CA2095304C - Polarization pattern diversity antenna - Google Patents
Polarization pattern diversity antennaInfo
- Publication number
- CA2095304C CA2095304C CA 2095304 CA2095304A CA2095304C CA 2095304 C CA2095304 C CA 2095304C CA 2095304 CA2095304 CA 2095304 CA 2095304 A CA2095304 A CA 2095304A CA 2095304 C CA2095304 C CA 2095304C
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- Prior art keywords
- antenna
- polarization
- diversity antenna
- pattern diversity
- feed
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- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
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- 238000005516 engineering process Methods 0.000 claims description 4
- 230000011664 signaling Effects 0.000 claims 1
- 230000005855 radiation Effects 0.000 abstract description 11
- 238000005562 fading Methods 0.000 abstract description 7
- 238000004519 manufacturing process Methods 0.000 abstract description 6
- 230000008878 coupling Effects 0.000 abstract description 5
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- 229910052802 copper Inorganic materials 0.000 abstract 2
- 239000010949 copper Substances 0.000 abstract 2
- 238000010295 mobile communication Methods 0.000 abstract 1
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- 238000002955 isolation Methods 0.000 description 3
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- DHSSDEDRBUKTQY-UHFFFAOYSA-N 6-prop-2-enyl-4,5,7,8-tetrahydrothiazolo[4,5-d]azepin-2-amine Chemical compound C1CN(CC=C)CCC2=C1N=C(N)S2 DHSSDEDRBUKTQY-UHFFFAOYSA-N 0.000 description 1
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Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q21/00—Antenna arrays or systems
- H01Q21/24—Combinations of antenna units polarised in different directions for transmitting or receiving circularly and elliptically polarised waves or waves linearly polarised in any direction
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q13/00—Waveguide horns or mouths; Slot antennas; Leaky-waveguide antennas; Equivalent structures causing radiation along the transmission path of a guided wave
- H01Q13/10—Resonant slot antennas
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q9/00—Electrically-short antennas having dimensions not more than twice the operating wavelength and consisting of conductive active radiating elements
- H01Q9/04—Resonant antennas
- H01Q9/0407—Substantially flat resonant element parallel to ground plane, e.g. patch antenna
Landscapes
- Variable-Direction Aerials And Aerial Arrays (AREA)
- Waveguide Aerials (AREA)
- Radio Transmission System (AREA)
Abstract
A polarization pattern diversity antenna is described that is easy to manufacture, has a compact planar shape and radiates a nearly omnidirectional radiation pattern in the horizontal plane. Two feed points, each one attached toa copper patch, are operated in phase and 180° out of phase to separately receive or transmit two different components of a signal. The copper patches are arranged symmetrically on one side of a dielectric layer in such a way as to reduce the r.f coupling between the two modes of operation and thus increase the radiation efficiency and isolate the overall input/output ports for the different signal components. The ground plane, situated on the underside of thedielectric layer, allows the antenna to operate like a resonant slot when the feed points are excited in phase. Using diversity, the antenna can reduce the multipath fading effects inherent in mobile communications
Description
-2- 2Q9~i3~
Field of Invention The present invention relates to antennas and, in particular, to ant~nn~c havinga comp~ct size and the ability to simultaneously receive or transmit two different components of electrom~gnetic energy.
Background Microwave antenn~ are used in many forms of wireless co~unication where information is bro~1c~ct through the air between a transmitter and a receiver.
The main advantage of broadcasting information is that it allows the transmitterand receiver to co~licate without the need for both termin~ to be connected 10 to electrical wires at fi~ed locations. However, there are limits to the locations and motions of the termin~l.s. These limits are imposed by different forms of signal loss that degrade the received signal--free-space loss, terrestrial loss,Doppler frequency shifting and multipath effects.
The multipath effects are the most significant form of loss at microwave 15 frequencies and are particularly problematic in cellular telephony. Between the transmitter and receiver, components of the broadcast signal will travel along different paths, some of which may come across obstacles that scatter, refract, absorb, reflect or re-polarize them. In outdoor co.. ~ ication, these obstacles are typically trees, buildings, cars and the terrain. For indoor co.. ~.~ications, 20 they may be desks, people, walls and partitions.
Some of the signal components will arrive at their destination, but with different amplitudes, phases, polarizations and arrival times. Signal components with different ph~eçfi may destructively interfere, resulting in .si~n~ partially or wholly c~ncelinE each other out. In addition, the polarizations of some of the 25 signal components may be different from the polarization of the receive antenna, leading to further power loss.
The final received signal will have an amplitude and phase that are diffficult to predict and will fluctuate in time with a multipath fading pattern as the receiver moves and the environm~nt changes. Theleîore, it is very diffficult to ensure a 30 clear, consistent signal at the receiver.
Deep fading of the signal as the rece*er moves every half wavelength is inherent in broadcast col~ ications and becomes a signifiç~nt problem at 3 20~5304 microwave frequencies, where a half wavelength is less than one metre. This problem could be overco~e if the components from every signal path are separately received and then comhined in such a way as to çlimin~qte destructiveinterference. However, this task is impossible. A more practical approach is to 5 separately receive two or more fiign~l.e and combine them so that destructive interference is reduced. Each signal can be received by a separate antenna.
Although the amplitude of each signal fluctuates with a multipath fading pattern, the combination of all .sign~l.e fades less frequently. The greatest reduction in destructive interference is achieved when the fiign~l.e have fading10 patterns that are statistically independent, or in other words, all the ~eign~lfi do not experience deep fades simultaneously.
