JPH11136086A - Electrode structure of serial arm resonator of acoustic wave filter for very high frequency - Google Patents

Electrode structure of serial arm resonator of acoustic wave filter for very high frequency

Info

Publication number
JPH11136086A
JPH11136086A JP29833097A JP29833097A JPH11136086A JP H11136086 A JPH11136086 A JP H11136086A JP 29833097 A JP29833097 A JP 29833097A JP 29833097 A JP29833097 A JP 29833097A JP H11136086 A JPH11136086 A JP H11136086A
Authority
JP
Japan
Prior art keywords
electrode
acoustic wave
comb
surface acoustic
wave filter
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.)
Granted
Application number
JP29833097A
Other languages
Japanese (ja)
Other versions
JP3378182B2 (en
Inventor
Kazushige Noguchi
和繁 野口
Toshio Tagami
俊男 田上
Hajime Shimamura
一 島村
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.)
Oki Electric Industry Co Ltd
Original Assignee
Oki Electric Industry Co Ltd
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 Oki Electric Industry Co Ltd filed Critical Oki Electric Industry Co Ltd
Priority to JP29833097A priority Critical patent/JP3378182B2/en
Publication of JPH11136086A publication Critical patent/JPH11136086A/en
Application granted granted Critical
Publication of JP3378182B2 publication Critical patent/JP3378182B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Abstract

PROBLEM TO BE SOLVED: To improve a frequency characteristic and also to prevent electrostatic destruction by adjusting an interval in a boundary part of a grating reflector (ground) and a comb-shaped electrode. SOLUTION: An electrode structure of a serial arm resonator of an acoustic wave filter of a ladder circuit configuration which has a dual mode resonance characteristic is provided with a comb-shaped electrode 7 which is formed on a piezo-electric substrate 1 and also is formed by interlocking an interdigital electrode 8 that is connected to an input terminal with an interdigital electrode 9 that is connected to an output terminal and grating reflectors 10 which are arranged at both sides of the electrode 7. The intervals of the outermost electrode fingers of the electrode 7 and the electrode fingers of the reflectors 10 which face the electrode fingers are adjusted.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は、移動体通信用機
器、特に超高周波用携帯電話器に用いられる段間用弾性
表面波フィルタの直列腕共振器の電極構造に関するもの
である。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an electrode structure of a series arm resonator of a surface acoustic wave filter for interstages used in mobile communication equipment, particularly, a super-high frequency portable telephone.

【0002】[0002]

【従来の技術】従来、このような分野の技術としては、
例えば、(1)「共振器型SAWフィルタ」沖研究開発
173 Vol.64,No.1 第79〜84頁、
(2)特開平9−167937号公報等に開示されるも
のがあった。例えば、我が国のNTT方式の自動車電話
および携帯電話の移動通信端末の送信周波数の帯域幅
は、932.5MHzを中心に±7.5MHzであり、
受信周波数の帯域幅は、877.5MHzを中心に±
7.5MHzである。弾性表面波フィルタはこのような
仕様を満たす必要がある。
2. Description of the Related Art Conventionally, techniques in such a field include:
For example, (1) “Resonator type SAW filter” Oki R & D 173 Vol. 64, no. 1 pp. 79-84,
(2) There is one disclosed in JP-A-9-167937. For example, the transmission frequency bandwidth of a mobile communication terminal of a Japanese NTT car and a mobile phone is ± 7.5 MHz centered on 932.5 MHz,
The bandwidth of the reception frequency is centered around 877.5 MHz ±
7.5 MHz. The surface acoustic wave filter needs to satisfy such specifications.

【0003】このような弾性表面波フィルタは、弾性表
面波素子を共振器とし、これを梯子型に接続した共振子
型のフィルタとして構成されている。図4はかかる従来
の超高周波用弾性表面波フィルタの回路図、図5は従来
の弾性表面波共振器の電極構造を示す図である。まず、
超高周波用弾性表面波フィルタの回路図について説明す
る。
[0003] Such a surface acoustic wave filter is configured as a resonator type filter in which a surface acoustic wave element is used as a resonator and connected to a ladder type. FIG. 4 is a circuit diagram of such a conventional surface acoustic wave filter for ultrahigh frequency, and FIG. 5 is a diagram showing an electrode structure of a conventional surface acoustic wave resonator. First,
A circuit diagram of the surface acoustic wave filter for ultrahigh frequency will be described.

