JPH05136602A - Strip line filter - Google Patents

Strip line filter

Info

Publication number
JPH05136602A
JPH05136602A JP32662291A JP32662291A JPH05136602A JP H05136602 A JPH05136602 A JP H05136602A JP 32662291 A JP32662291 A JP 32662291A JP 32662291 A JP32662291 A JP 32662291A JP H05136602 A JPH05136602 A JP H05136602A
Authority
JP
Japan
Prior art keywords
conductor
inner conductors
outer conductor
short
dielectric substrate
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
JP32662291A
Other languages
Japanese (ja)
Other versions
JP2667604B2 (en
Inventor
Moriyasu Miyazaki
守▲やす▼ 宮▲ざき▼
Osami Ishida
修己 石田
Tamotsu Sasaki
保 佐々木
Akira Yamada
朗 山田
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric 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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP3326622A priority Critical patent/JP2667604B2/en
Publication of JPH05136602A publication Critical patent/JPH05136602A/en
Application granted granted Critical
Publication of JP2667604B2 publication Critical patent/JP2667604B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Abstract

PURPOSE:To prevent the third harmonic wave by providing a groove on a dielectric substrate and bonding with an outer conductor and a continuous conductor on the surface of the groove. CONSTITUTION:Out of dielectric substrates 1a and 1b, at the position of about 1/3 of inner conductors 2a and 4a length from shorting parts 13a-15a and 13b-15b on one outer surface where outer conductors 5a and 5b are formed, grooves 12a and 12b in the direction to cross with inner conductors 2a-4a and 2b-4b are provided. On the surface of the grooves 12a and 12b, the outer conductors 5a and 5b and the continuous conductor are bonded. Thus, at the position of the grooves 12a and 12b, the interval of the inner conductors 2a-4a and the outer conductors 5a and 5b becomes narrow, an electric field becomes strong and a static capacitance becomes large. For the third harmonic wave where the inner conductors 2a-4a length becomes the about 3/4 wavelength, the electric field in the resonator becomes maximum at the position of the grooves 12a and 12b, and by the action of the static capacitance to occur at the grooves 12a and 12b, the resonance frequency becomes low.

Description

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

【0001】[0001]

【産業上の利用分野】この発明は、主としてVHF 帯、お
よびUHF 帯、およびマイクロ波帯で用いられるストリッ
プ線路フィルタの3倍波阻止手段に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a triple wave blocking means for a strip line filter used mainly in the VHF band, the UHF band and the microwave band.

【0002】[0002]

【従来の技術】図17は、例えば特公平2−11163
号公報に示されたような従来のストリップ線路フィルタ
の一例を示す概略構成図であり、図において、1a,1
bは互に対向する2枚の誘電体基板、2a〜4aは誘電
体基板1aの内面に導体膜を密着して相互に略平行に形
成された内導体、5aは誘電体基板1aの外面全面に導
体膜を密着して形成された外導体、5bは誘電体基板1
bの外面に導体膜を密着して形成された外導体、6〜8
は上記誘電体基板1a,1bと、内導体2a〜4aと、
外導体5a,5bとから成るトリプレート線路の共振
器、9aは内導体2aと内導体3a、内導体3aと内導
体4a間の中央部の誘電体基板1aを掘込んで設けられ
た結合量調整用の溝、9bは誘電体基板1bを掘込んで
設けられた結合量調整用の溝、10と11はそれらの内
導体がそれぞれ内導体2aと内導体4aの側面に直接接
続された入出力線路である。誘電体基板1aと1bは、
溝9aと溝9bが対向し重なるように重ね合され接着さ
れている。図17に示す一例では、内導体2a〜4aは
それぞれ長さが略1/4波長に設定されており、一端が
誘電体基板1a,1bの側面において外導体5a,5b
と接続され短絡部が形成されている。このため、共振器
6〜8は一端短絡他端開放の1/4波長共振器となって
いる。尚、この一例では、誘電体基板1aは内導体2a
〜4aの長手方向が誘電体基板1bより長く設定されて
おり、これら誘電体基板1aと誘電体基板1bを共振器
6〜8の短絡端側が揃うように配置することにより、内
導体2a〜4aの開放端側が露出しているものを例にと
る。
FIG. 17 shows, for example, Japanese Patent Publication No. 2-11163.
FIG. 1 is a schematic configuration diagram showing an example of a conventional stripline filter as disclosed in Japanese Patent Publication No.
b is two dielectric substrates facing each other, 2a to 4a are inner conductors formed by adhering a conductor film to the inner surface of the dielectric substrate 1a and formed substantially parallel to each other, and 5a is the entire outer surface of the dielectric substrate 1a. The outer conductor 5b is formed by closely adhering a conductor film to the dielectric substrate 1
an outer conductor formed by closely adhering a conductor film to the outer surface of b, 6 to 8
Are the dielectric substrates 1a and 1b, the inner conductors 2a to 4a,
A resonator of a triplate line composed of outer conductors 5a and 5b, and 9a is a coupling amount provided by digging the central dielectric substrate 1a between the inner conductor 2a and the inner conductor 3a and the inner conductor 3a and the inner conductor 4a. A groove for adjustment, 9b is a groove for adjusting the coupling amount provided by digging the dielectric substrate 1b, and 10 and 11 are the inlets whose inner conductors are directly connected to the side surfaces of the inner conductor 2a and the inner conductor 4a, respectively. It is an output line. The dielectric substrates 1a and 1b are
The groove 9a and the groove 9b are overlapped and bonded so as to face each other and overlap each other. In the example shown in FIG. 17, the length of each of the inner conductors 2a to 4a is set to about ¼ wavelength, and one end of each of the outer conductors 5a and 5b is located on the side surface of the dielectric substrate 1a, 1b.
And a short circuit portion is formed. Therefore, the resonators 6 to 8 are quarter-wave resonators in which one end is short-circuited and the other end is open. In this example, the dielectric substrate 1a is the inner conductor 2a.
4a are set to be longer than the dielectric substrate 1b, and by arranging the dielectric substrate 1a and the dielectric substrate 1b so that the short-circuited ends of the resonators 6 to 8 are aligned, the inner conductors 2a to 4a. Take the example where the open end side of is exposed.

【0003】動作は次のとおりである。共振器6〜8は
溝9a,9bの効果により隣接するもの相互が磁界結合
されており、その結合量は溝9a,9bの深さや隣接す
る内導体間の距離によって調整される。また、入出力の
結合量は、入出力線路10および入出力線路11の内導
体と内導体2aおよび内導体4aとの接続位置を変化さ
せて調整される。
The operation is as follows. Adjacent resonators 6 to 8 are magnetically coupled to each other due to the effect of grooves 9a and 9b, and the amount of coupling is adjusted by the depth of grooves 9a and 9b and the distance between adjacent inner conductors. Further, the input / output coupling amount is adjusted by changing the connection positions of the inner conductors of the input / output lines 10 and 11 and the inner conductors 2a and 4a.

【0004】今、内導体2a〜4aの開放端側の露出部
をトリミングしてこれら内導体の長さを調整すること
で、全ての共振器6〜8が同一の周波数、例えばf0で
共振しているものとすれば、その周波数f0では、共振
状態にある共振器6〜8は相互に強く結合しており、入
出力線路10への入射波は共振器6へ導かれ、共振器
7,8を通って入出力線路11より出力される。しかし
ながら、f0以外の周波数では、共振器6〜8相互の結
合は非常に弱く、入出力線路10あるいは11への入射
波はその電力のほとんどが反射される。このように、図
17に示したストリップ線路フィルタは帯域通過フィル
タとしての機能を有する。
Now, by trimming the exposed portions of the inner conductors 2a to 4a on the open end side and adjusting the lengths of these inner conductors, all the resonators 6 to 8 resonate at the same frequency, for example, f0. At that frequency f0, the resonators 6 to 8 in the resonance state are strongly coupled to each other, the incident wave to the input / output line 10 is guided to the resonator 6, and the resonator 7, It is output from the input / output line 11 through the signal line 8. However, at frequencies other than f0, the mutual coupling of the resonators 6 to 8 is very weak, and most of the power of the incident wave to the input / output line 10 or 11 is reflected. Thus, the strip line filter shown in FIG. 17 has a function as a band pass filter.

【0005】また、この一例では、共振器6〜8は周波
数f0で共振するように内導体長が約1/4波長に設定
されている。このため、f0の3倍の周波数3f0にお
いて内導体長が約3/4波長となり共振器6〜8は再び
共振する。したがって、図17のストリップ線路フィル
タは、図18に示すように周波数f0の基本波の他に3
f0の3倍高調波も通過させる性質をもつ。このため図
17のフィルタをマイクロ波電力増幅器と組み合わせて
使用する場合には、電力増幅器が通常のスプリアスとし
て発信する3倍高調波を阻止するための手段を、別途施
す必要がある。
Further, in this example, the resonators 6 to 8 have the inner conductor length set to about 1/4 wavelength so as to resonate at the frequency f0. Therefore, at a frequency 3f0 that is three times f0, the inner conductor length becomes about 3/4 wavelength, and the resonators 6 to 8 resonate again. Therefore, as shown in FIG. 18, the stripline filter of FIG.
It also has the property of passing the triple harmonic of f0. For this reason, when the filter of FIG. 17 is used in combination with the microwave power amplifier, it is necessary to separately provide a means for blocking the third harmonic generated by the power amplifier as a normal spurious.

【0006】[0006]

【発明が解決しようとする課題】従来のストリップ線路
フィルタは以上のように構成されているので、共振器6
〜8は周波数f0で内導体長が約1/4波長となり共振
する他、f0の3倍の周波数3f0においても内導体長
が約3/4波長となり再び共振する。このため、周波数
f0の基本波の他に3f0の3倍高調波も通過さてしま
うという問題点があった。
Since the conventional strip line filter is constructed as described above, the resonator 6
˜8, the inner conductor length resonates at about 1/4 wavelength at frequency f0, and resonates again at about 3/4 wavelength at 3f0, which is three times f0. Therefore, there is a problem that, in addition to the fundamental wave of the frequency f0, the triple harmonic of 3f0 also passes through.

【0007】本発明は上記のような問題点を解決するた
めになされたもので、周波数f0の基本波を通過させ,
かつ、f0の3倍の周波数3f0の3倍高調波を阻止す
る機能を有するストリップ線路フィルタを得ることを目
的とする。
The present invention has been made to solve the above-mentioned problems, in which a fundamental wave of frequency f0 is passed through,
Moreover, it is an object of the present invention to obtain a strip line filter having a function of blocking a triple harmonic of a frequency 3f0 which is triple the frequency of f0.

【0008】[0008]

【課題を解決するための手段】第1の発明に係るストリ
ップ線路フィルタは、誘電体基板1a,1bのうち少な
くとも外導体が形成された一枚の外面の、短絡部13a
〜15a,13b〜15bから上記内導体2a〜4a長
の約1/3の位置に上記内導体2a〜4a,2b〜4b
と交差する方向の溝12a,12bを設け、かつ上記溝
12a,12bの表面に上記外導体と連続する導体を密
着した。
A stripline filter according to a first aspect of the present invention is a short-circuit portion 13a of one outer surface of a dielectric substrate 1a, 1b on which at least an outer conductor is formed.
.About.15a, 13b to 15b to the inner conductors 2a to 4a, 2b to 4b at positions of about 1/3 of the length of the inner conductors 2a to 4a.
Grooves 12a and 12b are formed in a direction intersecting with, and conductors continuous with the outer conductor are adhered to the surfaces of the grooves 12a and 12b.

【0009】第2の発明に係るストリップ線路フィルタ
は、誘電体基板1a,1bのうち少なくとも外導体が形
成された一枚の外面の、短絡部13a〜15a,13b
〜15bから上記内導体2a〜4a長の約2/3の位置
に上記内導体2a〜4a,2b〜4bと交差する方向の
溝16a,16bを設け、かつ上記溝16a,16bの
表面に上記外導体と連続する導体を密着した。
In the strip line filter according to the second invention, the short-circuited portions 13a to 15a, 13b on one outer surface of the dielectric substrate 1a, 1b on which at least the outer conductor is formed.
.About.15b to about 2/3 of the length of the inner conductors 2a to 4a, grooves 16a and 16b in a direction intersecting with the inner conductors 2a to 4a and 2b to 4b are provided, and the grooves 16a and 16b are provided on the surfaces thereof. The outer conductor and the continuous conductor were adhered.

