Patent Application
20130196608
The present invention relates to a coaxial resonator, and a dielectric filter, a wireless communication module, and a wireless communication device that employ the coaxial resonator.
As a resonator in which resonance occurs at a predetermined frequency, there is known a coaxial resonator composed of an inner conductor disposed in the inside of a through hole formed in a dielectric block, and an outer conductor disposed on the outside of the dielectric block (refer to Patent Literature 1, for example).
Patent Literature 1: Japanese Unexamined Patent Publication JP-A 1-227501 (1989)
However, the conventional coaxial resonator as proposed in Patent Literature 1 has difficulty in achieving both a rise in Q value in the first resonant mode and a widening of the gap in resonant frequency between the first resonant mode and the second resonant mode. Note that the first resonant mode refers to, among a multiplicity of coaxial resonator's resonant modes, a resonant mode of the lowest resonant frequency, whereas the second resonant mode refers to a resonant mode of the second lowest resonant frequency. In general, the first resonant mode of coaxial resonators is utilized, wherefore a rise in Q value in the first resonant mode involves improvements in the electrical characteristics of coaxial resonators. Moreover, it is desirable that the second resonant mode corresponding to a spurious mode is apart in respect of frequency from the first resonant mode.
The invention has been devised in view of the problem associated with the conventional art as mentioned supra, and accordingly an object thereof is to provide a coaxial resonator having a high Q value in the first resonant mode and a wide resonant frequency gap between the first resonant mode and the second resonant mode, as well as to provide a dielectric filter, a wireless communication module, and a wireless communication device that employ the coaxial resonator.
A coaxial resonator according to the invention comprises: a first outer conductor connected to a reference potential; a dielectric block which is a dielectric body having a rectangular parallelepiped shape, the dielectric block being provided with a through hole formed so as to pass therethrough from a first side surface to a second side surface opposed to the first side surface of the dielectric block, and being so disposed that a first main surface of the dielectric block abuts on the first outer conductor; an inner conductor disposed in an inside of the through hole; and a second outer conductor which is shaped like a rectangular box having its one face which is opened toward the first outer conductor, the second outer conductor having an inside dimension such that the dielectric block can be housed therein so as to be spaced from its second main surface, third side surface, and fourth side surface, and being connected to the reference potential.
Moreover, a dielectric filter according to the invention includes: the above-mentioned coaxial resonator including a plurality of the inner conductors, the inner conductors being spaced apart in a row in a direction from the third side surface to the fourth side surface; and terminal electrodes electrically or electromagnetically connected to an inner conductor on a third side surface side and an inner conductor on a fourth side surface side, respectively, the inner conductor on the third side surface side and the inner conductor on the fourth side surface side each being an endmost conductor of the row.
Further, a wireless communication module according to the invention includes: an RF section including the above-mentioned dielectric filter; and a baseband section connected to the RF section.
Still further, a wireless communication device according to the invention includes: the above-mentioned wireless communication module; and an antenna connected to the RF section of the wireless communication module.
According to the coaxial resonator of the invention, it is possible to obtain a coaxial resonator having a high Q value in the first resonant mode and a wide resonant frequency gap between the first resonant mode and the second resonant mode.
Moreover, according to the dielectric filter of the invention, since a bandpass filter is constructed by using the above-mentioned coaxial resonator having a high Q value in the first resonant mode and a wide resonant frequency gap between the first resonant mode and the second resonant mode, it follows that the dielectric filter excels in frequency selectivity with the advantages of low losses and the absence of spurious components in the vicinity of a pass band.
Further, according to the wireless communication module and the wireless communication device of the invention, since wave filtering is performed on communication signals by using the above-mentioned dielectric filter having low losses and excellent frequency selectivity, it is possible to decrease attenuation and noise of communication signals, and thereby allow the wireless communication module and the wireless communication device to have high-quality communication performance capability and high reliability.
Hereinafter, a coaxial resonator of the present embodiment will be described in detail with reference to the accompanying drawings.
As shown in
The first outer conductor 21, which is a sheet-like conductor placed on the main surface of the dielectric substrate 11, is connected to a reference potential (ground potential).
The dielectric block 30, which is a dielectric body having a rectangular parallelepiped shape, is provided with a through hole 31 formed so as to pass therethrough from a first side surface 30c to a second side surface 30d opposed to the first side surface 30c of the dielectric block, and is so disposed that a first main surface 30a of the dielectric block 30 abuts on the first outer conductor 21. Note that the term “rectangular parallelepiped shape” is construed as encompassing the shape of a hexahedron with six rectangular faces having, for example, a protrusion or recess formed in part of one specific face thereof. Moreover, the inner conductor 41 is disposed in the inside of the through hole 31.
