TRI-FREQUENCY MULTI-POLARISATION OMNIDIRECTIONAL ANTENNA

Abstract

A tri-frequency multi-polarisation omnidirectional antenna comprising: a first plurality of curved electrically conductive strips arranged on the first face and being arranged to form an outer-loop; second plurality of curved electrically conductive strips arranged on the first face and being arranged to form an inner-loop; third plurality of curved electrically conductive strips arranged on the first face and being arranged to form middle-loop; a first power divider and a second power divider each connected to the strips of the inner-loop; a dielectric resonator comprising a first face, the first face arranged on the first face of the substrate; an electrically conductive probe being arranged at least partially within the dielectric resonator and extending at least part way along the symmetry axis.

Claims

1. A tri-frequency multi-polarisation omnidirectional antenna comprising: an electrically insulating substrate comprising first and second faces; a first plurality of curved electrically conductive strips arranged on the first face and being arranged to form an outer loop with each strip being spaced apart from the adjacent strip of the loop; a second plurality of curved electrically conductive strips arranged on the first face and being arranged to form an inner loop with each strip being spaced apart from the adjacent strip of the loop; a third plurality of curved electrically conductive strips arranged on the first face and being arranged to form middle loop with each strip being spaced apart from the adjacent strip of the loop; the three loops being concentric with each loop centered on a common symmetry point, the axis normal to the first face and passing through the common symmetry point being the symmetry axis; the middle loop having a larger diameter than the inner loop and the outer loop having a larger diameter than the middle loop; a first power divider connected to the strips of the outer loop; a second power divider connected to the strips of the inner loop; a dielectric resonator comprising a first face, the first face arranged on the first face of the substrate; an electrically conductive probe being arranged at least partially within the dielectric resonator and extending at least part way along the symmetry axis.

2. A tri-frequency multi-polarisation omnidirectional antenna as claimed in claim 1, wherein the loops are circular.

3. A tri-frequency multi-polarisation omnidirectional antenna as claimed in claim 1, wherein the dielectric resonator is cylindrical and comprises first and second faces and a side wall extending therebetween, the resonator comprising a dielectric axis extending from the center of the first face to the center of the second face, the dielectric axis being coaxial with the symmetry axis.

4. A tri-frequency multi-polarisation omnidirectional antenna as claimed in claim 3, wherein the dielectric resonator comprises at least one step change in diameter part way along its length.

5. A tri-frequency multi-polarisation omnidirectional antenna as claimed in claim 1, wherein the dielectric resonator is dimensioned such that when excited by an microwave signal provided to it by the probe it excites vertically polarised TM modes in a lower band and an upper band, the lower band containing 2.4 GHz and the upper band containing 5.2 GHz and 5.8 GHz.

6. A tri-frequency multi-polarisation omnidirectional antenna as claimed in claim 1, wherein the dielectric resonator is glass.

7. A tri-frequency multi-polarisation omnidirectional antenna as claimed in claim 1 further comprising a probe signal source connected to the probe, the probe signal source being configured to provide a microwave signal at at least one of 2.4 GHz, 5.2 GHz and 5.8 GHz.

8. A tri-frequency multi-polarisation omnidirectional antenna as claimed in claim 1 wherein the loops are circular.

9. A tri-frequency multi-polarisation omnidirectional antenna as claimed in claim 1, wherein the middle loop is arranged proximate to the inner loop such that the two are electrically coupled together to form a composite electrical structure.

10. A tri-frequency multi-polarisation omnidirectional antenna as claimed in claim 9 wherein the strips of the composite electrical structure are dimensioned such that when excited by a microwave signal the composite electrical structure excites horizontally polarised TE modes in an upper frequency band, the upper frequency band containing 5.2 GHz and 5.8 GHz.

11. A tri-frequency multi-polarisation omnidirectional antenna as claimed in claim 1, further comprising a second signal source connected to the second power divider, the second signal source being configured to provide a microwave signal at at least one of 5.2 GHz and 5.8 GHz.

12. A tri-frequency multi-polarisation omnidirectional antenna as claimed in claim 1, wherein the strips of the outer loop are dimensioned such that when excited by a microwave signal the outer loop excites a horizontally polarised TE mode in a lower frequency band, the lower frequency band containing 2.4 GHz.

13. A tri-frequency multi-polarisation omnidirectional antenna as claimed in claim 1 further comprising a first signal source connected to the first power divider, the first signal source being configured to provide a microwave signal at 2.4 GHz.

14. A tri-frequency multi-polarisation omnidirectional antenna as claimed in claim 1 further comprising an electrically conductive ground plane on the second side of the substrate.