【0010】第3の発明に係るストリップ線路フィルタ
は、内導体2a〜4a,2b〜4bの短絡部13a〜1
5a,13b〜15bから上記内導体2a〜4a長の約
1/3の位置に上記内導体2a〜4a,2b〜4bを幅
方向に延長した突起部17a,17bを設けた。
A stripline filter according to a third aspect of the present invention is a short-circuited portion 13a-1 of the inner conductors 2a-4a, 2b-4b.
Protrusions 17a and 17b, which are formed by extending the inner conductors 2a to 4a and 2b to 4b in the width direction, are provided at positions about 1/3 of the length of the inner conductors 2a to 4a from 5a and 13b to 15b.

【0011】第4の発明に係るストリップ線路フィルタ
は、内導体2a〜4a,2b〜4bの短絡部13a〜1
5a,13b〜15bから上記内導体2a〜4a長の約
2/3の位置に上記内導体2a〜4a,2b〜4bを幅
方向に延長した突起部18a,18bを設けた。
A strip line filter according to a fourth aspect of the present invention is a short-circuited portion 13a-1 of the inner conductors 2a-4a, 2b-4b.
Protrusions 18a and 18b obtained by extending the inner conductors 2a to 4a and 2b to 4b in the width direction are provided at positions ⅔ of the length of the inner conductors 2a to 4a from 5a, 13b to 15b.

【0012】第5の発明に係るストリップ線路フィルタ
は、誘電体基板1aのうちの外導体5aが形成された面
の、上記短絡部13a〜15aから内導体2a〜4a長
の約1/3の位置に上記内導体2a〜4aと交差する方
向の溝12aを設け、かつ上記溝12aの表面に上記外
導体15aと連続する導体を密着した。
In the strip line filter according to the fifth aspect of the invention, the length of the surface of the dielectric substrate 1a on which the outer conductor 5a is formed is about 1/3 of the length from the short-circuited portions 13a to 15a to the inner conductors 2a to 4a. A groove 12a is provided at a position in a direction intersecting with the inner conductors 2a to 4a, and a conductor continuous with the outer conductor 15a is adhered to the surface of the groove 12a.

【0013】第6の発明に係るストリップ線路フィルタ
は、誘電体基板1aのうちの外導体5aが形成された面
の、短絡部13a〜15aから内導体2a〜4a長の約
2/3の位置に上記内導体2a〜4aと交差する方向の
溝16aを設け、かつ上記溝16aの表面に上記外導体
5aと連続する導体を密着した。
In the strip line filter according to the sixth aspect of the present invention, the surface of the dielectric substrate 1a on which the outer conductor 5a is formed is located at about ⅔ of the length from the short-circuited portions 13a to 15a to the inner conductors 2a to 4a. A groove 16a in a direction intersecting with the inner conductors 2a to 4a is provided in the above, and a conductor continuous with the outer conductor 5a is adhered to the surface of the groove 16a.

【0014】第7の発明に係るストリップ線路フィルタ
は、内導体2a〜4aの短絡部13a〜15aから上記
内導体2a〜4a長の約1/3の位置に上記内導体2a
〜4aを幅方向に延長した突起部17aを設けた。
In the strip line filter according to the seventh invention, the inner conductor 2a is located at a position approximately 1/3 of the length of the inner conductors 2a to 4a from the short-circuited portions 13a to 15a of the inner conductors 2a to 4a.
4a to 4a are provided in the width direction to provide a protrusion 17a.

【0015】第8の発明に係るストリップ線路フィルタ
は、上記内導体2a〜4aの短絡部13a〜15aから
上記内導体2a〜4a長の約2/3の位置に内導体2a
〜4aを幅方向に延長した突起部18aを設けた。
In the strip line filter according to the eighth aspect of the invention, the inner conductor 2a is located at a position approximately ⅔ of the length of the inner conductors 2a to 4a from the short-circuited portions 13a to 15a of the inner conductors 2a to 4a.
4a to 4a are provided in the width direction to provide a protrusion 18a.

【0016】第9の発明に係るストリップ線路フィルタ
は、短絡部13a〜15aから上記内導体2a〜4a長
の約1/3の位置の上記内導体2a〜4a上に、棒状あ
るいは板状の誘電体22を上記内導体2a〜4aと交差
する方向に密着して設けた。
The strip line filter according to the ninth aspect of the present invention comprises a rod-shaped or plate-shaped dielectric on the inner conductors 2a-4a at a position approximately 1/3 of the length of the inner conductors 2a-4a from the short-circuited portions 13a-15a. The body 22 was provided in close contact with the inner conductors 2a to 4a in a direction crossing the inner conductors 2a to 4a.

【0017】第10の発明に係るストリップ線路フィル
タは、短絡部13a〜15aから内導体2a〜4a長の
約2/3の位置の上記内導体2a〜4a上に、棒状ある
いは板状の誘電体23を上記内導体2a〜4aと交差す
る方向に密着して設けた。
The stripline filter according to the tenth aspect of the present invention is a rod-shaped or plate-shaped dielectric material on the inner conductors 2a-4a at a position approximately 2/3 of the length of the inner conductors 2a-4a from the short-circuited portions 13a-15a. 23 was provided in close contact with the inner conductors 2a to 4a.

【0018】[0018]

【作用】第1の発明に係わるストリップ線路フィルタ
は、誘電体基板1a,1bのうち少なくとも外導体5
a,5bが形成された一枚の外面の、上記短絡部13a
〜15a,13b〜15bから内導体2a〜4a長の約
1/3の位置に上記内導体2a〜4a,2b〜4bと交
差する方向の溝12a,12bを設け、かつ上記溝12
a,12bの表面に上記外導体5a,5bと連続する導
体を密着したので、上記溝12a,12bの位置では上
記内導体2a〜4a,2b〜4bと上記外導体5a,5
bとの間隔が狭まり、電界が強まって静電容量が大きく
なる。このとき、上記内導体2a〜4a長が約1/4波
長になる基本波に対しては共振器内の電界が上記溝12
a,12bの位置で比較的小さいので、上記溝12a,
12bの影響は少なく共振器の共振周波数は変化しない
が、上記内導体2a〜4a長が約3/4波長になる3倍
高調波に対しては共振器内の電界が上記溝12a,12
bの位置で最大となるので、上記溝12a,12bで生
じる静電容量の作用により共振周波数が低くなる。
The strip line filter according to the first aspect of the present invention includes at least the outer conductor 5 of the dielectric substrates 1a and 1b.
The short-circuited portion 13a on the outer surface of one sheet on which a and 5b are formed.
.About.15a, 13b-15b, and grooves 12a, 12b in a direction intersecting with the inner conductors 2a-4a, 2b-4b are provided at positions of about 1/3 of the length of the inner conductors 2a-4a, and the groove 12 is provided.
Since the conductors continuous with the outer conductors 5a and 5b are adhered to the surfaces of the a and 12b, the inner conductors 2a to 4a and 2b to 4b and the outer conductors 5a and 5b are located at the positions of the grooves 12a and 12b.
The distance from b is narrowed, the electric field is strengthened, and the capacitance is increased. At this time, with respect to the fundamental wave whose lengths of the inner conductors 2a to 4a are about 1/4 wavelength, the electric field in the resonator is the groove 12
Since the positions a and 12b are relatively small, the grooves 12a,
Although the influence of 12b is small and the resonance frequency of the resonator does not change, the electric field in the resonator is affected by the electric field in the groove 12a, 12 for the third harmonic wave in which the length of the inner conductors 2a to 4a becomes about 3/4 wavelength.
Since it becomes the maximum at the position of b, the resonance frequency is lowered by the action of the electrostatic capacitance generated in the grooves 12a and 12b.

【0019】第2の発明に係わるストリップ線路フィル
タは、誘電体基板1a,1bのうち少なくとも外導体5
a,5bが形成された一枚の外面の、上記短絡部13a
〜15a,13b〜15bから内導体2a〜4a長の約
2/3の位置に内導体2a〜4a,2b〜4bと交差す
る方向の溝16a,16bを設け、かつ上記溝16a,
16bの表面に上記外導体と連続する導体を密着したの
で、上記溝16a,16bの位置では上記内導体2a〜
4a,2b〜4bと上記外導体5a,5bとの間隔が狭
まり、電界が強まって静電容量が大きくなる。このと
き、上記内導体2a〜4a長が約1/4波長になる基本
波に対しては共振器内の電界が上記溝16a,16bの
位置で大きいので、上記溝16a,16bで生じる静電
容量の作用により共振周波数は低くなるが、上記内導体
2a〜4a長が約3/4波長になる3倍高調波に対して
は共振器内の電界が上記溝16a,16bの位置でほぼ
0となるので、上記溝16a,16bの影響はなく共振
周波数は変化しない。
The stripline filter according to the second invention is at least the outer conductor 5 of the dielectric substrates 1a and 1b.
The short-circuited portion 13a on the outer surface of one sheet on which a and 5b are formed.
.About.15a, 13b to 15b, and grooves 16a and 16b in a direction intersecting with the inner conductors 2a to 4a and 2b to 4b are provided at positions approximately 2/3 of the length of the inner conductors 2a to 4a.
Since the conductor continuous with the outer conductor is adhered to the surface of 16b, the inner conductors 2a to
The distance between the outer conductors 4a, 2b-4b and the outer conductors 5a, 5b is narrowed, the electric field is strengthened, and the electrostatic capacitance is increased. At this time, since the electric field in the resonator is large at the positions of the grooves 16a and 16b with respect to the fundamental wave in which the lengths of the inner conductors 2a to 4a are about 1/4 wavelength, the static electricity generated in the grooves 16a and 16b. Although the resonance frequency is lowered by the action of the capacitance, the electric field in the resonator is almost zero at the positions of the grooves 16a and 16b for the third harmonic wave in which the length of the inner conductors 2a to 4a is about 3/4 wavelength. Therefore, the grooves 16a and 16b are not affected and the resonance frequency does not change.

【0020】第3の発明に係わるストリップ線路フィル
タは、内導体2a〜4a,2b〜4bの短絡部13a〜
15a,13b〜15bから上記内導体2a〜4a長の
約1/3の位置に上記内導体2a〜4a,2b〜4bを
幅方向に延長した突起部17a,17bを設けたので、
上記突起部17a,17bの位置では上記内導体2a〜
4a,2b〜4bの幅が広くなり上記外導体5a,5b
との間の静電容量が大きくなる。このとき、上記内導体
2a〜4a長が約1/4波長になる基本波に対しては共
振器内の電界が上記突起部17a,17bの位置で比較
的小さいので、上記突起部17a,17bの影響は少な
く共振周波数は変化しないが、上記内導体2a〜4a長
が約3/4波長になる3倍高調波に対しては共振器内の
電界が上記突起部17a,17bの位置で最大となるの
で、上記突起部17a,17bで生じる静電容量の作用
により共振周波数が低くなる。
The stripline filter according to the third aspect of the present invention comprises a short-circuit portion 13a-of the inner conductors 2a-4a, 2b-4b.
Since the inner conductors 2a to 4a and 2b to 4b are provided with the projections 17a and 17b extending in the width direction from the positions 15a and 13b to 15b at positions of about 1/3 of the length of the inner conductors 2a to 4a,
At the positions of the protrusions 17a and 17b, the inner conductors 2a to
The outer conductors 5a and 5b are widened by widening the widths of 4a and 2b to 4b.
The capacitance between and becomes large. At this time, since the electric field in the resonator is relatively small at the positions of the protrusions 17a and 17b with respect to the fundamental wave whose lengths of the inner conductors 2a to 4a are about 1/4 wavelength, the protrusions 17a and 17b are relatively small. Although the resonance frequency does not change, the electric field in the resonator is maximum at the positions of the protrusions 17a and 17b for the third harmonics in which the length of the inner conductors 2a to 4a is about 3/4 wavelength. Therefore, the resonance frequency is lowered by the action of the electrostatic capacitance generated in the protrusions 17a and 17b.

