# Patent

## Title
Combining multiple-port patch antenna

## Abstract

An exemplary apparatus providing an antenna for radiating electromagnetic energy is disclosed as having: a first dielectric substrate having opposite first and second surfaces, a patch of conducting material disposed on the first surface, a ground plane of conducting material disposed of the second surface, at least three input means coupled to a plurality of microstrip feed lines wherein the microstrip feed lines have an aspect ratio suitably configured to maximize antenna bandwidth. Disclosed features and specifications may be variously controlled, adapted or otherwise optionally modified to improve and/or modify the performance characteristics of the antenna. Exemplary embodiments of the present invention generally provide an antenna for providing wideband power combining and wideband radiation functions.

## Background
FIELD OF INVENTION
The present invention generally provides improved systems, compositions and methods for an improved antenna for radiating electromagnetic energy; and more particularly, representative and exemplary, embodiments of the present invention generally relate to an improved microstrip patch antenna.
BACKGROUND OF INVENTION
Certain applications require the power from multiple microwave sources to be combined in order to create a single high-power output signal, which is then radiated by a single antenna. This is typically accomplished using one or more power combiners, such as microstrip power combiners, that combine the power from multiple amplifiers and feed it to a conventional single- or two-port antenna using one or two microstrip lines. Power combiners, however, occupy a significant amount of circuit-board space. If the outputs of a large number of microwave sources are to be combined, the area occupied by power-combining circuitry can be a significant fraction of the total circuit board area. Problems can also occur with this power-combining approach for high-power applications since all the power is concentrated into one or two microstrip lines, which may be very narrow. If too much power is fed through the microstrip lines, it may cause an electrical breakdown.
Furthermore, these same applications sometimes require some degree of polarization diversity, i.e., the ability to radiate different polarizations (such as right- or left-handed circular polarization, or horizontal or vertical linear polarization) from a single antenna.
Choi et al., “A V-band Single-Chip MMIC Oscillator Array Using a 4-port Microstrip Patch Antenna,” 2003 IEEE MTT-S Digest Volume 2, June 2003, pp. 881-884, describes an array of four field-effect transistor (FET) oscillators whose outputs are combined using a four-port patch antenna. Two parallel pairs of FET oscillators operating in a push-pull mode drive opposite sides of a rectangular patch antenna, which combines the outputs of the four oscillators and provides feedback due partly to impedance mismatches at each port, resulting in a strongly coupled system. That is, the antenna is an integral part of the oscillator array, and cannot be considered separately. This configuration is effective as a power combiner because the impedance mismatch is not detrimental to system operation. It cannot be used, however, if each port is to be driven by independent microwave sources or if circularly polarized radiation is desired.
U.S. Pat. No. 5,880,694 issued to Wang et at. discloses a phased-array antenna using a stacked-disk radiator. Two orthogonal pairs of excitation probes are coupled to a lower excitable disk. The polarization of the antenna can be single linear polarization, dual linear polarization, or circular polarization, depending on whether a single pair or two pairs of excitation probes are excited. This antenna, however, cannot be used as a power combiner for multiple sources.
U.S. Pat. No. 6,549,166 issued to Bhattacharyya et al. discloses a four-port patch antenna capable of generating circularly-polarized radiation. This antenna comprises a radiating patch, a ground plane having at least four slots placed under the radiating patch, at least four feeding circuits (one for each slot), and a hybrid network each of whose outputs feed one of the feed networks and having a right-hand circularly polarized input port, a left-hand circularly polarized input port, and two matched terminated ports. The input impedances at the individual ports of the antenna need not be matched to those of the feed lines; the two matched terminated ports of the hybrid network absorb most of the energy reflected by the antenna, increasing the return loss at the input port. Use of the hybrid network prevents use of the antenna for combining the outputs of more than two microwave sources. In addition, the hybrid network requires a significant area for implementation.
Hence, there is a need in the art for an improved system or method for combining the power from multiple microwave sources that reduces the need for conventional power-combining circuitry and is suitable for high-power applications and for radiating microwave energy with greater polarization diversity than prior art systems.
SUMMARY OF THE INVENTION
In representative aspects, the present invention provides systems, devices and methods for providing an antenna for radiating electromagnetic energy utilizing a first dielectric substrate, a patch of conducting material, a ground plane of conducting material, and at least three input means comprising microstrip feed lines. Advantages of the present invention will be set forth in the Detailed Description which follows and may be apparent from the Detailed Description or may be learned by practice of exemplary embodiments of the invention. Still other advantages of the invention may be realized by means of any of the instrumentalities, methods or combinations particularly disclosed herein.



BRIEF DESCRIPTION OF THE DRAWINGS
Representative elements, operational features, applications and/or advantages of the present invention reside in the details of construction and operation as more fully hereafter depicted, described and claimed—reference being made to the accompanying drawings forming a part hereof, wherein like numerals refer to like parts throughout. Other elements, operational features, applications and/or advantages may become apparent in light of certain exemplary embodiments recited in the Detailed Description, wherein:
FIGS. 1a-1d are diagrams of a four-port implementation of an antenna designed in accordance with an illustrative embodiment of the teachings of the present invention;
FIG. 1a shows a three-dimensional view. FIG. 1b shows a side view. FIG. 1c shows a front view, and FIG. 1d shows a back view.
FIG. 2 is a diagram showing the location of the feed points in a circular patch in accordance with an illustrative embodiment of the teachings of the present invention;
FIG. 3 is a graph of measured effective return loss vs. frequency in a prototype four-port antenna designed in accordance with an illustrative embodiment of the teachings of the present invention;
FIGS. 4a and 4b are illustrations showing the two orthogonal linearly polarized outputs and the corresponding inputs of a four-port antenna designed in accordance with an illustrative embodiment of the teachings of the present invention;
FIG. 5a is a diagram of an illustrative embodiment of the present invention with an equilateral triangular patch and three input ports;
FIG. 5b is a diagram of an illustrative embodiment of the present invention with a circular patch and three input ports;
FIG. 6 is a diagram of an illustrative embodiment of the present invention with a sixteen-sided patch and eight input ports;
FIGS. 7a and 7b are illustrations showing the two orthogonal linearly polarized outputs of an eight-port antenna illustrative of the teachings of the present invention;
FIGS. 8a and 8b are diagrams of an illustrative embodiment of an antenna of the present invention with an alternative method for feeding the antenna. FIG. 8a shows a normal view and FIG. 8b shows an exploded view;
FIGS. 9a and 9b are diagrams showing the current best mode embodiment of the present invention. FIG. 9a shows a normal view and FIG. 9b shows an exploded view;
FIG. 10 is a graph of measured effective return loss vs. frequency in a prototype four-port antenna designed in accordance with an illustrative embodiment of the teachings of the present invention;
FIGS. 11a and 11b are diagrams of a sixteen-port version of the antenna designed in accordance with an illustrative embodiment of the teachings of the present invention;
FIG. 12 is a graph of measured effective return loss vs. frequency in a prototype sixteen-port antenna designed in accordance with an illustrative embodiment of the teachings of the present invention;
FIG. 13 is a diagram of an illustrative system for radiating high power microwave energy designed in accordance with the teachings of the present invention;
FIGS. 14a, 14b and 14c are diagrams showing construction of feed lines for a four-input system for radiating high power microwave energy designed in accordance with the teaching of the present invention;
FIG. 15 is a diagram showing construction of feed lines for an eight-input system for radiating high power microwave energy designed in accordance with the teaching of the present invention;
FIG. 16 is a diagram showing an exploded view of an exemplary system for radiating high power microwave energy designed in accordance with the teaching of the present invention; and
FIG. 17 is a graph of the calculated effective reflection coefficient of the optimized patch antenna shown in FIG. 15.



