JPS60145704A - Dielectric filter - Google Patents

Dielectric filter

Info

Publication number
JPS60145704A
JPS60145704A JP221884A JP221884A JPS60145704A JP S60145704 A JPS60145704 A JP S60145704A JP 221884 A JP221884 A JP 221884A JP 221884 A JP221884 A JP 221884A JP S60145704 A JPS60145704 A JP S60145704A
Authority
JP
Japan
Prior art keywords
dielectric
input
output line
output
dielectric resonator
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.)
Pending
Application number
JP221884A
Other languages
Japanese (ja)
Inventor
Masayuki Ishizaki
石崎 正之
Toshiyuki Saito
俊幸 斉藤
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.)
Fujitsu Ltd
Original Assignee
Fujitsu 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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP221884A priority Critical patent/JPS60145704A/en
Publication of JPS60145704A publication Critical patent/JPS60145704A/en
Pending 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
    • H01P1/207Hollow waveguide filters
    • H01P1/208Cascaded cavities; Cascaded resonators inside a hollow waveguide structure

Abstract

PURPOSE:To prevent degradation of frequency characteristics by separating a dielectric substrate, where an input/output line constituted with microstrip lines is formed, and a substrate holding a dielectric resonator from each other. CONSTITUTION:Dielectric resonators 2 are held on a metallic plate 17 through dielectric substrates 11 having a low dielectric constant. Input/output parts 12 and 13 of the input/output line constituted with microstrip lines are formed on a dielectric substrate 10. For the purpose of extending the interval between coupling parts 14 and 15 of the input/output line, coupling parts are bent at right angles to input/output parts 12 and 13 and substrates 10 and 11 are separated from each other and are arranged and fixed. An end part (c) of the dielectric substrate 10 is cut while leaving a length (d) shorter than a used line width W as it is to couple the coupling part 14 and the dielectric resonator more close, thus obtaining characteristics having a wide fractional band.

Description

【発明の詳細な説明】 (81発明の技術分野 本発明は誘電体ろ波器に係り、特に誘電体共振器と結合
するマイクロ波集積回路で構成された入出力線路の結合
部に関するものである。
Detailed Description of the Invention (81) Technical Field of the Invention The present invention relates to a dielectric filter, and more particularly to a coupling section of an input/output line composed of a microwave integrated circuit coupled to a dielectric resonator. .

(b) 従来技術と問題点 最近、誘電体材料は盛んに開発が進められマイクロ波か
らミリ波に及ぶ周波数帯に於いて損失が少なく、温度特
性の良好なものが得られる様になってきた。
(b) Conventional technology and problems Recently, dielectric materials have been actively developed, and it has become possible to obtain materials with low loss and good temperature characteristics in the frequency band ranging from microwaves to millimeter waves. .

従来、高周波帯に於ける共振器は金属製の容器を使った
大きく且つ重い空洞共振器や同軸共振器であった。
Conventionally, resonators in high frequency bands have been large and heavy cavity resonators or coaxial resonators using metal containers.

これに反して、最近の誘電体共振器は小型軽量で構造が
簡単で、その上に加工費や材料費が安い為にマイクロ波
からミリ波に及ぶ周波数帯域でろ波器や発振器の安定化
共振器として広く使用される様になってきた。
On the other hand, recent dielectric resonators are small and lightweight, have a simple structure, and have low processing and material costs, so they can stabilize filters and oscillators in frequency bands ranging from microwaves to millimeter waves. It has come to be widely used as a vessel.

第1図はよ(使用される誘電体共振器の形状とその基本
共振モー1−に於L)る電磁界分布を示す。
FIG. 1 shows the electromagnetic field distribution depending on the shape of the dielectric resonator used and its fundamental resonance mode.

同図に示す様に、誘電体共振器の形状は円柱形と立方体
形が主として用いられる。その寸法は共振周波数に依っ
て異なり、例えは20GIIzの共振周波数を持つAγ
方体形の誘電体共振器の司法は約3X3 X (1−1
,5) mmである。
As shown in the figure, the shapes of the dielectric resonators are mainly cylindrical and cubic. Its dimensions vary depending on the resonant frequency, for example Aγ with a resonant frequency of 20GIIz
The square dielectric resonator has a diameter of approximately 3×3× (1-1
, 5) mm.