【0021】第4の発明に係わるストリップ線路フィル
タは、内導体2a〜4a,2b〜4bの短絡部13a〜
15a,13b〜15bから上記内導体2a〜4a長の
約2/3の位置に上記内導体2a〜4a,2b〜4bを
幅方向に延長した突起部18a,18bを設けたので、
上記突起部18a,18bの位置では上記内導体2a〜
4a,2b〜4bの幅が広くなり上記外導体5a,5b
との間の静電容量が大きくなる。このとき、上記内導体
2a〜4a長が約1/4波長になる基本波に対しては共
振器内の電界が上記突起部18a,18bの位置で大き
いので、上記突起部18a,18bで生じる静電容量の
作用により共振周波数は低くなるが、上記内導体2a〜
4a長が約3/4波長になる3倍高調波に対しては共振
器内の電界が上記突起部18a,18bの位置でほぼ0
となるので、上記突起部18a,18bの影響はなく共
振周波数は変化しない。
The stripline filter according to the fourth aspect of the present invention comprises a short-circuit portion 13a of the inner conductors 2a-4a and 2b-4b.
Since the inner conductors 2a to 4a and 2b to 4b are provided with the protrusions 18a and 18b extending in the width direction from the positions 15a and 13b to 15b at positions of about 2/3 of the length of the inner conductors 2a to 4a,
At the positions of the protrusions 18a and 18b, the inner conductor 2a ...
The outer conductors 5a and 5b are widened by widening the widths of 4a and 2b to 4b.
The capacitance between and becomes large. At this time, since the electric field in the resonator is large at the positions of the protrusions 18a and 18b with respect to the fundamental wave in which the lengths of the inner conductors 2a to 4a are about 1/4 wavelength, they are generated at the protrusions 18a and 18b. Although the resonance frequency is lowered due to the action of the electrostatic capacitance, the inner conductors 2a ...
For the third harmonic of which the length of 4a is about 3/4 wavelength, the electric field in the resonator is almost zero at the positions of the protrusions 18a and 18b.
Therefore, the resonance frequency does not change because there is no influence of the protrusions 18a and 18b.

【0022】第5の発明に係わるストリップ線路フィル
タは、誘電体基板1aのうちの外導体5aが形成された
面の、短絡部13a〜15aから内導体2a〜4a長の
約1/3の位置に上記内導体2a〜4aと交差する方向
の溝12aを設け、かつ溝12aの表面に外導体5aと
連続する導体を密着したので、上記溝12aの位置では
上記内導体2a〜4aと上記外導体5aとの間隔が狭ま
り、電界が強まって静電容量が大きくなる。このとき、
上記内導体2a〜4a長が約1/4波長になる基本波に
対しては共振器内の電界が上記溝12aの位置で比較的
小さいので、上記溝12aの影響は少なく共振周波数は
変化しないが、上記内導体2a〜4a長が約3/4波長
になる3倍高調波に対しては共振器内の電界が上記溝1
2aの位置で最大となるので、上記溝12aで生じる静
電容量の作用により共振周波数が低くなる。
In the strip line filter according to the fifth aspect of the present invention, a position of the dielectric substrate 1a on which the outer conductor 5a is formed is located at about 1/3 of the length from the short-circuited portions 13a to 15a to the length of the inner conductors 2a to 4a. Since a groove 12a in a direction intersecting with the inner conductors 2a to 4a is provided on the surface of the groove 12a and a conductor continuous with the outer conductor 5a is adhered to the surface of the groove 12a, at the position of the groove 12a, the inner conductors 2a to 4a and the outer conductor The space between the conductor 5a and the conductor 5a is narrowed, the electric field is strengthened, and the electrostatic capacitance is increased. At this time,
Since the electric field in the resonator is relatively small at the position of the groove 12a for the fundamental wave whose lengths of the inner conductors 2a to 4a are about 1/4 wavelength, the influence of the groove 12a is small and the resonance frequency does not change. However, the electric field in the resonator is not affected by the electric field in the resonator for the third harmonic wave in which the length of the inner conductors 2a to 4a is about 3/4 wavelength.
Since it becomes maximum at the position of 2a, the resonance frequency becomes low due to the action of the electrostatic capacitance generated in the groove 12a.

【0023】第6の発明に係わるストリップ線路フィル
タは、誘電体基板1aのうちの上記外導体5aが形成さ
れた面の、短絡部13a〜15aから上記内導体2a〜
4a長の約2/3の位置に上記内導体2a〜4aと交差
する方向の溝16aを設け、かつ、上記溝16aの表面
に外導体5aと連続する導体を密着したので、上記溝1
6aの位置では上記内導体2a〜4aと上記外導体5a
との間隔が狭まり、電界が強まって静電容量が大きくな
る。このとき、上記内導体2a〜4a長が約1/4波長
になる基本波に対しては共振器内の電界が上記溝16a
の位置で大きいので、上記溝16aで生じる静電容量の
作用により共振周波数は低くなるが、上記内導体2a〜
4a長が約3/4波長になる3倍高調波に対しては共振
器内の電界が上記突起部16aの位置でほぼ0となるの
で、上記溝16aの影響はなく共振周波数は変化しな
い。
In the strip line filter according to the sixth aspect of the invention, the short-circuited portions 13a to 15a on the surface of the dielectric substrate 1a on which the outer conductor 5a is formed are connected to the inner conductors 2a to 2a.
Since a groove 16a in a direction intersecting with the inner conductors 2a to 4a is provided at a position of about 2/3 of the length of 4a, and a conductor continuous with the outer conductor 5a is adhered to the surface of the groove 16a, the groove 1 is formed.
At the position of 6a, the inner conductors 2a to 4a and the outer conductor 5a.
The distance between and decreases, the electric field increases, and the capacitance increases. At this time, with respect to the fundamental wave whose lengths of the inner conductors 2a to 4a are about 1/4 wavelength, the electric field in the resonator is changed to the groove 16a.
, The resonance frequency is lowered by the action of the capacitance generated in the groove 16a, but the inner conductors 2a ...
As for the third harmonic having a length of 4a of about 3/4 wavelength, the electric field in the resonator becomes almost 0 at the position of the protrusion 16a, so that the groove 16a does not affect the resonance frequency.

【0024】第7の発明に係わるストリップ線路フィル
タは、内導体2a〜4aの短絡部13a〜15aから上
記内導体2a〜4a長の約1/3の位置に上記内導体2
a〜4aを幅方向に延長した突起部17aを設けたの
で、上記突起部17aの位置では上記内導体2a〜4a
の幅が広くなり上記外導体5aとの間の静電容量が大き
くなる。このとき、上記内導体2a〜4a長が約1/4
波長になる基本波に対しては共振器内の電界が上記突起
部17aの位置で比較的小さいので、上記突起部17a
の影響は少なく共振周波数は変化しないが、上記内導体
2a〜4a長が約3/4波長になる3倍高調波に対して
は共振器内の電界が上記突起部17aの位置で最大とな
るので、上記突起部17aで生じる静電容量の作用によ
り共振周波数が低くなる。
In the strip line filter according to the seventh aspect of the present invention, the inner conductor 2 is located at a position approximately 1/3 of the length of the inner conductors 2a-4a from the short-circuited portions 13a-15a of the inner conductors 2a-4a.
Since the protrusions 17a are formed by extending a to 4a in the width direction, the inner conductors 2a to 4a are located at the positions of the protrusions 17a.
Becomes wider and the capacitance between the outer conductor 5a and the outer conductor 5a becomes larger. At this time, the length of the inner conductors 2a to 4a is about 1/4.
Since the electric field in the resonator is relatively small for the fundamental wave having the wavelength at the position of the protrusion 17a, the protrusion 17a
The resonance frequency does not change, but the electric field in the resonator becomes maximum at the position of the protrusion 17a for the third harmonic wave in which the length of the inner conductors 2a to 4a is about 3/4 wavelength. Therefore, the resonance frequency is lowered by the action of the electrostatic capacitance generated in the protrusion 17a.

【0025】第8の発明に係わるストリップ線路フィル
タは、内導体2a〜4aの短絡部13a〜15aから上
記内導体2a〜4a長の約2/3の位置に上記内導体2
a〜4aを幅方向に延長した突起部18aを設けたの
で、上記突起部18aの位置では上記内導体2a〜4a
の幅が広くなり上記外導体5aとの間の静電容量が大き
くなる。このとき、上記内導体2a〜4a長が約1/4
波長になる基本波に対しては共振器内の電界が上記突起
部18aの位置で大きいので、上記突起部18aで生じ
る静電容量の作用により共振周波数は低くなるが、上記
内導体2a〜4a長が約3/4波長になる3倍高調波に
対しては共振器内の電界が上記突起部18aの位置でほ
ぼ0となるので、上記突起部18aの影響はなく共振周
波数は変化しない。
In the strip line filter according to the eighth aspect of the present invention, the inner conductor 2 is located at a position approximately ⅔ of the length of the inner conductors 2a to 4a from the short-circuited portions 13a to 15a of the inner conductors 2a to 4a.
Since the protrusions 18a are provided by extending the a to 4a in the width direction, the inner conductors 2a to 4a are located at the positions of the protrusions 18a.
Becomes wider and the capacitance between the outer conductor 5a and the outer conductor 5a becomes larger. At this time, the length of the inner conductors 2a to 4a is about 1/4.
Since the electric field in the resonator is large with respect to the fundamental wave having the wavelength at the position of the protruding portion 18a, the resonance frequency becomes low due to the action of the capacitance generated in the protruding portion 18a, but the inner conductors 2a to 4a. For the third harmonic having a length of about 3/4 wavelength, the electric field in the resonator becomes almost zero at the position of the protrusion 18a, so that the protrusion 18a has no influence and the resonance frequency does not change.

【0026】第9の発明に係わるストリップ線路フィル
タは、短絡部13a〜15aから内導体2a〜4a長の
約1/3の位置の上記内導体2a〜4a上に、棒状ある
いは板状の誘電体22を上記内導体2a〜4aと交差す
る方向に密着して設けたので、誘電体22の位置では静
電容量が大きくなる。このとき、内導体2a〜4a長が
約1/4波長になる基本波に対しては共振器内の電界が
上記誘電体22の位置で比較的小さいので、上記誘電体
22の影響は少なく共振周波数は変化しないが、上記内
導体2a〜4a長が約3/4波長になる3倍高調波に対
しては共振器内の電界が上記誘電体22位置で最大とな
るので、上記誘電体22で大きくなる静電容量の作用に
より共振周波数が低くなる。
A strip line filter according to the ninth invention is a rod-shaped or plate-shaped dielectric on the inner conductors 2a-4a at a position approximately 1/3 of the length of the inner conductors 2a-4a from the short-circuited portions 13a-15a. Since 22 is provided in close contact with the inner conductors 2a to 4a in a direction intersecting with each other, the capacitance is large at the position of the dielectric 22. At this time, since the electric field in the resonator is relatively small at the position of the dielectric 22 with respect to the fundamental wave in which the lengths of the inner conductors 2a to 4a are about 1/4 wavelength, the influence of the dielectric 22 is small and the resonance occurs. Although the frequency does not change, the electric field in the resonator becomes maximum at the position of the dielectric member 22 with respect to the third harmonic wave in which the length of the inner conductors 2a to 4a becomes about 3/4 wavelength. The resonance frequency is lowered by the action of the electrostatic capacitance which becomes large at.

【0027】第10の発明に係わるストリップ線路フィ
ルタは、短絡部13a〜15aから内導体2a〜4a長
の約2/3の位置の上記内導体2a〜4a上に、棒状あ
るいは板状の誘電体23を上記内導体2a〜4aと交差
する方向に密着して設けたので、誘電体23の位置では
静電容量が大きくなる。このとき、上記内導体2a〜4
a長が約1/4波長になる基本波に対しては共振器内の
電界が上記誘電体23の位置で大きいので、上記誘電体
23で生じる静電容量の作用により共振周波数は低くな
るが、上記内導体2a〜4a長が約3/4波長になる3
倍高調波に対しては共振器内の電界が上記誘電体23の
位置でほぼ0となるので、上記誘電体23の影響はなく
なり共振周波数は変化しない。
The strip line filter according to the tenth aspect of the present invention is a rod-shaped or plate-shaped dielectric on the inner conductors 2a-4a at a position approximately ⅔ of the length of the inner conductors 2a-4a from the short-circuited portions 13a-15a. Since 23 is provided so as to be in close contact with the inner conductors 2a to 4a, the capacitance becomes large at the position of the dielectric 23. At this time, the inner conductors 2a-4
Since the electric field in the resonator is large at the position of the dielectric 23 with respect to the fundamental wave having the length a of about 1/4 wavelength, the resonance frequency is lowered by the action of the capacitance generated in the dielectric 23. , The length of the inner conductors 2a to 4a becomes about 3/4 wavelength 3
Since the electric field in the resonator becomes almost 0 at the position of the dielectric 23 for the double harmonic, the influence of the dielectric 23 disappears and the resonance frequency does not change.

