JPS58145214A - Surface acoustic wave device - Google Patents

Surface acoustic wave device

Info

Publication number
JPS58145214A
JPS58145214A JP1598082A JP1598082A JPS58145214A JP S58145214 A JPS58145214 A JP S58145214A JP 1598082 A JP1598082 A JP 1598082A JP 1598082 A JP1598082 A JP 1598082A JP S58145214 A JPS58145214 A JP S58145214A
Authority
JP
Japan
Prior art keywords
electrode
chirp
surface acoustic
acoustic wave
wave device
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
JP1598082A
Other languages
Japanese (ja)
Other versions
JPH0247887B2 (en
Inventor
Takeshi Okamoto
猛 岡本
Shoichi Minagawa
皆川 昭一
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.)
Faurecia Clarion Electronics Co Ltd
Original Assignee
Clarion 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 Clarion Co Ltd filed Critical Clarion Co Ltd
Priority to JP1598082A priority Critical patent/JPS58145214A/en
Publication of JPS58145214A publication Critical patent/JPS58145214A/en
Publication of JPH0247887B2 publication Critical patent/JPH0247887B2/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
    • H03H9/14502Surface acoustic wave [SAW] transducers for a particular purpose
    • H03H9/14508Polyphase SAW 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
    • H03H9/02543Characteristics of substrate, e.g. cutting angles
    • H03H9/02574Characteristics of substrate, e.g. cutting angles of combined substrates, multilayered substrates, piezoelectrical layers on not-piezoelectrical substrate
    • 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
    • H03H9/14502Surface acoustic wave [SAW] transducers for a particular purpose
    • H03H9/14505Unidirectional SAW transducers
    • 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
    • H03H9/14502Surface acoustic wave [SAW] transducers for a particular purpose
    • H03H9/14514Broad band transducers

Landscapes

  • Physics & Mathematics (AREA)
  • Acoustics & Sound (AREA)
  • Surface Acoustic Wave Elements And Circuit Networks Thereof (AREA)
  • Length Measuring Devices Characterised By Use Of Acoustic Means (AREA)

Abstract

PURPOSE:To realize broad band characteristics, by providing a unidirectional transducer combining normal electrodes and chirp electrodes, taking one as the power feeding section and the other as the reflection section. CONSTITUTION:The normal form electrode 14 and the chirp electrode 15 are provided on the surface of an elastic substance substrate 13 so as to be orthogonal to the propagating direction X of the surface acoustic wave and both electrodes are arranged to contact at a vertical line Y-Y' on a common electrode 16. In using the normal form electrode 14 as the power feeding section and the chirp electrode 15 as the reflection section, a signal source 10 is connected to the electrode 14 via a matching circuit 11, a reactance circuit 12 is connected to the electrode 15, acting like the unidirectional transducer. Thus, the broad band characteristics are realized.

Description

【発明の詳細な説明】 本発明は、広帯琥特性の実現を可能ならしめる一方向性
トランスジューサを備えた弾性表面波装置に関するもの
である。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a surface acoustic wave device equipped with a unidirectional transducer that makes it possible to achieve broadband characteristics.

弾性体の平らな表面に沿ってエネルギーが集中した形で
伝搬する波いわゆる弾性表面波は、従来用いられている
バルク波に比較して・種々の点で優れているのでこの性
質を利用してフィルタを初めとする各種の電子部品に対
して弾性表面波デバイスとして適用されつつある。第1
図はその一例としてフィルタを示すもので、lは圧電体
基板、2は一対のすだれ状電極3A、3Bからなる入力
用トランスジューサ、4は一対のすだれ状電極5A。
Waves that propagate with concentrated energy along the flat surface of an elastic body, so-called surface acoustic waves, are superior in various respects to conventionally used bulk waves. Surface acoustic wave devices are being applied to various electronic components including filters. 1st
The figure shows a filter as an example, where 1 is a piezoelectric substrate, 2 is an input transducer consisting of a pair of interdigital electrodes 3A and 3B, and 4 is a pair of interdigital electrodes 5A.

