JPH07202531A - Dielectric resonator and filter device - Google Patents

Dielectric resonator and filter device

Info

Publication number
JPH07202531A
JPH07202531A JP35155593A JP35155593A JPH07202531A JP H07202531 A JPH07202531 A JP H07202531A JP 35155593 A JP35155593 A JP 35155593A JP 35155593 A JP35155593 A JP 35155593A JP H07202531 A JPH07202531 A JP H07202531A
Authority
JP
Japan
Prior art keywords
mode dielectric
dielectric resonator
resonance frequency
mode
loop
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.)
Granted
Application number
JP35155593A
Other languages
Japanese (ja)
Other versions
JP3282341B2 (en
Inventor
Shuichi Wada
秀一 和田
Makoto Abe
眞 阿部
Toru Kurisu
徹 栗栖
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.)
Murata Manufacturing Co Ltd
Original Assignee
Murata Manufacturing Co Ltd
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 Murata Manufacturing Co Ltd filed Critical Murata Manufacturing Co Ltd
Priority to JP35155593A priority Critical patent/JP3282341B2/en
Priority to DE69428509T priority patent/DE69428509T2/en
Priority to EP94120856A priority patent/EP0661770B1/en
Priority to FI946115A priority patent/FI115338B/en
Publication of JPH07202531A publication Critical patent/JPH07202531A/en
Priority to US08/534,311 priority patent/US5638037A/en
Priority to US08/638,881 priority patent/US5708404A/en
Application granted granted Critical
Publication of JP3282341B2 publication Critical patent/JP3282341B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Abstract

PURPOSE:To miniaturize the filter device having a multistage constitution by providing one of TM mode dielectric resonators constituting a double mode dielectric resonator with a hole for resonance frequency adjustment. CONSTITUTION:The end part of one TM mode dielectric resonator 3b among two orthogonal TM mode dielectric resonators 3a ana 3b is pierced by a hole 5 for resonance frequency adjustment. Though both TM mode dielectric resonators 3a and 3b have the same resonance frequency without the hole 5, the resonator 3b has the effective dielectric constant reduced to have a higher resonance frequency when the hole 5 is provided in the TM mode dielectric resonator 3b or its diameter is increased. Consequently, this fact is utilized to correct the deviation of the resonance frequency due to coupling between TM mode dielectric resonators 3a and 3b.

Description

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

【0001】[0001]

【産業上の利用分野】本発明は誘電体共振器及びフィル
タ装置に関する。具体的にいうと、フィルタ等のQeル
ープとの結合段に使用できるTM二重モードの誘電体共
振器に関する。また、当該誘電体共振器を用いた多段構
成のフィルタ装置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a dielectric resonator and a filter device. Specifically, it relates to a TM dual mode dielectric resonator that can be used in a coupling stage with a Qe loop such as a filter. Further, the present invention relates to a multistage filter device using the dielectric resonator.

【0002】[0002]

【従来の技術】図5に示すものは、2個の単モード誘電
体共振器52,53と1個の二重モード誘電体共振器5
4を金属ケース55内に納めた4段構成のフィルタ装置
51の構造を示す一部破断した斜視図である。単モード
誘電体共振器52,53は、導波管として機能する導電
性のケース56内にTMモード誘電体共振子57を収納
したものである。また、二重モード誘電体共振器54
は、2つのTMモード誘電体共振子58,59を互いに
直交するように十字形に一体化したTM二重モード誘電
体共振子60を導電性のケース61内に収納したもので
あって、例えば特開昭61−121502号公報に開示
されている。
2. Description of the Related Art FIG. 5 shows two single mode dielectric resonators 52 and 53 and one dual mode dielectric resonator 5.
4 is a partially cutaway perspective view showing the structure of a four-stage filter device 51 in which 4 is housed in a metal case 55. FIG. The single-mode dielectric resonators 52 and 53 have a TM-mode dielectric resonator 57 housed in a conductive case 56 that functions as a waveguide. In addition, the dual mode dielectric resonator 54
Is a TM double mode dielectric resonator 60 in which two TM mode dielectric resonators 58 and 59 are integrated in a cross shape so as to be orthogonal to each other, and is housed in a conductive case 61. It is disclosed in Japanese Patent Laid-Open No. 61-121502.

