JPH08237064A - Transversely coupled dual-mode surface acoustic wave filter - Google Patents

Transversely coupled dual-mode surface acoustic wave filter

Info

Publication number
JPH08237064A
JPH08237064A JP6494995A JP6494995A JPH08237064A JP H08237064 A JPH08237064 A JP H08237064A JP 6494995 A JP6494995 A JP 6494995A JP 6494995 A JP6494995 A JP 6494995A JP H08237064 A JPH08237064 A JP H08237064A
Authority
JP
Japan
Prior art keywords
acoustic wave
surface acoustic
mode
wave filter
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
Application number
JP6494995A
Other languages
Japanese (ja)
Inventor
Toru Onodera
徹 小野寺
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.)
Kyocera Crystal Device Corp
Original Assignee
Kyocera Crystal Device Corp
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 Kyocera Crystal Device Corp filed Critical Kyocera Crystal Device Corp
Priority to JP6494995A priority Critical patent/JPH08237064A/en
Publication of JPH08237064A publication Critical patent/JPH08237064A/en
Pending legal-status Critical Current

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  • Surface Acoustic Wave Elements And Circuit Networks Thereof (AREA)

Abstract

(57)【要約】 【目的】 本発明の目的は、特性が良く信頼性の高い通
過帯域の挟帯域の横結合二重モード弾性表面波フイルタ
を製作できるようにすることである。 【構成】 横結合二重モード弾性表面波フイルタの縦続
接続した接続部と接地間に容量を入れることによって、
弾性表面波フイルタの振動モードのSモード及びAモー
ドの反共振点の周波数を下げることにより、目的が達成
できた。なお、前記の横結合二重モード弾性表面波フイ
ルタの縦続接続した接続部と接地間に入れる容量は、前
記接続部側の櫛型電極の共通バーの外側の近傍に接地電
極を配置することで実現している。
(57) [Summary] [PROBLEMS] An object of the present invention is to make it possible to fabricate a laterally coupled dual-mode surface acoustic wave filter having a narrow band of a pass band having good characteristics and high reliability. [Structure] By inserting a capacitance between the cascaded connection of the laterally coupled dual-mode surface acoustic wave filter and the ground,
The object was achieved by lowering the frequencies of the anti-resonance points of the S mode and the A mode of the vibration mode of the surface acoustic wave filter. In addition, the capacitance to be inserted between the connection portion of the transversely coupled dual-mode surface acoustic wave filters connected in cascade and the ground is obtained by arranging the ground electrode near the outside of the common bar of the comb-shaped electrode on the connection portion side. Has been realized.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】横結合二重モード弾性表面波フイ
ルタにおける、通過帯域の狭帯域化技術に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a technique for narrowing a pass band in a laterally coupled dual mode surface acoustic wave filter.

【0002】[0002]

【従来の技術】従来より、横結合二重モード弾性表面波
フイルタの通過帯域を狭くする方法は、図4に示すよう
に櫛型電極の間隔Gを離すことで結合を粗にして行われ
るのが一般的であった。
2. Description of the Related Art Conventionally, a method of narrowing the pass band of a laterally coupled dual-mode surface acoustic wave filter is performed by coarsely coupling the gaps G between the comb-shaped electrodes as shown in FIG. Was common.

【0003】[0003]

【発明が解決しようとする課題】従来技術では、櫛型電
極の間隔Gを離すことで櫛型電極の結合を粗にする方法
では、一般的にはフイルタの比帯域(通過帯域/中心周
波数)を0.6×10-3より狭くしようとすると、横結
合二重モード弾性表面波フイルタの挿入損失が増大する
という課題があった。比帯域とは、フイルタの通過帯域
(3dB低下の点の幅)をフイルタの中心周波数で割っ
た値を言う。
In the prior art, the method of roughening the coupling of the comb-shaped electrodes by separating the gap G between the comb-shaped electrodes is generally used in general in a specific band (passband / center frequency) of the filter. However, there is a problem in that the insertion loss of the laterally coupled dual-mode surface acoustic wave filter is increased if the value is smaller than 0.6 × 10 −3 . The ratio band is a value obtained by dividing the filter pass band (the width of the point at which the filter is lowered by 3 dB) by the center frequency of the filter.

