JPS58161402A - Distributed constant filter - Google Patents

Distributed constant filter

Info

Publication number
JPS58161402A
JPS58161402A JP4425882A JP4425882A JPS58161402A JP S58161402 A JPS58161402 A JP S58161402A JP 4425882 A JP4425882 A JP 4425882A JP 4425882 A JP4425882 A JP 4425882A JP S58161402 A JPS58161402 A JP S58161402A
Authority
JP
Japan
Prior art keywords
conductive film
dielectric
depth
dielectric block
coupling
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
JP4425882A
Other languages
Japanese (ja)
Other versions
JPS6340484B2 (en
Inventor
Hiroshi Tamura
博 田村
Sadahiro Tamura
禎啓 田村
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 JP4425882A priority Critical patent/JPS58161402A/en
Priority to GB08228112A priority patent/GB2109641B/en
Priority to DE19823236664 priority patent/DE3236664A1/en
Publication of JPS58161402A publication Critical patent/JPS58161402A/en
Publication of JPS6340484B2 publication Critical patent/JPS6340484B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01PWAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
    • H01P1/00Auxiliary devices
    • H01P1/20Frequency-selective devices, e.g. filters
    • H01P1/201Filters for transverse electromagnetic waves
    • H01P1/205Comb or interdigital filters; Cascaded coaxial cavities
    • H01P1/2056Comb filters or interdigital filters with metallised resonator holes in a dielectric block

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Control Of Motors That Do Not Use Commutators (AREA)

Abstract

PURPOSE:To reduce the insertion loss and to decrease the size and the coupling coefficient, by providing the depth of a through-hole toward the axial length, giving a recess and a cavity for the outer surface of a dielectric block and setting the degree of coupling between a couple of resonance units. CONSTITUTION:A fitting member 26 made of a conductor, e.g. metallic cylinder or conductive paste, is fixed to the other end of a conductive film 14 electrically and mechanically, and an opposing electrode 25 is fixed to the member 26 electrically and mechanically. The resonance frequency is decided with the electric length of the conductive film 13 or 14 reduced by the permeability of the dielectric 10. The two resonance units are coupled with the odd mode and the even mode. A through-cavity 27 has e.g. rectangular cross section. The recess or a groove 27a provided at the bottom has the depth DELTAt and the depth is decided for the objective value. In changing the value DELTAt/t, the degree of coupling is reduced without increasing the insertion loss by increasing the depth DELTAt.

Description

【発明の詳細な説明】 この発明は、たとえば数100MH2域で用いられる新
規な分布定数形フィルタに関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a novel distributed constant type filter used, for example, in the several 100 MH2 range.

従来、数100M)12域のフィルタとしては、LC共
振回路を用いたものや同軸共振器を用いたものがあった
が、構造的に不安定あるいは複雑であったり、特性的に
満足できない、調整に手間がかかる、1ストが引下げら
れない、などの問題点があった。
Conventionally, filters with several 100 M) 12 bands have been made using LC resonant circuits or coaxial resonators, but they are structurally unstable or complex, have unsatisfactory characteristics, and require adjustment. There were problems such as it took a lot of time and the first stroke could not be lowered.

そこで、構造が単純で、特性的にも満足できしかも低コ
ストの分布定数形フィルタが、本願発明者によって発明
され、出願(特願昭56−107548号)、された。
Therefore, the inventor of the present invention invented and filed an application (Japanese Patent Application No. 107548/1982) for a distributed constant type filter that has a simple structure, satisfactory characteristics, and low cost.

この先順発明の要旨は、少な1くとも二つの貫通孔を一
定間隔をおいて並んだ状態で誘電体ブロックに設け、こ
の貫通孔内面に導電膜を設けるとともに誘電体ブロック
の少なくとも西側面に導電膜を設け、貫通孔内面に設け
た導電膜と誘電体ブロックの少なくとも西側面に設けた
導電膜と、介在する誘電体とで共振ユニットを構成し、
少なくとも隣接する一対の共振ユニット簡の誘電体ブロ
ックに空洞を設け、さらに、外部回路と共振ユニットと
を静電結合させたことである。前記空洞は、一対の共振
ユニット藺の結合度の設定のために段けられる。
The gist of this prior invention is to provide a dielectric block with at least two through holes lined up at a constant interval, provide a conductive film on the inner surface of the through holes, and provide a conductive film on at least the west side of the dielectric block. a conductive film provided on the inner surface of the through hole, a conductive film provided on at least the west side of the dielectric block, and the intervening dielectric to constitute a resonant unit;
A cavity is provided in at least a pair of adjacent resonant unit dielectric blocks, and furthermore, an external circuit and the resonant unit are electrostatically coupled. The cavity is divided to set the degree of coupling between the pair of resonant units.

