JP4105017B2 - Waveguide type dielectric filter - Google Patents

Waveguide type dielectric filter Download PDF

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Publication number
JP4105017B2
JP4105017B2 JP2003101047A JP2003101047A JP4105017B2 JP 4105017 B2 JP4105017 B2 JP 4105017B2 JP 2003101047 A JP2003101047 A JP 2003101047A JP 2003101047 A JP2003101047 A JP 2003101047A JP 4105017 B2 JP4105017 B2 JP 4105017B2
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Prior art keywords
dielectric
input
waveguide
filter
output
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JP2004312217A (en
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主一 谷田部
洋 小島
弘幸 加藤
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Toko Inc
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Toko Inc
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Description

【0001】
【発明の属する技術分野】
本発明はGHz帯といった高周波領域で使用する導波管型誘電体フィルタに係るもので、所望の減衰極を得ることのできる導波管型誘電体フィルタに関するものである。
【0002】
【従来の技術】
【特許文献1】
米国特許第5926079号
【特許文献2】
特開平6−177607号公報
【0003】
誘電体導波管共振器を複数結合させることにより、さまざまな形態の導波管型誘電体フィルタを実現することができる。図10はそのような導波管型誘電体フィルタを示すもので、誘電体ブロック21に3個の共振器22A、22B、22Cを構成し、共振器間にはアイリスを形成して結合を調整している。入出力端の共振器22A、22Cの底面から端面に向かって伸びる導体ストリップを入力電極25、出力電極26としている。入出力電極の両側およびそれらに接する端面の一部のみ誘電体が露出しており、その他の全面は導体膜で覆われている。なお、この例では、両端の共振器の外側に入出力電極が底面に形成された長さの短い誘電体部分が形成されている。
【0004】
上記の誘電体をプリント基板等の配線基板などの平面回路に実装できる。この実装構造については発明者らが特願平2001−216919号等で提案している。しかし、これまでの導波管型誘電体フィルタの構造では、フィルタとして必要となる減衰極を任意の帯域に発生させることができなかった。フィルタとしての選択特性を上げるためには、通過帯域の高域側あるいは低域側または双方に減衰極を得ることが必要となる。
【0005】
【発明が解決しようとする課題】
本発明は、一体構造の導波管型誘電体フィルタにおいて任意の減衰極を得る構造を提供するもので、有極型の導波管型誘電体フィルタを簡単で生産性の高い構造で実現するものである。また、波管型誘電体フィルタをプリント基板などの配線基板に形成された平面回路に実装した際に、フィルタの入出力端子と基板の信号線の不連続を極力減少させて、入出力部での電磁界の反射や放射によって引き起こされる損失を低減させるものである。
【0006】
【課題を解決するための手段】
本発明は、共振器を付加することによって、上記の課題を解決するものである。すなわち、複数の誘電体導波管が誘電体ブロックに一体に構成されてなる導波管型誘電体フィルタにおいて、誘電体ブロックにはフィルタを構成する複数の誘電体導波管が形成されるとともに、減衰極を形成するための誘電体導波管が少なくともそれらの片側に形成されてその間に入出力用の誘電体が配置され、入出力用の誘電体の底面に、一端が側端面に引き出され、分岐した他端がフィルタを構成する誘電体導波管の底面と減衰極を形成するための誘電体導波管の底面に伸びる導体ストリップによる入出力電極を具えたことに特徴を有するものである。
【0007】
【発明の実施の形態】
本発明による導波管型誘電体フィルタの基本構成要素は以下のようになる。
(1)フィルタ部を構成する複数の共振器を構成する誘電体と少なくとも一端側に配置される誘電体導波管共振器が一体に形成された誘電体ブロックで、共振器間はアイリス等で結合が調整される、
(2)その間に有極型直交入出力構造としての誘電体の底面に形成され、両側の共振器の底面に達するとともに誘電体の側端面に伸びる導体ストリップからなる入出力電極、