【0004】[0004]

【課題を解決する手段】課題を解決するために、横結合
二重モード弾性表面波フイルタの縦続接続した接続部と
接地間に容量を入れることによって、弾性表面波フイル
タの振動モードのSモード及びAモードの反共振点の周
波数を下げることにより、課題が解決された。なお、前
記の横結合二重モード弾性表面波フイルタの縦続接続し
た接続部と接地間に入れる容量は、前記接続部側の櫛型
電極の共通バーの外側の近傍に接地電極を配置すること
で実現している。
In order to solve the problem, by inserting a capacitance between a cascaded connection portion of a laterally coupled dual mode surface acoustic wave filter and a ground, the S mode of the vibration mode of the surface acoustic wave filter and The problem was solved by lowering the frequency of the anti-resonance point of the A mode. In addition, the capacitance to be inserted between the connection portion of the transversely coupled dual-mode surface acoustic wave filters connected in cascade and the ground is obtained by arranging the ground electrode near the outside of the common bar of the comb-shaped electrode on the connection portion side. Has been realized.

【0005】[0005]

【実施例】図1に、本発明の横結合二重モード弾性表面
波フイルタのパターン図を示す。圧電基板1の上に櫛型
電極2と反射器3からなる第一の弾性表面波素子5と、
第二の弾性表面波素子6が縦続接続されている。
FIG. 1 shows a pattern diagram of a laterally coupled dual mode surface acoustic wave filter of the present invention. A first surface acoustic wave element 5 including a comb-shaped electrode 2 and a reflector 3 on the piezoelectric substrate 1;
The second surface acoustic wave elements 6 are connected in cascade.

【0006】横結合二重モード弾性表面波フイルタの通
過帯域を、通常の手段で狭くするには、前述したように
図4に示すように櫛型電極の間隔Gを大きくして櫛型電
極2の結合を粗にして行われるが、この手段には挿入損
失が増大すると言う欠点があり、比帯域0.6×10-3
程度が限界であり、これより以上に比帯域を小さくする
には、本発明が有効である。
In order to narrow the pass band of the laterally coupled dual mode surface acoustic wave filter by a conventional means, the gap G between the comb electrodes is increased as shown in FIG. However, this method has a drawback that the insertion loss increases, and the specific bandwidth is 0.6 × 10 −3.
The degree is the limit, and the present invention is effective in further reducing the specific band.

【0007】図2に,比帯域が0.6×10-3より大き
い場合のインピーダンスと周波数の関係を示す。周波数
がSモードの共振点(Sor)<Sモードの反共振点
(Soa)<Aモードの共振点(Aor)<Aモードの
反共振点(Aoa)と並んで良好な特性である。この並
びを維持しつつフイルタの通過帯域を狭めるには、櫛型
電極の縦続接続部4と接地間に容量を入れることであ
る。この様子を図2で示すと、容量が追加されるためS
モードの反共振点(Soa)とAモードの反共振点(A
oa)の周波数が下がり、その結果Sモードの反共振点
(Soa)とAモードの反共振点(Aoa)が矢印のよ
うに左の方向に移行してフイルタの通過帯域が狭くな
る。
FIG. 2 shows the relationship between impedance and frequency when the ratio band is larger than 0.6 × 10 -3 . The frequency has good characteristics along with S-mode resonance point (Sor) <S-mode anti-resonance point (Soa) <A-mode resonance point (Aor) <A-mode anti-resonance point (Aoa). In order to narrow the pass band of the filter while maintaining this arrangement, it is necessary to insert a capacitance between the cascade connection 4 of the comb electrodes and the ground. This situation is shown in FIG. 2. Since capacity is added, S
Mode anti-resonance point (Soa) and A-mode anti-resonance point (A
The frequency of oa) decreases, and as a result, the anti-resonance point (Soa) of the S mode and the anti-resonance point (Aoa) of the A mode move to the left as indicated by the arrows, and the pass band of the filter becomes narrow.

