JPS60185416A - Surface acoustic wave element - Google Patents

Surface acoustic wave element

Info

Publication number
JPS60185416A
JPS60185416A JP4031184A JP4031184A JPS60185416A JP S60185416 A JPS60185416 A JP S60185416A JP 4031184 A JP4031184 A JP 4031184A JP 4031184 A JP4031184 A JP 4031184A JP S60185416 A JPS60185416 A JP S60185416A
Authority
JP
Japan
Prior art keywords
surface acoustic
acoustic wave
electrode
common electrode
wave
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
JP4031184A
Other languages
Japanese (ja)
Inventor
Kazushi Watanabe
一志 渡辺
Takashi Shiba
隆司 芝
Akitsuna Yuhara
章綱 湯原
Jun Yamada
純 山田
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 JP4031184A priority Critical patent/JPS60185416A/en
Publication of JPS60185416A publication Critical patent/JPS60185416A/en
Pending 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
    • H03H9/02535Details of surface acoustic wave devices
    • H03H9/02818Means for compensation or elimination of undesirable effects
    • H03H9/02866Means for compensation or elimination of undesirable effects of bulk wave excitation and reflections

Abstract

PURPOSE:To suppress electrode multiple reflection by using a reed screen electrode where a bonding pad for a common electrode end is provided at the midpoint between the common electrode end and an effective aperture end at the outside of the effective aperture exciting a surface acoustic wave or receiving a wave. CONSTITUTION:A pair of wave transmission/reception reed screen electrodes are provided on a surface acoustic wave substrate including a piezoelectric substance. The reed screen electrodes consist of a bonding pad 16, a common electrode end 17, non-crossing apertures 18, 18' and the effective aperture 19. It is desirous to increase the electrode finger resistance for the suppression of electrode multiplex reflection (TTE). Thus, the non-crossing apertures 18, 18' are sized large. Since the non-crossing aperture is not directly related to the excitation or reception of the surface acoustic wave, when the bonding pad 16 is provided between the end of the effective aperture 19 and the common electrode end 17, the chip size in the direction perpendicular to the surface acoustic wave propagation is decreased without giving any effect on the surface acoustic wave at all.

Description

【発明の詳細な説明】 〔発明の利用分野〕 本発明は電極多重反射が良く抑制され、かつ小形な弾性
表面波素子に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Application of the Invention] The present invention relates to a small surface acoustic wave device in which multiple electrode reflections are well suppressed.

〔発明の背景〕[Background of the invention]

弾性表面波素子の問題点の一つに電極多重反射(Tri
ple Transit Echo 、 111%称T
T E )かある。TTEは弾性表面波素子の振幅、位
相周波数特性にリップルを生ずる原因となり、特に周波
数帯域特性の平坦なことを要求される素子で1・)はT
TE抑圧は不可欠である。
One of the problems with surface acoustic wave devices is electrode multiple reflection (Tri
ple Transit Echo, 111% T
There is a T E ). TTE causes ripples in the amplitude and phase frequency characteristics of surface acoustic wave devices, and in particular in devices that require flat frequency band characteristics, 1.) is TTE.
TE suppression is essential.