(3)入出力電極の両側および上記端面の入出力電極に接する部分を除く誘電体ブロックの表面を覆い、アース電位に接続される導体膜。
【0008】
入出力電極をプリント回路基板等の配線基板の信号線と接続し、配線基板からの信号が減衰極を発生する有極型入出力構造を構成する導波管共振器の共振モードと導波管フィルタ内部の共振モードに結合される。入出力電極を形成する誘電体と減衰極を発生する導波管共振器、フィルタを構成する共振器との間は、誘電体の幅を狭くすることによってフィルタと極を発生する共振器との間の結合を調整する。
【0009】
【実施例】
以下、図面を参照して、本発明の実施例について説明する。図1は、3素子の有極型入出力構造を有する本発明による導波管型誘電体フィルタの斜視図である。ほぼ直方体の誘電体ブロック11内に、3素子のフィルタを構成する共振器12A、12B、12Cが配置され、それらの間は側面から溝が形成されてできたアイリスによって結合が調整されている。この例では入力側に有極型入出力構造を構成するすなわち減衰極を得るための共振器13が配置され、その間に入出力部となる誘電体14を配置する。入出力部となる誘電体の底面には、側端面から内部に伸びて誘電体14の底面で分岐し、フィルタ部方向と減衰極を形成する共振器13まで伸ばされて終端された入力電極15、フィルタの反対側に反対側の端面に伸びる出力電極16が形成されている。
【0010】
フィルタ部および減衰極を得るための共振器と有極型入出力構造の誘電体の間の結合を調整するため、フィルタ部と有極型入出力構造の接続部の幅を狭めるために、側面から溝を形成する。また、有極型入出力構造から入力側への放射による損失を防ぐため、有極型入出力構造の入出力部の誘電体も幅を狭めてある。
【0011】
また、側端面には一部誘電体が露出した導体パターン(導波管共振器より幅が狭く露出している)が形成されている。なお、それ以外の面については導体膜で誘電体が覆われており(端面および入出力電極のある底面には誘電体が露出した部分がある)、隣接する面の導体膜は互いに接続されている。この例では、出力電極16は有極型入出力構造を介さずに形成されている。上記の入出力電極は、図2に示したように、配線基板18、19に搭載され、その表面に形成された導体ストリップによる信号線路に接続される。導体ストリップと入出力電極は1本の連続する導体ストリップとなるので、入出力部の不整合による放射を抑えることができる。
【0012】
前記先願の特願2001−216919号に記載された従来の3素子の導波管型誘電体フィルタと本発明による3素子の有極型入出力構造を有する導波管型誘電体フィルタの電気特性(伝送特性)の比較を図3に示す。この例において、本発明による導波管型誘電体フィルタは通過帯域の高域側に減衰極があり、従来のフィルタよりも減衰極付近の減衰特性が大幅に改善されていることが分かる。
【0013】
本発明の他の実施例を説明する。図4は有極型入出力構造として入力側に2段の共振器を具えたもので、構造的には図1に示したものと同じである。また図6は入出力の両側に配置したもので減衰極を多段化できる。有極型入出力構造となる共振器の形状および結合状態を調節することによって減衰極の周波数等を調整することができる。なお、フィルタを構成する共振器間の結合調整は貫通孔等によっても可能である。図5と図7は入出力電極の導体パターンの例を示すもので、図5は図4のように片側のみに減衰極を得るための共振器を付加した場合、図7は図6のように両側に配置したものである。図8は搭載する配線基板の導体パターンを示したもので、誘電体の入出力電極と配線基板のストリップ線路とを連続した同一の形状と不連続を解消したものである。なお、フィルタだけでなく、デユプレクサ等にも応用できることはいうまでもない。
【0014】
実際のサンプルとして図1に示した構造の3段のフィルタを試作した。誘電体のサイズは長さが45.5mm、幅が10.2mm、厚みが3.2mmとしたところ、3.45GHzを中心周波数とし、通過帯域の高域側に減衰極の出現するフィルタが得られた。その特性を図9に示すが、通過帯域内のリターンロス特性も良好でフィルタとして十分に利用可能であることが確認された。
【0015】
【発明の効果】
本発明の効果を列挙すると以下のようになる。
1.配線基板(プリント回路基板)上の信号線路が延長したような連続的な形で入出力導体パターンが形成されているので、信号線路に接続された底面の導体パターンによって引き起こされた導波管共振器内部の電磁界が、減衰極を発生する導波管共振器とフィルタ部の導波管共振器の基本共振モードと結合し、結果として外部回路との結合が生じるので、任意の減衰極を持つ有極型のフィルタを実現できる。
2.フィルタの入出力端子がプリント回路基板等の平面回路の信号線と同じ平面にあるため、プリント回路板の信号線とフィルタの入出力端子の連続性がよく保たれ、不連続部によって生じる高周波信号の反射を抑制することができるので、プリント基板等の配線基板に搭載でき、低損失の素子を得られる。
3.側面の導体パターンにおいて導波管共振器に比べて誘電体が露出する部分の幅が狭くなっているので、減衰極を得る共振器と共振器の基本共振モードの周波数に対しては遮断導波路となり、低損失を実現できる。
