JPS6314510A - Surface acoustic wave device - Google Patents

Surface acoustic wave device

Info

Publication number
JPS6314510A
JPS6314510A JP15927286A JP15927286A JPS6314510A JP S6314510 A JPS6314510 A JP S6314510A JP 15927286 A JP15927286 A JP 15927286A JP 15927286 A JP15927286 A JP 15927286A JP S6314510 A JPS6314510 A JP S6314510A
Authority
JP
Japan
Prior art keywords
electrode
surface acoustic
excitation
acoustic wave
shield
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
JP15927286A
Other languages
Japanese (ja)
Inventor
Yoshihiko Yasuhara
安原 吉彦
Masao Nozaki
野崎 正男
Yumi Habara
羽原 由美
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.)
Toshiba Corp
Toshiba Development and Engineering Corp
Original Assignee
Toshiba Corp
Toshiba Electronic Device Engineering 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 Toshiba Corp, Toshiba Electronic Device Engineering Co Ltd filed Critical Toshiba Corp
Priority to JP15927286A priority Critical patent/JPS6314510A/en
Publication of JPS6314510A publication Critical patent/JPS6314510A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To suppress the occurrence of a retarded ripple while preventing electromagnetic, electrostatic induction and direct induction by providing a cut-off part or a recessed part to a part of a shield electrode and interposing an exciting electrode to the cut-off part or the recessed part. CONSTITUTION:The cut-off part 14a formed by removing the electrode pattern near an exciting electrode 12, that is, nearly at the middle of the shield electrode 14 is formed to the shield electrode 14. The exciting electrode 12 is interposed in the cut-off part 14a so as to approach the shield electrode 14. Thus, the distance between the exciting electrode 12 and a reception electrode 13 is minimized. Thus, the occurrence of a retarded ripple due to a tripple transit echo is suppressed while providing a shield electrode preventing the electromagnetic, electrostatic induction and direct induction. Moreover, a recessed part is provided to the shield electrode in place of the cut-off part and the exciting electrode is interpolsed to the recessed part so as to obtain the similar effect.

Description

【発明の詳細な説明】 [発明の目的] (産業上の利用分野) 本発明は、発振器、遅延線等に用いられる弾性表面波装
置に関する。
DETAILED DESCRIPTION OF THE INVENTION [Object of the Invention] (Field of Industrial Application) The present invention relates to a surface acoustic wave device used for an oscillator, a delay line, etc.

(従来の技術) 一般に発振器や遅延線等に用いられる弾性表面波装置は
、たとえば第4図に示す溝光(こされている。
(Prior Art) A surface acoustic wave device generally used for an oscillator, a delay line, etc. has a grooved light beam as shown in FIG. 4, for example.

同図において、符号1は圧電基板てあり、この圧電基板
1の一主面上に、へβからなる電(へパターンが形成さ
れている。プ゛なわら符号2は一対のくし両市、(へ2
a、2aを交差してなりかつ各電極指の長さを変えるこ
とにより重みっけがなされたアポグイズ型の励振電(う
1である。またこの励4辰電極2から励振される弾i生
表面波の伝播方向の一方の側に所定の間隔をもって一対
のくし歯電極3a、3aを交差してなる受信電極3が形
成されている。
In the figure, reference numeral 1 denotes a piezoelectric substrate, and on one main surface of this piezoelectric substrate 1, an electric pattern consisting of β is formed. to 2
a and 2a, and weighted by changing the length of each electrode finger. A receiving electrode 3 is formed by crossing a pair of comb-shaped electrodes 3a, 3a at a predetermined interval on one side in the wave propagation direction.

そしてこれら励撮電、恒2と受信電極3との間にシール
ド電極4を形成し、ざらに所定の位置にダミー電極5を
形成してなる。
A shield electrode 4 is formed between the excitation electrode 2 and the reception electrode 3, and dummy electrodes 5 are formed at roughly predetermined positions.

そしてこのように構成された弾性表面波装置によれば、
励振霜囲2から励振された弾性表面波は圧電基板1を伝
播し、受信型1へ3により受信される。その際、上記し
たように励振型(か2と受信電極3との間に形成された
シールド電極4により、励振電極2から受信電極3への
電[6的、□静電的、直接誘導を防止している(特開昭
52−103938号参照)。またダミー電(へ5によ
り位相速度に差異が生じることを防止している。
According to the surface acoustic wave device configured in this way,
The surface acoustic waves excited from the excitation frost enclosure 2 propagate through the piezoelectric substrate 1 and are received by the receiving mold 1 . At that time, as described above, the shield electrode 4 formed between the excitation electrode 2 and the reception electrode 3 conducts electrostatic and direct induction from the excitation electrode 2 to the reception electrode 3. (Refer to Japanese Patent Application Laid-Open No. 103938/1983.) Furthermore, the dummy electric current (5) prevents the occurrence of a difference in phase velocity.

