JPS5910609B2 - surface acoustic wave device - Google Patents
surface acoustic wave deviceInfo
- Publication number
- JPS5910609B2 JPS5910609B2 JP4509376A JP4509376A JPS5910609B2 JP S5910609 B2 JPS5910609 B2 JP S5910609B2 JP 4509376 A JP4509376 A JP 4509376A JP 4509376 A JP4509376 A JP 4509376A JP S5910609 B2 JPS5910609 B2 JP S5910609B2
- Authority
- JP
- Japan
- Prior art keywords
- electrode
- surface acoustic
- comb
- acoustic wave
- wave device
- 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
Links
- 238000010897 surface acoustic wave method Methods 0.000 title claims description 18
- 239000010408 film Substances 0.000 claims description 14
- 239000010409 thin film Substances 0.000 claims description 6
- 239000000758 substrate Substances 0.000 description 4
- 238000004519 manufacturing process Methods 0.000 description 3
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- 238000002592 echocardiography Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- WABPQHHGFIMREM-UHFFFAOYSA-N lead(0) Chemical compound [Pb] WABPQHHGFIMREM-UHFFFAOYSA-N 0.000 description 1
- 238000001259 photo etching Methods 0.000 description 1
- 230000001052 transient effect Effects 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03H—IMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
- H03H9/00—Networks comprising electromechanical or electro-acoustic elements; Electromechanical resonators
- H03H9/02—Details
- H03H9/02535—Details of surface acoustic wave devices
- H03H9/02818—Means for compensation or elimination of undesirable effects
- H03H9/02866—Means for compensation or elimination of undesirable effects of bulk wave excitation and reflections
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03H—IMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
- H03H9/00—Networks comprising electromechanical or electro-acoustic elements; Electromechanical resonators
- H03H9/02—Details
- H03H9/02228—Guided bulk acoustic wave devices or Lamb wave devices having interdigital transducers situated in parallel planes on either side of a piezoelectric layer
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03H—IMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
- H03H9/00—Networks comprising electromechanical or electro-acoustic elements; Electromechanical resonators
- H03H9/02—Details
- H03H9/02535—Details of surface acoustic wave devices
- H03H9/02543—Characteristics of substrate, e.g. cutting angles
- H03H9/02574—Characteristics of substrate, e.g. cutting angles of combined substrates, multilayered substrates, piezoelectrical layers on not-piezoelectrical substrate
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03H—IMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
- H03H9/00—Networks comprising electromechanical or electro-acoustic elements; Electromechanical resonators
- H03H9/02—Details
- H03H9/02535—Details of surface acoustic wave devices
- H03H9/02818—Means for compensation or elimination of undesirable effects
- H03H9/02842—Means for compensation or elimination of undesirable effects of reflections
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03H—IMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
- H03H9/00—Networks comprising electromechanical or electro-acoustic elements; Electromechanical resonators
- H03H9/02—Details
- H03H9/125—Driving means, e.g. electrodes, coils
- H03H9/145—Driving means, e.g. electrodes, coils for networks using surface acoustic waves
- H03H9/14544—Transducers of particular shape or position
- H03H9/14552—Transducers of particular shape or position comprising split fingers
Landscapes
- Physics & Mathematics (AREA)
- Acoustics & Sound (AREA)
- Surface Acoustic Wave Elements And Circuit Networks Thereof (AREA)
Description
【発明の詳細な説明】
本発明は弾性表面波装置、特に新しい構成のトランスジ
ューサを有する弾性表面波装置に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a surface acoustic wave device, and more particularly to a surface acoustic wave device having a transducer of a new configuration.
従来、圧電性薄膜を使用した弾性表面波装置としては、
第1図に示すような構造のものが使用されている。Conventionally, surface acoustic wave devices using piezoelectric thin films include:
A structure as shown in FIG. 1 is used.
すなわち、図において、1は基板、2はその表面に形成
された1対の櫛型電極、3は電極2の表面を含めて、基
板1の表面に形成された圧電性薄膜、4は対向電極で、
このトランスジューサの実効的電気機械結合係数を増大
させるだめのものである。That is, in the figure, 1 is a substrate, 2 is a pair of comb-shaped electrodes formed on the surface thereof, 3 is a piezoelectric thin film formed on the surface of the substrate 1 including the surface of electrode 2, and 4 is a counter electrode. in,
This serves to increase the effective electromechanical coupling coefficient of the transducer.
このような装置において、その中心周波数における弾性
表面波の波長をλ。In such a device, the wavelength of the surface acoustic wave at its center frequency is λ.
とすると、櫛型電極λ
2の寸法は、電極指の巾が−j1電極指の間隙が?であ
る。Then, the dimensions of the comb-shaped electrode λ2 are: the width of the electrode fingers is -j1, and the gap between the electrode fingers is? It is.
かかる構成は、弾性表面波を励振または受信するための
、もつとも簡単で効率のよいものである。Such a configuration is extremely simple and efficient for exciting or receiving surface acoustic waves.