又、電磁界分布は同図に示す様に円柱形、立方体形共に
同一であるが、前者の場合はTEo1rモート、f&8
の場合はTEn6モートと云っている。
Also, as shown in the figure, the electromagnetic field distribution is the same for both the cylindrical and cubic shapes, but in the former case, the TEo1r moat, f&8
In this case, it is called TEn6 mote.

図中、■は電界が紙面上から下に抜けている状態を示し
、■はその逆である。
In the figure, ■ indicates a state in which the electric field passes from the top to the bottom of the paper, and ■ indicates the opposite.

第2図は入出力部が導波管の場合の誘電体共振器の配置
の状態を説明する為の図で、第2図telは導波管の上
面を、第2図(blは側面をそれぞれ取除いた場合の図
である。
Figure 2 is a diagram for explaining the arrangement of dielectric resonators when the input/output section is a waveguide. It is a figure when each is removed.

図中、■は横中へ×縦中Bの標準導波管部を、2は円柱
形の誘電体共振器を、3は横巾ax縦巾Bの遮断導波管
部をそれぞれ示す。
In the figure, ■ indicates a standard waveguide section with a width in the middle x a length in the middle, 2 indicates a cylindrical dielectric resonator, and 3 indicates a cutoff waveguide section with a width ax and a length B.

第2図telに於いて、横巾AX縦中Bの標準導波管部
1を伝播してきた導波管モートは横巾aX縦巾Bの遮断
導波管部3で遮断されこの中を伝播する事ができない。
In Fig. 2 tel, the waveguide moat propagating through the standard waveguide section 1 with width AX and length B is blocked by the blocking waveguide section 3 with width a and length B, and propagates therein. I can't do it.

しかし、この遮断導波管部3に配列・固定された誘電体
共振器2と共振した波だけがこの遮断導波管部3を通り
抜ける事ができる。
However, only waves that resonate with the dielectric resonators 2 arranged and fixed in this cut-off waveguide section 3 can pass through this cut-off waveguide section 3.

第3図は入出力線路部がマイクロストリップ線路で構成
された誘電体共振器の従来例を説明する為の図で、第3
図(alは平面図を、第3図(blは第3図talのA
−X断面図をそれぞれ示す。
Figure 3 is a diagram for explaining a conventional example of a dielectric resonator in which the input/output line portion is composed of a microstrip line.
Figure (al is the plan view, Figure 3 (bl is A of Figure 3 tal)
-X cross-sectional views are shown respectively.

図中、4は例えばアルミナ基板を、2は誘電体共振器を
、5は金属例えば金を蒸着して得られたマイクロストリ
ップ線路を、6は全面に金属を芸着した接地導体面をそ
れぞれ示す。
In the figure, 4 indicates, for example, an alumina substrate, 2 indicates a dielectric resonator, 5 indicates a microstrip line obtained by depositing a metal such as gold, and 6 indicates a ground conductor surface whose entire surface is coated with metal. .

第3図fatに示す様に、一枚の誘電体基板4の上には
誘電体共振器2が配列・固定されると共に、この誘電体
共振器と結合する入出力線路5及び7が形成される。そ
してマイクロストリップ線路5及び7は希望の中心周波
数に対して開放部より約λg/4離れた線路長の位置で
誘電体共振器2と磁界結合して誘電体ろ波器を構成して
いる。
As shown in FIG. 3, dielectric resonators 2 are arranged and fixed on one dielectric substrate 4, and input/output lines 5 and 7 coupled to the dielectric resonators are formed. Ru. The microstrip lines 5 and 7 are magnetically coupled to the dielectric resonator 2 at a line length distance of approximately λg/4 from the open portion with respect to a desired center frequency to form a dielectric filter.

第4図は第3図に示した誘電体ろ波器の周波数特性を示
す図で、実線の様に高い方の周波数で減衰(i;が少な
くなると共にb点でスプリアスモートによる共振が見ら
れる。
Figure 4 is a diagram showing the frequency characteristics of the dielectric filter shown in Figure 3.As shown by the solid line, attenuation (i;) decreases at higher frequencies, and resonance due to spurious moat can be seen at point b. .

