The present invention relates to a dielectric waveguide resonator and a dielectric waveguide filter including the dielectric waveguide resonator.
Along with an increase in speed and capacity of mobile communication, the millimeter waveband is more frequently being used. As a filter used at, for example, a base station for mobile communication using the millimeter waveband, a dielectric waveguide filter is suitable.
As a dielectric waveguide filter used in the millimeter waveband or the like, for example, Japanese Unexamined Patent Application Publication No. 2018-125717 is disclosed. The dielectric waveguide filter includes a dielectric waveguide resonator in which a first conductor layer and a second conductor layer are respectively formed on a first surface and a second surface of a dielectric plate, the first surface and the second surface facing each other, and a post wall is formed using a large number of via conductors connecting the conductor layers at both the surfaces.
Japanese Unexamined Patent Application Publication No. 2018-125717 also shows that a resonant frequency of the dielectric waveguide resonator is adjusted by causing a blind via having a via conductor formed therein to protrude from the first surface in an inward direction and connecting the conductor layer and the via conductor by a metal wiring portion.
Generally, since a dielectric material which is low in dielectric loss can be used for a dielectric waveguide resonator and a conductor portion is basically composed of a conductor extending in a planar form, conductor loss can be kept low.
In the dielectric waveguide filter illustrated in Japanese Unexamined Patent Application Publication No. 2018-125717, however, since electric field strength between a distal end of the via conductor formed in the blind via inside the dielectric substrate and the conductor layer which the distal end faces is high and currents concentrate at a distal end portion of the via conductor, a relatively large resistance loss occurs in the portion with a high current density. That is, a dielectric waveguide resonator having a high Q factor is hard to obtain, which leads to the problem of the difficulty in obtaining a dielectric waveguide filter having a low insertion loss.
Preferred embodiments of the present invention provide dielectric waveguide resonators each including a structure for resonant frequency adjustment and having a high Q factor and a dielectric waveguide filter having a low insertion loss.
A dielectric waveguide resonator as an example of a preferred embodiment of the present disclosure includes a dielectric plate including a first principal surface and a second principal surface facing each other and a side surface connecting an outer edge of the first principal surface and an outer edge of the second principal surface, a first surface conductor at the first principal surface, a second surface conductor at the second principal surface, a connection conductor inside the dielectric plate and connecting the first surface conductor and the second surface conductor, and an internal conductor extending in a perpendicular direction to the first principal surface and electrically connected to neither the first surface conductor nor the second surface conductor. The dielectric waveguide resonator includes a dielectric waveguide resonant space which is surrounded by the first surface conductor, the second surface conductor, and the connection conductor.
According to the dielectric waveguide resonator with the above-described configuration, since the internal conductor is isolated from the first surface conductor and the second surface conductor, that is, the internal conductor is floating galvanically from potentials of the first surface conductor and the second surface conductor, the degree of concentration of currents at an end portion of the internal conductor is low. For this reason, a dielectric waveguide resonator including a resonant frequency adjustment structure and having a high Q factor is obtained.
Further, a dielectric waveguide filter as an example of a preferred embodiment of the present disclosure includes a dielectric waveguide resonator. The dielectric waveguide resonator includes a dielectric plate which includes a first principal surface and a second principal surface facing each other and a side surface connecting an outer edge of the first principal surface and an outer edge of the second principal surface, a first surface conductor at the first principal surface, a second surface conductor at the second principal surface, and a connection conductor inside the dielectric plate and connecting the first surface conductor and the second surface conductor. The dielectric waveguide filter further includes an internal conductor inside the dielectric waveguide resonator, extending in a perpendicular direction to the first principal surface, and electrically connected to neither the first surface conductor nor the second surface conductor.