5Bからなる出力用トランスジューサで、入力端子IN
から加えられた信号は上記入力用トランスジューサ2に
より弾性表面波に変換され、矢印で示すように圧電体基
板1表面を伝搬して上記出力用トランスジューサ4に到
達した後、電気信号に変換されて出力端子OUTから取
り出されるように構成される。
Output transducer consisting of 5B, input terminal IN
The input signal is converted into a surface acoustic wave by the input transducer 2, propagates on the surface of the piezoelectric substrate 1 as shown by the arrow, and reaches the output transducer 4, where it is converted into an electrical signal and output. It is configured to be taken out from the terminal OUT.

ところで第1図の構造の表面波デバイスのように、各々
一対のすだれ状電極3A、3Bおよび5A、5Bを含む
2個のトランスジューサ2.4を配置したフィルムにあ
っては、これらトランスジューサ2.4が各々左右の双
方向に表面波を伝搬させるように働くために電気−機械
変換損失が避けられずフィルタとして損失が多くなる欠
点がある。
By the way, in the case of a film in which two transducers 2.4 each including a pair of interdigital electrodes 3A, 3B and 5A, 5B are arranged, as in the surface wave device having the structure shown in FIG. Since each acts to propagate surface waves in both left and right directions, electro-mechanical conversion loss is unavoidable, and there is a drawback that the loss increases as a filter.

この欠点を除くために圧電体基板表面の一方向のみに表
面波を伝搬させるように工夫されたいわゆる一方向性ト
ランスジューサが提案された。この一方向性トランスジ
ューサの具体的構成としては第4図のように120”移
相器を用いる方法、あるいは虹移相器を用いる方法、さ
らには第3図のように反射器を用いる方法が知られてい
る。
In order to eliminate this drawback, a so-called unidirectional transducer has been proposed, which is designed to propagate surface waves only in one direction on the surface of a piezoelectric substrate. Specific configurations of this unidirectional transducer include a method using a 120" phase shifter as shown in Fig. 4, a method using a rainbow phase shifter, and a method using a reflector as shown in Fig. 3. It is being

第2図において6.6A、6Bはお互いに120“の位
相差なもった電極でそして6は他の電極6Aとの間に空
隙7あるいは絶縁膜が介在されるように構成されて表面
波を一方向のみに伝搬させるように働く。
In FIG. 2, 6.6A and 6B are electrodes having a phase difference of 120", and 6 is constructed such that a gap 7 or an insulating film is interposed between it and another electrode 6A to generate surface waves. It works to propagate in one direction only.

しかしながらこのように移相器を用いる方法は、上記の
よ5Th電極に交叉部分を設ける必要があるために製造
工程が複雑となる欠点がある。また所望特性を得るため
の移相器自体の設計も非常に複雑となるので調整が困難
となり、広帯域特性の実現が難かしいという問題がある
However, this method of using a phase shifter has the disadvantage that the manufacturing process is complicated because it is necessary to provide a crossing portion in the 5Th electrode as described above. Furthermore, the design of the phase shifter itself to obtain desired characteristics is extremely complicated, making adjustment difficult and making it difficult to achieve broadband characteristics.