Two or more ~ntenn~.e used in this way are collectively known as a diversity antenna. These antenn~.e can be used in different ways to achieve different forms of diversity. Some of these for_s of diversity are described by William C.15 Y. Lee in Mobile Communica~ion~ Engineering, New York: McGraw-Hill, 1982, pp. 273-289; they are: space diversity, frequency diversity, time diversity, pattern diversity and polarization diversity. Polarization diversity and patterndiversity are employed by the present invention because these forms of diversityenable a compact ~nt~nn~ structure to be designed without requiring any system 20 level changes to the co.~ ications system.
In cellular telephony, diversity (mainly space diversity) has been used at the base stations for a number of years. However, at the portable co.--.. ic~tor side, diversity reception has not been used because of the lack of comp~ct and aesthetic inventions. Therefore, what is needed is an antenna that provides 25 diversity in the receive frequency band of a portable con-n-~-.-icator. The antenna must have a compact and planar shape so that it can conform to the shape of a vehicle or fit inside a portable commtmicator. It must also be built with a simple design and inexpensive materials so that it is easy to manufacture. Furthermore,the mutual coupling between the different modes of operation should be low to 30 provide high radiation efficiency and high isolation between the overall input/oul~u~ ports for the different signal cu~ u~ents.
Field of Invention The present invention relates to antennas and, in particular, to ant~nn~c havinga comp~ct size and the ability to simultaneously receive or transmit two different components of electrom~gnetic energy.
Background Microwave antenn~ are used in many forms of wireless co~unication where information is bro~1c~ct through the air between a transmitter and a receiver.
The main advantage of broadcasting information is that it allows the transmitterand receiver to co~licate without the need for both termin~ to be connected 10 to electrical wires at fi~ed locations. However, there are limits to the locations and motions of the termin~l.s. These limits are imposed by different forms of signal loss that degrade the received signal--free-space loss, terrestrial loss,Doppler frequency shifting and multipath effects.
The multipath effects are the most significant form of loss at microwave 15 frequencies and are particularly problematic in cellular telephony. Between the transmitter and receiver, components of the broadcast signal will travel along different paths, some of which may come across obstacles that scatter, refract, absorb, reflect or re-polarize them. In outdoor co.. ~ ication, these obstacles are typically trees, buildings, cars and the terrain. For indoor co.. ~.~ications, 20 they may be desks, people, walls and partitions.
Some of the signal components will arrive at their destination, but with different amplitudes, phases, polarizations and arrival times. Signal components with different ph~eçfi may destructively interfere, resulting in .si~n~ partially or wholly c~ncelinE each other out. In addition, the polarizations of some of the 25 signal components may be different from the polarization of the receive antenna, leading to further power loss.
The final received signal will have an amplitude and phase that are diffficult to predict and will fluctuate in time with a multipath fading pattern as the receiver moves and the environm~nt changes. Theleîore, it is very diffficult to ensure a 30 clear, consistent signal at the receiver.
Deep fading of the signal as the rece*er moves every half wavelength is inherent in broadcast col~ ications and becomes a signifiç~nt problem at 3 20~5304 microwave frequencies, where a half wavelength is less than one metre. This problem could be overco~e if the components from every signal path are separately received and then comhined in such a way as to çlimin~qte destructiveinterference. However, this task is impossible. A more practical approach is to 5 separately receive two or more fiign~l.e and combine them so that destructive interference is reduced. Each signal can be received by a separate antenna.
Although the amplitude of each signal fluctuates with a multipath fading pattern, the combination of all .sign~l.e fades less frequently. The greatest reduction in destructive interference is achieved when the fiign~l.e have fading10 patterns that are statistically independent, or in other words, all the ~eign~lfi do not experience deep fades simultaneously.
Two or more ~ntenn~.e used in this way are collectively known as a diversity antenna. These antenn~.e can be used in different ways to achieve different forms of diversity. Some of these for_s of diversity are described by William C.15 Y. Lee in Mobile Communica~ion~ Engineering, New York: McGraw-Hill, 1982, pp. 273-289; they are: space diversity, frequency diversity, time diversity, pattern diversity and polarization diversity. Polarization diversity and patterndiversity are employed by the present invention because these forms of diversityenable a compact ~nt~nn~ structure to be designed without requiring any system 20 level changes to the co.~ ications system.
In cellular telephony, diversity (mainly space diversity) has been used at the base stations for a number of years. However, at the portable co.--.. ic~tor side, diversity reception has not been used because of the lack of comp~ct and aesthetic inventions. Therefore, what is needed is an antenna that provides 25 diversity in the receive frequency band of a portable con-n-~-.-icator. The antenna must have a compact and planar shape so that it can conform to the shape of a vehicle or fit inside a portable commtmicator. It must also be built with a simple design and inexpensive materials so that it is easy to manufacture. Furthermore,the mutual coupling between the different modes of operation should be low to 30 provide high radiation efficiency and high isolation between the overall input/oul~u~ ports for the different signal cu~ u~ents.
4 2~9~
Most of the liver~ily antenna research to date has employed space diversity, which is impractical for use in hand held radios because the distance between the antenn-s-q is so large. There is, however, some important work in this area that concentrates on antenna ~le~qign-C with a flat profile.
Most of the liver~ily antenna research to date has employed space diversity, which is impractical for use in hand held radios because the distance between the antenn-s-q is so large. There is, however, some important work in this area that concentrates on antenna ~le~qign-C with a flat profile.
