JPH05335806A - Dielectric microwave filter - Google Patents
Dielectric microwave filterInfo
- Publication number
- JPH05335806A JPH05335806A JP14134392A JP14134392A JPH05335806A JP H05335806 A JPH05335806 A JP H05335806A JP 14134392 A JP14134392 A JP 14134392A JP 14134392 A JP14134392 A JP 14134392A JP H05335806 A JPH05335806 A JP H05335806A
- Authority
- JP
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- Prior art keywords
- dielectric
- resonator
- dielectric coaxial
- coaxial resonators
- adjacent
- Prior art date
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Abstract
Description
【0001】[0001]
【産業上の利用分野】この発明は、誘電体ブロックに構
成された複数の誘電体同軸共振器を用いた誘電体マイク
ロ波フィルタに関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a dielectric microwave filter using a plurality of dielectric coaxial resonators formed in a dielectric block.
【0002】[0002]
【従来の技術】一般に、誘電体同軸共振器は、アンテナ
共用器、ディプレクサ(Diplexer)、デュプレ
クサ(Duplexer)、マルチプレクサ(Mult
iplexer)、分波器、合波器、コンバイナあるい
は送信共用器などと呼ばれるものにおいて、フィルタを
構成するのに使用されている。誘電体同軸共振器を用い
た従来のこの種の誘電体マイクロ波フィルタの一例を図
3および図4に示す。2. Description of the Related Art Generally, a dielectric coaxial resonator includes an antenna duplexer, a diplexer, a duplexer, and a multiplexer.
It is used to construct a filter in what is called an Iplexer, a demultiplexer, a multiplexer, a combiner or a transmission duplexer. An example of a conventional dielectric microwave filter of this type using a dielectric coaxial resonator is shown in FIGS. 3 and 4.
【0003】上記誘電体マイクロ波フィルタは、たとえ
ば酸化チタン系のセラミック誘電体からなる直方体形状
を有する誘電体ブロック1に、3組の誘電体同軸共振器
2,2,2を構成したものである。各誘電体同軸共振器
2は、誘電体ブロック1の一つの端面1aからそれに対
向するいま一つの端面1bに貫通する貫通孔3の内壁面
に形成された共振器電極4と、上記貫通孔3を取り囲む
誘電体ブロック1の外側面に形成されたアース電極5
と、上記各誘電体同軸共振器2が1/4波長共振器とな
るように誘電体ブロック1の上記いま一つの端面1bを
短絡端として、上記共振器電極4とアース電極5とを短
絡する短絡電極6とからなる。そして、隣り合う誘電体
同軸共振器2,2の間には、これら誘電体同軸共振器
2,2の結合を取るための結合用孔7を有する。The above-mentioned dielectric microwave filter comprises a dielectric block 1 having a rectangular parallelepiped shape made of, for example, a titanium oxide ceramic dielectric, and three sets of dielectric coaxial resonators 2, 2 and 2. . Each dielectric coaxial resonator 2 has a resonator electrode 4 formed on the inner wall surface of a through hole 3 penetrating from one end surface 1a of the dielectric block 1 to another end surface 1b opposite to the end surface 1a, and the through hole 3 described above. Electrode 5 formed on the outer surface of the dielectric block 1 surrounding the
Then, the resonator electrode 4 and the ground electrode 5 are short-circuited by using the other end face 1b of the dielectric block 1 as a short-circuit end so that each of the dielectric coaxial resonators 2 becomes a quarter wavelength resonator. It is composed of a short-circuit electrode 6. A coupling hole 7 for coupling the dielectric coaxial resonators 2 and 2 is provided between the adjacent dielectric coaxial resonators 2 and 2.
