1. Field of the Invention
The present invention relates to an input/output structure for a dielectric waveguide, and more particularly, to a structure for conversion between the dielectric waveguide and a coaxial line.
2. Description of the Related Art
A dielectric waveguide, which is obtained by providing an electrically conductive layer on a surface of a dielectric material, can eliminate the need for using a thick electrically conductive wall and effectively shorten an electromagnetic wave transmitted therethrough by virtue of the dielectric material, thereby to facilitate substantial reduction in size of the waveguide device as compared to a traditionally used hollow waveguide. Such a reduced in size waveguide device is small enough to be directly mounted on a substrate. Thus, an input/output structure has been used which employs a structure for conversion between the dielectric waveguide and the microstrip, formed by soldering the dielectric waveguide to a mounted substrate comprising a microstrip line for performing an input/output operation (see, for example, JP 2012-147286A).
A printed circuit board 8 has a front surface having an island-shaped electrode 8b and a back surface having a microstrip 8a. The printed circuit board 8 also comprises a via-hole 8c for coupling the island-shaped electrode 8b and the microstrip 8a together. The dielectric waveguides la and le are arranged to allow the island-shaped electrodes 5a and 5e each provided on the respective bottom surface of the dielectric waveguides 1a and 1e to be opposed to the island-shaped electrodes 8b and 8b each provided on the respective front surface of the printed circuit boards 8 and 8, respectively.
Patent Document 1: JP 2012-147286A
Patent Document 2: JP 2003-318614A
The inner portion of the dielectric waveguide is filled with the dielectric body. Thus, it is impossible to insert any structure into the dielectric waveguide. Therefore, when it is desired to couple the dielectric waveguide to a coaxial line, it is difficult to use a structure that has been used in a conventional hollow waveguide for conversion between a hollow waveguide and a coaxial line, in which the structure is formed by inserting a probe into the hollow waveguide. For this reason, it is required, as illustrated in
According to the present invention, there is provided an input/output structure for a dielectric waveguide having a dielectric body and an electrically conductive layer covering the dielectric body, wherein the dielectric waveguide comprises: a rectangular-parallelepiped-shaped dielectric block, a plate-shaped dielectric plate, and a feeder line comprising a line-shaped electrically conductive foil sandwiched between the dielectric block and the dielectric plate.
The dielectric waveguide input/output structure of the present invention makes it possible to achieve an input/output structure with less degradation in performance because it can perform conversion directly between the dielectric waveguide and the coaxial line without without converting the waveguide to a microstrip. Further, this dielectric waveguide input/output structure makes it possible to reduce the size of the input/output structure because it eliminates the need for using a printed circuit board for the microstrip line.
(First Embodiment)
A first embodiment of the present invention will now be described with reference to the drawings.
The dielectric block 20 and the dielectric plate 30 are coupled together using a joining glass, and the external electrically conductive layer, the island-shaped electrode 90 and the feeder line 60 are formed by printing a silver paste followed by sintering.
The dielectric waveguide 18 as described above exhibits less degradation in performance because it can perform conversion directly between the dielectric waveguide and the coaxial line. Further, the dielectric waveguide 18 can provide a downsized dielectric waveguide input/output structure because it eliminates the need for using a printed circuit board for the microstrip line.
This type of structure having a convex portion in the resonator, which is referred to as a re-entrant structure, is known to reduce the length in the axial direction of the dielectric waveguide to decrease the area occupied by the dielectric waveguide, and to be capable of suppressing a third harmonic that is not easy to be suppressed. If the dielectric waveguide 18 does not have the through-hole 50, it cannot be successfully oscillated by feeding electrical signals therewith from the direction of the side surface. Thus, providing the through-hole 50 has an effect that the dielectric waveguide 18 can be operated in a successful manner, that the length of the waveguide can be reduced, and that the third harmonic can be suppressed. Further, the dielectric waveguide 18 also has an effect of reducing unwanted radiations because it has a conversion section not exposed to the outside but located in the dielectric body.
In the re-entrant structure, the bottom surface 50a of the through-hole 50 has less influence on the characteristic of the structure even when it allows the dielectric body to be exposed. Thus, it may be possible to provide no electrically conductive layer on the bottom surface 50a of the through-hole 50.
Further, it is considered that the dielectric block 20 is operating in a mode close to a TE mode, while the dielectric plate 30 is operating in a mode close to a TEM mode. Thus, it is considered that the dielectric block 20 and the dielectric plate 30 are operating in different operation modes. Therefore, the boundary between the dielectric block 20 and the dielectric plate 30 has a small influence on the characteristic of the structure, and it has a small influence on the characteristic even in the presence of a gap caused by the joining glass between the dielectric block 20 and the dielectric plate 30. Preferably, the joining glass has a relative permittivity close to those of the dielectric block 20 and the dielectric plate 30.