Further, a dielectric waveguide filter as an example of a preferred embodiment of the present disclosure includes a plurality of dielectric waveguide resonators and a main coupling portion to couple adjacent dielectric waveguide resonators of the plurality of dielectric waveguide resonators. Each of the plurality of dielectric waveguide resonators includes a dielectric plate including a first principal surface and a second principal surface facing each other and a side surface connecting an outer edge of the first principal surface and an outer edge of the second principal surface, a first surface conductor at the first principal surface, a second surface conductor at the second principal surface, and a connection conductor inside the dielectric plate and connecting the first surface conductor and the second surface conductor. Each of one, some, or all of the plurality of dielectric waveguide resonators further includes a respective internal conductor inside the corresponding dielectric waveguide resonator, extends in a perpendicular direction to the first principal surface, and is electrically connected to neither the first surface conductor nor the second surface conductor.
The dielectric waveguide filters with the above-described configurations each include a dielectric waveguide resonator in which the degree of concentration of currents at an internal conductor is low and which has a high Q factor, as described above. Thus, a dielectric waveguide filter having a low insertion loss is obtained.
According to preferred embodiments of the present invention, dielectric waveguide resonators each including a structure for resonant frequency adjustment and having a high Q factor and a dielectric waveguide filter having a low insertion loss are provided.
The above and other elements, features, steps, characteristics and advantages of the present invention will become more apparent from the following detailed description of the preferred embodiments with reference to the attached drawings.
Hereinafter, preferred embodiments of the present invention will be illustrated with several specific examples with reference to the drawings. The same components are denoted by the same reference characters in the detailed description of the drawings. Although preferred embodiments are separately illustrated for convenience in view of description of points or ease of understanding, partial replacement or combination of configurations illustrated in different preferred embodiments is possible. In second and subsequent preferred embodiments, a description of matters in common with the first preferred embodiment will be omitted, and only differences will be described. In particular, the same operational effects by the same configurations will not be mentioned one by one in each preferred embodiment.
The dielectric waveguide filter 101 includes a dielectric plate 1. The dielectric plate 1 is obtained by processing, for example, dielectric ceramic, crystal, or resin into the shape of a rectangular parallelepiped. The dielectric plate 1 has a first principal surface MS1 and a second principal surface MS2 which face each other, and four side surfaces SS (
A first surface conductor 21 is provided at the first principal surface MS1 of the dielectric plate 1, and a second surface conductor 22 is provided at the second principal surface MS2 of the dielectric plate 1. Side conductor films 8A to 8D (8A, 8B, 8C, 8D) are provided at the side surfaces SS of the dielectric plate 1. The first surface conductor 21, the second surface conductor 22, and the side conductor films 8A to 8D are, for example, copper films which are formed by sputtering.
Internal conductors 7A to 7D (7A, 7B, 7C, 7D) which extend in a perpendicular direction to the first principal surface MS1 and are electrically connected to neither the first surface conductor 21 nor the second surface conductor 22 are provided inside the dielectric plate 1. Structures and functions of the internal conductors 7A to 7D will be described in detail later.
As shown in, for example,
As indicated in, for example,
The I/O electrodes 24A and 24B, the ground electrodes 23A to 23D, and the like are, for example, conductor patterns made of copper films. The through via conductors 2A to 2G and the via conductors 3A to 3V are, for example, conductors obtained by, for example, firing conductor paste.
As shown in
Hereinafter, a “dielectric waveguide resonator” will also be simply referred to as a “resonator”. The resonators R1, R2, R3, and R4 are all resonators which have the TE101 mode as dominant modes. That is, the TE101 mode is a resonant mode with an electromagnetic field distribution, in which the Z direction shown in
The internal conductors 7A to 7D shown in, for example,
With the local capacitances generated by the internal conductors 7A to 7D, resonant frequencies of the resonators R1, R2, R3, and R4 can be adjusted. Since capacitive components in the dielectric waveguide resonant spaces increase, a size of a dielectric waveguide resonator to achieve a predetermined resonant frequency can be reduced.