【0004】上記誘電体ブロック1の両端部分にそれぞ
れ位置する誘電体同軸共振器2の各貫通孔3には、図示
しない外部回路からの信号を上記誘電体マイクロ波フィ
ルタに入力するとともに、上記誘電体マイクロ波フィル
タから信号を取り出すために、外周部に樹脂等の誘電体
材料8を被着してなる結合棒9が挿通される(図4参
照)。これら結合棒9の一つに上記外部回路から信号が
供給され、また、いま一つの結合棒9から上記誘電体マ
イクロ波フィルタでフィルタされた信号が取り出され
る。隣り合う誘電体同軸共振器2,2間の必要な結合
は、これら誘電体同軸共振器2,2間の間隔を調節した
り、結合用孔7の寸法や形状を変えることにより調整し
ている。Signals from an external circuit (not shown) are input to the dielectric microwave filter through the through holes 3 of the dielectric coaxial resonators 2 located at both ends of the dielectric block 1, and the dielectric microwave filter is also provided. In order to extract a signal from the body microwave filter, a coupling rod 9 formed by coating a dielectric material 8 such as resin on the outer peripheral portion is inserted (see FIG. 4). A signal is supplied to the one of the coupling rods 9 from the external circuit, and the signal filtered by the dielectric microwave filter is extracted from the other coupling rod 9. Necessary coupling between the adjacent dielectric coaxial resonators 2 and 2 is adjusted by adjusting the distance between the dielectric coaxial resonators 2 and 2 or changing the size and shape of the coupling hole 7. .
【0005】[0005]
【発明が解決しようとする課題】ところで、上記従来の
誘電体マイクロ波フィルタにおいて、狭帯域特性を得る
には、結合用孔7の寸法を小さくするか、誘電体同軸共
振器2,2間の間隔を広くするかのいずれかの構造が採
用される。しかし、上記のように結合用孔7の寸法を小
さくするのは、誘電体ブロック1の成形の点から困難で
あり、また、誘電体同軸共振器2,2間の間隔を大きく
すると、誘電体マイクロ波フィルタの形状が大きくなる
という問題があった。By the way, in the above-mentioned conventional dielectric microwave filter, in order to obtain a narrow band characteristic, the size of the coupling hole 7 should be reduced, or the dielectric coaxial resonators 2 and 2 should be separated from each other. Either structure that widens the intervals is adopted. However, it is difficult to reduce the size of the coupling hole 7 as described above from the viewpoint of the molding of the dielectric block 1. Further, if the distance between the dielectric coaxial resonators 2 and 2 is increased, the dielectric material is reduced. There is a problem that the shape of the microwave filter becomes large.
【0006】本発明の目的は、製作が容易で小型の狭帯
域特性を有する誘電体マイクロ波フィルタを提供するこ
とである。It is an object of the present invention to provide a dielectric microwave filter which is easy to manufacture and has a small band characteristic.
【0007】[0007]
【課題を解決するための手段】このため、本発明は、誘
電体ブロックと、その互いに対向する面の一方から他方
に貫通する複数の貫通孔と、各貫通孔内壁面に形成され
た共振器電極と、上記誘電体ブロックの外面に形成され
たアース電極とを備え、上記共振器電極、アース電極お
よびその間に存在する上記誘電体ブロックを構成してい
る誘電体により上記誘電体ブロックに複数の誘電体同軸
共振器が構成されてなり、隣り合う誘電体同軸共振器ど
うしが互いに電磁的に結合してなる誘電体マイクロ波フ
ィルタであって、隣り合う誘電体同軸共振器の貫通孔が
上記誘電体ブロック内で互いに直交し、隣り合う誘電体
同軸共振器の各々がそれぞれ発生する電磁界が互いに直
交しており、隣り合う誘電体同軸共振器の間に配置され
て電磁界の上記直交を乱して隣り合う上記誘電体同軸共
振器を互いに電磁的に結合させる結合手段を備えている
ことを特徴としている。Therefore, according to the present invention, a dielectric block, a plurality of through holes penetrating from one of the surfaces facing each other to the other, and a resonator formed on the inner wall surface of each through hole. An electrode and an earth electrode formed on the outer surface of the dielectric block, and a plurality of dielectric electrodes are formed on the dielectric block by the dielectric constituting the resonator electrode, the earth electrode, and the dielectric block existing therebetween. A dielectric microwave filter comprising dielectric coaxial resonators, wherein adjacent dielectric coaxial resonators are electromagnetically coupled to each other. Electromagnetic fields generated by adjacent dielectric coaxial resonators that are orthogonal to each other in the body block are orthogonal to each other, and are arranged between adjacent dielectric coaxial resonators so that It is characterized in that it comprises a coupling means for electromagnetically coupling with each other the dielectric coaxial resonators adjacent to disturb.