5 Nishikawa et al. as disclosed in U.S. patent 5,146,232 issued on September 8, 1992 have designed two flat antenns..q-- one a table antenna, the other resçmhling a folded F antenna--that operate in diversity when separated by more than 0.4 wavelengths. Although this design is too large for a handset, it can be mounted on a vehicle, rerl~s.~ng the traditional monopoles that can bend 10 or break and may not be aesthetically pleasing.
K. Tsunekawa has created a working diversity system using two planar inverted-F sntçnn~q as described in his article 'D~ fenn~J~ for Portable Telephones," 39th IEEE Vehicular Technology Conference, Vol. 1, May 1989, pp 50-56. By comhinin~ space and angle diversity, he was able to 15 reduce the distance between the antenns-q to 0.1 wavelenth, but the antenns..q are only weakly independent.
Some important work in single, comrsct diversity antenna design is provided by Arai et al as disclosed in '~ Flat Energy Density ~rltenn~ System for Mobile Telephone,"IEEE Trn~ ctic!ns on Vehicular Technol~y, Vol. 40, No. 2, 20 May 1992, pp. 483-486. Their Antenns consists of a center-fed disk above a ground plane with four slots cut radially into the disk. In the plane of this flat-profile antenna, the disk receives an electric field component while the slots receive a msgnetic field component. Thus, field component diversity is achieved in one integrated unit. However, with a diameter of over 0.6 wavelength, this 25 antenna is also impractical for use in a handset.
A simple polarization diversity s~hçme was taught by Lalezari et al over 10 years ago as disclosed in his U.S. patent 4,464,663 issued on August 7, 1984 wherein two feed line nelworhs independently feed a pair of square microstrip patches. This system provides hori7.on~sl and vertical polarizations 30 independently and is said to minimi7.e the coupling between the feed ports, but again, size is a problem. To isolate the patches and make room for the two feed nelwolhs, the structure must be 0.95 wavelenth long.
- 5 - ~ 3 ~ ~i Polarization diversity has been studied by a number of engineers, for e~mple:
Bergman and Arnold as described in 'Polarization Diversity in Portable Communication~ Environment,"Electronic~ Letters, Vol 22, No. 11, 1986;
and W.C.Y. Lee reference previously. The results of these studies conclude that 5 polarization diversity ~ntenn~ offer subshnti~l signal strength i~ rovement over conventional antenn~e in most outdoor en-vilo..ments and in indoor systems where there is no direct line of sight between the fixed base station and the portable CO.. -.f icator. When there is a line of sight, diversity ant~nn~
perform only slightly better than a conventional monopole ~ntenn~ This is 10 because only one polarization of the received signal (usually vertical) is domin~nt. In this case, however, the signal level is usually high and the multipath fading effects are not as severe.
Pattern diversity (or angle diversity) makes use of the observation that most ofthe components of a signal all;villg from different paths also have different 15 angles of arrival. In most mobile envilo.-ment~, the signal components from different angles of arrival will have fading patterns that are statistically independent. Therefore, Lversi~y can be achieved if directional ~ntenn~ are used to isolate these signal components. Research on pattern diversity shows that it offers an improvement in received signal strength over conventional 20 antenna reception, particularly in ellviro~lm~nte where .sign~ are arriving from many different angles. The directivities of the ~nt~nn~.~ must be chosen carefully, however; using highly directional antennas gives good statistical independence but less signal coverage area while using ant~nn~.~ with low directivity gives a broad signal coverage area at the expense of poorer statistical 25 independence.
Summary of Invention The invention herein is directed to a comp~ct, polarization pattern diversity antenna that is (le~igned with hand held cellular telephones in mind. This diversity system is capable of separately and simultaneously receiving both 30 orthogonal polarizations (vertical and horizontal) of an incoming signal and~or components of a signal with different angles of arrival. Whether polarization -6- 2~5~4 diversity or pattern diversity is the main s~hçme in use depends on the orientation of the antenna with respect to the incQming .signs~l.c.
The invention herein employs a pair of conductive patches that are either implanted inside or layered on top of a dielectric material. The patches are 5 rectangular in the preferred embodiment and separated by a narrow gap that resonates like a slot antenna, providing one of the two re.son~nt modes. The other mode is provided by a second slot ~ntçnn~ formed between the two patches and a conductive ground plane affixed beneath the dielectric.
The rlimen.cions of the patches and how and where they are terminated are 10 crucial to the operation of the divel~ily antenna. The back edges of both patches connect to the ground plane, creating a short circuit. This forces an open circuit along the front edges that are a quarter wavelength away at the resonant frequency. The two feed points are located near these front edges, on both sidesof the gap between the two patches. When they are fed with .cign~ of equal 15 ~mplitude and opposite phase, currents form near the gap. These currents giverise to an electrom~gnetic field that radiates across the gap. The polarization of the field is in the direction orthogonal to that of the gap (hereafter referred to as the vertical polarization). When fed by .cign~l.c of equal amplitude and equal phase, the feed points excite currents in the patch that, because of the open 20 circuit condition, can only flow along the front edges of the two patches. Hence, an electric potential is eshhli.ched between these front edges and the ground plane resulting in an electromagnetic field that radiates from the structure with a polarization perpendicular to a line between the feed points (hereafter calledthe horizontal polarization).
25 The dielectric material is not es.s~nti~l to the operation of the antenna, but it provides mech~nical stability and decreases the physical size. Materials with larger dielectric con~t~nts will decrease the size even further, but at the ç~rpen.ce of concentrating the electrom~gnetic fields inside the material and thus preventing some radiation.