As shown in
The main coupling portion MC12 shown in
The main coupling portion MC23 shown in
The sub coupling portion SC14 shown in
Since the main coupling portion MC12 acts as an inductive coupling window which limits widths (widths in the X direction) orthogonal to the electric field direction of the resonators R1 and R2 by the presence of the through via conductor 2D, the resonators R1 and R2 are inductively coupled together. Since the main coupling portion MC34 acts as an inductive coupling window which limits widths (widths in the X direction) orthogonal to the electric field direction of the resonators R3 and R4 by the presence of the through via conductor 2G, the resonators R3 and R4 are inductively coupled together. Since the sub coupling portion SC14 acts as an inductive coupling window which limits widths (widths in the Y direction) orthogonal to the electric field direction of the resonators R1 and R4 by the presence of the through via conductors 2A, 2B, and 2C, the resonators R1 and R4 are inductively coupled together. In contrast, since the main coupling portion MC23 acts as a capacitive coupling window which limits widths in the electric field direction (Z direction) of the resonators R2 and R3 by the presence of the via conductors 3A to 3F and the window conductors 25A and 25B, the resonators R2 and R3 are capacitively coupled together. Note that although the through via conductors 2E and 2F limit widths (widths in the Y direction) orthogonal to the electric field direction of the resonators R2 and R3, action limiting the widths in the electric field direction (Z direction) of the via conductors 3A to 3F and the window conductors 25A and 25B is strong in this example, and the resonators R2 and R3 are capacitively coupled together.
Transmission lines, such as a strip line, a microstrip line, and a coplanar line, which connect with the I/O lands 15A and 15B are provided at the circuit board 90.
Signals in a TEM mode propagate to the strip conductors 16A and 16B inside the dielectric plate 1 shown in, for example,
In the dielectric waveguide filter 101 of the present preferred embodiment, the resonators R1, R2, R3, and R4 and the main coupling portions MC12, MC23, and MC34, as shown in
In the dielectric waveguide filter 101 of the present preferred embodiment, a main coupling portion between the resonator R1 that inputs and outputs signals from and to the outside and the resonator R2 that is coupled to the resonator R1 is an inductive coupling portion. Similarly, a main coupling portion between the resonator R4 that inputs and outputs signals from and to the outside and the resonator R3 that is coupled to the resonator R4 is an inductive coupling portion.
In the dielectric waveguide filter 101 of the present preferred embodiment, the resonator R1 and the resonator R4 are arranged along the sub coupling portion SC14 (
The internal conductor 7B includes a planar conductor PC (
A permittivity of the dielectric layer 1A between the first surface conductor 21 and the internal conductor 7B and a permittivity of the dielectric layer 1C between the second surface conductor 22 and the internal conductor 7B are higher than a permittivity of a dielectric (the dielectric layer 1B) in a different region.
In the dielectric waveguide resonant space, a parasitic resonant mode may appear in which an electric field faces in a direction along the first surface conductor 21 and the second surface conductor 22 (that is, a magnetic field rotates in a perpendicular direction (the Z direction shown in
Although the internal conductor 7B is shown in
According to the present preferred embodiment, since the internal conductor 7 is isolated from the first surface conductor and the second surface conductor 22, that is, the internal conductor 7 is floating galvanically from potentials of the first surface conductor 21 and the second surface conductor 22, the degree of concentration of currents at the internal conductor 7 is low (current-concentrated portions are dispersed). For this reason, a dielectric waveguide resonator having a high Q factor is obtained.
Here, a non-limiting example of improvement in Q factor will be illustrated. A dielectric plate used in each simulation is made of low-temperature fired ceramics (LTCC) having a relative permittivity εr of 8.5, sizes of the first surface conductor 21 and the second surface conductor 22 are set to 1.6 mm×1.6 mm, and a distance between the first surface conductor 21 and the second surface conductor 22 is set to 0.55 mm. In this case, a resonant frequency in the TE101 mode is 45.4 GHz, and unloaded Q (hereinafter denoted as “Qo”) is 350. If the conductor 7P of the comparative example shown in
A relationship between a position of an internal conductor in the dielectric plate 1 and a Q factor will next be illustrated.
In
As described above, in
The reason why polarized characteristics appear in the above-described manner is as follows.
