The present invention relates generally to millimeter wave radio frequency (RF) systems and, more particularly, to efficient design of antennas operable in the millimeter wave frequency band.
The 60 GHz band is an unlicensed band which features a large amount of bandwidth and a large worldwide overlap. The large bandwidth means that a very high volume of information can be transmitted wirelessly. As a result, multiple applications, each requiring transmission of large amounts of data, can be developed to allow wireless communication around the 60 GHz band. Examples for such applications include, but are not limited to, wireless high definition TV (HDTV), wireless docking stations, wireless Gigabit Ethernet, and many others.
In order to facilitate such applications, there is a need to develop integrated circuits (ICs) such as amplifiers, mixers, radio frequency (RF) analog circuits, and active antennas that operate in the 60 GHz frequency range. An RF system typically comprises active and passive modules. The active modules (e.g., a phased array antenna) require control and power signals for their operation, which are not required by passive modules (e.g., filters). The various modules are fabricated and packaged as radio frequency integrated circuits (RFICs) that can be assembled on a printed circuit board (PCB). The size of the RFIC package may range from several to a few hundred square millimeters.
In the consumer electronics market, the design of electronic devices, and thus RF modules integrated therein, should meet be designed to minimize cost, size, power consumption, and weight. The design of the RF modules should also take into consideration the current assembled configuration of electronic devices and, particularly, handheld devices such as laptop, smartphones, and tablet computers, in order to enable efficient transmission and reception of millimeter wave signals. Furthermore, the design of the RF module should account for minimal power loss of receive and transmit RF signals as well as for maximum radio coverage.
A schematic diagram of a RF module 100 designed for transmission and reception of millimeter wave signals is shown in
In the transmit mode, the RF circuitry 120 typically performs up-conversion, using a mixer (not shown in
In both receive and transmit modes, the operation of the RF circuitry 120 is controlled by the baseband module using a control signal. The control signal is utilized for functions such as gain control, RX/TX switching, power level control, beam steering operations, and so on. In certain configurations, the baseband module also generates the LO and power signals and transfers such signals to the RF circuitry 120. The power signals are DC voltage signals that power the various components of the RF circuitry 120. Normally, the IF signals are also transferred between the baseband module and the RF circuitry 120.
In common design techniques, the array of active antennas 110-1 to 110-N are implemented on the substrate upon which the IC of the RF circuitry 120 is also mounted. An IC is typically fabricated on a multi-layer substrate and metal vias that connect between the various layers. The multi-layer substrate may be a combination of metal and dielectric layers and can be made of materials such as a laminate (e.g., FR4 glass epoxy, Bismaleimide-Triazine), ceramic (e.g., low temperature co-fired ceramic LTCC), polymer (e.g., polyimide), PTFE (Polytetrafluoroethylene) based compositions (e.g., PTFE/Ceramic, PTFE/Woven glass fiber), Woven glass reinforced materials (e.g., woven glass reinforced resin), wafer level packaging, and other packaging, technologies and materials. The cost of the multi-layer substrate is a function of the area of the layer—the greater the area of the layer, the greater the cost of the substrate.
Antenna elements of the array of active antennas 110-1 to 110-N are typically implemented by having metal patterns in a multilayer substrate. Each antenna element can utilize several substrate layers. In conventional implementations for millimeter wave communications, antenna elements are designed to occupy a single side of the multi-layer substrate side. This is performed in order to allow the antenna radiation to properly propagate.
For example, a millimeter wave (mm-wave) RF module 200 depicted in
In order to maximize the coverage of a millimeter wave RF module, the RF module operates according to the specification of the IEEE 802.11ad (also known as the WiGig), such that a large number of antennas should be included in the RF module. Some conventional RF designs require implementing a number of active antennas on one side of the substrate, thereby providing a constraint that limits the number of antennas of the RF module. Another conventional design includes placing a number of antennas on different sides of the substrate, thereby enabling the RF signal to radiate in all directions.