第1図は従来の弾性表面波素子の模式図である。出猟1
体よりなる弾性表面波基板1上に、弾性表面波の送波す
だれ状電極2と受波すたれ状電極2′か形成され、送波
すだれ#0.電極2には入1、力信号源4が、また受波
すだれ状電極2′には出力負荷インピーダンス5が接続
されている。また送波すだれ状IM、@2と受波すたれ
状電極2′との間には、入力端から面接出力端に入力す
る電磁波を防止する直達波防止電極7が、さらに端、2
、面反射波を抑圧するため弾性表面波吸音体6゜6′が
形成されている。通常、送波すたれ状電極2丈たは受波
すたれ状電極2′には振幅、位相特性を満足させるため
に電極指交差幅に重み付けが施された構造となっている
。なお、3は電極□指の共通電極端のホンデイングパ′
ツドである。
FIG. 1 is a schematic diagram of a conventional surface acoustic wave element. Hunting 1
On a surface acoustic wave substrate 1 made of a surface acoustic wave body, a surface acoustic wave transmitting blind-shaped electrode 2 and a wave receiving blind-shaped electrode 2' are formed, and the transmitting blind #0. An input 1 and a force signal source 4 are connected to the electrode 2, and an output load impedance 5 is connected to the receiving interdigital electrode 2'. Further, between the transmitting interdigital IM @2 and the receiving interdigital electrode 2', there is a direct wave prevention electrode 7 for preventing electromagnetic waves from inputting from the input end to the surface output end.
, surface acoustic wave sound absorbers 6° 6' are formed to suppress surface reflected waves. Normally, the length of the transmitting stranded electrode 2 or the receiving stranded electrode 2' has a structure in which the intersecting width of the electrode fingers is weighted in order to satisfy amplitude and phase characteristics. In addition, 3 is the Honda pin pad at the common electrode end of the electrode □ finger.
It's Tsudo.

なお、第2図は通常のすだれ状電極(単独)を示す図で
、8は共通電、極端、9はそのボンデ・イングバツドで
ある。
In addition, FIG. 2 is a diagram showing a normal interdigital electrode (single), where 8 is a common electrode, an extreme electrode, and 9 is a bonding electrode thereof.

TTEを抑圧する方法としては、電源あるい111は負
荷コンダクタンスGeと弾性表面波素子のす。
As a method for suppressing TTE, the power source or 111 is a load conductance Ge and a surface acoustic wave element.

たれ状電極の放射コンダクタンスGaの比を大きくする
方法が一般的とされている。しかし、この方法では開口
設計の自由度が小さくなる。そこで本発明者等は、第3
図に示すように、非交1−。
A common method is to increase the ratio of the radiation conductance Ga of the droop-like electrode. However, this method reduces the degree of freedom in designing the opening. Therefore, the present inventors proposed the third
As shown in the figure, non-intersecting 1-.

蓋開口部10.10’を延長し、各電極指抵抗を増加さ
せることによりT ’J’ B抑圧を行っていた。
T'J'B suppression was performed by extending the lid opening 10,10' and increasing the resistance of each electrode finger.

しかし、この従来の本発明者等の方法では、非。However, this conventional method of the present inventors does not.

交差開口部を相当(通常300〜1000μm)大きく
する必要かあり、その上、共通電極端11の外部、1、
にポンティングバッド12ヲ設けていたため、チップサ
イズが大きくなるという欠点があった。
It is necessary to make the cross opening considerably large (usually 300 to 1000 μm), and in addition, the outside of the common electrode end 11, 1,
Since the ponting pad 12 was provided in the chip, there was a drawback that the chip size became large.

また、チップサイズを小さくするため第4図に示すよう
に、ホンティングバッド13ヲ、共通電極端14の内側
に、一部が有効開口部15にかか“るように設けると、
ボンディングパッドにおいて弾性表面波の反射か生じ、
不要な遅延信号が発生し、弾性表面波素子の振幅、位相
周波数特性に太きなリップルとして現れ、この素子をテ
・レビジョン受信機に用いれはゴーストを発生し111
てし才うという欠点があった。
Further, in order to reduce the chip size, as shown in FIG. 4, if the honting pad 13 is provided inside the common electrode end 14 so that a part thereof overlaps the effective opening 15,
Reflection of surface acoustic waves occurs at the bonding pad,
Unnecessary delayed signals are generated, which appear as thick ripples in the amplitude and phase frequency characteristics of the surface acoustic wave device, and when this device is used in a television receiver, ghosts occur.111
He had the disadvantage of being very talented.

