The present invention relates to a microwave resonator. More particularly, but not exclusively, the present invention relates to a microwave resonator comprising a hollow tube defined by an electrically conductive tube wall, the tube being closed at both ends by closing plates and a plurality of dielectric spaced apart resonant pucks arranged in the tube, each puck being dimensioned to resonate in a doubly degenerate dominant mode, each puck comprising a symmetry breaking structure for modifying the frequency of one of the degenerate modes relative to the other and the coupling between the two modes. The present invention also relates to a microwave filter comprising a plurality of such microwave resonators. The present invention also relates to a microwave multiplexer comprising a plurality of such resonators.
Microwave resonators are common components in microwave devices such as microwave filters and multiplexers. Such microwave resonators must typically meet a number of requirements. Preferably they are small to minimise the size of the microwave device. They should have a high Q factor and should also generate low passive intermodulation products. Preferably they should be able to operate when receiving a high-power signal. They should also be simple and inexpensive to manufacture.
EP0742603 discloses a multimode resonator for a microwave filter. The resonator comprises a cavity and a dielectric resonator element disposed inside the cavity. Whilst in some embodiments the dielectric resonator element abuts the cavity at a plurality of spaced apart points there is a substantial air gap between the dielectric resonator element and the cavity which extends from one end of the dielectric resonator element to the other. As a result of this the resonator is large.
The present invention seeks to overcome the problems of the prior art.
Accordingly, in a first aspect, the present invention provides a microwave resonator comprising
a hollow tube comprising an electrically conductive tube wall which defines a tube bore, the tube extending along a length axis from a first end to a second end;
a first electrically conductive closing plate closing the first end of the tube;
a second electrically conductive closing plate closing the second end of the tube;
a plurality of dielectric resonant pucks, each puck comprising first and second end faces and a side wall extending therebetween, each puck being dimensioned such that its dominant mode is a doubly degenerate mode;
the pucks being arranged within the tube bore spaced apart from each other and the closing plates, each puck being arranged with its end faces normal to the length axis and centered on the length axis and its side wall abutting the tube wall such that there is no air gap between the puck and tube wall which extends from one end face to the other of the puck, the puck adjacent to the first closing plate being termed the input puck;
each puck being separated from the adjacent puck in the tube bore by a coupling gap, each coupling gap having an electrically conductive iris plate arranged therein, each iris plate being arranged normal to the length axis, each iris plate comprising at least one coupling slot extending therethrough;
an input microwave coupler adapted to receive a microwave signal and provide it to the input puck;
each puck comprising a symmetry breaking structure for modifying the frequency of one of the degenerate modes relative to the other and the coupling between the two modes.
The microwave resonator according to the invention is highly compact. It has a high Q and also produces low passive intermodulation products. It can receive a high power microwave signal. It is also simple to manufacture. In particular the lack of an air gap between the pucks and the tube wall changes the resonant behaviour of the pucks enabling a significant reduction in size without loss of performance.
Further, the microwave resonator according to the invention is highly flexible. By simple modification of the symmetry breaking structure to change the relative frequencies and coupling between modes one can significantly alter the behaviour of the resonator.
Preferably the pucks are all of the same thickness from one end face to the other.
Preferably each of the pucks is dimensioned such that the dominant mode is a doubly degenerate H111 mode.
Preferably the end faces of each puck are circular.
Preferably the pucks are equally spaced apart.
Preferably the separation between the first closing plate and the input puck is between 0.25 and 0.75 times the thickness of the input puck, more preferably between 0.4 and 0.6 times the thickness of the input puck.
Preferably the sidewall of each puck is coated with an electrically conductive layer, the electrically conductive layer forming a portion of the tube wall.
Preferably a portion of each iris plate forms a portion of the tube wall.
Preferably each iris plate comprises a single coupling slot.
Alternatively, each iris plate comprises two coupling slots, one normal to the other.
Preferably the microwave resonator comprises two pucks only, the two pucks having an iris plate arranged therebetween.
Preferably the face of the input puck adjacent to the first closing plate is termed the input face, the input microwave coupler comprising an electrically conductive coupling strip arranged on the input face.
Preferably the coupling strip is inclined to the at least one coupling slot.
Alternatively, the input microwave coupler comprises
Alternatively, the input microwave coupler comprises an electrically conductive iris plate arranged in the tube bore substantially normal to the length axis between the input puck and first closing plate, the iris plate having an aperture therein, and a central resonator body extending from the iris plate towards the first closing plate.