In both of the above noted approaches, an attempt to increase the number of active antennas would require increasing the area of substrate. Also, such an attempt would require increasing the length of the wires (traces) from the RF circuitry to the antenna elements. Further, some antennas require differential signal feeding via, e.g., a balun structure which consumes substrate area. In this case, a problem arises as some area of the substrate should be reserved for other structures, such as antenna feed lines. Any design of a RF module designed with a large number of antennas should meet the constraints of an efficient design. Such constraints necessitate that the physical dimensions, power consumption, heat transfer, and cost be minimized whenever possible.
Typically, the antennas that require differential signal feeding via, e.g., a balun structure, are dipole and Yagi-types antennas. More specifically, a dipole antenna is typically fed by two arms that are 180° out of phase with respect to each other. The arms must have equal electric field amplitude distribution. When a dipole is fed from an unbalanced source (unequal field distribution), such as a coax or microstrip, a balun is used to transition the source transmission line from an unbalanced state to a balanced state. The balanced transmission line is generally in the form of a two-wire line.
Additionally, when fed over a ground plane, a dipole antenna needs to be on the order of a quarter-wavelength from the ground so that the dipole is not shorted to the ground plane.
In existing solutions, the feed line from the ground to the dipole is typically designed using a balanced line. The balun is implemented in an earlier stage of the antenna as a separate component. This requires more space and line length, which are disadvantages in a system that is space limited. Other solutions use the quarter wavelength section from the ground as a matching section and part of the balun. However, this type of balun cannot support a broadband frequency range.
Another design constraint that should be considered when providing an RF module with a large number of millimeter-wave antennas is the connection of an antenna to multiple amplifiers for increased transmission power and/or reception sensitivity. Typically, such a connection requires an extra circuit element: a power combiner. The power combiner can be in the form of a simple T-junction or a more complex Wilkinson divider. In either case, extra line length and circuitry must be added for the combiner and any associated matching network. As a result, a problem arises with such designs as the area of the substrate is limited and should be reserved for other structures. Thus, an attempt to increase the number of antennas in a mm-wave RF module while meeting the above-noted constraints would significantly increase the area of the module's substrate and, therefore, reduce the efficiency of the RF module.
It would be therefore advantageous to provide an efficient design for mm-wave antennas that overcomes the disadvantages noted above.
Certain embodiments disclosed herein include a printed millimeter wave dipole antenna. In one embodiment, the dipole antenna comprises: a signal wing and at least one ground wing for propagating signals in a millimeter wave band; and an unbalanced feeding structure directly coupled to the signal wing, wherein the unbalanced feeding structure is boarded by a plurality of escorting vias to ensure equipotential grounds.
In another embodiment, the dipole antenna comprises a first dipole wing and a second dipole wing for propagating signals in a millimeter wave band; and a balanced feeding structure construed to include a first feed stripline connected to the first dipole wing and the second feed stripline connected to the second dipole wing.
In yet another embodiment, the dipole antenna comprises a first dipole wing and a second dipole wing for propagating signals in a millimeter wave band; and a balanced feeding structure construed to include a feed stripline and a balun, wherein the dipole antenna is printed on a metal layer between ground layers of a substrate.
The subject matter disclosed herein is particularly pointed out and distinctly claimed in the claims at the conclusion of the specification. The foregoing and other objects, features, and advantages of the disclosed embodiments will be apparent from the following detailed description taken in conjunction with the accompanying drawings.
It is important to note that the embodiments disclosed herein are only examples of the many advantageous uses of the innovative teachings herein. In general, statements made in the specification of the present application do not necessarily limit any of the various claimed inventions. Moreover, some statements may apply to some inventive features but not to others. In general, unless otherwise indicated, singular elements may be in plural and vice versa with no loss of generality. In the drawings, like numerals refer to like parts through several views.
As noted above, in order to increase the radio coverage of a mm-wave RF module, a large number of antennas should be included in the module. Various mm-wave antennas designed to allow a compact RF module while meeting design constraints are disclosed herein. The disclosed embodiments also include techniques for designing such mm-wave antennas.
According to one embodiment, a stripline fed dipole antenna may not include an explicit balun. Typically, a balun structure is utilized in an antenna fed with a differential signal. The disclosed embodiment allows designing a RF module with a differential dipole antenna while minimizing the substrate area.