30 Using the dielectric material also allows the use of printed circuit technology in its fabrication, which has many advantages. The manufacturing process is inexpensive and accurate, m~king it readily ~men~hle to mass production. Also, 7 2Q~3~4 this technology is compatible with integrated circuits, which can be mounted directly on the board, and feed lines and matching nelwo~hs can be fabricated onthe same dielectric. The light weight, compact size and planar geometry of the dielectric make it easy to use where small size is important or conformity with a 5 structure is required. Microstrip antennas like this one are also rugged enough to withstand climatic changes and are essentially maint~n~nce free.
Variations to the basic invention include embodiments where modifications have been made to any part of the antenna in order to change the physical or electrical properties without ~h~n~ing the basic operation of the ~nt~nn~ Such 10 modifications include but are not limited to cutting slots and~or holes of any shape into any of the conductive surfaces, carving wells into the dielectric, th:3nging the positions of the feed points, tapering any of the conductive surfaces, tapering the dielectric, using dielectrics with non-homo~eneous permittivities, curving or bending parts of or all of the embodiment, inserting 15 grounding posts, adding matching circuits, filters or rectifiers, removing the dielectric, enclosing one or more surfaces of the embodiment with dielectric material, and using physical designs other than printed circuit te-hnology.
Objects of In~e.ltion The objects of the present invention are to provide an antenna that:
20 1. is easy to manufacture;
2. has a compact and planar shape so that it can conform to the shape of a vehicle or fit inside a portable telephone or other co.-~n~..icator;
3. receives or transmits two components of a signal separately and simultaneously. These two components are received using polarization diversity 25 and/or pattern diversity. The motivation for this property is to reduce the multipath fading effects in mobile collln~ cations at high frequencies, but thisproperty can also be used for other applications and in other systems;
4. minimi7.eS the r.f. coupling between the two modes of operation so as to provide high radiation efficiency and high isolation between overall input/oul~ul 30 ports for the different polarizations;
5. radiates each desired polarization nearly omnidirect~o~lly in one plane of the antenna.
K. Tsunekawa has created a working diversity system using two planar inverted-F sntçnn~q as described in his article 'D~ fenn~J~ for Portable Telephones," 39th IEEE Vehicular Technology Conference, Vol. 1, May 1989, pp 50-56. By comhinin~ space and angle diversity, he was able to 15 reduce the distance between the antenns-q to 0.1 wavelenth, but the antenns..q are only weakly independent.
Some important work in single, comrsct diversity antenna design is provided by Arai et al as disclosed in '~ Flat Energy Density ~rltenn~ System for Mobile Telephone,"IEEE Trn~ ctic!ns on Vehicular Technol~y, Vol. 40, No. 2, 20 May 1992, pp. 483-486. Their Antenns consists of a center-fed disk above a ground plane with four slots cut radially into the disk. In the plane of this flat-profile antenna, the disk receives an electric field component while the slots receive a msgnetic field component. Thus, field component diversity is achieved in one integrated unit. However, with a diameter of over 0.6 wavelength, this 25 antenna is also impractical for use in a handset.
A simple polarization diversity s~hçme was taught by Lalezari et al over 10 years ago as disclosed in his U.S. patent 4,464,663 issued on August 7, 1984 wherein two feed line nelworhs independently feed a pair of square microstrip patches. This system provides hori7.on~sl and vertical polarizations 30 independently and is said to minimi7.e the coupling between the feed ports, but again, size is a problem. To isolate the patches and make room for the two feed nelwolhs, the structure must be 0.95 wavelenth long.
- 5 - ~ 3 ~ ~i Polarization diversity has been studied by a number of engineers, for e~mple:
Bergman and Arnold as described in 'Polarization Diversity in Portable Communication~ Environment,"Electronic~ Letters, Vol 22, No. 11, 1986;
and W.C.Y. Lee reference previously. The results of these studies conclude that 5 polarization diversity ~ntenn~ offer subshnti~l signal strength i~ rovement over conventional antenn~e in most outdoor en-vilo..ments and in indoor systems where there is no direct line of sight between the fixed base station and the portable CO.. -.f icator. When there is a line of sight, diversity ant~nn~
perform only slightly better than a conventional monopole ~ntenn~ This is 10 because only one polarization of the received signal (usually vertical) is domin~nt. In this case, however, the signal level is usually high and the multipath fading effects are not as severe.
Pattern diversity (or angle diversity) makes use of the observation that most ofthe components of a signal all;villg from different paths also have different 15 angles of arrival. In most mobile envilo.-ment~, the signal components from different angles of arrival will have fading patterns that are statistically independent. Therefore, Lversi~y can be achieved if directional ~ntenn~ are used to isolate these signal components. Research on pattern diversity shows that it offers an improvement in received signal strength over conventional 20 antenna reception, particularly in ellviro~lm~nte where .sign~ are arriving from many different angles. The directivities of the ~nt~nn~.~ must be chosen carefully, however; using highly directional antennas gives good statistical independence but less signal coverage area while using ant~nn~.~ with low directivity gives a broad signal coverage area at the expense of poorer statistical 25 independence.
Summary of Invention The invention herein is directed to a comp~ct, polarization pattern diversity antenna that is (le~igned with hand held cellular telephones in mind. This diversity system is capable of separately and simultaneously receiving both 30 orthogonal polarizations (vertical and horizontal) of an incoming signal and~or components of a signal with different angles of arrival. Whether polarization -6- 2~5~4 diversity or pattern diversity is the main s~hçme in use depends on the orientation of the antenna with respect to the incQming .signs~l.c.