このような先願発明によると、結合係数が2%〜10%
程度の比較的広帯域のものができるが、結合係数が1〜
2%より小さい狭帯域のものは実用化できなかった。す
なわち、第11図において、aを0.5++ueから1
0mmへと大きくしていくと、第12図に示すように、
結合係数は10%から1%程度までは小さくなるがそれ
以下にはなかなかならず、一方、フィルタの挿入損失は
1dBから40dBといった具合に急増し、aを約31
以上にしたものは実用上フィルタとして用いることがで
きない。この場合、第11図における値Cを大きくする
とQ値が増大し、挿入損失の低下は抑えられるが形状が
つ小形で結合係数をさらに小さくできる分布定数形のフ
ィルタを提供することである。
According to such prior invention, the coupling coefficient is 2% to 10%.
It is possible to achieve a relatively wide band with a coupling coefficient of 1 to
A narrow band smaller than 2% could not be put to practical use. That is, in FIG. 11, a is changed from 0.5++ue to 1
When increasing to 0mm, as shown in Figure 12,
The coupling coefficient decreases from 10% to about 1%, but does not easily decrease below that level.On the other hand, the insertion loss of the filter rapidly increases from 1dB to 40dB, reducing a to about 31%.
The above configuration cannot be used as a filter in practice. In this case, if the value C in FIG. 11 is increased, the Q value increases, and the reduction in insertion loss is suppressed, but the object is to provide a distributed constant type filter that is small in shape and can further reduce the coupling coefficient.

すなわち、この発明の要旨は、少なくとも二つの貫通孔
を一定間隔をおいて並んだ状態で誘電体ブロックに設置
J 、この貫通孔内面に導電膜を設けるとともに誘電体
ブロックの少なくとも西側面に導電膜を設置−J、II
通孔内面に設けた導電膜と、誘電体ブロックの少なくと
も西側面に設けた導電膜と、介在する誘電体とで共振ユ
ニットを構成し、少なくとも隣接する一対の共振ユニッ
ト間において前&!貫通孔の軸長方向に深さをもたせて
誘電体ブロックの外表面に凹部を設けるとともに空洞を
設け、一対の共振ユニット間の結合度を設定したことを
特徴とする分布定数形フィルタである。
That is, the gist of the present invention is to install at least two through holes in a dielectric block in a line at a constant interval, provide a conductive film on the inner surface of the through holes, and provide a conductive film on at least the west side of the dielectric block. Installed - J, II
The conductive film provided on the inner surface of the through hole, the conductive film provided on at least the west side of the dielectric block, and the intervening dielectric constitute a resonant unit, and between at least a pair of adjacent resonant units, the front &! This distributed constant type filter is characterized in that a concave portion is provided on the outer surface of the dielectric block with a depth in the axial direction of the through hole, and a cavity is provided to set the degree of coupling between a pair of resonant units.

以下にこの発明の実施例について図面を参照しながら説
明する。
Embodiments of the invention will be described below with reference to the drawings.

第1図はこの発明の一実施例の等価回路図である。FIG. 1 is an equivalent circuit diagram of an embodiment of the present invention.