これは、周波数が高くなると入力線路に加えられた電磁
波の一部が正規の伝播径路である誘電体共振器を迩ら一
→゛に誘電体基板4の内部を伝播したり、人力線路5の
先端部から間隔の狭い出力線路7の先端部に伝播される
為である。
This is because when the frequency increases, a part of the electromagnetic wave applied to the input line propagates through the dielectric resonator, which is the normal propagation path, inside the dielectric substrate 4, or on the human-powered line 5. This is because the signal is propagated from the tip to the tip of the output line 7, which has a narrow interval.

そのため、一枚の誘電体基板上にマイクロストリップ線
路を用いて構成した誘電体ろ波器は、周波数が高くなる
と希望の減衰特性が得られなくなると云う問題があった
Therefore, a dielectric filter constructed using a microstrip line on a single dielectric substrate has a problem in that desired attenuation characteristics cannot be obtained as the frequency increases.

面、この様な傾向はろ波器の次数の少ない場合は使用誘
電体共振器の数が少なくなる為に同し様な問題が発生す
る。
On the other hand, if the order of the filter is small, the number of dielectric resonators used will be small, and similar problems will occur.

tel 発明の目的 本発明は上記従来技術の問題に鑑みなされたも(dl 
発明の構成 上記発明の目的は一定空間内に少なくとも1 (fli
t以上のTEalE(TE++δ)モートを利用した誘
電体共振器及び該誘電体共振器と磁界結合する人出力線
路の結合部が配列・固定されてなる誘電体ろ波器に於い
て、マイクロストリップラインで構成された該入出力線
路の結合部が形成されている誘電体基板と該誘電体共振
器を保持する低誘電率誘電体基板とを分離する構造にし
た事を特徴とする誘電体ろ波器を提供する事により達成
される。
tel Object of the Invention The present invention has been made in view of the problems of the prior art described above.
Structure of the Invention The object of the above invention is to provide at least one (fli
In a dielectric filter in which a dielectric resonator using a TEalE (TE++δ) moat of t or more and a coupling part of a human output line that magnetically couples with the dielectric resonator are arranged and fixed, a microstrip line is used. A dielectric filter characterized by having a structure that separates a dielectric substrate on which a coupling part of the input/output line is formed and a low dielectric constant dielectric substrate holding the dielectric resonator. This is achieved by providing a vessel.

tel 発明の実施例 本発明は前記の様に誘電体共振器の周波数特性を劣化さ
せる原因となっている入出力線路の結合部間及び誘電体
基板内の直接結合を極力少な(する様に構成したもので
ある。
tel Embodiments of the Invention As mentioned above, the present invention is configured to minimize direct coupling between coupling parts of input/output lines and within a dielectric substrate, which causes deterioration of the frequency characteristics of a dielectric resonator. This is what I did.

のA−X断面図をそれぞれ示す。A-X cross-sectional views of each are shown.

図中、2は誘電体共振器を、10は誘電体基板を、工1
は低誘電率誘電体基板を、12及び13は入出力線路の
人出力部を、■4及び15は人出力線路の結合部を、1
6は接地導体面を、17は金属板をそれぞれ示す。
In the figure, 2 is a dielectric resonator, 10 is a dielectric substrate, and 1 is a dielectric resonator.
12 and 13 are the human output parts of the input/output lines; ■4 and 15 are the coupling parts of the human output lines;
Reference numeral 6 indicates a ground conductor surface, and reference numeral 17 indicates a metal plate.

同図に於て、入出力線路の結合部14と15との間隔を
広げる為に結合部は入出力線路の入出力部121(び1
3に苅して直角となる様に曲けると共に、入出力線路が
形成された誘電体基板(例えばアルミナ基板)10と誘
電体共振器を保持する低誘電率誘電体基板(例えば石英
)IIと1ま分離して配列・固定されている。
In the figure, in order to widen the distance between the coupling parts 14 and 15 of the input/output lines, the coupling parts are connected to the input/output parts 121 (and 1) of the input/output lines.
A dielectric substrate (e.g., alumina substrate) 10 on which input/output lines are formed, and a low-permittivity dielectric substrate (e.g., quartz) II holding the dielectric resonator. They are arranged and fixed separately.

