JPH07107967B2 - Surface acoustic wave device - Google Patents
Surface acoustic wave deviceInfo
- Publication number
- JPH07107967B2 JPH07107967B2 JP61003428A JP342886A JPH07107967B2 JP H07107967 B2 JPH07107967 B2 JP H07107967B2 JP 61003428 A JP61003428 A JP 61003428A JP 342886 A JP342886 A JP 342886A JP H07107967 B2 JPH07107967 B2 JP H07107967B2
- Authority
- JP
- Japan
- Prior art keywords
- surface acoustic
- acoustic wave
- electrode
- wave device
- 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.)
- Expired - Lifetime
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- Piezo-Electric Or Mechanical Vibrators, Or Delay Or Filter Circuits (AREA)
- Electrodes Of Semiconductors (AREA)
- Internal Circuitry In Semiconductor Integrated Circuit Devices (AREA)
- Surface Acoustic Wave Elements And Circuit Networks Thereof (AREA)
Description
【発明の詳細な説明】 〔発明の利用分野〕 本発明は、弾性表面波装置の信頼性向上に係り、特に大
電力を伝送する弾性表面波装置もしくは、大振幅の表面
波波動が定在波として存在する弾性表面波共振器に好適
な電極、反射器に関する。Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to improving the reliability of a surface acoustic wave device, and particularly relates to a surface acoustic wave device that transmits a large amount of electric power or a surface acoustic wave with a large amplitude standing wave. The present invention relates to an electrode and a reflector suitable for a surface acoustic wave resonator.
弾性表面波装置の応用範囲が拡がり、大電力を伝送する
弾性表面波フィルタや、大振幅の表面波波動が定在波と
して存在する弾性表面波共振器が用いられるようになっ
た。The range of applications of surface acoustic wave devices has expanded, and surface acoustic wave filters that transmit large amounts of power and surface acoustic wave resonators that have large amplitude surface wave waves as standing waves have come to be used.
ところが、上記の如き弾性表面波装置においてはその送
受波電極、反射器の微細なAl電極指において、電子通信
学会論文誌、巻J67C号、278頁〜285頁(1984年3月)に
示される様に、半導体集積回路のAl配線電極に生ずるエ
レクトロ・マイグレーションによる突起(ヒロック
ス)、空隙(ボイド)等の欠陥と同様の欠陥、すなわち
Alマイグレーションが発生し、弾性表面波共振器では共
振周波数のずれ、大電力を伝送する弾性表面波フィルタ
ではヒロックス生長による短絡、断線などの故障が頻発
していた。However, in the surface acoustic wave device as described above, the transmitting and receiving electrodes and the fine Al electrode fingers of the reflector are shown in the IEICE Transactions, Vol. J67C, pp. 278-285 (March 1984). Similarly, defects similar to defects such as protrusions (hillox) and voids due to electromigration that occur in the Al wiring electrodes of the semiconductor integrated circuit, that is,
Al migration frequently occurred, and the surface acoustic wave resonator had frequent deviations in the resonance frequency, and surface acoustic wave filters that transmitted large amounts of power often suffered short-circuiting and disconnection due to hillox growth.
上記文献では、この様な欠陥の発生メカニズムは「弾性
表面波によって生ずる基板表面の歪が、表面上に形成さ
れたAl薄膜に内部応力を発生させ、応力がある値を越え
た部分ではAlの結晶粒界移動が起こり、ボイド及びヒロ
ックスが生ずる。内部応力による粒界移動は、アイトリ
プルイー・トランザクション・パーツ・ハイブリッズ・
アンド・パッケージング、巻PHP−7、3号、134頁〜13
8頁(1971年9月)(IEEE Trans,Parts,Hybrids and Pa
ckag)に示される集積回路の温度サイクルにおける場合
と同じメカニズムと考えられる。」旨を述べている。上
記第1の文献では、このようなAlマイグレーションによ
る欠陥の対策として、半導体集積回路で用いられている
ようにAlに微量(1〜4%)の銅(Cu)を添加する方法
を述べ、Alマイグレーション抑圧に対する有効性を示し
ている。In the above-mentioned literature, the mechanism of occurrence of such a defect is that "the strain on the substrate surface caused by surface acoustic waves causes internal stress in the Al thin film formed on the surface, and the stress exceeds a certain value. Grain boundary migration occurs, resulting in voids and hillocks.Grain boundary migration due to internal stress is caused by eye triple e transaction parts hybrids
And Packaging, Volume PHP-7, Issue 3, pp. 13-13
Page 8 (September 1971) (IEEE Trans, Parts, Hybrids and Pa
It is considered that the mechanism is the same as in the temperature cycle of the integrated circuit shown in ckag). ". The above-mentioned first document describes a method of adding a trace amount (1 to 4%) of copper (Cu) to Al as used in a semiconductor integrated circuit as a countermeasure against such defects due to Al migration. It shows the effectiveness against the suppression of migration.