The second outer conductor 22 is a conductor shaped like a rectangular box having its one face which is opened, has an inside dimension such that the dielectric block 30 can be housed therein so as to be spaced from its second main surface 30b, third side surface 30e, and fourth side surface 30f. The second outer conductor 22 is, upon being placed so that its opening points toward the first outer conductor 21, connected to the first outer conductor 21 and is thereby connected to a reference potential (ground potential). The first outer conductor 21 and the second outer conductor 22 are positioned so as to surround the dielectric block 30 for serving as the outer conductor of the coaxial resonator. Moreover, in the case shown in
According to the coaxial resonator having such constitution of this embodiment, since a spacing is secured between the second outer conductor 22 which serves as part of the outer conductor of the coaxial resonator and each of the second main surface 30b, the third side surface 30e, and the fourth side surface 30f of the dielectric block 30, it follows that a low-dielectric-constant portion which is lower in dielectric constant than the dielectric block 30 is created between them. This makes it possible to decrease the effective dielectric constant in between the second outer conductor 22 serving as part of the outer conductor and the inner conductor 41 and thereby equalize the resonant frequency of the first resonant mode, and therefore, in contrast to a coaxial resonator in which the second outer conductor 22 is disposed so as not to be spaced from each of the second main surface 30b, the third side surface 30e, and the fourth side surface 30f of the dielectric block 30; that is, disposed so as to cover each of them, a rise in Q value in the first resonant mode, as well as a widening of the gap in resonant frequency between the first resonant mode and the second resonant mode, can be achieved.
Moreover, according to the coaxial resonator of this embodiment, the first main surface 30a of the dielectric block 30 is abutted on the first outer conductor 21, which allows the coaxial resonator to feature structural simplicity and ease of manufacture.
Further, according to the coaxial resonator of this embodiment, it is preferable that the inner conductor 41 is so disposed that its center is situated closer to the second main surface 30b beyond a position midway between the first main surface 30a and the second main surface 30b. That is, in the case of locating the inner conductor 41 closer to the second main surface 30b, in contrast to a case where the inner conductor 41 is located centrally of the dielectric block or located closer to the first main surface 30a, in the range between the first main surface 30a and the second main surface 30b, it is possible to increase the spaced interval between the inner conductor 41 and the first outer conductor 21, and thereby achieve both a further rise in Q value in the first resonant mode and a further widening of the gap in resonant frequency between the first resonant mode and the second resonant mode.
Although it is preferable to increase the spaced interval between the second outer conductor 22 and each of the second main surface 30b, the third side surface 30e, and the fourth side surface 30f of the dielectric block 30 in the interest of improvement in electrical characteristics, an increase in the spaced interval may cause the coaxial resonator to grow in size, and therefore the spaced interval should preferably be adjusted properly with consideration given to the required electrical characteristics and the permissible outer dimension of the coaxial resonator.
As shown in
It is noted that, in this embodiment, a structure including the outer conductor composed of the first outer conductor 21 and the second outer conductor 22, and one of a plurality of inner conductors 41 arranged in the dielectric block 30, for example, the inner conductor 41a, fulfills the conditions for constituting a coaxial resonator, and therefore, in the following description, a construction including a plurality of inner conductors 41a through 41f having a common outer conductor is assumed to have a plurality of coaxial resonators. That is, in
In the dielectric filter shown in
Moreover, on the second side surface 30d of the dielectric block 30, a capacitive coupling electrode (not shown) is disposed for each of the inner conductors 41a through 41f. A predetermined electrostatic capacitance is formed between the adjacent capacitive coupling electrodes for strengthening the electromagnetic coupling between the adjacent coaxial resonators. Further, at the first side surface 30c of the dielectric block 30, slits 61b through 61f are formed so as to lie between their respective adjacent ones of the inner conductors 41a through 41f.
Moreover, the first terminal electrode 51 is located below the inner conductor 41a on the third side surface side, and lies across the first side surface 30c and the first main surface 30a of the dielectric block 30 while being kept out-of-contact with the first outer conductor 21. Thus, the first terminal electrode 51 is electromagnetically connected to the inner conductor 41a on the third side surface side.
On the other hand, the second terminal electrode 52 is located below the inner conductor 41 on the fourth side surface side, and lies across the first side surface 30c and the first main surface 30a of the dielectric block 30 while being kept out-of-contact with the first outer conductor 21. Thus, the second terminal electrode 52 is electromagnetically connected to the inner conductor 41 on the fourth side surface side.