Elements in the Figures are illustrated for simplicity and clarity and have not necessarily been drawn to scale. For example, the dimensions of some of the elements in the Figures may be exaggerated relative to other elements to help improve understanding of various embodiments of the present invention. Furthermore, the terms “first”, “second”, and the like herein, if any, are generally used for distinguishing between similar elements and not necessarily for describing a sequential or chronological order. Moreover, the terms “front”, “back”, “top”, “bottom”, “over”, “under”, and the like, if any, are generally employed for descriptive purposes and not necessarily for comprehensively describing exclusive relative position or order. Any of the preceding terms so used may be interchanged under appropriate circumstances such that various embodiments of the invention described herein, for example, are capable of operation in orientations and environments other than those explicitly illustrated or otherwise described.
DETAILED DESCRIPTION OF EXEMPLARY EMBODIMENTS
The following representative descriptions of the present invention generally relate to exemplary embodiments and the inventor's conception of the best mode, and are not intended to limit the applicability or configuration of the invention in any way. Rather, the following description is intended to provide convenient illustrations for implementing various embodiments of the invention. As will become apparent, changes may be made in the function and/or arrangement of any of the elements described in the disclosed exemplary embodiments without departing from the spirit and scope of the invention.
The present invention eliminates the need to pre-combine the outputs of multiple microwave sources by providing a patch antenna with multiple input ports. The power sources are coupled directly to the antenna, and the power is combined in the antenna itself, rather than using separate circuit-based power combiners. The area that would otherwise be occupied by power combiners can be eliminated or used for other purposes. The total radiated power is spread over a much larger volume than if a single feed were to be used, reducing the possibility of overheating or electrical breakdown due to excessively high electromagnetic fields. The invention uses reflection cancellation to increase the return loss at each input port and thereby increase the overall bandwidth of the antenna system. By properly locating the feed points, the direct reflections from the individual ports are cancelled by the signals coupled from the other ports, eliminating the need for additional impedance-matching circuitry. Furthermore, a single multiple-port patch antenna designed in accordance with the present teachings can radiate right-handed circular polarization, left-handed circular polarization, or any desired linear polarization when driven by the appropriate set of inputs.
FIGS. 1a-1d are diagrams of a four-port implementation of an antenna 10 designed in accordance with an illustrative embodiment of the teachings of the present invention. FIG. 1a shows a three-dimensional view, FIG. 1b shows a side view. FIG. 1c shows a front view, and FIG. 1d shows a back view. The assembled antenna 10 includes a microstrip patch antenna and at least three input ports 22. The patch antenna 10 is comprised of a dielectric substrate 12 with opposite first and second surfaces 14 and 16, a patch 18 of conducting material disposed on the first surface 14, and a ground plane 20 of conducting material disposed on the second surface 16. Note that in FIG. 1b, the thickness of the patch 18 and ground plane 20 are exaggerated for illustrative purposes. The patch itself can be fabricated using conventional printed-circuit etching techniques.
In the illustrative embodiment of FIGS. 1a-1d, the patch 18 is circular. The size of the patch 18 is determined primarily by the desired frequency of operation. It is well known that the resonant frequencies of a circular patch of radius a are approximated by:




  
    
      
        f
        =
        
          
            
              χ
              mn
            
            ⁢
            c
          
          
            2
            ⁢
            π
            ⁢
            
              
            
            ⁢
            a
            ⁢
            
              
                
                  μ
                  r
                
                ⁢
                
                  ɛ
                  r
                
              
            
          
        
      
    
    
      
        [
        1
        ]
      
    
  




where χ′mn represents the nth zero of the derivative of the mth-order Bessel function Jm(x) of the first kind [i.e., J′mn(χ′mn)=0]. The frequency of interest is the lowest-order resonant frequency for which m=1, n=1, and χ′11=1.841. For example, if μr=1, εr=2.2, and f=1.03 GHz, the patch radius should be a=2.264 inches.
A plurality of input ports 22 are coupled to the patch 18. In the illustrative embodiment of FIGS. 1a-1d, the antenna 10 is fed by four coaxial ports 22, each attached directly to its feed point 26, i.e., the point at which the center conductor 24 of the coaxial port 22 is attached to the patch 18. The outer conductors of the coaxial ports 22 are connected to the ground plane 20.
FIG. 2 is a diagram showing the location of the feed points 26 in a circular patch 18 of radius a. In this embodiment, each input port 22 is placed directly opposite of its feed point 26, with the feed points 26 on the patch side 14 of the substrate 12 and the input ports 22 on the other side 16 of the substrate 12. In accordance with the teachings of the present invention, the feed points 26 are equally distributed around a circle of radius d having the same center as the patch 18. In FIG. 2, the four feed points are labeled 1, 2, 3, and 4, with port 1 opposite port 3, and port 2 opposite port 4.
Proper choice of patch size and proper placement of the feed points are the most critical elements in the design and construction of the present invention. With a single-port patch antenna, the return loss is maximized by placing the port at the proper distance from the center of the patch. With a four-port patch antenna, one cannot simply place the ports in the same locations they would occupy in a one-port design, since there is cross-coupling between ports that is not present in a single-port design. That is, if all four ports are excited simultaneously, the reflected wave at port 1, for example, is composed of contributions from all four ports: a directly-reflected wave from port 1, and cross-coupled waves from ports 2, 3, and 4.
In accordance with the teachings of the present invention, the feed points are placed so that the sum of the directly-reflected and cross-coupled waves is very small, i.e., the direct reflection from port 1 is nearly, cancelled by the cross-coupled waves from ports 2, 3, and 4. By, this reflection-cancellation technique, each port is matched without the need for additional impedance-matching elements.
If the amplitudes of the incident waves at the four ports are denoted A1, A2, A3, and A4, the amplitudes of the reflected waves B1, B2, B3, and B4 at each of the four ports are given by:




  
    [
    
      
        
          
            B
            1
          
        
      
      
        
          
            B
            2
          
        
      
      
        
          
            B
            3
          
        
      
      
        
          
            B
            4
          
        
      
    
    ]
  
  =
  
    
      [
      
        
          
            
              S
              11
            
          
          
            
              S
              12
            
          
          
            
              S
              13
            
          
          
            
              S
              14
            
          
        
        
          
            
              S
              21
            
          
          
            
              S
              22
            
          
          
            
              S
              23
            
          
          
            
              S
              24
            
          
        
        
          
            
              S
              31
            
          
          
            
              S
              32
            
          
          
            
              S
              33
            
          
          
            
              S
              34
            
          
        
        
          
            
              S
              41
            
          
          
            
              S
              42
            
          
          
            
              S
              43
            
          
          
            
              S
              44
            
          
        
      
      ]
    
    ⁡
    
      [
      
        
          
