JP2003304101A - Band pass filter and shared transmitter/receiver using multiple mode dielectric resonator - Google Patents

Band pass filter and shared transmitter/receiver using multiple mode dielectric resonator

Info

Publication number
JP2003304101A
JP2003304101A JP2002107495A JP2002107495A JP2003304101A JP 2003304101 A JP2003304101 A JP 2003304101A JP 2002107495 A JP2002107495 A JP 2002107495A JP 2002107495 A JP2002107495 A JP 2002107495A JP 2003304101 A JP2003304101 A JP 2003304101A
Authority
JP
Japan
Prior art keywords
conductor wall
resonators
dielectric resonator
resonator
filter
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Withdrawn
Application number
JP2002107495A
Other languages
Japanese (ja)
Inventor
Yuji Takahashi
雄治 高橋
Tomomi Suzuki
知視 鈴木
Akira Ikeda
昌 池田
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Tokin Corp
Original Assignee
NEC Tokin Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by NEC Tokin Corp filed Critical NEC Tokin Corp
Priority to JP2002107495A priority Critical patent/JP2003304101A/en
Publication of JP2003304101A publication Critical patent/JP2003304101A/en
Withdrawn legal-status Critical Current

Links

Abstract

<P>PROBLEM TO BE SOLVED: To provide a band pass filter and shared transmitter/receiver fulfilling attenuating characteristics applying deep attenuation and low insertion loss at the same time in the neighborhood of a pass band without increasing the shape of a filter. <P>SOLUTION: In this band pass filter configured of a plurality of resonators including at least one multi-mode dielectric resonator, an inter-resonator conductor wall configuring a boundary between the multi-mode dielectric resonator and the adjacent resonator therewith is formed with slits inducing electromagnetic connection, and one of those slits is configured to pass the center of the inter-resonator conductor wall as a first rectangular slit formed in parallel with another conductor wall orthogonal to the conductor wall, and the other slit is configured as a second rectangular slit formed so as to be almost orthogonal to the first rectangular slit. <P>COPYRIGHT: (C)2004,JPO

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【発明の属する技術分野】本発明は、無線通信基地局装
置などのマイクロ波・ミリ波回路に用いられる多重モー
ド誘電体共振器を使った帯域通過フィルタおよび送受信
共用器に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a bandpass filter and a duplexer using a multimode dielectric resonator used in a microwave / millimeter wave circuit such as a radio communication base station device.

【0002】[0002]

【従来の技術】無線通信基地局装置などに用いられる帯
域通過フィルタや送受信共用器、特に受信機に用いられ
るフィルタは、他システムからの電波干渉を防止するた
め、通過帯域近傍の減衰量を深くとる必要がある。
2. Description of the Related Art A band pass filter used in a wireless communication base station device or a transmission / reception duplexer, particularly a filter used in a receiver, has a deep attenuation near the pass band in order to prevent radio wave interference from other systems. Need to take.

【0003】従来の、高い選択性を持つ多重モード誘電
体共振器を用いた帯域通過フィルタの構成例を示す。図
11は多重モード誘電体共振器を2個用い、入出力整合
用の結合棒を介して構成した3段の帯域通過フィルタを
示し、図11(a)はその斜視図、図11(b)はB-
B断面図である。
A configuration example of a conventional bandpass filter using a multimode dielectric resonator having high selectivity will be shown. FIG. 11 shows a three-stage bandpass filter using two multimode dielectric resonators and a coupling rod for input / output matching, and FIG. 11A is a perspective view thereof, and FIG. Is B-
It is a B sectional view.

【0004】図11(a)において、14は金属カバー
A、11は金属筐体A、13は多重モード誘電体共振
器、15は入出力整合用の結合棒、そして16は入出力
端子である。なお金属カバーAは分離して描かれてい
る。
In FIG. 11A, 14 is a metal cover A, 11 is a metal housing A, 13 is a multimode dielectric resonator, 15 is a coupling rod for input / output matching, and 16 is an input / output terminal. . The metal cover A is drawn separately.

【0005】図11(b)において、31は従来の共振
器間の導体壁、41は縦長スリットを示す。
In FIG. 11B, 31 is a conventional conductor wall between resonators, and 41 is a vertically elongated slit.