しかし、Cuを用いた場合には、膜の硬度が大きくなりや
すく、ワイヤボンディングが打ちにくくなる欠点があっ
た。また、高周波化を図り、微細電極を高精度に形成す
るドライエッチング法を導入するに際し、電極の腐食等
が発生しやすく、歩留まりが大幅に低下する問題点があ
った。さらに、高周波では伝送電力あるいは振幅が変わ
らなくとも表面波歪が大きくなるので、上記第1の文献
に見られる抵抗加熱あるいはEB加熱蒸着によるCu添加Al
電極では、大電力(大振幅)動作時には十分な寿命が保
証できなくなる。However, when Cu is used, the hardness of the film tends to increase, and there is a drawback that wire bonding becomes difficult to hit. Further, when introducing a dry etching method for achieving high frequency and forming a fine electrode with high precision, there is a problem that corrosion of the electrode is likely to occur and the yield is significantly reduced. Furthermore, at high frequencies, the surface wave distortion increases even if the transmitted power or amplitude does not change.
With electrodes, a sufficient life cannot be guaranteed when operating at high power (large amplitude).
本発明の目的は、ワイヤボンディングが打ちやすく、微
細電極の高精度化、高歩留り化を容易にするドライエッ
チングを容易に導入できると同時に、Alマイグレーショ
ンを抑圧することにより大電力(大振幅)動作を可能に
する電極を有する弾性表面波装置を提供することにあ
る。An object of the present invention is to facilitate wire bonding, to easily introduce dry etching that facilitates high precision and high yield of fine electrodes, and at the same time, suppresses Al migration to operate at high power (large amplitude). An object of the present invention is to provide a surface acoustic wave device having an electrode that enables the above.
本発明では、上記目的を達成するために、Alに添加する
元素として反応生成塩化物CuCl3の沸点が高いCuではな
く、変わりに塩化物TiCl4の沸点が低く、ドライエッチ
ングも容易であるものの、電気抵抗の大幅な増大を招く
ものとして、電極材料であるAlに添加することなど通常
では到底考えられなかったTiを用いることとした。しか
も蒸着法に変え組成の制御の安定したスパッタ法、例え
ばDCスパッタ法を適用して高周波弾性表面波装置の電極
を形成した。In the present invention, in order to achieve the above object, not the Cu having a high boiling point of the reaction product chloride CuCl 3 as an element to be added to Al, instead the boiling point of the chloride TiCl 4 is low, and dry etching is also easy. It was decided to use Ti, which could not be usually considered by adding it to Al, which is an electrode material, because it causes a large increase in electric resistance. Moreover, the electrode of the high frequency surface acoustic wave device was formed by applying a sputtering method with stable composition control instead of the vapor deposition method, for example, a DC sputtering method.
これにより、ドライエッチング時に反応生成塩化物が揮
発して電極の腐食が発生せず、ドライエッチングが容易
になる。また、弾性表面波基板上に薄膜断面の全体にわ
たりTiを分布させて添加したAl電極を具備しているの
で、その論理的帰結として結晶の粒界だけでなく、結晶
の粒内でも強化されており、その結果として優れた耐電
力性を確認したものである。なお、電極であるAlにTiを
添加しているために電気抵抗が増大するものの、実際に
は動作に影響を与えるような問題はなかった。As a result, the chloride produced by the reaction does not volatilize during the dry etching, and the electrodes do not corrode. In addition, since the surface acoustic wave substrate is equipped with an Al electrode added with Ti distributed over the entire cross section of the thin film, the logical consequence is that it is strengthened not only within the crystal grain boundaries but also within the crystal grains. As a result, excellent power resistance was confirmed. It should be noted that although the electrical resistance increases because Ti is added to the electrode Al, there is no problem that actually affects the operation.