Preferably the puck adjacent to the second closing plate is termed the output puck, the microwave resonator further comprising an output microwave coupler adapted to receive a microwave signal from the output puck.
Preferably the face of the output puck adjacent to the second closing face is termed the output face, the output microwave coupler comprising an electrically conductive strip arranged on the output face.
Alternatively, the output microwave coupler comprises
Alternatively, the output microwave coupler comprises an electrically conductive iris plate arranged in the tube bore substantially normal to the length axis between the output puck and the second closing plate, the iris plate having an aperture therein, and a central resonator body extending from the iris plate towards the second closing plate.
Preferably the symmetry breaking structure of at least one puck comprises a first electrically conductive adjustment strip arranged on a face of the puck, the adjustment strip extending along a first adjustment strip axis passing through the center of the puck.
Preferably the symmetry breaking structure further comprises a second electrically conductive adjustment strip arranged on the same face of the puck as the first, the second electrically conductive adjustment strip extending along a second adjustment strip axis passing through the center of the puck.
Preferably the first and second adjustment strip axes meet at an angle of 25 and 65 degrees, more preferably between 40 and 50 degrees, more preferably between 43 and 47 degrees, more preferably 45 degrees.
Preferably each adjustment strip extends from the tube wall towards the center of the puck face.
Alternatively, each adjustment strip extends from a point proximate to but spaced apart from the tube wall towards the center of the puck face.
Preferably the symmetry breaking structure of at least one puck comprises at least one, preferably a plurality of apertures extending through the puck from one end face to the other parallel to but spaced apart from the length axis.
Preferably for a plurality of pucks, preferably each puck the symmetry breaking structure comprises at least one, preferably a plurality of apertures extending through the puck from one end face to the other parallel to but spaced apart from the length axis.
Preferably for at least one puck the at least one aperture is of a different diameter or different distance from the length axis to the apertures of the remaining pucks.
Preferably for at least one puck the symmetry breaking structure comprises a further aperture extending along the length axis from one face to the other.
Preferably the symmetry breaking structure of at least one puck comprises at least one sot in the puck arranged in a plane normal to the length axis and part way between the first and second end faces of the puck.
Preferably the slot is arranged mid-way between the first and second end faces of the puck.
Preferably a plurality of pucks, preferably each puck, comprise such slots, the dimensions of the at least one slot of at least one puck being different to the dimensions of the slots of the remaining pucks.
Preferably the symmetry breaking structure of at least one puck comprises at least one aperture extending from the side wall of the puck into the puck normal to the length axis.
Preferably the at least one aperture is arranged mid way between the end faces of the puck.
Preferably a plurality of pucks, preferably each puck comprises at least one such aperture, the diameter of the aperture of at least one puck being different to those of the remaining pucks.
In a further aspect, the present invention provides a microwave filter comprising a plurality of microwave resonators as claimed in any one of claims 1 to 34
In a further aspect, the present invention provides a microwave multiplexer comprising a plurality of microwave resonators as claimed in any one of claims 1 to 34
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—
Shown in
The microwave resonator 1 comprises a hollow tube 2. The tube 2 comprises an electrically conductive tube wall 3 which defines a tube bore 4. The tube bore 4 extends along a length axis 5 from a first end 6 of the tube 2 to the second end 7 of the tube 2. The tube bore 4 of this embodiment of the invention is circular normal to the length axis 5.
A first electrically conductive closing plate 8 closes the first end 6 of the tube 2. A second electrically conductive closing plate 9 closes the second end 7 of the tube 2.
Arranged within the tube bore 4 are first and second dielectric resonant pucks 10,11. Each puck 10,11 comprises first and second end faces 12,13 and a side wall 14 extending therebetween. In this embodiment, the end faces 12,13 of each of the pucks 10,11 are circular. The diameter of each of the end faces 12,13 is equal to the diameter of the tube bore 4 such that the side wall 14 abuts the tube bore 4 over the entirety of the side wall 14 such that there is no air gap between the side wall 14 of the puck and the tube wall 3 which extends from one end face 12 of the puck 10,11 to the other end face 13. To put this another way if one were to look along the bore 4 of the tube one could not see past the puck 10,11 through a gap between the puck 10,11 and the tube wall 3. In practice the tube 2 is heated causing it to expand slightly. The pucks 10,11 are then inserted into the tube 2 and the tube 2 is then allowed to cool and contract so gripping the pucks 10,11 and holding them in place.