            
              A
              1
            
          
        
        
          
            
              A
              2
            
          
        
        
          
            
              A
              3
            
          
        
        
          
            
              A
              4
            
          
        
      
      ]
    
  




where the elements Sij are the S parameters for the four-port patch antenna. If it is desired to radiate circular polarization, then the inputs at each port must be of nearly equal amplitude and 90° out of phase with those of its immediate neighbors. For example, let:

A1=ej0=1=1∠0°

A2=ejπ/2=j=1∠90°,

A3=ejπ=−1=1∠180°,

A4=ej3π/2=−j=1∠270°;   [3]

This set of inputs will yield a right-hand circularly-polarized (RHCP) output. To obtain a left-hand circularly-polarized (LHCP) output, simply let A2=−j and A4=j in Eqn. (3). The amplitude of the reflected wave at port 1 for the inputs given in Eqn. (3) is then given by:




  
    
      
        
          
            
              
                B
                1
              
              =
              
                
                  
                    S
                    11
                  
                  ⁢
                  
                    A
                    1
                  
                
                +
                
                  
                    S
                    12
                  
                  ⁢
                  
                    A
                    2
                  
                
                +
                
                  
                    S
                    13
                  
                  ⁢
                  
                    A
                    3
                  
                
                +
                
                  
                    S
                    14
                  
                  ⁢
                  
                    A
                    4
                  
                
              
            
          
        
        
          
            
              =
              
                
                  S
                  11
                
                +
                
                  j
                  ⁢
                  
                    
                  
                  ⁢
                  
                    S
                    12
                  
                
                -
                
                  S
                  13
                
                -
                
                  j
                  ⁢
                  
                    
                  
                  ⁢
                  
                    S
                    14
                  
                
              
            
          
        
        
          
            
              =
              
                
                  S
                  11
                
                -
                
                  S
                  13
                
                +
                
                  j
                  ⁡
                  
                    (
                    
                      
                        S
                        12
                      
                      -
                      
                        S
                        14
                      
                    
                    )
                  
                
              
            
          
        
      
    
    
      
        [
        4
        ]
      
    
  




Clearly, the amplitude of the reflected wave will be identically equal to zero if the following conditions are satisfied:

S11=S13,

S12=S14   [5]

Since both the antenna and the placement of the ports are symmetric, as shown in FIG. 2, identical conditions will hold at the three remaining ports. Moreover, the symmetry of the patch and the port placement guarantees that the coupling from port 2 to port 1 is nearly identical to that from port 4 to port 1, so that S12≈S14. Therefore, reflections can be minimized by choosing the proper distance d from the center of the patch at which to place each of the four ports so that |S11−S13| is minimized.
A prototype four-port patch antenna was designed to operate at a frequency of f=1.03 GHz. Eqn. 1 was used to calculate a starting value of a0=2.264 inches for the patch radius. The distances d and a were determined iteratively. For the four-port patch shown in FIGS. 1a-1d, the best parameters were found to be a=2.198 inches and d=0.380 inches. This design was fabricated and its S parameters were measured using a network analyzer. FIG. 3 is a graph of measured effective return loss vs. frequency in the prototype four-port antenna, in which the amplitude of the reflected wave at each port is calculated using Eqn. 2 with the set of inputs given in Eqn. 3. The effective return loss is the magnitude of the ratio of the reflected power to the incident power, measured on a logarithmic scale:




  
    
      
        
          Return
          ⁢
          
            
          
          ⁢
          Loss
          ⁢
          
            
          
          ⁢
          at
          ⁢
          
            
          
          ⁢
          Port
          ⁢
          
            
          
          ⁢
          n
        
        =
        
          
            20
            ⁢
            
              log
              10
            
            ⁢
            
              
              
                R
                n
              
              
            
          
          =
          
            
              -
              20
            
            ⁢
            
              log
              10
            
            ⁢
            
              
              
                
                  B
                  n
                
                
                  A
                  n
                
              
              
            
          
        
      
    
    
      
        [
        6
        ]
      
    
  




Note that the center frequency is approximately 2 MHz too high, and the worst-case return loss is slightly less than 15 dB at the center frequency. Further design refinements can be made to correct the center frequency and increase the return loss at the center frequency.
By choosing a different set of input phases, the same design can also be made to radiate a linearly-polarized wave. Suppose that the inputs are given by:

A1=ej0=1,

A2=ej0=1,

A3=ejπ=−1,

A4=ejπ−1;   [7]

In this case, the amplitude of the reflected wave at port 1 is:




  
    
      
        
          
            
              
                B
                1
              
              =
              
              ⁢
              
                
                  
                    S
                    11
                  
                  ⁢
                  
                    A
                    1
                  
                
                +
                
                  
                    S
                    12
                  
                  ⁢
                  
                    A
                    2
                  
                
                +
                
                  
                    S
                    13
                  
                  ⁢
                  
                    A
                    3
                  
                
                +
                
                  
                    S
                    14
                  
                  ⁢
                  
                    A
                    4
                  
                
              
            
          
        
        
          
            
              =
              
              ⁢
              
                
                  S
                  11
                
                -
                
                  S
                  13
                
                +
                
                  S
                  12
                
                -
                
                  S
                  14
                
              
            
          
        
        
          
            
              ≈
              
              ⁢
              
                
                  S
                  11
                
                -
                
                  S
                  13
                
              
            
          
        
      
    
    
      
        [
        8
        ]
      
    
  




since S12≈S14 (S12 and S14 will be nearly equal in a real antenna). This is the same matching condition as for circular polarization, so the same antenna will radiate either polarization with the appropriate change in input phases.

In fact, the antenna can radiate either of two orthogonal linear polarizations, depending on the phases of the inputs. FIGS. 4a and 4b illustrate the two orthogonal linearly polarized outputs and the corresponding inputs as seen viewed from the back of the antenna In FIG. 4a, the inputs are given by Eqn. 6 and the output polarization is in the direction from port 1 to port 4. In FIG. 4b, A1=1, A2=−1, A3=−1, and A4=1, and the output polarization is in the direction from port 1 to port 2.
The present invention is not limited to patches that are circular in shape with four ports. Patches of other shapes may be used without departing from the scope of the present teachings. Furthermore, the invention may have any number of input ports greater than two. FIG. 5a is a diagram of an illustrative embodiment of the present invention with an equilateral triangular patch 18 with three ports 22. The ports 22 can be placed at 120° intervals on a circle centered on the center of the patch, as illustrated in FIG. 5a. Notice that the triangle whose vertices are the three ports 22 is rotated with respect to the patch 18. It is not necessary that the ports be placed along the bisectors of each side or along the bisectors of each angle.
In this geometry, each port 22 sees exactly the same environment as the other two ports, so that if one port is matched, all the ports are matched. The same is true of the antenna shown in FIG. 5b, in which the triangular patch has been replaced by a circular patch.
In general, an N-port patch antenna can be constructed by utilizing a suitable geometric figure having N-fold rotational symmetry; that is, a figure that is invariant when rotated about its axis of symmetry by any integer multiple of 360/N degrees. A special case is a circle, which is invariant under any rotation about its center. Design of such an N-port patch antenna is greatly simplified when the geometry “seen” by each port is the same, for if one port is matched, all of the ports are matched. This condition is satisfied by distributing the ports at equal intervals around a circle centered on the axis of symmetry of the patch. In the case of a circular patch, the ports are equally distributed around a circle having the same center as the patch.
As an example, consider an 8-port patch antenna constructed from a 16-sided polygon with ports arranged as shown in FIG. 6. The ports 22 are located every 45° on a circle of radius d centered on the polygon's axis of rotational symmetry. The ports 22 are labeled 1 through 8, with port 1 opposite port 5, port 2 opposite 6, port 3 opposite port 7, and port 4 opposite port 8. The patch geometry and the radius d are chosen to minimize the total power reflected from each port. By properly choosing the phases at the input ports, the antenna can be made to radiate either left-hand circular polarization (LHCP) or right-hand circular polarization (RHCP). The following is a set of inputs for RHCP:

A1=Aej0=A∠0°,

A2=Aejπ/4=A∠45°,

A3=Aej2π/4=Aejπ/2=jA=A∠90°,

A4=Aej3π/4=A∠135°,

A5=Aej4π/4=Aejπ=−A=A∠180°,

A6=Aej3π/4=Aejπ=−A=A∠180°,

A7=Aej6π/4=Aej3π/2=A∠270°,

A8=Aej7π/4=A∠315°;   [9]

The following inputs can be used for LHCP:

A1=Aej0=Aφ0°,

A2=Aej7π/4=A∠315°,

A3=Aej6π/4=Aej3π/2=−jA=A∠270°,

A4=Aej5π/4=A∠225°,

A5=Aej4π/4=Aejπ=−A=A∠180°,

A6=Aej3π/4=A∠135°,

A7=Aej2π/4 =Aejπ/2=A∠90°,

A8=Aejπ/4=A∠45°;   [10]

For example, for the set of inputs yielding a RHCP output, the total reflected wave at port 1 is given by:




  
    
      
        
          
            
              
                B
                1
              
              =
              
              ⁢
              
                
                  
                    S
                    11
                  
                  ⁢
                  
                    A
                    1
                  
                
                +
                
                  
                    S
                    12
                  
                  ⁢
                  
                    A
                    2
                  
                
                +
                
                  
                    S
                    13
                  
                  ⁢
                  
                    A
                    3
                  
                
                +
                
                  
                    S
                    14
                  
                  ⁢
                  
                    A
                    4
                  
                
                +
                
                  
                    S
                    15
                  
                  ⁢
                  
                    A
                    5
                  
                
                +
              
            
          
        
        
          
            
              
              ⁢
              
                
                  
                    S
                    16
                  
                  ⁢
                  
                    A
                    6
                  
                
                +
                
                  
                    S
                    17
                  
                  ⁢
                  
                    A
                    7
                  
                
                +
                
                  
                    S
                    18
                  
                  ⁢
                  
                    A
                    8
                  
                
              
            
          
        
        
          
            
              =
              
              ⁢
              
                A
                (
                
                  
                    S
                    11
                  
                  +
                  
                    
                      e
                      
                        (
                        
                          jπ
                          /
                          4
                        
                        )
                      
                    
                    ⁢
                    
                      S
                      12
                    
                  
                  +
                  
                    
                      e
                      
                        (
                        
                          jπ
                          /
                          2
                        
                        )
                      
                    
                    ⁢
                    
                      S
                      13
                    
                  
                  +
                  
                    
                      e
                      
                        (
                        
                          j
                          ⁢
                          
                            
                          
                          ⁢
                          3
                          ⁢
                          
                            π
                            /
                            4
                          
                        
                        )
                      
                    
                    ⁢
                    
                      S
                      14
                    
                  
                  -
                  
                    S
                    15
                  
                  -
                  
                    e
                    
                      (
                      
                        jπ
                        /
                        4
                      
                      )
                    
                  
                
              
            
          
        
        
          
            
              
              ⁢
              
                
                  S
                  16
                
                -
                
                  
                    e
                    
                      (
                      
                        jπ
                        /
                        2
                      
                      )
                    
                  
                  ⁢
                  
                    S
                    17
                  
                  ⁢
                  
                    e
                    
                      (
                      
                        j3π
                        /
                        4
                      
                      )
                    
                  
                  ⁢
                  
                    S
                    18
                  
                
              
              )
            
          
        
        
          
            
              =
              
              ⁢
              
                A
                [
                
                  
                    (
                    
                      
                        S
                        11
                      
                      -
                      
                        S
                        15
                      
                    
                    )
                  
                  +
                  
                    
                      e
                      
                        (
                        
                          jπ
                          /
                          4
                        
                        )
                      
                    
                    ⁡
                    
                      (
                      
                        
                          S
                          12
                        
                        -
                        
                          S
                          16
                        
                      
                      )
                    
                  
                  +
                  
                    
                      e
                      
                        jπ
                        /
                        2
                      
                    
                    ⁡
                    
                      (
                      
                        
                          S
                          13
                        
                        -
                        
                          S
                          17
                        
                      
                      )
                    
                  
                  +
                
              
            
          
        
        
          
            
              
              ⁢
              
                e
                
                  
                    (
                    
                      j3π
                      /
                      4
                    
                    )
                  
                  ⁢
                  
                    (
                    
                      
                        S
                        14
                      
                      -
                      
                        S
                        18
                      
                    
                    )
                  
                
              
            
          
        
      
    
    
      
        [
        11
        ]
      
    
  




To minimize the reflected wave amplitude, the antenna must be designed to minimize:




  
    
      
        
          
            
              
                R
                1
              
              =
              
              ⁢
              
                
                  B
                  1
                
                A
              
            
          
        
        
          
            
              =
              
              ⁢
              
                
                  (
                  
                    
                      S
                      11
                    
                    -
                    
                      S
                      15
                    
                  
                  )
                
                +
                
                  
                    e
                    
                      (
                      
                        jπ
                        /
                        4
                      
                      )
                    
                  
                  ⁢
                  
                    (
                    
                      
                        S
                        12
                      
                      -
                      
                        S
                        16
                      
                    
                    )
                  
                
                +
              
            
          
        
        
          
            
              
              ⁢
              
                
                  
                    e
                    
                      (
                      
                        jπ
                        /
                        2
                      
                      )
                    
                  
                  ⁡
                  
                    (
                    
                      
                        S
                        13
                      
                      -
                      
                        S
                        17
                      
                    
                    )
                  
                
                +
                
                  
                    e
                    
                      (
                      
                        j
                        ⁢
                        
                          
                        
                        ⁢
                        3
                        ⁢
                        
                          π
                          /
                          4
                        
                      
                      )
                    
                  
                  ⁡
                  
                    (
                    
                      
                        S
                        14
                      
                      -
                      
                        S
                        18
                      
                    
                    )
                  
                
              
            
          
        
      
    
    
      
        [
        12
        ]
      
    
  




The procedure by which this is achieved is similar to that for the four-port circular patch described earlier.
In general, for an antenna having N ports, the phases at the input to each port should be increased in increments of 360/N degrees, proceeding from port to port in either a clockwise direction, to yield a left-hand circularly-polarized radiated wave, or in a counter-clockwise direction, to yield a right-hand circular-polarized radiated wave.
Thus, the eight-port patch antenna can radiate both right-hand and left-hand circular polarization. Since a linearly-polarized wave is simply the superposition of two equal-amplitude circularly polarized waves of opposite helicity, a vertically-polarized output can be obtained by driving the antenna with the same superposition of inputs that yield the corresponding circularly-polarized waves, as given by the following:




  
    
      
        
          
            A
            
              V
              ⁢
              
                
              
              ⁢
              1
            
          
          =
          
            
              
                1
                2
              
              ⁢
              
                (
                
                  
                    A
                    1
                    
                      L
                      ⁢
                      
                        
                      
                      ⁢
                      H
                      ⁢
                      
                        
                      
                      ⁢
                      C
                      ⁢
                      
                        
                      
                      ⁢
                      P
                    
                  
                  +
                  
                    A
                    1
                    RHCP
                  
                
                )
              
            
            =
            1
          
        
        ,
        
          

        
        ⁢
        
          
            A
            
              V
              ⁢
              
                
              
              ⁢
              2
            
          
          =
          
            
              
                1
                2
              
              ⁢
              
                (
                
                  
                    A
                    2
                    
                      L
                      ⁢
                      
                        
                      
                      ⁢
                      H
                      ⁢
                      
                        
                      
                      ⁢
                      C
                      ⁢
                      
                        
                      
                      ⁢
                      P
                    
                  
                  +
                  
                    A
                    2
                    RHCP
                  
                
                )
              
            
            =
            
              1
              
                2
              
            
          
        
        ,
        
          

        
        ⁢
        
          
            A
            
              V
              ⁢
              
                
              
              ⁢
              3
            
          
          =
          
            
              
                1
                2
              
              ⁢
              
                (
                
                  
                    A
                    3
                    
                      L
                      ⁢
                      
                        
                      
                      ⁢
                      H
                      ⁢
                      
                        
                      
                      ⁢
                      C
                      ⁢
                      
                        
                      
                      ⁢
                      P
                    
                  
                  +
                  
                    A
                    3
                    RHCP
                  
                
                )
              
            
            =
            0
          
        
        ,
        
          

        
        ⁢
        
          
            A
            
              V
              ⁢
              
                
              
              ⁢
              4
            
          
          =
          
            
              
                1
                2
              
              ⁢
              
                (
                
                  
                    A
                    4
                    
                      L
                      ⁢
                      
                        
                      
                      ⁢
                      H
                      ⁢
                      
                        
                      
                      ⁢
                      C
                      ⁢
                      
                        
                      
                      ⁢
                      P
                    
                  
                  +
                  
                    A
                    4
                    RHCP
                  
                
                )
              
            
            =
            
              -
              
                1
                
                  2
                
              
            
          
        
        ,
        
          

        
        ⁢
        
          
            A
            
              V
              ⁢
              
                
              
              ⁢
              5
            
          
          =
          
            
              
                1
                2
              
              ⁢
              
                (
                
                  
                    A
                    5
                    
                      L
                      ⁢
                      
                        
                      
                      ⁢
                      H
                      ⁢
                      
                        
                      
                      ⁢
                      C
                      ⁢
                      
                        
                      
                      ⁢
                      P
                    
                  
                  +
                  
                    A
                    5
                    RHCP
                  
                
                )
              
            
            =
            
              -
              1
            
          
        
        ,
        
          

        
        ⁢
        
          
            A
            
              V
              ⁢
              
                
              
              ⁢
              6
            
          
          =
          
            
              
                1
                2
              
              ⁢
              
                (
                
                  
                    A
                    6
                    
                      L
                      ⁢
                      
                        
                      
                      ⁢
                      H
                      ⁢
                      
                        
                      
                      ⁢
                      C
                      ⁢
                      
                        
                      
                      ⁢
                      P
                    
                  
                  +
                  
                    A
                    6
                    RHCP
                  
                
                )
              
            
            =
            
              -
              
                1
                
                  2
                
              
            
          
        
        ,
        
          

        
        ⁢
        
          
            A
            
              V
              ⁢
              
                
              
              ⁢
              7
            
          
          =
          
            
              
                1
                2
              
              ⁢
              
                (
                
                  
                    A
                    7
                    
                      L
                      ⁢
                      
                        
                      
                      ⁢
                      H
                      ⁢
                      
                        
                      
                      ⁢
                      C
                      ⁢
                      
                        
                      
                      ⁢
                      P
                    
                  
                  +
                  
                    A
                    7
                    RHCP
                  
                
                )
              
            
            =
            0
          
        
        ,
        
          

        
        ⁢
        
          
            
              A
              
                V
                ⁢
                
                  
                
                ⁢
                8
              
            
            =
            
              
                
                  1
                  2
                
                ⁢
                
                  (
                  
                    
                      A
                      8
                      
                        L
                        ⁢
                        
                          
                        
                        ⁢
                        H
                        ⁢
                        
                          
                        
                        ⁢
                        C
                        ⁢
                        
                          
                        
                        ⁢
                        P
                      
                    
                    +
                    
                      A
                      8
                      RHCP
                    
                  
                  )
                
              
              =
              
                1
                
                  2
                
              
            
          
          ;
        
      
    
    
      
        [
        13
        ]
      
    
  




FIG. 7a is a diagram of an eight-port patch antenna with the inputs given by Eqn. 13. The output is linearly polarized in the direction from port 1 to port 5 (vertically in FIG. 7a).
Horizontal linear polarization is obtained from the same set of inputs simply by rotating the inputs by 90° clockwise or counter clockwise with respect to ports 1 through 8, as given by:




  
    
      
        
          
            A
            
              H
              ⁢
              
                
              
              ⁢
              1
            
          
          =
          
            
              A
              
                V
                ⁢
                
                  
                
                ⁢
                7
              
            
            =
            0
          
        
        ,
        
          

        
        ⁢
        
          
            A
            
              H
              ⁢
              
                
              
              ⁢
              2
            
          
          =
          
            
              A
              
                V
                ⁢
                
                  
                
                ⁢
                8
              
            
            =
            
              1
              
                2
              
            
          
        
        ,
        
          

        
        ⁢
        
          
            A
            
              H
              ⁢
              
                
              
              ⁢
              3
            
          
          =
          
            
              A
              
                V
                ⁢
                
                  
                
                ⁢
                1
              
            
            =
            1
          
        
        ,
        
          

        
        ⁢
        
          
            A
            
              H
              ⁢
              
                
              
              ⁢
              4
            
          
          =
          
            
              A
              
                V
                ⁢
                
                  
                
                ⁢
                2
              
            
            =
            
              1
              
                2
              
            
          
        
        ,
        
          

        
        ⁢
        
          
            A
            
              H
              ⁢
              
                
              
              ⁢
              5
            
          
          =
          
            
              A
              
                V
                ⁢
                
                  
                
                ⁢
                3
              
            
            =
            0
          
        
        ,
        
          

        
        ⁢
        
          
            A
            
              H
              ⁢
              
                
              
              ⁢
              6
            
          
          =
          
            
              A
              
                V
                ⁢
                
                  
                
                ⁢
                4
              
            
            =
            
              -
              
                1
                
                  2
                
              
            
          
        
        ,
        
          

        
        ⁢
        
          
            A
            
              H
              ⁢
              
                
              
              ⁢
              7
            
          
          =
          
            
              A
              
                V
                ⁢
                
                  
                
                ⁢
                5
              
            
            =
            1
          
        
        ,
        
          

        
        ⁢
        
          
            A
            
              H
              ⁢
              
                
              
              ⁢
              8
            
          
          =
          
            
              A
              
                V
                ⁢
                
                  
                
                ⁢
                6
              
            
            =
            
              -
              
                
                  1
                  
                    2
                  
                
                .
              