【0008】図3に、回路図で説明する。第一の弾性表
面波素子5と、第二の弾性表面波素子6が縦続接続され
ている。この二つの素子の間の縦続接続部4には元来浮
遊容量CSが存在している。この状態は比帯域が0.6
×10-3より大きい場合である。次に本発明の縦続接続
部4と接地間に入る容量はCAで表わされる。このこと
により第一の弾性表面波素子5と、第二の弾性表面波素
子6両方の素子のSモードの反共振点(Soa)とAモ
ードの反共振点(Aoa)の周波数が下がりその結果横
結合二重モード弾性表面波フイルタの通過帯域を比帯域
0.6×10-3を越えて狭くできる。
A circuit diagram is shown in FIG. The first surface acoustic wave element 5 and the second surface acoustic wave element 6 are connected in cascade. The stray capacitance CS originally exists in the cascade connection 4 between the two elements. In this state, the bandwidth is 0.6
This is the case where it is larger than × 10 -3 . Next, the capacitance between the cascade connection 4 of the present invention and the ground is represented by CA. As a result, the frequencies of the S-mode anti-resonance point (Soa) and the A-mode anti-resonance point (Aoa) of both the first surface acoustic wave element 5 and the second surface acoustic wave element 6 are lowered. The pass band of the laterally coupled dual mode surface acoustic wave filter can be narrowed beyond the specific band of 0.6 × 10 -3 .

【0009】図1の第一の弾性表面波素子5、第二の弾
性表面波素子6の縦続接続さた部分に示すように、第一
及び第二の弾性表面波素子の櫛型電極2の縦続接続部4
に接続されている各々の櫛型電極2の共通バー7の外側
(櫛の歯が出ていない側)の近傍に、各々接地電極8を
配置して共通バー7との間で容量を構成させている。な
お容量の値は、共通バー7と接地電極8の対向する距離
と間隔に関係している。共通バー7と接地電極8の対向
する距離を長く、間隔を狭くすれば容量値は増大し、逆
に共通バー7と接地電極8の対向する距離を短く、間隔
を広くすれば容量値は減少するので、共通バー7と接地
電極8の配置によって設定できる。
As shown in FIG. 1 in which the first surface acoustic wave element 5 and the second surface acoustic wave element 6 are connected in cascade, the comb-shaped electrodes 2 of the first and second surface acoustic wave elements are formed. Cascade connection 4
The ground electrodes 8 are arranged near the outside (the side where the teeth of the comb are not projected) of the common bar 7 of each comb-shaped electrode 2 connected to each other to form a capacitance with the common bar 7. ing. The value of the capacitance is related to the distance and the distance between the common bar 7 and the ground electrode 8 facing each other. If the distance between the common bar 7 and the ground electrode 8 is long and the distance between them is narrow, the capacitance value increases. On the contrary, if the distance between the common bar 7 and the ground electrode 8 is short, and the distance is wide, the capacitance value decreases. Therefore, it can be set by the arrangement of the common bar 7 and the ground electrode 8.

【0010】[0010]

【発明の効果】本発明による第一及び第二の弾性表面波
素子の縦続接続部に接続されている櫛型電極の共通バー
と近傍に配置した接地電極で容易に希望する値の容量を
実現できるので、通過帯域が挟くて特性の良好な、挿入
損失の少ない横結合二重モード弾性表面波フイルタが容
易に製作できるようになり、生産性と信頼性が向上した
ばかりでなく、コストダウンも実現できた。
According to the present invention, the capacitance of a desired value can be easily realized by the common bar of the comb-shaped electrodes connected to the cascade connection of the first and second surface acoustic wave devices and the ground electrode arranged in the vicinity thereof. As a result, it becomes possible to easily manufacture a laterally coupled dual-mode surface acoustic wave filter with a narrow insertion band and good characteristics, and a low insertion loss, which not only improves productivity and reliability but also reduces costs. Was also realized.