In the dielectric filter having such constitution of this embodiment, upon the input of an electric signal to, for example, the first terminal electrode 51, then resonance occurs in the plurality of coaxial resonators formed of the inner conductors 41a through 41f and the outer conductor consisting of the first outer conductor 21 and the second outer conductor 22, whereupon output of electric signal is produced from the second terminal electrode 52. At that time, with the selective passage of signals lying in a frequency band including the resonant frequencies of the plurality of coaxial resonators, the dielectric filter functions as a bandpass filter. Thus, the dielectric filter of this embodiment is constructed by forming a plurality of coaxial resonators of the first embodiment as described previously, and a bandpass filter can be implemented by establishing electromagnetic coupling between the plurality of coaxial resonators.
According to the dielectric filter having such constitution of this embodiment, the coaxial resonators having a high Q value in the first resonant mode and a wide resonant frequency gap between the first resonant mode and the second resonant mode are used to fabricate a bandpass filter, wherefore the dielectric filter has excellent frequency selectivity with the advantages of low losses and the absence of spurious components in the vicinity of the pass band.
Moreover, in the dielectric filter of this embodiment, the dielectric block 30 has a protrusion 32. The protrusion 32 has its surface made continuous with the second side surface 30d, the third side surface 30e, and the fourth side surface 30f. The protrusion 32 alone has a rectangular parallelepiped shape, and is formed on the second main surface 30b of the dielectric block 30 so as to be situated closer to the second side surface 30d.
There may be cases where a secondary resonant mode of the coaxial resonator constituting the dielectric filter of this embodiment is not a λ mode which is a normal high-order mode for coaxial resonators but a so-called cavity mode. In this case, the magnitude of an electric field in the secondary resonant mode is, in a direction from the first side surface 30c to the second side surface 30d of the dielectric block 30, greater in the middle region yet is smaller at both end regions. On the other hand, the magnitude of an electric field in a primary resonant mode of the coaxial resonator constituting the dielectric filter of this embodiment is, in the direction from the first side surface 30c to the second side surface 30d, zero in the middle region yet rises to a maximum at both end regions in the form of open ends.
It is therefore preferable to shape the dielectric block 30 so that, in the direction from the first side surface 30c to the second side surface 30d, at least one of the end located on the first side surface 30c side and the end located on the second side surface 30d side, is greater than the midportion thereof in respect of the distance between the first main surface 30a and the second main surface 30b.
Thus, in the case where, just as with the dielectric filter of this embodiment, the dielectric block 30 has the protrusion 32, the dielectric block 30 takes on the configuration in which, in the direction from the first side surface 30c to the second side surface 30d, a distance between the first main surface 30a and the second main surface 30b at one of the opposite ends of the dielectric block is greater than a distance between the first main surface 30a and the second main surface 30b at the midportion of the dielectric block 30. This makes it possible to widen the gap in resonant frequency between the primary resonant mode and the secondary resonant mode, as well as to strengthen the electromagnetic coupling between the adjacent coaxial resonators.
Moreover, when the secondary resonant mode of the coaxial resonator constituting the dielectric filter of this embodiment is the cavity mode, an electric field in the secondary resonant mode is, in the direction from the first side surface 30c to the second side surface 30d of the dielectric block 30, highest in intensity in the middle region, yet is weakened gradually from the middle region to each end region and eventually becomes zero at a certain point. That is, the electric field at each end region is weak inversely with that at the middle region. The point at which the electric field becomes zero exists within the range from each end to a point spaced therefrom by a distance equivalent to a quarter of the entire length between the first side surface 30c and the second side surface 30d. Accordingly, it is desirable that, in the dielectric block 30, in the direction from the first side surface 30c to the second side surface 30d, that part thereof, which lies within the range from at least one of the opposite ends to a point spaced therefrom by a distance equivalent to a quarter of the length between the first side surface 30c and the second side surface 30d, is greater in the distance between the first main surface 30a and the second main surface 30b than the midportion thereof.