図において、1は入力端子、2は出力端子、3は入力結
合静電容量、4は出力結合静電容量、5゜6は1/4波
長共振回路を集中定数回路として示したものである。し
たがって、実施例は、1/4波長共振回路同士は誘導結
合され、外部回路と、1/4波長共振回路とが静電容■
結合されたフィルタである。第2図〜第7図はその具体
的構造の一例を示す。図において、10は酸化チタン系
のセラミック誘電体からなる立方体状の誘電体ブロック
、11.12は貫通孔で、一定間隔をおいて並んだ状態
で誘電体ブロック10に設けである。13.14はそれ
ぞれ貫通孔11.12の内面に設けた導電膜、15は、
誘電体ブロック10の少なくとも西側面に設けた導電膜
である。16は誘電体ブロック10の底面に設けた導電
膜であって、導電膜13.14の一端側と導電膜15を
短絡して1/4波長共振を生じさせるためのものである
。17は導電113の他端側に接続される入力結合用コ
ンデンサで、円柱状誘電体18に対向電極19.20を
有したものである。よりくわしくのべると、導電膜13
の他端側には、導電体たとえば金属内IJ体あるいは導
電ペーストからなる取付部材21を電気的かつ機械的に
接続固定してあり、対向電極20をこの取付部材21に
電気的かつ機械的に接続固定しである。22は導電膜1
4′の他端側に接続される出力結合用コンデンサで、円
柱状誘電体23に対向電極24.25を有したものであ
る。よりくわしくのべると、導電1!A14の他端側に
は導電体たとえば金属円柱体あるいは導電ペーストから
なる取付部材26を電気的かつ機械的に接続固定しCあ
り、対向電極25をこの取付部材26に電気的かつ機械
的に接続固定しである。誘電体10の誘電率によって短
縮された導電膜13あるいは14の電気長で共振周波数
が決定される。電気長は図示実施例のように、1/4波
長でもよいし1/2波長でもよい。1/2波長のときは
、導電$116は不要であ−る。なお、各図の導電膜、
電極■は理解のために強調された膜厚で描いている。い
ずれにしても、この実施例では二つの共振ユニットが構
成されている。各共振ユニットはオツドモード、イブ7
′モードによって結合されている。27は貫通空洞で、
−例としては断面長方形状である。27aは第2図にお
ける底面側に設けた凹部または溝で、溝27aの深さΔ
tで結合度を目標値に設定する。いま、第11図におい
て、a=2++mにしておき、第7図におけるΔ1./
lを変化させたときの状態を第13図に示す。グラフか
らもあきらかなように、深さΔtを深くすると、挿入損
失が増加することなく結合係数を小さくできる。この傾
向はaやその他の寸法が異なるものについてもいえる。
In the figure, 1 is an input terminal, 2 is an output terminal, 3 is an input coupling capacitance, 4 is an output coupling capacitance, and 5°6 is a 1/4 wavelength resonant circuit shown as a lumped constant circuit. Therefore, in the embodiment, the 1/4 wavelength resonant circuits are inductively coupled to each other, and the external circuit and the 1/4 wavelength resonant circuit have a capacitance of
It is a combined filter. FIGS. 2 to 7 show an example of its specific structure. In the figure, 10 is a cubic dielectric block made of a titanium oxide based ceramic dielectric, and 11 and 12 are through holes, which are arranged in the dielectric block 10 at regular intervals. 13 and 14 are conductive films provided on the inner surfaces of the through holes 11 and 12, respectively, and 15 are
This is a conductive film provided at least on the west side of the dielectric block 10. Reference numeral 16 denotes a conductive film provided on the bottom surface of the dielectric block 10, and is used to short-circuit one end side of the conductive films 13, 14 and the conductive film 15 to generate 1/4 wavelength resonance. Reference numeral 17 denotes an input coupling capacitor connected to the other end of the conductor 113, which has a cylindrical dielectric 18 and counter electrodes 19 and 20. In more detail, the conductive film 13
On the other end side, a mounting member 21 made of a conductor such as an IJ body in metal or a conductive paste is electrically and mechanically connected and fixed, and the counter electrode 20 is electrically and mechanically connected to this mounting member 21. The connection is fixed. 22 is a conductive film 1
4' is an output coupling capacitor connected to the other end side, and has counter electrodes 24 and 25 on a cylindrical dielectric body 23. In more detail, conductivity is 1! A mounting member 26 made of a conductor such as a metal cylinder or a conductive paste is electrically and mechanically connected and fixed to the other end of A14, and the counter electrode 25 is electrically and mechanically connected to this mounting member 26. It is fixed. The resonant frequency is determined by the electrical length of the conductive film 13 or 14, which is shortened by the dielectric constant of the dielectric 10. The electrical length may be 1/4 wavelength or 1/2 wavelength as in the illustrated embodiment. When the wavelength is 1/2, the conductivity of $116 is not necessary. In addition, the conductive film in each figure,
Electrode ■ is drawn with exaggerated film thickness for understanding. In any case, two resonant units are constructed in this embodiment. Each resonance unit is in Otsudo mode, Eve7
’ mode. 27 is a through cavity,
- Examples include rectangular cross-sections. 27a is a recess or groove provided on the bottom side in FIG. 2, and the depth of the groove 27a is Δ
The degree of coupling is set to a target value at t. Now, in FIG. 11, a=2++m, and Δ1. in FIG. /
FIG. 13 shows the state when l is changed. As is clear from the graph, by increasing the depth Δt, the coupling coefficient can be reduced without increasing the insertion loss. This tendency also applies to those having different dimensions such as a.

