This application is a U.S. non-provisional application claiming the benefit of French Patent Application No. 23 13998 filed on Dec. 12, 2023, the contents of which are incorporated herein by reference in their entirety.
The present invention relates to array antennas of the type which has a plurality of planar radiating elements (or “patch” antennas) fed in series—SFPA (“Series-Fed Patch Antenna”).
An antenna 101 results from the vertical series connection of a plurality of planar radiating elements 102i, of length Li and width Wi, making it possible to generate a vertically polarized wave, i.e., parallel to the axis V along which the different planar radiating elements of the antenna are arranged.
The antenna geometry relies directly on the TM10 resonance mode of each planar radiating element.
In the resonance mode, as illustrated on the central element 1023, the electric field between the ground plane and the metal plane which are constituents of the lower face and the upper face, respectively, of the planar radiating element is anti-symmetrical with respect to the horizontal axis H, which is the axis orthogonal to the vertical axis V. On the upper and lower horizontal edges, the electric field is homogeneous, i.e., is either positive or negative, and substantially constant. On the other hand, on the left- and right-hand edges, the electric potential varies and changes sign at the horizontal axis H.
Such a potential structure serves to generate a wave the electric field E of which is oriented along the vertical axis V, i.e., a vertically polarized wave.
Under such conditions, in order to propagate the resonance mode TM10 from one element to the neighbor thereof, a microstrip feed line 105i is used, which electrically connects the center of the horizontal edge, e.g., the upper edge, of a radiating element 102i and the center of the lower horizontal edge of the neighbor radiating element 102i+1. Moreover, the single line has a length equal to λg/2 (with λg the wavelength guided in the line) in order to invert the electric field between the two ends of the line, i.e., the field on the upper horizontal edge, with respect to the field on the lower horizontal edge, and thereby make resonate in phase the two radiating elements thereby connected.
In array antenna 101, the feed is provided by a single excitation point PV located on the axis V, but distant from the axis H.
For the entire antenna to resonate at the desired frequency, all radiating elements must also resonate at the same frequency. Consequently, the length Li of each element is substantially identical from one element to another and is close to λg/2 (the electric field of the lower and upper edges of the same element being in phase opposition). Strictly speaking, as each element does not have the same neighbors, different couplings are established, which shifts the resonance frequency. The shift may be compensated by adjusting the length Li of each element.
In polarimetric radar applications, such as Synthetic-Aperture Radar (SAR), antennas with orthogonal polarizations are required.
In the case of linear V/H polarization, to provide the symmetry of the radiation patterns and good integrability, it is necessary that antennas operating in horizontal polarization and same operating in vertical polarization have the same physical footprint.
However, at present, there is no SFPA antenna operating with a polarization oriented along the axis orthogonal to the axis of the array of planar radiating elements, i.e., under horizontal polarization when the radiating elements are vertically aligned.
Therefore, the goal of the present invention is to propose an SFPA antenna under horizontal polarization.
To this end, the subject matter of the invention is an array antenna of the type including a plurality of planar radiating elements fed in series, the planar radiating elements being arranged along a so-called vertical axis, a so-called horizontal axis, orthogonal to the vertical axis, intersects the latter at a central point, characterized in that, for operation under horizontal polarization, two successive planar radiating elements along the vertical axis are electrically connected to each other by a pair of differential lines, each line of the pair of differential lines having a length equal to an integer of wavelength guided along the line, an end of a line of the pair of differential lines being connected to a horizontal edge of a planar radiating element and the other end of the line being connected to the horizontal edge facing the other planar radiating element, the guided wavelength corresponding to the resonance frequency of the array antenna, a single planar radiating element of the plurality of planar radiating elements being provided with at least one horizontal excitation point, for an operation under horizontal polarization, the horizontal excitation point being outside the vertical axis, preferably in proximity to a vertical edge of the planar radiating element.
According to other advantageous aspects of the invention, the antenna includes one or a plurality of the following features, taken individually or according to all technically possible combinations:
The invention will be clearer upon reading the following description, given only as an example, but not limited to, and making reference to the drawings wherein:
An antenna 1 results from the series connection along a vertical axis V of a plurality of N planar radiating elements 2i (or elementary patch antennas) for an operation under horizontal polarization. N is an integer greater than or equal to two. Each element is indexed by an integer i between 1 and N.
Antenna 1 includes, e.g., five elements: a second lower element 21, a first lower element 22, a central element 23, a first upper element 24 and a second upper element 25.
The different planar radiating elements 2i are arranged along the vertical axis V. The axis orthogonal to the vertical axis V is the horizontal axis H. Same intersects the vertical axis V at the origin point O.
Antenna 1 is symmetrical with respect to vertical axis V.
Antenna 1 is symmetrical with respect to horizontal axis H.
The center O is thus a center of symmetry of antenna 1.
In the embodiment shown in
Each element 2i has a width Wi along axis H and a length Li along axis V.
In the embodiment shown in
Two successive planar radiating elements 2i and 2i+1 along axis V are electrically connected to each other by a pair of differential feed lines, e.g., microstrip lines 3i and 4i.
More precisely, the upper horizontal edge of element 2i and the lower horizontal edge of adjacent element 2i+1, situated immediately above element 2i, are connected, on the one hand, by a line 3i to the left of the vertical axis V and, on the other hand, by a line 4i to the right of the vertical axis V.
In this way, a differential coupling is established between two successive planar radiating elements of the array antenna.
