The present application is related to co-filed application Ser. No. 10/273,872 filed on an even date herewith entitled “A Construction Approach for an EMXT-Based Phased Array Antenna” invented by John C. Mather, Christina M. Conway, James B. West, Gary E. Lehtola, and Joel M. Wichgers. The co-filed application is incorporated by reference herein in its entirety. All applications are assigned to the assignee of the present application.
This invention relates to antennas, phased array antennas, and specifically to a method and structure for interconnecting elements of a phased array antenna.
Phased array antennas offer significant system level performance enhancement for advanced communications, data link, radar, and satellite communications (SATCOM) systems. The ability to rapidly scan the radiation pattern of the array allows the realization of multi-mode operation, LPI/LPD (low probability of intercept and detection), and A/J (antijam) capabilities. One of the major challenges in phased array design is to provide a cost effective and environmentally robust interconnect scheme for the large number of phase shifters within the phased array assembly.
It is well known within the art that the operation of a phased array is approximated to the first order as the product of the array factor and the radiation element pattern as shown in Equation 1 for a linear array 10 of
Standard spherical coordinates are used in Equation 1 and θ is the scan angle referenced to bore sight of the array 10 in
To prevent beam squinting as a function of frequency, broadband phased arrays utilize true time delay (TTD) devices rather than traditional phase shifters to steer the antenna beam. Expressions similar to Equation 1 for the TTD beam steering case are readily available in the literature.
The isotropic radiation element 15 in
The isotropic radiating element 15 is an infinitesimally small, nonphysical mathematical concept that is useful for array analysis purposes. On the other hand, all operational arrays utilize physical radiating elements 25 of finite size as shown in the array 20 of
A comparison of
What is needed is an interconnect scheme for phased array antennas that is low profile and high density and allows it to be embedded within the phased array structure.
A phased array antenna with a plurality of phase shifter elements for phase shifting and beam steering a radiated beam of the phased array antenna is disclosed. The phase shifter elements are interconnected with an interconnect structure comprising a plurality of substrate slats that form walls of the phased array antenna. Each of the substrate slats has a metal substrate for supporting the substrate slat. A first dielectric layer is applied to the metal substrate in selected areas. Metal bias/control circuitry is applied to the selected areas on the first dielectric layer. A second dielectric layer is applied over the bias/control circuitry. A shielding metal layer is applied over the second dielectric layer. Circuit terminations are connected to the metal bias/control circuitry for control signals and bias voltages and to the shielding metal layer for a ground connection. A phase shifter device is attached to the substrate slat and connected to the circuit terminations and is used for phase shifting and beam steering the radiated beam of the phased array antenna. Additional circuit terminations are connected to the metal bias/control circuitry and the shielding metal layer for receiving supply voltages and phase shifter control signals from an external beam steering computer.
The substrate slat may have a connection between the shielding layer and the metal substrate formed by a path through the first dielectric layer and the second dielectric layer. The circuit terminations may be located on the same side of the substrate slat as the metal bias/control circuitry. Alternately, the circuit terminations may be located on a side opposite of the metal bias/control circuitry on the substrate slat.
The phase shifter device may be attached to the substrate slat by solder bump connections to the circuit terminations. Alternately the phase shifter device may be attached to the substrate slat with a bonding method and wirebond connections are made to the circuit terminations. The bonding method may be an adhesive bonding method or a metallurgical bonding method.
The phase shifter device may be a digital phase shifter and may be a true time delay device, MEMS switched line, high pass/low pass, reflection, reactive loaded line and a latching ferrite.
The phase shifter device may be an analog phase shifter and may be an MMIC FET, varactor microstrip, varactor stripline, ferrite microstrip, ferro microstrip, ferrite stripline, ferro stripline, EMXT sidewall, reciprocal ferrite, ferroelectric, and latching ferrite.
It is an objective of the present invention to eliminate the need for bulky and complicated bias and control wiring harnesses for a phased array antenna.