The invention herein employs a pair of conductive patches that are either implanted inside or layered on top of a dielectric material. The patches are 5 rectangular in the preferred embodiment and separated by a narrow gap that resonates like a slot antenna, providing one of the two re.son~nt modes. The other mode is provided by a second slot ~ntçnn~ formed between the two patches and a conductive ground plane affixed beneath the dielectric.
The rlimen.cions of the patches and how and where they are terminated are 10 crucial to the operation of the divel~ily antenna. The back edges of both patches connect to the ground plane, creating a short circuit. This forces an open circuit along the front edges that are a quarter wavelength away at the resonant frequency. The two feed points are located near these front edges, on both sidesof the gap between the two patches. When they are fed with .cign~ of equal 15 ~mplitude and opposite phase, currents form near the gap. These currents giverise to an electrom~gnetic field that radiates across the gap. The polarization of the field is in the direction orthogonal to that of the gap (hereafter referred to as the vertical polarization). When fed by .cign~l.c of equal amplitude and equal phase, the feed points excite currents in the patch that, because of the open 20 circuit condition, can only flow along the front edges of the two patches. Hence, an electric potential is eshhli.ched between these front edges and the ground plane resulting in an electromagnetic field that radiates from the structure with a polarization perpendicular to a line between the feed points (hereafter calledthe horizontal polarization).
25 The dielectric material is not es.s~nti~l to the operation of the antenna, but it provides mech~nical stability and decreases the physical size. Materials with larger dielectric con~t~nts will decrease the size even further, but at the ç~rpen.ce of concentrating the electrom~gnetic fields inside the material and thus preventing some radiation.
30 Using the dielectric material also allows the use of printed circuit technology in its fabrication, which has many advantages. The manufacturing process is inexpensive and accurate, m~king it readily ~men~hle to mass production. Also, 7 2Q~3~4 this technology is compatible with integrated circuits, which can be mounted directly on the board, and feed lines and matching nelwo~hs can be fabricated onthe same dielectric. The light weight, compact size and planar geometry of the dielectric make it easy to use where small size is important or conformity with a 5 structure is required. Microstrip antennas like this one are also rugged enough to withstand climatic changes and are essentially maint~n~nce free.
Variations to the basic invention include embodiments where modifications have been made to any part of the antenna in order to change the physical or electrical properties without ~h~n~ing the basic operation of the ~nt~nn~ Such 10 modifications include but are not limited to cutting slots and~or holes of any shape into any of the conductive surfaces, carving wells into the dielectric, th:3nging the positions of the feed points, tapering any of the conductive surfaces, tapering the dielectric, using dielectrics with non-homo~eneous permittivities, curving or bending parts of or all of the embodiment, inserting 15 grounding posts, adding matching circuits, filters or rectifiers, removing the dielectric, enclosing one or more surfaces of the embodiment with dielectric material, and using physical designs other than printed circuit te-hnology.
Objects of In~e.ltion The objects of the present invention are to provide an antenna that:
20 1. is easy to manufacture;
2. has a compact and planar shape so that it can conform to the shape of a vehicle or fit inside a portable telephone or other co.-~n~..icator;
3. receives or transmits two components of a signal separately and simultaneously. These two components are received using polarization diversity 25 and/or pattern diversity. The motivation for this property is to reduce the multipath fading effects in mobile collln~ cations at high frequencies, but thisproperty can also be used for other applications and in other systems;
4. minimi7.eS the r.f. coupling between the two modes of operation so as to provide high radiation efficiency and high isolation between overall input/oul~ul 30 ports for the different polarizations;
5. radiates each desired polarization nearly omnidirect~o~lly in one plane of the antenna.
Brief Description of the Drawings The above and further objects and advantages of the invention will be better understood by referring to the foliowing description in conjunction with the accompanying drawings, in which:
FIG. 1 is a perspective view of a polarization/pattern diversity antenna constructed in acccordance with the invention.
FIG. 2 is a cross-sectional view of the antenna shown in FIG. 1 taken along cutting line A-A'.
FIG. 3 is a perspective view of the diversity antenna of FIG. 1 connected via matching circuits to a hybrid circuit, which may be used to separate the two components of the received signal.
FIG. 4 is a plan view of the back wall of the invention.
FIG. 5a is a graph of horizontal mode antenna radiation measurements of the vertical polarization in the YZ-plane of Figure 1.
FIG. 5b is a graph of horizontal mode antenna radiation measurements of the horizontal polarization in the YZ-plane of Figure 1.
FIG. 5c is a graph of vertical mode antenna radiation measurements of the vertical polarization in the YZ-plane of Figure 1.
FIG. 5d is a graph of vertical mode antenna radiation measurements of the horizontal polarization in the YZ-plane of Figure 1.
FIG. 6 is a perspective view of an alternate embodiment of a polarization/pattern diversity antenna constructed in accordance with the invention.
Description of Preferred Embodiment.
Referring now to Fig. 1 which depicts a perspective view of the invention, a polarization/pattern diversity antenna 1. The antenna 1 comprises a dielectric layer 2 which supports a pair of similar conductive patches 3 on one side and a continuous conductive layer 4 on the other, which serves as a ground plane. The patches 3 and the ground plane 3 o 4 are connected along the back by a conductive wall 5. This wall short circuits the back edge of each patch 3 to the ground plane 4 so that they have zero voltage potential there.
The length a of the patches 3 is one quarter of a wavelength at the resonant frequency. From simple transmission line calculations, that makes the impedance equal to that of an open circuit along the front 5edges of the patches 3. Because of the dielectric layer 2, a wavelength is smaller than a free space wavelength by a factor equal to the inverse of the square root of the material's effective dielectric constant.