しかし、トランスジューサにおける弾性表面波の反射が
大きく、この種装置の設計上、大きな問題となっていた
。However, the reflection of surface acoustic waves in the transducer is large, which has been a major problem in the design of this type of device.
この反射を軽減するために、櫛型電極を、第2図に示す
ような、いわゆるスプリット型とすることが行なわれて
いる。In order to reduce this reflection, the comb-shaped electrode is made into a so-called split type as shown in FIG.
これは、その電極指の巾、λ0
および電極指の間隙が、それぞれWときわめて狭いもの
である。This is because the width of the electrode fingers, λ0, and the gap between the electrode fingers are W, which are extremely narrow.
電極指の巾が狭いと、当然、製造時にその線切れが生じ
やすくなり、量産化する上で、大きな問題となっている
。If the width of the electrode fingers is narrow, it is natural that the wires are likely to break during manufacturing, which poses a major problem in mass production.
本発明は、かかる問題を解決することができる・表面弾
性波装置を提供しようとするものである。The present invention aims to provide a surface acoustic wave device that can solve such problems.
以下、その一実施例について第3図Aの断面図、同図B
の平面図を用いて説明する。The following is a cross-sectional view of FIG. 3A and FIG. 3B for one embodiment.
This will be explained using a plan view.
なお、第3図Aは同図Bのc−c’線に沿った断面図で
ある。Note that FIG. 3A is a sectional view taken along line cc' in FIG. 3B.
図において、11は基板で、その一方の表面に1対の櫛
型電極12、圧電性膜13、および対向電極14力順次
形成されている。In the figure, 11 is a substrate, on one surface of which a pair of comb-shaped electrodes 12, a piezoelectric film 13, and a counter electrode 14 are sequentially formed.
3 櫛型電極12の電極指の巾は『λ。3 The width of the electrode fingers of the comb-shaped electrode 12 is λ.
であり、電λ0 極指の間隙は1「である。, and the electric λ0 The gap between the pole fingers is 1".
対向電極14は櫛型電極12の電極指の間隙上にそれぞ
れ電極指の長手方向に平行配置されてお3 λ。The counter electrodes 14 are arranged parallel to each other in the longitudinal direction of the electrode fingers on the gaps between the electrode fingers of the comb-shaped electrode 12 and have a width of 3 λ.
一、り、その線巾および間隙はそれぞれWλo ,s
Lある。1, the line width and the gap are Wλo and s, respectively
There is L.
対向電極14と櫛型電極12とは、一方の電極の中央が
、他方の電極の間隙に位置するよう、配置されている。The counter electrode 14 and the comb-shaped electrode 12 are arranged so that the center of one electrode is located in the gap between the other electrode.
このように構成すると、対向電極14の導電膜λ。With this configuration, the conductive film λ of the counter electrode 14.
の端部と、櫛型電極12の導電膜の端部とはiだけずれ
ることになり、端部における弾性表面波λ。The end of the comb-shaped electrode 12 and the end of the conductive film of the comb-shaped electrode 12 are shifted by i, and the surface acoustic wave λ at the end.
の反射波は丁ずれることになって、それぞれによる反射
波が相殺しあって、その振巾が減少する,無論、電極1
2.14の位置を互いに入れ換えても、同じことが言え
る。The reflected waves of the electrode 1 are shifted, and the reflected waves of each cancel each other out, reducing the amplitude.
The same thing can be said even if the positions of 2.14 are swapped with each other.
上記電極の相対的な位置関係が保持される限り,いわゆ
る重みづけしたトランスジューサ、すなわち、櫛型電極
の電極指の長さ、または対向電極の導電性膜の長さを、
その位置によって変化させて重みづけの特性をもたせる
ものについても、反射波を抑圧する効果を得ることがで
きる。As long as the relative positional relationship of the electrodes is maintained, the length of the electrode fingers of the so-called weighted transducer, i.e. the comb-shaped electrode, or the conductive film of the counter electrode,
It is also possible to obtain the effect of suppressing reflected waves by changing the weighting characteristics depending on the position.
また、製造時において、しばしば、櫛型電極と対向電極
との位置合わせに誤差を生ずることがあり、対向電極の
導電性膜の電位が一定にならないことがある。Furthermore, during manufacturing, errors often occur in the alignment between the comb-shaped electrode and the counter electrode, and the potential of the conductive film of the counter electrode may not be constant.
これは、対向電極を構成する各導電性膜を電気的に接続
することにより、防止することができる。This can be prevented by electrically connecting the conductive films forming the counter electrode.
その電気的な接続は、対向電極の形成時に一体に形成す
るか、あるいはそれを形成してからリード線で接続すれ
ばよい。The electrical connection may be formed integrally when forming the counter electrode, or may be formed and then connected using a lead wire.
以上説明したように、本発明にかかる弾性表面波装置は
、圧電性薄膜の一方の両側に櫛型電極を配置するととも
に、その他方の面側に対向電極を構成する導電性膜を、
その中央が櫛型電極の電極指の間隙の中央に位置するよ
う配置してなり、櫛型電極の電極指の巾および対向電極
の導電性膜の巾をそれぞれジλ0とするとともに、電極
指の間8 λ。As explained above, the surface acoustic wave device according to the present invention has a comb-shaped electrode arranged on both sides of one side of a piezoelectric thin film, and a conductive film constituting a counter electrode on the other side.
