Patent Application
20050099355
The present invention relates to the field of communications, and more particularly, to a multiband phased array antenna.
Existing microwave antennas include a wide variety of configurations for various applications, such as satellite reception, remote broadcasting, or military communication. The desirable characteristics of low cost, light weight, low profile and mass producibility are provided in general by printed circuit antennas.
The simplest forms of printed circuit antennas are microstrip antennas wherein flat conductive elements, such as monopole or dipole antenna elements, are spaced from a single essentially continuous ground plane by a dielectric sheet of uniform thickness. An example of a microstrip antenna is disclosed in U.S. Pat. No. 6,417,813 to Durham, which is assigned to the current assignee of the present invention and is incorporated herein by reference in its entirety.
The antennas are designed in an array and may be used for communication systems requiring such characteristics as low cost, light weight and a low profile. The bandwidth of such antennas is about 10-to-1. However, a 10-to-1 bandwidth can be limiting for certain applications. For example, electronic warfare support measures (ESM) and electronic intelligence (ELINT) radar systems require antennas having a bandwidth typically greater than 20-to-1, which offers a higher probability of intercepting signals.
One approach for increasing the bandwidth of an array of dipole antenna elements is disclosed in U.S. Pat. No. 6,552,687 to Rawnick et al., which is also assigned to the current assignee of the present invention and is incorporated herein by reference in its entirety. The multiband phased array antenna in the '687 patent includes a first array of dipole antenna elements operating over a first frequency band, and a second array of dipole antenna elements operating over a second frequency band so that the phased array antenna is a multiband antenna.
The size of the dipole antenna elements in the first array is different from the size of the dipole antenna elements in the second array. Consequently, the ground plane spacing is different between the first and second arrays. One disadvantage of this configuration is that since the higher frequency dipole antenna elements are surrounded by the lower frequency dipole antenna elements, there is a gap or hole in the aperture distribution of the lower frequency dipole antenna elements. Consequently, the layout of the different size antenna elements in the '687 patent presents difficulties in controlling the antenna pattern since this gap or hole may have undesired effects, such as raising the sidelobe levels of the antenna. In addition, the fact that the physical aperture size does not change over a large bandwidth (approximately 10:1) means that the electrical size of the aperture will vary considerably over the band, making this approach unsuitable as a feed for a reflector.
A different type antenna that offers a wide bandwidth (greater than 20-to-1) is a spiral antenna. To cover multiple frequency bands, multiple spirals may be used, i.e., a spiral for each frequency band. However, the multiple spirals are non-concentric about the focal point of the antenna when operating as a feed for a reflector, which results in a loss of efficiency due to scan loss compared to that of a completely concentric aperture. In addition, another disadvantage is that the efficiency of spiral antennas is typically much less than 50% since their performance depends on an absorber-filled back cavity.
In view of the foregoing background, it is therefore an object of the present invention to provide a multiband antenna that has high efficiency while achieving a constant beamwidth and pattern control.
This and other objects, features, and advantages in accordance with the present invention are provided by a multiband phased array antenna comprising a substrate, and a plurality of dipole element arrays extending outwardly from an imaginary center point on the substrate. Each dipole element array may comprise a plurality of dipole antenna elements arranged in an end-to-end relation and having a dipole size different than a dipole size of dipole antenna elements of at least one other dipole element array.
The plurality of dipole element arrays may be radially distributed from the imaginary center point, with the radial distribution being symmetrical. The radial distribution of the dipole element arrays advantageously provides a constant beamwidth when operating the multiband phased array antenna as a reflector feed since all of the arrays use the same focal point. In addition, the pattern of the multiband phased array antenna can be more easily controlled because the radial distribution of the dipole element arrays provides a choice of the radial feed point location, thereby allowing the electrical size of the aperture to be kept relatively constant.
The multiband phased array antenna further comprises a ground plane adjacent the plurality of dipole element arrays, and a spacing between the plurality of dipole element arrays and the ground plane may be different between the dipole element arrays having different size dipole antenna elements. The ground plane may have a plateau shape for providing the different spacing between the plurality of dipole element arrays.
Each dipole antenna element may comprise a printed conductive layer. The plurality of dipole antenna elements are preferably sized and relatively positioned within each respective dipole element array so that the multiband phased array antenna has a total bandwidth equal to or greater than 20-to-1.