4.入出力信号線と連続性が高く、信号線が共振器底面で終端される構造を採用することにより、フィルタを搭載するプリント基板上のパターンは、底面の導体パターンの電気的終端位置が変化しないパターンならばどのようなパターンでも許容される。例えば、連続したT分岐のストリップ線路の上に本発明によるフィルタを搭載すれば、フィルタの寸法が若干変化した場合でも基板上の導体パターンを作製し直す必要がなく、利便性が高い。
【図面の簡単な説明】
【図1】 本発明の実施例を示す斜視図
【図2】 基板への搭載方法を示す斜視図
【図3】 本発明による導波管型誘電体フィルタの特性の説明図
【図4】 本発明の他の実施例を示す斜視図
【図5】 本発明の実施例を示す底面図
【図6】 本発明の他の実施例を示す斜視図
【図7】 本発明の他の実施例を示す底面図
【図8】 本発明の他の実施例を示す斜視図
【図9】 本発明による導波管型誘電体フィルタの特性の説明図
【図10】 従来の導波管型誘電体フィルタを示す斜視図
【符号の説明】
11:誘電体ブロック
12:共振器
13:有極型入出力構造(共振器)
14:入出力部
15:入力電極
16:出力電極
18、19:配線基板
[0001]
BACKGROUND OF THE INVENTION
The present invention relates to a waveguide type dielectric filter used in a high frequency region such as the GHz band, and relates to a waveguide type dielectric filter capable of obtaining a desired attenuation pole.
[0002]
[Prior art]
[Patent Document 1]
US Patent No. 5926079 [Patent Document 2]
Japanese Patent Laid-Open No. 6-177607
By coupling a plurality of dielectric waveguide resonators, various types of waveguide dielectric filters can be realized. FIG. 10 shows such a waveguide-type dielectric filter. The resonator block 21 includes three resonators 22A, 22B, and 22C, and an iris is formed between the resonators to adjust the coupling. is doing. Conductor strips extending from the bottom surfaces of the resonators 22A and 22C at the input / output ends to the end surfaces are used as the input electrode 25 and the output electrode 26, respectively. The dielectric is exposed only on both sides of the input / output electrodes and a part of the end face in contact with them, and the other entire surface is covered with a conductor film. In this example, a short dielectric portion having input / output electrodes formed on the bottom surface is formed outside the resonators at both ends.
[0004]
The above dielectric can be mounted on a planar circuit such as a printed circuit board. The inventors have proposed this mounting structure in Japanese Patent Application No. 2001-216919. However, conventional waveguide dielectric filter structures have been unable to generate an attenuation pole required as a filter in an arbitrary band. In order to improve the selection characteristics as a filter, it is necessary to obtain attenuation poles on the high band side or low band side or both of the pass band.