〔発明の実施例〕 以下、本発明の実施例を第1図により説明する。[Embodiment of the Invention] An embodiment of the present invention will be described below with reference to FIG.
本図において、1は弾性表面波基板でSTcut水晶を用
い、該基板表面上に1組の送受波電極2,2′が開口1000
μm、28対で、互いに弾性表面波を送受するように設け
られており、該電極は母線電極(図示せず)を通してボ
ンディングパッド3,3′と接続され、ボンディングパッ
ド3,3′はAl線もしくは金線のボンディングワイヤ(図
示せず)をもって、カンパッケージのステムの入出力ピ
ン4,4′に電気的に接続されており、送受波電極の接地
側母線電極(図示せず)は接地側ボンディングパッド
(図示せず)を通じてカンパッケージのステム6に接地
されている。また上記の1組の送受波電極2,2′の両側
に750本の金属ストリップから成る反射器電極10,10′が
設けられ、2開口弾性表面波共振器を構成している。上
記送受波電極2,2′及び反射器電極10,10′の膜厚は0.1
μmで、共振周波数は697MHz、Q≒4000となっている。
電極材料は2wt%のTiを添加したAlであり、DCマグネト
ロンスパッタ法により、被着形成された後、ホトエッチ
ングによりパターン形成されたものである。なお、本実
施例では、AlにTiを2wt%添加しているので、電極の電
気抵抗が増大するものの、動作に影響を与えるような問
題は生じなかった。また、Cu添加に見られるが如き過大
な膜硬度が解消されるので、ワイヤボンディングが容易
に行える。In this figure, reference numeral 1 is a surface acoustic wave substrate using STcut quartz, and a pair of transmitting and receiving electrodes 2, 2 ′ has an opening 1000 on the surface of the substrate.
μm, 28 pairs, which are provided so as to transmit and receive surface acoustic waves to each other. The electrodes are connected to the bonding pads 3, 3 ′ through bus bar electrodes (not shown), and the bonding pads 3, 3 ′ are Al wires. Alternatively, a gold wire bonding wire (not shown) is electrically connected to the input / output pins 4, 4'of the stem of the can package, and the ground side busbar electrode (not shown) of the transmitting / receiving electrode is the ground side. It is grounded to the stem 6 of the can package through a bonding pad (not shown). Further, reflector electrodes 10 and 10 'made up of 750 metal strips are provided on both sides of the above-mentioned pair of transmitting / receiving electrodes 2 and 2', thus forming a two-port surface acoustic wave resonator. The thickness of the transmitting / receiving electrodes 2, 2'and the reflector electrodes 10, 10 'is 0.1
In μm, the resonance frequency is 697 MHz and Q≈4000.
The electrode material is Al to which 2 wt% of Ti has been added, which is deposited by the DC magnetron sputtering method and then patterned by photo-etching. In this example, since 2 wt% of Ti was added to Al, the electric resistance of the electrode increased, but there was no problem that affected the operation. Further, since the excessive film hardness as seen in Cu addition is eliminated, wire bonding can be easily performed.
本実施例の弾性表面波共振器の加速劣化試験の結果を第
2図に示す。なお、比較例としてCu入りAlのEB蒸着によ
る試料の試験結果を示す。横軸には添加元素の膜中の濃
度をwt%で示し、縦軸には劣化時間TF(Time to Failur
e)を示している。この場合のTFは共振周波数の変化し
た時点の時間をもって示している。加速劣化試験条件は
温度120℃、入力電力100mWである。第2図中11は比較例
として示したCu添加AlのEB蒸着による試料の実験結果で
あるが、同図中12で示した本発明のTi添加Alスパッタ電
極を用いた実施例は比較例にたいし、劣化時間は10倍以
上で、耐電力性が大幅に向上している。また、同図12で
はTiの添加の無い場合、すなわち純Alの場合にも同図11
に比べTFが大きくなっている。TFの増大分は、電極膜被
着法をEB蒸着法あるいは抵抗熱蒸着法に変え、スパッタ
法にした効果である。このことは、Ti添加による電気抵
抗の若干の増大分の影響は無視できるとともに、スパッ
タ法によって膜の機械的強度が大きくなることが反映し
たものと見られる。The results of the accelerated deterioration test of the surface acoustic wave resonator of this example are shown in FIG. As a comparative example, test results of a sample obtained by EB vapor deposition of Cu-containing Al are shown. The horizontal axis shows the concentration of the additive element in the film in wt%, and the vertical axis shows the deterioration time TF (Time to Failur).
