JPS6324708A - Surface acoustic wave filter - Google Patents

Surface acoustic wave filter

Info

Publication number
JPS6324708A
JPS6324708A JP16746086A JP16746086A JPS6324708A JP S6324708 A JPS6324708 A JP S6324708A JP 16746086 A JP16746086 A JP 16746086A JP 16746086 A JP16746086 A JP 16746086A JP S6324708 A JPS6324708 A JP S6324708A
Authority
JP
Japan
Prior art keywords
surface acoustic
acoustic wave
electrode
frequency
electrodes
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
JP16746086A
Other languages
Japanese (ja)
Inventor
Hiromi Yatsuda
博美 谷津田
Yoshihiko Takeuchi
嘉彦 竹内
Toichi Koda
国府田 東一
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.)
Japan Radio Co Ltd
Original Assignee
Japan Radio 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 Japan Radio Co Ltd filed Critical Japan Radio Co Ltd
Priority to JP16746086A priority Critical patent/JPS6324708A/en
Priority to GB8716588A priority patent/GB2193060B/en
Priority to CA000541984A priority patent/CA1271817A/en
Priority to US07/073,976 priority patent/US4878036A/en
Priority to FR878710021A priority patent/FR2601824B1/en
Priority to DE3723545A priority patent/DE3723545C2/en
Publication of JPS6324708A publication Critical patent/JPS6324708A/en
Pending legal-status Critical Current

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  • Surface Acoustic Wave Elements And Circuit Networks Thereof (AREA)

Abstract

PURPOSE:To obtain a band-pass filter having a desired frequency characteristics, by arranging a dot shape structure which makes an surface acoustic wave having a prescribed frequency reflect and scatter at a prescribed position between a pair of electrodes. CONSTITUTION:A scattered reflector 42 that is the dot shape structure arranged along the propagating direction of the surface acoustic wave, is formed at the prescribed position between an input electrode 20, and an output electrode 22. The surface acoustic wave passing each of channels A, B, C,... is synthesized and outputted if no scattered reflector 42 exists. However, for example, in case of arranging the scattered reflector 42 on the channel C, the surface acoustic wave passing the channel C is prevented from arriving at the output electrode 22 because it is reflected and scattered, and as a result, an output signal OUT has the frequency characteristic in which the surface acoustic wave in the neighborhood of a center frequency is missing.

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フィルタに関し、特に所望の周波数
特性を有する信号を取り出すことの出来る弾性表面波フ
ィルタに関する。
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a surface acoustic wave filter, and particularly to a surface acoustic wave filter that can extract signals having desired frequency characteristics.

(従来の技術) 従来技術に係る弾性表面波フィルタの例を第6図に示す
。このフィルタ旦は圧電体40表面上に入力電極加と出
力電極22とが形成されている。入力電極加は二つの共
通電極24a、24bを有し、共通電極2I4aには他
方の共通電極24 bに向けて互いの先端部が徐々に接
近した複数の電極指26 aが櫛歯状に形成されている
。一方、共通電極24 bには共通電極24 aに向け
て互いにその先端部が徐々に拡開した複数の電極指26
 bが櫛歯状に形成されている。そして、これらの電極
指26a、26bは相互に噛合するようにして配設され
ている。なお、出力電極nは入力電極加の場合と同様に
して一対の共通電極28a、28bを有し、これらの共
通電極28a、28bに形成された電極指30a、30
bは夫々入力電極20と同様の状態で配設されている。
(Prior Art) FIG. 6 shows an example of a surface acoustic wave filter according to the prior art. In this filter, an input electrode and an output electrode 22 are formed on the surface of a piezoelectric body 40. The input electrode has two common electrodes 24a and 24b, and the common electrode 2I4a has a plurality of electrode fingers 26a formed in a comb-teeth shape, the tips of which gradually approach each other toward the other common electrode 24b. has been done. On the other hand, the common electrode 24b has a plurality of electrode fingers 26 whose tips gradually widen toward the common electrode 24a.
b is formed in a comb-teeth shape. These electrode fingers 26a, 26b are arranged so as to mesh with each other. Note that the output electrode n has a pair of common electrodes 28a, 28b in the same manner as in the case of adding input electrodes, and electrode fingers 30a, 30 formed on these common electrodes 28a, 28b.
b are arranged in the same state as the input electrodes 20, respectively.