【0003】しかして、このフィルタ装置51において
は、両端面のコネクタ62の内面側に設けられたQeル
ープ63と初段の単モード誘電体共振器52のTMモー
ド誘電体共振子57とが磁気結合し、このTMモード誘
電体共振子57とTM二重モード誘電体共振子60とが
電磁結合し、さらに当該TM二重モード誘電体共振子6
0と最終段の単モード誘電体共振器53のTMモード誘
電体共振子57とが電磁結合し、当該TMモード誘電体
共振子57と他方のコネクタ62に設けられたQeルー
プ63とが磁気結合し、4段フィルタを構成している。
In this filter device 51, however, the Qe loop 63 provided on the inner surface side of the connector 62 on both end surfaces and the TM mode dielectric resonator 57 of the first-stage single mode dielectric resonator 52 are magnetically coupled. Then, the TM mode dielectric resonator 57 and the TM dual mode dielectric resonator 60 are electromagnetically coupled to each other, and the TM dual mode dielectric resonator 6 is further coupled.
0 and the TM mode dielectric resonator 57 of the final-stage single mode dielectric resonator 53 are electromagnetically coupled, and the TM mode dielectric resonator 57 and the Qe loop 63 provided on the other connector 62 are magnetically coupled. And constitutes a four-stage filter.

【0004】[0004]

【発明が解決しようとする課題】二重モード誘電体共振
器を用いると、2つのTMモード誘電体共振子が十字形
に一体化されているので、2つの単モード誘電体共振器
を2個並べて配置する場合に比較して、フィルタ装置を
小型化できる。従って、上記のような4段構成のフィル
タ装置においても、2つの二重モード誘電体共振器を用
いることができれば、フィルタ装置をより一層小型化す
ることが期待される。
When a dual mode dielectric resonator is used, two TM mode dielectric resonators are integrated in a cross shape, so two two single mode dielectric resonators are used. The filter device can be downsized as compared with the case where they are arranged side by side. Therefore, even in the above-described four-stage filter device, if two dual-mode dielectric resonators can be used, it is expected that the filter device will be further downsized.

【0005】しかしながら、従来の二重モード誘電体共
振器では、フィルタ装置等に組込まれていない単体の状
態で2つのTMモード誘電体共振子が等しい共振周波数
を有していた。このため、この二重モード誘電体共振器
を上記のようなフィルタ装置に組み込む場合、Qeルー
プとの結合段に配置すると、Qeループの影響を受ける
ため、Qeループと磁気結合しているTMモード誘電体
共振子とQeループと結合していないTMモード誘電体
共振子とが共振周波数のずれを発生するという問題があ
った。すなわち、両TMモード誘電体共振子の共振周波
数が異なると、いわゆるevenモードとoddモード
との各共振周波数feven,foddから両モード間の結合
係数を決めることができなくなる。
However, in the conventional dual-mode dielectric resonator, the two TM-mode dielectric resonators have the same resonance frequency in a single state not incorporated in the filter device or the like. For this reason, when this double mode dielectric resonator is incorporated in the filter device as described above, if it is arranged in the coupling stage with the Qe loop, it is affected by the Qe loop, and therefore the TM mode magnetically coupled with the Qe loop is obtained. There is a problem in that the dielectric resonator and the TM mode dielectric resonator that is not coupled to the Qe loop cause a shift in resonance frequency. That is, when the resonance frequencies of both TM mode dielectric resonators are different, it becomes impossible to determine the coupling coefficient between both modes from the resonance frequencies feven and fodd of the so-called even mode and odd mode.