The puck 10 adjacent to the first closing plate 8 is termed the input puck. The face 12 of the input puck 10 adjacent to the first closing plate 8 is termed the input face. The puck 11 adjacent to the second closing plate 9 is termed the output puck. The face 13 of the output puck 11 adjacent to the second closing plate 9 is termed the output face,
Each puck 10 has a thickness measured along the length axis 5 from one end face 12 to the other end face 13. The separation between the first closing plate 8 and the input face 12 of the input puck 10 is typically between 0.25 and 0.75 times the thickness of the input puck 10, more preferably between 0.4 and 0.6 times the thickness of the input puck 10. In this embodiment, the separation between the first closing plate 8 and the input face 12 is 0.5 times the thickness of the input puck 10.
Similarly, the separation between the second closing plate 9 and the output face 13 of the output puck 11 is typically between 0.25 and 0.75 times the thickness of the output puck 11, more preferably between 0.4 and 0.6 times the thickness of the output puck 11. In this embodiment the separation between the second closing plate 9 and the output face 13 of th output puck 11 is 0.5 times the thickness of the output puck 11.
The dielectric of each puck 10,11 typically has a dielectric constant in the range 10 to 80. More typically the dielectric constant has any of the values 10, 20 40 and 80 to within ten percent. Higher dielectric constants are used in resonators operating at lower frequencies.
The two pucks are identical 10,11. Each puck 10,11 is dimensioned such that its dominant mode is a doubly degenerate mode, preferably the H111 mode.
The two pucks 10,11 are spaced apart by a coupling gap 15 extending therebetween. Arranged within the coupling gap 15 is an electrically conductive iris plate 16. The iris plate 16 in this embodiment is arranged equally spaced apart from the two pucks 10,11. The iris plate 16 is arranged normal to the length axis 5 as shown. The iris plate 16 is circular and has a diameter equal to that of the tube bore 4 such that the edge of the iris plate 16 abuts the tube bore 4 around the edge of the iris plate 16.
Shown in
As can be seen the iris plate 16 comprises two coupling slots 17, one normal to the other. The function of the iris plate 16 and the coupling slots 17 is explained in more detail below.
The microwave resonator 1 further comprises an input microwave coupler 18. The input microwave coupler 18 is adapted to receive an input microwave signal and provide it to the input puck 10. In this embodiment, the input microwave coupler 18 comprises an electrically conductive input coupling strip 19 arranged on the input face 12 of the input puck 10. The input coupling strip 19 is inclined to the coupling slots 17 as shown.
The microwave resonator 1 further comprises an output microwave coupler 20 which receives the microwave signal from the output puck 11. The output microwave coupler 20 comprises an electrically conductive output coupling strip 21 arranged on the output face 13 of the output puck 11. The output coupling strip 21 is inclined to the coupling slots 17.
Each puck 10,11 further comprises a symmetry breaking structure 22. The symmetry breaking structure 22 modifies the frequency of one of the modes relative to the other so that they are no longer degenerate. It also modifies the coupling between the two modes.
In this embodiment, each adjustment strip 23,24 extends from (and is electrically connected to) the tube wall 3 towards the center of the puck face 12. In alternative embodiments, the adjustment strips 23,24 extend from a point proximate to but spaced apart from the tube wall 3 towards the center of the puck face 12.
In use a microwave signal is provided to the input coupling strip 19. This signal couples to the two degenerate modes of the input puck 10. The microwave signal passes through the coupling slots 17 in the iris plate 16 and excites corresponding modes in the output puck 11. The two modes in the output puck 11 couple to the output coupling strip 21 so producing the output signal. The interaction between the two degenerate modes of the input puck 10 and the two degenerate modes of the output puck 11 results in the microwave resonator 1 having two transmissions zeros.
The operation of the microwave resonator 1 according to the invention can be explained in more detail with reference to the equivalent circuit shown in
Returning to
The action of the symmetry breaking structure 22 is more complex. The position of the first and second adjustment strips 23,24 is set relative to the coupling slots 17 of the iris plate 16. One can rotate the first and second adjustment strips 23,24 on the puck face 12 about the center of the puck 10 without altering the behaviour of the microwave resonator 1 provided one makes an appropriate corrective change to the relative lengths of the first and second adjustment strips 23,24. If one holds the position of the adjustment strips 23,24 constant and changes their relative lengths, or rotates the strips 23,24 and makes a change other than the appropriate change (or no change at all), one changes the coupling between the two modes in the puck 10,11 and also their relative frequencies M11 and M22. It is possible that in some embodiments of the invention the required length of one of the adjustment strips 23,24 is zero in which case the symmetry breaking structure 22 comprises only one adjustment strip 23,24.