e) is shown. In this case, TF is shown as the time when the resonance frequency changes. The accelerated deterioration test conditions are a temperature of 120 ° C and an input power of 100 mW. Reference numeral 11 in FIG. 2 is an experimental result of a sample obtained by EB vapor deposition of Cu-added Al shown as a comparative example, but the embodiment using the Ti-added Al sputtered electrode of the present invention shown in 12 in the figure is a comparative example. On the other hand, the deterioration time is more than 10 times, and the power resistance is greatly improved. In addition, in FIG. 12, when Ti is not added, that is, in the case of pure Al, the same FIG.
TF is larger than. The increase in TF is the effect of changing the electrode film deposition method to the EB vapor deposition method or the resistance heat vapor deposition method and using the sputtering method. This is considered to reflect the fact that the effect of a slight increase in electric resistance due to the addition of Ti can be ignored and that the mechanical strength of the film is increased by the sputtering method.
上記実施例は、金属膜ストリップによる反射器を用いた
2開口弾性表面波共振器の場合であるが、本発明はそれ
に限定を受けることなく、1開口弾性表面波共振器、入
力側電極から出力側電極に大きな電力を送る弾性表面波
フィルタであっても、弾性表面波送受波器を共振器とし
て利用したものであってもその効果には変わりが無い。
また弾性表面波基板もSTcut水晶に限定を受けることな
くLiNbO3、LiTaO3等各種基板、カット面方位であっても
有効である。The above-mentioned embodiment is a case of a 2-aperture surface acoustic wave resonator using a reflector made of a metal film strip, but the present invention is not limited thereto, and the 1-aperture surface acoustic wave resonator and the output from the input side electrode are output. Even if it is a surface acoustic wave filter that sends a large amount of power to the side electrode, or one that uses a surface acoustic wave transmitter / receiver as a resonator, the effect is the same.
Also, the surface acoustic wave substrate is not limited to STcut quartz, but is also effective for various substrates such as LiNbO 3 and LiTaO 3 and cut plane orientations.
本発明では、電極であるAlにTiを添加したことにより、
Alマイグレーションを抑圧することから耐電力性が大幅
に向上し、劣化時間が10倍以上である弾性表面波装置を
得ることができた。さらに、それと同時に従来のCu添加
AlのEB加熱蒸着、抵抗加熱蒸着による電極に変えて、Ti
添加のAl薄膜をスパッタ法により形成した電極としたこ
とにより、ドライエッチング導入が容易となることから
微細電極の高精度化、高歩留り化が高くなった。また、
Ti添加によりCu添加に見られるが如き過大な膜硬度が解
消されるので、ワイヤボンディング歩留りも高くなっ
た。In the present invention, by adding Ti to the electrode Al,
Since the Al migration is suppressed, the power resistance is significantly improved, and a surface acoustic wave device having a deterioration time of 10 times or more can be obtained. Furthermore, at the same time, conventional Cu addition
Instead of the electrode by Al EB heating evaporation or resistance heating evaporation, Ti
By using the added Al thin film as the electrode formed by the sputtering method, the introduction of dry etching was facilitated, so that the precision of the fine electrode and the yield were improved. Also,
The addition of Ti eliminates the excessive film hardness seen in addition of Cu, thus increasing the wire bonding yield.