Therefore, the dielectric layer 2 not only provides mechanical stability and durability but also makes the antenna more compact.
10The width b of the patches 3 is not critical. It can be widened or narrowed to change the bandwidths or impedance matches.
Accordingly, the total width c of the antenna 1 is also adjustable. Care should be taken to make the total width c and total length d of the antenna 1 as small as possible in an effort to make the structure as 15compact as possible without jeopardizing its operation. The size of the ground plane 4 (which does not have to be the same size of the antenna 1 as shown) is of particular importance. The smaller a ground plane is, the more it will lose its ideal properties and therefore the more the operation of the antenna 1 will be hampered.
20The two feed points 6 of the antenna 1 are each located on its respective patch 3 near the front edge of the patch 3 and ciose to the line of symmetry B-B'. The positions of the feed points 6 are adjustable, however, they can be moved towards the back or to the outside to change the input impedances or any other parameter.
25As stated earlier, the two modes of the antenna 1 are provided by exciting the feed points 6 in phase or 180~ out of phase. When they are excited in phase, an electric field is created across a slot between the front edge of each patch 3 and the ground plane 4. Both sides of the gap between the patches 3 are at the same potential so an electric field 30cannot exist across it. There is therefore little coupling between the electric field from the patches 3 to the ground plane 4 and the electric - lo - ~Oq530~
field across the gap.
When the feed points 6 are excited out of phase, the potential across the gap creates an electric field whose polarization is orthogonal to the electric field between the patch 3 and ground 4. The electric potential on one side of the gap is different from ground and therefore an electric field can be created between that side and the ground plane 4, but because an equal and opposite potential exists on the other side of the gap, the two fields cancel each other out. Therefore, the antenna 1 has inherent isolation between its two modes of operation.
0 A cross-sectional view of the antenna 1 through the xy plane containing A-A' is given in Fig. 2. In the preferred embodiment the feed points 6 are connected to feed connectors 7a and 7b via feed posts 8 through the dielectric material 2 and the ground plane 4. In this particular embodiment, the feed connectors 7a and 7b may be screwed or soldered onto the ground plane 4. In a minor variation to this embodiment, matching circuits, filters or other circuits are connected between the feed posts 8 and the feed connectors 7a and 7b. It is not necessary that the antenna 1 is fed through the dielectric 2 and the ground plane 4. The antenna 1 could be fed from the top. However, the former method is preferred as the feed connectors 7a and 7b and any connecting circuits are out of the way of the radiating fields. Referring to Fig. 3, there is illustrated in a perspective view, the diversity antenna of Fig. 1 connected via matching circuits to a hybrid circuit.
To separate the two components of the received signal (which 2 5 will have different polarizations and/or different angles of arrival, depending on the orientation of the antenna), a hybrid circuit may be used. This hybrid circuit splits and then combines the signals form the feed connectors 7a and 7b with different phases to create the two components out the left hand side.
Fig. 4 is a view of the back wall 5 of the antenna 1. In the main embodiment, the wall 5 is a continuous conductive surface, although it - 11 - 20q5304 could just as easily be a series of conductive posts or a conductive mesh (this also applies to the ground plane 4 and the conductive patches 3).
The dotted line 9 illustrates one method of reducing the resonant frequencies without increasing the length a of the patches 3. By cutting out the area bordered by the dotted line 9, the gap between the two patches 3 is lengthened by an amount f, or, put another way, the length a is now reduced by an amount f.
The height e of the dielectric layer 2 is variable. Thicker dielectrics will increase the bandwidth of the horizontally-polarized signal 0 and may reduce the length a of the patches 3 (if the method just described is used) but will make the antenna bulky in the y direction.
Measured radiation patterns of one version of the invention are given for the horizontal (yz) plane in Fig. 5. This is the plane where polarization diversity exists. Figs. 5a and 5b show the vertically-polarized and horizontally-polarized radiation, respectively, when the antenna is in horizontal mode. The horizontal polarization is strong and nearly omnidirectional while the vertical polarization is much weaker. On average, the horizontal polarization is 23.6 dB stronger than the vertical.
A similar situation is found when the antenna is in vertical mode (as shown in Figs. 5c and 5d). The vertical polarization is strong and fairly close to omnidirectional in the horizontal (yz) plane while the horizontal polarization is 19.9 dB weaker on average.
In the xy and xz planes, this version of the invention exhibits pattern diversity.
Referring to FIG. 6, there is shown an alternate embodiment of a polarization/pattern diversity antenna, generally indicated by the reference numeral 1 1. This embodiment has a structure that is identical to that of antenna 1 of the previous embodiment, except that the dielectric layer 2 has been removed, leaving only air 12 to serve as a 3 o dielectric. Additionally, the elements of this embodiment are dimensioned on a larger scale than the corresponding elements of the previous embodiment. Specifically, and except as to scale, conductive patches 13, a continuous conductive layer 14, a conductive wall 15 and feed points 16, of this embodiment are configured in an identical manner to the conductive patches 3, the continuous conductive layer 4, the conductive wall 5 and the feed points 16 of the previous embodiment, respectively.
As was mentioned above, use of a dielectric layer results in a wavelength that is smaller than a free space wavelength by a factor equal to the inverse of the square root of the material's effective 0 dielectric constant. Use, in this embodiment, of air, only as the dielectric, therefore results in a larger wavelength, and the need for a correspondingly larger antenna 11.
The functionality of the antenna 11, of this embodiment, is identical to the functionality of the antenna 1 of the previous embodiment.