このように構成されたフィルタ6により得られる出力信
号OUTの周波数特性は第7図に示すような略矩形状と
なることが知られている。ここで、第7図において幅a
はフィルタ互により得られる通過周波数帯域幅であり、
この幅aは複数の電極指26 aおよび26b、または
30 aおよび30 bの最大間隔および最小間隔によ
り決定される。
It is known that the frequency characteristic of the output signal OUT obtained by the filter 6 configured in this manner has a substantially rectangular shape as shown in FIG. Here, in Fig. 7, the width a
is the pass frequency bandwidth obtained by filter rotation,
The width a is determined by the maximum and minimum spacing between the plurality of electrode fingers 26a and 26b or 30a and 30b.

(発明が解決しようとする問題点) しかしながら、このフィルタ6より得られる出力信号O
UTの周波数特性は単純な略矩形状であり、所望の複雑
な周波数特性を有する出力信号を得るためには、圧電体
4の表面上に異なる周波数特性を有する複数の入力電極
20および出力電極乙の対を配設し、それらの出力信号
を組み合わせる必要があった。そのためフィルタの構成
が複雑となり大きくなると云う欠点があった。また、所
望の周波数特性を有する出力信号を得るために、フィル
タ6をコイル、コンデンサ等から成るフィルタと組み合
わせることが考えられるが、外部の電気部品を必要とす
ることは構成がさらに複雑となる欠点がある。
(Problem to be solved by the invention) However, the output signal O obtained from this filter 6
The frequency characteristics of the UT are simple and approximately rectangular, and in order to obtain an output signal with the desired complex frequency characteristics, a plurality of input electrodes 20 and output electrodes with different frequency characteristics are placed on the surface of the piezoelectric body 4. It was necessary to arrange a pair of and combine their output signals. Therefore, there is a drawback that the configuration of the filter becomes complicated and large. Additionally, in order to obtain an output signal with desired frequency characteristics, it is conceivable to combine the filter 6 with a filter consisting of a coil, a capacitor, etc., but the disadvantage is that the configuration becomes more complicated as it requires external electrical components. There is.

このような欠点を解消する目的で、圧電体の表面上に形
成された一対の電極間の所定の箇所に1弾性表面波の一
部分を反射するグレーディング構造物を配設したことが
、特許類昭和60年第130,679号に開示されてい
る。
In order to eliminate such drawbacks, a grading structure that reflects a portion of one surface acoustic wave was disposed at a predetermined location between a pair of electrodes formed on the surface of a piezoelectric material, as disclosed in patents in the Showa era. No. 130,679 of 1960.

(問題点を解決するための手段) 本発明は、同様に前記の欠点を解消するために成された
もので、圧電体の表面上に形成した一対の電極のうち少
なくとも一方を8弾性表面波の伝搬方向と直交する方向
に沿って徐々に拡開および接近する櫛歯状電極で構成さ
れた弾性表面波フィルタにおいて、前記一対の電極間の
所定の箇所に所定周波数の弾性表面波を反射散乱させる
ドツト状構造物を配設したものである。
(Means for Solving the Problems) The present invention has been made in order to solve the above-mentioned drawbacks, and it is possible to use at least one of a pair of electrodes formed on the surface of a piezoelectric material using 8 surface acoustic wave waves. In a surface acoustic wave filter composed of comb-like electrodes that gradually expand and approach in a direction perpendicular to the propagation direction of It is equipped with dot-shaped structures that allow

(実施例) 第1図は本発明に係わる弾性表面波フィルタの一実施例
を示す平面図で、上は該弾性表面波フィルタを示し、4
は圧電体、20は入力電極。
(Embodiment) FIG. 1 is a plan view showing an embodiment of a surface acoustic wave filter according to the present invention, in which the surface acoustic wave filter is shown at the top, four
is a piezoelectric body, and 20 is an input electrode.

