JPH0443707A - Surface acoustic wave device - Google Patents
Surface acoustic wave deviceInfo
- Publication number
- JPH0443707A JPH0443707A JP15189790A JP15189790A JPH0443707A JP H0443707 A JPH0443707 A JP H0443707A JP 15189790 A JP15189790 A JP 15189790A JP 15189790 A JP15189790 A JP 15189790A JP H0443707 A JPH0443707 A JP H0443707A
- Authority
- JP
- Japan
- Prior art keywords
- electrode
- surface acoustic
- acoustic wave
- wave device
- comb
- 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
Links
- 238000010897 surface acoustic wave method Methods 0.000 title claims abstract description 33
- 239000000758 substrate Substances 0.000 claims description 11
- 230000001681 protective effect Effects 0.000 claims description 7
- 230000000694 effects Effects 0.000 abstract description 6
- 230000006866 deterioration Effects 0.000 abstract description 4
- 238000009413 insulation Methods 0.000 abstract description 3
- 229910052782 aluminium Inorganic materials 0.000 description 5
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 5
- 239000012212 insulator Substances 0.000 description 5
- 238000000034 method Methods 0.000 description 4
- 239000013078 crystal Substances 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 239000007772 electrode material Substances 0.000 description 2
- 238000004519 manufacturing process Methods 0.000 description 2
- 229910052751 metal Inorganic materials 0.000 description 2
- 239000002184 metal Substances 0.000 description 2
- 150000002739 metals Chemical class 0.000 description 2
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 1
- 229910011131 Li2B4O7 Inorganic materials 0.000 description 1
- RTAQQCXQSZGOHL-UHFFFAOYSA-N Titanium Chemical compound [Ti] RTAQQCXQSZGOHL-UHFFFAOYSA-N 0.000 description 1
- 230000015556 catabolic process Effects 0.000 description 1
- 229910052802 copper Inorganic materials 0.000 description 1
- 239000010949 copper Substances 0.000 description 1
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- 238000006731 degradation reaction Methods 0.000 description 1
- 230000005684 electric field Effects 0.000 description 1
- 238000005530 etching Methods 0.000 description 1
- 239000010410 layer Substances 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 230000001902 propagating effect Effects 0.000 description 1
- 239000011241 protective layer Substances 0.000 description 1
- 239000007787 solid Substances 0.000 description 1
- 238000004544 sputter deposition Methods 0.000 description 1
- 239000010936 titanium Substances 0.000 description 1
- 229910052719 titanium Inorganic materials 0.000 description 1
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野]
本発明は圧電基板上に櫛形を極が形成された弾性表面波
装置に関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a surface acoustic wave device in which comb-shaped poles are formed on a piezoelectric substrate.
[従来の技術]
弾性表面波装置は固体表面を伝播する弾性表面波を用い
た素子である0弾性表面波装置の一例を第3図に示す。[Prior Art] FIG. 3 shows an example of a surface acoustic wave device, which is an element using surface acoustic waves propagating on a solid surface.
圧電基板10の中央に正規型櫛形電極12が形成され、
正規型櫛形を極12の両側に一対の反射器14.16が
形成されている。正規型櫛形電極12は、数μm幅の微
細な多数のアルミニウム製の電極で構成された2つの櫛
形$極12a、12bが互いに各tSが噛み合うように
配置されている。櫛形電極12a、12bの根元にはボ
ンディング用パッド18.20が形成されている。弾性
表面波は櫛形電極12a、12b上を第3図の左右の方
向に伝播する。A regular comb-shaped electrode 12 is formed in the center of the piezoelectric substrate 10,
A pair of reflectors 14, 16 are formed on either side of the regular comb-shaped pole 12. In the regular comb-shaped electrode 12, two comb-shaped $ poles 12a and 12b each made of a large number of fine aluminum electrodes with a width of several μm are arranged so that each tS is engaged with each other. Bonding pads 18 and 20 are formed at the bases of the comb-shaped electrodes 12a and 12b. The surface acoustic waves propagate on the comb-shaped electrodes 12a and 12b in the left and right directions in FIG.