Moreover, in the dielectric filter of this embodiment, the dielectric block 30 is formed with the slits 61b through 61f. Also by virtue of the slits 61b through 61f, it is possible to achieve both a rise in Q value in the primary resonant mode and a widening of the gap in resonant frequency between the primary resonant mode and the secondary resonant mode. In addition, the provision of the slits 61b through 61f allows adjustment to the electromagnetic coupling between the adjacent resonators. Note that, in the case of forming the slits 61b through 61f only at the first side surface 30c or the second side surface 30d, capacitive coupling can be readily established between coaxial resonators at the side surface free from the slits 61b through 61f, whereas, in the case of forming the slits 61b through 61f so as to extend across the first side surface 30c and the second side surface 30d, it is possible to achieve both a further rise in Q value in the primary resonant mode and a further widening of the gap in resonant frequency between the primary resonant mode and the secondary resonant mode.
In the dielectric filter of this embodiment, and in the above-mentioned coaxial resonator of the first embodiment as well, as the material of construction of the dielectric block 30, a resin material such as epoxy resin and a ceramic material such for example as a ceramic dielectric can be used. For example, a dielectric ceramic material containing BaTiO3, Pb4Fe2Nb2O12, TiO2, etc. can be preferably used. As the material of construction of various electrodes and conductors, for example, an electrically conductive material composed predominantly of Ag or a Ag alloy such as Ag—Pd or Ag—Pt, a Cu-based conductive material, a W-based conductive material, a Mo-based conductive material, a Pd-based conductive material, and so forth are preferably used. The thickness of each of the electrodes and conductors is adjusted to fall in a range from 0.001 mm to 0.2 mm, for example.
In order to attain the effects as above described, it is preferable to form the slit 61a, 61g between the inner conductor 41a on the third side surface and the third side surface 30c or between the inner conductor 41f on the fourth side surface and the fourth side surface 30d in proximity to the inner conductor 41a on the third side surface or the inner conductor 41f on the fourth side surface. Moreover, in the case shown in
Next,
The wireless communication module 80 of this embodiment comprises: a baseband section 81 configured to process baseband signals; and an RF section 82 connected to the baseband section 81, configured to process RF signals obtained after modulation and before demodulation of baseband signals. The RF section 82 includes a dielectric filter 821 based on the above-mentioned second embodiment, so that, out of RF signals resulting from modulation of baseband signals or received RF signals, those that lie outside the communication band are attenuated by the dielectric filter 821.
As specific configuration, the baseband section 81 includes a baseband IC 811. Moreover, the RF section 82 includes an RF IC 822 connected between the dielectric filter 821 and the baseband section 81. Note that another circuit may be interposed between these circuits. Upon connecting an antenna 84 to the dielectric filter 821 of the wireless communication module 80, construction of the wireless communication device 85 of this embodiment capable of transmission and reception of RF signals can be completed.
According to the wireless communication module 80 and wireless communication device 85 having such constitution of this embodiment, since wave filtering is performed on communication signals with use of the dielectric filter 821 having low losses and excellent frequency selectivity, it is possible to decrease attenuation and noise of communication signals, and thereby obtain a wireless communication module 80 and wireless communication device 85 having high-quality communication performance capability.
It should be understood that the application of the invention is not limited to the specific embodiments described heretofore, and that various changes and modifications are possible without departing from the spirit and scope of the invention.
While the first to third embodiments have been described with respect to the case where the inner conductor is opened at both ends thereby constituting a half-wavelength resonator, it does not constitute any limitation. The invention may be implemented as a coaxial resonator with an inner conductor which is connected to a reference potential at one end thereby constituting a quarter-wavelength resonator, and a dielectric filter using the coaxial resonator.
Moreover, while the first to third embodiments have been described with respect to the case where the space between the dielectric block 30 and the second outer conductor 22 is filled with air, it does not constitute any limitation. For example, a vacuum may be created in the space between the dielectric block 30 and the second outer conductor 22, or the space between the dielectric block 30 and the second outer conductor 22 may be filled with a dielectric material (including air) which is lower in dielectric constant than the dielectric block 30.
Moreover, while the dielectric filter of the second embodiment has been described with respect to the case where the dielectric block 30 has the protrusion 32 which is situated closer to the second side surface 30d, it does not constitute any limitation. For example, the dielectric block 30 may have a protrusion 32 which is situated closer to the first side surface 30c, or the dielectric block 30 may have protrusions 32 that are situated closer to the first side surface 30c and the second side surface 30d, respectively. Further, in a case where the level of required electrical characteristics is not so high, instead of forming the protrusion 32 as shown in
Moreover, while the dielectric filter of the second and third embodiments has been described with respect to the case where there are provided six coaxial resonators by using the outer conductor consisting of the first outer conductor 21 and the second outer conductor 22 and the inner conductors 41a through 41f disposed in the insides of the through holes 31a through 31f, respectively, it does not constitute any limitation, and it is therefore possible to constitute a dielectric filter by using any number, for example two or more, of coaxial resonators. However, in general, the number of coaxial resonators is preferably less than or equal to about 20, because an increase in the number of coaxial resonators leads to an increase in size.