nは出力電極、 24a 、24b 、28i 、28
bは共通電極、 26a 、 26b 、 30a 、
 30bは電極指、42は散乱反射体である。圧電体4
0表面上に金属薄膜等から成る一対の入力電極加および
出力電極nが蒸着等によって形成されている。入力電極
20は、櫛歯状となった複数の電極指26 aを有する
共通電極24 aと、櫛歯状となった複数の電極指26
 bを有する共通電極24bとから構成され。
n is an output electrode, 24a, 24b, 28i, 28
b is a common electrode, 26a, 26b, 30a,
30b is an electrode finger, and 42 is a scattering reflector. Piezoelectric body 4
A pair of input and output electrodes made of a thin metal film or the like are formed on the surface of the substrate 0 by vapor deposition or the like. The input electrode 20 includes a common electrode 24a having a plurality of comb-shaped electrode fingers 26a, and a plurality of comb-shaped electrode fingers 26a.
and a common electrode 24b having a common electrode 24b.

これらの電極指26a、26bが互いに噛合するように
配設される。この場合、一方の複数の電極指26 aの
先端部間は共通電極24 bに向けて徐々に接近し、他
方の複数の電極指26 bの先端部間は共通電極24 
aに向けて徐々に拡開するよう形成する。出力電極ηは
複数の電極指30aを有する共通電極28 aと複数の
電極指30bを有する共通電極28 bとから構成され
ており、入力電極加と同様の形状で圧電体4の表面上に
配設される。
These electrode fingers 26a, 26b are arranged so as to mesh with each other. In this case, the tips of one of the plurality of electrode fingers 26a gradually approach the common electrode 24b, and the tips of the other plurality of electrode fingers 26b approach the common electrode 24b.
It is formed so that it gradually expands toward a. The output electrode η is composed of a common electrode 28a having a plurality of electrode fingers 30a and a common electrode 28b having a plurality of electrode fingers 30b, and is arranged on the surface of the piezoelectric body 4 in the same shape as the input electrode. will be established.

これらの電極指26a 、 26b 、 30aおよび
30 bは。
These electrode fingers 26a, 26b, 30a and 30b are.

入力電極加と出力電極22との間の弾性表面波の伝搬方
向Tと略直交する方向に指向して配役される。
It is arranged to be oriented in a direction substantially perpendicular to the propagation direction T of the surface acoustic wave between the input electrode and the output electrode 22.

一方、入力電極冗と出力電極22との間の所定位置には
弾性表面波の伝搬方向Tと直交する方向に指向し、伝搬
方向Tに沿って配設されたドツト状構造物である散乱反
射体42が形成される。
On the other hand, at a predetermined position between the input electrode 22 and the output electrode 22, there is a scattering reflector which is a dot-shaped structure oriented in a direction perpendicular to the propagation direction T of the surface acoustic wave and arranged along the propagation direction T. A body 42 is formed.

この散乱反射体42は入力電極加および出力電極nと同
一の金属薄膜等より成り、これらの電極印、22と同時
に蒸着等によって形成すると好適である。
This scattering reflector 42 is made of the same metal thin film as the input electrode and the output electrode n, and is preferably formed by vapor deposition or the like at the same time as these electrode marks 22.

散乱反射体42を形成するドツト状構造物のドツト形状
としては、四角形状のものや円形状のものなど種々考え
られる。第2図はドツト構造物のドツト形状の一例を示
す図である。第2図において1弾性表面波の伝搬方向T
に対して散乱反射体42のドツトの間隔を一定に保ち、
かつ弾性表面波の%波長の整数倍に合わせれば1反射散
乱の効率が最良となる。
Various dot shapes can be considered for the dot-like structure forming the scattering reflector 42, such as a square shape and a circular shape. FIG. 2 is a diagram showing an example of the dot shape of the dot structure. In Fig. 2, the propagation direction T of one surface acoustic wave is
The distance between the dots of the scattering reflector 42 is kept constant,
If the wavelength is set to an integral multiple of the % wavelength of the surface acoustic wave, the efficiency of 1 reflection and scattering becomes the best.

また、第2図に示すように、ドツトの形状を弾性表面波
の伝搬方向Tに対して直交する方向から傾斜させておけ
ば、該散乱反射体42で反射した弾性表面波を入力電極
20で受信することがなく1周波数特性の劣化の原因の
一つを取り除くことが出来ろ。
Furthermore, as shown in FIG. 2, if the shape of the dot is inclined from a direction perpendicular to the propagation direction T of the surface acoustic wave, the surface acoustic wave reflected by the scattering reflector 42 can be transmitted to the input electrode 20. It would be possible to remove one of the causes of deterioration of the frequency characteristics without receiving signals.