It is an objective of the present invention to orient the bias/control wiring so its thickness, rather than its width, is in the space between radiating elements of a phased array antenna.
It is an advantage of the present invention to be applicable to a wide range of phased array antenna topologies and phase shifter architectures.
It is an advantage of the present invention to create vertical and horizontal interconnect schemes for two-dimensional and three-dimensional (generally conformal) array architectures.
It is a feature of the present invention to offer an interconnect scheme reliability improvement because part of the control circuitry can be embedded within the array, reducing the conductor count between the beam steering computer and the phased array.
The invention may be more fully understood by reading the following description of the preferred embodiments of the invention in conjunction with the appended drawings wherein:
The invention described herein effectively resolves the phased array interconnect problem by utilizing fine pitch, high-density circuitry in a thin self-shielding multi-layer printed wiring assembly. The new approach utilizes the thickness dimension of an array aperture wall (parallel to bore sight axis) to provide the surface area and volume required to implement all of the conductive traces for phase shifter bias, ground, and control lines. The thickness of the printed wiring assemblies 35 are now in the x-y plane (front view) of the radiating elements 25 in the phased array 30 as shown in
The phased array antenna interconnect concept described herein has wide ranging utility for several classes of existing and next generation RF/microwave/millimeter wave phase shifter technologies.
In an end fire array, end fire radiating elements may be disposed on four walls in a square configuration with parallel pairs of walls and with an open input end and an open radiating end similar to a waveguide array shown in
The waveguide phased array antenna is made up of an array of waveguides located adjacent to each other as shown in
The first option is a PWB (printed wiring board) centered in the waveguide in horizontal or vertical planes (block 44). Again digital 45 and analog 46 phase shifter options exist. In the digital 45 category, the same type of phase shifters may be used as with the end fire printed antenna as indicted by block 42. In the analog (block 46) category, the same type of phase shifters may be used as with the end fire antenna as indicated by block 43. The centered PWB 44 options in
The second waveguide phase shifter interconnect option is for phase shifter substrates on the waveguide sidewalls in a vertical plane as indicted by block 49. Analog (block 50) category phase shifters include EMXT (electromagnetic crystal) sidewall phase shifters (51). EMXT devices are also known as tunable photonic band gap (PBG) and tunable electromagnetic band gap (EBG) substrates in the art. A detailed description of a waveguide section with tunable EBG phase shifter technologies is available in a paper by J. A. Higgins et al. “Characteristics of Ka Band Waveguide using Electromagnetic Crystal Sidewalls” 2002 IEEE MTT-S International Microwave Symposium, Seattle, Wash., June 2002.
The third waveguide phase shifter interconnect option is for material loaded waveguides with interconnect either in a vertical or horizontal plane (block 52). Analog 53 category phase shifters include reciprocal ferrite or ferroelectric phase shifters as shown by block 55. Digital 54 phase shifters include latching ferrite devices as shown by block 56.
While it is understood that
The phase shifters described in
Digital phase shifters are typically controlled with a parallel bus with a control line count equal to the number of bits in the phase shifter. For example, a 5-bit phase shifter needs five control lines plus ± voltage lines and chassis ground. Also, since an electrically large phased array requires an enormous amount of digital control data, a serial bus is typically used between a beam steering computer (BSC) and the phased array, with a serial-to-parallel translation occurring at the radiating element level. An additional feature of this invention is that the serial-to-parallel bus translation can occur by means of embedded digital circuitry within the interconnect assembly 35 of
The analog class of phase shifters in
The subsequent detailed descriptions of the invention embodiments emphasize microwave and millimeter wave phase shifting and true time delay (TTD) technologies along with conventional printed wiring board metallic interconnect lines. Note that this invention can be generalized to include optical circuit interconnect, block 48 in
Given the above, the packaging and interconnect challenge is to create an interconnect scheme to deliver electrical signals to each phase shifting device/circuit in a phased array antenna (or an antenna sub-array) having multiple (even hundreds or thousands) active elements. For simplicity and clarity, the present interconnect invention is discussed in detail by describing its application to a specific implementation. Extension and scalability of the ideas from this specific example to other situations should then be readily apparent to those skilled in the art.