【0028】[0028]

【実施例】図1は第1の発明に係わるストリップ線路フ
ィルタの一実施例を示す概略構成図、図2は図1の実施
例の断面図である。図において、1a,1bは互に対向
する2枚の誘電体基板、2a〜4aは誘電体基板1aの
内面に導体膜を密着して相互に略平行に形成された内導
体、2b〜4bは誘電体基板1bの内面に導体膜を密着
して相互に略平行に形成された内導体、5aは誘電体基
板1aの外面全面に導体膜を密着して形成された外導
体、5bは誘電体基板1bの外面全面に導体膜を密着し
て形成された外導体、6〜8は誘電体基板1a,1b
と、内導体2a〜4a、内導体2b〜4bと、外導体5
a、5bとから成るトリプレート線路の共振器、10と
11はそれぞれ内導体2a,2b,4a,4bに内導体
が直接接続された入出力線路、12aは誘電体基板1a
の外導体5aが密着された面を内導体2a〜4aと直交
する向きに掘り込んで設けられた溝、12bは誘電体基
板1bの外導体5bが密着された面を内導体2b〜4b
と直交する向きに掘り込んで設けられた溝、13a〜1
5aと13b〜15bは短絡部である。誘電体基板1a
と1bは、内導体2aと2b、内導体3aと3b、およ
び内導体4aと4bがそれぞれ対向し重なるように重ね
合され、対向する内導体どうしが電気的に接触するよう
に接着されている。内導体2a〜4a,2b〜4bは薄
膜あるいは厚膜で形成され、フォトエッチング等により
整形される。上記内導体2a〜4aは本実施例ではそれ
ぞれ長さが所望の基本波に対して約1/4波長に設定さ
れており、内導体2a〜4a,2b〜4bは一端が誘電
体基板1a,1bの側面の短絡部13a〜15a、短絡
部13b〜15bにおいて外導体5a,5bと接続され
短絡されている。このため、共振器6〜8は一端短絡他
端開放の1/4波長共振器となっている。上記溝12a
および溝12bは短絡部13a〜15a,短絡部13b
〜15bから内導体2a〜4a,内導体2b〜4bの長
手方向にこれら内導体長の約1/3の位置に設けられて
いる。溝12a,12bの表面は延長された外導体5
a,5bにより密着され覆われている(第1の発明)。
尚図1、図2においては従来の場合と同様に、誘電体基
板1aは内導体2a〜4aの長手方向が誘電体基板1b
より長く設定され、かつ、これら誘電体基板1aと誘電
体基板1bを共振器6〜8の短絡端側が揃うように配置
することにより、内導体2a〜4aの開放端側を露出さ
せているものを例にとる。
1 is a schematic structural view showing an embodiment of a strip line filter according to the first invention, and FIG. 2 is a sectional view of the embodiment of FIG. In the figure, 1a and 1b are two dielectric substrates facing each other, and 2a to 4a are inner conductors formed by adhering a conductor film to the inner surface of the dielectric substrate 1a and being substantially parallel to each other. An inner conductor 5a formed by closely adhering a conductor film to the inner surface of the dielectric substrate 1b and formed substantially parallel to each other is an outer conductor 5a formed by closely adhering a conductor film to the entire outer surface of the dielectric substrate 1a, and 5b is a dielectric material. Outer conductors formed by closely adhering a conductor film to the entire outer surface of the substrate 1b, 6 to 8 being dielectric substrates 1a and 1b
And inner conductors 2a to 4a, inner conductors 2b to 4b, and outer conductor 5
Tri-plate line resonators 10a and 10b are input / output lines in which the inner conductors are directly connected to the inner conductors 2a, 2b, 4a, 4b, and 12a is a dielectric substrate 1a.
Groove formed by digging the surface of the dielectric substrate 1b in close contact with the inner conductors 2a to 4a. Reference numeral 12b represents the surface of the dielectric substrate 1b in contact with the outer conductor 5b of the inner conductors 2b to 4b.
Grooves provided by being dug in a direction orthogonal to
5a and 13b to 15b are short-circuited portions. Dielectric substrate 1a
And 1b are overlapped so that the inner conductors 2a and 2b, the inner conductors 3a and 3b, and the inner conductors 4a and 4b face and overlap with each other, and are bonded so that the facing inner conductors are in electrical contact with each other. .. The inner conductors 2a to 4a and 2b to 4b are formed of a thin film or a thick film and are shaped by photo etching or the like. In the present embodiment, the length of each of the inner conductors 2a to 4a is set to about 1/4 wavelength of a desired fundamental wave, and one end of each of the inner conductors 2a to 4a and 2b to 4b is a dielectric substrate 1a. Short-circuit portions 13a to 15a and short-circuit portions 13b to 15b on the side surface of 1b are connected to the outer conductors 5a and 5b and short-circuited. Therefore, the resonators 6 to 8 are quarter-wave resonators in which one end is short-circuited and the other end is open. The groove 12a
And the groove 12b are short-circuited portions 13a to 15a, short-circuited portion 13b.
˜15b to the inner conductors 2a to 4a and the inner conductors 2b to 4b in the longitudinal direction at a position of about ⅓ of the inner conductor length. The outer conductor 5 in which the surfaces of the grooves 12a and 12b are extended
It is closely adhered and covered by a and 5b (first invention).
1 and 2, the dielectric substrate 1a has a dielectric substrate 1b whose longitudinal direction is the inner conductors 2a to 4a, as in the conventional case.
The longer end is set and the dielectric substrate 1a and the dielectric substrate 1b are arranged so that the short-circuited ends of the resonators 6 to 8 are aligned to expose the open ends of the inner conductors 2a to 4a. Take as an example.

【0029】動作は次のとおりである。共振器6〜8は
溝12a,12bの効果により長さが1/4波長より短
縮されるため、隣接するもの相互の電界結合が弱めら
れ、従来の場合と同様に主として磁界により相互に結合
されている。その結合量は溝12a,12bの深さや隣
接する内導体間の距離によって調整される。
The operation is as follows. Since the lengths of the resonators 6 to 8 are shortened to less than 1/4 wavelength due to the effect of the grooves 12a and 12b, the electric field coupling between adjacent ones is weakened, and the resonators 6 to 8 are mainly coupled to each other by a magnetic field as in the conventional case. ing. The amount of coupling is adjusted by the depth of the grooves 12a and 12b and the distance between adjacent inner conductors.

【0030】今、内導体2a〜4aの開放端側の露出部
をトリミングしてこれら内導体の長さを調整すること
で、全ての共振器6〜8が同一の周波数、例えばf0で
共振しているものとすれば、その周波数f0では、共振
状態にある共振器6〜8は相互に強く結合しており、入
出力線路10への入射波は共振器6へ導かれ、共振器
7,8を通って入出力線路11より出力される。しかし
ながら、f0以外の周波数では、共振器6〜8相互の結
合は非常に弱く、入出力線路10あるいは11への入射
波はその電力のほとんどが反射される。このように、図
1に示したストリップ線路フィルタは帯域通過フィルタ
としての機能を有する。
Now, by trimming the exposed portions of the inner conductors 2a to 4a on the open end side and adjusting the lengths of these inner conductors, all the resonators 6 to 8 resonate at the same frequency, for example, f0. At that frequency f0, the resonators 6 to 8 in the resonance state are strongly coupled to each other, the incident wave to the input / output line 10 is guided to the resonator 6, and the resonator 7, It is output from the input / output line 11 through the signal line 8. However, at frequencies other than f0, the mutual coupling of the resonators 6 to 8 is very weak, and most of the power of the incident wave to the input / output line 10 or 11 is reflected. Thus, the stripline filter shown in FIG. 1 has a function as a bandpass filter.

【0031】図1のストリップ線路フィルタの共振器6
〜8は基本波に対して1/4波長共振器として動作し、
共振器縦断面内における基本波の電位は図3に実線で示
す分布となる。また、基本波の3倍の周波数をもつ3倍
高調波に対しては3/4波長共振器として動作し、共振
器縦断面内における3倍高調波の電位は図3に破線で示
すように分布する。一方、溝12aおよび12bと内導
体2a〜4bおよび内導体2b〜4bの交差位置では、
これら内導体と外導体5aおよび外導体5bとの間隔が
局部的に狭まり、かつ、角部を形成するため、電界が集
中し静電容量が大きくなる。この溝12a,12bを短
絡部13a〜15a、13b〜15bから内導体2a〜
4a,内導体2b〜4bの長手方向に内導体2a〜4a
長の約1/3の位置に設ると、もともとこの位置で電位
の低い基本波に対しては共振器の共振周波数はほとんど
変化しないが、この位置で電位が最大となる3倍高調波
に対しては溝により静電容量が大きくなり共振周波数が
低くなる。このため図1のストリップ線路フィルタの通
過特性は図4のようになる。すなわち、基本波の周波数
を第1の通過周波数f0とすると、第2の通過周波数は
3f0より低いほうへシフトする。したがって、図1の
ストリップ線路フィルタは基本波の3倍の3倍高調波を
阻止する機能を有する。
Resonator 6 of the stripline filter of FIG.
~ 8 operates as a quarter-wave resonator with respect to the fundamental wave,
The potential of the fundamental wave in the longitudinal section of the resonator has the distribution shown by the solid line in FIG. Also, it operates as a 3/4 wavelength resonator for the triple harmonic having a frequency three times that of the fundamental wave, and the potential of the triple harmonic in the longitudinal section of the resonator is as shown by the broken line in FIG. To be distributed. On the other hand, at the intersecting positions of the grooves 12a and 12b and the inner conductors 2a to 4b and the inner conductors 2b to 4b,
Since the distance between the inner conductor and the outer conductor 5a and the outer conductor 5b is locally narrowed and a corner is formed, the electric field is concentrated and the capacitance is increased. The grooves 12a, 12b are connected to the inner conductors 2a through the short-circuited portions 13a through 15a, 13b through 15b.
4a, the inner conductors 2a to 4a in the longitudinal direction of the inner conductors 2b to 4b.
When it is installed at a position of about 1/3 of the length, the resonance frequency of the resonator hardly changes with respect to the fundamental wave whose potential is originally low at this position, but it becomes a triple harmonic wave where the potential becomes maximum at this position. On the other hand, the groove increases the capacitance and lowers the resonance frequency. Therefore, the pass characteristic of the strip line filter of FIG. 1 is as shown in FIG. That is, assuming that the frequency of the fundamental wave is the first pass frequency f0, the second pass frequency shifts to a position lower than 3f0. Therefore, the strip line filter of FIG. 1 has a function of blocking the third harmonic of the fundamental wave.

【0032】図5は第2の発明に係わるストリップ線路
フィルタの一実施例を示す概略構成図である。図中、図
1と同じものは同一の符号を付して説明を省略する。本
実施例は図1の溝12aおよび溝12bの代わりに短絡
部13a〜15a,短絡部13b〜15bから内導体2
a〜4a,内導体2b〜4bの長手方向にこれら内導体
長の約2/3の位置に溝16aおよび溝16bを設けた
場合である(第2の発明)。図6から分かるように基本
波の電位はこの位置で比較的高いのに対して、3倍高調
波の電位はほぼ0となる。このため、基本波の共振周波
数は低いほうへシフトし、3倍高調波の共振周波数は変
化しない。このとき図5のストリップ線路フィルタの通
過特性は図7のようになる。すなわち、シフトした基本
波の周波数を新めて第1の通過周波数f0とすると、第
2の通過周波数は3f0より高いほうへシフトする。し
たがって、図5のストリップ線路フィルタは、図1の場
合と同様に基本波の3倍の周波数の3倍高調波を阻止す
る機能を有する。
FIG. 5 is a schematic diagram showing an embodiment of the stripline filter according to the second invention. In the figure, the same parts as those in FIG. 1 are designated by the same reference numerals and the description thereof will be omitted. In this embodiment, instead of the groove 12a and the groove 12b of FIG. 1, the short conductors 13a to 15a and the short conductors 13b to 15b are connected to the inner conductor 2.
This is a case where the grooves 16a and 16b are provided in the longitudinal direction of the a to 4a and the inner conductors 2b to 4b at positions of about ⅔ of these inner conductor lengths (second invention). As can be seen from FIG. 6, the potential of the fundamental wave is relatively high at this position, while the potential of the triple harmonic wave is almost zero. Therefore, the resonance frequency of the fundamental wave shifts to the lower side, and the resonance frequency of the triple harmonic does not change. At this time, the pass characteristic of the strip line filter of FIG. 5 is as shown in FIG. That is, if the frequency of the shifted fundamental wave is newly set as the first pass frequency f0, the second pass frequency shifts to a higher position than 3f0. Therefore, the strip line filter of FIG. 5 has the function of blocking the triple harmonic of the frequency three times the fundamental wave, as in the case of FIG.

