JPS6114688B2 - - Google Patents

Info

Publication number
JPS6114688B2
JPS6114688B2 JP12961577A JP12961577A JPS6114688B2 JP S6114688 B2 JPS6114688 B2 JP S6114688B2 JP 12961577 A JP12961577 A JP 12961577A JP 12961577 A JP12961577 A JP 12961577A JP S6114688 B2 JPS6114688 B2 JP S6114688B2
Authority
JP
Japan
Prior art keywords
electrode
surface acoustic
acoustic wave
electrodes
present
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
Application number
JP12961577A
Other languages
Japanese (ja)
Other versions
JPS5463651A (en
Inventor
Jun Yamada
Takeshi Hazama
Yoshihiko Noro
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP12961577A priority Critical patent/JPS5463651A/en
Publication of JPS5463651A publication Critical patent/JPS5463651A/en
Publication of JPS6114688B2 publication Critical patent/JPS6114688B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03HIMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
    • H03H9/00Networks comprising electromechanical or electro-acoustic devices; Electromechanical resonators
    • H03H9/02Details
    • H03H9/125Driving means, e.g. electrodes, coils
    • H03H9/145Driving means, e.g. electrodes, coils for networks using surface acoustic waves
    • H03H9/14544Transducers of particular shape or position
    • H03H9/14547Fan shaped; Tilted; Shifted; Slanted; Tapered; Arched; Stepped finger transducers
    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03HIMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
    • H03H9/00Networks comprising electromechanical or electro-acoustic devices; Electromechanical resonators
    • H03H9/02Details
    • H03H9/02535Details of surface acoustic wave devices
    • H03H9/02818Means for compensation or elimination of undesirable effects
    • H03H9/02881Means for compensation or elimination of undesirable effects of diffraction of wave beam
    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03HIMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
    • H03H9/00Networks comprising electromechanical or electro-acoustic devices; Electromechanical resonators
    • H03H9/02Details
    • H03H9/125Driving means, e.g. electrodes, coils
    • H03H9/145Driving means, e.g. electrodes, coils for networks using surface acoustic waves
    • H03H9/14544Transducers of particular shape or position
    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03HIMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
    • H03H9/00Networks comprising electromechanical or electro-acoustic devices; Electromechanical resonators
    • H03H9/02Details
    • H03H9/125Driving means, e.g. electrodes, coils
    • H03H9/145Driving means, e.g. electrodes, coils for networks using surface acoustic waves
    • H03H9/14517Means for weighting
    • H03H9/1452Means for weighting by finger overlap length, apodisation

Description

【発明の詳細な説明】 本発明は、不要信号波を除去した弾性表面波フ
イルタに関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a surface acoustic wave filter that removes unnecessary signal waves.

弾性表面波フイルタは、一般に第1図に示すよ
うに、圧電性基板1の表面上に、電気信号を弾性
表面波に変換するための入力電極2、弾性表面波
の伝搬路4、および弾性表面波を再び電気信号に
変換するための出力電極3から構成される。5は
入力電極2に供給される高周波信号源、6は出力
電極3に接続される抵抗を示す。
Generally, as shown in FIG. 1, a surface acoustic wave filter has an input electrode 2 for converting an electric signal into a surface acoustic wave, a surface acoustic wave propagation path 4, and an elastic surface on the surface of a piezoelectric substrate 1. It consists of an output electrode 3 for converting waves back into electrical signals. Reference numeral 5 indicates a high frequency signal source supplied to the input electrode 2, and reference numeral 6 indicates a resistor connected to the output electrode 3.