            
          
        
      
    
    
      
        [
        14
        ]
      
    
  




FIG. 7b is a diagram of an eight-port patch antenna with the inputs given by Eqn. 14. The output is linearly polarized in the direction from port 7 to port 3.
The condition that all ports see the same geometry simplifies the design of the multiple-port patch antenna, but it is not a requirement. Other antenna configurations in which different ports see different geometries may be used without departing from the scope of the present teachings.
In the illustrative embodiment of FIGS. 1a-1d, the antenna is fed by four coaxial ports, each attached directly to its feed point. This configuration may be inconvenient in some cases in that the feed points are so close together that any connectors will interfere with each other. Other configurations for feeding the antenna may be used without departing from the scope of the present teachings.
FIGS. 8a and 8b are diagrams of an illustrative embodiment of an antenna 10A of the present invention with an alternative method for feeding the antenna that decouples the feed points from the location of the input ports. FIG. 8a shows a normal view and FIG. 8b shows an exploded view. In this configuration, the patch 18 lies on one outer face of a two-layer circuit, and a microstrip feed network 30 lies on the other face. The patch 18 lies on a first surface of a first dielectric substrate 12, and a ground plane 20 lies on the second surface of the first dielectric substrate 12. A first surface of a second dielectric substrate 32 lies on the ground plane 20, and the microstrip feed network 30 lies on the second surface of the second dielectric substrate 32. Thus, the patch antenna 18 and the microstrip feed network 30 share a common ground plane. Each port 22 (i.e., the coaxial connector) makes a transition to the microstrip. A microstrip transmission line 30 then carries the energy delivered by the port 22 to a point directly under the corresponding feed point 26 on the antenna 18. At this point, a metallic probe 34 carries the energy from the microstrip transmission line 30 through a hole in the common ground plane 20 to the feed point 26 on the lower surface of the patch 18.
There are several advantages to this method of feeding the antenna. First, it allows scaling the multiple-port patch antenna to all frequencies, as one no longer need be concerned with mechanical interference between adjacent connectors at high frequencies (where the distance between feed points is smaller than the size of the connectors). It also allows one to make use of the area on the microstrip-feed side of the board for circuitry. For example, if it is required to protect the microwave sources feeding the antenna from large reflections, surface-mount isolators can be mounted on the back of the antenna, possibly eliminating the need for a circuit board elsewhere in a larger system.
FIGS. 9a and 9b are diagrams showing the current best mode embodiment of the invention. FIG. 9a shows a normal view and FIG. 9b shows an exploded view of a four-port version of the multiple-port patch antenna. The antenna 10B includes two dielectric substrates 12 and 32. The patch 18 (which is circular in this example) is disposed on a first surface of the first dielectric substrate 12. The second surface of the first substrate 12 faces a first surface of the second substrate 32. The ground plane 20 is disposed on the second surface of the second substrate 32. The coaxial connectors 22 feed microwave energy to microstrip feed lines 30 that are sandwiched between the two dielectric substrates 12 and 32. The four coaxial connectors 22 are attached to the ground plane 20, arranged in a circle around the circular patch 18. The center conductors of the coaxial ports 22 are each connected to a microstrip feed line 30. For each coaxial port 22, the distance of the point of connection from the end of the corresponding microstrip feed line 30 is chosen to minimize the reflected power from the coaxial-to-microstrip transition. The microstrip feed lines 30 carry the microwave signal to the ends of the feed lines 40, where it is radiated into the volume between the patch 18 and the ground plane 20. The locations of the ends of the feed lines 40 are determined in a similar manner as described above for the feed points 26 in the other embodiments. In this example, the ends of the feed lines 40 are equally distributed around a circle having the same center as the patch 18.
A prototype four-port patch antenna utilizing the best-mode embodiment was constructed. The design procedure is the same as that for the four-port circular patch described earlier. For the four-port patch shown in FIGS. 9a and 9b, the radius a of the circular patch 18 is 2.073 inches, and the ends of each of the four microstrip feed lines 30 are arranged on a circle of radius 1.72 inches. Both the first substrate 12 and the second substrate 32 are 0.125 inches thick and have a dielectric constant of 2.2. FIG. 10 is a graph of the measured effective return loss vs. frequency of each port of the prototype four-port patch antenna. Note that the center frequency is approximately 5 MHz too high, and the worst-case return loss is approximately 27 dB at the center frequency. Further design refinements can be made to correct the center frequency and to reduce the spread in the center frequencies of the individual ports.
FIGS. 11a and 11b are diagrams of a sixteen-port version of the antenna designed in accordance with an illustrative embodiment of the teachings of the present invention. FIG. 11a shows a normal view and FIG. 11b shows an exploded view. The antenna 10C is similar to that of FIGS. 10a and 10b, except having sixteen ports 22 and microstrip feed lines 30. This antenna is designed to radiate a circularly-polarized wave. To achieve this, the phases at the input to each port increase in increments of 22.5 degrees; that is, if port 1 is 0 degrees (where any port can be chosen as port 1), then the phase at the input to port 2 should be 22.5 degrees, the input to port 3 should be 45 degrees, etc., proceeding from port to port in either a clockwise direction, which will yield a left-hand circularly-polarized radiated wave, or in a counter-clockwise direction, which will yield a right-hand circular-polarized radiated wave.
A prototype sixteen-port patch antenna was constructed using the design shown in FIGS. 11a and 11b. For the sixteen-port patch shown in FIGS. 11a and 11b, the radius a of the circular patch 18 is 2.023 inches, and the ends of each of the sixteen microstrip feed lines 30 are arranged on a circle of radius 1.908 inches. Both the first substrate 12 and the second substrate 32 are 0.125 inches thick and have a dielectric constant of 2.2. FIG. 12 is a graph of the measured effective return loss vs. frequency of each port of the prototype sixteen-port patch antenna. Note that the center frequency is approximately 7 MHz too high, and the worst-case return loss is approximately 21 dB at the center frequency. Further design refinements can be made to correct the center frequency and to reduce the spread in the center frequencies of the individual ports.
Unfortunately, however, as the number of feed ports and microstrip feed lines 30 increase, they tend to crowd together making the design of patches 18 having more than approximately eight ports 22 problematic. Difficulties may arise not only in the placement and arrangement of feed lines 30, but their close proximity may result in detrimental electrical interference. Accordingly, in an alternative embodiment of the present invention, modifications to the geometry or the microstrip feed lines 30 may facilitate their placement and distribution upon the second dielectric substrate 32. Of additional benefit, the modifications to the geometry of the microstrip feed lines 30 may be further used to control the central frequency and bandwidth characteristics of the antenna 10. With reference to FIG. 14, it may be preferable that the approximate width of the feed lines 30 diminish as each feed line 30 approaches the center of the patch 18.
Generally, the modifications to the feed line 30 geometry may be formed with the following algorithm. The algorithm is simply provided to illustrate a suitable method that may be used to create the feed lines 30 having the described geometry. The example algorithm describes a suitable process for creating a feed structure having only four feed lines 30. The feed lines 30 are constructed by initially metallizing a square area 1410 upon a substrate layer 1405 (see FIG. 14a). From the square area 1410, a series of triangular areas 1415 are removed by an etching process. The etching process may include any etching process, whether now known or subsequently hereafter described in the art. The size and number of triangular sections 1415 will be generally be determined by the number and size of the feed lines 30. In FIG. 14b, there are four isosceles triangular sections 1415 that correspond to the four inputs. The triangular sections 1415 have been removed from the metallized square area 1410. The triangular sections 1415 have an angle 1425 that is formed by the connection of the triangular section's 1415 congruent sides. In this case, the angle 1425 is approximately 80 degrees. The triangular sections 1415 are oriented such that the point formed by angle 1425 lays upon the center of metallized area 1410. The side of the triangular section 1415 that is opposite the angle 1425 lays upon the outer boundary 1420 of the metallized area 1410. Finally, with reference to FIG. 14c, a central portion 1420 of the square area 1410 is removed. In this example, the removed portion 1420 comprises a rotated square shape that is subtracted from the original metallized square area 1410. The square shape is selected to substantially correspond with that of the originally metallized area 1410—although it will generally be smaller in area.
With reference to FIG. 15, a more general process for creating the improved feed lines 30 may be described for antennas 10 having N feed lines 30. First, a metallized area 1410 is created upon a substrate 1405. The metallized area 1410 has an outer boundary 1430 and has N-fold rotational symmetry, where N is the number of inputs and feed lines 30. From that area, a series of triangular shapes 1415 will be removed. In an antenna 10 having N inputs, there will be N triangular portions 1415 that will be removed from the originally metallized area 1410. In alternative embodiments, the number of feed lines 30 may not be equal to the number of inputs. For example, each input may feed into two or more feed lines 30. Alternatively, each input may serve a differing number of feed lines 30 depending upon the specific application. Generally, the triangular sections 1415 will all be approximately the same size. In the majority of cases, the triangular sections 1415 will be isosceles triangles having an angle 1425 formed by the connection of the triangular section's congruent sides. They will generally be oriented so that the base of the triangular section 1415 (the side opposite the angle 1425) will lie upon the outer boundary 1430 of the metallized area 1410. The point of the angle 1425 will generally lie upon the center of the metallized area 1410. In the majority of cases, the triangular sections 1415 will be equally distributed around the metallized area 1410. Note that although this example removes triangular shapes 1415 from the metallized area 1410 in order to separate the feed lines 30, other shapes may also be used. For example, instead of triangles, rectangular areas may be used. It is only necessary that the feed lines 30 be physically separated.
Finally, a central portion 1420 of the metallized area 1410 will be removed. The central portion will generally comprise an area having N-fold rotational symmetry and so will have the same general shape as the original metallized area 1410. However, the central portion 1420 will be smaller than that of the originally metallized portion 1410. Accordingly, the outer boundary 1435 of the central portion 1420 also defines the inner boundary 1435 of the feed lines 30. In some cases, as reflected in FIG. 15 the central portion 1420 will be rotated by some angle 1540 that is approximately determined by the value of N. In FIG. 15, assuming that the central portion 1420 is initially oriented in the same manner as the originally metallized area 1410, the central portion 1420 will be rotated by