【0008】[0008]
【作用】誘電体ブロック内で貫通孔が互いに直交する隣
り合う誘電体同軸共振器の各々がそれぞれ発生する電磁
界が互いに直交する。上記結合手段は、この電磁界の直
交を乱す。これにより、隣り合う誘電体同軸共振器が互
いに電磁的に結合する。The electromagnetic fields generated by the adjacent dielectric coaxial resonators whose through holes are orthogonal to each other in the dielectric block are orthogonal to each other. The coupling means disturbs the orthogonality of this electromagnetic field. As a result, the adjacent dielectric coaxial resonators are electromagnetically coupled to each other.
【0009】[0009]
【発明の効果】本発明によれば、隣り合う誘電体同軸共
振器の共振器電極が誘電体ブロック内で互いに直交して
いるので、隣り合う誘電体同軸共振器の間に配置された
結合手段により隣り合う誘電体同軸共振器の各々がそれ
ぞれ発生する電磁界の直交を乱しても各誘電体同軸共振
器を流れる高周波電流分布は大きな影響を受けることが
なく、各誘電体同軸共振器の無負荷Qの劣化が殆どな
い、小型で狭帯域の誘電体マイクロ波フィルタを得るこ
とができる。According to the present invention, since the resonator electrodes of the adjacent dielectric coaxial resonators are orthogonal to each other in the dielectric block, the coupling means arranged between the adjacent dielectric coaxial resonators. Therefore, even if the electromagnetic field generated by each of the adjacent dielectric coaxial resonators is disturbed, the high-frequency current distribution flowing through each dielectric coaxial resonator is not significantly affected. It is possible to obtain a small-sized and narrow-band dielectric microwave filter with almost no deterioration of the unloaded Q.
【0010】[0010]
【実施例】以下に、添付の図面を参照して本発明の実施
例を説明する。本発明にかかる誘電体マイクロ波フィル
タの一実施例の構成を図1および図2に示す。Embodiments of the present invention will be described below with reference to the accompanying drawings. The construction of one embodiment of the dielectric microwave filter according to the present invention is shown in FIGS.
【0011】上記誘電体マイクロ波フィルタは、図3お
よび図4において説明した従来の誘電体マイクロ波フィ
ルタと同様に、たとえば酸化チタン系のセラミック誘電
体からなる誘電体ブロック11(図2参照)に、図示し
ない外部回路から信号が入力する入力側の誘電体同軸共
振器12、それに隣る中間の誘電体同軸共振器12およ
びこの中間の誘電体同軸共振器12に隣り、図示しない
外部回路へ信号を出力する出力側の誘電体同軸共振器1
2の3組の誘電体同軸共振器12,12,12を構成し
たものである。上記誘電体ブロック11の6つの面に
は、アース電極15,15,…が形成され、上記誘電体
ブロック11は、これらアース電極15,15,…によ
り被覆される。The above-mentioned dielectric microwave filter is arranged in a dielectric block 11 (see FIG. 2) made of, for example, a titanium oxide-based ceramic dielectric, similarly to the conventional dielectric microwave filter described in FIGS. , A dielectric coaxial resonator 12 on the input side to which a signal is input from an external circuit (not shown), an intermediate dielectric coaxial resonator 12 adjacent to the input dielectric coaxial resonator 12, and a dielectric coaxial resonator 12 adjacent to the intermediate dielectric coaxial resonator 12 Output side dielectric coaxial resonator 1 for outputting
Two sets of two dielectric coaxial resonators 12, 12, 12 are configured. The ground electrodes 15, 15, ... Are formed on the six surfaces of the dielectric block 11, and the dielectric block 11 is covered with the ground electrodes 15, 15 ,.
【0012】3組の上記誘電体同軸共振器12,12,
12は、隣り合うものの共振器電極14どうしが誘電体
ブロック11内にて互いに直交する。Three sets of the above dielectric coaxial resonators 12, 12,
12, adjacent resonator electrodes 14 are orthogonal to each other in the dielectric block 11.
