JPH0630432B2 - Surface acoustic wave device - Google Patents
Surface acoustic wave deviceInfo
- Publication number
- JPH0630432B2 JPH0630432B2 JP22242787A JP22242787A JPH0630432B2 JP H0630432 B2 JPH0630432 B2 JP H0630432B2 JP 22242787 A JP22242787 A JP 22242787A JP 22242787 A JP22242787 A JP 22242787A JP H0630432 B2 JPH0630432 B2 JP H0630432B2
- Authority
- JP
- Japan
- Prior art keywords
- surface acoustic
- acoustic wave
- electrode
- propagation path
- idt
- 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.)
- Expired - Fee Related
Links
Landscapes
- Surface Acoustic Wave Elements And Circuit Networks Thereof (AREA)
Description
【発明の詳細な説明】 〔産業上の利用分野〕 本発明は弾性表面波の音響的結合を利用した弾性表面波
多重モードフィルタに関し、特に多重モードフィルタの
高性能化に関する。Description: TECHNICAL FIELD The present invention relates to a surface acoustic wave multimode filter that utilizes acoustic coupling of surface acoustic waves, and more particularly to improving the performance of a multimode filter.
従来、弾性表面波の音響的結合を利用した多重モードフ
ィルタはいろいろな構成が提案されており、例えばH.F.
Tierstenらが1975年にIEEE Ultrasonics Symposium(ウ
ルトラソニクスシンポジウム)第293〜294頁で報
告している。このタイプのフィルタ(第2図)の比帯域
は共振子の幅Wと共振子間距離Dで決まる。Conventionally, various configurations of multi-mode filters utilizing acoustic coupling of surface acoustic waves have been proposed.
Tiersten et al. Reported in 1975, IEEE Ultrasonics Symposium, pages 293-294. The bandwidth of this type of filter (FIG. 2) is determined by the width W of the resonator and the distance D between the resonators.
上述のパラメータWとDは、比帯域だけでなく、入力出
力インピーダンスも決めるため、現実的には自由度が極
めて低いという欠点がある。Since the above parameters W and D determine not only the ratio band but also the input output impedance, there is a drawback that the degree of freedom is extremely low in reality.
〔問題点を解決するための手段〕 上記欠点を解消するため、本発明の弾性表面波装置は、
圧電基板上に設けられ弾性表面波を励振する入力側交叉
指状電極と、前記弾性表面波の伝搬路上に配置された第
1のダミー電極と、前記弾性表面波の伝搬路と横結合す
るように前記伝搬路と垂直方向でかつ前記第1のダミー
電極と隣合うよう配置され、前記横結合で得られた弾性
表面波を受信する出力側交叉指状電極と、前記横結合で
得られた弾性表面波の伝搬路上でかつ前記入力側交叉指
状電極と隣合うよう配置された第2のダミー電極とから
構成されている。[Means for Solving Problems] In order to solve the above-mentioned drawbacks, the surface acoustic wave device of the present invention is
An input side interdigital electrode provided on the piezoelectric substrate for exciting the surface acoustic wave, a first dummy electrode arranged on the surface acoustic wave propagation path, and laterally coupled to the surface acoustic wave propagation path. In the direction perpendicular to the propagation path and adjacent to the first dummy electrode, and the output-side interdigital electrode that receives the surface acoustic wave obtained by the lateral coupling and the lateral coupling. The second dummy electrode is arranged on the propagation path of the surface acoustic wave and adjacent to the input side interdigital electrode.
次に、本発明の実施例について図面を参照して説明す
る。Next, embodiments of the present invention will be described with reference to the drawings.
まず、本発明の動作原理について説明する。First, the operating principle of the present invention will be described.
交叉指状電極(以下IDTと略す)は電極指幅がλ/4
のシングル電極の場合、電極部分と電極ない部分の音響
インピーダンスZm,Z0の比 で求まるインピーダンス不連続計数εと電極指本数Nの
積Nεが大きい場合、例えばNε>0.55の場合、各電極
指で生じる内部反射は無視できなくなり、そのIDTは
それ自身で共振子となることが知られている。このこと
は、例えばY.Koyamada et al.,"Narrow-band filters e
mploying surface-acorstic wave resonators"(ナロー
バンド・フィルターズ・エンプロイング・サーフェイス
−アコースティック・ウエイブ・レゾネーターズ)Pro
c.of IEEE,vol.64,NO.5,pp685-687に詳細に述べられて
いる。The interdigital electrode (hereinafter abbreviated as IDT) has an electrode finger width of λ / 4.