【図面の簡単な説明】[Brief description of drawings]

【図1】本発明の実施例を示すパターン図である。FIG. 1 is a pattern diagram showing an embodiment of the present invention.

【図2】本発明のフイルタ素子のインピーダンスと周波
数の関係を示すグラフである。
FIG. 2 is a graph showing a relationship between impedance and frequency of the filter element of the present invention.

【図3】本発明の実施例を示す回路図である。FIG. 3 is a circuit diagram showing an embodiment of the present invention.

【図4】従来技術の挟帯域化の手法を示す図である。FIG. 4 is a diagram showing a conventional band narrowing technique.

【図5】従来技術を示すパターン図である。FIG. 5 is a pattern diagram showing a conventional technique.

【符号の説明】[Explanation of symbols]

1 圧電基板 2 櫛型電極 3 反射器 4 縦続接続部 5 第一の弾性表面波素子 6 第二の弾性表面波素子 7 共通バー 8 接地電極 DESCRIPTION OF SYMBOLS 1 Piezoelectric substrate 2 Comb type electrode 3 Reflector 4 Cascade connection section 5 First surface acoustic wave element 6 Second surface acoustic wave element 7 Common bar 8 Ground electrode

─────────────────────────────────────────────────────
─────────────────────────────────────────────────── ───

【手続補正書】[Procedure amendment]

【提出日】平成7年3月3日[Submission date] March 3, 1995

【手続補正1】[Procedure Amendment 1]

【補正対象書類名】明細書[Document name to be amended] Statement

【補正対象項目名】全文[Correction target item name] Full text

【補正方法】変更[Correction method] Change

【補正内容】[Correction content]

【書類名】 明細書[Document name] Statement

【発明の名称】 横結合二重モード弾性表面波フイルタTitle: Transversely coupled dual-mode surface acoustic wave filter

【特許請求の範囲】[Claims]

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】横結合二重モード弾性表面波フイ
ルタにおける、通過帯域の狭帯域化技術に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a technique for narrowing a pass band in a laterally coupled dual mode surface acoustic wave filter.

【0002】[0002]

【従来の技術】従来より、横結合二重モード弾性表面波
フイルタの通過帯域を狭くする方法は、図4に示すよう
に櫛型電極の間隔Gを離すことで結合を粗にして行われ
るのが一般的であった。
2. Description of the Related Art Conventionally, a method of narrowing the pass band of a laterally coupled dual-mode surface acoustic wave filter is performed by coarsely coupling the gaps G between the comb-shaped electrodes as shown in FIG. Was common.

【0003】[0003]

【発明が解決しようとする課題】従来技術では、櫛型電
極の間隔Gを離すことで櫛型電極の結合を粗にする方法
では、一般的にはフイルタの比帯域(通過帯域/中心周
波数)を0.6×10-3より狭くしようとすると、横結
合二重モード弾性表面波フイルタの挿入損失が増大する
という課題があった。比帯域とは、フイルタの通過帯域
(3dB低下の点の幅)をフイルタの中心周波数で割っ
た値を言う。
In the prior art, the method of roughening the coupling of the comb-shaped electrodes by separating the gap G between the comb-shaped electrodes is generally used in general in a specific band (passband / center frequency) of the filter. However, there is a problem in that the insertion loss of the laterally coupled dual-mode surface acoustic wave filter is increased if the value is smaller than 0.6 × 10 −3 . The ratio band is a value obtained by dividing the filter pass band (the width of the point at which the filter is lowered by 3 dB) by the center frequency of the filter.