第6図は結合部の部分を拡大した図で、第6図(8)は
平面図を、第6図+b)は第6図talのA−X断面図
を示す。尚、図中の記号は第5図の記号と同しである。
FIG. 6 is an enlarged view of the joint part, FIG. 6(8) is a plan view, and FIG. 6+b) is a sectional view taken along line A-X in FIG. Note that the symbols in the figure are the same as those in FIG.

同図に於いて、誘電体基板IOの端部Cはそこで使用す
る線路中Wよりも狭い間隔dを残して切断する事により
、結合部14と誘電体共振器との結合が密になり比帯域
の大きな特性が得られる。
In the same figure, by cutting the end C of the dielectric substrate IO leaving a spacing d narrower than the width W in the line used there, the coupling between the coupling part 14 and the dielectric resonator becomes denser, and A characteristic with a large band can be obtained.

第7図は本発明の別の実施例で、入出力線路の引出しを
互いにすらセで入出力線路の結合部の間隔を広くしてい
る。
FIG. 7 shows another embodiment of the present invention, in which the leads of the input and output lines are evenly spaced from each other to widen the interval between the coupling parts of the input and output lines.

尚、第5図及び第7図に示す誘電体ろ波器の周波数特性
を第4図点線に示すが、従来のものに比較して良好な特
性が得られた。
Incidentally, the frequency characteristics of the dielectric filter shown in FIGS. 5 and 7 are shown by the dotted line in FIG. 4, and better characteristics were obtained compared to the conventional filter.

tri 発明の詳細 な説明した様に、本発明によれは誘電体共振器と結合す
る人力線路と出力線路の結合部間のII口剛1を離すと
共に、誘電体共振器を保持する低誘電率誘電体基板と入
出力線路の結合部を形成する誘電体基板とを分離して希
望しない電値波の結合を減少する様にした。
As described in detail, the present invention provides a structure that separates the II opening 1 between the coupling portion of the human power line and the output line that are coupled to the dielectric resonator, and also provides a low dielectric constant for holding the dielectric resonator. The dielectric substrate and the dielectric substrate forming the coupling portion of the input/output line are separated to reduce the coupling of undesired electric value waves.

一方、誘電体基板の端部をそこに使用する結合部の線路
l】より狭い巾を残して切断する事により結合部と誘電
体共振器の結合を強くした為に良好な周波数特性を持つ
誘電体ろ波を得ることが出来た。
On the other hand, by cutting the end of the dielectric substrate while leaving a narrower width, the coupling between the coupling part and the dielectric resonator is strengthened, resulting in a dielectric with good frequency characteristics. I was able to get body filtering.

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

第1図は誘電体共振器の形状を説明する為の図を、第2
図は入出力部が導波管の場合の誘電体共振器の配置を説
明する為の図を、第3図は入出力線路部がマイクIIス
トリップ線路の場合の誘電体J(振器の従来の構成例を
説明する為の図を、第4図は第3図及び第6図又は第7
図に示す誘電体ろ波器の特性を示す図を、第5図は本発
明の一実施例を、第6図は第5図の人出力線路の結合部
の拡大図を、第7図は本発明の別の実施例をそれぞれ示
“1゜ 図中、2は誘電体共振器を、1oは誘電体基板を、II
は低誘電率誘電体基板を、12及び13は人出力線I?
δの入出力部を、14及び15は入出力線路の結合部を
、16は接地導体面を、17は金属板をそれぞれ示す。 蓼10 h′ 草2ざ (12) ネタ1図 (I2) 第4図 崗J−秋 草5図 α) 蓼ぎ口 と4) ’ (b) 5 第7図
Figure 1 is a diagram for explaining the shape of a dielectric resonator, and Figure 2 is a diagram for explaining the shape of a dielectric resonator.
The figure is a diagram for explaining the arrangement of dielectric resonators when the input/output section is a waveguide, and Figure 3 is a diagram for explaining the arrangement of dielectric resonators when the input/output line section is a microphone II strip line (conventional method for resonators). Figure 4 is a diagram for explaining an example of the configuration of Figure 3 and Figure 6 or Figure 7.
5 shows an embodiment of the present invention, FIG. 6 shows an enlarged view of the coupling part of the human output line in FIG. 5, and FIG. 7 shows the characteristics of the dielectric filter shown in FIG. Another embodiment of the present invention is shown in the figure "2", "2" is a dielectric resonator, "1o" is a dielectric substrate, and "II" is a dielectric resonator.
is a low dielectric constant dielectric substrate, and 12 and 13 are human output lines I?
14 and 15 are input/output line coupling parts, 16 is a ground conductor surface, and 17 is a metal plate. Grass 10 h' Grass 2 Za (12) Figure 1 (I2) Figure 4 Gang J - Autumn Grass 5 Figure α) Grass opening and 4) ' (b) 5 Figure 7

