Patent Publication Number: US-10312596-B2

Title: Dual-polarization, circularly-polarized, surface-wave-waveguide, artificial-impedance-surface antenna

Description:
CROSS REFERENCE TO RELATED APPLICATIONS 
     This application is related to U.S. patent application Ser. No. 13/744,295 filed Jan. 17, 2013 and entitled “Surface Wave Guiding Apparatus and Method”, the disclosure of which is hereby incorporated herein by reference. 
     STATEMENT REGARDING FEDERALLY SPONSORED RESEARCH OR DEVELOPMENT 
     None. 
     TECHNICAL FIELD 
     This invention provides an antenna capable of dual-polarization, circularly-polarized simultaneous Right Hand Circular Polarization (RHCP) and Left Hand Circular Polarization (LHCP) operation. 
     BACKGROUND 
     Linearly-polarized AIS Antennas 
     Artificial impedance surface antennas (AISAs) are realized by launching a surface wave across an artificial impedance surface (AIS), whose impedance is spatially modulated across the AIS according a function that matches the phase fronts between the surface wave on the AIS and the desired far-field radiation pattern. 
     In the prior art, an artificial impedance surface antenna (AISA) is formed from modulated artificial impedance surfaces (AIS). The prior art, in this regard, includes: 
     (1) Patel (see, for example, Patel, A. M.; Grbic, A., “ A Printed Leaky - Wave Antenna Based on a Sinusoidally - Modulated Reactance Surface”, IEEE Transactions on Antennas and Propagation , vol. 59, no. 6, pp. 2087-2096, June 2011) demonstrated a scalar AISA using an endfire-flare-fed one-dimensional, spatially-modulated AIS consisting of a linear array of metallic strips on a grounded dielectric. 
     (2) Sievenpiper, Colbum and Fong (see, for example, D. Sievenpiper et al, “ Holographic AISs for conformal antennas ”, 29th Antennas Applications Symposium, 2005 &amp; 2005 IEEE Antennas and Prop. Symp. Digest, vol. 1B, pp. 256-259, 2005; and B. Fong et al, “ Scalar and Tensor Holographic Artificial Impedance Surfaces ”, IEEE TAP., 58, 2010) have demonstrated scalar and tensor AISAs on both flat and curved surfaces using waveguide-fed or dipole-fed, two-dimensional, spatially-modulated AIS consisting of a grounded dielectric topped with a grid of metallic patches. 
     (3) Gregoire (see, for example, D. J. Gregoire and J. S. Colbum, “ Artificial impedance surface antennas ”, Proc. Antennas Appl. Symposium 2011, pp. 460-475; D. J. Gregoire and J. S. Colbum, “ Artificial impedance surface antenna design and simulation ”, Proc. Antennas Appl. Symposium 2010, pp. 288-303) has examined the dependence of AISA operation on its design properties. 
     The basic principle of AISA operation is to use the grid momentum of the modulated AIS to match the wavevector of an excited surface-wave front to a desired plane wave. In the one-dimensional case, this can be expressed as
 
 k   sw   =k   o  sin θ o   −k   p ,  (Eqn. 1)
 
where k o  is the radiation&#39;s free-space wavenumber at the design frequency, θ o  is the angle of the desired radiation with respect to the AIS normal, k p =2π/p is the AIS grid momentum where p is the AIS modulation period, and k sw =n o k o  is the surface wave&#39;s wavenumber, where n o  is the surface wave&#39;s refractive index averaged over the AIS modulation. The Surface Wave (SW) impedance is typically chosen to have a pattern that modulates the SW impedance sinusoidally along the Surface Wave Guide (SWG) according to the following equation:
 
 Z ( x )= X+M  cos(2π×/ p )  (Eqn. 2)
 
where p is the period of the modulation, X is the mean impedance, and M is the modulation amplitude. X, M and p are chosen such that the angle of the radiation θ in the x-z plane w.r.t the z axis is determined by
 
θ=sin −1 ( n   0 −λ 0   /p )  (Eqn. 3)
 
where n 0  is the mean SW index and λ 0  is the free-space wavelength of radiation. n 0  is related to Z(x) by
 
     
       
         
           