The plurality of dipole antenna elements in each dipole element array are preferably arranged in rows and columns, with outer columns of dipole antenna elements being resistively loaded. The passive elements in the outer columns allow the active elements in the center column to receive sufficient current, which is normally conducted through the dipole antenna elements on the substrate. Feed lines are connected to at least one inner column of dipole antenna elements.
Each dipole antenna element comprises a medial feed portion and a pair of legs extending outwardly therefrom. Adjacent legs of adjacent dipole antenna elements may include respective spaced apart end portions having predetermined shapes and relative positioning to provide increased capacitive coupling between the adjacent dipole antenna elements. Each leg may comprise an elongated body portion, and an enlarged width end portion is connected to an end of the elongated body portion. The spaced apart end portions in adjacent legs may comprise interdigitated portions.
The multiband phased array antenna may further comprise a respective impedance element electrically connected between the spaced apart end portions of adjacent legs of adjacent dipole antenna elements for further increasing the capacitive coupling therebetween. Alternately, a respective printed impedance element may be adjacent the spaced apart end portions of adjacent legs of adjacent dipole antenna elements for further increasing the capacitive coupling therebetween.
Another aspect of the present invention is directed to a method for making a multiband phased array antenna by providing a substrate or multiple substrates, and forming a plurality of dipole element arrays extending outwardly from an imaginary center point on the substrate. Each dipole element array may comprise a plurality of dipole antenna elements arranged in end-to-end relation and having a dipole size different than a dipole size of dipole antenna elements of at least one other dipole element array.
The present invention will now be described more fully hereinafter with reference to the accompanying drawings, in which preferred embodiments of the invention are shown. This invention may, however, be embodied in many different forms and should not be construed as limited to the embodiments set forth herein. Rather, these embodiments are provided so that this disclosure will be thorough and complete, and will fully convey the scope of the invention to those skilled in the art. Like numbers refer to like elements throughout, and prime, double prime and triple prime notations are used to indicate similar elements in alternative embodiments.
Referring initially to
Since the multiband phased array antenna 50 covers multiple frequency bands, each transceiver 561-56n functions over one or more frequency bands. The BFN 54 controls the phase of the multiband phased array antenna 50 to create the desired sum and difference patterns, which forms the desired antenna beams, as readily understood by those skilled in the art. An example BFN 54 is a Butler matrix.
One aspect of the multiband phased array antenna 50 comprises a substrate 60, and a plurality of dipole element arrays 62, 64 extending outwardly from an imaginary center point 66 on the substrate, as illustrated in
Each dipole element array 62, 64 comprises a plurality of dipole antenna elements 70a, 70b arranged in an end-to-end relation and having a dipole size different than a dipole size of dipole antenna elements of at least one other dipole element array. Each dipole element array 62, 64 is arranged in rows and columns, such as the 3×5 arrays illustrated in
As will be discussed in greater detail below, the center column of dipole antenna elements 70a, 70b are active, whereas the outer columns of dipole antenna elements are passive. The passive elements in the outer columns allow the active elements in the center column to receive sufficient current, which is normally conducted through the dipole antenna elements 70a, 70b on the substrate 60.
The multiband phased array antenna 50 illustrated in
To increase the total bandwidth, additional dipole element arrays may simply be added to the substrate 60 to cover a different frequency range. For example, if the additional dipole element arrays (not shown) cover 1 to 4 GHz, then the total bandwidth is significantly increased to 28-to-1.
The size of the dipole antenna elements 70b in the low-frequency band arrays 64 is different than the size of the dipole antenna elements 70a in the high-frequency band arrays 62. In particular, the size of the dipole antenna elements 70a in the high-frequency band arrays 62 is less than the size of the dipole antenna elements 70b in the low-frequency band arrays 64.
The multiband phased array antenna 50 further includes a ground plane 80.
The different spacing between the ground plane 80 and the respective dipole antenna elements 70a, 70b may be provided by a plateau shaped ground plane. In other words, the ground plane 80 has a stepped shape or thickness between the low-frequency band arrays 64 and the high-frequency band arrays 62. A dielectric material 81 may be between the ground plane 80 and the respective dipole antenna elements 70.
Referring now to
Between 2 and 4 GHz, however, the VSWR significantly increases for the outer ports (ports 4 and 5), whereas for the inner ports (ports 1, 2 and 3), the VSWR slightly increases. Each port 72 is a different radial distance from the phase center of the multiband phased array antenna—which is the imaginary center point 66 on the substrate 60.