  
    (
    
      360
      N
    
    )
  
  2




degrees.

In cases where the antenna 10 has a large number of inputs and feed lines 30, the manufacturing process may become excessively cumbersome as largely faceted shapes become difficult and expensive to manufacture accurately. Fortunately, as the number of inputs increases, the N-fold rotationally symmetric shapes will begin to approximate circles. Because circular shapes can be easier to manufacture, it may be beneficial to simply use a circular shape to define the outer and inner boundaries of the feed lines 30 rather than use N-fold rotationally symmetric shapes. Note that antennas having a relatively small number of inputs may similarly benefit from the use of circular shapes to define the inner and outer boundaries of the feed lines 30 instead of employing N-fold rotationally symmetric shapes.
Similar benefits may be derived from simplifying construction of the patch 18. In an antenna 10 having N ports 22 and N feed lines 30, it is generally preferable that the outer boundary of the patch 18 have N-fold symmetry. However, in many applications, a circular patch 18 satisfies the N-fold symmetry requirement. This is especially true for systems having a relatively high number of feed lines 30 because as N increases, N-sided polygons having N-fold rotational symmetry become functionally equivalent to circles.
The bandwidth of the N port antenna 10 can be controlled by altering the size and shape of the patch 18, the outer boundary 1430 of the feed lines 30, and the inner boundary 1435 of the feed lines 30. In an exemplary embodiment where the patch 18 approximates a circle having a radius of 1.93 inches, the outer boundary 1430 of the feed lines 30 approximates a circle having a radius of 2.3 inches, and the inner boundary 1435 of the feed lines 30 approximates a circle having a radius of approximately 1.499 inches, the band over which VSWR is less than 2 extends from 1.08 GHz to 1.82 GHz, yielding a center frequency of 1.45 GHz and a fractional bandwidth of 51% (see FIG. 17). It should be noted that in this particular exemplary embodiment, the feed lines 30 are separated by small rectangles of non-conducting material having approximate width of 100 mm. The small rectangles are generally oriented such that a line running parallel to the length and through the center of any of the rectangles would pass through the center of the patch 18.
FIG. 16 is a diagram showing a specific construction of the best mode of the present embodiment. This description is in no way intended to limit the scope of the current invention. With reference to FIG. 16, patch 18 is printed upon a first surface 1610 of a sheet of 5 mil 5880 Duroid having 1⁄2oz. copper. Although Duroid is used in the present embodiment, any other suitable material such as PCB materials including Rogers® 4000, DuPont® Teflon®, polyimide, polystyrene, cross-linked polystyrene, copper clad laminates, glass laminates, and/or Kapton-based materials may be used. The second surface 1615 of 5 mil 5880 Duroid XX is coupled to a bonding film 1620 which is, in turn, coupled to a first surface 1625 of a sheet of Rohacell Foam 1630 having an approximate thickness of 0.625′′. The Rohacell Foam 1630 is generally a high-frequency low-loss dielectric foam having an εR value of approximately 1.05. Other suitable materials include other Polymethyl methacrylate products, Expanded polystyrene, Extruded polystyrene, polypropylene, Polyethylene foams, and others. The second surface 1635 of the Rohacell foam 1630 is coupled to a bonding film 1640 which is, in turn, coupled to a first surface 1645 of a second sheet of 5 mil Duroid XX 1650—again, alternative materials may be suitable depending upon the application. The second sheet of 5 mil Duroid 1650 further comprises feed lines 30 which are printed upon its first surface 1645. The second surface 1655 of the second sheet of 5 mil Duroid 1650 is coupled to a bonding film 1660 which is, in turn, coupled to a first surface 1665 of a second sheet of Rohacell foam 1670 having an approximate thickness of 0.5′′. The second surface 1675 of the second sheet of Rohacell foam 1670 is coupled to a bonding film 1675 which is, in turn, coupled to aluminum ground plane 1680. SMA connectors 1685 allow for electrical inputs to be coupled to the antenna 10. The SMA connectors 1685 are coaxial-conductors that have a center conductor that is coupled to the feed lines 30 and an outer conductor that is coupled to the aluminum ground plane 1680. SMA connectors 1685 need not be coaxial conductors and may comprise any suitable connectors for coupling electrical components. During construction, a series of holes 1690 may be used to facilitate correct orientation and placement of the various components of the antenna 10.
This invention requires that a means must be provided for controlling the phase and the amplitude at the input to each port of the antenna. Amplitude and phase control can be achieved by several means. FIG. 13 is a diagram of an illustrative module 50 for radiating high power microwave energy designed in accordance with the teachings of the present invention. In most cases, each port 22 of the antenna 10 will be driven by a separate microwave power amplifier 54. An amplitude control unit 56 is used to control the amplitude of the input to each amplifier 54, and a phase control unit 58 is used to control the phase of the input to each amplifier 54. The master signal amplified by each amplifier 54 may be derived from a master oscillator 52, so that the inputs to each amplitude control unit 56 are in phase. A number of different means are available for implementation of the amplitude control unit 56, including digitally-controlled variable attenuators. The phase control unit 58 can take the form of a ferrite phase shifter or a digital delays line at the input or output of each amplifier 54. It is also possible to “hard wire” the phase shifts simply by connecting the antenna 10 to the output of each amplifier 54 by using lengths of transmission line (coaxial cable, for example) cut to the length required to yield the desired phase at the input to each port 22 of the antenna 10.
In the foregoing specification, the invention has been described with reference to specific exemplary embodiments; however, it will be appreciated that various modifications and changes may be made without departing from the scope of the present invention as set forth herein. The specification and Figures are to be regarded in an illustrative manner, rather than a restrictive one and all such modifications are intended to be included within the scope of the present invention. Accordingly, the scope of the invention should be determined by the claims and their legal equivalents rather than by merely the examples described above.
For example, the steps recited in any method or process claim may be executed in any order and are not limited to the specific order presented in the claims. Additionally, the components and/or elements recited in any apparatus embodiment may be assembled or otherwise operationally configured in a variety of permutations to produce substantially the same result as the present invention and are accordingly not limited to the specific configuration recited in the claims.
Benefits, other advantages and solutions to problems have been described above with regard to particular embodiments; however, any benefit, advantage, solution to problem or any element that may cause any particular benefit, advantage or solution to occur or to become more pronounced are not to be construed as critical, required or essential features or components of the invention.
As used herein, the terms “comprising”, “having”, “including” or any variation thereof, are intended to reference a non-exclusive inclusion, such that a process, method, article, composition or apparatus that comprises a list of elements does not include only those elements recited, but may also include other elements not expressly listed or inherent to such process, method, article, composition or apparatus. Other combinations and/or modifications of the above-described structures, arrangements, applications, proportions, elements, materials or components used in the practice of the present invention, in addition to those not specifically recited, may be varied or otherwise particularly adapted to specific environments, manufacturing specifications, design parameters or other operating requirements without departing from the general principles of the same.