このような弾性表面波装置に大電力を伝送させると素子
が劣化するという間肋があった0弾性表面波装置の劣化
状況を観察したところ櫛形電極の電極部分の劣化が支配
的故障原因であることが明らかになった。すなわち、電
力の印加により櫛形@極の電極上にしロックが発生し、
このしロックの成長に件って隣接する電極間で短絡が発
生して大電流が流れ、最終的に電極が溶断してしまう。When transmitting large amounts of power to such a surface acoustic wave device, the device deteriorates. When we observed the deterioration status of the surface acoustic wave device, we found that the main cause of failure was the deterioration of the electrode part of the comb-shaped electrode. It became clear. In other words, when power is applied, a lock occurs on the comb-shaped @pole electrode.
As the lock grows, a short circuit occurs between adjacent electrodes, causing a large current to flow, eventually causing the electrodes to melt.
[発明が解決しようとする課1!!!]このような櫛形
電極の劣化を防止するため、電極材料のアルミニウムに
チタンや銅等の他の金属を添加して耐電力性を増す方法
が試みられている。[Lesson 1 that the invention attempts to solve! ! ! ] In order to prevent such deterioration of the comb-shaped electrode, attempts have been made to add other metals such as titanium and copper to the aluminum electrode material to increase the power resistance.
しかしながら電極材料の組成を変更すると、弾性表面波
装置の設計パラメータを根本から見直す必要があるとい
う問題があった。また、アルミニウムに他の金属を添加
して@極材料を構成した場合、常に均一な組成の電極を
形成することが困難であり、その結果、弾性表面波装置
の特性がばらつくという問題があった。However, there is a problem in that changing the composition of the electrode material requires a fundamental review of the design parameters of the surface acoustic wave device. In addition, when other metals are added to aluminum to form the @ electrode material, it is difficult to form electrodes with a uniform composition, and as a result, there is a problem that the characteristics of the surface acoustic wave device vary. .
本発明は上記事情を考慮してなされたもので、従来から
の設計パラメータを変更することなく、耐電力性に優れ
、しかも素子特性のばらつきの少ない弾性表面波装置を
捉供することを目的とする。The present invention has been made in consideration of the above circumstances, and it is an object of the present invention to provide a surface acoustic wave device that has excellent power durability and less variation in element characteristics without changing conventional design parameters. .
[課題を解決するための手段]
上記目的は、圧電基板上に櫛形電極が形成された弾性表
面波装置において、前記櫛形電極の各電極の弾性表面波
伝播方向の側壁が絶縁性保護膜で覆われていることを特
徴とする弾性表面波装置によって達成される。[Means for Solving the Problem] The above object is to provide a surface acoustic wave device in which a comb-shaped electrode is formed on a piezoelectric substrate, in which the side wall of each electrode of the comb-shaped electrode in the surface acoustic wave propagation direction is covered with an insulating protective film. This is achieved by a surface acoustic wave device characterized by:
[作用]
本発明によれば、櫛形電極の各電極の弾性表面波伝播方
向の側壁を絶縁性保護膜で覆ったので、櫛形電極の機械
的強度を補強し、非連続点が分散され弾性表面波による
ストレスが集中することがなく、耐電力性を改善するこ
とができる。また、絶縁性保護膜は各電極の側壁に設け
られ、各電極の上面は露出したままであるので、従来が
らの弾性表面波装置の設計パラメータを変更する必要も
ない。[Function] According to the present invention, since the side wall of each electrode of the comb-shaped electrode in the surface acoustic wave propagation direction is covered with an insulating protective film, the mechanical strength of the comb-shaped electrode is reinforced, discontinuous points are dispersed, and the elastic surface is Stress caused by waves is not concentrated, and power durability can be improved. Further, since the insulating protective film is provided on the side wall of each electrode and the upper surface of each electrode remains exposed, there is no need to change the design parameters of the conventional surface acoustic wave device.
[実施例]
本発明の一実施例による弾性表面波装置を第1図を用い
て説明する。[Example] A surface acoustic wave device according to an example of the present invention will be described with reference to FIG.