一方、第3図において、8Aおよび8Bはすだれ状電極
の一部を構成するように設けられた給電部および反射部
でともに正規形電極からなっており、9は上記電極8A
、8Bに対する共通電極、10は信号源、・1】は整合
回路、12はリアクタンス回路である。以上において信
号源10から整合回路11を経て加えられた信号は上記
給電部8Aから弾性表面波とされて左右の双方向に伝搬
される。この時左方向に伝搬された表面波はりアクタン
ス回路12を接続した反射部8Bにより反射されて右方
向へ戻され、給電部8Aにおいて右方向へ向かう表面波
と反射された表面波との合成が行われる。この結果表面
波において中心周波数同士の場合は両波は重ね合わさる
が1、中心周波数からずれている場合は両波は打ち消し
合うように作用するためにPI的とする一方向と逆方向
に表面波が伝搬してしまうことになる。したがって表面
波の伝搬特性が狭帯域特性に制限される欠点がある。
On the other hand, in FIG. 3, 8A and 8B are a power feeding part and a reflecting part provided to constitute a part of the interdigital electrode, both of which are regular electrodes, and 9 is the electrode 8A.
, 8B, 10 is a signal source, .multidot.1 is a matching circuit, and 12 is a reactance circuit. In the above, the signal applied from the signal source 10 via the matching circuit 11 is converted into a surface acoustic wave from the power feeding section 8A and propagated in both left and right directions. At this time, the surface wave propagated in the left direction is reflected by the reflection section 8B connected to the actance circuit 12 and returned to the right direction, and the surface wave propagated in the right direction and the reflected surface wave are combined in the power feeding section 8A. It will be done. As a result, when the center frequencies of surface waves are the same, the two waves overlap, but when they deviate from the center frequency, the waves act to cancel each other out, so the surface waves move in the opposite direction to the PI direction. will be propagated. Therefore, there is a drawback that the propagation characteristics of the surface waves are limited to narrow band characteristics.

本発明は以上の問題に対処してなされたもので、正規形
電極とチャーブ電極とが並設され、一方の電極が給電部
として用いられると共に他方の電極が反射部として用い
られるように構成されたトランスジューサを備える弾性
表面波装置を提供することを目的とするものである。以
下図面を参照し゛C本発明実施例を説明する。
The present invention has been made in response to the above problems, and is configured such that a regular electrode and a chilblain electrode are arranged side by side, and one electrode is used as a power feeding section and the other electrode is used as a reflecting section. An object of the present invention is to provide a surface acoustic wave device including a transducer. Embodiments of the present invention will be described below with reference to the drawings.

第4図(al、 (b)は本発明実施例による弾性表面
波装置を示す概略上面図および概略断面図で、圧電体か
らなる弾性体基板13表面には電極周期が同等に形成さ
れた正規形電極14および電極周期が弾性表面波の伝搬
方向Xに対して変化するように形成されたチャープ電極
15が上記伝搬方向Xに垂直となるように設けられ、こ
れら両電極14.15は共通電極16上の垂直線Y−Y
’で接触するように配置される。ここで今、上記正規形
電極14ヲ給電部としてまたチャープ電極15ヲ反射部
として用いるとすると、給電部電極14には整合回路I
n介して信号源10が接続され、また反射部電極I5に
はりアクタンス回路12が接続される。
4(a) and 4(b) are a schematic top view and a schematic sectional view showing a surface acoustic wave device according to an embodiment of the present invention, in which regular electrodes are formed with equal electrode periods on the surface of an elastic substrate 13 made of a piezoelectric material. A shaped electrode 14 and a chirp electrode 15 formed so that the electrode period changes with respect to the propagation direction X of the surface acoustic wave are provided perpendicular to the propagation direction X, and these electrodes 14 and 15 are a common electrode. Vertical line Y-Y on 16
' are arranged so that they touch each other. Now, if the normal electrode 14 is used as a power supply part and the chirp electrode 15 is used as a reflection part, the power supply part electrode 14 is equipped with a matching circuit I.
A signal source 10 is connected to the reflector electrode I5, and an actance circuit 12 is connected to the reflector electrode I5.

以上において、上記給電部電極14から発生されて弾性
体基板13表面の左右方向に伝搬された弾性表面波のう
ち、左方向に伝搬された表面波はりアクタンス回路12
によって終端されている反射部電極15が存在している
ためにこの反射部電極15により反射されて再び右方向
に戻らされる。この時給電部電極14において表面波が
発生するとみなせる点(等測的表面波発生点)をCとし
て、この点(゛から前記両電極14. 15の接触線Y
−Yまでの距離’tlとすると、この距離lに対応した
トランジット角θ0は以下のように表わせる。
In the above, among the surface acoustic waves generated from the power feeding part electrode 14 and propagated in the left-right direction on the surface of the elastic substrate 13, the surface waves propagated in the left direction actance circuit 12.
Since there is a reflective part electrode 15 terminated by , the light is reflected by this reflective part electrode 15 and returned to the right again. At this time, the point (isometric surface wave generation point) at which a surface wave can be considered to be generated in the power supply electrode 14 is designated as C, and the contact line Y between the electrodes 14 and 15 from this point (゛)
If the distance to -Y is 'tl, then the transit angle θ0 corresponding to this distance l can be expressed as follows.