(作 用) 第1図において、入力電極20の共通電極24a。(for production) In FIG. 1, the common electrode 24a of the input electrodes 20.

24 b間に入力信号INが印加されると、圧電体4は
圧電効果によって振動し、その振動が圧電体4の表面上
を弾性波として伝搬し、出力電極nに到達する。ここで
、出力電極nに伝搬される弾性表面波の周波数帯域は、
前述したように。
When an input signal IN is applied between 24b and 24b, the piezoelectric body 4 vibrates due to the piezoelectric effect, and the vibration propagates on the surface of the piezoelectric body 4 as an elastic wave and reaches the output electrode n. Here, the frequency band of the surface acoustic wave propagated to the output electrode n is
As previously mentioned.

入力電極孔および出力電極22における複数の電極指2
6 aおよび26b、または3Qaおよび30bの最大
間隔および最小間隔に依存する。入力電極孔と出力電極
nとの間における弾性表面波の伝搬域を、第1図に示す
ように伝搬方向Tと平行な複数のチャンネルに分割した
場合、各々のチャンネルA、B、C,D、・・・・・・
では、夫々中心周波数の異なる正規型周波数分布の弾性
表面波が伝搬される。これらの各チャンネルA、B、C
A plurality of electrode fingers 2 in the input electrode hole and the output electrode 22
Depending on the maximum and minimum spacing of 6a and 26b or 3Qa and 30b. When the propagation region of the surface acoustic wave between the input electrode hole and the output electrode n is divided into a plurality of channels parallel to the propagation direction T as shown in Fig. 1, each channel A, B, C, D ,・・・・・・
In this case, surface acoustic waves having normal frequency distributions with different center frequencies are propagated. Each of these channels A, B, C
.

D、・・・・・ を通過する弾性表面波を出力電極nに
より電気信号に変換して得られろ出力信号OUTの周波
数特性は、散乱反射体42が存在しなげれば、各チャン
ネルA、B、C,D、・・・・・・を通過する弾性表面
波が合成され、第7図に示す特性になる。
If the scattering reflector 42 is not present, the frequency characteristics of the output signal OUT obtained by converting the surface acoustic waves passing through the channels A, . The surface acoustic waves passing through B, C, D, . . . are synthesized, resulting in the characteristics shown in FIG.

しかしながら1本実施例では入力型極印と出力電極nと
の間の例えばチャンネルCに散乱反射体42を配設して
いる。従って、このチャンネルCを通過する弾性表面波
は、散乱反射体42によって反射散乱されるため出力電
極22に到達することがなく、出力電極nより得られる
出力信号OUTは、チャンネルCに相当する中心周波数
の近傍の弾性表面波が欠落した周波数特性を有すること
となる。
However, in this embodiment, a scattering reflector 42 is disposed, for example, in the channel C between the input type pole mark and the output electrode n. Therefore, the surface acoustic waves passing through this channel C are reflected and scattered by the scattering reflector 42 and do not reach the output electrode 22, and the output signal OUT obtained from the output electrode n is at the center corresponding to the channel C. The surface acoustic waves near the frequency will have a missing frequency characteristic.

第3図はこの時の周波数特性を示すものであり。FIG. 3 shows the frequency characteristics at this time.

bは反射された周波数阻止域を示す。このような周波数
阻止域すを有する周波数特性は1例えばテレビ信号の映
像帯域中の音声信号を除去するためのノツチフィルタと
して有効に活用し得るものである。
b indicates the reflected frequency stopband. A frequency characteristic having such a frequency stop band can be effectively utilized as a notch filter for removing an audio signal in the video band of a television signal, for example.