第1図は弾性表面波装置の櫛形電極の一部を拡大した断
面図である。圧電基板10上に櫛形電極12の各電極1
3が形成されている。圧電基板10としては、電気機械
結合定数の大きなLi2B4O7単結晶基板、LiNb
0.単結晶基板等が用いられる。櫛形電極12の各電極
13はアルミニウムで作られる。各電極13は数μmの
幅を有し、数μm間隔で配されている。FIG. 1 is an enlarged cross-sectional view of a part of a comb-shaped electrode of a surface acoustic wave device. Each electrode 1 of the comb-shaped electrode 12 is placed on the piezoelectric substrate 10.
3 is formed. As the piezoelectric substrate 10, Li2B4O7 single crystal substrate with a large electromechanical coupling constant, LiNb
0. A single crystal substrate or the like is used. Each electrode 13 of the comb-shaped electrode 12 is made of aluminum. Each electrode 13 has a width of several μm and is arranged at intervals of several μm.
本実施例では各電極13のIPIWを、5iozl!J
、5iSN4!l!等の絶縁物保護M15で覆って耐電
力性を強化している。すなわち、各電極13の側壁に、
電力印加によって引き起こされる電極の劣化が隣接する
電極に及ぼす影響を抑制するのに十分であって、かつ、
弾性表面波装置の特性に及ぼす影響が無視できる程度の
厚さの絶縁物保11M15を形成して保護する0本実施
例では各電極13の側壁に50〜100A程度の絶縁物
保護層15を形成している。In this example, the IPIW of each electrode 13 is 5iozl! J
,5iSN4! l! It is covered with an insulator protection M15 such as M15 to strengthen the power resistance. That is, on the side wall of each electrode 13,
sufficient to suppress the effects of electrode degradation caused by the application of power on adjacent electrodes, and
In this embodiment, an insulating protective layer 15 of about 50 to 100 A is formed on the side wall of each electrode 13 to protect it by forming an insulating layer 11M15 with a thickness such that the effect on the characteristics of the surface acoustic wave device is negligible. are doing.
このように本実施例によれば各@極13の側壁を絶縁性
保111M15で覆ったので、この絶縁性保護膜15が
圧電基板10と電極13の側壁に密着して櫛形電極12
の機械的強度を補強し、耐電力性を改善することができ
る。また、各電極13の側壁を絶縁性保護M15で覆う
ことにより、非連続点が分散され弾性表面波によるスト
レスが集中することがない、電界の不′i!A続境界(
各電極13の端部)と質量の不連続境界(絶縁性保11
WA15の端部)が分離され、ストレスの集中をさらに
緩和することができる。According to this embodiment, since the side wall of each @ electrode 13 is covered with the insulating film 111M15, the insulating protective film 15 is in close contact with the side wall of the piezoelectric substrate 10 and the electrode 13, and the comb-shaped electrode 12 is
It can strengthen the mechanical strength and improve the power resistance. In addition, by covering the side wall of each electrode 13 with an insulating protection M15, discontinuous points are dispersed, stress caused by surface acoustic waves is not concentrated, and the electric field is improved! A-continued boundary (
end of each electrode 13) and mass discontinuous boundary (insulating
The ends of the WA 15) are separated, and stress concentration can be further alleviated.
また、本実施例によれば、絶縁性保護膜15を設けても
、各電極13の上面が露出したままであり、しかも、そ
の厚さが弾性表面波装置の特性に及ぼす影響が無、視で
きる程度であるので、従来からの弾性表面波装置の設計
パラメータを変更することなくそのまま使用できる。Further, according to this embodiment, even if the insulating protective film 15 is provided, the upper surface of each electrode 13 remains exposed, and the effect of its thickness on the characteristics of the surface acoustic wave device is negligible. Therefore, conventional surface acoustic wave devices can be used as they are without changing their design parameters.
本実施例による弾性表面波装置の製造方法を第2図を用
いて説明する。A method of manufacturing the surface acoustic wave device according to this embodiment will be explained using FIG. 2.
まず、圧電基板10上にアルミニウムをエツチングして
ストライプ状の電極13を形成する(第2図(a))。First, aluminum is etched on the piezoelectric substrate 10 to form striped electrodes 13 (FIG. 2(a)).