【0033】図5の実施例は、図1の場合と同様の動作
原理および利点を有する他、第2の通過周波数を基本波
の3倍の周波数より高い側にシフトでき、阻止帯域幅を
広くとれるという利点を有する。
The embodiment of FIG. 5 has the same operating principle and advantages as those of FIG. 1, and can shift the second pass frequency to the higher side of the frequency three times the fundamental wave, thereby widening the stop band width. It has the advantage that it can be taken.

【0034】図8は第3の発明に係わるストリップ線路
フィルタの一実施例を示す概略構成図、図9は図8の実
施例の内導体パターン図である。図中、図1と同じもの
は同一の符号を付して説明を省略する。本実施例は短絡
部13a〜15a,短絡部13b〜15bから内導体2
a〜4a,内導体2b〜4bの長手方向に内導体2a〜
4a長の約1/3の位置に、溝12aおよび溝12bを
設ける代わりに内導体の突起部17aおよび突起部17
bを設けた場合である(第3の発明)。突起部17a,
突起部17bは内導体2a〜4a,内導体2b〜4bを
幅方向に延長して形成されている。突起部17a,17
bを設けた位置では内導体幅が局所的に広がるため、外
導体5a,外導体5bとの間の静電容量が大きくなる。
このため、溝12a,溝12bを設けた図1の場合と同
様に、もともとこの位置で電位の低い基本波に対しては
共振器の共振周波数はほとんど変化しないが、この位置
で電位が最大となる3倍高調波に対しては溝により静電
容量が大きくなり共振周波数は低いほうへシフトする。
FIG. 8 is a schematic structural view showing an embodiment of the strip line filter according to the third invention, and FIG. 9 is an inner conductor pattern diagram of the embodiment of FIG. In the figure, the same parts as those in FIG. 1 are designated by the same reference numerals and the description thereof will be omitted. In this embodiment, the short conductors 13a to 15a and the short conductors 13b to 15b are connected to the inner conductor 2.
a to 4a, inner conductors 2a to 4b in the longitudinal direction of the inner conductors 2a to 4b.
Instead of providing the groove 12a and the groove 12b at the position of about 1/3 of the length of the 4a, the protrusion 17a and the protrusion 17 of the inner conductor are provided.
This is the case where b is provided (third invention). Protrusion 17a,
The protruding portion 17b is formed by extending the inner conductors 2a to 4a and the inner conductors 2b to 4b in the width direction. Protrusions 17a, 17
Since the inner conductor width locally widens at the position where b is provided, the capacitance between the outer conductor 5a and the outer conductor 5b increases.
Therefore, as in the case of FIG. 1 in which the groove 12a and the groove 12b are provided, the resonance frequency of the resonator hardly changes with respect to the fundamental wave having a low electric potential at this position, but the electric potential becomes maximum at this position. For the third harmonic wave, the capacitance increases due to the groove, and the resonance frequency shifts to the lower side.

【0035】図8の実施例は、図1の場合と同様の動作
原理および利点を有する他、誘電体基板1a,1bを掘
り込んだ溝12a,12bの加工が不要であり、また、
突起部17a,17bを内導体2a〜4a,内導体2b
〜4bと同様にフォトエッチングにより形成できるの
で、加工が容易になるという利点を有する。
The embodiment shown in FIG. 8 has the same operating principle and advantages as those shown in FIG. 1, and does not require the processing of the grooves 12a and 12b in which the dielectric substrates 1a and 1b are dug.
The protrusions 17a and 17b are connected to the inner conductors 2a to 4a and the inner conductor 2b.
Since it can be formed by photo-etching similarly to 4b, it has an advantage of easy processing.

【0036】図10は第4の発明に係わるストリップ線
路フィルタの一実施例を示す概略構成図である。図中、
図5と同じものは同一の符号を付して説明を省略する。
本実施例は短絡部13a〜15a,短絡部13b〜15
bから内導体2a〜4a,内導体2b〜4bの長手方向
に内導体2a〜4a長の約2/3の位置に、溝16aお
よび溝16bを設ける代わりに内導体の突起部18aお
よび突起部18bを設けた場合である(第4の発明)。
突起部18a,突起部18bは内導体2a〜4a,内導
体2b〜4bを幅方向に延長して形成されている。突起
部18a,突起部18bを設けた位置では内導体幅が局
所的に広がるため、外導体5a,外導体5bとの間の静
電容量が大きくなる。従って、図5の実施例と同様に基
本波の電位はこの突起部18a,突起部18bの位置で
比較的高いのに対して、3倍高調波の電位はほぼ0とな
るので、基本波の共振周波数は低いほうへシフトし、3
倍高調波の共振周波数は変化しない。
FIG. 10 is a schematic block diagram showing an embodiment of the strip line filter according to the fourth invention. In the figure,
The same parts as those in FIG. 5 are designated by the same reference numerals and the description thereof will be omitted.
In this embodiment, the short-circuit parts 13a to 15a and the short-circuit parts 13b to 15 are used.
b to the inner conductors 2a to 4a and the inner conductors 2b to 4b at the positions of about 2/3 of the length of the inner conductors 2a to 4a in the longitudinal direction, the protrusions 18a and the protrusions of the inner conductor are provided instead of the grooves 16a and 16b. This is the case where 18b is provided (fourth invention).
The protrusions 18a and 18b are formed by extending the inner conductors 2a to 4a and the inner conductors 2b to 4b in the width direction. Since the inner conductor width locally expands at the positions where the protrusions 18a and 18b are provided, the capacitance between the outer conductors 5a and the outer conductors 5b increases. Therefore, as in the embodiment of FIG. 5, the potential of the fundamental wave is relatively high at the positions of the protrusions 18a and 18b, while the potential of the third harmonic is almost 0, so that The resonance frequency shifts to the lower side, 3
The resonance frequency of the double harmonic does not change.

【0037】図10の実施例は、図5の場合と同様の動
作原理および利点を有する他、誘電体基板1a,1bを
掘り込んだ溝16a,16bの加工が不要であり、ま
た、突起部18a,18bを内導体2a〜4a,内導体
2b〜4bと同様にフォトエッチングにより形成できる
ので、加工が容易になるという利点を有する。
The embodiment shown in FIG. 10 has the same operating principle and advantages as those shown in FIG. 5, and does not require the processing of the grooves 16a and 16b in which the dielectric substrates 1a and 1b are dug, and the protrusions are not necessary. Since the inner conductors 18a and 18b can be formed by photoetching similarly to the inner conductors 2a to 4a and the inner conductors 2b to 4b, there is an advantage that processing becomes easy.

【0038】図11は第5の発明に係わるストリップ線
路フィルタの一実施例を示す概略構成図である。図中、
図1と同じものは同一の符号を付して説明を省略する。
本実施例は図において、図1の実施例におけるトリプレ
ート線路の共振器6〜8の代わりにマイクロストリップ
線路の共振器19〜21を用いて構成するとともに、誘
電体基板1aと、上記誘電体基板1aの一方の面に形成
された外導体5aと、上記誘電体基板の他方の面に相互
に略平行に形成され、一端が上記外導体5aに接続され
て短絡部13a〜15aを形成する複数の内導体2a〜
4aとを備え、上記誘電体基板1aのうちの上記外導体
5aが形成された面の、上記短絡部13a〜15aから
上記内導体2a〜4a長の約1/3の位置に上記内導体
2a〜4aと交差する方向に溝12aを設け、かつ上記
溝12aの表面に上記外導体5aと連続する導体を密着
した場合である(第5の発明)。
FIG. 11 is a schematic diagram showing an embodiment of the stripline filter according to the fifth invention. In the figure,
The same parts as those in FIG. 1 are designated by the same reference numerals and the description thereof will be omitted.
In this embodiment, the resonators 6 to 8 of the microplate line are used instead of the resonators 6 to 8 of the triplate line in the embodiment of FIG. 1, and the dielectric substrate 1a and the dielectric material are used. The outer conductor 5a formed on one surface of the substrate 1a and the other surface of the dielectric substrate are formed substantially parallel to each other, and one ends thereof are connected to the outer conductor 5a to form short-circuited portions 13a to 15a. A plurality of inner conductors 2a
4a, and the inner conductor 2a is located on the surface of the dielectric substrate 1a on which the outer conductor 5a is formed, at a position approximately 1/3 of the length of the inner conductors 2a to 4a from the short-circuited portions 13a to 15a. This is a case where the groove 12a is provided in a direction intersecting with the grooves 4a to 4a, and a conductor continuous with the outer conductor 5a is adhered to the surface of the groove 12a (fifth invention).

【0039】図11の実施例は、図1の場合と同様の動
作原理および利点を有する他、内導体2a〜4a、およ
び入出力線路10,11の内導体が全て露出されている
ので、入出力結合量、共振器間結合量、および共振器1
9〜21の共振周波数を容易に調整できるという利点を
有する。
The embodiment shown in FIG. 11 has the same operating principle and advantages as those shown in FIG. 1, and since the inner conductors 2a to 4a and the inner conductors of the input / output lines 10 and 11 are all exposed, the embodiment shown in FIG. Output coupling amount, inter-resonator coupling amount, and resonator 1
It has an advantage that the resonance frequencies of 9 to 21 can be easily adjusted.

【0040】図12は第6の発明に係わるストリップ線
路フィルタの一実施例を示す概略構成図である。図中、
図5および図11と同じものは同一の符号を付して説明
を省略する。本実施例は図5の実施例におけるトリプレ
ート線路の共振器6〜8の代わりにマイクロストリップ
線路の共振器19〜21を用いて構成するとともに、上
記誘電体基板1aのうちの上記外導体5aが形成された
面の、上記短絡部13a〜15aから上記内導体2a〜
4a長の約2/3の位置に上記内導体2a〜4aと交差
する方向の溝16aを設け、かつ上記溝16aの表面に
上記外導体5aと連続する導体を密着した場合である
(第6の発明)。
FIG. 12 is a schematic configuration diagram showing an embodiment of a strip line filter according to the sixth invention. In the figure,
The same parts as those in FIGS. 5 and 11 are designated by the same reference numerals and the description thereof will be omitted. In this embodiment, resonators 19 to 21 of microstrip lines are used instead of the resonators 6 to 8 of the triplate line in the embodiment of FIG. 5, and the outer conductor 5a of the dielectric substrate 1a is used. From the short-circuited portions 13a to 15a of the surface on which the inner conductor 2a to
This is a case where a groove 16a in a direction intersecting with the inner conductors 2a to 4a is provided at a position of about ⅔ of the length of 4a, and a conductor continuous with the outer conductor 5a is adhered to the surface of the groove 16a (sixth). Invention).

【0041】図12の実施例は、図5の場合と同様の動
作原理および利点を有する他、内導体2a〜4a、およ
び入出力線路10,11の内導体が全て露出されている
ので、入出力結合量、共振器間結合量、および共振器1
9〜21の共振周波数を容易に調整できるという利点を
有する。
The embodiment of FIG. 12 has the same operating principle and advantages as those of FIG. 5, and since all the inner conductors 2a to 4a and the inner conductors of the input / output lines 10 and 11 are exposed, the embodiment shown in FIG. Output coupling amount, inter-resonator coupling amount, and resonator 1
It has an advantage that the resonance frequencies of 9 to 21 can be easily adjusted.

【0042】図13は第7の発明に係わるストリップ線
路フィルタの一実施例を示す概略構成図である。図中、
図8及び図11と同じものは同一の符号を付して説明を
省略する。本実施例は図8の実施例におけるトリプレー
ト線路の共振器6〜8の代わりにマイクロストリップ線
路の共振器19〜21を用いて構成するとともに、上記
内導体の短絡部13a〜15aから、上記内導体2a〜
4a長の約1/3の位置に上記内導体2a〜4aを幅方
向に延長した突起部17aを設けた場合である(第7の
発明)。
FIG. 13 is a schematic block diagram showing an embodiment of the strip line filter according to the seventh invention. In the figure,
The same parts as those in FIGS. 8 and 11 are designated by the same reference numerals and the description thereof will be omitted. This embodiment is configured by using resonators 19 to 21 of microstrip lines instead of the resonators 6 to 8 of the triplate line in the embodiment of FIG. 8, and from the short-circuited portions 13a to 15a of the inner conductor, Inner conductor 2a-
This is a case where the protrusion 17a obtained by extending the inner conductors 2a to 4a in the width direction is provided at a position of about ⅓ of the length of 4a (seventh invention).