【0006】また、多重モード誘電体共振器を2個と、
その外側に半同軸共振器と入出力整合用の結合棒を介し
て構成した8段の帯域通過フィルタの例もある。
In addition, two multimode dielectric resonators,
There is also an example of an eight-stage bandpass filter formed outside of it with a semi-coaxial resonator and a coupling rod for input / output matching.

【0007】さらに、多重モード誘電体共振器を4個用
いて、入出力整合用の結合棒を介して構成した12段の
帯域通過フィルタの例もある。
Further, there is also an example of a 12-stage band pass filter constructed by using four multimode dielectric resonators through a coupling rod for input / output matching.

【0008】以上のような従来例の帯域通過フィルタ
は、通過帯域近傍の減衰量を深くとるために、通常はフ
ィルタ段数を増やして構成し、減衰量特性を満足させて
いた。
The conventional band-pass filter as described above is usually constructed by increasing the number of filter stages in order to deepen the attenuation amount near the pass band, thereby satisfying the attenuation characteristic.

【0009】[0009]

【発明が解決しようとする課題】従来の多重モード誘電
体共振器を用いた帯域通過フィルタでは、中心周波数を
対称とする有極化構成が困難とされ、減衰量を深くとる
ために多段構成としていた。したがって、フィルタ形状
が大きく、そして挿入損失が増大するという欠点があっ
た。
In a conventional bandpass filter using a multimode dielectric resonator, it is difficult to make a polarized structure having a center frequency symmetrical, and a multistage structure is adopted to make the attenuation deep. I was there. Therefore, there are drawbacks that the filter shape is large and the insertion loss is increased.

【0010】本発明の目的は、フィルタ形状を大きくせ
ず、通過帯域近傍において、深い減衰量を与える特性と
同時に低い挿入損失を満足できる帯域通過フィルタを提
供することにある。
It is an object of the present invention to provide a bandpass filter which does not increase the size of the filter and can satisfy the characteristics of providing a deep attenuation in the vicinity of the passband and at the same time a low insertion loss.

【0011】[0011]

【課題を解決するための手段】従来の多重モード誘電体
共振器を利用した6段の帯域通過フィルタの構成例は既
に図11に示したとおりである。このときのフィルタの
等価回路は図12のようになる。図12において、M0
1bは入出力端子と第1段または第6段のフィルタとの
結合を示し、C12b、C23b、C34b、C45
b、およびC56bは段間のキャパシタンスを示す。ま
た一点鎖線で囲まれた部分が1つの多重モード誘電体共
振器に相当している。
A configuration example of a conventional six-stage bandpass filter using a multimode dielectric resonator is as shown in FIG. The equivalent circuit of the filter at this time is as shown in FIG. In FIG. 12, M0
Reference numeral 1b indicates the coupling between the input / output terminal and the first-stage or sixth-stage filter.
b and C56b represent the capacitance between the stages. The portion surrounded by the alternate long and short dash line corresponds to one multimode dielectric resonator.

【0012】このフィルタにおいて中心周波数を対称と
する有極化は、例えば2段目と5段目の間に結合を生じ
させることで実現できることは知られている。その様子
を図6によって説明する。図6において、M11が2段
目と5段目の間の結合を示す。
It is known that the polarization in which the center frequency is made symmetric in this filter can be realized by, for example, causing coupling between the second stage and the fifth stage. This will be described with reference to FIG. In FIG. 6, M11 indicates the coupling between the second and fifth stages.

【0013】また、M01は入出力端子と第1段または
第6段のフィルタとの結合を示し、C12、C23、C
34、C45、およびC56は段間のキャパシタンスを
示す。また一点鎖線で囲まれた部分が1つの多重モード
誘電体共振器に相当している。
Further, M01 represents the coupling between the input / output terminal and the filter of the first stage or the sixth stage, and C12, C23, C
34, C45, and C56 represent interstage capacitance. The portion surrounded by the alternate long and short dash line corresponds to one multimode dielectric resonator.

【0014】本発明においては、多重モード誘電体共振
器13のそれぞれ第3の共振を磁界結合させている導体
壁を利用し、第1から第6の共振間の結合と負の結合、
すなわち電界結合を生じさせる導体壁の形状が見出され
ている。
In the present invention, the conductor walls that magnetically couple the third resonances of the multimode dielectric resonator 13 are utilized, and the coupling between the first to sixth resonances and the negative coupling,
That is, the shape of the conductor wall that causes electric field coupling has been found.