第8図は別の実施例を示し、上記実施例における入力結
合用コンデンナ17、出力結合用コンデンサ22を省略
しようとするものである。28は入力端子ビン、29は
出力端子ビンである。ビン28は、導電膜13に近接さ
せて、導電膜13からみて空洞27と反対側の誘電体ブ
ロック10部分に埋めこまれている。同様にビン29は
、導電膜14に近接させて、導電膜14からみて空洞2
7と反゛対側の誘電体ブロック10部分に埋めこまれて
いる。したがって、入力端子ビン28と導電膜13間に
は一定容量の静電容量が存在し、出力端子ビン29と導
1!躾14間にも一定容量の静電容量が存在することに
なる。この第8図示構造は、第2図〜第7図示構造のも
のよりコンデンサ2個が省略され、より構造が簡単にな
るとともにコストダウンが達成できる。第9図はさらに
別の実施例を水ず。
FIG. 8 shows another embodiment in which the input coupling capacitor 17 and the output coupling capacitor 22 in the above embodiment are omitted. 28 is an input terminal bin, and 29 is an output terminal bin. The bottle 28 is embedded in a portion of the dielectric block 10 on the opposite side of the cavity 27 when viewed from the conductive film 13 in close proximity to the conductive film 13 . Similarly, the bottle 29 is placed close to the conductive film 14 and has a cavity 2 when viewed from the conductive film 14.
It is embedded in a portion of the dielectric block 10 on the opposite side to the dielectric block 7. Therefore, a certain amount of capacitance exists between the input terminal pin 28 and the conductive film 13, and the output terminal pin 29 and the conductor 1! A certain amount of capacitance also exists between the capacitors 14. In the structure shown in FIG. 8, two capacitors are omitted compared to the structures shown in FIGS. 2 to 7, and the structure becomes simpler and costs can be reduced. FIG. 9 shows yet another embodiment of the water tank.

第9図の分布定数形フィルタにおいては、内面に導電膜
13,14を夫々形成した誘電体ブロック10の孔11
.12に、第10図に示すような誘電体ユニット41.
41を夫々圧入している。
In the distributed constant type filter shown in FIG.
.. 12, a dielectric unit 41 as shown in FIG.
41 are press-fitted respectively.

上記誘電体ユニット41は、第10図に示すように直径
が例えば0.5IllIlφの導線42の一部に、プラ
スチックあるいは酸化チタン系の誘電体材料等を被着し
て柱状に成形し、上記導線42が軸心部を貫通するよう
にしたものであって、上記誘電体ユニット41の先端部
には、誘電体ブロック10の孔11.12への圧入を容
易にするため、テーバ部43を設ける一方、上記誘電体
ユニット41の後端部には、誘電体ブロック10の上記
孔11.12の導電11115の非形成側の開口周縁に
当て止めされる7ランジ部44を設けている。
As shown in FIG. 10, the dielectric unit 41 is formed by covering a part of a conductive wire 42 having a diameter of, for example, 0.5IllIlφ with plastic or titanium oxide dielectric material and forming it into a columnar shape. 42 passes through the axial center, and a tapered portion 43 is provided at the tip of the dielectric unit 41 to facilitate press-fitting into the hole 11.12 of the dielectric block 10. On the other hand, the rear end portion of the dielectric unit 41 is provided with a seven flange portion 44 that rests on the opening periphery of the hole 11.12 of the dielectric block 10 on the side where the conductor 11115 is not formed.

