The present disclosure relates to compound loop antenna.
As new generations of cellular phones and other wireless communication devices become smaller and embedded with increased applications, new antenna designs are required to address inherent limitations of these devices and to enable new capabilities. With conventional antenna structures, a certain physical volume is required to produce a resonant antenna structure at a particular frequency and with a particular bandwidth. However, effective implementation of such antennas is often confronted with size constraints due to a limited available space in the device.
Antenna efficiency is one of the important parameters that determine the performance of the device. In particular, radiation efficiency is a metric describing how effectively the radiation occurs, and is expressed as the ratio of the radiated power to the input power of the antenna. A more efficient antenna will radiate a higher proportion of the energy fed to it. Likewise, due to the inherent reciprocity of antennas, a more efficient antenna will convert more of a received energy into electrical energy. Therefore, antennas having both good efficiency and compact size are often desired for a wide variety of applications.
Conventional loop antennas are typically current fed devices, which generate primarily a magnetic (H) field. As such, they are not typically suitable as transmitters. This is especially true of small loop antennas (i.e. those smaller than, or having a diameter less than, one wavelength). The amount of radiation energy received by a loop antenna is, in part, determined by its area. Typically, each time the area of the loop is halved, the amount of energy which may be received is reduced by approximately 3 dB. Thus, the size-efficiency tradeoff is one of the major considerations for loop antenna designs.
Voltage fed antennas, such as dipoles, radiate both electric (E) and H fields and can be used in both transmit and receive modes. Compound antennas are those in which both the transverse magnetic (TM) and transverse electric (TE) modes are excited, resulting in performance benefits such as wide bandwidth (lower Q), large radiation intensity/power/gain, and good efficiency. There are a number of examples of two dimensional, non-compound antennas, which generally include printed strips of metal on a circuit board. Most of these antennas are voltage fed. An example of one such antenna is the planar inverted F antenna (PIFA). A large number of antenna designs utilize quarter wavelength (or some multiple of a quarter wavelength), voltage fed, dipole antennas.
Use of MIMO (multiple input multiple output) technologies is increasing in today's wireless communication devices to provide enhanced data communication rates while minimizing error rates. A MIMO system is designed to mitigate interference from multipath environments by using several transmit (Tx) antennas at the same time to transmit different signals, which are not identical but are different variants of the same message, and several receive (Rx) antennas at the same time to receive the different signals. A MIMO system can generally offer significant increases in data throughput without additional bandwidth or increased transmit power by spreading the same total transmit power over the antennas so as to achieve an array gain. MIMO protocols constitute a part of wireless communication standards such as IEEE 802.11n (WiFi), 4G, Long Term Evolution (LTE), WiMAX and HSPA+. However, in a configuration with multiple antennas, size constraints tend to become severe, and interference effects caused by electromagnetic coupling among the antennas may significantly deteriorate transmission and reception qualities. At the same time, efficiency may deteriorate in many instances where multiple paths are energized and power consumption increases.
An antenna system is provided, including a first antenna, a second antenna, a ground plane, and a resonant isolator coupled to the first and second antennas. Each of the antennas is configured to be a capacitively-coupled compound loop antenna, and the resonant isolator is configured to provide isolation between the two antennas at resonance. The two antennas may be symmetrical or asymmetrical and include a first element that emits a magnetic field and a second element that generates an electrical field that is orthogonal to the magnetic field. The radiating element of the second element may be capacitively coupled to the remainder of the second element. The resonate isolator may be comprised of a single conductive element or two conductive elements that are capacitively coupled.