FIG. 1 is a perspective view of a polarization/pattern diversity antenna constructed in acccordance with the invention.
FIG. 2 is a cross-sectional view of the antenna shown in FIG. 1 taken along cutting line A-A'.
FIG. 3 is a perspective view of the diversity antenna of FIG. 1 connected via matching circuits to a hybrid circuit, which may be used to separate the two components of the received signal.
FIG. 4 is a plan view of the back wall of the invention.
FIG. 5a is a graph of horizontal mode antenna radiation measurements of the vertical polarization in the YZ-plane of Figure 1.
FIG. 5b is a graph of horizontal mode antenna radiation measurements of the horizontal polarization in the YZ-plane of Figure 1.
FIG. 5c is a graph of vertical mode antenna radiation measurements of the vertical polarization in the YZ-plane of Figure 1.
FIG. 5d is a graph of vertical mode antenna radiation measurements of the horizontal polarization in the YZ-plane of Figure 1.
FIG. 6 is a perspective view of an alternate embodiment of a polarization/pattern diversity antenna constructed in accordance with the invention.
Description of Preferred Embodiment.
Referring now to Fig. 1 which depicts a perspective view of the invention, a polarization/pattern diversity antenna 1. The antenna 1 comprises a dielectric layer 2 which supports a pair of similar conductive patches 3 on one side and a continuous conductive layer 4 on the other, which serves as a ground plane. The patches 3 and the ground plane 3 o 4 are connected along the back by a conductive wall 5. This wall short circuits the back edge of each patch 3 to the ground plane 4 so that they have zero voltage potential there.
The length a of the patches 3 is one quarter of a wavelength at the resonant frequency. From simple transmission line calculations, that makes the impedance equal to that of an open circuit along the front 5edges of the patches 3. Because of the dielectric layer 2, a wavelength is smaller than a free space wavelength by a factor equal to the inverse of the square root of the material's effective dielectric constant.
Therefore, the dielectric layer 2 not only provides mechanical stability and durability but also makes the antenna more compact.
10The width b of the patches 3 is not critical. It can be widened or narrowed to change the bandwidths or impedance matches.
Accordingly, the total width c of the antenna 1 is also adjustable. Care should be taken to make the total width c and total length d of the antenna 1 as small as possible in an effort to make the structure as 15compact as possible without jeopardizing its operation. The size of the ground plane 4 (which does not have to be the same size of the antenna 1 as shown) is of particular importance. The smaller a ground plane is, the more it will lose its ideal properties and therefore the more the operation of the antenna 1 will be hampered.
20The two feed points 6 of the antenna 1 are each located on its respective patch 3 near the front edge of the patch 3 and ciose to the line of symmetry B-B'. The positions of the feed points 6 are adjustable, however, they can be moved towards the back or to the outside to change the input impedances or any other parameter.
25As stated earlier, the two modes of the antenna 1 are provided by exciting the feed points 6 in phase or 180~ out of phase. When they are excited in phase, an electric field is created across a slot between the front edge of each patch 3 and the ground plane 4. Both sides of the gap between the patches 3 are at the same potential so an electric field 30cannot exist across it. There is therefore little coupling between the electric field from the patches 3 to the ground plane 4 and the electric - lo - ~Oq530~
field across the gap.
When the feed points 6 are excited out of phase, the potential across the gap creates an electric field whose polarization is orthogonal to the electric field between the patch 3 and ground 4. The electric potential on one side of the gap is different from ground and therefore an electric field can be created between that side and the ground plane 4, but because an equal and opposite potential exists on the other side of the gap, the two fields cancel each other out. Therefore, the antenna 1 has inherent isolation between its two modes of operation.
0 A cross-sectional view of the antenna 1 through the xy plane containing A-A' is given in Fig. 2. In the preferred embodiment the feed points 6 are connected to feed connectors 7a and 7b via feed posts 8 through the dielectric material 2 and the ground plane 4. In this particular embodiment, the feed connectors 7a and 7b may be screwed or soldered onto the ground plane 4. In a minor variation to this embodiment, matching circuits, filters or other circuits are connected between the feed posts 8 and the feed connectors 7a and 7b. It is not necessary that the antenna 1 is fed through the dielectric 2 and the ground plane 4. The antenna 1 could be fed from the top. However, the former method is preferred as the feed connectors 7a and 7b and any connecting circuits are out of the way of the radiating fields. Referring to Fig. 3, there is illustrated in a perspective view, the diversity antenna of Fig. 1 connected via matching circuits to a hybrid circuit.
To separate the two components of the received signal (which 2 5 will have different polarizations and/or different angles of arrival, depending on the orientation of the antenna), a hybrid circuit may be used. This hybrid circuit splits and then combines the signals form the feed connectors 7a and 7b with different phases to create the two components out the left hand side.
Fig. 4 is a view of the back wall 5 of the antenna 1. In the main embodiment, the wall 5 is a continuous conductive surface, although it - 11 - 20q5304 could just as easily be a series of conductive posts or a conductive mesh (this also applies to the ground plane 4 and the conductive patches 3).
The dotted line 9 illustrates one method of reducing the resonant frequencies without increasing the length a of the patches 3. By cutting out the area bordered by the dotted line 9, the gap between the two patches 3 is lengthened by an amount f, or, put another way, the length a is now reduced by an amount f.
The height e of the dielectric layer 2 is variable. Thicker dielectrics will increase the bandwidth of the horizontally-polarized signal 0 and may reduce the length a of the patches 3 (if the method just described is used) but will make the antenna bulky in the y direction.