(発明が解決しようとする問題点) ところでこのような弾性表面波装置において、励振型(
へ2と受信型(へ3との間に生じる電気反射いわゆるト
リプルトランジットエコーにより発生する遅延リップル
は、 ΔT=4Jα・Ta/(1−α)・・・・・ペイ)ただ
しΔT:遅延リップル Ta:遅延時間 αニトリプルトランシットエコーの主 信号に対する大きさ で表わされる。
(Problems to be solved by the invention) By the way, in such surface acoustic wave devices, the excitation type (
The delay ripple caused by the electrical reflection so-called triple transit echo that occurs between He 2 and the receiving type (He 3) is: ΔT=4Jα・Ta/(1-α)...Pay) where ΔT: Delay ripple Ta : Delay time α is expressed by the magnitude of the triple transit echo relative to the main signal.

一方、上記した弾性表面波装置のように、励振電極2と
受信電極3との間にシールド電極4を形成する場合、こ
のシールド電極4を形成するための所定のスペースが必
要とされる。そしてこのようなスペースにより、励振電
極2と受信型)水3との間隔が大きくなり、遅延時間T
aが長くなる。
On the other hand, when forming the shield electrode 4 between the excitation electrode 2 and the reception electrode 3 as in the surface acoustic wave device described above, a predetermined space is required for forming the shield electrode 4. Due to such a space, the distance between the excitation electrode 2 and the receiving type water 3 increases, and the delay time T
a becomes longer.

このため上記した式(イ)から明らかなようにトリプル
トランジットエコーにより発生する遅延リップルΔ丁が
大きくなるという問題がおる。
Therefore, as is clear from the above equation (a), there is a problem in that the delay ripple Δd generated by the triple transit echo becomes large.

本発明は、上記した事情に鑑みて創案されたもので、電
磁的、静電的、直接誘導を防止しつつ、遅延リップルの
発生を抑えた弾性表面波装置を提供することを目的とし
ている。
The present invention was devised in view of the above-mentioned circumstances, and an object of the present invention is to provide a surface acoustic wave device that prevents electromagnetic, electrostatic, and direct induction while suppressing the occurrence of delay ripples.

[発明の構成] (問題点を解決するための手段) すなわち本発明の弾性表面波装置は、弾性表面波を伝播
する基板と、この基板の一主面上に形成された一対のく
し南電(勇を交差してなりかつ重みづけがなされた励振
電極と、この励振電極から励振される弾性表面波の伝播
方向に所定の間隔をもって形成された一対のくし歯電極
を交差しでなる受信電極と、前記励振電極と前記受信電
極との間に形成されたシールド電極とを尚えた弾性表面
波装置において、前記シールド電(へか、前記励振電極
の近接する位置に、分断部または])a記励振電極に向
けて凹部を有し、これら分断部または凹部に前記励振型
(水を介在させている。
[Structure of the Invention] (Means for Solving the Problems) That is, the surface acoustic wave device of the present invention includes a substrate that propagates surface acoustic waves, and a pair of comb-shaped electric conductors formed on one main surface of the substrate. (A receiving electrode consisting of an excitation electrode that intersects and is weighted, and a pair of comb-shaped electrodes that are formed at a predetermined interval in the propagation direction of the surface acoustic waves excited from this excitation electrode.) and a shield electrode formed between the excitation electrode and the reception electrode. It has a concave portion facing the excitation electrode, and the excitation type (water is interposed in these divided portions or concave portions).

(作用) 本発明の弾性表面波装置において、シールド電・1両が
、励振型1両の近接する位置に、分断部またはこの励振
型)勇に向けて四部を有し、これら分断部または四部に
励振電極を介在己uることにより、励振電極と受信型(
魚との距離を最小限にすることかできる。このため電磁
的、静電的、直接誘導を防止することかできるシールド
電極を具1lii (、、ながらも、遅延リップルの発
生を抑えることか可能となる。
(Function) In the surface acoustic wave device of the present invention, the shield electric cable has a divided part or four parts facing the excitation type one in the vicinity of the excitation type one car, and these divided parts or four parts By interposing the excitation electrode in the excitation electrode and the reception type (
You can minimize the distance between you and the fish. For this reason, it is possible to use a shield electrode that can prevent electromagnetic, electrostatic, and direct induction (although it is possible to suppress the occurrence of delay ripples).