The signal wing 310 is fed through a stripline 330. In one embodiment, the stripline 330 is a transmission line guided by two ground layers 340-1 and 340-2 of substrate 350. The substrate 350 is the substrate of the RF module (see for example,
In an exemplary embodiment, the length of each of the dipole wings 310 and 320 is about a quarter of wavelength in the material and together the dipole wings form a simple and efficient half wavelength dipole. The distance between the shielding vias 361 and the dipole wings 310 and 320 is also about one quarter wavelength in the material in order to ensure constructive interference and forward radiation direction. The disclosed stripline fed dipole antenna is specifically designed to transmit/receive millimeter wave signals at the 60 GHz frequency band.
The stripline fed dipole antenna illustrated in
It should be appreciated from
It should be noted that the stripline fed antenna, once designed to meet the constraints, permanently remains after the design process such that the structure performance can be optimized despite the un-balanced signals caused due to the lack of a balun device feeding the antenna.
In another embodiment, a millimeter-wave dipole antenna is printed on a multilayer substrate and is fed by two separate stripline feed points that combine to a differential line at the antenna. Such a structure behaves as an antenna, as a power combiner, and as a stripline to a differential line transformer all in one package or element. According to an embodiment, the combined element can be implemented as a single dipole or as a dipole that feeds Yagi-Uda type directors.
A section 703 of the ground plane extends out over the differential feed line in order to reduce the impedance of the line to improve the impedance match. The design shown in
It should be further noted that the dipole antenna structure as shown in
According to another embodiment, the antenna dipole 700 can act as a Yagi-Uda driven element. A Yagi-Uda antenna is a directional antenna that includes a driven element and additional parasitic elements, commonly known as directors. According to this embodiment, a ground layer of the substrate of the RF module (see for example,
In one embodiment, the directors 705 and 706 can be placed in the same plane with the dipoles wings' and grounds' plane. In another embodiment, not shown in
It should be appreciated that the proposed solution allows the antenna to cover an appropriately broad bandwidth in a dense antenna environment with less impact on the routing and feeding footprint because the balun, power divider, and impedance transformer are all incorporated into the structure of the antenna. The proposed solution is also useful in designs where high gain and beam forming requirements demand the use of multiple antennas and architecture limitations require that they be fitted in a small area. It should be further appreciated that the proposed solution allows the antenna to be fed with twice the output power, or a 3 dB increase in equivalent isotropically radiated power (EIRP), without external circuitry.
In another embodiment, a millimeter-wave dipole antenna is printed on a multilayer substrate and fed by a tapered balun. The tapered balun transitions from unbalanced stripline to balanced stripline and is part of the quarter wavelength section that feeds the dipole from the ground plane to save space. In one embodiment, the tapered balun can also be utilized to feed Yagi-Uda type directors.
The tapered balun 1010 extends from the ground layers to the signal wing 1001. In one embodiment, the tapered balun is shaped as a trapezoid where the base 1012 of the tapered balun 1010 is wider than the base 1011. In one embodiment, the base 1012 tapers to the width of the signal line at the feed point of the balun 1010. The width of the base 1012 is designed to be several ground layer (plane) spacings wide, where ground layer spacing is the dielectric thickness between the ground layer and signal layer in a microstrip or stripline transmission line.
The length of the base 1012 should be determined based on several considerations. These considerations may include, but are not limited to, impedance and balance effects and ground space effects. As a non-limiting example, if the based 1012 is too wide, then the taper 1010 can act as an extended ground plane for the dipole distributing the quarter wave spacing. Also, because after two or three ground plane spacings from the signal line the electric field is very weak, there is no benefit of having the taper start out wider than more than two to three ground plane spacings. In another non-limiting example, if the base 1012 of a tapered balun 1010 is too narrow, this would result in a large discontinuity, thereby disturbing the balance of the feed lines and the impedance match causing a reduction in impedance bandwidth. The discontinuity also makes the feed line sensitive to other bends and radii in the feed network. In an exemplary and non-limiting embodiment, the width of the base is 2 ground plane spacings.