入力または、出力電極としては、第2図に示す
ようなくし歯状電極7と8が互いに交差した構造
のすだれ状電極が通常使用される。この弾性表面
波フイルタの帯域内特性は、この入出力電極とし
て用いられるすだれ状電極の形状で決定される。
即ち、すだれ状電極の交差幅aを適当に変化させ
ることにより、所望のフイルタ特性を得られるこ
とは、既にシー・エス・ハートマン等(C.S・
Hartmann et.al,IEEE Trans.MTT−21,4,
162(1973))により、指摘されている通りであ
る。しかし、上記手法により、弾性表面波フイル
タを作成すると、トラツプ周波数において、大き
な不要信号応答を生じる。これは、すだれ状電極
の交差幅のうち、波長と同程度及びそれ以下の交
差幅より励起された弾性表面波が、一方向だけに
進行するのではなく、無指向性に近づき、回折効
果を生じるためであると考えられており、その解
析手法としては、ジー・ダブリユ・フアーネル等
(G・W・Farnell et.al.IEEE Trans.SU−18,
1,35(1971))の提唱したASPW法(Angular
Spectrum of Plane Wave Method)が一般に用
いられており、上記の弾性表面波の回折現象をよ
く説明している。そして、弾性表面波フイルタに
おけるこの回折効果を補償するために、従来は、
第1図において入力電極の開口長bと出力電極の
開口長cを適当な比でとつていたが(J.D.
Maines et.al.Electronics Lett.8,17(1972))、
この方法では弾性表面波フイルタの寸法が、長大
となり、装置として高価なものとなつてしまうと
いう不具合があつた。
As the input or output electrodes, interdigital electrodes having a structure in which interdigitated electrodes 7 and 8 cross each other as shown in FIG. 2 are usually used. The in-band characteristics of this surface acoustic wave filter are determined by the shape of the interdigital electrodes used as the input and output electrodes.
That is, it has already been shown by C.S. Hartman et al. (CS.
Hartmann et.al, IEEE Trans. MTT-21, 4,
162 (1973)). However, when a surface acoustic wave filter is created using the above method, a large unnecessary signal response occurs at the trap frequency. This is because the surface acoustic waves excited by the intersecting widths of the interdigital electrodes, which are equal to or smaller than the wavelength, do not propagate in only one direction, but approach omnidirectionality, causing diffraction effects. It is thought that this is due to the occurrence of
1, 35 (1971)) proposed the ASPW method (Angular
Spectrum of Plane Wave Method) is commonly used and provides a good explanation of the above-mentioned surface acoustic wave diffraction phenomenon. In order to compensate for this diffraction effect in surface acoustic wave filters, conventionally,
In Figure 1, the aperture length b of the input electrode and the aperture length c of the output electrode were set at an appropriate ratio (JD
Maines et.al.Electronics Lett.8, 17 (1972)),
This method has the disadvantage that the surface acoustic wave filter becomes long and large, making the device expensive.

本発明の目的は、前述のごとき弾性表面波の回
折現象により生じる不要信号を除去し、かつ、従
来技術の不具合を改善し、良効な周波数特性を有
する弾性表面波フイルタを提供することにある。
An object of the present invention is to provide a surface acoustic wave filter that eliminates unnecessary signals caused by the above-mentioned surface acoustic wave diffraction phenomenon, improves the problems of the prior art, and has good frequency characteristics. .

本発明の要点を以下に説明する。すだれ状電極
に高周波電圧を印加すると、その電極の交差幅と
同じ幅の弾性歪みを生じるわけであるが、従来の
電極構成(第2図)では、電極の開口面に沿つた
上記弾性歪みは一様分布となる。そして、その為
に電極交差幅が波長と同程度以下の場合、前述し
た如く回折効果を生じ、トラツプ周波数近傍で減
衰特性の劣化を起こす。そこで本発明は開口面に
沿つた電極交差部分に、中心に電極幅の太い分布
をもたせることにより、中心部の電界強度が強ま
り、そのため弾性歪みもまた中心に密に分布する
こととなり、それらの集合で生じる弾性表面波
は、中心部分に集中するので、回折効果が軽減出
来、良効な周波数特性を得られる。
The main points of the present invention will be explained below. When a high-frequency voltage is applied to the interdigital electrodes, an elastic strain with a width equal to the cross width of the electrodes is generated. However, in the conventional electrode configuration (Figure 2), the elastic strain along the opening surface of the electrodes is It becomes a uniform distribution. For this reason, when the electrode crossing width is less than or equal to the wavelength, a diffraction effect occurs as described above, causing deterioration of the attenuation characteristics near the trap frequency. Therefore, in the present invention, the electric field strength at the center is strengthened by providing a thick distribution of electrode width at the center of the electrode intersection portion along the aperture surface, and as a result, the elastic strain is also densely distributed at the center. Since the aggregated surface acoustic waves are concentrated at the center, the diffraction effect can be reduced and good frequency characteristics can be obtained.

本発明の一実施例の電極構成を第3図に示す。
図において、9は電極の中央部の幅を太くした、
いわゆる樽型電極を示す。
FIG. 3 shows an electrode configuration according to an embodiment of the present invention.
In the figure, 9 has a thicker width at the center of the electrode.
This shows a so-called barrel-shaped electrode.