(実施例) 以下、本発明の実施例の詳?IIlを図面に基づいて説
明する。
(Example) Below, details of an example of the present invention will be described. IIl will be explained based on the drawings.

本発明の一実施例に係る弾性表面波装置の構j告を第1
図に示す。
The first embodiment of a surface acoustic wave device according to an embodiment of the present invention is described below.
As shown in the figure.

同図において、符号11は弾性表面波を伝播するたとえ
ば1−iTao3からなる圧電基板11てあり、この圧
電基板11の一主面上にはたとえば八℃からなる電極パ
ターンが形成されている。すなわち符号12は一対のく
し歯電極12a、12aを交差してなりかつ各電、1カ
指の長さを変えることにより車みづけがなされ通過帯域
内特性か決定されたアポダイズ型の励振型(奄である。
In the figure, reference numeral 11 denotes a piezoelectric substrate 11 made of, for example, 1-iTao3, which propagates surface acoustic waves, and an electrode pattern made of, for example, 8° C. is formed on one main surface of this piezoelectric substrate 11. In other words, the reference numeral 12 is an apodized excitation type (apodized type excitation type) consisting of a pair of interdigitated electrodes 12a, 12a, which are connected by changing the length of one finger of each electrode, and whose characteristics within the passband are determined. It is Amami.

この励振電極12から励振される弾性表面波の1云播方
向の一方の側に一対のくし歯電極13a、13aを交差
してなる受信型4へ13が上記励振型1へ12と所定の
間隔をもって形成されている。また励振型(Φ12と受
信電極13との間には、アース電位にされたシールド電
極14が形成されている。このシールド電極14は、励
振電極12の接近する位置ずなわちこのシールド電極1
4のほぼ中央に、電極パターンか除去された分断部14
aが形成されている。そしてこの分断部14a内に、励
振電極12がシールド電極14と近接するようにして介
在されている。ざらに励振電極12のシールド電1両1
4に近接する側のクシ@電極12aはシー、ルド電(画
14と同電位のアース電位とされている。
A pair of comb-shaped electrodes 13a, 13a are intersected on one side in the propagation direction of the surface acoustic waves excited from the excitation electrode 12, and the reception type 4 13 is spaced at a predetermined interval from the excitation type 1 12. It is formed with. Further, a shield electrode 14 which is set to a ground potential is formed between the excitation type (Φ12 and the reception electrode 13).
4, there is a divided part 14 from which the electrode pattern has been removed.
a is formed. The excitation electrode 12 is interposed in the divided portion 14a so as to be close to the shield electrode 14. Roughly excitation electrode 12 shield electric 1 car 1
The comb@electrode 12a on the side adjacent to the shield electrode 4 is at the ground potential, which is the same potential as the shield electrode (the comb 14).

また所定の位置にはダミー電極15か形成されている。Further, a dummy electrode 15 is formed at a predetermined position.

すなわちこのダミー電極15により各弾性表面波伝播路
上に電極パターンの存在する長さがほぼ同一となるよう
にされ、電圧基板11上を伝播する弾性表面波の位相速
lxの差異をなくしている。
That is, the dummy electrodes 15 ensure that the lengths of the electrode patterns on each surface acoustic wave propagation path are approximately the same, eliminating differences in the phase velocity lx of the surface acoustic waves propagating on the voltage substrate 11.

このように構成された本実施例の弾性表面波装置におい
て、励振電極12から励振された弾性表面波は圧電基板
11上を伝播し、受信電極13により受信される。その
際、励振電極12と受信電極13との間に形成されたシ
ールド電極14および励振型(へ12のアース電位にさ
れたくし歯電極12aの受信型(伽13側に近い電極指
12bにより、励振電価12から受信型、)へ13への
電磁的、静電的、直接誘導を防止することかできるよう
になる。また励振型(へ12は分断部14a内に介在さ
れ、この励振電極12と受信電極13との距離が非常に
小さいちのとされている。このため遅延時間Taを短く
することができ、トリプルトランジットエコーにより発
生する遅延リップルΔ丁を極力抑えることかできる(従
来例式(イ)参照)。
In the surface acoustic wave device of this embodiment configured as described above, the surface acoustic wave excited from the excitation electrode 12 propagates on the piezoelectric substrate 11 and is received by the reception electrode 13. At that time, the shield electrode 14 formed between the excitation electrode 12 and the reception electrode 13 and the reception type (electrode finger 12b near the side of the comb 13) of the comb-shaped electrode 12a which is set to the ground potential of the excitation type (to 12) It becomes possible to prevent electromagnetic, electrostatic, and direct induction from the electric potential 12 to the receiving type () 13. Also, the excitation type (12) is interposed within the dividing portion 14a, and this excitation electrode 12 The distance between the receiver electrode 13 and the receiver electrode 13 is considered to be very small.For this reason, the delay time Ta can be shortened, and the delay ripple Δd generated by the triple transit echo can be suppressed as much as possible (conventional example formula ( b) see).