             
               n 
               0 
             
             = 
             
               
                 
                   1 
                   p 
                 
                 ⁢ 
                 
                   
                     ∫ 
                     0 
                     p 
                   
                   ⁢ 
                   
                     
                       
                         1 
                         + 
                         
                           
                             Z 
                             ⁡ 
                             
                               ( 
                               x 
                               ) 
                             
                           
                           2 
                         
                       
                     
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     d 
                     ⁢ 
                     
                         
                     
                     ⁢ 
                     x 
                   
                 
               
               ≈ 
               
                 
                   
                     1 
                     + 
                     
                       X 
                       2 
                     
                   
                 
                 . 
               
             
           
         
       
     
     The AISA impedance modulation of Eqn. 2 can be generalized for an AISA of any shape as
 
 Z ({right arrow over ( r )})= X+M  cos( k   o   n   o   r−{right arrow over (k)}   o   ·{right arrow over (r)} )
 
where {right arrow over (k)} o  is the desired radiation wave vector, {right arrow over (r)} is the three-dimensional position vector of the AIS, and r is the distance along the AIS from the surface-wave source to {right arrow over (r)} along a geodesic on the AIS surface. This expression can be used to determine the index modulation for an AISA of any geometry, flat, cylindrical, spherical, or any arbitrary shape. In some cases, determining the value of r is geometrically complex. For a flat AISA, it is simply r=√{square root over (x 2 +y 2 )}.
 
     For a flat AISA designed to radiate into the wavevector at {right arrow over (k)} o =k o (sin θ o {circumflex over (x)}+cos θ o {circumflex over (z)}), with the surface-wave source located at x=y=0, the modulation function is
 
 Z ( x,y )= X+M  cos γ
 
where γ≡ k   0 ( n   0   r−x  sin θ 0 ).  (Eqn. 4)
 
     The cos function in Eqn. 2 and Eqn. 3 can be replaced with any periodic function and the AISA will still operate as designed, but the details of the side lobes, bandwidth and beam squint will be affected. 
     The AIS can be realized as a grid of metallic patches disposed on a grounded dielectric that produces the desired index modulation by varying the size of the patches according to a function that correlates the patch size to the surface wave index. The correlation between index and patch size can be determined using simulations, calculation and/or measurement techniques. For example, Colburn and Fong (see references cited above) use a combination of HFSS unit-cell eigenvalue simulations and near field measurements of test boards to determine their correlation function. Fast approximate methods presented by Luukkonen (see, for example, O. Luukkonen et al, “Simple and accurate analytical model of planar grids and high-impedance surfaces comprising metal strips or patches”, IEEE Trans. Antennas Prop., vol. 56, 1624, 2008) can also be used to calculate the correlation. However, empirical correction factors are often applied to these methods. In many regimes, these methods agree very well with HFSS eigenvalue simulations and near-field measurements. They break down when the patch size is large compared to the substrate thickness, or when the surface-wave phase shift per unit cell approaches 180°. 
     Circularly-polarized AIS Antennas 
     An AIS antenna can be made to operate with circularly-polarized (CP) radiation by using an impedance surface whose impedance properties are anisotropic. Mathematically, the impedance is described at every point on the AIS by a tensor. In a generalization of the modulation function of equation (3) for the linear-polarized AISA [4], the impedance tensor of the CP AISA may have a form like 
     
       
         
           
             
               
                 
                   
                     Z 
                     = 
                     
                       [ 
                       
                         
                           
                             
                               X 
                               - 
                               
                                 M 
                                 ⁢ 
                                 
                                     
                                 
                                 ⁢ 
                                 cos 
                                 ⁢ 
                                 
                                     
                                 
                                 ⁢ 
                                 ϕ 
                                 ⁢ 
                                 
                                     
                                 
                                 ⁢ 
                                 cos 
                                 ⁢ 
                                 
                                     
                                 
                                 ⁢ 
                                 γ 
                               
                             
                           
                           
                             
                               
                                 1 
                                 2 
                               
                               ⁢ 
                               M 
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                               ⁢ 
                               
                                 sin 
                                 ⁡ 
                                 
                                   ( 
                                   
                                     γ 
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                                     ϕ 
                                   
                                   ) 
                                 
                               
                             
                           
                         
                         
                           
                             
                               
                                 1 
                                 2 
                               
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                               M 
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                                 sin 
                                 ⁡ 
                                 
                                   ( 
                                   
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                               X 
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                                 ⁢ 
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                                 ⁢ 
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                   ; 
                 
               
               
                 
                   ( 
                   
                     Eqn 
                     . 
                     