In addition, while the dielectric filter of the second and third embodiments has been described with respect to the case where the first and second terminal electrodes 51 and 52 are electromagnetically connected to the inner conductors 41a and 41f, respectively, the first and second terminal electrodes 51 and 52 may be electrically connected to the inner conductors 41a and 41f, respectively.
Next, concrete examples of the coaxial resonator of the present embodiment will be described.
Firstly, the electrical characteristics of the coaxial resonator of the first embodiment shown in
In the dielectric body constituting the dielectric block 30 used in the simulation, the relative permittivity was 10, and the dielectric tangent was 0.0005. Moreover, the electrical conductivity of each of various conductors and electrodes was 58×106 S/m. The dielectric block 30 was given a rectangular parallelepiped shape which was 13 mm in height (the distance from the first main surface 30a to the second main surface 30b) and in width (the distance from the third side surface 30e to the fourth side surface 30f), and 28 mm in length (the distance from the first side surface 30c to the second side surface 30d).
Further, the through hole 31 was given a cylindrical shape which was 3 mm in diameter, and, the center of the through hole 31 was spaced by a distance of 10 mm away from the first main surface 30a, and was located centrally between the third side surface 30e and the fourth side surface 30f. The inner conductor 41 was placed in the inside of the through hole 31. In addition, the first outer conductor 21 was given a rectangular shape which was 38 mm in length and 20 mm in width, and the dielectric block 30 was situated in the middle of the first outer conductor 21. The second outer conductor 22 was shaped like a rectangular box having its one face which is opened, which was 38 mm in length and 20 mm in width and in height.
According to the result of the simulation, the resonant frequency of the first resonant mode was 2.05 GHz; the Q value thereof was 1450; and the resonant frequency of the second resonant mode was 3.6 GHz. Moreover, a simulation was conducted as to the electrical characteristics of a coaxial resonator of a comparative example in which an inner conductor having a diameter of 3 mm and a length of 23 mm was disposed centrally of a dielectric block which was 23 mm in length and 20 mm in width and height, and this dielectric block was placed in the middle of an outer conductor having a space which was 33 mm in length and 20 mm in width and height in the direction of the length thereof. According to the result of the simulation, the resonant frequency of the first resonant mode was 1.99 GHz; the Q value thereof was 1319; and the resonant frequency of the second resonant mode was 2.7 GHz. Thus, the coaxial resonator of the first embodiment had a high Q value of the primary resonant mode than the coaxial resonator of the comparative example. Moreover, the coaxial resonator of the first embodiment, although it was nearly equal to the coaxial resonator of the comparative example in respect of the resonant frequency of the primary resonant mode, is higher than the coaxial resonator of the comparative example in respect of the resonant frequency of the secondary resonant mode; that is, there was a wide gap in resonant frequency between the first resonant mode and the second resonant mode.
Accordingly, it has been confirmed that the coaxial resonator can be obtained that includes: the first outer conductor 21 connected to a reference potential; the dielectric block 30 which is a dielectric body having a rectangular parallelepiped shape, is provided with the through hole 31 formed so as to pass therethrough from the first side surface 30c to the second side surface 30d opposed to the first side surface 30c, and is so disposed that its first main surface 30a abuts on the first outer conductor 21; the inner conductor 41 disposed in the inside of the through hole 31; and the second outer conductor 22 which is shaped like a rectangular box having its one face which is opened toward the first outer conductor 21, has an inside dimension such that the dielectric block 30 can be housed therein so as to be spaced from its second main surface 30b, third side surface 30e, and fourth side surface 30f, and is connected to a reference potential, and thus, wherein, the Q value in the first resonant mode is high and a gap in resonant frequency between the first resonant mode and the second resonant mode is wide.
Next, the electrical characteristics of the dielectric filter of the second embodiment shown in
Where the dimension of the dielectric block 30 excluding the protrusion 32 is concerned, the height, viz., the distance from the first main surface 30a to the second main surface 30b was 8.5 mm; the width, viz., the distance from the third side surface 30e to the fourth side surface 30f was 56 mm; and the length, viz., the distance from the first side surface 30c to the second side surface 30d was 23.7 mm. Moreover, the protrusion 32 has its surface made continuous with the second side surface 30d, the third side surface 30e, and the fourth side surface 30f of the dielectric block 30, and the protrusion 32 alone was given a rectangular parallelepiped shape. Where the dimension of the protrusion 32 is concerned, the height from the second main surface 30b was 2 mm; the length in the direction from the first side surface 30c to the second side surface 30d was 4 mm; and the width, viz., the distance from the third side surface 30e to the fourth side surface 30f was 56 mm.