First, a transmission phase of a resonator is 90° behind on a low-frequency side of a resonant frequency of the resonator and is 90° ahead on a high-frequency side of the resonant frequency. Since inductive coupling and capacitive coupling have a relationship in which phases thereof are reverse to each other, if inductive coupling and capacitive coupling are combined, there is a frequency at which a signal traveling through a main coupling portion and a signal traveling through a sub coupling portion have opposite phases and the same amplitude. An attenuation pole appears at the frequency. In the dielectric waveguide filter 101 of the present preferred embodiment, since the first resonator R1 and the second resonator R2 are inductively coupled, the second resonator R2 and the third resonator R3 are capacitively coupled, the third resonator R3 and the fourth resonator R4 are inductively coupled, and the first resonator R1 and the fourth resonator R4 are sub-coupled with the second resonator R2 and the third resonator R3 bypassed (cross-coupling with an even number of stages bypassed is performed), phases at the main coupling portions from the first resonator R1 to the fourth resonator R4 and a phase at the sub coupling portion from the first resonator R1 to the fourth resonator R4 are reverse to each other on the low-frequency side of the pass band and are also reverse to each other on the high-frequency side. That is, attenuation poles appear on both the low-frequency side and the high-frequency side of the pass band.
Note that although an internal conductor is preferably a solid cylindrical via conductor in the above-described example, an internal conductor may be a tubular via conductor in the shape of, for example, a hollow cylinder.
A second preferred embodiment will illustrate a dielectric waveguide filter different in, for example, the number of stages of resonators from that illustrated in the first preferred embodiment.
The dielectric waveguide filter 102 includes a dielectric plate 1. The dielectric plate 1 is obtained by processing, for example, dielectric ceramic, crystal, or resin into the shape of a rectangular parallelepiped. The dielectric plate 1 includes a first principal surface MS1 and a second principal surface MS2 which face each other, as shown in
Internal conductors 7A to 7F which extend in a perpendicular direction to the first principal surface MS1 and are electrically connected to neither the first surface conductor 21 nor the second surface conductor 22 are provided inside the dielectric plate 1.
I/O electrodes 24A and 24B and the ground electrode 23 are provided at a bottom surface of the dielectric plate 1. Strip conductors 16A and 16B which are connected to the I/O electrodes 24A and 24B through via conductors 3U and 3V are provided inside the dielectric plate 1. Via conductors 3A to 3S which connect the ground electrode 23 to the second surface conductor 22 are close to the bottom surface of the dielectric plate 1.
Window conductors 25A and 25B are inner layers of the dielectric plate 1. Through via conductors 2A to 2F which extend from the first surface conductor 21 to the second surface conductor 22 are also provided in the dielectric plate 1. Additionally, via conductors 3A and 3B, as shown in
Through via conductors 9A to 9V which connect the first surface conductor 21 and the second surface conductor 22 are also formed along side surfaces of the dielectric plate 1 inside the dielectric plate 1.
As shown in
The internal conductors 7A to 7F shown in, for example,
A main coupling portion MC12 is provided between the resonators R1 and R2, a main coupling portion MC23 is provided between the resonators R2 and R3, a main coupling portion MC34 is provided between the resonators R3 and R4, a main coupling portion MC45 is provided between the resonators R4 and R5, and a main coupling portion MC56 is provided between the resonators R5 and R6. A sub coupling portion SC25 is provided between the resonators R2 and R5.
As for any of the main coupling portions MC12, MC23, MC45, and MC56, there is no through via that an opening in a horizontal direction narrows. The respective dielectric waveguide resonant spaces of the resonators R1 to R6 are determined by the size of a resonant space demarcated by the first surface conductor 21, the second surface conductor 22, as shown in
None of the main coupling portions MC12, MC23, MC45, and MC56 has a window which limits a width in an electric field direction (the Z direction) of the resonator, and the main coupling portions MC12, MC23, MC45, and MC56 perform inductive coupling.
The main coupling portion MC34 includes the via conductors 3A, 3B, 3C, and 3D and the window conductors 25A and 25B shown in
Since the sub coupling portion SC25 acts as an inductive coupling window which limits the width of the resonators R2 and R5 (width in the Y direction) perpendicular to the electric field direction by the presence of the through via conductors 2E and 2F, the resonators R2 and R5 are inductively coupled together.