上記誘電体ユニット41.41は、第9図に示すように
、そのテーパ部43.43側から、内面に導電膜13、
14を形成した誘電体ブロック10の、上記孔11.1
2に誘電体ユニット41.41の7ラン9部44.44
が誘電体ブロック10に当接するまで圧入している。
As shown in FIG. 9, the dielectric unit 41.41 has a conductive film 13 on the inner surface from the tapered portion 43.43 side.
Said hole 11.1 of the dielectric block 10 formed with 14
7 run 9 part 44.44 of dielectric unit 41.41 in 2
is press-fitted until it contacts the dielectric block 10.

上記のようにすれば、導線42.42と誘電体ブロック
10の孔11.12の内面に形成された導電1!13゜
14は、誘電体ユニット41.41の誘電体部分により
用コンデンサ17や出力結合用コンデンサ22は不要と
なる。
With the above arrangement, the conductive wires 42, 42 and the conductive wires 1!13°14 formed on the inner surface of the holes 11,12 of the dielectric block 10 can be connected to the capacitors 17 and 14 by the dielectric parts of the dielectric units 41,41. The output coupling capacitor 22 becomes unnecessary.

従って、入力結合用コンデンサ17や出力結合用コンデ
ンサ22の場合のような面倒な取付は作業の必要はなく
なる。
Therefore, there is no need for troublesome installation work as in the case of the input coupling capacitor 17 and the output coupling capacitor 22.

以上の実施例からもあきらかなように、この発明の分布
定数フィルタは、少なくとも二つの貫通孔を一定間隔を
おいて並んだ状態で誘電体ブロックに設け、この嘴通孔
内面に導電膜を設けるとともに誘電体ブロックの少なく
とも西側面に導電膜を設け、貫通孔内面に設けた導電膜
と、誘電体ブロックの少なくとも西側面に設けた導電膜
と、介在する誘電体とで共振ユニットを構成し、少なく
とも隣接する一対の共振ユニット間において前配興通孔
の軸長方向に深さをもたせて誘電体ブロックの外表面に
凹部を設けるとともに空洞を設け、一対の共振ユニット
間の結合度を設定したものであるから、挿入損失の増加
なしに、小形で狭帯域型のフィルタが得られる。
As is clear from the above embodiments, the distributed constant filter of the present invention has at least two through holes lined up at a constant interval in a dielectric block, and a conductive film is provided on the inner surface of the beak through hole. At the same time, a conductive film is provided on at least the west side of the dielectric block, and a resonant unit is constituted by the conductive film provided on the inner surface of the through hole, the conductive film provided on at least the west side of the dielectric block, and the intervening dielectric, At least between a pair of adjacent resonant units, a recess is provided on the outer surface of the dielectric block with a depth in the axial direction of the pre-arranged through hole, and a cavity is provided to set the degree of coupling between the pair of resonant units. As a result, a small, narrow-band filter can be obtained without increasing insertion loss.