Since the wavelength changes as the frequency changes, it is preferred that the multiband phased array antenna 50 remains electrically the same for the different size dipole antenna elements 70a, 70b. The radial distance of each port 72 from the phase center 66 determines the beamwidth. Consequently, a corresponding transceiver 561-56n may be connected to any one of the five ports 72 and receive substantially the same antenna performance. This is because the electrical size of the various feeds 90 remains substantially the same as the frequency varies across the multiband phased array antenna by choosing the correct port 50.
Nonetheless, the transceivers 561-56, may be selectively connected to a particular port 72 within the radial distribution of dipole antenna elements 70a, 70b to achieve constant beamwidth and pattern control. Similarly, the dipole antenna elements 70 for the different frequency bands may be weighted (e.g., amplitude weighted) to also achieve constant beamwidth and pattern control, as readily appreciated by those skilled in the art.
A single transceiver may be connected to one or more of the five ports 72 on the low-frequency band arrays 64, or multiple transceivers may connected. For example, a first transceiver 561 operating over the frequency range of 4-to-8 GHz may be connected to port 1, a second transceiver 562 operating over the frequency range of 8-to-12 GHz may be connected to port 2, and a third transceiver 563 operating over the frequency range of 12-to-18 GHz may be connected to port 3. Different transceivers 564-56n may likewise be connected to the different ports on the high-frequency band arrays 62.
Since the high and low frequency band arrays 62, 64 operate over different frequency bands, the respective transceivers 561-56n can operate simultaneously. Even though the illustrated low and high frequency bands are continuous (4-to-18 GHz and 18-to-28 GHz), the multiband phased array antenna 50 may be designed to operate over non-continuous frequency bands, as readily appreciated by those skilled in the art. For example, the low-frequency band arrays 64 may still cover 4 to 18 GHz, but the high-frequency band arrays 62 may cover a different frequency band, such as 30 to 33 GHz instead of 18 to 28 GHz, for example.
Referring to
Adjacent legs 74 of adjacent dipole antenna elements 76 have respective spaced apart end portions 78 to provide increased capacitive coupling between the adjacent dipole antenna elements, as shown in
The adjacent dipole antenna elements 76 have predetermined shapes and relative positioning to provide the increased capacitive coupling. For example, the capacitance between adjacent dipole antenna elements 76 is between about 0.016 and 0.636 picofarads (pF), and preferably between 0.159 and 0.239 pF. Of course, these values will vary as required depending on the actual application to achieve the same desired bandwidth, as readily understood by one skilled in the art.
As shown in
Each dipole antenna element array 62, 64 has a desired frequency range (4 to 18 GHz or 18 to 28 GHz, for example) and the spacing between the end portions 78 of adjacent legs 74 is less than about one-half a wavelength of a highest desired frequency.
Alternatively, as shown in
To further increase the capacitive coupling between adjacent dipole antenna elements 76, a respective discrete or bulk impedance element 110″ is electrically connected across the spaced apart end portions 78″ of adjacent legs 74″ of adjacent dipole antenna elements, as illustrated in
In the illustrated embodiment, the spaced apart end portions 78″ have the same width as the elongated body portions 82″. The discrete impedance elements 110″ are preferably soldered in place after the dipole antenna elements 70a, 70b have been formed so that they overlay the respective adjacent legs 74″ of adjacent dipole antenna elements 76. This advantageously allows the same capacitance to be provided in a smaller area, which helps to lower the operating frequency of the respective dipole antenna element arrays 62, 64.
The illustrated discrete impedance element 70″ includes a capacitor 112″ and an inductor 114″ connected together in series. However, other configurations of the capacitor 112″ and inductor 114″ are possible, as would be readily appreciated by those skilled in the art. For example, the capacitor 112″ and inductor 114″ may be connected together in parallel, or the discrete impedance element 110″ may include the capacitor without the inductor or the inductor without the capacitor. Depending on the intended application, the discrete impedance element 110″ may even include a resistor.
The discrete impedance element 110″ may also be connected between the adjacent legs 74 with the overlapping or interdigitated portions 80 illustrated in
Another advantage of the respective discrete impedance elements 110″ is that they may have different impedance values so that the bandwidth of the respective dipole antenna element arrays 62, 64 can be tuned for different applications, as would be readily appreciated by those skilled in the art. In addition, the impedance is not dependent on the impedance properties of the adjacent dielectric layer 81. Since the discrete impedance elements 110″ are not effected by the dielectric layer 81, this approach advantageously allows the impedance between the dielectric layer 81 and the impedance of the discrete impedance element 110″ to be decoupled from one another.