【0015】詳しくは、本発明の帯域通過フィルタは、
少なくとも1つの多重モード誘電体共振器を含む複数の
共振器を構成要素とする帯域通過フィルタであって、前
記多重モード誘電体共振器とこれに隣接する共振器との
境界をなす共振器間の導体壁には電磁界結合を誘導する
スリットが設けられ、前記スリットの1つは前記共振器
間の導体壁の中心を通り、かつこの共振器間の導体壁と
直交する他の導体壁に平行に設けられた第1の矩形のス
リットであり、前記スリットの他の1つは、前記第1の
矩形のスリットにほぼ直交するように設けられた第2の
矩形のスリットである。
More specifically, the bandpass filter of the present invention is
A bandpass filter having a plurality of resonators including at least one multimode dielectric resonator as a constituent element, wherein the resonator forms a boundary between the multimode dielectric resonator and a resonator adjacent thereto. A slit for inducing electromagnetic field coupling is provided on the conductor wall, and one of the slits passes through the center of the conductor wall between the resonators and is parallel to another conductor wall orthogonal to the conductor wall between the resonators. Is a first rectangular slit, and the other one of the slits is a second rectangular slit provided so as to be substantially orthogonal to the first rectangular slit.

【0016】また、前記第1および第2の矩形スリット
が設けられた共振器間の導体壁は2つの多重モード誘電
体共振器を対称に配置した6段の帯域通過フィルタにお
ける2つの多重モード誘電体共振器間の境界をなす導体
壁であってもよい。
The conductor wall between the resonators provided with the first and second rectangular slits has two multimode dielectrics in a six-stage bandpass filter in which two multimode dielectric resonators are symmetrically arranged. It may be a conductor wall that forms a boundary between the body resonators.

【0017】また、前記第1および第2の矩形スリット
が設けられた共振器間の導体壁は多重モード誘電体共振
器と半同軸誘電体共振器の境界をなす導体壁であっても
よい。
The conductor wall between the resonators provided with the first and second rectangular slits may be a conductor wall that forms a boundary between the multimode dielectric resonator and the semi-coaxial dielectric resonator.

【0018】また、前記第1および第2矩形のスリット
が設けられた共振器間の導体壁は多重モード誘電体共振
器とTE01δモード誘電体共振器の境界をなす導体壁
であってもよい。
Further, the conductor wall between the resonators provided with the first and second rectangular slits may be a conductor wall which forms a boundary between the multimode dielectric resonator and the TE 01δ mode dielectric resonator. .

【0019】また、本発明の送受信共用器は、本発明の
帯域通過フィルタを用いて構成することができる。
The transmission / reception duplexer of the present invention can be constructed using the bandpass filter of the present invention.

【0020】[0020]

【発明の実施の形態】以下に本発明の実施の形態を図面
に基づいて説明する。
BEST MODE FOR CARRYING OUT THE INVENTION Embodiments of the present invention will be described below with reference to the drawings.

【0021】(実施の形態1)まず、本実施の形態にお
ける多重モード誘電体共振器に用いる誘電体ブロックに
ついて説明する。図3は多重モード誘電体共振器に用い
る誘電体ブロックの形状を示す斜視図である。図3に示
すように、その形状は、ほぼ直方体の誘電体ブロックの
平行でない2つの綾部が切り取られた形状である。この
形状により、3つの共振モードが結合された3重モード
の誘電体共振器が形成され、1個の誘電体ブロックで3
段のフィルタに相当する特性が得られる。
(Embodiment 1) First, a dielectric block used in a multimode dielectric resonator according to the present embodiment will be described. FIG. 3 is a perspective view showing the shape of a dielectric block used in a multimode dielectric resonator. As shown in FIG. 3, the shape is a shape in which two non-parallel twill portions of a substantially rectangular parallelepiped dielectric block are cut off. With this shape, a triple-mode dielectric resonator in which three resonance modes are coupled is formed, and one dielectric block can form three
A characteristic equivalent to a stage filter is obtained.