【0043】図13の実施例は、図8の場合と同様の動
作原理および利点を有する他、内導体2a〜4a、突起
部17a、および入出力線路10,11の内導体が全て
露出されているので、入出力結合量、共振器間結合量、
共振器19〜21の共振周波数、および突起部17aの
位置を容易に調整できるという利点を有する。
The embodiment shown in FIG. 13 has the same operating principle and advantages as those shown in FIG. 8, and the inner conductors 2a to 4a, the protrusion 17a, and the inner conductors of the input / output lines 10 and 11 are all exposed. Therefore, the input / output coupling amount, the coupling amount between resonators,
This has an advantage that the resonance frequency of the resonators 19 to 21 and the position of the protrusion 17a can be easily adjusted.

【0044】図14は第8の発明に係わるストリップ線
路フィルタの一実施例を示す概略構成図である。図中、
図10及び図11と同じものは同一の符号を付して説明
を省略する。本実施例は図10の実施例におけるトリプ
レート線路の共振器6〜8の代わりにマイクロストリッ
プ線路の共振器19〜21を用いて構成するとともに、
上記内導体2a〜4aの短絡部13a〜15aから上記
内導体2a〜4a長の約2/3の位置に上記内導体2a
〜4aを幅方向に延長した突起部18aを設けた場合で
ある(第8の発明)。
FIG. 14 is a schematic diagram showing an embodiment of the strip line filter according to the eighth invention. In the figure,
The same parts as those in FIGS. 10 and 11 are designated by the same reference numerals and the description thereof will be omitted. This embodiment is constructed by using resonators 19 to 21 of microstrip line in place of the resonators 6 to 8 of triplate line in the embodiment of FIG.
The inner conductor 2a is located at a position approximately ⅔ of the length of the inner conductors 2a to 4a from the short-circuited portions 13a to 15a of the inner conductors 2a to 4a.
This is the case where the protrusion 18a is formed by extending the widths 4a to 4a (eighth invention).

【0045】図14の実施例は、図10の場合と同様の
動作原理および利点を有する他、内導体2a〜4a、突
起部18a、および入出力線路10,11の内導体が全
て露出されているので、入出力結合量、共振器間結合
量、共振器19〜21の共振周波数、および突起部18
aの位置を容易に調整できるという利点を有する。
The embodiment of FIG. 14 has the same operating principle and advantages as those of FIG. 10, and in addition, the inner conductors 2a to 4a, the protruding portion 18a, and the inner conductors of the input / output lines 10 and 11 are all exposed. Therefore, the input / output coupling amount, the inter-resonator coupling amount, the resonance frequencies of the resonators 19 to 21, and the protruding portion 18
This has the advantage that the position of a can be easily adjusted.

【0046】図15は第9の発明に係わるストリップ線
路フィルタの一実施例を示す概略構成図である。図中、
図11と同じものは同一の符号を付して説明を省略す
る。本実施例は図11の短絡部13a〜15aから内導
体2a〜4aの長手方向に内導体2a〜4a長の約1/
3の位置に溝12aを設ける代わりに棒状あるいは板状
の誘電体としての棒状誘電体22を設けた場合である。
棒状誘電体22は内導体2a〜4aと直交する方向に、
内導体2a〜4aと密着するように接着剤等により固定
されている(第9の発明)。棒状誘電体22と内導体2
a〜4aとが交わる位置では棒状誘電体の効果により静
電容量が大きくなる。従って図11の実施例の場合と同
様に、もともとこの位置で電位の低い基本波に対しては
共振器の共振周波数はほとんど変化しないが、この位置
で電位が最大となる3倍高調波に対しては棒状誘電体2
2により静電容量が大きくなり共振周波数は低いほうへ
シフトする。
FIG. 15 is a schematic block diagram showing an embodiment of the strip line filter according to the ninth invention. In the figure,
The same parts as those in FIG. 11 are designated by the same reference numerals and the description thereof will be omitted. In this embodiment, about 1 / the length of the inner conductors 2a to 4a in the longitudinal direction of the inner conductors 2a to 4a from the short-circuited portions 13a to 15a in FIG.
This is a case where a rod-shaped dielectric 22 as a rod-shaped or plate-shaped dielectric is provided instead of providing the groove 12a at the position of 3.
The rod-shaped dielectric 22 is formed in a direction orthogonal to the inner conductors 2a to 4a,
It is fixed with an adhesive or the like so as to be in close contact with the inner conductors 2a to 4a (the ninth invention). Rod-shaped dielectric 22 and inner conductor 2
At the position where a to 4a intersect, the capacitance increases due to the effect of the rod-shaped dielectric. Therefore, as in the case of the embodiment of FIG. 11, the resonance frequency of the resonator hardly changes with respect to the fundamental wave having a low electric potential at this position, but for the third harmonic wave having the maximum electric potential at this position. For rod-shaped dielectric 2
By 2, the capacitance increases and the resonance frequency shifts to the lower side.

【0047】図15の実施例は、図11の場合と同様の
動作原理および利点を有する他、棒状誘電体22の位置
や誘電率を変化させることにより、フィルタの第2の通
過周波数を3倍高調波の周波数からシフトさせる量を容
易に調整できるという利点を有する。
The embodiment shown in FIG. 15 has the same operating principle and advantages as those shown in FIG. 11, and in addition, the second pass frequency of the filter is tripled by changing the position and permittivity of the rod-shaped dielectric 22. This has the advantage that the amount of shift from the harmonic frequency can be easily adjusted.

【0048】図16は第10の発明に係わるストリップ
線路フィルタの一実施例を示す概略構成図である。図
中、図12と同じものは同一の符号を付して説明を省略
する。本実施例は図12の短絡部13a〜15aから内
導体2a〜4aの長手方向に内導体2a〜4a長の約2
/3の位置に溝16aを設ける代わりに棒状あるいは板
状の誘電体としての棒状誘電体23を設けた場合であ
る。棒状誘電体23は内導体2a〜4aと直交する方向
に、内導体2a〜4aと密着するように接着剤等により
固定されている(第10の発明)。棒状誘電体23と内
導体2a〜4aとが交わる位置では棒状誘電体23の効
果により静電容量が大きくなる。従って図12の実施例
の場合と同様に、基本波に対しては電位が棒状誘電体2
3の位置で比較的高いので、共振周波数は低いほうへシ
フトするが、3倍高調波に対しては電位がほぼ0となる
ので、共振周波数は変化しない。
FIG. 16 is a schematic diagram showing an embodiment of the strip line filter according to the tenth invention. In the figure, the same parts as those in FIG. 12 are designated by the same reference numerals and the description thereof will be omitted. In this embodiment, the length of the inner conductors 2a to 4a is about 2 in the longitudinal direction of the inner conductors 2a to 4a from the short-circuited portions 13a to 15a in FIG.
This is a case where the rod-shaped dielectric 23 as a rod-shaped or plate-shaped dielectric is provided instead of providing the groove 16a at the position of / 3. The rod-shaped dielectric 23 is fixed by an adhesive or the like so as to be in close contact with the inner conductors 2a to 4a in a direction orthogonal to the inner conductors 2a to 4a (the tenth invention). At the position where the rod-shaped dielectric 23 intersects with the inner conductors 2a to 4a, the capacitance increases due to the effect of the rod-shaped dielectric 23. Therefore, as in the case of the embodiment of FIG. 12, the potential of the rod-shaped dielectric 2 is different from that of the fundamental wave.
Since the resonance frequency is relatively high at the position of 3, the resonance frequency shifts to the lower side, but the resonance frequency does not change because the potential becomes almost 0 for the triple harmonic.

【0049】図16の実施例は、図12の場合と同様の
動作原理および利点を有する他、棒状誘電体23の位置
や誘電率を変化させることにより、フィルタの第2の通
過周波数を3倍高調波の周波数からシフトさせる量を容
易に調整できるという利点を有する。
The embodiment of FIG. 16 has the same operating principle and advantages as those of FIG. 12, and the position and dielectric constant of the rod-shaped dielectric 23 are changed to triple the second pass frequency of the filter. This has the advantage that the amount of shift from the harmonic frequency can be easily adjusted.

【0050】なお、上記各実施例では共振器の数が3個
の場合について説明したが、2個あるいは4個以上であ
ってもよく、上記実施例と同様の利点および効果を奏す
る。
In each of the above embodiments, the case where the number of resonators is 3 has been described. However, the number of resonators may be 2 or 4 or more, and the same advantages and effects as the above embodiments can be obtained.

【0051】また、上記各実施例では共振器として1/
4波長共振器を用いた場合について説明したが、n/4 波
長(nは3以上の奇数)共振器、あるいはm/2 波長(m
は1以上の整数)共振器であってもよく、上記実施例と
同様の利点および効果を奏する。
In each of the above embodiments, the resonator is 1 /
The case of using a 4-wavelength resonator has been described, but it is an n / 4 wavelength (n is an odd number of 3 or more) resonator or an m / 2 wavelength (m
May be an integer greater than or equal to 1) resonator, and the same advantages and effects as those of the above-described embodiment can be obtained.

【0052】[0052]

【発明の効果】第1の発明によれば、誘電体基板のうち
少なくとも外導体が形成された一枚の外面の、短絡部か
ら内導体長の約1/3の位置に上記内導体と交差する方
向の溝を設け、かつ上記溝の表面に上記外導体と連続す
る導体を密着したので、基本波に対する上記溝の影響は
少なく共振器の共振周波数は変化しないが、3倍高調波
に対しては上記溝の効果により共振周波数が低くなる。
このため、基本波の共振周波数が第1の通過周波数、3
倍高調波の共振周波数より低い周波数が第2の通過周波
数となり、3倍高調波を阻止する通過特性を有するスト
リップ線路フィルタが得られるという効果がある。
According to the first aspect of the present invention, at least one outer surface of the dielectric substrate on which the outer conductor is formed intersects with the inner conductor at a position approximately 1/3 of the inner conductor length from the short circuit portion. Since a groove continuous with the outer conductor is adhered to the surface of the groove, the effect of the groove on the fundamental wave is small and the resonance frequency of the resonator does not change, but for the third harmonic wave. As a result, the resonance frequency becomes low due to the effect of the groove.
Therefore, the resonance frequency of the fundamental wave is the first pass frequency, 3
The frequency lower than the resonance frequency of the double harmonic becomes the second pass frequency, and the strip line filter having the pass characteristic of blocking the triple harmonic can be obtained.

【0053】第2の発明によれば、誘電体基板のうち少
なくとも外導体が形成された一枚の外面の、短絡部から
内導体長の約2/3の位置に上記内導体と交差する方向
の溝を設け、かつ上記溝の表面に上記外導体と連続する
導体を密着したので、基本波に対しては上記溝の効果に
より共振器の共振周波数が低くなるが、3倍高調波に対
しては上記溝の影響はほとんどなく、共振周波数は変化
しない。このため、基本波の共振周波数が第1の通過周
波数、3倍高調波の共振周波数より高い周波数が第2の
通過周波数となり、3倍高調波を阻止する通過特性を有
するストリップ線路フィルタが得られるという効果があ
る。
According to the second aspect of the invention, a direction of intersecting the inner conductor at a position of about ⅔ of the inner conductor length from the short-circuited portion on the outer surface of at least one outer conductor of the dielectric substrate. Since the groove is provided and the conductor that is continuous with the outer conductor is adhered to the surface of the groove, the resonance frequency of the resonator is lowered for the fundamental wave due to the effect of the groove, but for the triple harmonic wave. As a result, the groove has almost no effect and the resonance frequency does not change. Therefore, the resonance frequency of the fundamental wave is higher than the resonance frequency of the first pass frequency and the triple harmonic wave, and the second pass frequency becomes the second pass frequency. Thus, the strip line filter having the pass characteristic of blocking the triple harmonic wave can be obtained. There is an effect.

【0054】第3の発明によれば、内導体の短絡部から
上記内導体長の約1/3の位置に上記内導体を幅方向に
延長した突起部を設けたので、基本波に対する上記突起
部の影響は少なく共振器の共振周波数は変化しないが、
3倍高調波に対しては上記突起部の効果により共振周波
数が低くなる。このため、基本波の共振周波数が第1の
通過周波数、3倍高調波の共振周波数より低い周波数が
第2の通過周波数となり、3倍高調波を阻止する通過特
性を有するストリップ線路フィルタが得られるという効
果がある。
According to the third aspect of the invention, since the protrusion extending from the short-circuited portion of the inner conductor to the width of the inner conductor is provided at a position about 1/3 of the inner conductor length, the protrusion for the fundamental wave is provided. The resonance frequency of the resonator does not change,
The resonance frequency becomes lower for the third harmonic due to the effect of the protrusion. Therefore, the resonance frequency of the fundamental wave is the first pass frequency, and the frequency lower than the resonance frequency of the triple harmonic is the second pass frequency, and the strip line filter having the pass characteristic of blocking the triple harmonic is obtained. There is an effect.

