric shape that is symmetric with respect to two directions X and Y of the plane XY of the radiating element, the etched pattern consisting of at least one metallic patch and/or of at least one radiating slot;

introducing a dissymmetry, with respect to at least one of the directions X and/or Y, into the geometric shape of the etched pattern of at least one radiating element of the reflector array; and

calculating the dissymmetry on the basis of the radiation diagram of the desired far electromagnetic field in which the cross-polarization is zero and on the basis of the corresponding radiated electric field in the plane of the reflector array.

7. The method as claimed in claim 6, wherein the calculating the dissymmetry to be introduced into the radiating element comprises:

deducing, on the basis of the radiation diagram of the desired far electromagnetic field in which the cross-polarization is zero, the principal and cross-polarization components of the radiated electric field Er in the plane normal to the direction of propagation of the waves reflected by the reflector array;

calculating, for each radiating element of the reflector array, the components Erx and Ery of the corresponding radiated electric field in the plane of the reflector array;

calculating the components Eix and Eiy of the incident electric field Ei induced by the primary source on each radiating element of the reflector array; and

on the basis of the calculated components Erx, Ery, Eix and Eiy, deducing therefrom values of desired principal reflection coefficients Rxx, Ryy and cross-reflection coefficients Rxy, Ryx which must be induced by the corresponding dissymmetric radiating element.