In view of known limitations associated with conventional antennas, in particular with regard to radiation efficiency, a compound loop antenna (CPL), also referred to as a modified loop antenna, has been devised to provide both transmit and receive modes with greater efficiency than a conventional antenna with a comparable size. Examples of structures and implementations of the CPL antennas are described in U.S. Pat. No. 8,144,065, issued on Mar. 27, 2012, U.S. Pat. No. 8,149,173, issued on Apr. 3, 2012, and U.S. Pat. No. 8,164,532, issued on Apr. 24, 2012. Key features of the CPL antennas are summarized below with reference to the example illustrated in
Similar to a conventional loop antenna that is typically current fed, the loop element 108 of the planar CPL antenna 100 generates a magnetic (H) field. The radiating element 120, having the series resonant circuit characteristics, effectively operates as an electric (E) field radiator (which of course is an E field receiver as well due to the reciprocity inherent in antennas). The connection point of the radiating element 120 to the loop element 108 is critical in the planar CPL antenna 100 for generating/receiving the E and H fields that are substantially orthogonal to each other. This orthogonal relationship has the effect of enabling the electromagnetic waves emitted by the antenna to effectively propagate through space. In the absence of the E and H fields arranged orthogonal to each other, the waves will not propagate effectively beyond short distances. To achieve this effect, the radiating element 120 is placed at a position where the E field produced by the radiating element 120 is 90° or 270° out of phase relative to the H field produced by the loop element 108. Specifically, the radiating element 120 is placed at the substantially 90° (or 270°) electrical length along the loop element 108 from the feed point 112. Alternatively, the radiating element 120 may be connected to a location of the loop element 108 where current flowing through the loop element 108 is at a reflective minimum.
In addition to the orthogonality of the E and H fields, it is desirable that the E and H fields are comparable to each other in magnitude. These two factors, i.e., orthogonality and comparable magnitudes, may be appreciated by looking at the Poynting vector (vector power density) defined by P=E×H (Volts/m×Amperes/m=Watts/m2). The total radiated power leaving a surface surrounding the antenna is found by integrating the Poynting vector over the surface. Accordingly, the quantity E×H is a direct measure of the radiated power, and thus the radiation efficiency. First, it is noted that when the E and H are orthogonal to each other, the vector product gives the maximum. Second, since the overall magnitude of a product of two quantities is limited by the smaller, having the two quantities (|H| and |E| in this case) as close as possible will give the optimal product value. As explained above, in the planar CPL antenna, the orthogonally is achieved by placing the radiating element 120 at the substantially 90° (or 270°) electrical length along the loop element 108 from the feed point 112. Furthermore, the shapes and dimensions of the loop element 108 and the radiating element 120 can be each configured to provide comparable, high |H| and |E| in magnitude, respectively. Therefore, in marked contrast to a conventional loop antenna, the planar CPL antenna can be configured not only to provide both transmit and receive modes, but also to increase the radiation efficiency.
Size reduction can be achieved by introducing a series capacitance in the loop element and/or the radiating element of the CPL antenna. Such an antenna structure, referred to as a capacitively-coupled compound loop antenna (C2CPL), has been devised to provide both transmit and receive modes with greater efficiency and smaller size than a conventional antenna. Examples of structures and implementations of the C2CPL antennas are described in U.S. patent application Ser. No. 13/669,389, entitled “Capacitively Coupled Compound Loop Antenna,” filed Nov. 5, 2012. Key features of C2CPL antennas are summarized below with reference to the example illustrated in
As explained above, the C2CPL antennas are capable of achieving high efficiency with reduced size; thus, these antennas are good candidates to be used for a multiple antenna system such as a MIMO system, a USB dongle, etc.
In this example of
As illustrated in
As mentioned earlier, in a configuration where multiple antennas are closely packed, interference effects caused by electromagnetic coupling among the antennas may significantly deteriorate transmission and reception qualities and efficiency. Therefore, an antenna isolation scheme is often needed for a multi-antenna system. This document describes implementations of a resonant isolator configured to couple two antennas in the system to achieve electromagnetic isolation of the antennas at resonance.
In the example of
The first and second end portions, labeled 412B-1 and 412B-2, of the resonant isolator 428 are coupled to the feed points 412A-1 and 412A-2 of Antenna 1 and Antenna 2, respectively. Vertical vias are formed in the first and second layers between points 412A-1/412B-1 and 412A-2/412B-2, with the first via coupling the first end portion 412B-1 of the resonant isolator 428 to the feed point 412A-1 of Antenna 1, and the second via coupling the second end portion 412B-2 of the resonant isolator 428 to the feed point 412A-2 of Antenna 2. The location of the resonant isolator 428 in the second layer is predetermined so as to overlap with the foot print of the first ground plane 418A formed in the first layer. In other words, the first ground plane 418A is configured to overhang the resonant isolator 428. This configuration allows for better frequency tuning than may otherwise be obtainable.