【0004】[0004]

【課題を解決する手段】課題を解決するために、横結合
二重モード弾性表面波フイルタの縦続接続した接続部と
接地間に容量を入れることによって、弾性表面波フイル
タの振動モードのSモード及びAモードの反共振点の周
波数を下げることにより、課題が解決された。なお、前
記の横結合二重モード弾性表面波フイルタの縦続接続し
た接続部と接地間に入れる容量は、前記接続部側の櫛型
電極の共通バーの外側の近傍に接地電極を配置すること
で実現している。
In order to solve the problem, by inserting a capacitance between a cascaded connection portion of a laterally coupled dual mode surface acoustic wave filter and a ground, the S mode of the vibration mode of the surface acoustic wave filter and The problem was solved by lowering the frequency of the anti-resonance point of the A mode. In addition, the capacitance to be inserted between the connection portion of the transversely coupled dual-mode surface acoustic wave filters connected in cascade and the ground is obtained by arranging the ground electrode near the outside of the common bar of the comb-shaped electrode on the connection portion side. Has been realized.

【0005】[0005]

【実施例】図1に、本発明の横結合二重モード弾性表面
波フイルタのパターン図を示す。圧電基板1の上に櫛型
電極2と反射器3からなる第一の弾性表面波素子5と、
第二の弾性表面波素子6が縦続接続されている。
FIG. 1 shows a pattern diagram of a laterally coupled dual mode surface acoustic wave filter of the present invention. A first surface acoustic wave element 5 including a comb-shaped electrode 2 and a reflector 3 on the piezoelectric substrate 1;
The second surface acoustic wave elements 6 are connected in cascade.

【0006】横結合二重モード弾性表面波フイルタの通
過帯域を、通常の手段で狭くするには、前述したように
図4に示すように櫛型電極の間隔Gを大きくして櫛型電
極2の結合を粗にして行われるが、この手段には挿入損
失が増大すると言う欠点があり、比帯域0.6×10-3
程度が限界であり、これより以上に比帯域を小さくする
には、本発明が有効である。
In order to narrow the pass band of the laterally coupled dual mode surface acoustic wave filter by a conventional means, the gap G between the comb electrodes is increased as shown in FIG. However, this method has a drawback that the insertion loss increases, and the specific bandwidth is 0.6 × 10 −3.
The degree is the limit, and the present invention is effective in further reducing the specific band.

【0007】図2に,比帯域が0.6×10-3より大き
い場合のインピーダンスと周波数の関係を示す。周波数
がSモードの共振点(Sor)<Sモードの反共振点
(Soa)<Aモードの共振点(Aor)<Aモードの
反共振点(Aoa)と並んで良好な特性である。この並
びを維持しつつフイルタの通過帯域を狭めるには、櫛型
電極の縦続接続部4と接地間に容量を入れることであ
る。この様子を図2で示すと、容量が追加されるためS
モードの反共振点(Soa)とAモードの反共振点(A
oa)の周波数が下がり、その結果Sモードの反共振点
(Soa)とAモードの反共振点(Aoa)が矢印のよ
うに左の方向に移行してフイルタの通過帯域が狭くな
る。
FIG. 2 shows the relationship between impedance and frequency when the ratio band is larger than 0.6 × 10 -3 . The frequency has good characteristics along with S-mode resonance point (Sor) <S-mode anti-resonance point (Soa) <A-mode resonance point (Aor) <A-mode anti-resonance point (Aoa). In order to narrow the pass band of the filter while maintaining this arrangement, it is necessary to insert a capacitance between the cascade connection 4 of the comb electrodes and the ground. This situation is shown in FIG. 2. Since capacity is added, S
Mode anti-resonance point (Soa) and A-mode anti-resonance point (A
The frequency of oa) decreases, and as a result, the anti-resonance point (Soa) of the S mode and the anti-resonance point (Aoa) of the A mode move to the left as indicated by the arrows, and the pass band of the filter becomes narrow.