θQ・−2πf−l/fo・λ0 ここでfo:表面波の中心周波数 λ0:中心周波数の波長 N 、給電部電極の対数 f :動作周波数 またチャープ電極からなる反射部電極15は、その形状
的性質から表面波の反射点は動作周波数によって異なっ
てくる。今動作周波数fにおけるその反射点(等測的表
面波反射点)をDとして、この点りから上記接触線Y−
Yまでの距離な11とすると、この距離llに対応した
トランジット角θ1は以下のように表わせる。
θQ・−2πf−l/fo・λ0 where fo: center frequency of surface wave λ0: wavelength N of center frequency, logarithm of feeding section electrode f: operating frequency, and reflection section electrode 15 consisting of a chirp electrode is Due to its nature, the reflection point of surface waves differs depending on the operating frequency. Now let the reflection point (isometric surface wave reflection point) at the operating frequency f be D, and from this point the above contact line Y-
Assuming that the distance to Y is 11, the transit angle θ1 corresponding to this distance ll can be expressed as follows.

θl−2πf−ll/fO・λ0        ・・
・(2)ここで上記給電部電極14および反射部電極1
5を含むトランスジューサを一方向性として動作させる
には、給電部電極14から右方向に伝搬する表面波と左
方向に伝搬して反射部電極15により反射されて右方向
に戻ってきた表面波との位相を合わせる必要がある。こ
のためには反射して戻ってきた表面波のトランジット角
θが以下の式を満足するように反射部電極15(チャー
プ電極)を形成することが条件となる。
θl-2πf-ll/fO・λ0...
- (2) Here, the power feeding part electrode 14 and the reflecting part electrode 1
In order to operate the transducer including 5 as unidirectional, a surface wave propagating to the right from the feed electrode 14, a surface wave propagating to the left, reflected by the reflection electrode 15, and returning to the right. It is necessary to match the phase. For this purpose, it is necessary to form the reflective part electrode 15 (chirp electrode) so that the transit angle θ of the reflected and returned surface wave satisfies the following expression.

θ−(θ0+θ1)X2=2 n (2N+−)   
 −(3)以上の(1)〜(3)式tt a合すること
により以下の式が導かれる。
θ-(θ0+θ1)X2=2 n (2N+-)
-(3) By combining the above equations (1) to (3) tta, the following equation is derived.

このように上記式(3)および(4)を満足するように
反射部電極として動作するチャープ電極を設計すること
により、広い動作周波数範囲にわたって前記したような
両表面波の位相を合わせることができるので一方向性ト
ランスジューサとして動作させることができる。また以
上の条件ヲ満足するためのトランスジューサの電極形状
は周知のフォトエツチング技術を利用することにより容
易に製造することができる。さらにこのようにして形成
された反射部電極なりアクタンス回路により終端するこ
とでその調整も容易に行うことができるようになる。
By designing a chirp electrode that operates as a reflector electrode so as to satisfy equations (3) and (4) above, it is possible to match the phases of both surface waves as described above over a wide operating frequency range. Therefore, it can be operated as a unidirectional transducer. Furthermore, the electrode shape of the transducer that satisfies the above conditions can be easily manufactured using well-known photoetching techniques. Further, by terminating with the reflector electrode or actance circuit formed in this way, the adjustment can be easily performed.