ざらにこの場合、この弾性表面波装置全体の長さを短く
することができ、小型軽量化によるコストダウンを図る
ことができるようになる。
In this case, the overall length of the surface acoustic wave device can be shortened, and costs can be reduced by making it smaller and lighter.

次にこの実施例装置を実際に製作し、さらに従来の弾性
表面波装置を製作しこれらの群遅延特性および周波数特
性を測定した結果を第2図に示す。
Next, this embodiment device was actually manufactured, and a conventional surface acoustic wave device was also manufactured, and the group delay characteristics and frequency characteristics of these devices were measured. The results are shown in FIG.

同図において、(イ)はこの実施例装置の周波数特性を
示し、(ロ)はその一部を10倍に拡大したものを示し
、(ハ)はその群遅延特性を示している。また(二)は
従来装置の周波数特性を示し、(ホ)はその一部を10
倍に拡大したものを示し、(へ)はその群遅延特性を示
している。
In the figure, (a) shows the frequency characteristics of this example device, (b) shows a part of it enlarged ten times, and (c) shows its group delay characteristics. In addition, (2) shows the frequency characteristics of the conventional device, and (e) shows a part of it at 10
The image is shown enlarged twice, and () shows its group delay characteristics.

これらから明らかなように本実施例装置の群遅延特性お
よび周波数特性は、従来例のものと比較し非常に良好で
市り、遅延リップルの発生が抑えられていることが確認
された。またこの装置の面積は従来のものと比べ約7%
縮小することができた。
As is clear from the above, the group delay characteristics and frequency characteristics of the device of this example were very good compared to the conventional example, and it was confirmed that the occurrence of delay ripples was suppressed. In addition, the area of this device is approximately 7% compared to conventional ones.
I was able to reduce it.

なあ、上述した実施例ににれはシールド電極14に分断
部14aを設けるものでおったが、本発明はこれに限定
されることなく、シールド電極か励振電極に向けて凹部
を有し、この凹部に励振電価を介在されてもほぼ同様の
効果を得ることかできる。
Incidentally, in the above-mentioned embodiment, the shield electrode 14 was provided with the divided portion 14a, but the present invention is not limited to this, and the present invention has a recessed portion toward either the shield electrode or the excitation electrode. Almost the same effect can be obtained even if an excitation voltage is interposed in the recess.

またシールド電極14と励振電極12とは分離されるも
のでめったが、これに限定されることなく、第3図に示
すようにアース電位にされた励振電極12aの電極指1
2bとシールド電極14とを接合させてつまり一体にさ
けても同様の効果を得ることができる。
Further, although the shield electrode 14 and the excitation electrode 12 are rarely separated, the electrode finger 1 of the excitation electrode 12a set to the ground potential as shown in FIG. 3 is not limited to this.
The same effect can be obtained even if the shield electrode 2b and the shield electrode 14 are joined together, that is, they are not integrated.

[発明の効果] 以上説明したように本発明の弾性表面波装置によれば、
電磁的、静電的、直接誘導を防止し、かつ3延リツプル
の発生を充分に抑えることかでさる。
[Effects of the Invention] As explained above, according to the surface acoustic wave device of the present invention,
It is important to prevent electromagnetic, electrostatic, and direct induction, and to sufficiently suppress the occurrence of triple ripple.