The specific implementation example is an EMXT (electromagnetic crystal)-based phased array antenna using waveguide radiating elements operating at 38 GHz as represented by block 51 in
To illustrate some representative dimensions, an example beam former antenna operating at 38.5 GHz is shown in
A circuitized substrate slat 80 approach for achieving reliable EMXT device 61 (see
A semiconductor-based EMXT device 61 is relatively brittle and fragile. Accordingly, its mounting structure should provide some protection from mechanical shock, flexing, and/or stressing due to expansion/contraction during temperature cycling. The coefficient of thermal expansion (CTE) expansion of the mounting structure should be closely matched to that of the EMXT device 61. Kovar or Alloy 42 would be good choices, having CTE of approximately 5.0 to 5.5 ppm/° C. Thickness in the range of 0.005″ is suitable for the mounting structure 80.
To fabricate circuitry, alternating layers of thinfilm dielectric material(s) and metal(s) are deposited and configured (imaged) in sequence. Applicable well-established deposition processes include spinning, curtain coating, vacuum deposition, electrodeposition, and/or electroless deposition. Configuring/imaging processes may include machining (including laser), etching, or the like to remove unwanted material; or deposition through a contact mask so the deposited material reaches the substrate slat 80 only in the desired locations. For some dielectric material types, photosensitive versions are available to facilitate imaging.
An example application sequence for the substrate slat 80 in
It may be desirable to have the shielding layer 84 grounded to the metal substrate 82. One approach is to ensure that dielectric material from the first layer 81 and the second layer 88 is absent from selected areas on the metal substrate 82 prior to deposition of the shielding layer 84, so the electrical connection to the metal substrate 82 is made during shielding layer 84 deposition. This connection path can be accomplished in a continuous manner or through a series of closely spaced small holes 89 that are formed in the dielectric layers 81 and 88 using a laser ablation process or some alternate method. Coatings/circuitry can be applied to one or both sides of a substrate slat 80, as required.
The location of circuit terminations 85 and 86 for electrical connection to the EMXT device 61 can be on either side of the substrate slat 80. Terminations 85 and 86 may be on the same side of the substrate slat 80 as the shielded bias/control circuitry 83. An opening in the shielding layer may be required to reveal each electrically isolated bias pad 85. Ground connections 86 may be made directly to the shielding metal substrate 82.
Terminations 85 and 86 may be on the side of the substrate slat 80 opposite the shielded bias/control circuitry 83. Ground connections 86 may be made directly to the metal substrate 82. Bias connections 85 require a via through the substrate 80 and electrical isolation from the metal substrate 82. Metalization of the via can be accomplished during bias/control circuit 83 creation.
Additional circuit terminations 87 may be required elsewhere on the substrate to facilitate attachment of a connector or other means for receiving bias/ground and control signals from a source external to the substrate slat 80.
There are at least two options for EMXT device 61 mechanical attachment and electrical connection. Solder bump attachment to the EMXT device 61 backside may be used to secure the device and accomplish the required ground 86 and bias 85 connections. Underfill of the EMXT device 61 may be used to enhance the attachment ruggedness. Wirebonds to the EMXT device 61 topside for ground 86 and bias 85 connections may be made and a bonding method such as adhesive or metallurgical bonding may be used to attach the device backside to the substrate slat 80. To accomplish this alternative, it may be necessary to extend the metal substrate 82 so the substrate bond pads 85 and 86 lie beyond the periphery of the EMXT device 61. Extending the metal substrate 82 in this manner may have a negative effect on antenna performance.
The overall approach described above permits assembly of devices 61 to one face of a substrate slat 80 or possibly to both faces. If the device 61 attachment is to one face of the substrate slat 80, then device/slat subassemblies may be placed back-to-back without electrical interaction because the bias circuitry 83 is fully enclosed/shielded.