【0004】図4に示すように、共振子型のフィルタ1
00は、例えば、第1の弾性表面波共振器110と第2
の弾性表面波共振器120とからなる多段構成のフィル
タである。第1の弾性表面波共振器110は並列腕11
2に、第2の弾性表面波共振器120は直列腕122に
接続されている。これらの弾性表面波共振器110およ
び120は、図5に示すような、入力すだれ状電極13
1と出力すだれ状電極132からなる櫛形電極130か
ら構成されている。この図において、133は接地され
るグレーティング反射器、x1 は正規に形成された櫛形
電極の最も外側の電極指とこの電極指に面した前記グレ
ーティング反射器の電極指との間隔、λは櫛形電極周期
である。
[0004] As shown in FIG.
00 is, for example, the first surface acoustic wave resonator 110 and the second surface acoustic wave resonator 110.
And a surface acoustic wave resonator 120 of the present embodiment. The first surface acoustic wave resonator 110 has a parallel arm 11
Second, the second surface acoustic wave resonator 120 is connected to the series arm 122. These surface acoustic wave resonators 110 and 120 are connected to the input IDT 13 as shown in FIG.
1 and a comb-shaped electrode 130 composed of an output interdigital electrode 132. In this figure, 133 grating reflector is grounded, x 1 is the interval between the grating reflector electrode fingers facing the electrode finger and the outermost electrode fingers of the comb-shaped electrodes formed on a regular, lambda is comb This is the electrode cycle.

【0005】また、この櫛形電極130はその抵抗分を
無視すると、図6に示すような等価回路140で示され
る。ここで、Cdは櫛形電極の静電容量、C1 ,L1
等価定数であり、この等価回路140を図7のように示
す。また、図8(a)及び図8(b)には、櫛形電極1
30を等価回路140で示したときのインピーダンス
(x)およびアドミタンス(B)の周波数特性が示され
ている。
The comb electrode 130 is represented by an equivalent circuit 140 as shown in FIG. 6 ignoring its resistance. Here, Cd is the capacitance of the comb-shaped electrode, C 1 and L 1 are equivalent constants, and this equivalent circuit 140 is shown in FIG. FIGS. 8A and 8B show the comb-shaped electrode 1.
The frequency characteristics of impedance (x) and admittance (B) when 30 is represented by an equivalent circuit 140 are shown.

【0006】これらの図からわかるように、2つの共振
周波数fg,fhを持つ2重共振特性となる。ここで、
fgを共振周波数と呼び、fhを反共振周波数と呼ぶ。
このような2重共振特性を持つ共振器をそれぞれ直列腕
および並列腕に配置し、さらに並列腕の反共振周波数f
hpを直列腕のfgsと略一致させると、これらの周波
数を中心周波数とするバンドパスフィルタの特性を示す
回路ができる。
As can be seen from these figures, a double resonance characteristic having two resonance frequencies fg and fh is obtained. here,
fg is called a resonance frequency, and fh is called an anti-resonance frequency.
Resonators having such double resonance characteristics are arranged in the series arm and the parallel arm, respectively, and the anti-resonance frequency f
When hp is substantially equal to fgs of the serial arm, a circuit showing the characteristics of the band-pass filter having these frequencies as center frequencies is obtained.

【0007】その理由について説明すると、図9(a)
のイミタンスの周波数特性に示すように、fhp≒fg
sである中心周波数の付近では通過域となり、中心周波
数から離れた領域では減衰域となるからである。したが
って、図4に示す構成の共振子型のフィルタ100は、
図9(b)に示す周波数特性となる。
The reason will be described below.
As shown in the frequency characteristic of the immittance of fhp ≒ fg
This is because a pass band is formed near the center frequency s, and an attenuation band is formed in a region far from the center frequency. Therefore, the resonator type filter 100 having the configuration shown in FIG.
The frequency characteristic is as shown in FIG.