(他の実施例) 第4図は本発明に係わる弾性表面波フィルタの他の実施
例を示す平面図で、2は該弾性表面波フィルタを示し、
4は圧電体、20は入力電極22は出力電極、 44 
、46は散乱反射体である。入力電極孔および出力電極
22の構造は第1図に示すものと同一である。第4図に
おいて、入力電極20と出力電極nとの間には1弾性表
面波の伝搬域の異なるチャンネルに、散乱反射体44 
、46の二つのドツト状構造物を配設している。この実
施例では、二つの異なる周波数の近傍の弾性 2表面波
は散乱反射体44 、46によって夫々反射散乱され、
第5図に示すような二つの周波数阻止域c、dを有する
周波数特性を得ることが出来る。
(Other Embodiments) FIG. 4 is a plan view showing another embodiment of the surface acoustic wave filter according to the present invention, and 2 indicates the surface acoustic wave filter,
4 is a piezoelectric body, 20 is an input electrode 22 is an output electrode, 44
, 46 are scattering reflectors. The structure of the input electrode hole and the output electrode 22 is the same as that shown in FIG. In FIG. 4, between the input electrode 20 and the output electrode n, a scattering reflector 44 is provided between channels in different propagation regions of surface acoustic waves.
, 46 are arranged. In this embodiment, two nearby elastic surface waves with different frequencies are reflected and scattered by the scattering reflectors 44 and 46, respectively.
A frequency characteristic having two frequency stopbands c and d as shown in FIG. 5 can be obtained.

(発明の効果〕 以上本発明によれば1弾性表面波の伝搬方向と直交する
方向に沿って、徐々に拡開および接近する櫛歯状の電極
で構成された弾性表面波フィルタの一対の電極間の所定
の箇所に1弾性表面波の一部を反射散乱させるドツト状
構造物を配設したことにより、任意の周波数の信号を除
去することが出来る等、所望の周波数特性を有する帯域
通過フィルタが得られる利点がある。
(Effects of the Invention) According to the present invention, a pair of electrodes of a surface acoustic wave filter are constructed of comb-shaped electrodes that gradually expand and approach each other along a direction perpendicular to the propagation direction of surface acoustic waves. By arranging a dot-shaped structure that reflects and scatters a portion of one surface acoustic wave at a predetermined location between the two, it is possible to remove signals of any frequency, thereby creating a bandpass filter that has desired frequency characteristics. There are advantages that can be obtained.

またドツト状に構成された構造物の散乱反射体は、入力
電極および出力電極と共に蒸着等により同時に製作する
ことが出来るので、製造コストが安く、外部に電気部品
を付加することなく。
Further, the scattering reflector having a dot-shaped structure can be manufactured simultaneously with the input electrode and the output electrode by vapor deposition, etc., so the manufacturing cost is low and there is no need to add any external electrical parts.

複雑な周波数特性のフィルタを実現することが出来る等
の利点がある。
It has advantages such as being able to realize a filter with complex frequency characteristics.

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

第1図は本発明に係わる弾性表面波フィルタの一実施例
を示す平面図、第2図は本発明に係わるドツト状構造物
のドツト形状の一例を示す図、第3図は第1図に示すフ
ィルタの周波数特性図、第4図は本発明に係わる弾性表
面波フィルタの他の実施例を示す平面図、第5図は第1
1図に示すフィルタの周波数特性図、第6図は従来技術
に係わる弾性表面波フィルタの平面図。 第7図は第6図に示すフィルタの周波数特性図である。 1,2.6・・・フィルタ、4・・・圧電体、20・・
・入力電極、22.、、出力電極、 24a 、24b
 、28a 、28b・・・共通電極+ 26a +2
6b 、30a 、30b ・・・電極指。 42 、44 、46・・・散乱反射体。
FIG. 1 is a plan view showing an embodiment of the surface acoustic wave filter according to the present invention, FIG. 2 is a diagram showing an example of the dot shape of the dot-shaped structure according to the present invention, and FIG. 3 is similar to FIG. FIG. 4 is a plan view showing another embodiment of the surface acoustic wave filter according to the present invention, and FIG. 5 is a frequency characteristic diagram of the filter shown in FIG.
1 is a frequency characteristic diagram of the filter shown in FIG. 1, and FIG. 6 is a plan view of a surface acoustic wave filter according to the prior art. FIG. 7 is a frequency characteristic diagram of the filter shown in FIG. 6. 1, 2.6...filter, 4...piezoelectric body, 20...
- Input electrode, 22. ,,output electrode, 24a, 24b
, 28a, 28b... common electrode + 26a +2
6b, 30a, 30b...electrode fingers. 42, 44, 46... scattering reflector.