## Claims

1. An antenna for radiating electromagnetic energy comprising:
a first dielectric substrate having opposite first and second surfaces;
a patch of conducting material disposed on said first surface;
a ground plane of conducting material disposed on said second surface; and
at least three input means, each input means coupled to a respective one of a plurality of microstrip feed lines, said input means and said microstrip feed lines adapted to electrically couple an input signal to said patch at respective feed points, wherein said feed points are positioned to minimize the total power reflected from each input means, each of said microstrip feed lines having a first end and a second end, said first end oriented away from said patch and said second end oriented towards the center of the patch and said microstrip feed lines tapered such that the width of said microstrip feed lines diminishes along the length of said microstrip feed lines, said width being greater proximate said first end than proximate said second end.

2. The antenna of claim 1, wherein said second end of said microstrip feed lines approximately defining an inner boundary of said microstrip feed lines, the geometry of said inner boundary approximating a shape having at least N-fold rotational symmetry, where N is the number of input means.

3. The antenna of claim 1, wherein said second end of said microstrip feed lines approximately defining an inner boundary of said microstrip feed lines, the geometry of said inner boundary approximating a circle.

4. The antenna of claim 1, wherein said first end of said microstrip feed lines approximately defining an outer boundary, said outer boundary approximating a geometrical shape having at least N-fold rotational symmetry, where N is the number of input means.

5. The antenna of claim 1, wherein said first end of said microstrip feed lines approximately defining an outer boundary, said outer boundary approximating a circle.

6. The antenna of claim 1, wherein said microstrip feed lines being separated by a plurality of gaps that are defined by said microstrip feed lines, said gaps being suitably configured to physically separate each of said microstrip feed lines.

7. The antenna of claim 1, wherein said feed lines are positioned such that for each input means, a directly-reflected signal from said input means is nearly cancelled by cross-coupled signals from the other input means.

8. The antenna of claim 1, wherein said feed lines are positioned to minimize B=SA, where B is a vector of the amplitudes of the reflected waves at each input means, S is a matrix of the S parameters of the antenna, and A is a vector of the amplitudes of the incident waves at each input means.

9. The antenna of claim 1, wherein the size of said patch is chosen to minimize the total power reflected from each input means.

10. The antenna of claim 1, wherein the geometry of said patch is chosen to minimize the total power reflected from each input means.

11. The antenna of claim 1, wherein said patch has N-fold rotational symmetry, where N is the number of input means.

12. The antenna of claim 11 wherein said feed points are equally distributed around a circle centered on the axis of symmetry of said patch.

13. The antenna of claim 12, wherein the radius d of said circle is chosen to minimize the total power reflected from each input means.

14. The antenna of claim 13, wherein the radius d of said circle is determined such that directly-reflected signals from each individual input means are cancelled by cross-coupled signals from the other input means.

15. The antenna of claim 1, wherein said feed lines are positioned such that the geometry of the antenna seen at each feed point is the same for all feed points.

16. The antenna of claim 1, wherein said patch is circular.

17. The antenna of claim 1, wherein said patch is in the shape of a polygon having a multiple of N sides, where N is the number of input means.

18. The antenna of claim 1, wherein said input means further include input ports, each port coupled to at least one of said microstrip feed lines.

19. The antenna of claim 18, wherein said input ports are coaxial connectors.

20. The antenna of claim 1, wherein said dielectric substrate includes two layers.

21. The antenna of claim 20, wherein said microstrip feed lines being disposed between said two layers.

22. The antenna of claim 1, wherein said antenna further includes a second dielectric substrate having opposite third and fourth surfaces.

23. The antenna of claim 22, wherein said third surface is coupled to said ground plane.

24. The antenna of claim 1, wherein said microstrip feed lines are disposed on said fourth surface.

25. The antenna of claim 1, wherein said electromagnetic energy is microwave energy.

26. The antenna of claim 1, wherein at least one of the size of said patch, size of said inner boundary, and size of said outer boundary are substantially configured to optimize the performance of said antenna.

27. The antenna of claim 1, wherein at least one of the size of said patch, size of said inner boundary, and size of said outer boundary are substantially configured to control at least one of the central frequency and the bandwidth of the antenna.