【0022】図1は、本実施の形態1の帯域通過フィル
タを示す斜視図である。また、図2は、本発明における
第1の形状の共振器間の導体壁を示す断面図であり、図
1におけるA-A断面を示す。図2において、第1の矩
形スリット21は、共振器間の主結合である磁界結合を
誘導するものである。この第1の矩形スリット21にほ
ぼ直交するように、ある幅と長さで設けられた第2の矩
形スリット22は、それぞれの多重モード誘電体共振器
13の第1の共振あるいは第2の共振を結合させてい
て、その結合は主結合と負の結合を誘導させている。
FIG. 1 is a perspective view showing a bandpass filter according to the first embodiment. 2 is a cross-sectional view showing a conductor wall between the resonators of the first shape according to the present invention, which is taken along the line AA in FIG. In FIG. 2, the first rectangular slit 21 guides the magnetic field coupling which is the main coupling between the resonators. The second rectangular slit 22 provided with a certain width and length so as to be substantially orthogonal to the first rectangular slit 21 has a first resonance or a second resonance of each multimode dielectric resonator 13. Are bound together, and the bond induces a main bond and a negative bond.

【0023】その結果、既に図6に示した等価回路にお
ける結合M11が発生する。なお、図6は本実施の形態
1におけるフィルタ等価回路であり、M01は入出力端
子と第1段または第6段のフィルタとの結合を示し、C
12、C23、C34、C45、およびC56は段間の
キャパシタンスを示す。また一点鎖線で囲まれた部分が
1つの多重モード誘電体共振器に相当している。
As a result, the coupling M11 in the equivalent circuit already shown in FIG. 6 occurs. 6 is a filter equivalent circuit according to the first embodiment, and M01 indicates a coupling between the input / output terminal and the first or sixth stage filter, and C1
12, C23, C34, C45, and C56 indicate interstage capacitance. The portion surrounded by the alternate long and short dash line corresponds to one multimode dielectric resonator.

【0024】このような結合M11により、通過帯域の
中心周波数からほぼ同じ周波数間隔の位置に減衰極が生
じる。この減衰極の位置は、矩形スリット22の位置に
より変化し、また、幅d11および長さL11によって
も変化する。
Due to such coupling M11, an attenuation pole is generated at a position of substantially the same frequency interval from the center frequency of the pass band. The position of the attenuation pole changes depending on the position of the rectangular slit 22, and also changes depending on the width d11 and the length L11.

【0025】従来例の図11の共振器間の導体壁31を
本発明における第1の形状の共振器間の導体壁12に置
き換えて、本実施の形態の帯域通過フィルタが得られ
る。このときのフィルタ伝送特性(S21)を図5に示
す。ここで、従来例との特性比較を明確にするため、従
来例の特性を破線で示す。
The bandpass filter of this embodiment can be obtained by replacing the conductor wall 31 between the resonators of FIG. 11 of the conventional example with the conductor wall 12 between the resonators of the first shape according to the present invention. The filter transmission characteristic (S 21 ) at this time is shown in FIG. Here, in order to clarify the characteristic comparison with the conventional example, the characteristic of the conventional example is shown by a broken line.

【0026】図5においては、生成した減衰極により、
通過帯域の近傍において、従来例よりも深い減衰量が得
られていることが分かる。
In FIG. 5, due to the generated attenuation pole,
It can be seen that a deeper attenuation amount is obtained in the vicinity of the pass band than in the conventional example.

【0027】(実施の形態2)次に、多重モード誘電体
共振器2個とその外側に半同軸共振器を1個ずつ配置し
た形態を説明する。図7は本実施の形態2における帯域
通過フィルタを示す斜視図である。17は金属筐体B、
18は半同軸共振器、19は金属カバーBを示す。ま
た、他の図面と共通の符号(番号)は、実質的に同じ部
材を示す。
(Embodiment 2) Next, a mode in which two multimode dielectric resonators and one semi-coaxial resonator are arranged outside each of them will be described. FIG. 7 is a perspective view showing a bandpass filter according to the second embodiment. 17 is a metal casing B,
18 is a semi-coaxial resonator, and 19 is a metal cover B. Further, reference numerals (numbers) common to the other drawings indicate substantially the same members.

【0028】この形態においても、本発明における第1
形状の共振器間の導体壁12を用いることにより、通過
帯域の中心周波数から同じ周波数間隔の位置に減衰極を
生成することができる。そのフィルタ伝送特性
(S21)を図9に示す。また、比較のために、第1形
状の共振器間の導体壁12に換えて、従来の共振器間の
導体壁31を用いた場合のフィルタ伝送特性も図9に含
める。
Also in this mode, the first aspect of the present invention
By using the conductor wall 12 between the shaped resonators, it is possible to generate attenuation poles at positions having the same frequency interval from the center frequency of the pass band. The filter transmission characteristic (S 21 ) is shown in FIG. Further, for comparison, FIG. 9 also includes the filter transmission characteristics when the conventional conductor wall 31 between the resonators is used instead of the conductor wall 12 between the resonators of the first shape.