In the dielectric waveguide filter 102 of the present preferred embodiment, as shown in
In the dielectric waveguide filter 102 of the present preferred embodiment, a main coupling portion between the resonator R1 that inputs and outputs signals from and to the outside and the resonator R2 that is coupled to the resonator R1 is an inductive coupling portion. Similarly, a main coupling portion between the resonator R6 that inputs and outputs signals from and to the outside and the resonator R5 that is coupled to the resonator R6 is an inductive coupling portion.
In the dielectric waveguide filter 102 of the present preferred embodiment, the resonator R2 and the resonator R5 are also arranged along the sub coupling portion SC25. That is, the sub coupling portion SC25 is provided between the resonator R2 and the resonator R5. The sub coupling portion SC25 is an inductive coupling portion, and coupling in the sub coupling portion SC25 is weaker than coupling in the main coupling portions MC12, MC23, MC34, MC45, and MC56.
A third preferred embodiment will illustrate a dielectric waveguide filter including eight stages of dielectric waveguide resonators and one dielectric waveguide resonator for a trap resonator.
The dielectric waveguide filter 103 includes a dielectric plate 1. The dielectric plate 1 is obtained by processing, for example, dielectric ceramic, crystal, or resin into the shape of a rectangular parallelepiped, as shown in
I/O electrodes 24A and 24B and the ground electrode 23 are provided at a bottom surface of the dielectric plate 1. Strip conductors 16A and 16B which are connected to the I/O electrodes 24A and 24B through via conductors 3U and 3V are provided inside the dielectric plate 1. A plurality of via conductors which connect the ground electrode 23 to the second surface conductor 22 are formed close to the bottom surface of the dielectric plate 1.
Through via conductors 2A to 2N which extend from the first surface conductor 21 to the second surface conductor 22 are provided in the dielectric plate 1.
Through via conductors 9A to 9U which connect the first surface conductor 21 and the second surface conductor 22 are also provided along side surfaces of the dielectric plate 1 inside the dielectric plate 1.
As shown in, for example,
Internal conductors 7A to 7H and 7T shown in, for example,
Of the above-described resonators R1 to R8, the four resonators R1 to R4 are a first group of resonators, and the four resonators R5 to R8 are a second group of resonators. A main coupling portion MC45 is provided between the resonator R4 at a last stage in the first group and the resonator R5 at a first stage in the second group. The resonator R1 at a first stage of the first group and the resonator R8 at a last stage of the second group are resonators as I/O portions.
A main coupling portion MC12 is provided between the resonators R1 and R2, a main coupling portion MC23 is provided between the resonators R2 and R3, and a main coupling portion MC34 is provided between the resonators R3 and R4. That is, as for the first group of resonators, the four resonators R1 to R4 are series-connected via the main coupling portions. The main coupling portion MC45 is provided between the resonators R4 and R5. A main coupling portion MC56 is provided between the resonators R5 and R6, a main coupling portion MC67 is provided between the resonators R6 and R7, and a main coupling portion MC78 is provided between the resonators R7 and R8. That is, as for the second group of resonators, the four resonators R5 to R8 are series-connected via the main coupling portions. Additionally, a sub coupling portion SC27 is provided between the resonators R2 and R7, and a sub coupling portion SC36 is provided between the resonators R3 and R6.
The through via conductor 2i shown in
As for the main coupling portions MC34, MC45, and MC56, there is no through via that an opening in the horizontal direction narrows. Inductive coupling is performed at each of the portions because of the size of a resonant space demarcated by the first surface conductor 21, the second surface conductor 22, and the through via conductors 9A to 9U and resonant frequencies to be used.
A space where the internal conductor 7T is provided defines and functions as one trap resonator RT. The trap resonator RT is provided between the resonator R3 that is one stage ahead of the resonator R4 at the last stage of the first group and the resonator R6 that is one stage behind the resonator R5 at the first stage of the second group.