【0008】[0008]

【発明が解決しようとする課題】しかしながら、特に、
超高周波(1.9GHz)用のフィルタになると、第2
高調波に対する対策が必要になる。また、上記した従来
の2重モード共振特性を有する梯子型回路構成の弾性表
面波共振器は、回路の入出力端子及び、接地するための
ワイヤボンディングを行うパターンが、超高周波(1.
9GHz)用のフィルタであるため、極めて細い電極指
に比べて十分大きく、組み立て工程でのダイスボンディ
ング後の硬化及びワイヤボンディング時のチップに加え
る熱履歴により、ワイヤボンディング用のパターンに帯
電された静電気が、図5に示す接地されたグレーティン
グ反射器133と櫛形電極130の境界部分(x1
分)において、静電破壊を引き起こすという問題があっ
た。
However, in particular,
When it comes to a filter for ultra-high frequency (1.9 GHz),
It is necessary to take measures against harmonics. Further, in the above-described conventional surface acoustic wave resonator having a ladder-type circuit configuration having a dual mode resonance characteristic, the input / output terminals of the circuit and the pattern for performing wire bonding for grounding have an extremely high frequency (1.
9 GHz), it is sufficiently large compared to extremely thin electrode fingers, and is charged in the wire bonding pattern by curing after die bonding in the assembly process and heat history applied to the chip during wire bonding. but there is a problem that at the boundary of the grating reflector 133 and comb electrodes 130 which is grounded is shown in FIG. 5 (x 1 portion) and cause electrostatic breakdown.

【0009】本発明は、上記問題点を除去し、グレーテ
ィング反射器(接地)と櫛形電極の境界部分における間
隔を調整することにより、周波数特性の向上を図ること
ができる超高周波用弾性表面波フィルタの直列腕共振器
の電極構造を提供することを目的とする。
The present invention eliminates the above problems and adjusts the spacing at the boundary between the grating reflector (ground) and the comb-shaped electrode, thereby improving the frequency characteristics. It is an object of the present invention to provide an electrode structure of the series arm resonator.

【0010】[0010]

【課題を解決するための手段】本発明は、上記目的を達
成するために、〔1〕2重モード共振特性を有する梯子
型回路構成の弾性表面波フィルタの直列腕共振器の電極
構造において、圧電体基板上に形成されるとともに、入
力端子に接続されるすだれ状電極と出力端子に接続され
るすだれ状電極とを噛み合わせてなる櫛形電極と、この
櫛形電極の両側に配置されるグレーティング反射器と、
前記櫛形電極の最も外側の電極指と、この電極指に面し
た前記グレーティング反射器の電極指との間隔を調整す
る手段とを具備するようにしたものである。
According to the present invention, there is provided an electrode structure of a series arm resonator of a surface acoustic wave filter having a ladder type circuit configuration having dual mode resonance characteristics. Comb-shaped electrodes formed on the piezoelectric substrate and interdigitated with interdigital electrodes connected to the input terminals and output terminals, and grating reflections arranged on both sides of the interdigital electrodes Vessels,
The apparatus includes a means for adjusting a distance between an outermost electrode finger of the comb-shaped electrode and an electrode finger of the grating reflector facing the electrode finger.

【0011】〔2〕上記〔1〕記載の超高周波用弾性表
面波フィルタの直列腕共振器の電極構造において、正規
に配置されるべき前記グレーティング反射器の前記櫛形
電極の最も外側の電極指に面した電極指をなくし、前記
櫛形型電極の最も外側の電極指と、この電極指に面した
前記グレーティング反射器の電極指との間隔を広げるよ
うにしたものである。
[2] In the electrode structure of the series arm resonator of the surface acoustic wave filter for ultra-high frequency waves described in [1], the outermost electrode finger of the comb-shaped electrode of the grating reflector to be properly arranged. The electrode fingers facing away are eliminated, and the distance between the outermost electrode finger of the comb-shaped electrode and the electrode finger of the grating reflector facing this electrode finger is increased.

【0012】〔3〕上記〔2〕記載の超高周波用弾性表
面波フィルタの直列腕共振器の電極構造において、前記
広げられた間隔が3×s/4μm(ただし、sは縮小
率)となるようにしたものである。
[3] In the electrode structure of the series arm resonator of the surface acoustic wave filter for ultrahigh frequency waves described in [2], the widened interval is 3 × s / 4 μm (where s is a reduction ratio). It is like that.