Yet another aspect of the present invention is directed to selectively coupling a discrete impedance element 110a″-110n″ between a respective pair of adjacent legs 74″ of adjacent dipole antenna elements, as illustrated in
A switch controller 77″ is connected to all of the switches 75″ in the multiband phased array antenna 50. The switch controller 77″ may operate so that the respective impedance elements 110a″-110n″ associated with all of the dipole antenna elements 70a, 70b are synchronously switched. Alternately, the respective impedance elements 110a″-110n″ for each dipole antenna element 70a, 70b may be asynchronously switched with respect to the other dipole antenna elements.
The switches 75″ and corresponding impedance elements 110a″-110n″ advantageously allow the multiband phased array antenna 50 to be retuned. For example, the frequency band of the phased array antenna may be adjusted, i.e., lower or higher. This adjustment may be as much as 10 to 20 percent of the frequency band depending on the range of the impedance values associated with the impedance elements 110a″-110n″. In addition, better performance may be achieved at specific frequencies, particularly where the antenna can be better matched, i.e., to operate with a lower VSWR. The active switching may also be combined with the variable height ground plane 80, as readily appreciated by those skilled in the art.
Yet another approach to further increase the capacitive coupling between adjacent dipole antenna elements 76 includes placing a respective printed impedance element 110″′ adjacent the spaced apart end portions 78″′ of adjacent legs 74″′ of adjacent dipole antenna elements 76, as illustrated in
The respective printed impedance elements 110″′ are separated from the adjacent legs 74″′ by a dielectric layer, and are preferably formed before the dipole antenna layer is formed so that they underlie the adjacent legs 74″′ of the adjacent dipole antenna elements 76. Alternatively, the respective printed impedance elements 110″′ may be formed after the dipole antenna layer has been formed. For a more detailed explanation of the printed impedance elements, reference is directed to U.S. patent application Ser. No. 10/308,424 which is assigned to the current assignee of the present invention, and which is incorporated herein by reference.
Referring now to
The resistive load may include a discrete resistor 120, as illustrated in
The respective printed resistive elements 122 may be printed before, during or after formation of the dipole antenna elements 70a, 70b, as would also be readily appreciated by those skilled in the art. The resistance of the load is typically selected to match the impedance of a feed line connected to an active dipole antenna element, which is in a range of about 50 to 100 ohms.
Other aspects of the present invention will now be discussed. One such aspect is still directed to a multiband phased array antenna 150, as illustrated in
However, the multiband phased array antenna 150 comprises a substrate 160, and a plurality of dipole element arrays 161, 162, 163, 164 and 165 extending outwardly from an imaginary center point 166 on the substrate 160. The imaginary center point 166 is not necessarily the center of the substrate 160, but may be slightly off center.
Each dipole element array 161-165 comprises a plurality of dipole antenna elements (generally referred to by reference numeral 170) arranged in end-to-end relation and having a dipole size different than a dipole size of dipole antenna elements of at least one other dipole element array. In other words, each dipole element array 161-165 is sized to cover a respective frequency band so that collectively, the multiband phased array antenna 150 covers a wide bandwidth.
As the dipole element arrays 161-165 decrease from a larger size to a smaller size, the frequency inversely changes, as readily understood by those skilled in the art. For example, the five dipole element arrays may cover the following five frequency bands: 0.1 to 1 GHz for dipole element array 161, 1 to 2 GHz for dipole element array 162, 2 to 4 GHz for dipole element array 163, 4 to 8 GHz for dipole element array 164, and 8 to 16 GHz for dipole element array 165.