Methods for forming circuits can place the bias connection pads 85 for the EMXT device 61 on either side of the substrate slat 80, either on the circuit 83 side of the slat 80 or on the side of the substrate slat 80 opposite the circuit traces 83. The decision regarding whether to attach the phase shifting devices 61 to the circuit side or to the substrate side may depend on mechanical issues surrounding the application.
The thickness of the circuitized metal substrate 82 is minimized when a thinfilm approach is used. This is particularly attractive for higher frequency antennas where space is at a greater premium because λo/2 decreases with increasing frequency. For the analog EMXT-based phase array being discussed, the bias conductors 83 ideally do not carry any current, so conductor cross section may be quite small. For reference, typical dimensions for this thinfilm approach are as follows. Dielectric layers 61 may range from approximately 1 to 25 μm (micrometers), depending on the type of material and application method. A typical spin-on polyimide thickness is from approximately 1 to 2 μm. A typical paraylene-C thickness ranges from 10 to 25 μm. Parylene is a common generic name for a series of polymer coatings based on paraxylene. Metal layer 83 and 84 thickness could range widely, depending on the need and the method of deposition. Typical thickness from vacuum deposition is about 0.1 to 2 μm. Typical thickness from electroless deposition is about 0.3 to 3 μm and typical thickness from electrodeposition is about 1 to 50 μm. Thus, the entire thickness of a substrate slat 80 with one shielded circuit structure might be about 0.0064″. The metal substrate 82 is approximately 127 μm (0.005″), two dielectric layers 81 at 15 μm each totals 30 μm (0.0012″) and two metal layers at 2 μm each total 4 μm (0.0002″) for grand total of 161 μm (0.0064″). The 0.0064″ total meets the target value of approximately 0.013″ established for two circuitized substrates. If the metal substrate has shielded circuitry on two sides, the total thickness is about 195 μm, or less than 0.008″.
There is a printed wiring board (pwb) technology alternative to the thinfilm approach delineated above. Very thin pwb circuit materials may be utilized to create the shielded circuitry. One candidate is Kapton polyimide flexible circuit material, which is available in 1- and 2-mil dielectric film thickness and with 0.5-oz (0.0007″ thick) copper on each side (total thickness 0.0024″ for the 1-mil film version). A circuit may be fabricated so one copper face is the shield layer and the other is the bias/control circuitry. The bias/control side of the circuit would be bonded to the substrate using typical pwb lamination material and processes, yielding a bondline thickness of approximately 0.002″. The ground interconnect to the substrate can be achieved using laser ablated blind holes that are then plated to form the connection. The total thickness for a substrate with circuitry on one side would be about 0.010″. Note that although the discussion above indicates one layer of bias/control interconnect circuitry, it would be possible to create multiple layers of bias lines with each layer pair being separated by dielectric.
There are manufacturing and test related advantages to the interconnect methodology presented herein. The important factor is that active devices and/or circuits are assembled on the flat circuitized substrate. Industry standard automated placement and solder reflow attachment of devices can readily be accomplished. Additionally, these populated subassemblies can be DC probed and/or actively tested (e.g., RF reflection test) prior to irreversibly committing the subassembly to a phased array assembly. Individual devices that are found to be defective may be removed and replaced.
Other phase shifter types have current density and voltage bias and control requirements that differ from those required by the EMXT waveguide phase shifters discussed in detail herein. The invention disclosed herein is readily adaptable to these cases.
It is believed that the method and structure for phased array antenna interconnect of the present invention and many of its attendant advantages will be understood by the foregoing description, and it will be apparent that various changes may be made in the form, construction and arrangement of the components thereof without departing from the scope and spirit of the invention or without sacrificing all of its material advantages, the form herein before described being merely an explanatory embodiment thereof. It is the intention of the following claims to encompass and include such changes.
This invention was made under Government contract No. CAAD19-01-9-001 awarded by DARPA. The Government may have certain rights in the invention.
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