【0013】[0013]

【発明の実施の形態】以下、本発明の実施の形態につい
て詳細に説明する。図1は本発明に係る超高周波用弾性
表面波フィルタの回路図、図2は本発明の第1実施例を
示す静電破壊対策を行った超高周波用弾性表面波フィル
タの直列腕共振器の電極構造を示す図である。
Embodiments of the present invention will be described below in detail. FIG. 1 is a circuit diagram of an ultra-high frequency surface acoustic wave filter according to the present invention, and FIG. 2 is a circuit diagram of a series arm resonator of an ultra-high frequency surface acoustic wave filter according to a first embodiment of the present invention, which has taken measures against electrostatic breakdown. It is a figure showing an electrode structure.

【0014】図1において、共振子型のフィルタ2は、
例えば、第1の弾性表面波共振器3と第2の弾性表面波
共振器4とからなる多段構成のフィルタである。第1の
弾性表面波共振器3は並列腕5に、第2の弾性表面波共
振器4は直列腕6に接続されている。その直列腕6に接
続される第2の弾性表面波共振器4は、図2に示すよう
に、圧電体基板1上に形成される入力すだれ状電極8と
出力すだれ状電極9からなる櫛形電極7から構成されて
いる。この櫛形電極7の両側には接地されるグレーティ
ング反射器10が配置されている。この図において、x
は櫛形電極7の最も外側の電極指と、この電極指に面し
た前記グレーティング反射器10の電極指との間隔、λ
は櫛形電極周期である。
In FIG. 1, a resonator type filter 2 comprises:
For example, the filter is a multi-stage filter including the first surface acoustic wave resonator 3 and the second surface acoustic wave resonator 4. The first surface acoustic wave resonator 3 is connected to the parallel arm 5 and the second surface acoustic wave resonator 4 is connected to the series arm 6. As shown in FIG. 2, a second surface acoustic wave resonator 4 connected to the series arm 6 is a comb-shaped electrode composed of an input interdigital electrode 8 and an output interdigital electrode 9 formed on the piezoelectric substrate 1. 7. Grating reflectors 10 that are grounded are arranged on both sides of the comb-shaped electrode 7. In this figure, x
Is the distance between the outermost electrode finger of the comb-shaped electrode 7 and the electrode finger of the grating reflector 10 facing this electrode finger;
Is the comb electrode period.

【0015】また、図1には、弾性表面波共振器を直列
腕IDTS1…Sn及び並列腕IDTP1…IDTPn
に配置した二重モード共振特性を有する梯子型回路構成
の弾性表面波フィルタを示しており、図2に示した超高
周波用弾性表面波フィルタの電極構造は、直列腕IDT
S1…Snに用いられる。この実施例では、グレーティ
ング反射器(接地)10と櫛形電極7の境界部分の距
離、つまり、櫛形電極7の最も外側の電極指と、この電
極指に面した前記グレーティング反射器10の電極指と
の間隔xを、従来例で示した正規の間隔x1を調整する
ことにより、周波数特性の向上を図ることができる。
FIG. 1 shows that a surface acoustic wave resonator is composed of serial arms IDTS1... Sn and parallel arms IDTP1.
FIG. 2 shows a surface acoustic wave filter having a ladder-type circuit configuration having a dual mode resonance characteristic, and the electrode structure of the surface acoustic wave filter for ultra-high frequency shown in FIG.
Used for S1... Sn. In this embodiment, the distance between the boundary between the grating reflector (ground) 10 and the comb-shaped electrode 7, that is, the outermost electrode finger of the comb-shaped electrode 7, and the electrode finger of the grating reflector 10 facing this electrode finger the distance x, by adjusting the distance x 1 regular shown in the conventional example, it is possible to improve the frequency characteristics.

【0016】図3は本発明のグレーティング反射器(接
地)と櫛形電極の境界部分の距離xの調整と周波数特性
を示す図である。この図において、縦軸は減衰量、横軸
は周波数(f)を示している。この図から明らかなよう
に、グレーティング反射器(接地)と櫛形電極の境界部
分の距離xが基準となる曲線(実線)に比べて大きくな
ると周波数の共振点が下がり、a曲線(点線)のように
なり、その距離xが基準となる曲線(実線)に比べて小
さくなると周波数の共振点が上がり、b曲線(一点線)
のように調整することができる。
FIG. 3 is a diagram showing the adjustment of the distance x between the grating reflector (ground) and the comb-shaped electrode of the present invention and the frequency characteristics. In this figure, the vertical axis shows the attenuation, and the horizontal axis shows the frequency (f). As is clear from this figure, when the distance x between the boundary between the grating reflector (ground) and the comb-shaped electrode becomes larger than the reference curve (solid line), the resonance point of the frequency decreases, and as shown by the curve a (dotted line). When the distance x becomes smaller than the reference curve (solid line), the resonance point of the frequency increases, and the curve b (dotted line)
It can be adjusted as follows.