The array antenna is excited by a suitable electrical signal, which is applied to the metal plane of one of the elements, preferably the central element 23, at an excitation point PH.
The point PH is situated on horizontal axis H, but outside vertical axis V, preferably close to an edge, e.g., the left vertical edge, of the central element 23 in order to provide good linear polarization.
Application of the electric excitation signal to the point PH serves to make element 23 resonate according to the mode TM01.
The electric field in the planar radiating element 23 is represented schematically in
Thereby, excitation of the radiating element according to the TM01 mode serves to generate a horizontally polarized wave, i.e., the electric field E of which is oriented along horizontal axis H.
In order to electrically associate two neighboring planar radiating elements, 2i and 2i+1, and make them resonate in phase, lines 3i and 4i have a length d′ equal to the guided wavelength λg (or to an integer multiple of the guided wavelength λg) so as to add in a phase shift of 360° between the electric field at one end of the lines and the electric field at the other end of lines 3i and 4i.
The wavelength λg is determined at the resonance frequency F0 of array antenna 1.
In this way, the same distribution of the electric field is obtained in each of elements 2i.
In other words, the radiating elements are excited in phase according to mode TM01.
The performance of antenna 1 is adapted in the same way as for antenna 101 according to the prior art.
The adjustment of widths Wi makes it possible to set the resonance frequency, and the adjustment of lengths Li makes it possible to give the aperture of the antenna a variable width by setting the gain of each radiating element and thereby creating a weighting for minimizing the side lobes.
Antenna 1 has a parameter S having the shape shown in
The radiation patterns, CV for antenna 101 and CH for antenna 1, are very close, both in elevation (plane containing axis V and the normal to the plane of the radiating elements) (
A very important datum when doing polarimetry is the cross-polarization, i.e., the energy radiated in the polarization orthogonal to the desired polarization. The lower the value, the more efficient the antenna is for a polarimetry application. The topology of antenna 1 makes it possible to achieve cross-polarization values on the order of −25 dB, without special adjustments.
In a variant, instead of being rectilinear, the interconnection lines between planar radiating elements may form one or a plurality of meanders. By folding the lines in this way, the spacing between the elements may be reduced, while maintaining the requirement on the length of the lines. More particularly, as a result, it is possible to impart the array antenna according to the invention with a physical footprint identical to that of the antenna shown in
In a variant, the microstrip lines may be replaced by coplanar lines or else by striplines.
In the embodiment shown in
More generally, it is possible to produce the feed by considering all known types of feed for patch antennas. In particular, it is possible to provide the feed by two vias, arranged along axis H, symmetrically with respect to center O of the element to be excited, and supplied in phase opposition (differential assembly). It is also possible to provide the feed by coupling through one or a plurality of slots arranged in a ground plane of the radiating element, vertically in line with the excitation point on the metallic plane forming the upper surface of the radiating element.
The advantage of using two excitation points for horizontal polarization operation and/or two excitation points for vertical polarization operation, makes it quite easy to gain 3 dB of radiated power in emission, while improving quality of the isolation with cross-polarization and symmetry of the diagram.
In the embodiment shown in
As illustrated in
For example, in the first variant of
For example, in the second variant of
In the two variants, the positioning of excitation point PH makes it possible to propagate the mode TM01 from the central element to the peripheral elements of the array antenna.
An antenna 401 combines the SFPA topology under horizontal polarization and the SFPA topology under vertical polarization, thereby making possible a dual polarization operation.
For this purpose, each radiating element 402i has a substantially square shape so as to be able to be excited according to the TM10 mode and the TM01 mode.
The central element 4023 is provided with two feed points, a point PH for exciting the horizontal polarization, and a point PV for exciting the vertical polarization. It is then possible to choose the desired polarization by suitably feeding each of the ports.
As explained hereinabove, two adjacent radiating elements are connected by three lines:
The lines that connect two radiating elements being of different length, one or other of the tracks no longer being rectilinear, but curvilinear (curved, bent, meandering, etc.)
To minimize the problems of coupling the signal from the horizontal polarization by common mode to the vertical polarization, the spacing and impedance of the differential lines can be varied.
Moreover, by exciting the two ports simultaneously with a selected phase shift, it is possible to have agility under polarization so as to generate circular polarizations or polarizations inclined with respect to axes H and V.
It is also possible to have the vertical configuration V and the horizontal configuration H which operate in two different frequency bands. For this purpose, it suffices to play with the vertical and horizontal dimensions of the unitary antenna elements.
The fields of application of the invention are radars, jammers, radios and data links, as well as multifunction systems using electronic scanning array antennas.
Most particularly, the present invention finds an application for radars with large numbers of unit antennas, where it may be advantageous to couple the radiating elements directly to each other by feed lines, and only have to excite the array antenna by a single element. As a result, it possible to reduce the number of transmission/reception modules for generating the electrical signal in transmission, or for acquiring the electrical signal in reception.
The present invention is also compatible with conventional bandwidth broadening techniques, such as stacked patch antennas, as presented in the reference A. A. Serra, P. Nepa, G. Manara, G. Tribellini and S. Cioci, “A Wide-Band Dual-Polarized Stacked Patch Antenna,” in IEEE Antennas and Wireless Propagation Letters, Vol. 6, pp. 141-143, 2007, doi: 10.1109/LAWP.2007.893101.
| Number | Date | Country | Kind |
|---|---|---|---|
| 2313998 | Dec 2023 | FR | national |