【0008】図3に、回路図で説明する。第一の横結合
弾性表面波素子5と、第二の横結合弾性表面波素子6が
縦続接続されている。この二つの素子の間の縦続接続部
4には元来浮遊容量CSが存在している。この状態は比
帯域が0.6×10-3より大きい場合である。次に本発
明の縦続接続部4と接地間に入る容量はCAで表わされ
る。このことにより第一の横結合弾性表面波素子5と、
第二の横結合弾性表面波素子6両方の素子のSモードの
反共振点(Soa)とAモードの反共振点(Aoa)の
周波数が下がりその結果横結合二重モード弾性表面波フ
イルタの通過帯域を比帯域0.6×10-3を越えて狭く
できる。
A circuit diagram is shown in FIG. The first laterally coupled surface acoustic wave element 5 and the second laterally coupled surface acoustic wave element 6 are connected in cascade. The stray capacitance CS originally exists in the cascade connection 4 between the two elements. This state is when the specific band is larger than 0.6 × 10 −3 . Next, the capacitance between the cascade connection 4 of the present invention and the ground is represented by CA. As a result, the first laterally coupled surface acoustic wave element 5 and
Second laterally coupled surface acoustic wave element 6 The frequencies of the anti-resonance point (Soa) of S mode and the anti-resonance point (Aoa) of A mode of both elements decrease, and as a result, the passage of the laterally coupled dual mode surface acoustic wave filter. The band can be narrowed beyond the specific band of 0.6 × 10 −3 .

【0009】図1の第一の横結合弾性表面波素子5、第
二の横結合弾性表面波素子6の縦続接続さた部分に示す
ように、第一及び第二の横結合弾性表面波素子の櫛型電
極2の縦続接続部4に接続されている各々の櫛型電極2
の共通バー7の外側(櫛の歯が出ていない側)の近傍
に、各々接地電極8を配置して共通バー7との間で容量
を構成させている。なお容量の値は、共通バー7と接地
電極8の対向する距離と間隔に関係している。共通バー
7と接地電極8の対向する距離を長く、間隔を狭くすれ
ば容量値は増大し、逆に共通バー7と接地電極8の対向
する距離を短く、間隔を広くすれば容量値は減少するの
で、共通バー7と接地電極8の配置によって設定でき
る。
As shown in the first and second transversely coupled surface acoustic wave elements 5 and 6 in FIG. 1 in which the first and second laterally coupled surface acoustic wave elements 6 are connected in cascade. Each comb-shaped electrode 2 connected to the cascade connection part 4 of the comb-shaped electrode 2 of
The ground electrodes 8 are arranged near the outside of the common bar 7 (on the side where the teeth of the comb are not exposed) to form a capacitance with the common bar 7. The value of the capacitance is related to the distance and the distance between the common bar 7 and the ground electrode 8 facing each other. If the distance between the common bar 7 and the ground electrode 8 is long and the distance between them is narrow, the capacitance value increases. On the contrary, if the distance between the common bar 7 and the ground electrode 8 is short, and the distance is wide, the capacitance value decreases. Therefore, it can be set by the arrangement of the common bar 7 and the ground electrode 8.

【0010】[0010]

【発明の効果】本発明による第一及び第二の横結合弾性
表面波素子の縦続接続部に接続されている櫛型電極の共
通バーと近傍に配置した接地電極で容易に希望する値の
容量を実現できるので、通過帯域が挟くて特性の良好
な、挿入損失の少ない横結合二重モード弾性表面波フイ
ルタが容易に製作できるようになり、生産性と信頼性が
向上したばかりでなく、コストダウンも実現できた。
According to the present invention, the common bar of the comb-shaped electrodes connected to the cascade connection of the first and second laterally coupled surface acoustic wave devices and the ground electrode arranged in the vicinity thereof make it easy to obtain a desired capacitance. Since it is possible to realize, it becomes possible to easily manufacture a laterally coupled dual-mode surface acoustic wave filter with good characteristics by narrowing the pass band, and with low insertion loss, which not only improves productivity and reliability, but also We were able to reduce costs.