〔発明の目的〕[Purpose of the invention]

本発明の目的は、上記各種の欠点、不具合がない、小形
でT ’[” Eが良く抑圧された弾性表面波素子を提
供することにある。 1゜ 〔発明の概要〕 上記目的を達成1−るために本発明においては、弾性表
面波伝搬方向に対して、異極性の電極指が交差せず、弾
性表面波励振または受波を行う有効開口部から外れた、
共通t a=端と有効開0.1゜部端との中間個所に、
共通電極端用ホンディングバッドを設け、従来の如く共
通電極端の外側。
An object of the present invention is to provide a small surface acoustic wave element that is free from the various drawbacks and problems described above, and in which T'[''E is well suppressed. 1. [Summary of the Invention] Achievement of the above object In order to avoid this, in the present invention, electrode fingers of different polarity do not intersect with respect to the surface acoustic wave propagation direction and are out of the effective opening for excitation or reception of the surface acoustic wave.
At the midpoint between the common t a = end and the effective opening 0.1° end,
A honding pad is provided for the common electrode end, and is placed outside the common electrode end as before.

にポンディングパッドを設けた場合に比し、表面波伝搬
方向に直角な方向のチップサイズが小゛さくなるように
した。第5図は本発明に係るす1だれ状電極の模式図で
、16はホンディングバッド、17は共通電極端、18
.18’は非交差開口部、19は有効開口部である。前
述の如く、TTE抑。
The chip size in the direction perpendicular to the surface wave propagation direction is made smaller compared to the case where a bonding pad is provided on the surface. FIG. 5 is a schematic diagram of the interdigital electrode according to the present invention, in which 16 is a honding pad, 17 is a common electrode end, and 18
.. 18' is a non-intersecting opening, and 19 is an effective opening. As mentioned above, TTE suppression.

土のためには電極指抵抗を大きくすることが望・ましい
。そのため非交差開口部18.18’を太きくl()と
っである。この非交差開口部は弾性表面波の・励振また
は受波には直接関与しないから、このような、共通電極
端17オ有効開口部19の端部と。
For soil, it is desirable to increase the electrode finger resistance. Therefore, the non-intersecting openings 18 and 18' are made thicker. Since these non-intersecting openings are not directly involved in excitation or reception of surface acoustic waves, the common electrode end 17 and the end of the effective opening 19 are similar to each other.

の間にホンディングパッド16を設けれは、弾性表面波
には全く影譬を及ぼさずに、弾性表面波、。
By providing the honding pad 16 between them, the surface acoustic waves can be transmitted without affecting the surface acoustic waves at all.

伝搬方向に直角な方向のチップサイズを小さく出来、そ
れだけ原価を低減できる。また、この。
The chip size in the direction perpendicular to the propagation direction can be reduced, and the cost can be reduced accordingly. Also, this.

ようにすれは、比較的容易に電極指抵抗を太きくできる
ので、TTE抑圧特性の良い弾性表面波素子が得られる
In this case, the electrode finger resistance can be increased relatively easily, so that a surface acoustic wave element with good TTE suppression characteristics can be obtained.

才だ、上記のように非交差開口部の電極指抵抗を増加さ
せることがTTE抑圧に有効である゛から、有効開口部
から外れ、共通電極端に至る才での中間個所で、電極指
を1回又はそれ以上折り曲げたり、更に、電極指を有効
開口部では3TTE抑圧に有効なスプリット型、それ以
外の。
As mentioned above, increasing the electrode finger resistance of non-crossing apertures is effective in suppressing TTE, so it is possible to The electrode finger can be bent once or more, and the electrode finger can be split into an effective aperture to suppress 3TTE.

非交差開口部ではソリッド型とすれば一層よい結果が得
られる。第6図は、この様にした電極・の模式図で、1
8a、18a’は折り曲げたソリッド型電極指よりなる
非交差開口部、19aはスブリツ1〔1ト型電極指より
なる有効開口部である。勿論、非交差開口部を折り曲げ
ただけで、有効開口部をソリッド型にしても良く、才だ
、非交差開口。
Better results can be obtained with a solid type for non-intersecting openings. Figure 6 is a schematic diagram of an electrode constructed in this way.
8a and 18a' are non-intersecting openings made of bent solid electrode fingers, and 19a is an effective opening made of sublit 1 [1-shaped electrode fingers]. Of course, you can just bend the non-intersecting openings and make the effective openings solid, which is great.