なお、共振ユニットの段数は二段に限定されるものでは
なく、任意段設けることができるし、インターディジタ
ル形に共振ユニットを配設することもできる。
Note that the number of stages of resonance units is not limited to two stages, and any number of stages can be provided, and the resonance units can also be arranged in an interdigital configuration.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は、この発明の一実施例等価回路図、第2図は、
同、正面図、第3図は、同、左側面図、第4図は、同、
右側面図、第5図は、同、平面図第6図は、同、裏面図
、第7図は、同、断面図、第8図はいま一つの実施例の
断面図、第9図は、いま「つの実施例の断面図、第10
図は誘電体ユニットの正面図、第11図は従来例の寸法
図、第12図は従来例の特性図、第13図は本発明一実
施例の特性図である。 3は入力結合静電容量、4は出力結合静電容量5.6は
1/4波長共振回路、27は空洞、27aは凹部。 特  許  出  願  人 株式会社村田製作所 菌30    躬4m
FIG. 1 is an equivalent circuit diagram of an embodiment of the present invention, and FIG. 2 is an equivalent circuit diagram of an embodiment of the present invention.
Same, front view, Figure 3 is same, left side view, Figure 4 is same,
Figure 5 is a right side view, Figure 5 is a top view, Figure 6 is a back view, Figure 7 is a cross-sectional view, Figure 8 is a cross-sectional view of another embodiment, and Figure 9 is a cross-sectional view of another embodiment. , now ``Cross-sectional view of two embodiments, No. 10''
11 is a dimensional diagram of a conventional example, FIG. 12 is a characteristic diagram of a conventional example, and FIG. 13 is a characteristic diagram of an embodiment of the present invention. 3 is an input coupling capacitance, 4 is an output coupling capacitance 5.6 is a quarter wavelength resonant circuit, 27 is a cavity, and 27a is a recess. Patent application: Murata Manufacturing Co., Ltd. Bacteria 30 4m

Claims (1)

【特許請求の範囲】[Claims] 少なくとも二つの貫通孔を一定間隔をおいて並んだ状態
で誘電体ブロックに設け、この貫通孔内面に導電膜を設
けるとともに誘電体ブロックの少なくとも西側面に導電
膜を設け、貫通孔内面に設けた導電膜と、誘電体ブロッ
クの少な(とも西側面に設けた導電膜と、介在する誘電
体とで共振ユニットを構成し、少なくとも隣接する一対
の共振ユニット間において前記貫通孔の軸長方向に深さ
をもたせて誘電体ブロックの外表面に凹部を設けるとと
もに空洞を設け、一対の共振ユニット間の結合度を設定
したことを特徴とする分布定数形フィルタ。
At least two through holes are provided in a dielectric block in a lined manner at a constant interval, a conductive film is provided on the inner surface of the through hole, and a conductive film is provided on at least the west side of the dielectric block, and a conductive film is provided on the inner surface of the through hole. A conductive film and a small number of dielectric blocks (both the conductive film provided on the west side and the intervening dielectric constitute a resonant unit, and the depth in the axial length direction of the through hole is formed between at least a pair of adjacent resonant units. 1. A distributed constant type filter characterized in that a recess is provided on the outer surface of a dielectric block and a cavity is provided to set the degree of coupling between a pair of resonant units.
JP4425882A 1981-10-02 1982-03-18 Distributed constant filter Granted JPS58161402A (en)

Priority Applications (3)

Application Number Priority Date Filing Date Title
JP4425882A JPS58161402A (en) 1982-03-18 1982-03-18 Distributed constant filter
GB08228112A GB2109641B (en) 1981-10-02 1982-10-01 Distributed constant type filter
DE19823236664 DE3236664A1 (en) 1981-10-02 1982-10-04 DISTRIBUTION CONSTANT TYPE FILTER

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4425882A JPS58161402A (en) 1982-03-18 1982-03-18 Distributed constant filter

Publications (2)

Publication Number Publication Date
JPS58161402A true JPS58161402A (en) 1983-09-26
JPS6340484B2 JPS6340484B2 (en) 1988-08-11

Family

ID=12686485

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4425882A Granted JPS58161402A (en) 1981-10-02 1982-03-18 Distributed constant filter

Country Status (1)

Country Link
JP (1) JPS58161402A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61201501A (en) * 1985-03-04 1986-09-06 Mitsubishi Electric Corp High frequency filter
JPS62234402A (en) * 1986-04-04 1987-10-14 Matsushita Electric Ind Co Ltd Dielectric mounted filter
JPH0167804U (en) * 1987-10-24 1989-05-01

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57125001U (en) * 1981-01-30 1982-08-04

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57125001U (en) * 1981-01-30 1982-08-04

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61201501A (en) * 1985-03-04 1986-09-06 Mitsubishi Electric Corp High frequency filter
JPS62234402A (en) * 1986-04-04 1987-10-14 Matsushita Electric Ind Co Ltd Dielectric mounted filter
JPH0167804U (en) * 1987-10-24 1989-05-01

Also Published As

Publication number Publication date
JPS6340484B2 (en) 1988-08-11

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