【0013】すなわち、誘電体ブロック11の一端部側
に位置する入力側の誘電体同軸共振器12は、上記誘電
体ブロック11の一つの面を開放端とする一方、この面
に対向する面を短絡端とし、その間にて上記誘電体ブロ
ック11を貫通する貫通孔13の内壁面に形成された共
振器電極14を有する。この共振器電極14は、入力側
の誘電体同軸共振器12の開放端側からギャップGをお
いて短絡端に達し、この短絡端にてその周りのアース電
極15に短絡される。このアース電極15は、短絡電極
として、上記共振器電極14をほかのアース電極15に
接続する。That is, the dielectric coaxial resonator 12 on the input side located on one end side of the dielectric block 11 has one surface of the dielectric block 11 as an open end and the surface opposite to this surface. The resonator electrode 14 is formed on the inner wall surface of the through hole 13 that penetrates the dielectric block 11 between the shorted ends. The resonator electrode 14 reaches the short-circuit end from the open end side of the dielectric coaxial resonator 12 on the input side with a gap G, and is short-circuited to the ground electrode 15 around the short-circuit end. The earth electrode 15 serves as a short-circuit electrode and connects the resonator electrode 14 to another earth electrode 15.
【0014】また、上記入力側の誘電体同軸共振器12
に隣る中間の誘電体同軸共振器12は、入力側の誘電体
同軸共振器12の上記開放端が存在する誘電体ブロック
11の面に隣る面を開放端とする一方、この面に対向す
る面を短絡端とし、その間にて誘電体ブロック11を貫
通する貫通孔13の内壁面に形成された共振器電極14
を有する。この共振器電極14は、中間の誘電体同軸共
振器12の開放端側からギャップGをおいて短絡端に達
し、この短絡端にてその周りのアース電極15に短絡さ
れる。このアース電極15は、短絡電極として、上記共
振器電極14をほかのアース電極15に接続する。The dielectric coaxial resonator 12 on the input side is also provided.
The intermediate dielectric coaxial resonator 12 adjacent to is the open end of the surface adjacent to the surface of the dielectric block 11 where the open end of the dielectric coaxial resonator 12 on the input side is present, and is opposed to this surface. The resonator electrode 14 formed on the inner wall surface of the through hole 13 penetrating the dielectric block 11 between the surfaces is
Have. The resonator electrode 14 reaches the short-circuit end from the open end side of the intermediate dielectric coaxial resonator 12 with a gap G, and is short-circuited to the surrounding ground electrode 15 at the short-circuit end. The earth electrode 15 serves as a short-circuit electrode and connects the resonator electrode 14 to another earth electrode 15.
【0015】さらに、上記中間の誘電体同軸共振器12
に隣る出力側の誘電体同軸共振器12は、入力側の誘電
体同軸共振器12の上記開放端が存在する誘電体ブロッ
ク11の面を開放端とする一方、この面に対向する面を
短絡端とし、その間にて誘電体ブロック11を貫通する
貫通孔13の内壁面に形成された共振器電極14を有す
る。この共振器電極14は、出力側の誘電体同軸共振器
12の開放端側からギャップGをおいて短絡端に達し、
この短絡端にて周りのアース電極15に短絡される。こ
のアース電極15は、短絡電極として、上記共振器電極
14をほかのアース電極15に接続する。Further, the intermediate dielectric coaxial resonator 12 is provided.
The dielectric coaxial resonator 12 on the output side adjacent to is the open end of the surface of the dielectric block 11 on which the open end of the dielectric coaxial resonator 12 on the input side is present, and the surface opposite to this surface. The resonator electrode 14 is formed on the inner wall surface of the through hole 13 penetrating the dielectric block 11 between the shorted ends. The resonator electrode 14 reaches the short-circuited end with a gap G from the open end side of the dielectric coaxial resonator 12 on the output side.
This short-circuited end is short-circuited to the surrounding earth electrode 15. The earth electrode 15 serves as a short-circuit electrode and connects the resonator electrode 14 to another earth electrode 15.
【0016】上記誘電体ブロック11は、入力側の誘電
体同軸共振器12と中間の誘電体同軸共振器12との間
に、入力側の誘電体同軸共振器12の開放端側の面から
短絡端側の面に貫通する結合用孔17を備える。同様
に、上記誘電体ブロック11は、中間の誘電体同軸共振
器12と出力側の誘電体同軸共振器12との間に、出力
側の誘電体同軸共振器12の開放端側の面から短絡端側
の面に貫通する結合用孔17を備える。The dielectric block 11 is short-circuited between the dielectric coaxial resonator 12 on the input side and the dielectric coaxial resonator 12 in the middle from the surface on the open end side of the dielectric coaxial resonator 12 on the input side. A coupling hole 17 penetrating the end surface is provided. Similarly, the dielectric block 11 is short-circuited between the intermediate dielectric coaxial resonator 12 and the output dielectric coaxial resonator 12 from the surface on the open end side of the output dielectric coaxial resonator 12. A coupling hole 17 penetrating the end surface is provided.