15. A tri-frequency multi-polarisation omnidirectional antenna as claimed in claim 14 further comprising a ring slot in the ground plane

16. A tri-frequency multi-polarisation omnidirectional antenna as claimed in claim 1 further comprising a recess in the first face of the dielectric resonator arranged about the symmetry axis.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0031] The present invention will now be described by way of example only and not in any limitative sense with reference to the accompanying drawings in which

[0032] FIG. 1 shows, in perspective view, a tri-frequency multi-polarisation omnidirectional antenna according to the invention.

[0033] FIG. 2 shows the first face of the electrically insulating substrate of the antenna of FIG. 1 in plain view from above;

[0034] FIG. 3 shows the tri-frequency multi-polarisation omnidirectional antenna of FIG. 1 in vertical cross section;

[0035] FIGS. 4(a) to 4(d) show simulated and measured parameters of an antenna according to the invention; and

[0036] FIGS. 5(a) to 5(f) show simulated and measured normalised radiation patterns from the antenna.

[0037] Shown in FIG. 1 is a tri-frequency multi-polarisation omnidirectional antenna 1 according to the invention. The tri-frequency multi-polarisation omnidirectional antenna 1 comprises an electrically insulating substrate 2 having first and second faces 3, 4. Arranged on the first face 3 is a plurality of loops 8, 12, 16 and power dividers 9, 13 which are described in more detail with reference to FIG. 2. Also arranged on the first face 3 is a dielectric resonator 20 having an electrically conductive probe 27 arranged therein. This is described in more detail with reference to FIG. 3.

[0038] Shown in FIG. 2 is the first face 3 of the electrically insulating substrate 2 in plain view. Arranged on the first face 3 is a first plurality of curved electrically conductive strips 7. The strips 7 are arranged to form an outer circular loop 8 with each strip 7 separated from each adjacent strip 7 of the loop 8 as shown. Connected to the strips 7 of the outer loop 8 is a first power divider 9. The first power divider 9 receives a microwave signal from a first port 10 and provides it to each of the curved strips 7. The curved strips 7 of the outer loop 8 are dimensioned such that when excited by a microwave signal from the first port 10 the outer loop 8 excites a horizontally polarised TE mode in a lower frequency band, the lower frequency band containing 2.4 GHz.

[0039] Also arranged on the first face 3 is a second plurality of curved electrically conductive strips 11. The strips 11 are arranged to form a circular inner loop 12 with each strip 11 separated from each adjacent strip 11 in the loop 12 as shown. Connected to the strips 11 of the inner loop 12 is a second power divider 13 which receives a microwave signal from a second port 14 and provides it to each of the curved strips 11.

[0040] Also arranged on the first face 3 is a third plurality of curved electrically conductive strips 15. The strips 15 are arranged to form a circular middle loop 16 with each strip 15 separated from each adjacent strip 15 in the loop 16 as shown.

[0041] The outer, inner and middle loops 8, 12, 16 are concentric with each loop 8, 12, 16 centered on a common symmetry point 17. The axis 18 passing through the common symmetry point 17 normal to the first face 3 of the substrate 2 is termed the symmetry axis 18.

[0042] The middle loop 16 has a larger diameter than the inner loop 12. The outer loop 8 has a larger diameter than the middle loop 16. The middle loop 16 is arranged proximate to the inner loop 12 such that the two are electrically coupled together to form a composite electrical structure 19. The effect of this is that the parasitic strips 15 of the middle loop 16 tune the modes of the inner loop 12.

[0043] The curved strips 11, 15 of the composite electrical structure 19 are dimensioned such that when excited by a microwave signal from the second port 14 the composite electrical structure 19 excites horizontally polarised TE modes in an upper frequency band, the upper frequency band containing 5.2 GHz and 5.8 GHz.

[0044] Shown in FIG. 3 is the tri-frequency multi-polarisation omnidirectional antenna 1 of FIG. 1 in vertical cross section. Arranged on the first face 3 is a cylindrical dielectric resonator 20. The dielectric resonator 20 is typically a glass. The dielectric resonator 20 comprises first and second faces 21, 22 and a side wall 23 extending therebetween. The dielectric resonator 20 has a dielectric axis 24 which extends from the middle of the first face 21 to the middle of the second face 22. The first face 21 of the dielectric resonator 20 is arranged on the first face 3 of the substrate 2 with the dielectric axis 24 coaxial with the symmetry axis 18 as shown. The dielectric resonator 20 has a step change in diameter part way along its length. Arranged in the first face 21 of the dielectric resonator 20 is a small recess 25 which reduces the cross polarised fields generated by the power dividers 9, 13.

