JPH03217109A - Surface acoustic wave resonator - Google Patents
Surface acoustic wave resonatorInfo
- Publication number
- JPH03217109A JPH03217109A JP1420990A JP1420990A JPH03217109A JP H03217109 A JPH03217109 A JP H03217109A JP 1420990 A JP1420990 A JP 1420990A JP 1420990 A JP1420990 A JP 1420990A JP H03217109 A JPH03217109 A JP H03217109A
- Authority
- JP
- Japan
- Prior art keywords
- acoustic wave
- surface acoustic
- electrode
- wave resonator
- piezoelectric substrate
- 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 44
- 239000000758 substrate Substances 0.000 claims abstract description 16
- 230000005284 excitation Effects 0.000 claims description 8
- 238000005530 etching Methods 0.000 abstract description 10
- 238000003780 insertion Methods 0.000 abstract description 10
- 230000037431 insertion Effects 0.000 abstract description 10
- 238000004519 manufacturing process Methods 0.000 description 2
- 230000007423 decrease Effects 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000007772 electrode material Substances 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 238000001259 photo etching Methods 0.000 description 1
Landscapes
- Surface Acoustic Wave Elements And Circuit Networks Thereof (AREA)
Abstract
Description
【発明の詳細な説明】
(イ)産業上の利用分野
本発明は、RFコンバータ等に使用される弾性表面波共
振子に関するものである。DETAILED DESCRIPTION OF THE INVENTION (a) Field of Industrial Application The present invention relates to a surface acoustic wave resonator used in RF converters and the like.
(口)従来の技術 第3図は弾性表面波共振子を示す図である。(mouth) Conventional technology FIG. 3 is a diagram showing a surface acoustic wave resonator.
(1)はLiTaOs等からなる圧電基板、(2)は弾
性表面波を励振する弾性表面波励振電極であり、圧電基
板上(1)にインターデジタル状に形成されている。(
3)(4)は弾性表面波励振電極(2)の両側に、対向
配置されている弾性表面波反射電極である。これら電極
(2 )(3 )(4 )はAj等よりなり、フォトエ
ッチングにより所定の形状に形成される。(1) is a piezoelectric substrate made of LiTaOs or the like, and (2) is a surface acoustic wave excitation electrode for exciting surface acoustic waves, which is formed in an interdigital manner on the piezoelectric substrate (1). (
3) (4) are surface acoustic wave reflecting electrodes placed on both sides of the surface acoustic wave excitation electrode (2) to face each other. These electrodes (2), (3), and (4) are made of Aj, etc., and are formed into a predetermined shape by photo-etching.
斯る表面波共振子の動作を簡単に説明する。The operation of such a surface wave resonator will be briefly explained.
励振電極(2)に所定の共振周波数の電気信号が、印加
されると、圧電基板(1.)表面に弾性表面波が励起さ
れる。励起された弾性表面波は反射電極(3 )(4
)で反射され、反射電極(3)(4)間で反射を繰り返
すことによって定在波となる。そして、再度励振電極(
2)にフィードバックされ、所定の周波数により発振す
る。When an electric signal of a predetermined resonance frequency is applied to the excitation electrode (2), a surface acoustic wave is excited on the surface of the piezoelectric substrate (1.). The excited surface acoustic waves pass through the reflective electrodes (3) (4
) and becomes a standing wave by repeating reflection between the reflective electrodes (3) and (4). Then, the excitation electrode (
2) and oscillates at a predetermined frequency.
このような弾性表面波共振子において、エッチングによ
り形成される電極は、弾性表面波の伝播方向(A)にお
ける断面形状が下辺が長い台形状となる。第4図に弾性
表面波の伝播方向における反射電極(3)の断面図を示
す。In such a surface acoustic wave resonator, the electrode formed by etching has a trapezoidal cross-sectional shape in the propagation direction (A) of the surface acoustic wave with a long lower side. FIG. 4 shows a cross-sectional view of the reflective electrode (3) in the propagation direction of surface acoustic waves.