【0017】上記誘電体ブロック11の両端部にそれぞ
れ位置する入力側の誘電体同軸共振器12および出力側
の誘電体同軸共振器12の各貫通孔13には、上記外部
回路からの信号を図1および図2の誘電体マイクロ波フ
ィルタに入力するとともに、具体的には図示しないが、
上記誘電体マイクロ波フィルタから信号を取り出すため
に、たとえば外周部に樹脂等の誘電体材料を被着してな
る、図3および図4において説明したものと同様の、結
合棒がそれぞれ挿通される。これら結合棒の一つに外部
回路から信号が供給され、また、いま一つの結合棒から
上記誘電体マイクロ波フィルタでフィルタされた信号が
取り出される。外部回路との接続は、上記のような結合
棒のほかに、入力側の誘電体同軸共振器12もしくは出
力側の誘電体同軸共振器12の共振器電極14に接続し
たコンデンサ(図示せず。)により行うこともできる。A signal from the external circuit is shown in each of the through holes 13 of the dielectric coaxial resonator 12 on the input side and the dielectric coaxial resonator 12 on the output side located at both ends of the dielectric block 11. 1 and input to the dielectric microwave filter of FIG. 2 and not specifically shown,
In order to extract a signal from the dielectric microwave filter, a coupling rod similar to that described with reference to FIGS. 3 and 4 in which a dielectric material such as a resin is attached to the outer peripheral portion is inserted. . A signal is supplied from an external circuit to one of the coupling rods, and a signal filtered by the dielectric microwave filter is taken out from another coupling rod. For connection with an external circuit, a capacitor (not shown) connected to the resonator electrode 14 of the dielectric coaxial resonator 12 on the input side or the dielectric coaxial resonator 12 on the output side in addition to the coupling rod as described above. ).
【0018】上記のように、3組の上記誘電体同軸共振
器12,12,12の隣り合うものの共振器電極14ど
うしが誘電体ブロック11内にて互いに直交していれ
ば、誘電体ブロック11内で貫通孔13が互いに直交す
る隣り合う誘電体同軸共振器12,12の各々がそれぞ
れ発生する電磁界が互いに直交する。このように、隣り
合う誘電体同軸共振器12,12の電磁界が互いに直交
していると、このままでは、これら誘電体同軸共振器の
間には結合は生じない。As described above, if the adjacent resonator electrodes 14 of the three sets of the dielectric coaxial resonators 12, 12, 12 are orthogonal to each other in the dielectric block 11, the dielectric block 11 is formed. The electromagnetic fields generated by the adjacent dielectric coaxial resonators 12, 12 in which the through holes 13 are orthogonal to each other are orthogonal to each other. In this way, if the electromagnetic fields of the adjacent dielectric coaxial resonators 12, 12 are orthogonal to each other, no coupling will occur between the dielectric coaxial resonators as they are.
【0019】しかし、上記実施例では、誘電体ブロック
11の入力側の誘電体同軸共振器12と中間の誘電体同
軸共振器12との間に結合用孔17が存在し、この結合
用孔17の近くで、入力側の誘電体同軸共振器12およ
び中間の誘電体同軸共振器12にて発生する電磁界が乱
れる。このため、入力側の誘電体同軸共振器12の電磁
界と中間の誘電体同軸共振器12の電磁界との直交性が
乱され、入力側の誘電体同軸共振器12の電磁界と中間
の誘電体同軸共振器12の電磁界との結合が生じる。同
様に、中間の誘電体同軸共振器12と出力側の誘電体同
軸共振器12との間に存在する結合用孔17により、中
間の誘電体同軸共振器12の電磁界と出力側の誘電体同
軸共振器12の電磁界との直行性が乱され、中間の誘電
体同軸共振器12と出力側の誘電体同軸共振器12との
結合が生じる。このとき、入力側の誘電体同軸共振器1
2、中間の誘電体同軸共振器12および出力側の誘電体
同軸共振器12の各共振器電極14が誘電体ブロック内
で互いに直交しているので、上記結合用孔17により隣
り合う誘電体同軸共振器12,12の各々がそれぞれ発
生する電磁界の直交を乱しても、各誘電体同軸共振器1
2を流れる高周波電流分布は大きな影響を受けることが
ない。このため、各誘電体同軸共振器12の無負荷Qの
劣化が殆どない。However, in the above embodiment, the coupling hole 17 exists between the dielectric coaxial resonator 12 on the input side of the dielectric block 11 and the intermediate dielectric coaxial resonator 12, and the coupling hole 17 is provided. Near, the electromagnetic fields generated in the dielectric coaxial resonator 12 on the input side and the dielectric coaxial resonator 12 in the middle are disturbed. Therefore, the orthogonality between the electromagnetic field of the dielectric coaxial