                         
                     
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                     5 
                   
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                     where 
                     ⁢ 
                     
                         
                     
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                     tan 
                     ⁢ 
                     
                         
                     
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                     ϕ 
                   
                   ≡ 
                   
                     
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                       x 
                     
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                   ( 
                   
                     Eqn 
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                     ⁢ 
                     6 
                   
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     In the article by B. Fong et al. identified above, the tensor impedance is realized with anisotropic metallic patches on a grounded dielectric substrate. The patches are squares of various sizes with a slice through the center of them. By varying the size of the patches and the angle of the slice through them, the desired tensor impedance of equation Eqn. 5 can be created across the entire AIS. Other types of tensor impedance elements besides the “sliced patch” can be used to create the tensor AIS. 
     Surface-wave Waveguide AIS Antennas 
     A variation on the AIS antennas utilizes surface-wave waveguides to confine the surface waves along narrow paths that form one-dimensional ES AISAs. Surface-wave waveguides (SWG) are surface structures that constrain surface-waves (SW) to propagate along a confined path (see, for example, D. J. Gregoire and A. V. Kabakian, “ Surface - Wave Waveguides ,” Antennas and Wireless Propagation Letters, IEEE, 10, 2011, pp. 1512-1515). In the simplest SWG, the structure interacts with surface waves in the same way that a fiber-optic transmission line interacts with light. The physical principle is the same: the wave preferentially propagates in a region of high refractive index surrounded by a region of low refractive index. In the case of the fiber optic, or any dielectric waveguide, the high- and low-index regions are realized with high and low-permittivity materials. In the case of the SWG, the high- and low-index regions can be realized with metallic patches of varying size and/or shape on a dielectric substrate. 
     The surface-wave fields across the width of the SWG are fairly uniform when the width of the SWG is less than approximately ¾ surface-wave wavelength. So, this is a good rule of thumb for the SWG. 
     In a linearly-polarized SWG AISA, the impedance of the SWG varies according to equation Eqn. 2. The impedance elements can be square patches of metal on the substrate or they can be strips that span the width of the SWG. The desired impedance modulation is created by varying the size of the impedance element dimensions with position. 
     In a circularly-polarized SWG, the tensor impedance varies according to equation Eqn. 5 with ϕ=0. The impedance elements can be the sliced patches as described by B. Fong et al. (see the B. Fong et al. article referenced above). The impedance element dimensions are varied with position to achieve the desired impedance variation. 
     BRIEF DESCRIPTION OF THE INVENTION 
     In one aspect the present invention provides a dual-polarization, circularly-polarized artificial-impedance-surface antenna comprising: (1) two adjacent tensor surface-wave waveguides (SWGs); (2) a waveguide feed coupled to each of the two SWGs; (3) a hybrid coupler (which is preferably a 90° coupler) having output ports, each output port of the hybrid coupler being connected to the waveguide feeds coupled to the two SWGs, the hybrid coupler, in use, combining the signals from input ports of the hybrid coupler with phase shifts at its output ports. 
     In another aspect the present invention provides a method of simultaneously transmitting two oppositely handed circularly polarized RF signals comprising the steps of: (i) providing a dielectric surface with a ground plane on one side there of and with a pair of elongate artificial impedance surface antennas, each of said artificial impedance surface antennas including a pattern of metallic geometric stripes or shapes disposed on said dielectric surface, the metallic geometric stripes or shapes having varying sizes which form a repeating moire pattern, the moire patterns of the each of said pair of elongate artificial impedance surface antennas having a angular relationship with reference to a major axis of said pair of elongate artificial impedance surface antennas, a first one of said pair of elongate artificial impedance surface antennas having a positive angular relationship to said major axis and second one of said pair of elongate artificial impedance surface antennas having a negative angular relationship to said major axis; and (ii) applying RF energy to said pair of elongate artificial impedance surface antennas, said RF energy applied to said pair of elongate artificial impedance surface antennas having different relative phases selected such that RF signals transmitted by said pair of elongate artificial impedance surface antennas is circularly polarized. 
     In yet another aspect the present invention provides a method of simultaneously receiving two oppositely handed circularly polarized RF signals comprising the steps of: (i) sending the signals received by two SWGs into two input ports of a 3 dB 90 degree hybrid coupler, the coupler also having two output ports; and (ii) extracting LHCP and RHCP signals from the output two ports of the hybrid coupler. 
    