According to an embodiment, the first and second end portions, 412B-1 and 412B-2 of the resonant isolator 428 are coupled to the feed points 412A-1 and 412A-2 of Antenna 1 and Antenna 2, respectively, which is at a point where the current has a maximum value in each antenna. Furthermore, the electrical length of the resonant isolator 428 is configured to be substantially 90° or its odd multiples (270°, 450°, etc.). This configuration provides optimal isolation between the two antennas.
Furthermore, the reflected wave associated with the resonant current on the resonant isolator 428 undergoes a 180° phase shift with respect to the forward wave, since the electrical length of the resonant isolator is set to be 90°. Therefore, the forward wave and the reflected wave, which have the 180° phase offset, are combined to effectively generate an open circuit with respect to the node of the current course, which represents Antenna 1. As such, Antenna 1 and Antenna 2 can be substantially isolated at resonance due to the presence of the resonant isolator 428 that has the electrical length of 90°.
As explained in the foregoing, the two-antenna system according to an embodiment includes two C2CPL antennas de-coupled by the resonant isolator having an electrical length of substantially 90° (or its odd multiple), wherein efficiency is enhanced due to the generation of substantially orthogonal E and H fields, size reduction is achieved by configuring the capacitively coupled antenna elements, and isolation between the two antennas at resonance is enhanced due to the resonant isolator de-coupling the two antennas.
The present disclosure includes just one example of a two C2CPL antenna structure and an embodiment of a resonant isolator. However, any C2CPL antennas, such as those described in the aforementioned U.S. patent application Ser. No. 13/669,389, as well as their variations, may be used to obtain a highly efficient and isolated two-antenna system with small size. It should also be noted that it is also possible to expand the use of the resonant isolator to N antenna systems. Hence, the present disclosure is not limited to only two C2CPL antennas nor is the present disclosure limited to only CPL antennas and could likewise be used with a wide variety of other antennas. In addition, while the resonant isolator for isolating the two antennas is configured for one particular resonance in the above examples, it is possible to reconfigure the resonant isolator to provide isolation at two or more resonances for a multi-band system.
The first and second end portions 912-1 and 912-2 of the resonant isolator 1028 are coupled to the locations near the feed points of Antenna 1 and Antenna 2, respectively, where the current has the maximum value in each antenna. Furthermore, the electrical length of the resonant isolator 928 is configured to be substantially 90° or its odd multiples (270°, 450°, etc.).
In the examples provided above, the two-antenna system operates at a single frequency and the resonant isolator is a contiguous conductive element. The example of a two-antenna system illustrated in
The other end portions of Antennas 1 and 2, which are each opposite to the capacitively coupled edge of the second loop section 1002B, are shorted to the first ground plane 1006A. Antennas 1 and 2 further include two radiating elements, each operating at a different frequency, that are formed in each of the loop sections 1002A and 1002B. For generating/receiving the E and H fields of Antenna 1, which are substantially orthogonal to each other, the radiating element of the second loop section 1002B is placed at the substantially 90° (or 270°) electrical length along the loop element 1002B from the feed point 1002A-1. The same configuration is followed in Antenna 2. The gap 1004 may be configured for size reduction purposes as discussed above.
The implementation of a capacitive loaded resonant isolator as illustrated in
In an embodiment, an antenna system comprises a first layer including at least a pair of antennas having a first antenna and a second antenna, the first layer further including a first ground plane; and a second layer including a resonant isolator and a second ground plane, the resonant isolator having a first end portion and a second end portion and being placed on or within the second layer isolated from the second ground plane, the resonant isolator being configured to isolate the first antenna from the second antenna at a resonance when the first antenna is connected to the first end portion by a first via and the second antenna is connected to the second end portion by a second via, the first via and the second via being vertical to the first layer and the second layer; and wherein each of the first antenna and the second antenna include: a first element that is coupled to a current feed point at a first end point and is shorted to the first ground plane at a second end point, the first element emitting a magnetic field; and a second element that is coupled to the first element at an electrical length of substantially 90 degrees or an odd multiple of substantially 90 degrees from the feed point, the second element generating an electrical field substantially orthogonal to the magnetic field.
In the embodiment, wherein the first element comprises a first section, a second section and a gap formed between the first section and the second section, and wherein the first section and the second section are capacitively coupled through the gap. In the embodiment, wherein the second element comprises a first section, a second section and a gap formed between the first section and the second section, and wherein the first section and the second section are capacitively coupled through the gap.