Claims (1)

【特許請求の範囲】 1、−電空間内に少なくとも1個以上のT E、、i 
(ゴEIIS)モートを利用した誘電体共振器及び該誘
電体共振器と磁界結合する入出力線路の結合部が配列・
固定されてなる誘電体ろ波器に於て、マイクロストリッ
プラインで構成された該入出力線路が形成されている誘
電体基板と該誘電体共振器を保持する低誘電率誘電体基
板とを分離する構造にした事を特徴とする誘電体ろ波器
。 2、マイクロストリップラインで構成された該入出力線
路は該誘電体共振器との結合する結合部と該結合部に直
角に接続された入出力部とから構成されている事を特徴
とする特許請求の範囲第1項記載の誘電体ろ波器。 3、該入出力線路が形成されている誘電体基板は該入出
力線路の結合部側の端部が該入出力線路の結合部の線路
11以内の巾を残して切断されている
[Claims] 1. - At least one T E,,i in the electric space
(GOEIIS) A dielectric resonator using a moat and a coupling part of an input/output line that magnetically couples with the dielectric resonator are arranged and
In a fixed dielectric filter, the dielectric substrate on which the input/output line composed of microstrip lines is formed is separated from the low dielectric constant dielectric substrate holding the dielectric resonator. A dielectric filter characterized by having a structure in which 2. A patent characterized in that the input/output line composed of a microstrip line is composed of a coupling part that couples with the dielectric resonator and an input/output part connected at right angles to the coupling part. A dielectric filter according to claim 1. 3. The dielectric substrate on which the input/output line is formed is cut at the end on the side where the input/output line is connected, leaving a width within the line 11 of the input/output line's connecting area.
JP221884A 1984-01-10 1984-01-10 Dielectric filter Pending JPS60145704A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP221884A JPS60145704A (en) 1984-01-10 1984-01-10 Dielectric filter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP221884A JPS60145704A (en) 1984-01-10 1984-01-10 Dielectric filter

Publications (1)

Publication Number Publication Date
JPS60145704A true JPS60145704A (en) 1985-08-01

Family

ID=11523216

Family Applications (1)

Application Number Title Priority Date Filing Date
JP221884A Pending JPS60145704A (en) 1984-01-10 1984-01-10 Dielectric filter

Country Status (1)

Country Link
JP (1) JPS60145704A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01137604U (en) * 1988-03-14 1989-09-20
US6052041A (en) * 1996-08-29 2000-04-18 Murata Manufacturing Co., Ltd. TM mode dielectric resonator and TM mode dielectric filter and duplexer using the resonator

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS519636B1 (en) * 1971-05-24 1976-03-29
JPS58120301A (en) * 1982-01-12 1983-07-18 Sony Corp Band pass filter

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS519636B1 (en) * 1971-05-24 1976-03-29
JPS58120301A (en) * 1982-01-12 1983-07-18 Sony Corp Band pass filter

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01137604U (en) * 1988-03-14 1989-09-20
US6052041A (en) * 1996-08-29 2000-04-18 Murata Manufacturing Co., Ltd. TM mode dielectric resonator and TM mode dielectric filter and duplexer using the resonator

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