The center thereof is located at the center of the gap between the electrode fingers of the comb-shaped electrode, and the width of the electrode fingers of the comb-shaped electrode and the width of the conductive film of the counter electrode are respectively set to λ0, and the width of the electrode fingers of the comb-shaped electrode is set to λ0. Between 8 λ.
隙および導電性膜の間隙をそれぞれj 七1−たこ;
とを特徴とする。The gap and the gap between the conductive films are respectively j 71-octopus;
It is characterized by.
この構成の装置によれば、電極での弾性表面波の反射に
よる3重反射信号(トリプル・トランジエント・エコー
)を、主信号に対して−40dB以下に抑圧することが
できる。According to the device having this configuration, triple reflected signals (triple transient echoes) caused by reflection of surface acoustic waves at the electrodes can be suppressed to -40 dB or less with respect to the main signal.
また、電極指や導電性膜の巾を、スプリット型の櫛1型
電極における電極指の巾の3倍とすることができ、ホト
エッチングにおけるいわゆる線切れもきわめて少なくな
り、装置の歩留りを大巾に低下させることができる。In addition, the width of the electrode fingers and conductive film can be made three times the width of the electrode fingers in a split-type comb type electrode, and the so-called line breakage during photoetching is extremely reduced, greatly increasing the yield of the device. can be lowered to
7 第1図は従来の弾性表面波装置の典型的な構造を示
す要部断面図、第2図は同じく弾性表面波の反射を軽減
させたトランスジューサの構造を示す図である。
第3図は本発明にかかる弾性表面波装置の一実施例の構
造を示し、同図Aはその要部断1面図、同mBはそのト
ランスジューサの位置関係を示す平面図である。
、11・・・・・・基板、12・・・・・・櫛型電極、
13・・・・・・圧電性薄膜、14・・・・・・対向電
極。
−37−7. FIG. 1 is a sectional view of a main part showing a typical structure of a conventional surface acoustic wave device, and FIG. 2 is a view showing the structure of a transducer that similarly reduces reflection of surface acoustic waves. FIG. 3 shows the structure of an embodiment of a surface acoustic wave device according to the present invention, and FIG. 3A is a cross-sectional view of a main part thereof, and FIG. 3B is a plan view showing the positional relationship of its transducers. , 11... substrate, 12... comb-shaped electrode,
13...Piezoelectric thin film, 14...Counter electrode. -37-
Claims (1)
もに、その他方の面側に、対向電極を構成する導電性膜
を、その中央が前記櫛型電極の電極指の間涼の中央に位
置するよう配置してなり、前記櫛型電極の電極指の巾お
よび前記対向電極の導3 電性膜の巾をそれぞれ『λ。 とF・かつ前記櫛型電極の電極指の間隙をそれぞれ『λ
。 とじたことを特徴とする弾性表面波装置(ただし、λ。 はこの装置の中心周波数におりる弾性表面波の波長であ
る)。 2 特許請求の範囲第1項の記載において、前記対向電
極の導電性膜をお互いに電気的に接続したことを特徴と
する弾性表面波装置。 3 特許請求の範囲第1項または第2項の記載において
、前記櫛型電極の電極指および前記対向電極の導電性膜
のうちの少なくともいずれか一方の長さを、位置によっ
て変化させ、重みづけしたことを特徴とする弾性表面波
装置。[Scope of Claims] 1. A comb-shaped electrode is arranged on one side of a piezoelectric thin film, and a conductive film constituting a counter electrode is arranged on the other side of the piezoelectric thin film. The width of the electrode fingers of the comb-shaped electrode and the width of the conductive film of the counter electrode are respectively "λ". and F, and the gap between the electrode fingers of the comb-shaped electrode is ``λ
. A surface acoustic wave device (where λ is the wavelength of the surface acoustic wave that falls at the center frequency of this device). 2. The surface acoustic wave device according to claim 1, wherein the conductive films of the opposing electrodes are electrically connected to each other. 3. In the description of claim 1 or 2, the length of at least one of the electrode fingers of the comb-shaped electrode and the conductive film of the counter electrode is changed depending on the position and weighted. A surface acoustic wave device characterized by:
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4509376A JPS5910609B2 (en) | 1976-04-20 | 1976-04-20 | surface acoustic wave device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4509376A JPS5910609B2 (en) | 1976-04-20 | 1976-04-20 | surface acoustic wave device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS52128034A JPS52128034A (en) | 1977-10-27 |
| JPS5910609B2 true JPS5910609B2 (en) | 1984-03-10 |
Family
ID=12709685
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP4509376A Expired JPS5910609B2 (en) | 1976-04-20 | 1976-04-20 | surface acoustic wave device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5910609B2 (en) |
-
1976
- 1976-04-20 JP JP4509376A patent/JPS5910609B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS52128034A (en) | 1977-10-27 |
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