resonator 12 on the input side and the electromagnetic field of the intermediate dielectric coaxial resonator 12 is disturbed, and the electromagnetic field between the electromagnetic field of the dielectric coaxial resonator 12 on the input side and the intermediate field Coupling with the electromagnetic field of the dielectric coaxial resonator 12 occurs. Similarly, due to the coupling hole 17 existing between the intermediate dielectric coaxial resonator 12 and the output-side dielectric coaxial resonator 12, the electromagnetic field of the intermediate dielectric coaxial resonator 12 and the output-side dielectric material are formed. The orthogonality of the coaxial resonator 12 with the electromagnetic field is disturbed, and coupling between the dielectric coaxial resonator 12 in the middle and the dielectric coaxial resonator 12 on the output side occurs. At this time, the dielectric coaxial resonator 1 on the input side
2. Since the resonator electrodes 14 of the intermediate dielectric coaxial resonator 12 and the output-side dielectric coaxial resonator 12 are orthogonal to each other in the dielectric block, the adjacent dielectric coaxial holes are formed by the coupling holes 17. Even if the electromagnetic fields generated by the resonators 12 and 12 are disturbed, the dielectric coaxial resonators 1
The high frequency current distribution flowing through 2 is not significantly affected. Therefore, the unloaded Q of each dielectric coaxial resonator 12 is hardly deteriorated.
【0020】また、もともと結合しない隣接する誘電体
同軸共振器12,12を、上記結合用孔17により、電
磁界の直交性を乱して結合させているので、誘電体同軸
共振器12,12どうしの結合度が小さく、したがっ
て、誘電体同軸共振器12,12の間隔が小さくなり、
小型で狭帯域の誘電体マイクロ波フィルタを得ることが
できる。Further, since the adjacent dielectric coaxial resonators 12 and 12 which are originally not coupled are coupled by disturbing the orthogonality of the electromagnetic field by the coupling hole 17, the dielectric coaxial resonators 12 and 12 are coupled. The degree of coupling between them is small, and therefore the distance between the dielectric coaxial resonators 12 and 12 is small,
A compact and narrow band dielectric microwave filter can be obtained.
【0021】上記実施例において、誘電体ブロック11
には、3組に限らず、2組以上の1/4波長の誘電体同
軸共振器12もしくは1/2波長の誘電体同軸共振器が
構成されていてもよい。なお、上記誘電体ブロック11
に、複数の1/2波長誘電体同軸共振器を構成したもの
では、誘電体同軸共振器の共振器電極14の両端が、ア
ース電極との間にギャップを有する。また、上記結合用
孔17にかえて、誘電体ブロック11内に誘電体同軸共
振器12の電磁界を乱す結合用の電極を形成するように
してもよい。In the above embodiment, the dielectric block 11
Is not limited to three sets, and two or more sets of 1/4 wavelength dielectric coaxial resonators 12 or 1/2 wavelength dielectric coaxial resonators may be configured. The dielectric block 11
In addition, in the case where a plurality of half-wavelength dielectric coaxial resonators are configured, both ends of the resonator electrode 14 of the dielectric coaxial resonator have a gap with the ground electrode. Further, instead of the coupling hole 17, a coupling electrode that disturbs the electromagnetic field of the dielectric coaxial resonator 12 may be formed in the dielectric block 11.
【図1】 本発明にかかる誘電体マイクロ波フィルタの
一実施例の斜視図である。FIG. 1 is a perspective view of an example of a dielectric microwave filter according to the present invention.
【図2】 図1の誘電体マイクロ波フィルタのI−I線に
沿う断面図である。FIG. 2 is a cross-sectional view of the dielectric microwave filter of FIG. 1 taken along the line I-I.