【0055】第4の発明によれば、内導体の短絡部から
上記内導体長の約2/3の位置に上記内導体を幅方向に
延長した突起部を設けたので、基本波に対しては上記突
起部の効果により共振器の共振周波数が低くなるが、3
倍高調波に対する突起部の影響はほとんどなく、共振周
波数は変化しない。このため、基本波の共振周波数が第
1の通過周波数、3倍高調波の周波数より高い周波数が
第2の通過周波数となり、3倍高調波を阻止する通過特
性を有するストリップ線路フィルタが得られるという効
果がある。
According to the fourth aspect of the invention, since the protrusion extending from the short-circuited portion of the inner conductor to the width of the inner conductor is provided at a position about ⅔ of the length of the inner conductor, the fundamental wave is Causes the resonance frequency of the resonator to decrease due to the effect of the above-mentioned protrusion,
There is almost no influence of the protrusion on the harmonics, and the resonance frequency does not change. For this reason, the resonance frequency of the fundamental wave is higher than the frequency of the first pass frequency and the triple harmonic wave, and the frequency is the second pass frequency. Thus, it is possible to obtain a strip line filter having a pass characteristic of blocking the triple harmonic wave. effective.

【0056】第5の発明によれば、誘電体基板のうちの
外導体が形成された面の短絡部から上記内導体長の約1
/3の位置に内導体と交差する方向の溝を設け、かつ上
記溝の表面に上記外導体と連続する導体を密着したの
で、基本波に対する上記溝の影響は少なく共振器の共振
周波数は変化しないが、3倍高調波に対しては上記溝の
効果により共振周波数が低くなる。このため、基本波の
共振周波数が第1の通過周波数、3倍高調波の共振周波
数より低い周波数が第2の通過周波数となり、3倍高調
波を阻止する通過特性を有するストリップ線路フィルタ
が得られるという効果がある。
According to the fifth aspect of the invention, the inner conductor length is about 1 from the short-circuited portion of the surface of the dielectric substrate on which the outer conductor is formed.
Since a groove intersecting the inner conductor is provided at the position of / 3, and a conductor continuous with the outer conductor is adhered to the surface of the groove, the influence of the groove on the fundamental wave is small and the resonance frequency of the resonator changes. However, the resonance frequency becomes lower for the third harmonic due to the effect of the groove. Therefore, the resonance frequency of the fundamental wave is the first pass frequency, and the frequency lower than the resonance frequency of the triple harmonic is the second pass frequency, and the strip line filter having the pass characteristic of blocking the triple harmonic is obtained. There is an effect.

【0057】第6の発明によれば、誘電体基板のうちの
外導体が形成された面の、短絡部から上記内導体長の約
2/3の位置に上記内導体と交差する方向の溝を設け、
かつ上記溝の表面に上記外導体と連続する導体を密着し
た。基本波に対しては上記溝の効果により共振器の共振
周波数は低くなるが、3倍高調波に対する溝の影響はほ
とんどなく、共振周波数は変化しない。このため、基本
波の共振周波数が第1の通過周波数、3倍高調波の周波
数より高い周波数が第2の通過周波数となり、3倍高調
波を阻止する通過特性を有するストリップ線路フィルタ
が得られるという効果がある。
According to the sixth invention, a groove in a direction intersecting with the inner conductor at a position of about 2/3 of the inner conductor length from the short-circuited portion on the surface of the dielectric substrate on which the outer conductor is formed. Is provided
Moreover, a conductor continuous with the outer conductor was adhered to the surface of the groove. The resonance frequency of the resonator is lowered with respect to the fundamental wave due to the effect of the groove, but the groove has little effect on the triple harmonic and the resonance frequency does not change. For this reason, the resonance frequency of the fundamental wave is higher than the frequency of the first pass frequency and the triple harmonic wave, and the frequency is the second pass frequency. Thus, it is possible to obtain a strip line filter having a pass characteristic of blocking the triple harmonic wave. effective.

【0058】第7の発明によれば、内導体の短絡部から
上記内導体長の約1/3の位置に上記内導体を幅方向に
延長した突起部を設けたので、基本波に対する上記突起
部の影響は少なく共振器の共振周波数は変化しないが、
3倍高調波に対しては上記突起部の効果により共振周波
数が低くなる。このため、基本波の共振周波数が第1の
通過周波数、3倍高調波の共振周波数より低い周波数が
第2の通過周波数となり、3倍高調波を阻止する通過特
性を有するストリップ線路フィルタが得られるという効
果がある。
According to the seventh aspect of the present invention, since the protruding portion extending in the width direction of the inner conductor is provided at a position approximately 1/3 of the inner conductor length from the short-circuited portion of the inner conductor, the protrusion for the fundamental wave is provided. The resonance frequency of the resonator does not change,
The resonance frequency becomes lower for the third harmonic due to the effect of the protrusion. Therefore, the resonance frequency of the fundamental wave is the first pass frequency, and the frequency lower than the resonance frequency of the triple harmonic is the second pass frequency, and the strip line filter having the pass characteristic of blocking the triple harmonic is obtained. There is an effect.

【0059】第8の発明によれば、内導体の短絡部から
上記内導体長の約2/3の位置に上記内導体を幅方向に
延長した突起部を設けたので、基本波に対しては上記突
起部の効果により共振器の共振周波数は低くなるが、3
倍高調波に対する上記突起部の影響はほとんどなく、共
振周波数は変化しない。このため、基本波の共振周波数
が第1の通過周波数、3倍高調波の共振周波数より高い
周波数が第2の通過周波数となり、3倍高調波を阻止す
る通過特性を有するストリップ線路フィルタが得られる
という効果がある。
According to the eighth aspect of the invention, since the protrusion extending in the width direction of the inner conductor is provided at a position about ⅔ of the inner conductor length from the short-circuited portion of the inner conductor, Causes the resonance frequency of the resonator to decrease due to the effect of the above-mentioned protrusions.
There is almost no influence of the above-mentioned protrusion on the harmonics, and the resonance frequency does not change. Therefore, the resonance frequency of the fundamental wave is higher than the resonance frequency of the first pass frequency and the triple harmonic wave, and the second pass frequency becomes the second pass frequency. Thus, the strip line filter having the pass characteristic of blocking the triple harmonic wave can be obtained. There is an effect.

【0060】第9の発明によれば、短絡部から内導体長
の約1/3の位置の上記内導体上に、棒状あるいは板状
の誘電体を上記内導体と交差する方向に密着して設けた
ので、基本波に対する上記棒状誘電体の影響は少なく共
振器の共振周波数は変化しないが、3倍高調波に対して
は上記棒状誘電体の効果により共振周波数が低くなる。
このため、基本波の共振周波数が第1の通過周波数、3
倍高調波の共振周波数より低い周波数が第2の通過周波
数となり、3倍高調波を阻止する通過特性を有するスト
リップ線路フィルタが得られるという効果がある。
According to the ninth aspect of the invention, a rod-shaped or plate-shaped dielectric is adhered in a direction intersecting the inner conductor on the inner conductor at a position of about 1/3 of the inner conductor length from the short-circuited portion. Since it is provided, the influence of the rod-shaped dielectric on the fundamental wave is small and the resonance frequency of the resonator does not change, but the resonance frequency is lowered for the triple harmonic due to the effect of the rod-shaped dielectric.
Therefore, the resonance frequency of the fundamental wave is the first pass frequency, 3
The frequency lower than the resonance frequency of the double harmonic becomes the second pass frequency, and the strip line filter having the pass characteristic of blocking the triple harmonic can be obtained.

【0061】第10の発明によれば、短絡部から内導体
長の約2/3の位置の上記内導体上に、棒状あるいは板
状の誘電体を上記内導体と交差する方向に密着して設け
たので、基本波に対しては上記突起部の効果により共振
器の共振周波数が低くなるが、3倍高調波に対する上記
突起部の影響はほとんどなく、共振周波数は変化しな
い。このため、基本波の周波数が第1の通過周波数、3
倍高調波の共振周波数より高い周波数が第2の通過周波
数となり、3倍高調波を阻止する通過特性を有するスト
リップ線路フィルタが得られるという効果がある。
According to the tenth aspect of the present invention, a rod-shaped or plate-shaped dielectric is adhered to the inner conductor at a position approximately ⅔ of the inner conductor length from the short-circuited portion in a direction intersecting with the inner conductor. Since the resonance frequency of the resonator is lowered with respect to the fundamental wave due to the effect of the protrusion, the protrusion has almost no influence on the triple harmonic, and the resonance frequency does not change. Therefore, the frequency of the fundamental wave is the first pass frequency, 3
The frequency higher than the resonance frequency of the double harmonic becomes the second pass frequency, and the strip line filter having the pass characteristic of blocking the triple harmonic can be obtained.

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

【図1】第1の発明の一実施例を示す概略構成図であ
る。
FIG. 1 is a schematic configuration diagram showing an embodiment of a first invention.

【図2】図1の実施例の断面図である。2 is a cross-sectional view of the embodiment of FIG.

【図3】図1の実施例の共振器縦断面内における電位分
布を説明するための図である。
FIG. 3 is a diagram for explaining a potential distribution in a vertical cross section of the resonator of the embodiment of FIG.

【図4】図1の実施例の通過特性を示す図である。FIG. 4 is a diagram showing a pass characteristic of the embodiment of FIG.

【図5】第2の発明の一実施例を示す概略構成図であ
る。
FIG. 5 is a schematic configuration diagram showing an embodiment of the second invention.

【図6】図5の実施例の共振器縦断面内における電位分
布を説明するための図である。
FIG. 6 is a diagram for explaining a potential distribution in a vertical cross section of the resonator of the embodiment of FIG.

【図7】図5の実施例の通過特性を示す図である。FIG. 7 is a diagram showing a pass characteristic of the embodiment of FIG.

【図8】第3の発明の一実施例を示す概略構成図であ
る。
FIG. 8 is a schematic configuration diagram showing an embodiment of the third invention.

【図9】図8の実施例の内導体パターンの一例を示す図
である。
9 is a diagram showing an example of an inner conductor pattern of the embodiment of FIG.

【図10】第4の発明の一実施例を示す概略構成図であ
る。
FIG. 10 is a schematic configuration diagram showing an embodiment of the fourth invention.

【図11】第5の発明の一実施例を示す概略構成図であ
る。
FIG. 11 is a schematic configuration diagram showing an embodiment of the fifth invention.

【図12】第6の発明の一実施例を示す概略構成図であ
る。
FIG. 12 is a schematic configuration diagram showing an embodiment of the sixth invention.

【図13】第7の発明の一実施例を示す概略構成図であ
る。
FIG. 13 is a schematic configuration diagram showing an embodiment of the seventh invention.

【図14】第8の発明の一実施例を示す概略構成図であ
る。
FIG. 14 is a schematic configuration diagram showing an embodiment of the eighth invention.

【図15】第9の発明の一実施例を示す概略構成図であ
る。
FIG. 15 is a schematic configuration diagram showing an embodiment of the ninth invention.

【図16】第10の発明の一実施例を示す概略構成図で
ある。
FIG. 16 is a schematic configuration diagram showing an embodiment of the tenth invention.

【図17】従来のストリップ線路フィルタの一例を示す
概略構成図である。
FIG. 17 is a schematic configuration diagram showing an example of a conventional stripline filter.

【図18】従来のストリップ線路フィルタの通過特性を
示す図である。
FIG. 18 is a diagram showing a pass characteristic of a conventional stripline filter.