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

第1図は本発明の一実施例の弾性表面波装置を示す斜視
図、第2図はこの実施例装置の効果を確認するために行
った測定結果を示すグラフ、第3図は本発明の弾性表面
波装置の変形例を示す平面図、第4図は従来の弾性表面
波装置を示す斜?5−図である。 12・・・・・・・・・励振型(Φ 13・・・・・・・・・受信型(へ 14・・・・・・・・・シール1−電(車14a・・・
・・・分断部 出願人      株式会社 東芝 出(預入      東芝電子デバイスエンジニアリン
グ株式会社 代理人 弁理士  須 山 1!L− ζ咽処苫垣= 巽(咲rjllI  の
Fig. 1 is a perspective view showing a surface acoustic wave device according to an embodiment of the present invention, Fig. 2 is a graph showing measurement results conducted to confirm the effect of this embodiment device, and Fig. 3 is a perspective view showing a surface acoustic wave device according to an embodiment of the present invention. A plan view showing a modified example of the surface acoustic wave device, and FIG. 4 is an oblique view showing a conventional surface acoustic wave device. 5-Fig. 12...... Excitation type (Φ 13...... Receiving type (to) 14...... Seal 1-Electric (car 14a...
... Separation Department Applicant: Toshiba Corporation (Deposit: Toshiba Electronic Device Engineering Co., Ltd. Agent: Patent Attorney: Suyama 1!L-

Claims (3)

【特許請求の範囲】[Claims] (1)弾性表面波を伝播する基板と、この基板の一主面
上に形成された一対のくし歯電極を交差してなりかつ重
みづけがなされた励振電極と、この励振電極から励振さ
れる弾性表面波の伝播方向に所定の間隔をもつて形成さ
れた一対のくし歯電極を交差してなる受信電極と、前記
励振電極と前記受信電極との間に形成されたシールド電
極とを備えた弾性表面波装置において、前記シールド電
極が、前記励振電極の近接する位置に、分断部または前
記励振電極に向けて凹部を有し、これら分断部または凹
部に前記励振電極を介在させていることを特徴とする弾
性表面波装置。
(1) A substrate that propagates surface acoustic waves, an excitation electrode formed by intersecting a pair of comb-shaped electrodes formed on one main surface of this substrate and weighted, and an excitation electrode that is excited from this excitation electrode. A receiving electrode formed by intersecting a pair of comb-shaped electrodes formed at a predetermined interval in the propagation direction of surface acoustic waves, and a shield electrode formed between the excitation electrode and the receiving electrode. In the surface acoustic wave device, the shield electrode has a divided portion or a recess toward the excitation electrode at a position adjacent to the excitation electrode, and the excitation electrode is interposed in the divided portion or the recess. Features of surface acoustic wave device.
(2)前記励振電極の前記シールド電極に近接する側の
くし歯電極が、前記シールド電極と同電位にされている
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。
(2) The surface acoustic wave device according to claim 1, wherein a comb-shaped electrode on the side of the excitation electrode adjacent to the shield electrode is set at the same potential as the shield electrode.
(3)前記励振電極の前記シールド電極の近接する側の
くし歯電極が、前記シールド電極と一体にされているこ
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) The surface acoustic wave device according to claim 1, wherein a comb-shaped electrode of the excitation electrode adjacent to the shield electrode is integrated with the shield electrode.
JP15927286A 1986-07-07 1986-07-07 Surface acoustic wave device Pending JPS6314510A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP15927286A JPS6314510A (en) 1986-07-07 1986-07-07 Surface acoustic wave device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP15927286A JPS6314510A (en) 1986-07-07 1986-07-07 Surface acoustic wave device

Publications (1)

Publication Number Publication Date
JPS6314510A true JPS6314510A (en) 1988-01-21

Family

ID=15690152

Family Applications (1)

Application Number Title Priority Date Filing Date
JP15927286A Pending JPS6314510A (en) 1986-07-07 1986-07-07 Surface acoustic wave device

Country Status (1)

Country Link
JP (1) JPS6314510A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0275215A (en) * 1988-09-09 1990-03-14 Toko Inc Surface acoustic wave resonator and filter
JPH04148577A (en) * 1990-10-12 1992-05-21 Kunitada Tanaka Laser
JPH04114225U (en) * 1991-03-26 1992-10-07 ミツミ電機株式会社 surface acoustic wave device
JP2015141183A (en) * 2014-01-30 2015-08-03 京セラクリスタルデバイス株式会社 Angular velocity sensor and sensor element

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0275215A (en) * 1988-09-09 1990-03-14 Toko Inc Surface acoustic wave resonator and filter
JPH0514443B2 (en) * 1988-09-09 1993-02-25 Toko Inc
JPH04148577A (en) * 1990-10-12 1992-05-21 Kunitada Tanaka Laser
JPH04114225U (en) * 1991-03-26 1992-10-07 ミツミ電機株式会社 surface acoustic wave device
JP2015141183A (en) * 2014-01-30 2015-08-03 京セラクリスタルデバイス株式会社 Angular velocity sensor and sensor element

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