[0045] An aperture 26 extends through the dielectric resonator 20 along the dielectric axis 24. Extending along the dielectric axis 24 is an electrically conductive probe 27 which is connected to a probe port 28 extending through the substrate 2 proximate to the dielectric axis 24. The dielectric resonator 20 is dimensioned such that when excited by a microwave signal provided by the probe 27 it excites vertically polarised TM modes in a lower band and an upper band, the lower band containing 2.4 GHz and the upper band containing 5.2 GHz and 5.8 GHz.

[0046] The probe port 28 is connected to a probe signal source 29. The probe signal source 29 is configured to provide a microwave signal at at least one of 2.4 GHz, 5.2 GHz and 5.8 GHz. Preferably the probe signal source 29 is configured to provide a microwave signal at all three frequencies. The first port 10 is connected to a first signal source 30. The first signal source 30 is configured to provide a microwave signal in a lower band at 2.4 GHz. The second port 14 is connected to a second signal source 31. The second signal source 31 is configured to provide a microwave signal in an upper band containing 5.2 GHz and 5.8 GHz. The antenna 1 further comprises a ring slot 32 etched in an electrically conductive ground plane 4a on the second side 4 of the substrate 2 for impedance matching of the probe port 28.

[0047] In use the probe signal source 29 provides a microwave signal to the probe 27. The probe 27 excites vertically polarised TM modes in the dielectric resonator 20 at one or more of 2.4 GHz, 5.2 GHz and 5.8 GHz. Simultaneously, the first signal source 30 provides a microwave signal to the strips 7 of the outer loop 8 which excites horizontally polarised TE modes in the strips 7 of the outer loop 8 at 2.4 GHz. In addition, the second signal source 31 provides a microwave signal to the strips 11 of the inner loop 12 which excites horizontally polarised TE modes in the composite electrical structure 19 of at least one of 5.2 GHz and 5.8 GHz. In use the antenna 1 according to the invention can therefore operate at all of 2.4 GHz, 5.2 GHz and 5.8 GHz in both TE and TM modes.

[0048] FIGS. 4(a) to 4(d) show the simulated and measured S-parameters, antenna gains, total efficiencies and envelope correlation coefficients for an antenna according to the invention. With reference to FIG. 4(a) the measured −10 dB impedance passbands for the probe port (28) are 2.2-2.7 GHz and 5.05-5.86 GHz. As for the first and second ports (10, 14) the measured passband is 2.38-2.5 GHz for the first port (10) and 4.9-5.27 GHz and 5.6-5.85 GHz for the second port (28). Overlapped bandwidths are 4.9% (2.38-2.5), 4.26% (5.05-5.27) and 4.36% (5.6-5.85) fully covering the three Wi-Fi bands. Among the three pairs of modes of orthogonal polarisations there are five dielectric resonator modes and one dielectric resonator loaded probe mode. Also, the port isolations are as high as 30 dB, 25 dB and 20 dB of the three bands. As shown in FIG. 4(b) the measured vertically polarised antenna gains at (φ=0 degrees, θ=sixty degrees) for the probe port (28) are 1, 0.3 and 1.3 dBi at the 2.4-, 5.2-, and 5.8-GHz bands respectively. The measured horizontally polarised gain at this direction is 3 dBi at 2.4 GHz band at the first port (10) whereas they are 2 and -0.75 dBi at the 5.2 and 5.8 GHz bands for the second port (14). The relatively low gain of the 5.8 GHz band is because the peak radiation direction is not at θ=sixty degrees, caused by the increased titled angle of radiation patterns. As can be seen from FIG. 4(c) the antenna total efficiencies of the probe port (28) are 93%, 77% and 72% at the three bands which takes impedance matching into account. As for the first and second ports (10, 14) the efficiencies of the three bands are 80%, 73% and 70%. The antenna efficiency of the 5 GHz band is generally lower than that of the 2.4 GHz band. This is expected as the loss caused by the glass increases with frequency. The envelope correlation coefficients (ECCs) of the antenna, which is a performance index for a MIMO antenna, are shown in FIG. 4(d). The simulated and measured ECCs were obtained from radiation patterns. Both the simulated and measured ECCs between different polarised ports are lower than −20, −28 and −18 dB for the 2.4-, 5.2- and 5.8 GHz bands respectively. Due to the orthogonal polarisation they are desirably much lower than the criteria of −3 dB.

[0049] FIGS. 5(a) to 5(f) show simulated and measured normalised radiation patterns at 2.44, 5.2 and 5.8 GHz. FIGS. 5(a) to 5(c) show the patterns for a signal provided to the probe port (28). FIG. 5(d) shows the pattern for a signal provided to the first port (10). FIGS. 5(e) and 5(f) show the radiation pattern for a signal provided to the second port (14). The solid lines show the simulated patterns. The dotted lines show the measured patterns.