One can analyse the behaviour of the equivalent circuit of
Changes to the design of the microwave resonator 1 can significantly alter its behaviour. Shown in
Shown in
Alternative forms of symmetry breaking structure 22 are possible. Shown in
More typically the symmetry breaking structure 22 comprises two apertures 25. Shown in
Shown in
The operation of such a microwave resonator 1 is very similar to that previously described except there are a larger number of degrees of freedom which can be adjusted in the design stage. A typical behaviour of such a resonator 1 is shown in
Shown in
In order to ensure the correct spacing between the end faces 12,13 of the puck 10,11 and both the iris plate 16 and the closing plates 8,9 each puck 10,11 has a collar portion 29 which extends from each end face 12,13 of the puck 10,11 as shown. In practice the puck 10,11 is manufactured as a wide disk and then wide recesses formed in each end to form the collar 29. The puck 10,11 is then coated with the metal film 28.
The manufacture of this embodiment of the microwave resonator 1 is simpler than the manufacture of the embodiment of
In all of the above embodiments the input microwave coupler 18 comprises an electrically conductive coupling strip 19 arranged on the input face 12 of the input puck 10. In practice this can be difficult to achieve. If the coupling strip 19 is not connected to the input face 12 along its full length this can affect the behaviour of the microwave resonator 1.
Shown in
The central resonator body 30, finger 31 and adjacent iris plate 32 together form a combline resonator. A microwave signal provided to the central resonator body 30 along a wire generates a magnetic field within the combline resonator. This passes through the slot 33 in the iris plate 32 and excites the input puck 10.
The structure of the output microwave coupler 20 is the same as that of the input microwave coupler 18. The magnetic field generated by the output puck 11 passes through the slot 33 in the iris plate 32 into the combline resonator from where it can be extracted by a wire connected to the central resonator body 30.
The electrical response of such a microwave resonator 1 is shown in
Shown in
Shown in
The behaviour of the microwave resonator 1 of
It is desired to reduce this spurious response.
One approach is shown in
An alternative approach is to suppress the coupling between the orthogonal HE112 modes within the resonator 1. Shown in
The plane of each puck 10a,10b,11 mid-way between its end faces 12,13 is a low field region in the HE112 mode. The effect of the slots 38 on the HE112 modes of the resonator 1 is therefore reduced compared to the effect on the HE111 modes. The modes will still couple strongly from the outside but the bandwidth of the dual mode spurious resonances will be reduced which simplifies the separation of the HE112 modes from the multiple dual mode resonant pucks 10a,10b,11.
Shown in
Shown in
All of the microwave resonators 1 as previously described may be employed in larger structures. They may be employed in filters comprising a plurality of such resonators 1. The resonators 1 may be connected together in parallel or cascade. They may also be employed in multiplexers (the term being used broadly to cover both multiplexers and demultiplexers). A multiplexer would typically employ a plurality of such resonators 1.
Number | Date | Country | Kind |
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1702449 | Feb 2017 | GB | national |
1715171 | Sep 2017 | GB | national |
Filing Document | Filing Date | Country | Kind |
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PCT/GB2018/050390 | 2/13/2018 | WO | 00 |
Publishing Document | Publishing Date | Country | Kind |
---|---|---|---|
WO2018/150171 | 8/23/2018 | WO | A |
Number | Name | Date | Kind |
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5880650 | Latouche et al. | Mar 1999 | A |
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10224588 | Weiß | Mar 2019 | B2 |
20100013578 | Memarian et al. | Jan 2010 | A1 |
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20160322688 | Weiss | Nov 2016 | A1 |
Number | Date | Country |
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1276922 | Dec 2000 | CN |
104485497 | Apr 2015 | CN |
106252797 | Nov 2016 | CN |
0742603 | Nov 1996 | EP |
2561384 | Feb 2016 | ES |
2013085357 | Jun 2013 | WO |
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Number | Date | Country | |
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20190386365 A1 | Dec 2019 | US |