【0029】図9からは、通過帯域の両側において、従
来例よりも深い減衰特性が得られていることが分かる。
It can be seen from FIG. 9 that deeper attenuation characteristics are obtained on both sides of the pass band than in the conventional example.

【0030】(実施の形態3)さらに、多重モード誘電
体共振器4個で構成した例を説明する。図8は本実施の
形態3における帯域通過フィルタ示す斜視図である。な
お、図中の符号(番号)は、他の図面で説明したとおり
である。
(Third Embodiment) Further, an example in which four multimode dielectric resonators are used will be described. FIG. 8 is a perspective view showing a bandpass filter according to the third embodiment. The reference numerals (numbers) in the figure are as described in other drawings.

【0031】この形態においても、本発明における第1
の形状の共振器間の導体壁12を用いることにより、通
過帯域の中心周波数から等間隔の周波数位置に減衰極を
発生させることができる。そのフィルタ特性を図10に
示す。また、比較のために、第1形状の共振器間の導体
壁12に換えて、従来の共振器間の導体壁31を用いた
場合のフィルタ伝送特性も図10に含める。
Also in this embodiment, the first aspect of the present invention
By using the conductor wall 12 between the resonators having the shape described above, it is possible to generate attenuation poles at frequency positions equidistant from the center frequency of the pass band. The filter characteristic is shown in FIG. Further, for comparison, FIG. 10 also includes the filter transmission characteristics when the conductor wall 31 between the resonators of the first shape is used instead of the conductor wall 12 between the resonators of the first shape.

【0032】図10からは、通過帯域の両側において、
従来例よりも深い減衰特性が得られていることが分か
る。
From FIG. 10, on both sides of the pass band,
It can be seen that a deeper damping characteristic is obtained than in the conventional example.

【0033】以上の実施の形態においては、共振器間の
導体壁として、第1の形状の共振器間の導体壁12を用
いたが、図4に示す構造または形状によっても同様な作
用(負の結合作用)を生じさせる導体壁が実現できる。
In the above-mentioned embodiments, the conductor wall 12 between the resonators of the first shape is used as the conductor wall between the resonators, but the same action (negative effect) can be obtained by the structure or shape shown in FIG. Can be realized.

【0034】図4(a)は第2の形状を示す断面図、図
4(b)は第3の形状を示す断面図である。この場合も
減衰極の位置は、幅d22、d33、および長さL2
2、L33によって変化させることができる。
FIG. 4A is a sectional view showing the second shape, and FIG. 4B is a sectional view showing the third shape. Also in this case, the positions of the attenuation poles are the widths d22, d33 and the length L2.
2, it can be changed by L33.

【0035】ところで、多段の帯域通過フィルタにおけ
る多重モード誘電体共振器とTE01 δモード誘電体共振
器の境界をなす共振器間の導体壁においても、上記の第
1、第2、または第3の形状の共振器間の導体壁を用い
ることにより、負の結合を誘導して、中心周波数から対
称な周波数位置に減衰極を生じさせることができる。そ
の結果、通過帯域近傍において、深い減衰量特性が得ら
れる。
By the way, also in the conductor wall between the resonators that form the boundary between the multimode dielectric resonator and the TE 01 δ mode dielectric resonator in the multistage bandpass filter, the above-mentioned first, second, or third. By using the conductor wall between the resonators in the shape of, the negative coupling can be induced and the attenuation pole can be generated at the symmetrical frequency position from the center frequency. As a result, a deep attenuation amount characteristic is obtained near the pass band.

【0036】また、上記の特性の帯域通過フィルタを用
いると、容易に送受信共用器を構成することができる。
Further, by using the band pass filter having the above characteristics, a duplexer can be easily constructed.

【0037】[0037]

【発明の効果】以上説明したとおり、本発明の多重モー
ド誘電体共振器を用いた帯域通過フィルタにおいては、
基本となる構成あるいは構造を変えることなく、有極フ
ィルタにすることができる。
As described above, in the bandpass filter using the multimode dielectric resonator of the present invention,
A polar filter can be obtained without changing the basic configuration or structure.