次に、スパッタリング等の成膜方法により、全面に5i
n2WA、Si)N4M等の絶縁膜17を形成する(第
2図(b))。Next, 5i is applied to the entire surface using a film forming method such as sputtering.
An insulating film 17 of n2WA, Si)N4M, etc. is formed (FIG. 2(b)).
次に、RIE等の異方性エツチング法により、電極13
上面が露出するまで絶縁117をエツチングすると、電
極13の側壁部分のみに絶縁1117が残り、絶縁物保
護膜15が形成される(第2図(C))。Next, the electrode 13 is etched by an anisotropic etching method such as RIE.
When the insulator 117 is etched until the upper surface is exposed, the insulator 1117 remains only on the side wall portion of the electrode 13, and an insulator protective film 15 is formed (FIG. 2(C)).
本発明は上記実施例に限らず種々の変形が可能である。The present invention is not limited to the above-mentioned embodiments, and various modifications are possible.
例えば、弾性表面波装置としては上記実施例のもの限ら
ずあらゆる種類の弾性表面波装置に本発明を適用するこ
とができる。また、櫛形電極に限らず反射器等の他のス
トリップ44[!の側壁にも絶縁物gAi!膜を形成し
てもよい。For example, the present invention can be applied to all types of surface acoustic wave devices, not just those of the above embodiments. In addition to the comb-shaped electrode, other strips 44 [! There is also insulation on the side walls of gAi! A film may also be formed.
[発明の効果]
以上の通り、本発明によれば、櫛形電極の各電極の弾性
表面波伝播方向の側壁を絶縁性像1iilWAで覆った
ので、従来の設計パラメータを変更することなく耐電力
性を強化することができる。[Effects of the Invention] As described above, according to the present invention, since the side wall of each electrode of the comb-shaped electrode in the surface acoustic wave propagation direction is covered with the insulating image 1iILWA, the power durability can be improved without changing the conventional design parameters. can be strengthened.
第1図は本発明の一実施例による弾性表面波装置の要部
を拡大した断面図、
第2図は本発明の一実施例による弾性表面波装置の製造
方法の工程図、
第3図は弾性表面波装置の一例を示す図である。
図において、
10・・・圧電基板
12・・・正規型櫛形電極
12a、12b・・・櫛形電極
13・・・@極
14.16・・・反射器
15・・・絶縁物像KM
17・・・絶縁膜FIG. 1 is an enlarged sectional view of the main parts of a surface acoustic wave device according to an embodiment of the present invention, FIG. 2 is a process diagram of a method for manufacturing a surface acoustic wave device according to an embodiment of the present invention, and FIG. FIG. 1 is a diagram showing an example of a surface acoustic wave device. In the figure, 10...Piezoelectric substrate 12...Regular comb-shaped electrodes 12a, 12b...Comb-shaped electrode 13...@pole 14.16...Reflector 15...Insulator image KM 17...・Insulating film
Claims (1)
において、前記櫛形電極の各電極の弾性表面波伝播方向
の側壁が絶縁性保護膜で覆われていることを特徴とする
弾性表面波装置。1. 1. A surface acoustic wave device in which a comb-shaped electrode is formed on a piezoelectric substrate, wherein a side wall of each electrode of the comb-shaped electrode in the surface acoustic wave propagation direction is covered with an insulating protective film.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP15189790A JPH0443707A (en) | 1990-06-11 | 1990-06-11 | Surface acoustic wave device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP15189790A JPH0443707A (en) | 1990-06-11 | 1990-06-11 | Surface acoustic wave device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH0443707A true JPH0443707A (en) | 1992-02-13 |
Family
ID=15528583
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP15189790A Pending JPH0443707A (en) | 1990-06-11 | 1990-06-11 | Surface acoustic wave device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0443707A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US7034435B2 (en) * | 2001-06-22 | 2006-04-25 | Oki Electric Industry Co., Ltd. | Saw device |
-
1990
- 1990-06-11 JP JP15189790A patent/JPH0443707A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US7034435B2 (en) * | 2001-06-22 | 2006-04-25 | Oki Electric Industry Co., Ltd. | Saw device |
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