第5図は本発明の他の実施例を示す概略上面図で、チャ
ープ電極15を給電部としてまた正規形電極1・1を反
射部として動作させる場合の構成を示すもので、給電部
電極15には整合回路1】を介して信号源10が接続さ
れ、また反射部電極14にはりアクタンス回路12が接
続される。この場合チャープ電極からなる給電部電極1
5はその形状的性質からその表面波発生点は動作周波数
により異なってくるが、正規形電極からなる反射部電極
14においてはすべての動作周波数に対して表面波反射
点は同一となる。そして前記実施例と同じ理由で、給電
都電$J+5から右方向に伝搬して反射部電極14によ
り゛反射されて左方向に戻された表面波は、発生点と同
一の給電部電極15位置に戻ってきて最初から左方向に
伝搬された表面波と位相が合わせられる。
FIG. 5 is a schematic top view showing another embodiment of the present invention, showing a configuration in which the chirp electrode 15 is operated as a power feeding section and the normal electrodes 1.1 are operated as a reflecting section. A signal source 10 is connected to the reflector electrode 14 via a matching circuit 1, and an actance circuit 12 is connected to the reflector electrode 14. In this case, the feeder electrode 1 consists of a chirp electrode.
5, the surface wave generation point differs depending on the operating frequency due to its geometrical properties, but in the reflecting part electrode 14 made of a regular electrode, the surface wave reflection point is the same for all operating frequencies. For the same reason as in the above embodiment, the surface wave that propagates to the right from the power supply streetcar $J+5, is reflected by the reflection section electrode 14, and returns to the left direction is located at the same position of the power supply section electrode 15 as the generation point. When it returns, it is matched in phase with the surface wave that was originally propagated to the left.

よってトランスジューサは左方向の一方向のみに表面波
を伝搬するように動作するので、同様な効果を得ること
ができる。
Therefore, the transducer operates so as to propagate the surface waves only in one direction, to the left, so that a similar effect can be obtained.

以上の各実施例ではチャーブ電極15とIE規形電極1
4とが垂直IIM(接触線)y−y’で接触している構
成の場合について述べたが、両電極が離れた場合でも前
記式(3)および(4)を満足する範囲内に配置されて
いれば一方向性トランスジューサとして動作させること
ができる。
In each of the above embodiments, the chirved electrode 15 and the IE square electrode 1
4 are in contact with each other at the vertical IIM (contact line) y-y'; If so, it can be operated as a unidirectional transducer.

なお弾性体基板13とし℃は圧電体に限らず、第6図(
a)〜(d)に示したように非圧電体基板17および圧
電膜18、あるいは金属膜19からなる組み合わせによ
って構成してもよい。
Note that the elastic substrate 13 is not limited to a piezoelectric material;
As shown in a) to (d), a combination of a non-piezoelectric substrate 17 and a piezoelectric film 18, or a metal film 19 may be used.

以上述べて明らかなように本発明によれは、正規形電極
とチャーブ電極とが並設され、−力の電極が給電部とし
て用いられると共に他方の電極が反射部として用いられ
るように一方向性トランスジューサを構成するものであ
るから、広帯域特性を実現することができる。また製造
工程がW5半となるために製造コストヲ低減することが
でき、さらに所望特性を得るための調整が容易となるの
でフィルタを初めとする各種の弾性表面波デバイスに広
範囲に適用することができる。
As is clear from the above description, according to the present invention, a normal electrode and a chilblain electrode are arranged side by side, and the unidirectional electrode is used as a power feeding part and the other electrode is used as a reflecting part. Since it constitutes a transducer, wideband characteristics can be achieved. In addition, since the manufacturing process is W5 and a half, manufacturing costs can be reduced, and adjustment to obtain desired characteristics is easy, so it can be widely applied to various surface acoustic wave devices such as filters. .