    
     
       BRIEF DESCRIPTION OF THE DRAWINGS 
         FIG. 1 a    is top view of one embodiment of the present invention disposed on a printed circuit broad while  FIG. 1 b    is a side elevational view thereof. 
         FIG. 2  is a schematic view of another embodiment of a SWG which may be used with the present invention. 
         FIG. 3  is a schematic view of yet another embodiment of a SWG which may be used with the present invention. 
     
    
    
     DETAILED DESCRIPTION 
     This invention provides a solution for a dual-polarization, circularly-polarized AISA with simultaneous Right Hand Circular Polarization (RHCP) and Left Hand Circular Polarization (LHCP) operation. 
     Referring to  FIGS. 1 a  and 1 b   , one possible embodiment of the invention includes a pair of linearly-polarized SWGs  101  and  102  to form the AISA. The polarization of the two SWGs  101 ,  102  is preferably rotated by 90° with respect to each other. The SWGs  101 ,  102  are connected to ports C and D of a 3-dB 90° hybrid coupler  103 , the operation of which is well understood in the state of the art (see, for example, www.microwaves101.com/encyclopedia/hybridcouplers.cfm). The signals at ports C and D are the sum of the signals at ports A and B with preferably either a 90° or a −90° phase shift between them, respectively. The combination of the radiation from the two SWGs  101 ,  102  with the 90° rotation in polarization and the 90° separation in phase results in circularly polarized radiation. It is well known that circularly polarized radiation can be created by combining radiation from two antennas with orthogonal polarization with a 90° phase shift between them. The signal connected to port A is transmitted or received with RHCP polarization while the signal connected to port B simultaneously is transmitted or received with LHCP polarization. Transmit-Receive (TR) switches  104  enable independent operation of each polarization in transmit or receive modes depending on the positions of switches  104 . The two channels are processed in receive mode by conventional front-end electronics  105  and the two channels are provided in transmit mode with transmit signals again by conventional front-end electronics  105 . The conventional front-end electronics  105  may be embodied in or by a transceiver with dual inputs (R 1  and R 2 ) and dual outputs (T 1  and T 2 ) or in or by separate transmitters and receivers or in or by a RF transmit/receive module. 
     Each of the SWGs  101 ,  102  is a linear array of tensor impedance elements  106  that radiate with a polarization preferably at a ±45° angle to the polarization of the SW electric field (in the x axis labeled in  FIG. 1 , the x axis also being the major axis or axis of common elongation of the two SWGs  101 ,  102 ). The tensor elements  106  are preferably metallic shapes printed or otherwise formed on the top surface of a dielectric substrate  109  which preferably has a ground plane  111  disposed the opposing (underside) surface of the dielectric substrate  109 . The metallic shapes can be stripes as shown in  FIGS. 1 a    and  2 , or they can be slit squares as shown in  FIG. 3 . Other electrically conductive shapes can alternatively be utilized as the tensor impedance elements  106  if desired. A ground potential associated with front-end electronics  105  is coupled with the ground plane  111  on bottom side of the dielectric substrate  109 . The SWGs  101 ,  102  should preferably be spaced apart a sufficient distance so that the fields adjacent the SWGs do not couple with each other. In practice the separation distance between SWGs  101 ,  102  is preferably at least ¼λ. 
     The tensor impedance elements  106  can be provided by metallic stripes disposed on a top side of the dielectric substrate  109  where the tensor impedance elements  106  in one channel are angled preferably at +45° with respect to the x axis, and the tilt angle of the stripes in the other channel is set to −45° with respect to that same axis. This variation in tilt angle produces radiation of different linear polarization, that when combined with a 90° phase shift via the 90° hybrid  103 , produces circularly polarized radiation in transmit mode or allow reception of circularly polarized radiation in receive mode. The impedance elements could also be square patches with slices through them as described in B. Fong et al, “ Scalar and Tensor Holographic Artificial Impedance Surfaces ”, noted above. Such an embodiment is depicted by  FIG. 3 . 
     The dielectric substrate  109  may preferably be made from Printed Circuit Board (PCB) material which has a metallic conductor (such as copper) disposed preferably on both of its major surfaces, the metallic conductor on the top or upper surface being patterned using conventional PCB fabrication techniques to define the aforementioned tensor impedance elements  106  from the metallic conductor originally formed on the upper surface of the PCB. The metallic conductor formed on the lower surface of the PCB would then become the ground plane. 
     In transmit operation, the front-end electronics  105  sends two independent signals from its transmit channels (T 1  and T 2 ) to the transmit connections of the two TR switches  104 . The TR switches  104  send the two transmit signals to ports A and B of the 90° hybrid coupler  103 . If the voltages at ports A and B are V A  and V B , then the voltages V C  and V D  at ports C and D are (iV A +V B )/√{square root over (2)} and (V A +iV B )√{square root over (2)}, respectively where i=√{square root over (−1)} and represents a 90° phase shift. 