Only five dipole element arrays 161-165 within a single “pie” section are illustrated in
Each dipole element array 161-165 includes an active dipole antenna element (which is the center element), and may include passive dipole antenna elements adjacent to the active element. The passive dipole antenna elements include a resistive load (not shown) connected across the medial feed portions. The resistive load may be a discrete resistor 120, as illustrated in
The actual size of each dipole element array 161-165 may vary, as readily appreciated by those skilled in the art. As illustrated in
As noted above, a ground plane for a multiband phased array antenna is preferably spaced from the different size dipole element arrays 161-165 less than about one-half a wavelength of a highest desired frequency within each respective array. Referring now to
In other words, the illustrated ground plane 180 is sloping so that the spacing between the ground plane and the dipole element arrays 161-165 increases. Alternately, the dipole element arrays 161-165 may be positioned so that the spacing between the ground plane 180 and the dipole element arrays 161-165 decreases. When the slope of the ground plane 180 increases, the lower frequency arrays are positioned on the substrate 160 further away from the imaginary center point 166, whereas the higher frequency arrays are positioned closer to the imaginary center point. Furthermore, the position of each dipole element array 161-165 on the substrate 160 may also be radially adjusted for the different frequency bands to achieve a constant beamwidth across the total bandwidth.
The slope of the ground plane 180 does not necessarily have to be constant. For example, the slope of the ground plane 180 may be logarithmic or exponential. In this case, position of the dipole element arrays 161-165 would be adjusted accordingly to provide the preferred spacing between the ground plane 180 and the respective dipole antenna elements 170 based upon their size. A dielectric material 181 is between the ground plane 180 and the respective dipole antenna elements 170.
Depending on the desired overall size of the multiband phased array antenna 150, crowding of the dipole antenna elements 170 within each pie section on the substrate 160 could be a problem. One approach to alleviating this problem is to turn the outermost passive dipole antenna elements near the edge of the substrate 90 degrees, as illustrated in
In this embodiment of the multiband phased array antenna 150′, the substrate has a first surface 160a′, and a second surface 160b′ adjacent thereto and defining an edge 169′ therebetween. In the illustrated embodiment, the second surface 160b′ is orthogonal to the first surface 160a′. The substrate 160a′, 160b′ may be a monolithic flexible substrate, and the second surface is formed by simply bending the substrate so that one of the legs of the edge elements 170b′ extends onto the second surface.
Dipole element arrays 163′, 164′ and 165′ extend outwardly from the imaginary center point 166′ only the first surface 160a′ of the substrate 160a′, and dipole element arrays 161′ and 162′ extend outwardly from the imaginary center point 166′ on both the first and second surfaces 160a′, 160b′ of the substrate. The dipole antenna elements on the first surface of the substrate 160a′ are indicated by reference 170a′, whereas the dipole antenna elements on the second surface of the substrate 160b′ (partially or fully thereon) are indicated by reference 170b′.
The dipole antenna elements 170b′ on the second surface 160b′ of the substrate may also be referred to as “edge elements.” A plot of the computed VSWR versus frequency for the low frequency dipole element array 161′ having a dipole antenna element 170b′ on the second surface 160b′ of the substrate is represented by line 186 in
Another aspect of the present invention is directed to a multiband phased array antenna 250, as illustrated in
Each dipole element array 262 comprises a plurality of dipole antenna elements 270a-270e arranged in end-to-end relation and having different dipole sizes for dipole antenna elements in a direction extending outwardly from the imaginary center point 266. In other words, the multiband phased array antenna 250 is “graded” in the sense that the size of the dipole antenna elements 270a-270e changes from the imaginary center point 266 toward the outer edge of the substrate 260.
Each illustrated dipole element array 262 comprises five active dipole antenna elements 270a-270e. The actual number of elements could vary depending on the intended application. The multiband phased array antenna 250 may cover the following frequency bands: dipole antenna element 270a covers 0.1 to 1 GHz, dipole antenna element 270b covers 1 to 2 GHz, dipole antenna element 270c covers 2 to 4 GHz, dipole antenna element 270d covers 4 to 8 GHz and dipole antenna element 270e covers 8 to 16 GHz. Of course, the active dipole antenna elements 270a-270e vary in size to cover different frequency bands, as readily appreciated by those skilled in the art.
As noted above, a ground plane for a multiband phased array antenna is preferably spaced from the different size dipole element arrays 262 less than about one-half a wavelength of a highest desired frequency within each respective array. Referring now to
The illustrated ground plane 280 is sloping so that the spacing between the ground plane and the dipole antenna elements 270a-270e increases as you move from the imaginary center point 266 toward the outer edge of the substrate 260. Consequently, the lower frequency dipole antenna elements 270d and 270e are positioned on the substrate 260 further away from the imaginary center point 266, whereas the higher frequency dipole antenna elements 270a, 270b and 270c are positioned closer to the imaginary center point.