Claims (2)

【特許請求の範囲】[Claims] (1)圧電体の表面に形成した一対の電極のうち少なく
とも一方を弾性表面波の伝搬方向と直交する方向に沿っ
て徐々に拡開および接近する櫛歯状の電極に形成し、所
定の周波数特性を有する信号を取り出す弾性表面波フィ
ルタにおいて、前記一対の電極間の所定の箇所に所定周
波数の弾性表面波を反射散乱させるドット状の散乱反射
体を配設したことを特徴とする弾性表面波フィルタ。
(1) At least one of the pair of electrodes formed on the surface of the piezoelectric body is formed into a comb-shaped electrode that gradually expands and approaches along the direction orthogonal to the propagation direction of the surface acoustic wave, and A surface acoustic wave filter for extracting a signal having a characteristic, characterized in that a dot-shaped scattering reflector that reflects and scatters surface acoustic waves of a predetermined frequency is disposed at a predetermined location between the pair of electrodes. filter.
(2)特許請求の範囲第1項のドット状の散乱反射体を
弾性表面波の伝搬方向に対して直交する方向から傾斜し
て配設したことを特徴とする弾性表面波フィルタ。
(2) A surface acoustic wave filter characterized in that the dot-shaped scattering reflectors according to claim 1 are arranged at an angle from a direction perpendicular to the propagation direction of surface acoustic waves.
JP16746086A 1986-07-16 1986-07-16 Surface acoustic wave filter Pending JPS6324708A (en)

Priority Applications (6)

Application Number Priority Date Filing Date Title
JP16746086A JPS6324708A (en) 1986-07-16 1986-07-16 Surface acoustic wave filter
GB8716588A GB2193060B (en) 1986-07-16 1987-07-14 Surface elastic wave filter
CA000541984A CA1271817A (en) 1986-07-16 1987-07-14 Surface elastic wave filter
US07/073,976 US4878036A (en) 1986-07-16 1987-07-15 Surface elastic wave filter
FR878710021A FR2601824B1 (en) 1986-07-16 1987-07-16 SURFACE ELASTIC WAVE FILTER
DE3723545A DE3723545C2 (en) 1986-07-16 1987-07-16 Acoustic surface wave filter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP16746086A JPS6324708A (en) 1986-07-16 1986-07-16 Surface acoustic wave filter

Publications (1)

Publication Number Publication Date
JPS6324708A true JPS6324708A (en) 1988-02-02

Family

ID=15850087

Family Applications (1)

Application Number Title Priority Date Filing Date
JP16746086A Pending JPS6324708A (en) 1986-07-16 1986-07-16 Surface acoustic wave filter

Country Status (1)

Country Link
JP (1) JPS6324708A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2010171805A (en) * 2009-01-23 2010-08-05 Japan Radio Co Ltd Surface acoustic wave filter

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS51114844A (en) * 1975-04-01 1976-10-08 Nippon Telegr & Teleph Corp <Ntt> Acoustic surface wave bandpass filter
JPS53147449A (en) * 1977-05-27 1978-12-22 Nippon Telegr & Teleph Corp <Ntt> Branching unit of elastic surface wave
JPS5763921A (en) * 1980-10-07 1982-04-17 Toshiba Corp Surface acoustic wave device
JPS60180318A (en) * 1984-02-28 1985-09-14 Japan Radio Co Ltd Surface acoustic wave filter

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS51114844A (en) * 1975-04-01 1976-10-08 Nippon Telegr & Teleph Corp <Ntt> Acoustic surface wave bandpass filter
JPS53147449A (en) * 1977-05-27 1978-12-22 Nippon Telegr & Teleph Corp <Ntt> Branching unit of elastic surface wave
JPS5763921A (en) * 1980-10-07 1982-04-17 Toshiba Corp Surface acoustic wave device
JPS60180318A (en) * 1984-02-28 1985-09-14 Japan Radio Co Ltd Surface acoustic wave filter

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2010171805A (en) * 2009-01-23 2010-08-05 Japan Radio Co Ltd Surface acoustic wave filter

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