【図3】 従来の誘電体マイクロ波フィルタの斜視図で
ある。FIG. 3 is a perspective view of a conventional dielectric microwave filter.
【図4】 図3の誘電体マイクロ波フィルタのII−II線
に沿う断面図である。4 is a sectional view taken along line II-II of the dielectric microwave filter of FIG.
11 誘電体ブロック 12 誘電体同軸共振器 13 貫通孔 14 共振器電極 15 アース電極 17 結合孔 11 Dielectric Block 12 Dielectric Coaxial Resonator 13 Through Hole 14 Resonator Electrode 15 Earth Electrode 17 Coupling Hole
Claims (1)
面の一方から他方に貫通する複数の貫通孔と、各貫通孔
内壁面に形成された共振器電極と、上記誘電体ブロック
の外面に形成されたアース電極とを備え、上記共振器電
極、アース電極およびその間に存在する上記誘電体ブロ
ックを構成している誘電体により上記誘電体ブロックに
複数の誘電体同軸共振器が構成されてなり、隣り合う誘
電体同軸共振器どうしが互いに電磁的に結合してなる誘
電体マイクロ波フィルタであって、隣り合う誘電体同軸
共振器の貫通孔が上記誘電体ブロック内で互いに直交
し、隣り合う誘電体同軸共振器の各々がそれぞれ発生す
る電磁界が互いに直交しており、隣り合う誘電体同軸共
振器の間に配置されて電磁界の上記直交を乱して隣り合
う上記誘電体同軸共振器を互いに電磁的に結合させる結
合手段を備えていることを特徴とする誘電体マイクロ波
フィルタ。1. A dielectric block, a plurality of through holes penetrating from one of the surfaces facing each other to the other, resonator electrodes formed on the inner wall surface of each through hole, and an outer surface of the dielectric block. A plurality of dielectric coaxial resonators are formed in the dielectric block by the dielectric constituting the dielectric block existing between the resonator electrode, the ground electrode and the ground electrode, A dielectric microwave filter in which adjacent dielectric coaxial resonators are electromagnetically coupled to each other, wherein through holes of adjacent dielectric coaxial resonators are orthogonal to each other in the dielectric block, and The electromagnetic fields generated by the respective body coaxial resonators are orthogonal to each other, and the electromagnetic coaxial fields are arranged between the adjacent dielectric coaxial resonators and disturb the orthogonality of the electromagnetic fields to adjoin the adjacent dielectric coaxial resonances. 1. A dielectric microwave filter, characterized in that it comprises a coupling means for electromagnetically coupling the chambers with each other.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP14134392A JP3239444B2 (en) | 1992-06-02 | 1992-06-02 | Dielectric microwave filter |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP14134392A JP3239444B2 (en) | 1992-06-02 | 1992-06-02 | Dielectric microwave filter |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH05335806A true JPH05335806A (en) | 1993-12-17 |
JP3239444B2 JP3239444B2 (en) | 2001-12-17 |
Family
ID=15289758
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP14134392A Expired - Lifetime JP3239444B2 (en) | 1992-06-02 | 1992-06-02 | Dielectric microwave filter |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP3239444B2 (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5537082A (en) * | 1993-02-25 | 1996-07-16 | Murata Manufacturing Co., Ltd. | Dielectric resonator apparatus including means for adjusting the degree of coupling |
US5929721A (en) * | 1996-08-06 | 1999-07-27 | Motorola Inc. | Ceramic filter with integrated harmonic response suppression using orthogonally oriented low-pass filter |
CN103779177A (en) * | 2014-01-21 | 2014-05-07 | 电子科技大学 | Medium resonant cavity for microwave plasma lamp |
-
1992
- 1992-06-02 JP JP14134392A patent/JP3239444B2/en not_active Expired - Lifetime
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5537082A (en) * | 1993-02-25 | 1996-07-16 | Murata Manufacturing Co., Ltd. | Dielectric resonator apparatus including means for adjusting the degree of coupling |
US5929721A (en) * | 1996-08-06 | 1999-07-27 | Motorola Inc. | Ceramic filter with integrated harmonic response suppression using orthogonally oriented low-pass filter |
CN103779177A (en) * | 2014-01-21 | 2014-05-07 | 电子科技大学 | Medium resonant cavity for microwave plasma lamp |
Also Published As
Publication number | Publication date |
---|---|
JP3239444B2 (en) | 2001-12-17 |
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