[0005]
[Problems to be solved by the invention]
The present invention provides a structure for obtaining an arbitrary attenuation pole in a monolithic waveguide type dielectric filter, and realizes a polarized type waveguide dielectric filter with a simple and highly productive structure. Is. In addition, when the wave tube type dielectric filter is mounted on a planar circuit formed on a printed circuit board or other wiring board, the discontinuity between the input / output terminals of the filter and the signal lines of the board is reduced as much as possible. The loss caused by the reflection and radiation of the electromagnetic field is reduced.
[0006]
[Means for Solving the Problems]
The present invention solves the above problems by adding a resonator. That is, in a waveguide type dielectric filter in which a plurality of dielectric waveguides are integrally formed in a dielectric block, a plurality of dielectric waveguides constituting the filter are formed in the dielectric block. A dielectric waveguide for forming an attenuation pole is formed on at least one side of the dielectric waveguide, and an input / output dielectric is disposed between the dielectric waveguides. One end of the dielectric waveguide is pulled out to the bottom surface of the input / output dielectric. Characterized in that the other end of the branch has an input / output electrode with a conductor strip extending to the bottom surface of the dielectric waveguide constituting the filter and the bottom surface of the dielectric waveguide to form an attenuation pole It is.
[0007]
DETAILED DESCRIPTION OF THE INVENTION
The basic components of the waveguide dielectric filter according to the present invention are as follows.
(1) A dielectric block in which a dielectric constituting a plurality of resonators constituting a filter unit and a dielectric waveguide resonator disposed at least on one end side are integrally formed. The bond is adjusted,
(2) In the meantime, an input / output electrode comprising a conductor strip formed on the bottom surface of the dielectric as a polarized orthogonal input / output structure and reaching the bottom surface of the resonator on both sides and extending to the side end surface of the dielectric;
(3) A conductor film that covers the surface of the dielectric block except for both sides of the input / output electrode and the portion of the end face that contacts the input / output electrode, and is connected to the ground potential.
[0008]
Resonance modes and waveguides of a waveguide resonator constituting a polarized input / output structure in which input / output electrodes are connected to signal lines of a wiring board such as a printed circuit board and a signal from the wiring board generates an attenuation pole Coupled to the resonant mode inside the filter. Between the resonator forming the input and output electrodes, the waveguide resonator generating the attenuation pole, and the resonator forming the filter, the filter and the resonator generating the pole are reduced by narrowing the width of the dielectric. Adjust the bond between.
[0009]
【Example】
Embodiments of the present invention will be described below with reference to the drawings. FIG. 1 is a perspective view of a waveguide type dielectric filter according to the present invention having a three-element polarized input / output structure. Resonators 12A, 12B, and 12C constituting a three-element filter are disposed in a substantially rectangular parallelepiped dielectric block 11, and the coupling is adjusted by an iris formed by forming a groove from the side. In this example, a resonator 13 for forming a polarized input / output structure, that is, an attenuation pole is arranged on the input side, and a dielectric 14 serving as an input / output unit is arranged therebetween. On the bottom surface of the dielectric serving as the input / output unit, the input electrode 15 extends from the side end surface to the inside and branches off at the bottom surface of the dielectric 14, and extends to the resonator 13 that forms the filter unit direction and the attenuation pole. An output electrode 16 extending on the opposite end face is formed on the opposite side of the filter.
[0010]
In order to adjust the coupling between the resonator for obtaining the filter part and the attenuation pole and the dielectric of the polarized input / output structure, in order to narrow the width of the connecting part of the filter part and the polarized input / output structure, Grooves are formed from In order to prevent loss due to radiation from the polarized input / output structure to the input side, the dielectric of the input / output portion of the polarized input / output structure is also narrowed.