【0017】また、櫛形電極と反射器の間隔を両方もし
くは片方変えることにより、反射器により反射されたエ
ネルギーの位相が、櫛形電極により励振されたエネルギ
ーの位相と異なった位相となり、それぞれの異なった位
相の合成により、電極の周波数特性を変動させることが
できる。このように、第1実施例によれば、櫛形電極と
反射器の間隔を任意に変えることにより、周波数特性を
変動させることができる。
Further, by changing both or one of the intervals between the comb-shaped electrode and the reflector, the phase of the energy reflected by the reflector becomes different from the phase of the energy excited by the comb-shaped electrode. By combining the phases, the frequency characteristics of the electrodes can be varied. As described above, according to the first embodiment, the frequency characteristic can be changed by arbitrarily changing the interval between the comb-shaped electrode and the reflector.

【0018】次に、本発明の第2実施例について説明す
る。図2に戻って、この実施例は、接地されたグレーテ
ィング反射器10と櫛形電極7の境界部分の距離xを調
整するが、その場合、従来例で示した、櫛形電極130
の最も外側の電極指と、この電極指に面した前記グレー
ティング反射器133の電極指との間隔x1 を広げるも
のであるが、その場合、従来例で示した、グレーティン
グ反射器133の櫛形電極130と面した電極指1本を
なくして、間隔を広げるようにしている。
Next, a second embodiment of the present invention will be described. Returning to FIG. 2, in this embodiment, the distance x between the grounded grating reflector 10 and the boundary between the comb-shaped electrode 7 is adjusted. In this case, the comb-shaped electrode 130 shown in the conventional example is adjusted.
The outermost electrode fingers, but is intended to widen the distance x 1 between the electrode fingers of the grating reflector 133 facing to the electrode fingers, in which case, as shown in the conventional example, the comb-shaped electrodes of the grating reflector 133 One electrode finger facing 130 is eliminated to increase the interval.

【0019】図5に示す従来の櫛形電極において、櫛形
電極周期をλ、帯域周波数の中心をf、音速をvとする
と、v=fλであり、λ=v/fであり、λは約3μm
である。また、x1 =λs/4〔ここで、sは縮小率
(約0.65)〕であるから、x1 は約0.5μmであ
る。つまり、1.9GHzの超高周波用弾性表面波フィ
ルタの直列腕共振器の場合、距離(間隔)x1 は0.5
μmである。
In the conventional comb-shaped electrode shown in FIG. 5, if the period of the comb-shaped electrode is λ, the center of the band frequency is f, and the sound speed is v, v = fλ, λ = v / f, and λ is about 3 μm
It is. Further, since x 1 = λs / 4 [where s is the reduction ratio (about 0.65)], x 1 is about 0.5 μm. That is, in the case of series arm resonators of the super high frequency surface acoustic wave filter of 1.9 GHz, the distance (interval) x 1 0.5
μm.

【0020】本発明の第2実施例では、図2に示すよう
に、その距離(間隔)x1 は0.5μmであったものを
グレーティング反射器10の櫛形電極7と面した電極指
1本をなくす、つまり、距離(間隔)xは3×x1
1.5μmとなるように広げるようにする。したがっ
て、図3において、共振点を下げるように調整するとと
もに、接地されたグレーティング反射器と櫛形電極の境
界部分xにおける静電破壊を防止することができる。
In the second embodiment of the present invention, as shown in FIG. 2, the distance (interval) x 1 is 0.5 μm, but one electrode finger facing the comb-shaped electrode 7 of the grating reflector 10 is used. , Ie, the distance (interval) x is 3 × x 1 =
Spread to 1.5 μm. Therefore, in FIG. 3, the resonance point can be adjusted so as to be lowered, and the electrostatic breakdown at the boundary x between the grounded grating reflector and the comb-shaped electrode can be prevented.