Measured radiation patterns of one version of the invention are given for the horizontal (yz) plane in Fig. 5. This is the plane where polarization diversity exists. Figs. 5a and 5b show the vertically-polarized and horizontally-polarized radiation, respectively, when the antenna is in horizontal mode. The horizontal polarization is strong and nearly omnidirectional while the vertical polarization is much weaker. On average, the horizontal polarization is 23.6 dB stronger than the vertical.
A similar situation is found when the antenna is in vertical mode (as shown in Figs. 5c and 5d). The vertical polarization is strong and fairly close to omnidirectional in the horizontal (yz) plane while the horizontal polarization is 19.9 dB weaker on average.
In the xy and xz planes, this version of the invention exhibits pattern diversity.
Referring to FIG. 6, there is shown an alternate embodiment of a polarization/pattern diversity antenna, generally indicated by the reference numeral 1 1. This embodiment has a structure that is identical to that of antenna 1 of the previous embodiment, except that the dielectric layer 2 has been removed, leaving only air 12 to serve as a 3 o dielectric. Additionally, the elements of this embodiment are dimensioned on a larger scale than the corresponding elements of the previous embodiment. Specifically, and except as to scale, conductive patches 13, a continuous conductive layer 14, a conductive wall 15 and feed points 16, of this embodiment are configured in an identical manner to the conductive patches 3, the continuous conductive layer 4, the conductive wall 5 and the feed points 16 of the previous embodiment, respectively.
As was mentioned above, use of a dielectric layer results in a wavelength that is smaller than a free space wavelength by a factor equal to the inverse of the square root of the material's effective 0 dielectric constant. Use, in this embodiment, of air, only as the dielectric, therefore results in a larger wavelength, and the need for a correspondingly larger antenna 11.
The functionality of the antenna 11, of this embodiment, is identical to the functionality of the antenna 1 of the previous embodiment.
Claims (11)
1. A polarization/pattern diversity antenna capable of simultaneously receiving or transmitting two different components of electromagnetic energy, said diversity antenna comprising:
a dielectric layer having an edge and first and second faces;
a pair or rectangular conductive patches, each having a length of one quarter of a wave length and a predetermined width, disposed on the first face in spaced relation defining a gap therebetween;
a ground plane disposed on the second face;
a conductive wall disposed on the edge and connecting the pair of rectangular conductive patches to the ground plane; and two feed points, each one positioned on a respective conductive patch remote from the conductive wall and adjacent the gap.
a dielectric layer having an edge and first and second faces;
a pair or rectangular conductive patches, each having a length of one quarter of a wave length and a predetermined width, disposed on the first face in spaced relation defining a gap therebetween;
a ground plane disposed on the second face;
a conductive wall disposed on the edge and connecting the pair of rectangular conductive patches to the ground plane; and two feed points, each one positioned on a respective conductive patch remote from the conductive wall and adjacent the gap.
2. The polarization/pattern diversity antenna of claim 1 wherein the feed points are connected to feed connectors through the dielectric layer and the ground plane.
3. The polarization/pattern diversity antenna of claim 1 wherein the feed points are connected to feed connectors on top of the antenna.
4. The polarization/pattern diversity antenna of claim 2 or 3 wherein matching circuits are placed between the feed points and the feed connectors.
5. The polarization/pattern diversity antenna of claim 4 wherein the feed connectors are connected to a hybrid circuit to achieve the in phase and 180~ out of phase signaling.
6. The polarization/pattern diversity antenna of claim 5 wherein the feed points are moved from their respective positions near the front inside corners of said conductive patch in such a way that does not change the basic operation of the antenna.
7. The polarization/pattern diversity antenna of claim 6 wherein the dielectric layer has a non-homogeneous permittivity.
8. The polarization/pattern diversity antenna of claim 7 wherein dielectric material surrounds at least one surfaces of the antenna.
9. The polarization/pattern diversity antenna of claim 8 wherein posts are inserted between the patches and the ground plane.
10. The polarization/pattern diversity antenna of claim 9 wherein the antenna comprises be printed circuit technology.
11. The polarization/pattern diversity antenna of claim 6 wherein the dielectric layer is air.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CA 2095304 CA2095304C (en) | 1993-04-30 | 1993-04-30 | Polarization pattern diversity antenna |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CA 2095304 CA2095304C (en) | 1993-04-30 | 1993-04-30 | Polarization pattern diversity antenna |
Publications (2)
Publication Number | Publication Date |
---|---|
CA2095304A1 CA2095304A1 (en) | 1994-10-31 |
CA2095304C true CA2095304C (en) | 1998-06-23 |
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Family Applications (1)
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CA 2095304 Expired - Fee Related CA2095304C (en) | 1993-04-30 | 1993-04-30 | Polarization pattern diversity antenna |
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CA (1) | CA2095304C (en) |
Families Citing this family (4)
Publication number | Priority date | Publication date | Assignee | Title |
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EP0997978B1 (en) * | 1998-10-27 | 2002-07-24 | Robert Bosch Gmbh | Radiation patterns for mobile phone |
JP2001111353A (en) | 1999-10-13 | 2001-04-20 | Mitsubishi Electric Corp | Mixer circuit |
US6920315B1 (en) | 2000-03-22 | 2005-07-19 | Ericsson Inc. | Multiple antenna impedance optimization |
EP3105817A1 (en) * | 2014-02-14 | 2016-12-21 | Nokia Solutions and Networks Oy | Antenna arrangement for orthogonally polarized omnidirectional transmission |
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1993
- 1993-04-30 CA CA 2095304 patent/CA2095304C/en not_active Expired - Fee Related
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