The transceivers 561-56n may be selectively connected to a particular port within the radial distribution of dipole antenna elements 270a-270e to achieve constant beamwidth and pattern control. Although not illustrated in
As noted above, the slope of the ground plane 280 does not necessarily have to be constant. For example, the slope of the ground plane 280 may be logarithmic or exponential. In this case, position of the dipole element arrays 262 would be adjusted accordingly to provide the preferred spacing between the ground plane 280 and the respective dipole antenna elements 270a-270c based upon their size. A dielectric material 281 is between the ground plane 280 and the respective dipole antenna elements 270a-270e.
Yet another aspect of the present invention is directed to a multiband phased array antenna 350, as illustrated in
The plurality of dipole element arrays 361-365 are concentric about the imaginary center point 366. This is in contrast to the dipole element arrays in the multiband phased array antennas 50, 150 and 250 as discussed above, which are all radially distributed with respect to an imaginary center point.
Each dipole element array 361-365 comprises a plurality of dipole antenna elements 370a-370e arranged in an end-to-end relation and having a dipole size different than a dipole size of dipole antenna elements of at least one other dipole element array. The specific features of the dipole antenna elements as discussed above are also applicable to the multiband phased array antenna 350, and will not be discussed in any greater detail.
In the illustrated embodiment, each concentric polygonal ring (i.e., a dipole element array) includes N individual dipole antenna elements, wherein N=8. The actual number N of individual dipole antenna elements can vary depending on the intended application. For example, the lower limit of N may be 3, and the upper end of N may be determined by the intended application.
The ground plane 380 for the multiband phased array antenna 350 is preferably spaced from the different size dipole element arrays 361-365 less than about one-half a wavelength of a highest desired frequency within each respective array. Referring now to
The illustrated ground plane 380 is sloping so that the spacing between the ground plane and the dipole antenna elements 370a-370e increases as you move from the imaginary center point 366 toward the outer edge of the substrate 360. Consequently, the lower frequency dipole antenna elements 370a, 370b (i.e., arrays 361, 362) are positioned on the substrate 360 further away from the imaginary center point 366, whereas the higher frequency dipole antenna elements 370a, 370b, 370c (i.e., 363, 364, 365) are positioned closer to the imaginary center point.
The transceivers 561-56n may be selectively connected to a particular concentric ring to achieve constant beamwidth and pattern control. As noted above, the slope of the ground plane 380 does not necessarily have to be constant. For example, the slope of the ground plane 380 may be logarithmic, exponential, or stepped. In this case, position of the dipole element arrays would be adjusted accordingly to provide the preferred spacing between the ground plane 380 and the respective dipole antenna elements 370a-370e based upon their size. A dielectric material 381 is between the ground plane 380 and the respective dipole antenna elements 370a-370e.
The concentric rings are illustrated as being circumscribed in a circle, but they may also be circumscribed in any other shape, such as an ellipse. The concentric rings may also be triangular or rectangular, as readily appreciated by those skilled in the art. In addition, the spacing of the concentric rings may be symmetrical, as shown in
Measured and computed VSWR versus frequency over a frequency band of 2 to 18 GHz for the multiband phased array antenna 350 is provided in
In addition, other features relating to the multiband phased array antennas are disclosed in copending patent applications filed concurrently herewith and assigned to the assignee of the present invention and are entitled PHASED ARRAY ANTENNA WITH SELECTIVE CAPACITIVE COUPLING AND ASSOClATED METHODS, attorney docket number GCSD-1493 (51349); MULTIBAND POLYGONALLY DISTRIBUTED PHASED ARRAY ANTENNA AND ASSOCIATED METHODS, attorney docket number GCSD-1488 (51350); MULTIBAND RADIALLY DISTRIBUTED GRADED PHASED ARRAY ANTENNA AND ASSOCIATED METHODS, attorney docket number GCSD-1487 (51351); and MULTIBAND RADIALLY DISTRIBUTED PHASED ARRAY ANTENNA WITH A SLOPING GROUND PLANE AND ASSOCIATED METHODS, attorney docket number GCSD-1486 (51352), the entire disclosures of which are incorporated herein in their entirety by reference.
Many modifications and other embodiments of the invention will come to the mind of one skilled in the art having the benefit of the teachings presented in the foregoing descriptions and the associated drawings. Therefore, it is understood that the invention is not to be limited to the specific embodiments disclosed, and that modifications and embodiments are intended to be included within the scope of the appended claims.