【0021】この製品の製造工程は、ホトリソグラフィ
によるウエハプロセスの工程を数回行い、ダイシングを
行ったチップを、パッケージ内にペーストを用いてダイ
スボンディングする。このチップを固定するには、ペー
ストを硬化させるため、ある程度の熱を加え、その後、
ワイヤボンディングを行うため、再びある程度の熱を加
える。
In the manufacturing process of this product, a wafer process by photolithography is performed several times, and the diced chips are die-bonded in a package using a paste. To fix the chip, apply some heat to harden the paste,
To perform wire bonding, some heat is applied again.

【0022】通常、前述のように製造工程では2度の熱
による負荷をチップに与えるのであるが、本発明が使用
されている製品は、超高周波弾性表面波受信フィルタで
あるため、設計上、電極の交差長が非常に短く、かつ、
超高周波(1.9GHz)用であるために、パターン幅
も非常に細い(0.5μm程度)構成となっているの
で、多少の静電気にも非常に破壊され易い電極構造とな
っている。因みに、例えば、入力すだれ状電極の電極指
の数は90本、出力すだれ状電極の電極指の数は91
本、グレーティング反射器の電極指の数は100本であ
る。
Normally, a load due to heat is applied to the chip twice in the manufacturing process as described above. However, the product to which the present invention is applied is an ultra-high frequency surface acoustic wave receiving filter. The electrode intersection length is very short, and
Since it is for ultrahigh frequency (1.9 GHz), the pattern width is very narrow (about 0.5 μm), so that the electrode structure is very easily destroyed even by some static electricity. Incidentally, for example, the number of electrode fingers of the input interdigital transducer is 90, and the number of electrode fingers of the output interdigital transducer is 91.
The number of electrode fingers of this and the grating reflector is 100.

【0023】そこで、交差長の短い電極に対して、図2
に示すように、接地されたグレーティング反射器と櫛形
電極の境界部分を、図5に示す従来のグレーティング反
射器の電極指を1本減らして、帯電された電荷による放
電の電位差に耐えられるように、接地部分と櫛形電極の
電極指の間隔を十分に空けるという電極構造にする。勿
論、櫛形電極の反対側に面したグレーティング反射器に
も同様な構成を施す。
Therefore, for an electrode having a short intersection length, FIG.
As shown in FIG. 5, the boundary between the grounded grating reflector and the comb-shaped electrode is reduced by one electrode finger of the conventional grating reflector shown in FIG. 5 so that it can withstand the potential difference of the discharge due to the charged electric charge. The electrode structure is such that the space between the ground portion and the electrode fingers of the comb-shaped electrode is sufficiently spaced. Of course, a similar configuration is applied to the grating reflector facing the opposite side of the comb-shaped electrode.

【0024】ここで、櫛形電極の両側のグレーティング
反射器の電極指を1本ずつ減らすことにより、1/2波
長の周期で配列された規則性が失われ、元のパターンに
より減衰極の周波数が多少変動するが、これに関しては
その電極のみのパターン幅(波長)を変えて補正を行
う。このように、第2実施例によれば、パターン幅0.
5μm程度の電極指が、プロセス時、及び組み立て時の
加熱で帯電された電荷による放電の電位差に耐えられる
ようになり、静電破壊を回避することができる。
Here, by reducing the number of electrode fingers of the grating reflector on both sides of the comb-shaped electrode one by one, regularity arranged at a period of 1/2 wavelength is lost, and the frequency of the attenuation pole is reduced by the original pattern. Although it fluctuates slightly, correction is performed by changing the pattern width (wavelength) of only the electrode. As described above, according to the second embodiment, the pattern width is 0.1 mm.
The electrode finger of about 5 μm can withstand the potential difference of the discharge due to the electric charge charged by the heating during the process and the assembling, and the electrostatic breakdown can be avoided.

【0025】なお、本発明は上記実施例に限定されるも
のではなく、本発明の趣旨に基づいて種々の変形が可能
であり、これらを本発明の範囲から排除するものではな
い。
It should be noted that the present invention is not limited to the above-described embodiment, and various modifications are possible based on the spirit of the present invention, and these are not excluded from the scope of the present invention.