部は折り曲げないソリッド型で、有効開口部を。The part is a solid type that does not bend and has an effective opening.

スプリット型にしても良い。 1゜ 〔発明の実施例〕 第7図は本発明の一実施例図である。電極構成は、入出
力すだれ状電極20 、20’とし、これらの具体的電
極構造は第5図や第6図に示したように、有効開口部端
と共通電極端の間にボンデ21、イングバツドを設けた
構造となっている。
It may also be a split type. 1. [Embodiment of the Invention] FIG. 7 is a diagram showing an embodiment of the present invention. The electrode configuration is input/output interdigital electrodes 20 and 20', and the specific electrode structure is as shown in FIGS. It has a structure with

電極材料はA1とし、膜厚は500 ’hとした。The electrode material was A1, and the film thickness was 500'h.

有効開口長は300μm1非交差開口長は450μmと
した。また弾性表面波基板はLiNbO3を用い、フィ
ルタ中心周波数は403 M、Hz、 3 dB帯域幅
は −30MHz、送波側(正規型)電極対数は15対
、受波側(重み付)電極対数は60対である。この。
The effective aperture length was 300 μm, and the non-intersecting aperture length was 450 μm. The surface acoustic wave substrate is made of LiNbO3, the filter center frequency is 403 M, Hz, the 3 dB bandwidth is -30 MHz, the number of electrode pairs on the transmitting side (regular type) is 15, and the number of electrode pairs on the receiving side (weighted) is 15 pairs. There are 60 pairs. this.

試料は、ホトリソグラフィ技術により作成し、Alt極
を化学エツチングにより形成し、リード線引出しはAu
ワイヤポンディングによってH1行った。
The sample was prepared using photolithography technology, the Alt electrode was formed by chemical etching, and the lead wire was made of Au.
H1 was performed by wire bonding.

測定は、ネットワークアナライザを用い50Ω系で行っ
た結果、良好な特性を有することが分。
Measurements were conducted using a network analyzer using a 50Ω system, and the results showed that it had good characteristics.

かった。またチップサイズも表面波伝搬方向に対して直
角な方向で300X2=600μmだけ小さl−。
won. The chip size is also smaller by 300×2=600 μm in the direction perpendicular to the surface wave propagation direction.

くできた。I was able to do it.

〔発明の効果〕〔Effect of the invention〕

以上説明したように本発明によれは、電極多重反射が良
く抑制され、しかも、弾性表面波伝。
As explained above, according to the present invention, multiple electrode reflections can be well suppressed, and surface acoustic wave transmission can be effectively suppressed.

振方向に直角な方向の素子寸法が縮小された弾、11性
表面波素子が得られる。
An elastic surface wave element having a reduced element size in a direction perpendicular to the vibration direction is obtained.

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

第1図は従来の弾性表面波素子の一般的な構成を示す模
式図、第2図は従来の通常のすだれ状電極を示す図、第
3図はT’ T E抑圧特性向上5のために電極指の非
交差部分を長くした従来の・すだれ状電極を示す図、第
4図は共通電極端用ホンディングパッドか共通電極端の
内側で有効開口部に重なる個所に配置されたすだれ状電
極を示す図、第5図、第6図は本発明に係るすだ1()
れ状電極の模式図、第7図は本発明の一実施例。 図である。 1・・・弾性表面波基板 2 、2’、 20 、20’・・・弾性表面波送受波
すだれ状電極 。 3.9,12,13.16・・・ホンディングバッド 
l。 8.11,14.17,178・・・共通電極端4・・
・入力信号源 5・・・出力負荷インピーダンス 6.6′・・・弾性表面波吸音体 7・・・直達波防止電極 7 ・ 10.10’ 、18.18’ 、18a、18a’・
・・電極指非交差開口部15.19.19a・・・有効
開口部 ・ 8 ・ 42図 竿づ図 2 幣4図 鞘5図 G
Fig. 1 is a schematic diagram showing the general configuration of a conventional surface acoustic wave element, Fig. 2 is a diagram showing a conventional normal interdigital electrode, and Fig. 3 is a diagram showing a conventional interdigital electrode. A diagram showing a conventional interdigital electrode in which the non-intersecting portions of the electrode fingers are lengthened. Figure 4 shows an interdigital electrode placed at the common electrode end honding pad or at a location inside the common electrode end overlapping the effective opening. Figures 5 and 6 are diagrams showing Suda 1 () according to the present invention.
A schematic diagram of a curved electrode, FIG. 7 is an embodiment of the present invention. It is a diagram. 1...Surface acoustic wave substrate 2, 2', 20, 20'...Surface acoustic wave transmitting/receiving interdigital electrode. 3.9,12,13.16...Honding Bad
l. 8.11, 14.17, 178... Common electrode end 4...
- Input signal source 5... Output load impedance 6.6'... Surface acoustic wave sound absorber 7... Direct wave prevention electrode 7 - 10.10', 18.18', 18a, 18a'.
・Electrode finger non-crossing opening 15.19.19a...Effective opening ・ 8 ・ 42 Figure 2 Figure 4 Scabbard 5 Figure G