【0006】このため従来にあっては、図5に示したフ
ィルタ装置のようにQeループとの結合段では単モード
誘電体共振器が用いられており、フィルタ装置をコンパ
クト化する障害となっていた。
Therefore, in the prior art, a single mode dielectric resonator is used in the coupling stage with the Qe loop as in the filter device shown in FIG. 5, which is an obstacle to making the filter device compact. It was

【0007】本発明は叙上の従来例の欠点に鑑みてなさ
れたものであって、その目的とするところは、二重モー
ド誘電体共振器の両TMモード誘電体共振子の各共振周
波数を個別に調整可能とし、一方のTMモード誘電体共
振子をQeループと結合させた状態で両TMモード誘電
体共振子の共振周波数が等しくなるように調整すること
にある。
The present invention has been made in view of the above-mentioned drawbacks of the conventional examples, and an object thereof is to determine the resonance frequencies of both TM mode dielectric resonators of a dual mode dielectric resonator. Each TM mode dielectric resonator is individually adjustable, and is adjusted so that the resonance frequencies of both TM mode dielectric resonators are equal in a state where one TM mode dielectric resonator is coupled to the Qe loop.

【0008】[0008]

【課題を解決するための手段】本発明の誘電体共振器
は、2つのTMモード誘電体共振子を互いに直交させて
一体に形成した二重モード誘電体共振子を導電性のケー
ス内に収納してなる誘電体共振器において、前記二重モ
ード誘電体共振子を構成する2つのTMモード誘電体共
振子のうち一方のTMモード誘電体共振子に共振周波数
調整用の孔を開口したことを特徴としている。
SUMMARY OF THE INVENTION In a dielectric resonator according to the present invention, a dual mode dielectric resonator in which two TM mode dielectric resonators are made orthogonal to each other and integrally formed is housed in a conductive case. In the dielectric resonator formed as described above, one of the two TM mode dielectric resonators constituting the dual mode dielectric resonator is provided with a hole for resonance frequency adjustment in the TM mode dielectric resonator. It has a feature.

【0009】また、本発明のフィルタ装置は、前記誘電
体共振器をQeループとの結合段に配置し、前記共振周
波数調整用の孔の大きさを調整することによりQeルー
プと結合したTMモード誘電体共振子とQeループと結
合していないTMモード誘電体共振子の各共振周波数が
等しくなるようにしたことを特徴としている。
Also, in the filter device of the present invention, the dielectric resonator is arranged in a coupling stage with the Qe loop, and the TM mode coupled with the Qe loop is adjusted by adjusting the size of the hole for adjusting the resonance frequency. It is characterized in that the resonance frequencies of the TM-mode dielectric resonator not coupled to the dielectric resonator and the Qe loop are made equal.

【0010】[0010]

【作用】本発明の誘電体共振器にあっては、一方のTM
モード誘電体共振子に共振周波数調整用の孔を設けてい
るので、この孔の大きさを調整することによりQeルー
プと結合したTMモード誘電体共振子とQeループと結
合していないTMモード誘電体共振子の共振周波数のず
れを調整することができる。また、直交するTMモード
誘電体共振子間の結合により発生した一方のTMモード
誘電体共振子の共振周波数のずれも同様に補正すること
ができる。
In the dielectric resonator of the present invention, one TM
Since the mode dielectric resonator has a hole for adjusting the resonance frequency, the TM mode dielectric resonator coupled to the Qe loop and the TM mode dielectric not coupled to the Qe loop are adjusted by adjusting the size of the hole. The deviation of the resonance frequency of the body resonator can be adjusted. Further, the shift of the resonance frequency of one TM mode dielectric resonator caused by the coupling between the orthogonal TM mode dielectric resonators can be similarly corrected.

【0011】このようにして、Qeループに結合させた
一方のTMモード誘電体共振子の共振周波数とQeルー
プに結合していない他方のTMモード誘電体共振子の共
振周波数とを等しくすることができるので、TM二重モ
ード誘電体共振器をフィルタ装置のQeループとの結合
段に使用することができ、多段構成のフィルタ装置をよ
り小型化することができる。
In this way, the resonance frequency of one TM mode dielectric resonator coupled to the Qe loop and the resonance frequency of the other TM mode dielectric resonator not coupled to the Qe loop can be made equal. Therefore, the TM dual mode dielectric resonator can be used in the coupling stage with the Qe loop of the filter device, and the filter device having a multi-stage configuration can be further downsized.