【0026】[0026]

【発明の効果】以上、詳細に説明したように、本発明に
よれば、次のような効果を奏することができる。 (1)請求項1記載の発明によれば、接地されたグレー
ティング反射器と櫛形電極の境界部分の距離、つまり、
櫛形電極の最も外側の電極指と、この電極指に面した前
記グレーティング反射器の電極指との間隔xを、従来例
で示した正規の間隔x1 を調整することにより、周波数
特性を向上させることができる。
As described above, according to the present invention, the following effects can be obtained. (1) According to the first aspect of the invention, the distance between the grounded grating reflector and the boundary between the comb-shaped electrode, that is,
The most and outer electrode fingers of the interdigital electrodes, the distance x between the electrode fingers of the grating reflector facing the electrode fingers, by adjusting the distance x 1 regular shown in the conventional example, to improve the frequency characteristic be able to.

【0027】(2)請求項2記載の発明によれば、櫛形
電極の最も外側の電極指と、この電極指に面した前記グ
レーティング反射器の電極指との間隔xを広げるように
したので、周波数の共振点を下げるとともに、静電破壊
を防止することができる。 (3)請求項3記載の発明によれば、従来の超高周波用
弾性表面波フィルタの直列腕共振器の電極の一部を除去
することにより、簡単に周波数の共振点を下げるととも
に、静電破壊を防止することができる。
(2) According to the second aspect of the invention, the distance x between the outermost electrode finger of the comb-shaped electrode and the electrode finger of the grating reflector facing this electrode finger is increased. The frequency resonance point can be lowered, and electrostatic breakdown can be prevented. (3) According to the third aspect of the invention, by removing a part of the electrode of the series arm resonator of the conventional surface acoustic wave filter for ultrahigh frequency, the resonance point of the frequency can be easily lowered and the electrostatic force can be reduced. Destruction can be prevented.

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

【図1】本発明に係る超高周波用弾性表面波フィルタの
回路図である。
FIG. 1 is a circuit diagram of an ultra-high frequency surface acoustic wave filter according to the present invention.

【図2】本発明の実施例を示す静電破壊対策を行った超
高周波用弾性表面波フィルタの直列腕共振器の電極構造
を示す図である。
FIG. 2 is a view showing an electrode structure of a series arm resonator of a surface acoustic wave filter for ultra-high frequency in which a countermeasure against electrostatic destruction according to an embodiment of the present invention is taken.

【図3】本発明のグレーティング反射器(接地)と櫛形
電極の境界部分の距離xの調整と周波数特性を示す図で
ある。
FIG. 3 is a diagram illustrating adjustment of a distance x between a grating reflector (ground) and a comb-shaped electrode and frequency characteristics according to the present invention.

【図4】従来の超高周波用弾性表面波フィルタの回路図
である。
FIG. 4 is a circuit diagram of a conventional ultra-high frequency surface acoustic wave filter.

【図5】従来の弾性表面波共振器の電極構造を示す図で
ある。
FIG. 5 is a diagram showing an electrode structure of a conventional surface acoustic wave resonator.

【図6】従来の弾性表面波共振器の等価回路図である。FIG. 6 is an equivalent circuit diagram of a conventional surface acoustic wave resonator.

【図7】従来の弾性表面波共振器の記号を示す図であ
る。
FIG. 7 is a diagram showing symbols of a conventional surface acoustic wave resonator.

【図8】従来の共振器のインピーダンスおよびアドミタ
ンスを示す図である。
FIG. 8 is a diagram showing impedance and admittance of a conventional resonator.

【図9】従来のフィルタのイミタンスおよび通過特性図
である。
FIG. 9 is a diagram showing immittance and pass characteristics of a conventional filter.

【符号の説明】[Explanation of symbols]

1 圧電体基板 2 共振子型のフィルタ 3 第1の弾性表面波共振器 4 第2の弾性表面波共振器 5 並列腕 6 直列腕 7 櫛形電極 8 入力すだれ状電極 9 出力すだれ状電極 10 グレーティング反射器 DESCRIPTION OF SYMBOLS 1 Piezoelectric substrate 2 Resonator type filter 3 First surface acoustic wave resonator 4 Second surface acoustic wave resonator 5 Parallel arm 6 Series arm 7 Comb electrode 8 Input interdigital electrode 9 Output interdigital electrode 10 Grating reflection vessel