【0038】従って、本発明よれば、段数を増やすこと
なく、通過帯域の近傍での減衰特性を深くすることが可
能となり、小型で低損失の帯域通過フィルタおよびこれ
を用いた送受信共用器を提供することができる。
Therefore, according to the present invention, it is possible to deepen the attenuation characteristics in the vicinity of the pass band without increasing the number of stages, and to provide a compact and low loss band pass filter and a transmission / reception duplexer using the same. can do.

【図面の簡単な説明】[Brief description of drawings]

【図1】実施の形態1の帯域通過フィルタを示す斜視
図。
FIG. 1 is a perspective view showing a bandpass filter according to a first embodiment.

【図2】本発明における第1の形状の共振器間の導体壁
を示す断面図。
FIG. 2 is a sectional view showing a conductor wall between resonators of a first shape according to the present invention.

【図3】多重モード誘電体共振器に用いる誘電体ブロッ
クの形状を示す斜視図。
FIG. 3 is a perspective view showing the shape of a dielectric block used in a multimode dielectric resonator.

【図4】本発明における共振器間の導体壁の形状を示す
断面図。図4(a)は第2の形状、図4(b)は第3の
形状。
FIG. 4 is a sectional view showing the shape of a conductor wall between resonators in the present invention. 4A shows the second shape, and FIG. 4B shows the third shape.

【図5】実施の形態1のフィルタ伝送特性。FIG. 5 is a filter transmission characteristic according to the first embodiment.

【図6】実施の形態1のフィルタ等価回路。FIG. 6 is a filter equivalent circuit according to the first embodiment.

【図7】実施の形態2の帯域通過フィルタの構造を示す
斜視図。
FIG. 7 is a perspective view showing a structure of a bandpass filter according to a second embodiment.

【図8】実施の形態3の帯域通過フィルタの構造を示す
斜視図。
FIG. 8 is a perspective view showing a structure of a bandpass filter according to a third embodiment.

【図9】実施の形態2のフィルタ伝送特性。FIG. 9 is a filter transmission characteristic according to the second embodiment.

【図10】実施の形態3のフィルタ伝送特性。FIG. 10 is a filter transmission characteristic according to the third embodiment.

【図11】従来の6段帯域通過フィルタの構造を示す
図。図11(a)はその斜視図、図11(b)はそのB
-B断面図。
FIG. 11 is a diagram showing a structure of a conventional 6-stage bandpass filter. 11 (a) is a perspective view thereof, and FIG. 11 (b) is a B thereof.
-B sectional view.

【図12】従来のフィルタ等価回路。FIG. 12 is a conventional filter equivalent circuit.

【符号の説明】[Explanation of symbols]

11 金属筐体A 12 本発明の共振器間の導体壁 13 多重モード誘電体共振器 14 金属カバーA 15 入出力整合用の結合棒 16 入出力端子 17 金属筐体B 18 半同軸共振器 19 金属カバーB 21 第1の矩形スリット 22 第2の矩形スリット 11 Metal case A 12 Conductor wall between resonators of the present invention 13 Multimode dielectric resonator 14 Metal cover A 15 Connecting rod for input / output matching 16 input / output terminals 17 Metal housing B 18 Semi-coaxial resonator 19 Metal cover B 21 First rectangular slit 22 Second rectangular slit

───────────────────────────────────────────────────── フロントページの続き Fターム(参考) 5J006 HA02 HC03 HC14 JA13 JA14 LA03 ND05    ─────────────────────────────────────────────────── ─── Continued front page    F term (reference) 5J006 HA02 HC03 HC14 JA13 JA14                       LA03 ND05

Claims (5)