[0011]
In addition, a conductor pattern (exposed narrower than the waveguide resonator) is formed on the side end face with a part of the dielectric exposed. The other surface is covered with a dielectric film (the end surface and the bottom surface with the input / output electrodes have exposed portions of the dielectric), and the adjacent conductive films are connected to each other. Yes. In this example, the output electrode 16 is formed without a polarized input / output structure. As shown in FIG. 2, the input / output electrodes are mounted on the wiring boards 18 and 19 and connected to a signal line by a conductor strip formed on the surface thereof. Since the conductor strip and the input / output electrode form one continuous conductor strip, radiation due to mismatch of the input / output portions can be suppressed.
[0012]
Electricity of a conventional three-element waveguide dielectric filter described in Japanese Patent Application No. 2001-216919 of the prior application and a waveguide dielectric filter having a three-element polarized input / output structure according to the present invention. A comparison of characteristics (transmission characteristics) is shown in FIG. In this example, it can be seen that the waveguide type dielectric filter according to the present invention has an attenuation pole on the high side of the pass band, and the attenuation characteristic near the attenuation pole is greatly improved as compared with the conventional filter.
[0013]
Another embodiment of the present invention will be described. FIG. 4 shows a polarized input / output structure with a two-stage resonator on the input side, and is structurally the same as that shown in FIG. Further, FIG. 6 is arranged on both the input and output sides, so that attenuation poles can be multistaged. The frequency and the like of the attenuation pole can be adjusted by adjusting the shape and coupling state of the resonator serving as the polarized input / output structure. The coupling adjustment between the resonators constituting the filter can also be performed by a through hole or the like. 5 and 7 show examples of the conductor patterns of the input / output electrodes. FIG. 5 shows a case where a resonator for obtaining an attenuation pole is added only on one side as shown in FIG. 4, and FIG. Are arranged on both sides. FIG. 8 shows a conductor pattern of a wiring board to be mounted, in which a dielectric input / output electrode and a strip line of the wiring board are continuously formed in the same shape and discontinuity is eliminated. Needless to say, the present invention can be applied not only to a filter but also to a duplexer.
[0014]
A three-stage filter having the structure shown in FIG. 1 was prototyped as an actual sample. When the dielectric size was 45.5 mm in length, 10.2 mm in width, and 3.2 mm in thickness, a filter with an attenuation pole appearing at the high frequency side of the passband with a central frequency of 3.45 GHz was obtained. The characteristics are shown in FIG. 9, and it was confirmed that the return loss characteristics in the passband were good and could be used sufficiently as a filter.
[0015]
【The invention's effect】
The effects of the present invention are listed as follows.
1. Since the input / output conductor pattern is formed in a continuous form as if the signal line on the wiring board (printed circuit board) was extended, the waveguide resonance caused by the bottom conductor pattern connected to the signal line The electromagnetic field inside the filter is coupled with the fundamental resonance mode of the waveguide resonator that generates the attenuation pole and the waveguide resonator of the filter unit, and as a result, coupling with an external circuit occurs. It is possible to realize a polarized filter with
2. Since the input / output terminals of the filter are on the same plane as the signal lines of a planar circuit such as a printed circuit board, the continuity between the signal lines of the printed circuit board and the input / output terminals of the filter is well maintained, and high-frequency signals generated by discontinuities Therefore, it can be mounted on a wiring board such as a printed board, and a low-loss element can be obtained.
3. Since the width of the portion where the dielectric is exposed in the conductor pattern on the side surface is narrower than that of the waveguide resonator, the cut-off waveguide is used for the frequency of the fundamental resonance mode of the resonator and the resonator to obtain the attenuation pole. Thus, low loss can be realized.
4). By adopting a structure that has high continuity with the input / output signal lines and the signal lines are terminated at the bottom of the resonator, the pattern on the printed circuit board on which the filter is mounted does not change the electrical termination position of the conductor pattern on the bottom Any pattern is acceptable. For example, if the filter according to the present invention is mounted on a continuous T-branch strip line, it is not necessary to re-create a conductor pattern on the substrate even when the filter dimensions are slightly changed, which is highly convenient.