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 2重モード共振特性を有する梯子型回路
構成の弾性表面波フィルタの直列腕共振器の電極構造に
おいて、(a)圧電体基板上に形成されるとともに、入
力端子に接続されるすだれ状電極と出力端子に接続され
るすだれ状電極とを噛み合わせてなる櫛形電極と、
(b)該櫛形電極の両側に配置されるグレーティング反
射器と、(c)前記櫛形電極の最も外側の電極指と、該
電極指に面した前記グレーティング反射器の電極指との
間隔を調整する手段とを具備することを特徴とする超高
周波用弾性表面波フィルタの直列腕共振器の電極構造。
1. An electrode structure of a series arm resonator of a surface acoustic wave filter having a ladder type circuit configuration having a dual mode resonance characteristic, wherein (a) the electrode structure is formed on a piezoelectric substrate and connected to an input terminal. A comb-shaped electrode formed by meshing the IDT and the IDT connected to the output terminal;
(B) adjusting the distance between the grating reflectors arranged on both sides of the comb-shaped electrode, and (c) adjusting the distance between the outermost electrode finger of the comb-shaped electrode and the electrode finger of the grating reflector facing the electrode finger. And an electrode structure of a series arm resonator of the surface acoustic wave filter for ultrahigh frequency.
【請求項2】 請求項1記載の超高周波用弾性表面波フ
ィルタの直列腕共振器の電極構造において、正規に配置
されるべき前記グレーティング反射器の前記櫛形電極の
最も外側の電極指に面した電極指をなくし、前記櫛形電
極の最も外側の電極指と、該電極指に面した前記グレー
ティング反射器の電極指との間隔を広げてなることを特
徴とする超高周波用弾性表面波フィルタの直列腕共振器
の電極構造。
2. The electrode structure of a series arm resonator of a surface acoustic wave filter for ultra-high frequency waves according to claim 1, wherein said grating reflector faces the outermost electrode finger of said comb-shaped electrode to be properly arranged. A series of super-high-frequency surface acoustic wave filters, characterized in that the electrode fingers are eliminated and the outermost electrode fingers of the comb-shaped electrode and the electrode fingers of the grating reflector facing the electrode fingers are widened. Electrode structure of arm resonator.
【請求項3】 請求項2記載の超高周波用弾性表面波フ
ィルタの直列腕共振器の電極構造において、前記広げら
れた間隔が3×s/4μm(ただし、sは縮小率)とな
るようにしたことを特徴とする超高周波用弾性表面波フ
ィルタの直列腕共振器の電極構造。
3. The electrode structure of a series arm resonator of a surface acoustic wave filter for ultra-high frequency waves according to claim 2, wherein the widened interval is 3 × s / 4 μm (where s is a reduction ratio). An electrode structure of a series arm resonator of a surface acoustic wave filter for ultra-high frequency, characterized in that:
JP29833097A 1997-10-30 1997-10-30 Electrode structure of series arm resonator of surface acoustic wave filter for ultra-high frequency Expired - Fee Related JP3378182B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP29833097A JP3378182B2 (en) 1997-10-30 1997-10-30 Electrode structure of series arm resonator of surface acoustic wave filter for ultra-high frequency

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP29833097A JP3378182B2 (en) 1997-10-30 1997-10-30 Electrode structure of series arm resonator of surface acoustic wave filter for ultra-high frequency

Publications (2)

Publication Number Publication Date
JPH11136086A true JPH11136086A (en) 1999-05-21
JP3378182B2 JP3378182B2 (en) 2003-02-17

Family

ID=17858274

Family Applications (1)

Application Number Title Priority Date Filing Date
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Country Status (1)

Country Link
JP (1) JP3378182B2 (en)

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JP2020028101A (en) * 2018-08-18 2020-02-20 京セラ株式会社 Acoustic wave filter

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2014196245A1 (en) * 2013-06-04 2014-12-11 京セラ株式会社 Branching filter and communication module
CN105191125A (en) * 2013-06-04 2015-12-23 京瓷株式会社 Branching filter and communication module
JPWO2014196245A1 (en) * 2013-06-04 2017-02-23 京セラ株式会社 Duplexer and communication module
US9912319B2 (en) 2013-06-04 2018-03-06 Kyocera Corporation Duplexer and communication module
CN105191125B (en) * 2013-06-04 2018-04-03 京瓷株式会社 Channel-splitting filter and communication module
JP2020028101A (en) * 2018-08-18 2020-02-20 京セラ株式会社 Acoustic wave filter

Also Published As

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