【特許請求の範囲】[Claims] 【請求項1】 少なくとも1つの多重モード誘電体共振
器を含む複数の共振器を構成要素とする帯域通過フィル
タにおいて、前記多重モード誘電体共振器とこれに隣接
する共振器との境界をなす共振器間の導体壁には電磁界
結合を誘導するスリットが設けられ、前記スリットの1
つは前記共振器間の導体壁の中心を通り、かつこの導体
壁と直交する他の導体壁に平行に設けられた第1の矩形
スリットであり、前記スリットの他の1つは、前記第1
の矩形スリットにほぼ直交するように設けられた第2の
矩形スリットであることを特徴とする帯域通過フィル
タ。
1. A bandpass filter having a plurality of resonators including at least one multimode dielectric resonator as a constituent element, wherein a resonance forming a boundary between the multimode dielectric resonator and a resonator adjacent thereto. A slit for inducing electromagnetic field coupling is provided on the conductor wall between the chambers.
One is a first rectangular slit provided through the center of the conductor wall between the resonators and parallel to another conductor wall orthogonal to this conductor wall, and another one of the slits is the first slit. 1
Band-pass filter, which is a second rectangular slit provided so as to be substantially orthogonal to the rectangular slit of.
【請求項2】 前記共振器間の導体壁は2つの多重モー
ド誘電体共振器を対称に配置した6段の帯域通過フィル
タにおける2つの多重モード誘電体共振器間の境界をな
す導体壁であることを特徴とする請求項1に記載の帯域
通過フィルタ。
2. The conductor wall between the resonators is a conductor wall that forms a boundary between two multimode dielectric resonators in a six-stage bandpass filter in which two multimode dielectric resonators are symmetrically arranged. The bandpass filter according to claim 1, wherein:
【請求項3】 前記共振器間の導体壁は多重モード誘電
体共振器と半同軸誘電体共振器との境界をなす導体壁で
あることを特徴とする請求項1に記載の帯域通過フィル
タ。
3. The band pass filter according to claim 1, wherein the conductor wall between the resonators is a conductor wall that forms a boundary between the multimode dielectric resonator and the semi-coaxial dielectric resonator.
【請求項4】 前記共振器間の導体壁は多重モード誘電
体共振器とTE01δモード誘電体共振器との境界をなす
導体壁であることを特徴とする請求項1に記載の帯域通
過フィルタ。
4. The bandpass filter according to claim 1, wherein the conductor wall between the resonators is a conductor wall that forms a boundary between the multimode dielectric resonator and the TE 01 δ mode dielectric resonator. .
【請求項5】 請求項1、2または3に記載の帯域通過
フィルタを用いたことを特徴とする送受信共用器。
5. A transmission / reception duplexer using the bandpass filter according to claim 1. Description:
JP2002107495A 2002-04-10 2002-04-10 Band pass filter and shared transmitter/receiver using multiple mode dielectric resonator Withdrawn JP2003304101A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2002107495A JP2003304101A (en) 2002-04-10 2002-04-10 Band pass filter and shared transmitter/receiver using multiple mode dielectric resonator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2002107495A JP2003304101A (en) 2002-04-10 2002-04-10 Band pass filter and shared transmitter/receiver using multiple mode dielectric resonator

Publications (1)

Publication Number Publication Date
JP2003304101A true JP2003304101A (en) 2003-10-24

Family

ID=29391504

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2002107495A Withdrawn JP2003304101A (en) 2002-04-10 2002-04-10 Band pass filter and shared transmitter/receiver using multiple mode dielectric resonator

Country Status (1)

Country Link
JP (1) JP2003304101A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2014169434A1 (en) * 2013-04-16 2014-10-23 华为技术有限公司 Dielectric resonator, dielectric filter and manufacturing methods therefor
KR102241711B1 (en) * 2019-11-11 2021-04-20 재단법인 파동에너지 극한제어 연구단 Cover unit of ultrasonic transducer

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2014169434A1 (en) * 2013-04-16 2014-10-23 华为技术有限公司 Dielectric resonator, dielectric filter and manufacturing methods therefor
US9780428B2 (en) 2013-04-16 2017-10-03 Huawei Technologies Co., Ltd. Dielectric resonator/filter including a metallized dielectric body having a blind hole therein with a demetallized notch that is sealed by a metallized sealing part
US10320044B2 (en) 2013-04-16 2019-06-11 Huawei Technologies Co., Ltd. Method of fabricating a dielectric resonator having a sealed demetallized notch formed therein and a dielectric filter formed therefrom
US10903539B2 (en) 2013-04-16 2021-01-26 Huawei Technologies Co., Ltd. Dielectric resonator having a sealed demetallized notch formed therein, for forming a dielectric filter and a base station therefrom
KR102241711B1 (en) * 2019-11-11 2021-04-20 재단법인 파동에너지 극한제어 연구단 Cover unit of ultrasonic transducer

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