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

第1図乃至第3図はいずれも従来例を示す概略図、第4
図(a)および第5図は共に本発明実施例を示す概略上
面図、第4図(b)および第6図(a)〜(d)は共に
本発明実施例を示す概略断面図である。 10・・・信号源、 II・・・整合回路、12・・・
リアクタンス回路、13・・・弾性体基板、14・・・
正規形電極、15・・・チャープ電極、16・・共通電
極、17・・・非圧電体基板、18・・・圧電膜、19
・・・金属膜。 特許出願人  クラリオン株式会社 代理人 弁理士  永 1)武 三 部4 A ′ilJ囮 (G) 6 乍4囮
Figures 1 to 3 are all schematic diagrams showing conventional examples;
Figures (a) and 5 are both schematic top views showing an embodiment of the present invention, and Figures 4 (b) and 6 (a) to (d) are both schematic sectional views showing an embodiment of the present invention. . 10... Signal source, II... Matching circuit, 12...
Reactance circuit, 13... Elastic substrate, 14...
Regular electrode, 15... Chirp electrode, 16... Common electrode, 17... Non-piezoelectric substrate, 18... Piezoelectric film, 19
...Metal film. Patent applicant Clarion Co., Ltd. agent Patent attorney Nagai 1) Take 3 part 4 A ′ilJ decoy (G) 6 乍4 decoy

Claims (1)

【特許請求の範囲】 正規形電極とチャープ電極とが並設され、一方の電極が
給電部として用いられると共に他方の電極が反射部とし
て用いられるように構成されたトランスジューサを備え
ることを特徴とする弾性表面波装置。 2、 上記給電部電極に信号源が接続されると共に反射
部電極にりアクタンスが接続されてなることを特徴とす
る特許請求の範囲第1項記載の弾性表面波装置。 3、 上記正規形電極とチャープ電極との接触線からチ
ャープ電極の動作周波数に対応する点までの距離lが、 1−(渇4)2f−f、2゜ 28    f となるようにチャープ電極が形成されてなることを特徴
とする特許請求の範囲第1項又は第2頂He載の弾性表
面波装置。 4、 上記チャープ電極が反射部として用いられること
を特徴とする特許請求の範囲第1頌乃至第3項のいずれ
かに記載の弾性表面波装置。
[Claims] A transducer is characterized in that a regular electrode and a chirp electrode are arranged side by side, one electrode is used as a power feeding section, and the other electrode is used as a reflecting section. Surface acoustic wave device. 2. The surface acoustic wave device according to claim 1, wherein a signal source is connected to the power feeding part electrode, and an actance is connected to the reflecting part electrode. 3. The chirp electrode is set so that the distance l from the contact line between the normal electrode and the chirp electrode to the point corresponding to the operating frequency of the chirp electrode is 1-(4)2f-f, 2°28 f. A surface acoustic wave device mounted on the first or second apex He of claim 1 or 2, characterized in that the surface acoustic wave device is formed by: 4. The surface acoustic wave device according to any one of claims 1 to 3, wherein the chirp electrode is used as a reflecting section.
JP1598082A 1982-02-03 1982-02-03 Surface acoustic wave device Granted JPS58145214A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1598082A JPS58145214A (en) 1982-02-03 1982-02-03 Surface acoustic wave device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1598082A JPS58145214A (en) 1982-02-03 1982-02-03 Surface acoustic wave device

Publications (2)

Publication Number Publication Date
JPS58145214A true JPS58145214A (en) 1983-08-30
JPH0247887B2 JPH0247887B2 (en) 1990-10-23

Family

ID=11903827

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1598082A Granted JPS58145214A (en) 1982-02-03 1982-02-03 Surface acoustic wave device

Country Status (1)

Country Link
JP (1) JPS58145214A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5028831A (en) * 1990-04-04 1991-07-02 Motorola, Inc. SAW reflectionless quarter-wavelength transducers
US5162689A (en) * 1991-05-01 1992-11-10 Motorola, Inc. Single-phase uni-directional acoustic wave transducer

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS55154815A (en) * 1979-05-21 1980-12-02 Matsushita Electric Ind Co Ltd Elastic surface wave filter

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS55154815A (en) * 1979-05-21 1980-12-02 Matsushita Electric Ind Co Ltd Elastic surface wave filter

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5028831A (en) * 1990-04-04 1991-07-02 Motorola, Inc. SAW reflectionless quarter-wavelength transducers
US5162689A (en) * 1991-05-01 1992-11-10 Motorola, Inc. Single-phase uni-directional acoustic wave transducer

Also Published As

Publication number Publication date
JPH0247887B2 (en) 1990-10-23

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