Further, the relative permittivities of the dielectric block 20 and the dielectric plate 30 may be varied. The dielectric material having higher relative permittivity is expensive. Thus, it may be possible to reduce the cost of the dielectric waveguide input/output structure by, for example, employing for the dielectric plate 30 a less expansive dielectric material with lower relative permittivity than the dielectric block 20.
(Second Embodiment)
As illustrated in
By providing the open stub 61a, it becomes possible to suppress the second harmonic. Further, by forming the feeder line 61 to have the distal end having a width y1 that is thicker than a width y0 of the root portion thereof, it becomes possible to improve the power durability by locating the distal end at a distance from the through-hole, and to achieve a larger bandwidth of the input/output structure by keeping the external Q at low level.
The dielectric waveguide 19 as described above can have an input/output structure with capability of suppressing the second harmonic, improved power durability and larger bandwidth by only changing the shape of the feeder line of the dielectric waveguide illustrated in the first embodiment.
(Third Embodiment)
Each of the dielectric waveguides 11 and 15 positioned at either side of the dielectric waveguide filter 100 comprises a rectangular-parallelepiped-shaped dielectric block 20, a plate-shaped dielectric plate 30 having a circular through-hole 50 with a diameter y in an approximately central region thereof, and a feeder line 61 comprising a line-shaped electrically conductive foil sandwiched between the dielectric block and the dielectric plate. The feeder line 61 has an end portion coupled to an island-shaped electrode 90 that is insulated from the electrically conductive layer provided on a side surface of the dielectric waveguides 11 and 15.
Each of the dielectric waveguides 11 and 15 is coupled to an external device which is not shown, via a connector 70 connected to the island-shaped electrode 90.
The feeder line 61 has a distal end having a width that is thicker than a width of a root portion thereof. Further, the feeder line 61 has an approximately quarter wavelength open stub 61a provided on each of opposite sides at a position spaced away from a distal end thereof by an approximately quarter wavelength.
The dielectric waveguide filter 100 as described above has an input/output structure with less degradation in performance because it employs a dielectric waveguide input/output structure that can perform conversion directly from the dielectric waveguide to the coaxial line. Further, this dielectric waveguide 100 can provide a reduced-in-size dielectric waveguide filter because it eliminates the need for using a printed circuit board for the microstrip line.
In each figure, frequency f [GHz] is shown on a horizontal axis, [dB] is shown on a vertical axis, characteristic of the dielectric waveguide filter 100 is depicted in solid line, and characteristic of the dielectric waveguide filter 1 is depicted in dotted line.
Each of the dielectric waveguide filters 1 and 100 in
In the dielectric waveguide filter 100, each component has the following dimensions:
The result in
Further, the result in
Moreover, the result in
Thus, the dielectric waveguide filter 100 of the present invention can exhibit less degradation in performance and can eliminate the need for using a printed circuit board for the microstrip line because it can perform conversion directly from the dielectric waveguide to the coaxial line without any conversion to the microstrip. Further, the dielectric waveguide filter 100 can provide a reduced-in-size dielectric waveguide input/output structure because the axial length of the dielectric waveguide can be shortened by having a re-entrant structure.
Further, the dielectric waveguide filter 100 makes it possible to suppress the second harmonic by having an open stub, and even to suppress the third harmonic, that is not easily suppressed, by having a re-entrant structure. Thus, a dielectric waveguide filter with lower harmonic generation can be achieved. As a result, it is not required to alternatively use a low-pass filter for suppressing the harmonic components.
Furthermore, the dielectric waveguide filter 100 also makes it possible to suppress unwanted radiations at the input/output conversion section because the feeder line and the open stub provided therewith are located within the waveguide and are not exposed to the outside.
The feeder line is drawn out to the direction orthogonal to the coupling direction of the dielectric waveguide. Alternatively, it may be drawn out to any direction. If the feeder line is pulled out to the longitudinal direction of the dielectric block, it is subject to less dimensional restriction than the case of being drawn out to the short-side direction, so that the distance between the distal end of the feeder line and the through-hole, for example, may be increased. This makes it possible to improve the power durability of the feeder line.
The dielectric waveguide input/output structure of the present invention is not limited to the input/output structure for the dielectric waveguide filter, but is applicable to various types of dielectric waveguide device having a connection to external devices.
Number | Date | Country | Kind |
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2013-071502 | Mar 2013 | JP | national |
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10-093311 | Apr 1998 | JP |
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Number | Date | Country | |
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20140292438 A1 | Oct 2014 | US |