     The signals from ports C and D of the 90° hybrid coupler  103  pass through optional coaxial cables  110  to end launch Printed Circuit Board (PCB) connectors  107  which are connected to surface-wave (SW) feeds  108 . The coaxial cables  110  and connectors  107  may be omitted if coupler  103  is connected directly the SW feeds  108 , for example. If coaxial cables  110  are utilized, then their respective center conductors are connected to the SW feeds  108  while their shielding conductors are connected to the ground plane  111 . Instead of using coaxial cables  110  to connect outputs of the coupler  103  to the feeds  108 , a link between the two can alternatively be provided by rectangular waveguides, microstrips, coplanar waveguides (CPWs), etc. The SW feeds  108  preferably have a 50 Ω impedance at the end that connects to coupler  103  via the end-launch connector  107  (if utilized). The SW feed  108  flares from one end, preferably in an exponential curve, until its width matches the width of the SWGs  101 ,  102 . The SW feeds  108  launch surface waves with a uniform field across their wide ends into the SWGs  101 ,  102 . The SW feeds  108  are preferably formed using the same techniques to form the tensor impedance elements  106  (this is, by forming them from them the metallic conductor found on a typical PCB). The widths of the SWGs  101 ,  102  is preferably between ⅛ to 2 wavelengths of an operational frequency (or frequencies) of the SWGs  102 ,  102 . 
     The SWGs  101 ,  102  are preferably composed of a series of metallic tensor impedance elements  106  whose sides are preferably angled at ±45° or having angled slices as in the embodiment of  FIG. 3  with respect to the SWG axis (the x-axis in  FIG. 1 ) as noted above. The slices are angled at ±45° with respect to the major axis of the SWGs  101 ,  102  axis so that the polarization angle of each SWG is aligned with its slices. It should be noted that series of metallic tensor impedance elements  106  with angled slices or sides could be angled at some other angle than ±45° with respect to the SWG axis (the x-axis in  FIG. 1 ), but in that case the hybrid coupler  103  has to have a phase shift that is different from 90 degrees at its outputs. Such a hybrid coupler  103  is not believed to be commercially available, so it would be a custom designed coupler, but such a coupler could designed and made if desired. So the angles of ±45° with respect to the SWG axis (the x-axis in  FIG. 1 ) set for the angles of the metallic tensor impedance elements  106  (or the angles of the slices or sides of the as in the embodiment of  FIG. 3 ) is preferred as those angles are believed to be compatible with commercially available hybrid couplers for element  103 . 
     The widths of the individual metallic tensor impedance elements  106  are typically much narrower than the widths of the SWGs  101 ,  102  which they form. In  FIG. 1  the widths of the individual metallic tensor impedance elements  106  averages about 1/7th of the width of the SWGs  101 ,  102 . Typically, the individual metallic tensor impedance elements  106  will be spaced by 1/20 to ⅕ of a wavelength apart from each other along the length of the SWGs  101 ,  102 . The width of the individual metallic tensor impedance elements  106  determines the SW propagation impedance locally along the SWG. The width of the tensor impedance elements  106  varies with distance along the SWG such that the SW impedance is modulated according to equation (Eqn. 2), in order to have the radiation pattern directed at an angle θ determined by equation (Eqn. 3) with respect to the z axis in the x-z plane noted on  FIG. 1 . This variation in the widths of the tensor impedance elements  106  can be seen in  FIG. 1  as a noticeable moire pattern caused by the changing widths of the tensor impedance elements  106 . This pattern repeats itself continuously along the length of the SWG, no matter how long the SWG is. The length of the SWG  101 ,  102  will depend on a number of factors related to the antenna&#39;s engineering parameters, such as desired radiation beam width, gain, instantaneous bandwidth, aperture efficiency, etc. Typically the length of the SWGs  101 ,  102  will fall in the range of 2 to 30 wavelengths at the operational frequency of the SWGs  101 ,  102 . 
     The relation between the impedance-element geometry (e.g. the strip width) and the SW impedance is well understood. See the papers by Patel, Sievenpiper, Colburn, Fong and Gregoire identified above. 
     The metallic tensor impedance elements  106  in SWG  101  are angled in a direction opposite to the tensor impedance elements  106  in the other SWG  102 . The radiation from the two SWGs will be polarized in the direction across the gaps between the strips. Therefore, the radiation from the two SWGs  101 ,  102  depicted by  FIG. 1  will be orthogonal to each other. When the 90° phase shift difference is applied to the feeds  108  with the hybrid power splitter  103 , the net radiation from the combination of the two SWGs  101 ,  102  is circularly polarized. However, as noted above other angles (than45°)for the metallic tensor impedance elements  106  relative to the x-axis can be utilized if a custom designed coupler  103  is employed and still the resulting polarization will be polar. 
     The radiation from each SWG  101 ,  102  is polarized as it is because the slanted metallic strips are tensor impedance elements  106  whose major principal axis is perpendicular to the long edge of the strips and the minor axis is along them. The local tensor admittance of the SWG in the coordinate frame of the principal axes is 
               Y   sw     =     [           Y   ⁡     (   x   )           0           0       0         ]           
where Y(x) is determined by the voltage applied to the metallic strips at position x. Then the SW current is
 