According to another embodiment, the antenna dipole 1000 can act as a Yagi-Uda driven element. In this embodiment, the ground layer of the substrate of the RF module acts as the reflector and signal directors 1005 and 1006 are placed in front of the dipole wings 1001 and 1002. In one embodiment, the directors 1005 and 1006 can be placed in the plane with the dipoles wings and ground's planes, respectively. In another embodiment, the directors 1005 and 1006 can be placed above and/or below the plane of the dipole at the same radial distance from the dipole as the in plane director. This arrangement increases the gain of the antenna without increasing the lateral extent of the array. It should be noted that the directors 1005 and 1006 appear to be in the same plane in
It should be appreciated that the proposed solution allows the antenna to cover an appropriately broad bandwidth in a dense antenna environment with less impact on the routing and feeding footprint, since the balun and impedance transformer are all incorporated into the structure of the antenna. According to an embodiment, the tapered balun 1010 acts as an impedance transformer, allowing the dipole to be more naturally matched to its resonant impedance by tapering the feed lines at their end points to the appropriate matching impedance. It should be noted that the natural impedance of the dipole may be slightly different from the feed line. In order to optimize the antenna match, the impedance of the feed line may be changed by tapering its width to more suitable impedance for maximum power transfer.
The millimeter-wave dipole antenna 1000 can be used in antenna sub-arrays located in the middle layer of a substrate of an RF module. An example for such RF module is further discussed in U.S. patent application Ser. No. 13/729,553, referenced above.
At S1450, a balun distance from the ground edge is defined such that the resulting differential mode is stable. At S1460, the antenna is simulated and check matching is performed. If this step does not result in achieving sufficient bandwidth, S1410 through S1440 and S1460 are repeated after increasing the space from the ground for wider matching, increasing or decreasing dipole length to reach lower or higher center frequency, and adjusting other parameters accordingly.
Once sufficient bandwidth has been achieved, the antenna pattern is simulated at S1470. Then, at S1480, the parameters ground size, distance to ground, distance to dielectric edge, and via distance to tune pattern are changed. In some embodiments, additional directors may be added for higher gain at the expense of antenna size. At S1490, the pattern simulation performed at S1470 is repeated to verify that matching is not affected. If matching has been affected, the pattern and matching must be co-tuned.
It should be noted that the method for designing optimized Quasi Yagi antenna and the dipole antennas disclosed herein, can be implemented in any computer aided design (CAD) tools utilized in the design of RFICs.
It is important to note that the disclosed embodiments are only examples of the many advantageous uses of the teachings discussed herein. Specifically, the teachings disclosed herein can be adapted in any type of consumer electronic devices where reception and transmission of millimeter wave signals is needed. More particularly, the teachings of the present invention can be used in design of miniaturized RFICs utilized in devices supporting applications operable in the 60 GHz frequency band. Such applications include, but are not limited to, wireless high definition TV (HDTV), wireless docking station, wireless Gigabit Ethernet, wireless local area network over 60 GHz, and many others. The 60 GHz frequency band applications are designed to be integrated in portable devices including, but not limited to, netbook computers, tablet computers, smartphones, laptop computers, and the like. It should be appreciated that as physical size of such devices is relatively small, thus the area for installing additional circuitry to support 60 GHz applications is limited, hence the disclosed techniques for designing millimeter wave antenna are highly suitable for implementation of RFICs for 60 GHz band applications.
All examples and conditional language recited herein are intended for pedagogical purposes to aid the reader in understanding the principles of the disclosed embodiments and the concepts contributed by the inventor to furthering the art, and are to be construed as being without limitation to such specifically recited examples and conditions. Moreover, all statements herein reciting principles, aspects, and embodiments of the invention, as well as specific examples thereof, are intended to encompass both structural and functional equivalents thereof. Additionally, it is intended that such equivalents include both currently known equivalents as well as equivalents developed in the future, i.e., any elements developed that perform the same function, regardless of structure.
This application claims the benefit of U.S. Provisional Application No. 61/831,963 filed Jun. 6, 2013, U.S. Provisional Application No. 61/881,123 filed Sep. 23, 2013, U.S. Provisional Application No. 61/881,119 filed Sep. 23, 2013, and U.S. Provisional Application No. 61/925,011 filed on Jan. 8, 2014. All of the applications referenced above are herein incorporated by reference.
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