従来、反射電極(3)は、エッチングにより所望の電極
幅(W)が得やすいように、断面の傾斜角(θ゜)(電
極(3)断面における電極側面(3a)と圧電基板(1
)表面とのなす角度)を約55度にしていた。これは、
反射電極(3)断面の傾斜角(θ゜)と形成される電極
幅(W)は、共にエッチング時間により決まるからであ
る。エッチング時間が長い徨、得られる電極の傾斜角(
θ゛)は大きくなり、電極幅(W)は狭くなる。Conventionally, the reflective electrode (3) has a cross-sectional inclination angle (θ°) (the electrode side surface (3a) in the electrode (3) cross section and the piezoelectric substrate (1)) in order to easily obtain the desired electrode width (W) by etching.
) The angle formed with the surface was approximately 55 degrees. this is,
This is because the inclination angle (θ°) of the cross section of the reflective electrode (3) and the width (W) of the formed electrode are both determined by the etching time. The longer the etching time, the tilt angle of the electrode obtained (
θ゛) becomes larger and the electrode width (W) becomes narrower.
(ハ)発明が解決しようとする課題
ところで、表面波共振子の挿入損失を改善する場合、反
射電極(3)(4)の反射効率を上げる必要がある。反
射効率を上げる方法としては、反射電極(3 )(4
)の本数を多くするか、開口長を大きくする方法がある
。しかしながら、この方法では電極パターンサイズが大
きくなるという問題がある。(c) Problems to be Solved by the Invention In order to improve the insertion loss of the surface acoustic wave resonator, it is necessary to increase the reflection efficiency of the reflection electrodes (3) and (4). One way to increase reflection efficiency is to use reflective electrodes (3) (4).
) or increase the aperture length. However, this method has a problem in that the electrode pattern size becomes large.
また、特開昭62−168410号公報(11031{
9/25)には、この問題を解消する弾性表面波共振
子が開示されている。この弾性表面波共振子においては
、3
反射電極を低密度層と高密度層を順次交互に積層して形
成することにより、反射電極の反射効率を高めている。Also, Japanese Patent Application Laid-open No. 168410/1983 (11031{
9/25) discloses a surface acoustic wave resonator that solves this problem. In this surface acoustic wave resonator, three reflective electrodes are formed by sequentially and alternately stacking low-density layers and high-density layers, thereby increasing the reflection efficiency of the reflective electrode.
しかしながら、斯る表面波共振子は低密度層と高密度層
を交互に積層しなければならないので、製造工数が多く
なるとともに2種類の電極材料が必要となるという問題
がある。However, since such a surface acoustic wave resonator requires alternating stacking of low-density layers and high-density layers, there are problems in that the number of manufacturing steps increases and two types of electrode materials are required.
そこで、本発明は電極パターンサイズを大きくすること
がなく、かつ製造工数の増加を来すことなく挿入損失を
改善した弾性表面波共振子を提供することを目的とする
。SUMMARY OF THE INVENTION Therefore, an object of the present invention is to provide a surface acoustic wave resonator with improved insertion loss without increasing the electrode pattern size or increasing the number of manufacturing steps.
(二)課題を解決するための手段
上述の問題に鑑み、本発明は圧電基板と、この圧電基板
上に形成される弾性表面波励振電極と、この弾性表面波
励振電極に対向配置される弾性表面波反射電極とを備え
る弾性表面波共振子であって、反射電極は、弾性表面波
伝播方向の断面における側面と圧電基板表面との為す角
度が60度ないし75度の範囲であることを特徴とする
ものである。(2) Means for Solving the Problems In view of the above-mentioned problems, the present invention includes a piezoelectric substrate, a surface acoustic wave excitation electrode formed on the piezoelectric substrate, and an elastic A surface acoustic wave resonator comprising a surface acoustic wave reflecting electrode, wherein the reflecting electrode is characterized in that the angle between the side surface and the piezoelectric substrate surface in a cross section in the surface acoustic wave propagation direction is in the range of 60 degrees to 75 degrees. That is.