In the embodiment, wherein the resonant isolator has an electrical length of substantially 90 degrees or an odd multiple of substantially 90 degrees that generates a forward wave and a reflective wave having a phase offset resulting in an open circuit at resonance when the forward and backward waves are combined and thereby providing isolation between the first antenna and the second antenna. In the embodiment, wherein the resonant isolator has an electrical length that provides one of a substantially 90 degree phase delay or an odd multiple of a substantially 90 degree phase delay between the first antenna and the second antenna.
In the embodiment, wherein the first via is coupled to the current feed point of the first antenna where a current value is maximum and the second via is coupled to the current feed point of the second antenna where the current value is maximum.
In the embodiment, wherein the first layer includes N pairs of antennas and the second layer includes N resonant isolators, wherein one resonant isolator among the N resonant isolators corresponds to each pair of antennas among the N pairs of antennas.
In the embodiment, wherein the antenna system is a multi-band antenna system and the resonant isolator is configured to isolate the first antenna from the second antenna at each resonance of the multi-band antenna system.
In the embodiment, wherein the resonant isolator includes a conductive line coupling the first end portion to the second end portion. In the embodiment, wherein the resonant isolator includes a gap formed between the first end portion and the second end portion, and wherein the first end portion and the second end portion are capacitively coupled through the gap.
In an embodiment, an antenna system comprises a first pair of antennas including a first antenna and a second antenna; a ground plane; and a resonant isolator having a first end portion coupled to the first antenna and a second end portion coupled to the second antenna, the resonant isolator being configured to isolate the first antenna from the second antenna at resonance when the first antenna is connected to the first end portion and the second antenna is connected to the second end portion, wherein each of the first antenna and the second antenna comprises: a first element that is coupled to a current feed point at a first end point and is shorted to the ground plane at a second end point, the first element emitting a magnetic field; a second element that is coupled to the first element at an electrical length of substantially 90° or an odd multiple of substantially 90 degrees from the feed point, the second element generating an electrical field substantially orthogonal to the magnetic field.
In the embodiment, wherein the first element comprises a first section, a second section and a gap formed between the first section and the second section, and wherein the first section and the second section are capacitively coupled through the gap. In the embodiment, wherein the second element comprises a first section, a second section and a gap formed between the first section and the second section, and wherein the first section and the second section are capacitively coupled through the gap.
In the embodiment, wherein the resonant isolator has an electrical length of substantially 90 degrees or an odd multiple of substantially 90 degrees that generates a forward wave and a reflective wave having a phase offset resulting in an open circuit at resonance when the forward and backward waves are combined and thereby providing isolation between the first antenna and the second antenna. In the embodiment, wherein the resonant isolator has an electrical length that provides one of a substantially 90 degree phase delay or an odd multiple of a substantially 90 degree phase delay between the first antenna and the second antenna.
In the embodiment, wherein the first end portion is coupled to the first antenna at the current feed point of the first antenna where a current value is maximum and the second end portion is coupled to the current feed point of the second antenna where the current value is maximum.
In the embodiment, wherein the resonant isolator includes a conductive line coupling the first end portion to the second end portion. In the embodiment, wherein the resonant isolator includes a gap formed between the first end portion and the second end portion, and wherein the first end portion and the second end portion are capacitively coupled through the gap.
In the embodiment, wherein the first element is a loop element and the second element is a radiating monopole element.
In the embodiment, wherein the radiating element operates at a first frequency, and wherein first element further includes a second radiating element operating at a second frequency substantially different from the first frequency.
In the embodiment, further comprising N pairs of antennas and N resonant isolators, wherein one resonant isolator among the N resonant isolators corresponds to each pair of antennas among the N pairs of antennas.
In the embodiment, wherein the antenna system is a multi-band antenna system and the resonant isolator is configured to isolate the first antenna from the second antenna at each resonance of the multi-band antenna system.
While this document contains many specifics, these should not be construed as limitations on the scope of an invention or of what may be claimed, but rather as descriptions of features specific to particular embodiments of the invention. Certain features that are described in this document in the context of separate embodiments can also be implemented in combination in a single embodiment. Conversely, various features that are described in the context of a single embodiment can also be implemented in multiple embodiments separately or in any suitable subcombination. Moreover, although features may be described above as acting in certain combinations and even initially claimed as such, one or more features from a claimed combination can in some cases be exercised from the combination, and the claimed combination may be directed to a subcombination or a variation of a subcombination.