Claims (1)

【特許請求の範囲】 1)圧電体を含む弾性表面波基板上ζこ、少なくとも1
対の送受波すだれ状箱2極を有する弾性□表面波素子に
おいて、弾性表面波伝搬方向に対して、異極性の電極指
が交差せず、弾性表面波素子または受波を行う有効開口
部から外れた、共通電極端と有効開口部端との中間個所
に、共通−極端用ホンディングパッドを設置・・けたす
たれ状電極を用いたことを特徴とする弾性表面波素子。 2)有効量し】部から外れ、共通型、極端に至るまでの
中間個所で霜1極指を1回又はそれ以上折り曲げたすだ
れ状電極を用いた特許請求の範1−。 回部1項記載の弾性表面波素子。 3)電極指を、廟効開口部ではスプリット型、有効開口
部から外れた個所ではソリッド型としたすだれ状電極を
用いた特許請求の範囲第1項才たは第2項記載の弾性表
面波素子。 、。
[Claims] 1) On a surface acoustic wave substrate containing a piezoelectric material, at least one
In an elastic □ surface wave element having two poles of a pair of wave transmitting/receiving interdigital boxes, electrode fingers of different polarity do not intersect with respect to the surface acoustic wave propagation direction, and the surface acoustic wave element or the effective opening for wave reception is A surface acoustic wave element characterized in that a common-to-extreme honding pad is installed at an intermediate location between the detached end of the common electrode and the end of the effective opening. 2) Using interdigital electrodes in which the frost pole fingers are bent one or more times at an intermediate point from the common type to the extremes. The surface acoustic wave device according to section 1. 3) The surface acoustic wave according to claim 1 or 2, which uses interdigital electrodes in which the electrode fingers are of a split type at the effective opening and solid at positions outside the effective opening. element. ,.
JP4031184A 1984-03-05 1984-03-05 Surface acoustic wave element Pending JPS60185416A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4031184A JPS60185416A (en) 1984-03-05 1984-03-05 Surface acoustic wave element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4031184A JPS60185416A (en) 1984-03-05 1984-03-05 Surface acoustic wave element

Publications (1)

Publication Number Publication Date
JPS60185416A true JPS60185416A (en) 1985-09-20

Family

ID=12577068

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4031184A Pending JPS60185416A (en) 1984-03-05 1984-03-05 Surface acoustic wave element

Country Status (1)

Country Link
JP (1) JPS60185416A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP1005154A2 (en) * 1998-11-25 2000-05-31 Murata Manufacturing Co., Ltd. Surface acoustic wave filter for improving flatness of a pass band and a method of manufacturing thereof

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP1005154A2 (en) * 1998-11-25 2000-05-31 Murata Manufacturing Co., Ltd. Surface acoustic wave filter for improving flatness of a pass band and a method of manufacturing thereof
EP1005154A3 (en) * 1998-11-25 2001-01-17 Murata Manufacturing Co., Ltd. Surface acoustic wave filter for improving flatness of a pass band and a method of manufacturing thereof

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