【0012】[0012]

【実施例】図1(a)(b)は本発明の一実施例による
二重モード誘電体共振器Aを示す斜視図及び側断面図で
ある。この二重モード誘電体共振器Aは、導波管として
機能する導電性のケース1内にTM二重モード誘電体共
振子2を一体化したものである。導電性のケース1は金
属ケース、あるいはTMモード誘電体共振子2と同時に
成形されたセラミック製ケース本体の表面に銀ペースト
等を焼き付けてアース電極を形成したものである。ま
た、TM二重モード誘電体共振子2は誘電体セラミック
スからなり、例えばTM110モードを有する2つのTM
モード誘電体共振子3a,3bを互いに直交させて一体
的に形成して十字形にしたものである。なお、ケース1
が金属製の場合には、各TMモード誘電体共振子3a,
3bの両端面に形成した銀の厚膜からなる導体層(図示
せず)によってTM二重モード誘電体共振子2はケース
1の内面に電気的及び機械的に結合されている。
1 (a) and 1 (b) are a perspective view and a side sectional view showing a dual mode dielectric resonator A according to an embodiment of the present invention. This dual-mode dielectric resonator A has a TM dual-mode dielectric resonator 2 integrated in a conductive case 1 that functions as a waveguide. The conductive case 1 is a metal case, or a ceramic case body formed at the same time as the TM mode dielectric resonator 2 is baked with silver paste or the like to form a ground electrode. The TM dual mode dielectric resonator 2 is made of a dielectric ceramic, and has two TM 110 modes, for example.
The mode dielectric resonators 3a and 3b are orthogonal to each other and integrally formed into a cross shape. Case 1
Is made of metal, each TM mode dielectric resonator 3a,
The TM double-mode dielectric resonator 2 is electrically and mechanically coupled to the inner surface of the case 1 by a conductor layer (not shown) made of a thick silver film formed on both end surfaces of 3b.

【0013】図1のTM二重モード誘電体共振子2に実
線矢印で示している電気力線はTM二重モード誘電体共
振子2内に発生するoddモードの電気力線Eoであ
り、破線矢印で示す電気力線はevenモードの電気力
線Eeである。このoddモードの電気力線Eoのみが
通過する一対の内隅部においてTM二重モード誘電体共
振子2の交差部分が溝状に切り欠かれているが、この溝
状切欠部4によってevenモードの共振振動とodd
モードの共振振動との間に結合を生じさせてあり、この
溝状切欠部4の大きさを調整することにより相互の結合
係数を調整できるようになっている。また、直交する2
つのTMモード誘電体共振子3a,3bのうち一方のT
Mモード誘電体共振子3bの端部には共振周波数調整用
孔5が貫通させられている。共振周波数調整用孔5が開
口されていない状態では、両TMモード誘電体共振子3
a,3bの共振周波数は等しいが、TMモード誘電体共
振子3bに共振周波数調整用孔5を開口し、もしくは共
振周波数調整用孔5の開口径を大きくすると、そのTM
モード誘電体共振子3bの実効誘電率が小さくなるの
で、共振周波数が高くなり、共振周波数調整用孔5の開
口径と両TMモード誘電体共振子同志の共振周波数の差
は図2に示すような関係で示される。
The lines of electric force indicated by solid arrows in the TM double-mode dielectric resonator 2 of FIG. 1 are the odd-mode lines of electric force Eo generated in the TM double-mode dielectric resonator 2 and are indicated by broken lines. The lines of electric force indicated by the arrows are lines of electric force Ee in the even mode. At the pair of inner corners through which only the odd-mode electric lines of force Eo pass, the intersecting portions of the TM double-mode dielectric resonator 2 are cut out in a groove shape. Resonance vibration and odd
Coupling is caused between the resonance vibrations of the modes, and the mutual coupling coefficient can be adjusted by adjusting the size of the groove-shaped notch 4. 2 orthogonal
T of one of the two TM mode dielectric resonators 3a and 3b
A resonance frequency adjusting hole 5 is penetrated through the end of the M-mode dielectric resonator 3b. When the resonance frequency adjusting hole 5 is not opened, both TM mode dielectric resonators 3 are formed.
Although the resonance frequencies of a and 3b are equal, when the resonance frequency adjusting hole 5 is opened in the TM mode dielectric resonator 3b or the opening diameter of the resonance frequency adjusting hole 5 is increased, the TM
Since the effective dielectric constant of the mode dielectric resonator 3b decreases, the resonance frequency increases, and the difference between the opening diameter of the resonance frequency adjusting hole 5 and the resonance frequency of both TM mode dielectric resonators is as shown in FIG. It is shown in a relationship.