4
(ホ)作用
反射電極断面の上記角度を上記範囲に規定することによ
り、従来この角度を約55度付近にしていたものに比べ
て反射電極の質量が増加するので、反射電極の反射効率
が向上する。4 (e) By defining the above-mentioned angle of the cross section of the working reflective electrode within the above range, the mass of the reflective electrode increases compared to when this angle was conventionally set at around 55 degrees, so the reflection efficiency of the reflective electrode increases. improves.
(へ)実施例 本発明の一実施例を以下に説明する。(f) Example An embodiment of the present invention will be described below.
本発明の弾性表面波共振子の電極構成は、例えば、第3
図に示した従来例と同様である。第1図は、その弾性表
面波共振子の弾性表面波伝播方向における反射電極部分
の断面図である。(1)はLiTags等よりなる圧電
基板、(3)は圧電基板(1)上に形成されたAl等よ
りなる反射電極である。(θ)は傾斜角であり、反射電
極(3)断面における圧電基板(1)表面と反射電極側
面(3a)とが為す角度を示す。The electrode configuration of the surface acoustic wave resonator of the present invention is, for example, a third
This is similar to the conventional example shown in the figure. FIG. 1 is a sectional view of a reflective electrode portion of the surface acoustic wave resonator in the surface acoustic wave propagation direction. (1) is a piezoelectric substrate made of LiTags or the like, and (3) is a reflective electrode made of Al or the like formed on the piezoelectric substrate (1). (θ) is an inclination angle, and indicates the angle formed between the surface of the piezoelectric substrate (1) and the side surface (3a) of the reflective electrode in the cross section of the reflective electrode (3).
この傾斜角(θ)を変化させたときの弾性表面波共振子
の挿入損失の特性を第2図に示す。この図より、傾斜角
(θ)が大きくなるにつれて挿入損失が小さくなってい
ることが分かる。例えば、傾斜角(θ)が60度のとき
は、55度のときに比べて約0.05dB改善されてい
る。FIG. 2 shows the insertion loss characteristics of the surface acoustic wave resonator when changing the tilt angle (θ). From this figure, it can be seen that the insertion loss decreases as the tilt angle (θ) increases. For example, when the inclination angle (θ) is 60 degrees, it is improved by about 0.05 dB compared to when it is 55 degrees.
挿入損失は傾斜角(θ)を大きくすることで改善される
が、あまり大きくすることはできない。それは、反射電
極の傾斜角(θ)は前述のようにエッチング時間により
決まるからである。即ち、エッチングによる傾斜角(θ
)を垂直に近付ける場合、エッチング時間を長く取らな
ければならい。エッチング時間を長くすると、電極幅(
W)はそれだけ細くなる。このため、所望の電極幅(W
)を得るためには、エッチング時間に応じた分だけ電極
パターン幅を広くしたフォトマスクを用いて、レジスト
を露光しなければならない。フォトマスクの電極パター
ン幅が広いと、フォトマスクの電極パターン間隔は狭く
なるので、充分にレジストが露光されず、エッチングが
充分に行われなくなるおそれがある。Insertion loss can be improved by increasing the tilt angle (θ), but it cannot be increased too much. This is because the tilt angle (θ) of the reflective electrode is determined by the etching time as described above. That is, the tilt angle (θ
), it is necessary to take longer etching time. Increasing the etching time increases the electrode width (
W) becomes that much thinner. Therefore, the desired electrode width (W
), it is necessary to expose the resist using a photomask whose electrode pattern width is increased by an amount corresponding to the etching time. If the electrode pattern width of the photomask is wide, the spacing between the electrode patterns of the photomask becomes narrow, so that the resist may not be sufficiently exposed and etching may not be performed satisfactorily.
よって、本発明の弾性表面波共振子では、生産性を考慮
して傾斜角(θ)の上限は請求の範囲に規定したように
75度とした。Therefore, in the surface acoustic wave resonator of the present invention, in consideration of productivity, the upper limit of the inclination angle (θ) is set to 75 degrees as defined in the claims.