In case of a single electrode, the ratio of the acoustic impedances Z m and Z 0 of the electrode part and the part without electrode If the product Nε of the impedance discontinuity count ε and the number N of electrode fingers obtained by is large, for example, Nε> 0.55, the internal reflection generated at each electrode finger cannot be ignored and the IDT itself may become a resonator. Are known. This can be seen, for example, in Y. Koyamada et al., "Narrow-band filters e
mploying surface-acorstic wave resonators "(Narrow Band Filters Employing Surface-Acoustic Wave Resonators) Pro
c.of IEEE, vol.64, NO.5, pp685-687.
この共振子として動作するIDTを弾性表面波の伝搬方
向に2つ対向して配置させると、2つのIDTは結合
し、縦モード共振が生じ、フィルタ又は共振器として用
いることができる。このことは、山田他,“多対IDT
を用いた2端子対弾性表面波共振器,日本音響学会誌
33巻,10号(1977),pp557−564,に述べら
れている。When two IDTs that operate as the resonator are arranged so as to face each other in the propagation direction of the surface acoustic wave, the two IDTs are coupled to each other and longitudinal mode resonance occurs, which can be used as a filter or a resonator. This is due to Yamada et al., “Many-to-IDT”.
Two-Terminal Pair Surface Acoustic Wave Resonator Using a Magnetic Field, Journal of Acoustical Society of Japan
33, No. 10 (1977), pp 557-564.
この構成を示したのが第3図である。この図は最も基本
的なSAWフィルタの構成であるが、前述のNεを例え
ば0.55以上にすることで共振器として動作し、低損失な
共振器型フィルタとして用いることができる。This configuration is shown in FIG. Although this diagram shows the most basic SAW filter configuration, it can be used as a low-loss resonator type filter by operating as a resonator by setting Nε to 0.55 or more.
同様にして、2つのIDTを弾性表面波の伝搬方向に対
し垂直な横方向に近接配置させると、2つのIDTによ
る伝搬路間で音響的に横結合が生じる。これは、マイク
ロ波ストリップラインや光導波路でもよく知られた性質
である。ここで、これらIDTのNεが例えば0.55以上
であると、IDTは共振子として動作し2つのIDT間
の横モード結合により、2つのIDTを入力・出力とし
た共振器となる。この構成を示したものが第2図であ
る。第2図では、反射器22,23があるがこれはID
Tからもれ出るエネルギーをとじ込め、IDT自身の共
振を強めるためのものである。Similarly, when the two IDTs are arranged close to each other in the lateral direction perpendicular to the propagation direction of the surface acoustic wave, acoustic lateral coupling occurs between the propagation paths of the two IDTs. This is a well-known property in microwave strip lines and optical waveguides. Here, when Nε of these IDTs is, for example, 0.55 or more, the IDT operates as a resonator, and the transverse mode coupling between the two IDTs results in a resonator having two IDTs as input and output. FIG. 2 shows this configuration. In FIG. 2, there are reflectors 22 and 23, which are ID
This is to contain the energy leaking from T and strengthen the resonance of the IDT itself.
本発明は、以上述べた縦モードと横モードを同時に利用
することで、弾性表面波フィルタの高性能化を目指した
ものである。The present invention aims to improve the performance of a surface acoustic wave filter by simultaneously using the longitudinal mode and the transverse mode described above.