【図面の簡単な説明】[Brief description of drawings]

【図1】本発明の実施例を示すパターン図である。FIG. 1 is a pattern diagram showing an embodiment of the present invention.

【図2】本発明のフイルタ素子のインピーダンスと周波
数の関係を示すグラフである。
FIG. 2 is a graph showing a relationship between impedance and frequency of the filter element of the present invention.

【図3】本発明の実施例を示す回路図である。FIG. 3 is a circuit diagram showing an embodiment of the present invention.

【図4】従来技術の挟帯域化の手法を示す図である。FIG. 4 is a diagram showing a conventional band narrowing technique.

【図5】従来技術を示すパターン図である。FIG. 5 is a pattern diagram showing a conventional technique.

【符号の説明】 1 圧電基板 2 櫛型電極 3 反射器 4 縦続接続部 5 第一の横結合弾性表面波素子 6 第二の横結合弾性表面波素子 7 共通バー 8 接地電極[Explanation of reference numerals] 1 piezoelectric substrate 2 comb-shaped electrode 3 reflector 4 cascade connection part 5 first laterally coupled surface acoustic wave element 6 second laterally coupled surface acoustic wave element 7 common bar 8 ground electrode

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】 圧電基板上に櫛型電極と反射器からなる
第一の弾性表面波素子と第二の弾性表面波素子を縦続接
続した横結合二重モード弾性表面波フイルタにおいて、 該横結合二重モード弾性表面波フイルタの通過帯域幅を
狭くする手段として、該第一の弾性表面波素子と該第二
の弾性表面波素子の縦続接続部と接地間に容量を設けた
ことを特徴とする横結合二重モード弾性表面波フイル
タ。
1. A laterally coupled dual-mode surface acoustic wave filter in which a first surface acoustic wave element and a second surface acoustic wave element each comprising a comb-shaped electrode and a reflector are cascade-connected on a piezoelectric substrate. As means for narrowing the pass band width of the dual mode surface acoustic wave filter, a capacitance is provided between the cascade connection of the first surface acoustic wave element and the second surface acoustic wave element and the ground. Horizontally coupled dual-mode surface acoustic wave filter.
【請求項2】 該第一及び第二の弾性表面波素子の櫛型
電極の該縦続接続部に接続された側の各々の櫛型電極の
共通バーの外側に各々接地電極を配置することを特徴と
する特許請求の範囲第1項記載の横結合二重モード弾性
表面波フイルタ。
2. A ground electrode is arranged outside a common bar of each comb-shaped electrode on the side connected to the cascade connection of the comb-shaped electrodes of the first and second surface acoustic wave devices. A transversely coupled dual-mode surface acoustic wave filter according to claim 1.
JP6494995A 1995-02-28 1995-02-28 Transversely coupled dual-mode surface acoustic wave filter Pending JPH08237064A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6494995A JPH08237064A (en) 1995-02-28 1995-02-28 Transversely coupled dual-mode surface acoustic wave filter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6494995A JPH08237064A (en) 1995-02-28 1995-02-28 Transversely coupled dual-mode surface acoustic wave filter

Publications (1)

Publication Number Publication Date
JPH08237064A true JPH08237064A (en) 1996-09-13

Family

ID=13272804

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6494995A Pending JPH08237064A (en) 1995-02-28 1995-02-28 Transversely coupled dual-mode surface acoustic wave filter

Country Status (1)

Country Link
JP (1) JPH08237064A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0899874A3 (en) * 1997-08-29 1999-12-29 Fujitsu Limited Surface acoustic wave filter of multistage connection type
US6177752B1 (en) 1998-12-25 2001-01-23 Nec Corporation Surface acoustic wave device and method of connecting surface acoustic wave filters

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0899874A3 (en) * 1997-08-29 1999-12-29 Fujitsu Limited Surface acoustic wave filter of multistage connection type
US6177752B1 (en) 1998-12-25 2001-01-23 Nec Corporation Surface acoustic wave device and method of connecting surface acoustic wave filters

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