第1図は本発明の実施例の弾性表面波2開口共振器とし
ての弾性表面波装置の断面図、第2図は本発明の効果を
示す加速劣化試験結果を示す図である。 1……弾性表面波装置 2,2′……送受波電極 3,3′……ボンディングパッド 4,4′……入出力ピン 6……カンパッケージのステム 10,10′……弾性表面波反射器 11……EB蒸着によるCu添加Alによる比較例 12……本発明のTi添加の効果を示す実施例FIG. 1 is a cross-sectional view of a surface acoustic wave device as a surface acoustic wave double aperture resonator of an embodiment of the present invention, and FIG. 2 is a diagram showing results of accelerated deterioration test showing effects of the present invention. 1 ... Surface acoustic wave device 2, 2 '... Transceiver electrode 3, 3' ... Bonding pad 4, 4 '... Input / output pin 6 ... Can package stem 10, 10' ... Surface acoustic wave reflection Vessel 11 …… Comparative example with Cu added Al by EB deposition 12 …… Example showing effect of Ti addition of the present invention
───────────────────────────────────────────────────── フロントページの続き (72)発明者 磯前 博己 茨城県勝田市大字稲田1410番地 株式会社 日立製作所東海工場内 (72)発明者 川窪 鐘治 茨城県勝田市大字稲田1410番地 株式会社 日立製作所東海工場内 (72)発明者 山田 純 神奈川県横浜市戸塚区吉田町292番地 株 式会社日立製作所家電研究所内 (56)参考文献 特開 昭58−202551(JP,A) ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Hiroki Isomae 1410 Inada, Katsuta City, Ibaraki Prefecture, Toda Factory, Hitachi Ltd. Inside the factory (72) Inventor Jun Yamada 292 Yoshida-cho, Totsuka-ku, Yokohama-shi, Kanagawa Inside Electric Appliances Research Laboratory, Hitachi, Ltd.
Claims (2)
たりTiを分布させて添加して成るAl薄膜の電極を備えた
構成を特徴とする弾性表面波装置。1. A surface acoustic wave device comprising a surface acoustic wave substrate provided with electrodes of an Al thin film obtained by distributing and adding Ti over the entire cross section of the thin film.
構成であ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 the Al thin film has a Ti addition amount of 2 wt% or less.
Priority Applications (4)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61003428A JPH07107967B2 (en) | 1986-01-13 | 1986-01-13 | Surface acoustic wave device |
| GB8700064A GB2186456B (en) | 1986-01-13 | 1987-01-05 | Surface acoustic wave device |
| DE3700789A DE3700789C2 (en) | 1986-01-13 | 1987-01-13 | Acoustic surface wave component |
| US07/549,643 US5144185A (en) | 1986-01-13 | 1990-07-09 | SAW device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61003428A JPH07107967B2 (en) | 1986-01-13 | 1986-01-13 | Surface acoustic wave device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS62163408A JPS62163408A (en) | 1987-07-20 |
| JPH07107967B2 true JPH07107967B2 (en) | 1995-11-15 |
Family
ID=11557104
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP61003428A Expired - Lifetime JPH07107967B2 (en) | 1986-01-13 | 1986-01-13 | Surface acoustic wave device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH07107967B2 (en) |
Families Citing this family (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH02274008A (en) * | 1989-04-17 | 1990-11-08 | Hitachi Ltd | Solid-state electronic equipment, its manufacture, and device utilizing it |
| JPH0340509A (en) * | 1989-07-06 | 1991-02-21 | Murata Mfg Co Ltd | bulk wave device |
| JP2500435B2 (en) * | 1993-04-09 | 1996-05-29 | 日本電気株式会社 | Dry etching method |
| JP3646116B2 (en) | 2003-07-17 | 2005-05-11 | Tdk株式会社 | Surface acoustic wave device, surface acoustic wave device, surface acoustic wave duplexer, and method of manufacturing surface acoustic wave device |
| JP2005347892A (en) | 2004-05-31 | 2005-12-15 | Fujitsu Media Device Kk | Surface acoustic wave device |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS58202551A (en) * | 1982-05-21 | 1983-11-25 | Hitachi Ltd | Wiring material of electro migration resistance |
-
1986
- 1986-01-13 JP JP61003428A patent/JPH07107967B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS62163408A (en) | 1987-07-20 |
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