               J   sw     =         Y   sw     ⁢     E   sw       =         [           Y   ⁡     (   x   )           0           0       0         ]     ⁢         E   sw     ⁡     [         1           1         ]       /     2         =       E   sw     /       2     ⁡     [         1           0         ]                   
which is along the major principal axis that is perpendicular to the long edge of the strips forming the tensor impedance elements  106 . The radiation is driven by the SW currents according to
 
 E   rad   ∝[∫[{{circumflex over (k)}×J   sw   }×{circumflex over (k)}]e   −ik·r′   dx]e   ik·r  
 
and is therefore polarized in the direction across the gaps between the strips.
 
     The preferred embodiment for a 12 GHz version of a radiating element of the invention is shown in  FIG. 1 . Everything is scaled to a free-space wavelength at 12 GHz is λ 0 =2.5 cm≅1.0″. The SWGs  101  and  102  are preferably ½λ 0  wide. The exponentially-tapered, surface-wave feeds  108  are preferably 2λ 0  long. The period of the tensor impedance elements  106 ≅ 1/12 λ 0 . 
       FIG. 2  illustrates a preferred embodiment where an RF feed assembly  108  is also disposed at the other of the SWGs with RF terminators  201  attached to the end. This prevents the surface-wave from reflecting off the end of the AISA which could lead to unwanted distortion in the radiation pattern. 
     This concludes the description of embodiments of the present invention. The foregoing description of these embodiments and the methods of making same has been presented for the purposes of illustration and description. It is not intended to be exhaustive or to limit the invention to the precise form or methods disclosed. Many modifications and variations are possible in light of the above teachings. It is intended that the scope of the invention be limited not by this detailed description, but rather by the claims appended hereto.