本発明のよる樽型電極構成の弾性表面波フイル
タをテレビジヨン受信機の中間周波用フイルタと
して用いたときのフイルタ特性及びこれと比較す
るための従来の電極構成によるフイルタ特性を第
4図に示す。この場合の電極としては、入力、出
力電極とも15対の樽型電極で、開口長1700μ、入
力電極と出力電極は3400μ離して配置した。第4
図において曲線10は従来の電極構成によるフイ
ルタ特性であり、曲線11は本発明によるフイル
タ特性を示す。図よりわかるごとく、音声トラツ
プ周波数60.25MHz、及び映像トラツプ周波数
52.75MHzにおける減衰量は改善され、特に音声
トラツプ周波数における減衰量の改善は著しく、
このためトラツプ周波数における不要信号の発生
は大幅に阻止される。
FIG. 4 shows the filter characteristics when the surface acoustic wave filter with the barrel-shaped electrode configuration according to the present invention is used as an intermediate frequency filter of a television receiver, and the filter characteristics with a conventional electrode configuration for comparison. . The electrodes in this case were 15 pairs of barrel-shaped electrodes for both the input and output electrodes, with an aperture length of 1700μ, and the input and output electrodes were placed 3400μ apart. Fourth
In the figure, a curve 10 shows a filter characteristic with a conventional electrode configuration, and a curve 11 shows a filter characteristic according to the present invention. As you can see from the figure, the audio trap frequency is 60.25MHz, and the video trap frequency is 60.25MHz.
The attenuation at 52.75MHz has been improved, especially at the audio trap frequency.
Therefore, the generation of unnecessary signals at the trap frequency is largely prevented.

次に本発明の他の実施例の電極構成を第5図に
示す。第5図に示す電極12は電極の片側のみを
樽型にした形状のもので、このような形状でも相
当程度フイルタ特性の改善がはかれる。なお、更
に電極のうち一部分にのみ、樽型形状としても効
果が期待できる。
Next, FIG. 5 shows an electrode configuration of another embodiment of the present invention. The electrode 12 shown in FIG. 5 has a barrel shape on only one side of the electrode, and even with this shape, the filter characteristics can be improved to a considerable extent. Furthermore, effects can be expected even if only a portion of the electrode is shaped like a barrel.

以上のように、本発明によれば、トラツプ周波
数における減衰特性を著しく改善出来、従つてト
ラツプ周波数における不要信号を大幅に阻止する
ことができる。
As described above, according to the present invention, the attenuation characteristics at the trap frequency can be significantly improved, and therefore, unnecessary signals at the trap frequency can be largely blocked.

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

第1図は弾性表面波フイルタの従来の一般的な
構成を示す図、第2図は従来のすだれ状電極の構
造を示す図、第3図は本発明の一実施例の電極構
成を示す図、第4図は本発明によるフイルタ特性
の効果を従来との比較で表わす図、第5図は本発
明の他の実施例の電極構成を示す図である。 1:圧電性基板、2:入力電極、3:出力電
極、9:樽型電極、12:一部樽型の電極。
FIG. 1 is a diagram showing the conventional general configuration of a surface acoustic wave filter, FIG. 2 is a diagram showing the structure of a conventional interdigital electrode, and FIG. 3 is a diagram showing the electrode configuration of an embodiment of the present invention. , FIG. 4 is a diagram showing the effect of the filter characteristics according to the present invention in comparison with the conventional filter, and FIG. 5 is a diagram showing the electrode configuration of another embodiment of the present invention. 1: piezoelectric substrate, 2: input electrode, 3: output electrode, 9: barrel-shaped electrode, 12: partially barrel-shaped electrode.

Claims (1)

【特許請求の範囲】[Claims] 1 電気信号を弾性表面波に変換するすだれ状電
極と、これにより生じる弾性表面波を伝搬せしめ
る物質及び弾性表面波を電気信号に変換するすだ
れ状電極より構成された弾性表面波装置におい
て、すだれ状電極のうち、少くとも一部が樽形の
形状を有することを特徴とする弾性表面波装置。
1. In a surface acoustic wave device consisting of a comb-like electrode that converts an electrical signal into a surface acoustic wave, a material that propagates the generated surface acoustic wave, and a comb-like electrode that converts the surface acoustic wave into an electrical signal, A surface acoustic wave device characterized in that at least a part of the electrode has a barrel shape.
JP12961577A 1977-10-31 1977-10-31 Elastic surface wave device Granted JPS5463651A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP12961577A JPS5463651A (en) 1977-10-31 1977-10-31 Elastic surface wave device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP12961577A JPS5463651A (en) 1977-10-31 1977-10-31 Elastic surface wave device

Publications (2)

Publication Number Publication Date
JPS5463651A JPS5463651A (en) 1979-05-22
JPS6114688B2 true JPS6114688B2 (en) 1986-04-19

Family

ID=15013835

Family Applications (1)

Application Number Title Priority Date Filing Date
JP12961577A Granted JPS5463651A (en) 1977-10-31 1977-10-31 Elastic surface wave device

Country Status (1)

Country Link
JP (1) JPS5463651A (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57199316A (en) * 1981-06-01 1982-12-07 Maruyasu Kogyo Kk Surface acoustic wave filter
JP2664228B2 (en) * 1988-12-23 1997-10-15 株式会社日立製作所 Surface acoustic wave device
DE10135871B4 (en) * 2001-07-24 2012-10-25 Epcos Ag Surface wave converter with improved suppression of spurious excitation

Also Published As

Publication number Publication date
JPS5463651A (en) 1979-05-22

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