第1図は本発明の基本構成を示す。2つのIDT12,
14の横には、IDTの電極指を電気的に短絡させた以
外は全くIDTと同一構造のダミー電極13,15が配
置されている。ダミー電極13,15は他方のIDT1
4,12に対向している。このような構造において、例
えばIDT12で励振された弾性表面波は、IDT内で内
部反射をくり返しながらIDT12とダミー電極15で
構成された、第1図で向かって上側のグレーディング導
波路は伝搬しながら、IDT14とダミー電極13で構
成された、向かって下側のグレーティング導波路に横モ
ード結合し、エネルギーはIDT14に流れる。ここ
で、第1図の構成は第3図の縦モード構成を保ったま
ま、第2図の横モード構成を生じるため、従来単独でし
か用い得なかった縦モードと横モードを同時に用いるこ
とができることになり、縦モードと横モードの複合によ
る多重モード化により、従来より、広帯域な高性能フィ
ルタが実現できる。FIG. 1 shows the basic configuration of the present invention. Two IDTs 12,
Beside 14 are arranged dummy electrodes 13 and 15 having the same structure as the IDT except that the electrode fingers of the IDT are electrically short-circuited. The dummy electrodes 13 and 15 are the other IDT1
It faces 4,12. In such a structure, for example, the surface acoustic wave excited by the IDT 12 repeats internal reflection in the IDT and is propagated through the grading waveguide on the upper side in FIG. 1, which is composed of the IDT 12 and the dummy electrode 15. , IDT 14 and dummy electrode 13 are coupled laterally to the grating waveguide on the lower side, and energy flows to IDT 14. Here, since the configuration of FIG. 1 produces the transverse mode configuration of FIG. 2 while maintaining the longitudinal mode configuration of FIG. 3, it is possible to simultaneously use the longitudinal mode and the transverse mode, which could only be used conventionally. As a result, it becomes possible to realize a high-performance filter with a wider band than ever before by combining multiple modes of vertical mode and horizontal mode.
以上説明したように、本発明によればフィルタ設計の自
由度が高くなり、高帯域化できる。As described above, according to the present invention, the degree of freedom in filter design is increased and the band can be increased.
第1図は本発明の実施例を示す平面図、第2図、第3図
はそれぞれ従来の弾性表面波フィルタを示す平面図であ
る。 11,21,31……圧電基板、12,14,24,2
5,32,33……交叉指状電極、13,15……ダミ
ー電極、22,23……グレーティング電極。FIG. 1 is a plan view showing an embodiment of the present invention, and FIGS. 2 and 3 are plan views showing a conventional surface acoustic wave filter. 11, 21, 31 ... Piezoelectric substrate, 12, 14, 24, 2
5, 32, 33 ... Interdigitated electrodes, 13, 15 ... Dummy electrodes, 22, 23 ... Grating electrodes.
Claims (1)
る入力側交叉指状電極と、 前記弾性表面波の伝搬路上に配置された第1のダミー電
極と、 前記弾性表面波の伝搬路と横結合するように前記伝搬路
と垂直方向でかつ前記第1のダミー電極と隣合うよう配
置され、前記横結合で得られた弾性表面波を受信する出
力側交叉指状電極と、 前記横結合で得られた弾性表面波の伝搬路上でかつ前記
入力側交叉指状電極と隣合うよう配置された第2のダミ
ー電極とから構成されたことを特徴とする弾性表面波装
置。1. An input side interdigital electrode provided on a piezoelectric substrate for exciting a surface acoustic wave, a first dummy electrode arranged on a propagation path of the surface acoustic wave, and a propagation path of the surface acoustic wave. An output-side crossed finger-shaped electrode that is disposed in a direction perpendicular to the propagation path so as to be laterally coupled to and adjacent to the first dummy electrode, and that receives the surface acoustic wave obtained by the lateral coupling. A surface acoustic wave device comprising a second dummy electrode arranged on a propagation path of the surface acoustic wave obtained by coupling and adjacent to the input side interdigital electrode.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP22242787A JPH0630432B2 (en) | 1987-09-04 | 1987-09-04 | Surface acoustic wave device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP22242787A JPH0630432B2 (en) | 1987-09-04 | 1987-09-04 | Surface acoustic wave device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6465915A JPS6465915A (en) | 1989-03-13 |
| JPH0630432B2 true JPH0630432B2 (en) | 1994-04-20 |
Family
ID=16782224
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP22242787A Expired - Fee Related JPH0630432B2 (en) | 1987-09-04 | 1987-09-04 | Surface acoustic wave device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0630432B2 (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0438129U (en) * | 1990-07-26 | 1992-03-31 | ||
| CN119178505B (en) * | 2024-11-11 | 2025-04-18 | 杭州爱华仪器有限公司 | Electrostatic actuator for surface microphone and test method thereof |
-
1987
- 1987-09-04 JP JP22242787A patent/JPH0630432B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6465915A (en) | 1989-03-13 |
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