【符号の説明】[Explanation of symbols]

1a,1b 誘電体基板 2a〜4a,2b〜4b 内導体 5a,5b 外導体 6〜8 トリプレート線路の共振器 9a,9b 縦溝 10,11 入出力線路 12a,12b 溝 13a〜15a,13b〜15b 短絡部 16a,16b 溝 17a,17b 突起部 18a,18b 突起部 19〜21 マイクロストリップ線路の共振器 22 棒状誘電体 23 棒状誘電体 1a, 1b Dielectric substrate 2a-4a, 2b-4b Inner conductor 5a, 5b Outer conductor 6-8 Triplate line resonator 9a, 9b Vertical groove 10,11 Input / output line 12a, 12b Groove 13a-15a, 13b- 15b Short-circuit part 16a, 16b Groove 17a, 17b Projection part 18a, 18b Projection part 19-21 Microstrip line resonator 22 Rod-shaped dielectric 23 Rod-shaped dielectric

───────────────────────────────────────────────────── フロントページの続き (72)発明者 山田 朗 尼崎市塚口本町8丁目1番1号 三菱電機 株式会社材料研究所内 ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Akira Yamada 8-1-1 Tsukaguchihonmachi, Amagasaki City Mitsubishi Electric Corporation

Claims (10)

【特許請求の範囲】[Claims] 【請求項1】 互に対向する2枚の誘電体基板と、上記
2枚の誘電体基板のそれぞれの外面に形成された外導体
と、上記誘電体基板のうち少なくとも1枚の内面に相互
に略平行に形成され、一端が上記外導体に接続されて短
絡部を形成する複数の内導体とを備えたストリップ線路
フィルタにおいて、上記誘電体基板のうち少なくとも上
記外導体が形成された一枚の外面の、上記短絡部から上
記内導体長の約1/3の位置に上記内導体と交差する方
向の溝を設け、かつ上記溝の表面に上記外導体と連続す
る導体を密着したことを特徴とするストリップ線路フィ
ルタ。
1. Two dielectric substrates facing each other, an outer conductor formed on the outer surface of each of the two dielectric substrates, and an inner surface of at least one of the dielectric substrates. In a stripline filter having a plurality of inner conductors which are formed substantially parallel to each other and one end of which is connected to the outer conductor to form a short circuit portion, a stripline filter including at least the outer conductor of the dielectric substrate is formed. A groove in a direction intersecting with the inner conductor is provided on the outer surface at a position approximately 1/3 of the inner conductor length from the short-circuited portion, and a conductor continuous with the outer conductor is closely adhered to the surface of the groove. Stripline filter.
【請求項2】 互に対向する2枚の誘電体基板と、上記
2枚の誘電体基板のそれぞれの外面に形成された外導体
と、上記誘電体基板のうち少なくとも1枚の内面に相互
に略平行に形成され、一端が上記外導体に接続されて短
絡部を形成する複数の内導体とを備えたストリップ線路
フィルタにおいて、上記誘電体基板のうち少なくとも上
記外導体が形成された一枚の外面の、上記短絡部から上
記内導体長の約2/3の位置に上記内導体と交差する方
向の溝を設け、かつ上記溝の表面に上記外導体と連続す
る導体を密着したことを特徴とするストリップ線路フィ
ルタ。
2. Two dielectric substrates facing each other, an outer conductor formed on the outer surface of each of the two dielectric substrates, and an inner conductor of at least one of the dielectric substrates. In a stripline filter having a plurality of inner conductors which are formed substantially parallel to each other and one end of which is connected to the outer conductor to form a short circuit portion, a stripline filter including at least the outer conductor of the dielectric substrate is formed. A groove in a direction intersecting with the inner conductor is provided on the outer surface at a position approximately ⅔ of the inner conductor length from the short-circuited portion, and a conductor continuous with the outer conductor is adhered to the surface of the groove. Stripline filter.
【請求項3】 互に対向する2枚の誘電体基板と、上記
2枚の誘電体基板のそれぞれの外面に形成された外導体
と、上記誘電体基板のうち少なくとも1枚の内面に相互
に略平行に形成され、一端が上記外導体に接続されて短
絡部を形成する複数の内導体とを備えたストリップ線路
フィルタにおいて、上記内導体の短絡部から上記内導体
長の約1/3の位置に上記内導体を幅方向に延長した突
起部を設けたことを特徴とするストリップ線路フィル
タ。
3. Two dielectric substrates facing each other, an outer conductor formed on the outer surface of each of the two dielectric substrates, and an inner conductor of at least one of the dielectric substrates mutually. In a stripline filter including a plurality of inner conductors which are formed substantially parallel to each other and one end of which is connected to the outer conductor to form a short-circuited portion, a stripline filter having a length of about 1/3 of a length of the inner conductor from the short-circuited portion of the inner conductor is provided. A stripline filter comprising a protrusion formed by extending the inner conductor in the width direction at a position.
【請求項4】 互に対向する2枚の誘電体基板と、上記
2枚の誘電体基板のそれぞれの外面に形成された外導体
と、上記誘電体基板のうち少なくとも1枚の内面に相互
に略平行に形成され、一端が上記外導体に接続されて短
絡部を形成する複数の内導体とを備えたストリップ線路
フィルタにおいて、上記内導体の短絡部から上記内導体
長の約2/3の位置に上記内導体を幅方向に延長した突
起部を設けたことを特徴とするストリップ線路フィル
タ。
4. Two dielectric substrates facing each other, outer conductors formed on the outer surfaces of each of the two dielectric substrates, and inner surfaces of at least one of the dielectric substrates mutually. In a stripline filter including a plurality of inner conductors that are formed substantially in parallel and one end of which is connected to the outer conductor to form a short-circuited portion, a stripline filter having a length of about 2/3 of the inner conductor length from the short-circuited portion of the inner conductor is provided. A stripline filter comprising a protrusion formed by extending the inner conductor in the width direction at a position.
【請求項5】 誘電体基板と、上記誘電体基板の一方の
面に形成された外導体と、上記誘電体基板の他方の面に
相互に略平行に形成され、一端が上記外導体に接続され
て短絡部を形成する複数の内導体とを備えたストリップ
線路フィルタにおいて、上記誘電体基板のうちの上記外
導体が形成された面の、上記短絡部から上記内導体長の
約1/3の位置に上記内導体と交差する方向の溝を設
け、かつ上記溝の表面に上記外導体と連続する導体を密
着したことを特徴とするストリップ線路フィルタ。
5. A dielectric substrate, an outer conductor formed on one surface of the dielectric substrate, and an outer conductor formed on the other surface of the dielectric substrate substantially parallel to each other, and one end of which is connected to the outer conductor. In a stripline filter including a plurality of inner conductors formed to form a short circuit portion, about 1/3 of a length of the inner conductor from the short circuit portion on a surface of the dielectric substrate on which the outer conductor is formed. A strip line filter characterized in that a groove extending in a direction intersecting with the inner conductor is provided at the position, and a conductor continuous with the outer conductor is adhered to the surface of the groove.
【請求項6】 誘電体基板と、上記誘電体基板の一方の
面に形成された外導体と、上記誘電体基板の他方の面に
相互に略平行に形成され、一端が上記外導体に接続され
て短絡部を形成する複数の内導体とを備えたストリップ
線路フィルタにおいて、上記誘電体基板のうちの上記外
導体が形成された面の、上記短絡部から上記内導体長の
約2/3の位置に上記内導体と交差する方向の溝を設
け、かつ上記溝の表面に上記外導体と連続する導体を密
着したことを特徴とするストリップ線路フィルタ。
6. A dielectric substrate, an outer conductor formed on one surface of the dielectric substrate, and an outer conductor formed on the other surface of the dielectric substrate substantially parallel to each other, and one end of which is connected to the outer conductor. In a stripline filter including a plurality of inner conductors formed to form a short circuit portion, about 2/3 of the inner conductor length from the short circuit portion on the surface of the dielectric substrate on which the outer conductor is formed. A strip line filter characterized in that a groove extending in a direction intersecting with the inner conductor is provided at the position, and a conductor continuous with the outer conductor is adhered to the surface of the groove.
【請求項7】 誘電体基板と、上記誘電体基板の一方の
面に形成された外導体と、上記誘電体基板の他方の面に
相互に略平行に形成され、一端が上記外導体に接続され
て短絡部を形成する複数の内導体とを備えたストリップ
線路フィルタにおいて、上記内導体の短絡部から上記内
導体長の約1/3の位置に上記内導体を幅方向に延長し
た突起部を設けたことを特徴とするストリップ線路フィ
ルタ。
7. A dielectric substrate, an outer conductor formed on one surface of the dielectric substrate, and an outer conductor formed on the other surface of the dielectric substrate substantially parallel to each other, and one end of which is connected to the outer conductor. A strip line filter having a plurality of inner conductors formed to form a short-circuited portion, a protrusion formed by extending the inner conductor in the width direction from the short-circuited portion of the inner conductor to a position of about 1/3 of the inner conductor length. A stripline filter characterized by being provided.
【請求項8】 誘電体基板と、上記誘電体基板の一方の
面に形成された外導体と、上記誘電体基板の他方の面に
相互に略平行に形成され、一端が上記外導体に接続され
て短絡部を形成する複数の内導体とを備えたストリップ
線路フィルタにおいて、上記内導体の短絡部から上記内
導体長の約2/3の位置に上記内導体を幅方向に延長し
た突起部を設けたことを特徴とするストリップ線路フィ
ルタ。
8. A dielectric substrate, an outer conductor formed on one surface of the dielectric substrate, and an outer conductor formed on the other surface of the dielectric substrate substantially parallel to each other, and one end of which is connected to the outer conductor. And a plurality of inner conductors that form a short-circuited portion, the protrusion being formed by extending the inner conductor in the width direction from the short-circuited portion of the inner conductor to a position of about ⅔ of the inner conductor length. A stripline filter characterized by being provided.
【請求項9】 誘電体基板と、上記誘電体基板の一方の
面に形成された外導体と、上記誘電体基板の他方の面に
相互に略平行に形成され、一端が上記外導体に接続され
て短絡部を形成する複数の内導体とを備えたストリップ
線路フィルタにおいて、上記短絡部から上記内導体長の
約1/3の位置の上記内導体上に、棒状あるいは板状の
誘電体を上記内導体と交差する方向に密着して設けたこ
とを特徴とするストリップ線路フィルタ。
9. A dielectric substrate, an outer conductor formed on one surface of the dielectric substrate, and an outer conductor formed on the other surface of the dielectric substrate substantially parallel to each other, and one end of which is connected to the outer conductor. In the strip line filter including a plurality of inner conductors that form a short-circuited portion, a rod-shaped or plate-shaped dielectric is provided on the inner conductor at a position approximately 1/3 of the inner conductor length from the short-circuited portion. A strip line filter provided in close contact with a direction intersecting with the inner conductor.
【請求項10】 誘電体基板と、上記誘電体基板の一方
の面に形成された外導体と、上記誘電体基板の他方の面
に相互に略平行に形成され、一端が上記外導体に接続さ
れて短絡部を形成する複数の内導体とを備えたストリッ
プ線路フィルタにおいて、上記短絡部から上記内導体長
の約2/3の位置の上記内導体上に、棒状あるいは板状
の誘電体を上記内導体と交差する方向に密着して設けた
ことを特徴とするストリップ線路フィルタ。
10. A dielectric substrate, an outer conductor formed on one surface of the dielectric substrate, and an outer conductor formed on the other surface of the dielectric substrate substantially parallel to each other, and one end of which is connected to the outer conductor. In a stripline filter including a plurality of inner conductors that form a short-circuited portion, a rod-shaped or plate-shaped dielectric is provided on the inner conductor at a position approximately ⅔ of the inner conductor length from the short-circuited portion. A strip line filter provided in close contact with a direction intersecting with the inner conductor.
JP3326622A 1991-11-14 1991-11-14 Stripline filter Expired - Fee Related JP2667604B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3326622A JP2667604B2 (en) 1991-11-14 1991-11-14 Stripline filter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3326622A JP2667604B2 (en) 1991-11-14 1991-11-14 Stripline filter

Publications (2)

Publication Number Publication Date
JPH05136602A true JPH05136602A (en) 1993-06-01
JP2667604B2 JP2667604B2 (en) 1997-10-27

Family

ID=18189860

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3326622A Expired - Fee Related JP2667604B2 (en) 1991-11-14 1991-11-14 Stripline filter

Country Status (1)

Country Link
JP (1) JP2667604B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2012023427A (en) * 2010-07-12 2012-02-02 New Japan Radio Co Ltd Distribution constant line type band-pass filter

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5646302A (en) * 1979-09-22 1981-04-27 Murata Mfg Co Ltd Strip line filter
JPS61100002A (en) * 1984-10-22 1986-05-19 Matsushita Electric Ind Co Ltd Plane type dielectric filter
JPS6390203A (en) * 1986-10-02 1988-04-21 Mitsubishi Electric Corp Dielectric filter

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5646302A (en) * 1979-09-22 1981-04-27 Murata Mfg Co Ltd Strip line filter
JPS61100002A (en) * 1984-10-22 1986-05-19 Matsushita Electric Ind Co Ltd Plane type dielectric filter
JPS6390203A (en) * 1986-10-02 1988-04-21 Mitsubishi Electric Corp Dielectric filter

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2012023427A (en) * 2010-07-12 2012-02-02 New Japan Radio Co Ltd Distribution constant line type band-pass filter

Also Published As

Publication number Publication date
JP2667604B2 (en) 1997-10-27

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