以上のように、反射電極の傾斜角(θ)を太き《するこ
とにより、反射効率が向上し、それによって挿入損失が
改善される。As described above, by increasing the inclination angle (θ) of the reflective electrode, the reflection efficiency is improved, thereby improving the insertion loss.
(ト)発明の効果
本発明の弾性表面波共振子は、反射電極の傾斜角を60
度ないし75度の範囲にすることにより、パターンサイ
ズを大きくすることなく挿入損失を改善することができ
る。(g) Effects of the invention The surface acoustic wave resonator of the invention has a reflective electrode with an inclination angle of 60
By setting the angle between degrees and 75 degrees, insertion loss can be improved without increasing the pattern size.
第1図は本発明の弾性表面波共振子の弾性表面波伝播方
向における反射電極部分の断面図、第2図は弾性表面波
共振子の反射電極断面の傾斜角に対する挿入損失を示す
図、第3図は弾性表面波共振子を示す平面図、第4図は
従米の弾性表面波共振子の弾性表面波伝播方向における
反射電極部分の断面図である。
(1)・・・圧電基板、(2)・・・弾性表面波励振電
極、(3)・・・弾性表面波反射電極。FIG. 1 is a cross-sectional view of the reflective electrode portion of the surface acoustic wave resonator of the present invention in the surface acoustic wave propagation direction, FIG. FIG. 3 is a plan view showing a surface acoustic wave resonator, and FIG. 4 is a cross-sectional view of a reflective electrode portion of the surface acoustic wave resonator made by Yomei in the surface acoustic wave propagation direction. (1)...Piezoelectric substrate, (2)...Surface acoustic wave excitation electrode, (3)...Surface acoustic wave reflecting electrode.
Claims (1)
射電極とを備える弾性表面波共振子において、 前記弾性表面波反射電極は、弾性表面波伝播方向の断面
における側面と圧電基板表面との為す角度が60度ない
し75度の範囲であることを特徴とする弾性表面波共振
子。(1) In a surface acoustic wave resonator comprising a piezoelectric substrate, a surface acoustic wave excitation electrode formed on the piezoelectric substrate, and a surface acoustic wave reflection electrode disposed opposite to the surface acoustic wave excitation electrode, the elastic A surface acoustic wave resonator characterized in that the surface acoustic wave reflecting electrode has an angle between the side surface and the surface of the piezoelectric substrate in a cross section in the surface acoustic wave propagation direction in a range of 60 degrees to 75 degrees.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1420990A JPH03217109A (en) | 1990-01-23 | 1990-01-23 | Surface acoustic wave resonator |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1420990A JPH03217109A (en) | 1990-01-23 | 1990-01-23 | Surface acoustic wave resonator |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH03217109A true JPH03217109A (en) | 1991-09-24 |
Family
ID=11854715
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1420990A Pending JPH03217109A (en) | 1990-01-23 | 1990-01-23 | Surface acoustic wave resonator |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH03217109A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US7893597B2 (en) | 2005-09-20 | 2011-02-22 | Kyocera Corporation | Surface acoustic wave element and surface acoustic wave device |
| WO2011145449A1 (en) * | 2010-05-19 | 2011-11-24 | 株式会社村田製作所 | Surface acoustic wave device |
-
1990
- 1990-01-23 JP JP1420990A patent/JPH03217109A/en active Pending
Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US7893597B2 (en) | 2005-09-20 | 2011-02-22 | Kyocera Corporation | Surface acoustic wave element and surface acoustic wave device |
| WO2011145449A1 (en) * | 2010-05-19 | 2011-11-24 | 株式会社村田製作所 | Surface acoustic wave device |
| JPWO2011145449A1 (en) * | 2010-05-19 | 2013-07-22 | 株式会社村田製作所 | Surface acoustic wave device |
| US9368712B2 (en) | 2010-05-19 | 2016-06-14 | Murata Manufacturing Co., Ltd. | Surface acoustic wave device |
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