【0014】このように二重モード誘電体共振器A単体
の場合には、共振周波数調整用孔5を設けるとTMモー
ド誘電体共振子3a,3b間に共振周波数のずれが発生
するが、これを利用すれば、直交するTMモード誘電体
共振子3a,3b間の結合によって発生したTMモード
誘電体共振子3a,3b間に発生した共振周波数のずれ
を補正することができる。また、一方のTMモード誘電
体共振子、例えば3aをQeループと磁気結合させた場
合にも、当該磁気結合のためTMモード誘電体共振子3
aに共振周波数のシフトが発生し、その共振周波数が大
きくなるが、他方のTMモード誘電体共振子、例えば3
bに共振周波数調整用孔5を設けることによりTMモー
ド誘電体共振子3bの共振周波数も大きくでき、共振周
波数調整用孔5の開口径を調整することによりQeルー
プと結合したTMモード誘電体共振子3aとQeループ
と結合していないTMモード誘電体共振子3bとの各共
振周波数を等しくできる。
As described above, in the case of the dual mode dielectric resonator A alone, when the resonance frequency adjusting hole 5 is provided, the resonance frequency shift occurs between the TM mode dielectric resonators 3a and 3b. By using, it is possible to correct the deviation of the resonance frequency generated between the TM mode dielectric resonators 3a and 3b caused by the coupling between the orthogonal TM mode dielectric resonators 3a and 3b. Also, when one TM mode dielectric resonator, for example, 3a is magnetically coupled to the Qe loop, the TM mode dielectric resonator 3 is magnetically coupled.
The resonance frequency shifts in a and the resonance frequency increases, but the other TM mode dielectric resonator, for example, 3
By providing the resonance frequency adjusting hole 5 in b, the resonance frequency of the TM mode dielectric resonator 3b can be increased, and by adjusting the opening diameter of the resonance frequency adjusting hole 5, the TM mode dielectric resonance coupled with the Qe loop is obtained. The resonance frequencies of the child 3a and the TM mode dielectric resonator 3b that is not coupled to the Qe loop can be made equal.

【0015】溝状切欠部4の深さないし大きさを変える
と、両TMモード誘電体共振子3a,3b同志の結合係
数を変化させることができるが、このとき両TMモード
誘電体共振子3a,3bの共振周波数が等しくなるよう
に調整されていると、evenモードの共振周波数fev
enとoddモードの共振周波数foddとから結合係数を
決めることができる。
By changing the depth or size of the groove-shaped notch 4, the coupling coefficient of both TM mode dielectric resonators 3a and 3b can be changed. At this time, both TM mode dielectric resonators 3a. , 3b are adjusted to have the same resonance frequency, the even mode resonance frequency fev
The coupling coefficient can be determined from en and the resonance frequency fodd of the odd mode.

【0016】図3は本発明に係る4段構成のフィルタ装
置Bを示す一部破断した斜視部、図4はその主要部の構
成を示す斜視図である。金属ケース11内には図1及び
図2のような構造の二重モード誘電体共振器A1,A2
を2個並べて納めてあり、いずれの二重モード誘電体共
振器A1,A2も水平方向を向いたTMモード誘電体共
振子3aと両端のコネクタ12の内面側に設けられたQ
eループ13とが磁気結合している。また、両二重モー
ド誘電体共振器A1,A2間にはストライプ状のスリッ
ト14を有する電極パターンを設けた仕切り板15が設
けられており、当該仕切り板15によって両二重モード
誘電体共振器A1,A2の鉛直方向を向いたTMモード
誘電体共振子3b,3b同志が互いに電界結合してい
る。
FIG. 3 is a partially broken perspective view showing a filter device B having a four-stage structure according to the present invention, and FIG. 4 is a perspective view showing the structure of the main part thereof. In the metal case 11, the dual mode dielectric resonators A1 and A2 having the structure as shown in FIGS.
2 of the dual mode dielectric resonators A1 and A2 are arranged side by side, and the Q mode provided on the inner surface side of the connector 12 at both ends and the TM mode dielectric resonator 3a oriented horizontally.
The e-loop 13 is magnetically coupled. Further, a partition plate 15 provided with an electrode pattern having stripe-shaped slits 14 is provided between the dual mode dielectric resonators A1 and A2. TM mode dielectric resonators 3b and 3b oriented in the vertical direction of A1 and A2 are electrically coupled to each other.