The trap resonator RT is provided at a position surrounded by the internal conductor 7D of the resonator R4 at the last stage of the first group, the internal conductor 7E of the resonator R5 at the first stage of the second group, the internal conductor 7C of the resonator R3 one stage ahead of the resonator R4 at the last stage of the first group, and the internal conductor 7F of the resonator R6 one stage behind the resonator R5 at the first stage of the second group.
A distance between the internal conductor 7D of the resonator R4 at the last stage of the first group and the internal conductor 7E of the resonator R5 at the first stage of the second group is narrower than a distance between the internal conductor 7C of the resonator R3 one stage ahead of the resonator R4 at the last stage of the first group and the internal conductor 7F of the resonator R6 one stage behind the resonator R5 at the first stage of the second group. With this configuration, regions, which are high in electric field strength, of the resonators R4, R5, and RT are close to each other, and the trap resonator RT is coupled to the resonators R4 and R5. From this, it can also be said that the trap resonator RT is a resonator branched from the resonators R4 and R5.
In the present preferred embodiment, a distance between the internal conductor 7D of the resonator R4 at the last stage of the first group and the internal conductor 7T for the trap resonator is equal to a distance between the internal conductor 7E of the resonator R5 at the first stage of the second group and the internal conductor 7T for the trap resonator. For this reason, strength of coupling of the resonator R4 to the trap resonator RT and strength of coupling of the resonator R5 to the trap resonator RT are equal.
Note that since the internal conductors 7C and 7T are away from each other and the internal conductors 7F and 7T are away from each other, that is, regions, which are high in electric field strength, of the resonators R3 and R6 and the trap resonator RT are relatively away from each other, the resonators R3 and R6 are not particularly coupled to the trap resonator RT.
As already described, in the dielectric waveguide filter 103 of the present preferred embodiment, the resonators R1, R2, R3, R4, R5, R6, R7, and R8 and the main coupling portions MC12, MC23, MC34, MC45, MC56, MC67, and MC78 are arranged along a main route for signal propagation. The main coupling portions MC12, MC23, MC34, MC45, MC56, MC67, and MC78 are all inductive coupling portions. The sub coupling portion SC27 is an inductive coupling portion, and the sub coupling portion SC36 is a capacitive coupling portion. Coupling in the sub coupling portion SC27 is weaker than coupling in the main coupling portions MC12, MC23, MC34, MC45, MC56, MC67, and MC78. Coupling in the sub coupling portion SC36 is weaker than coupling in the main coupling portions MC12, MC23, MC34, MC45, MC56, MC67, and MC78.
Finally, the description of the above-described preferred embodiments is illustrative in all respects and not to be restrictive. Modifications and changes can be appropriately made by those skilled in the art. The scope of the present invention is indicated not by the preferred embodiments but by the claims. Additionally, changes from the preferred embodiments within the scope equivalent to the claims are included in the scope of the present invention.
For example, the preferred embodiments described above have illustrated a dielectric waveguide filter including a plurality of dielectric waveguide resonators. It is also possible to provide a dielectric waveguide filter including a single dielectric waveguide resonator in the same manner.
The preferred embodiments described above have illustrated an example which provides a dielectric waveguide resonator having the TE101 mode as a dominant mode. For example, a high-order resonant mode, such as the TE201 mode or the TE102 mode, may be used.
While preferred embodiments of the present invention have been described above, it is to be understood that variations and modifications will be apparent to those skilled in the art without departing from the scope and spirit of the present invention. The scope of the present invention, therefore, is to be determined solely by the following claims.
Number | Date | Country | Kind |
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2019-222124 | Dec 2019 | JP | national |
This application claims the benefit of priority to Japanese Patent Application No. 2019-222124 filed on Dec. 9, 2019 and is a Continuation Application of PCT Application No. PCT/JP2020/039854 filed on Oct. 23, 2020. The entire contents of each application are hereby incorporated herein by reference.
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Number | Date | Country | |
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20220285809 A1 | Sep 2022 | US |
Number | Date | Country | |
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Parent | PCT/JP2020/039854 | Oct 2020 | WO |
Child | 17825022 | US |