Moreover, the through holes 31a through 31f were each given a cylindrical shape which was 3 mm in diameter, and, the center of each of the through holes 31a through 31f was spaced by a distance of 5 mm away from the first main surface 30a. These through holes 31 were so arranged that their centers are spaced equidistantly, and the inner conductor 41 was placed in the inside of each of the through holes 31. Further, the slits 61b through 61f formed so as to lie between their respective adjacent ones of the inner conductors 41a through 41f were each 1.0 mm in width, and 7.5 mm in depth in the direction from the first main surface 30a to the second main surface 30b. In addition, the first outer conductor 21 was given a rectangular shape which was 31.7 mm in length and 62 mm in width, and the dielectric block 30 was situated in the middle of the first outer conductor 21. The second outer conductor 22 was shaped like a rectangular box having its one face which is opened, which was 31.7 mm in length, 62 mm in width, and 15 mm in height.
The result of the simulation was shown in the graph of
Next, the electrical characteristics of the dielectric filter of the second and third embodiments shown in
Where the dimension of the dielectric block 30 excluding the protrusion 32 is concerned, the height, viz., the distance from the first main surface 30a to the second main surface 30b was 9.5 mm; the width, viz., the distance from the third side surface 30e to the fourth side surface 30f was 56 mm; and the length, viz., the distance from the first side surface 30c to the second side surface 30d was 23.7 mm. Moreover, the protrusion 32 had its surface made continuous with the second side surface 30d, the third side surface 30e, and the fourth side surface 30f of the dielectric block 30, and the protrusion 32 alone was given a rectangular parallelepiped shape. Where the dimension of the protrusion 32 is concerned, the height from the second main surface 30b was 4.2 mm; the length in the direction from the first side surface 30c to the second side surface 30d was 4 mm; and the width, viz., the distance from the third side surface 30e to the fourth side surface 30f was 56 mm.
Moreover, the through holes 31a through 31f were each given a cylindrical shape which was 3 mm in diameter, and, the center of each of the through holes 31a through 31f was spaced by a distance of 5 mm away from the first main surface 30a. The through holes 31a through 31f were so arranged that their centers are spaced equidistantly, and the inner conductor 41 was placed in the inside of each of the through holes 31. Further, the slits 61b through 61f formed so as to lie between their respective adjacent ones of the inner conductors 41a through 41f were each 1.0 mm in width, and 7.5 mm in depth in the direction from the first main surface 30a to the second main surface 30b. Still further, the first outer conductor 21 was given a rectangular shape which was 31.7 mm in length and 62 mm in width, and the dielectric block 30 was situated in the middle of the first outer conductor 21. The second outer conductor 22 was shaped like a rectangular box having its one face which is opened, which was 31.7 mm in length, 62 mm in width, and 15 mm in height. In addition, in the dielectric filter of the third embodiment shown in
According to the result of the simulation, in the dielectric filter of the second embodiment shown in
It has been found out from the result that, in the dielectric block 30, the provision of the slit 61a between the inner conductor 41a on the third side surface and the third side surface 30c, as well as the provision of the slit 61g between the inner conductor 41f on the fourth side surface and the fourth side surface 30d, allows both a further rise in Q value in the first resonant mode and a further widening of the gap in resonant frequency between the first resonant mode and the second resonant mode. Accordingly, it has been found out that the dielectric filter having the above-mentioned constitution affords more excellent frequency selectivity.
Moreover, since the dielectric filter of this embodiment has low losses and excellent frequency selectivity, it is possible to reduce attenuation and noise of communication signals through wave filtering on the communication signals, and it has thus been found out that, in the case of utilizing the dielectric filter of this embodiment for a wireless communication module and a wireless communication device, it is possible to allow the wireless communication module and the wireless communication device to have high-quality communication performance capability and high reliability.
| Number | Date | Country | Kind |
|---|---|---|---|
| 2010-219072 | Sep 2010 | JP | national |
| Filing Document | Filing Date | Country | Kind | 371c Date |
|---|---|---|---|---|
| PCT/JP2011/072420 | 9/29/2011 | WO | 00 | 3/28/2013 |