【0017】このようにQeループ13との結合段に二
重モード誘電体共振器A1,A2を配置した場合には、
Qeループ13と結合しているTMモード誘電体共振子
3aの共振周波数が影響を受けるが、このフィルタ装置
Bでは、共振周波数調整用孔5の開口径を調整すること
によりQeループ13と結合していないTMモード誘電
体共振子3bとQeループ13と結合しているTMモー
ド誘電体共振子3aとの共振周波数が等しくなるように
調整されている。従って、evenモードの共振周波数
fevenとoddモードの共振周波数foddとから結合係
数が所望値となるよう調整できる。従って、二重モード
誘電体共振器をQeループとの結合段にも使用可能とな
り、フィルタ装置を小型軽量化することができる。
When the dual mode dielectric resonators A1 and A2 are arranged in the coupling stage with the Qe loop 13 as described above,
The resonance frequency of the TM mode dielectric resonator 3a coupled to the Qe loop 13 is affected, but in this filter device B, the resonance frequency adjusting hole 5 is adjusted to adjust the resonance frequency to be coupled to the Qe loop 13. The resonance frequencies of the TM mode dielectric resonator 3b that is not connected and the TM mode dielectric resonator 3a that is coupled to the Qe loop 13 are adjusted to be equal. Therefore, it is possible to adjust the coupling coefficient to a desired value from the even mode resonance frequency feven and the odd mode resonance frequency fodd. Therefore, the dual-mode dielectric resonator can be used also in the coupling stage with the Qe loop, and the filter device can be reduced in size and weight.

【0018】[0018]

【発明の効果】本発明によれば、一方のTMモード誘電
体共振子に設けた共振周波数調整用の孔により当該TM
モード誘電体共振子の共振周波数を補正することができ
る。従って、Qeループに結合したTMモード誘電体共
振子とQeループに結合していないTMモード誘電体共
振子の各共振周波数を等しくすることができ、TM二重
モード誘電体共振器をフィルタ装置のQeループとの結
合段に使用することが可能になる。よって、多段構成の
フィルタ装置をより小型化することができる。
According to the present invention, the TM-mode dielectric resonator is provided with a hole for adjusting the resonance frequency.
The resonance frequency of the mode dielectric resonator can be corrected. Therefore, the resonance frequencies of the TM mode dielectric resonator coupled to the Qe loop and the TM mode dielectric resonator not coupled to the Qe loop can be equalized, and the TM dual mode dielectric resonator can be used as a filter device. It can be used in a coupling stage with a Qe loop. Therefore, it is possible to further reduce the size of the multi-stage filter device.

【0019】また、共振周波数調整用孔により、直交す
るTMモード誘電体共振子間の結合により生じた両TM
モード誘電体共振子間の共振周波数のずれも同様に補正
することができる。
The resonance frequency adjusting holes are used to form both TMs produced by coupling between orthogonal TM mode dielectric resonators.
The shift of the resonance frequency between the mode dielectric resonators can be similarly corrected.

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

【図1】(a)(b)は本発明の一実施例による誘電体
共振器を示す斜視図及び側断面図である。
1A and 1B are a perspective view and a side sectional view showing a dielectric resonator according to an embodiment of the present invention.

【図2】TMモード誘電体共振子に設けた孔の開口径と
両TMモード誘電体共振子間の共振周波数の差との関係
を示す図である。
FIG. 2 is a diagram showing a relationship between an opening diameter of a hole provided in a TM mode dielectric resonator and a difference in resonance frequency between both TM mode dielectric resonators.