[Brief description of the drawings]
FIG. 1 is a perspective view showing an embodiment of the present invention. FIG. 2 is a perspective view showing a mounting method on a substrate. FIG. 3 is an explanatory view of characteristics of a waveguide type dielectric filter according to the present invention. FIG. 5 is a bottom view showing an embodiment of the present invention. FIG. 6 is a perspective view showing another embodiment of the present invention. FIG. 7 is another embodiment of the present invention. FIG. 8 is a perspective view showing another embodiment of the present invention. FIG. 9 is an explanatory view of the characteristics of the waveguide type dielectric filter according to the present invention. FIG.
11: Dielectric block
12: Resonator
13: Polarized input / output structure (resonator)
14: Input / output section
15: Input electrode
16: Output electrode
18, 19: Wiring board

Claims (2)

複数の誘電体導波管が誘電体ブロックに一体に構成されてなる導波管型誘電体フィルタにおいて、
誘電体ブロックにはフィルタを構成する複数の誘電体導波管共振器が形成されるとともに、減衰極を形成するための誘電体導波管共振器が少なくとも片側の端部に形成され、
入出力端の導波管共振器と減衰極を形成するための誘電体導波管の間に配置された誘電体の底面に、側端面から内部に伸びて反対方向に分岐し、一方が入出力端の導波管共振器の底面に伸び、他方が減衰極形成するための導波管共振器の底面に伸びる導体ストリップによる入出力電極を具えた
ことを特徴とする導波管型誘電体フィルタ。
In a waveguide type dielectric filter in which a plurality of dielectric waveguides are integrally formed in a dielectric block,
The dielectric block is formed with a plurality of dielectric waveguide resonators constituting a filter, and a dielectric waveguide resonator for forming an attenuation pole is formed at least on one end,
The bottom surface of the dielectric placed between the waveguide resonator at the input / output end and the dielectric waveguide to form the attenuation pole extends inward from the side end surface and branches in the opposite direction, with one entering A waveguide-type dielectric comprising an input / output electrode with a conductor strip extending to the bottom surface of the waveguide resonator at the output end and the other end to the bottom surface of the waveguide resonator for forming an attenuation pole filter.
配線基板上に少なくとも一方が分岐する入出力電極と対向する導体ストリップが形成され、入出力電極が配線基板に搭載されてそれらの導体ストリップと接続される請求項1記載の導波管型誘電体フィルタ。  2. A waveguide type dielectric according to claim 1, wherein conductor strips are formed on the wiring board so as to face at least one of the branched input / output electrodes, and the input / output electrodes are mounted on the wiring board and connected to the conductor strips. filter.
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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH07277500A (en) * 1994-04-04 1995-10-24 Kouten Yoshikane Turning-over device for thin substance

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KR100586502B1 (en) * 2004-06-09 2006-06-07 학교법인 서강대학교 A dielectric ceramic filter with a metal guide-can
JP6330784B2 (en) * 2015-03-13 2018-05-30 株式会社村田製作所 Dielectric Waveguide, Dielectric Waveguide Mounting Structure, Dielectric Waveguide Filter, and Massive MIMO System
US10270147B2 (en) 2015-03-13 2019-04-23 Murata Manufacturing Co., Ltd. Dielectric waveguide, mounting structure for a dielectric waveguide, dielectric waveguide filter and massive MIMO system
CN109449546B (en) * 2018-11-08 2023-09-29 京信通信技术(广州)有限公司 Dielectric waveguide filter and input/output structure thereof
EP3912228A4 (en) 2019-01-17 2022-09-14 Kyocera International, Inc. Antenna array having antenna elements with integrated filters

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH07277500A (en) * 1994-04-04 1995-10-24 Kouten Yoshikane Turning-over device for thin substance

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