【図3】本発明に係る4段構成のフィルタ装置を示す一
部破断した斜視図である。
FIG. 3 is a partially cutaway perspective view showing a four-stage filter device according to the present invention.

【図4】同上のフィルタ装置における主要部の構成を示
す図である。
FIG. 4 is a diagram showing a configuration of a main part of the above filter device.

【図5】従来の4段構成のフィルタ装置を示す一部破断
した斜視図である。
FIG. 5 is a partially cutaway perspective view showing a conventional four-stage filter device.

【符号の説明】[Explanation of symbols]

A,A1,A2 二重モード誘電体共振器 B フィルタ装置 1 ケース 2 TM二重モード誘電体共振子 3a,3b TMモード誘電体共振子 4 溝状切欠部 5 共振周波数調整用孔 13 Qeループ A, A1, A2 Double mode dielectric resonator B Filter device 1 Case 2 TM Double mode dielectric resonator 3a, 3b TM mode dielectric resonator 4 Groove notch 5 Resonance frequency adjusting hole 13 Qe loop

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】 2つのTMモード誘電体共振子を互いに
直交させて一体に形成した二重モード誘電体共振子を導
電性のケース内に収納してなる誘電体共振器において、 前記二重モード誘電体共振子を構成する2つのTMモー
ド誘電体共振子のうち一方のTMモード誘電体共振子に
共振周波数調整用の孔を開口したことを特徴とする誘電
体共振器。
1. A dielectric resonator comprising a two-mode dielectric resonator in which two TM-mode dielectric resonators are formed orthogonally to each other and integrally formed, and is housed in a conductive case. A dielectric resonator, wherein one of the two TM mode dielectric resonators forming the dielectric resonator is provided with a hole for adjusting a resonance frequency in a TM mode dielectric resonator.
【請求項2】 請求項1に記載の誘電体共振器をQeル
ープとの結合段に配置し、前記共振周波数調整用の孔の
大きさを調整することによりQeループと結合したTM
モード誘電体共振子とQeループと結合していないTM
モード誘電体共振子の各共振周波数が等しくなるように
したことを特徴とするフィルタ装置。
2. A dielectric resonator according to claim 1, which is arranged in a coupling stage with a Qe loop, and which is coupled with the Qe loop by adjusting the size of the hole for adjusting the resonance frequency.
TM not coupled with mode dielectric resonator and Qe loop
A filter device characterized in that each resonance frequency of a mode dielectric resonator is made equal.
JP35155593A 1993-12-28 1993-12-28 Dielectric resonator and filter device Expired - Lifetime JP3282341B2 (en)

Priority Applications (6)

Application Number Priority Date Filing Date Title
JP35155593A JP3282341B2 (en) 1993-12-28 1993-12-28 Dielectric resonator and filter device
DE69428509T DE69428509T2 (en) 1993-12-28 1994-12-28 TM dual mode resonator and filter
EP94120856A EP0661770B1 (en) 1993-12-28 1994-12-28 TM dual mode dielectric resonator and filter
FI946115A FI115338B (en) 1993-12-28 1994-12-28 Dual mode dielectric TM resonator device and high frequency band pass filter device using said dual dielectric TM resonator device
US08/534,311 US5638037A (en) 1993-12-28 1995-09-27 TM dual mode dielectric resonator and filter utilizing different size resonators
US08/638,881 US5708404A (en) 1993-12-28 1996-04-25 TM dual mode dielectric resonator and filter utilizing a hole to equalize the resonators resonance frequencies

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP35155593A JP3282341B2 (en) 1993-12-28 1993-12-28 Dielectric resonator and filter device

Publications (2)

Publication Number Publication Date
JPH07202531A true JPH07202531A (en) 1995-08-04
JP3282341B2 JP3282341B2 (en) 2002-05-13

Family

ID=18418081

Family Applications (1)

Application Number Title Priority Date Filing Date
JP35155593A Expired - Lifetime JP3282341B2 (en) 1993-12-28 1993-12-28 Dielectric resonator and filter device

Country Status (1)

Country Link
JP (1) JP3282341B2 (en)

Also Published As

Publication number Publication date
JP3282341B2 (en) 2002-05-13

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