JPH11330904A - Resonator type surface acoustic wave filter - Google Patents
Resonator type surface acoustic wave filterInfo
- Publication number
- JPH11330904A JPH11330904A JP10129841A JP12984198A JPH11330904A JP H11330904 A JPH11330904 A JP H11330904A JP 10129841 A JP10129841 A JP 10129841A JP 12984198 A JP12984198 A JP 12984198A JP H11330904 A JPH11330904 A JP H11330904A
- Authority
- JP
- Japan
- Prior art keywords
- resonator
- piezoelectric substrate
- saw
- filter
- series
- 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 8
- 239000003990 capacitor Substances 0.000 claims abstract description 52
- 239000000758 substrate Substances 0.000 claims abstract description 47
- 230000008878 coupling Effects 0.000 claims abstract description 18
- 238000010168 coupling process Methods 0.000 claims abstract description 18
- 238000005859 coupling reaction Methods 0.000 claims abstract description 18
- 238000010586 diagram Methods 0.000 description 21
- 238000003780 insertion Methods 0.000 description 16
- 230000037431 insertion Effects 0.000 description 16
- 229910013641 LiNbO 3 Inorganic materials 0.000 description 8
- 230000005540 biological transmission Effects 0.000 description 8
- 239000010409 thin film Substances 0.000 description 8
- 239000000463 material Substances 0.000 description 6
- 238000013461 design Methods 0.000 description 5
- 239000013078 crystal Substances 0.000 description 4
- 238000000034 method Methods 0.000 description 4
- 238000004519 manufacturing process Methods 0.000 description 3
- 229910004298 SiO 2 Inorganic materials 0.000 description 2
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 2
- 239000000956 alloy Substances 0.000 description 2
- 229910045601 alloy Inorganic materials 0.000 description 2
- 238000004891 communication Methods 0.000 description 2
- 239000004020 conductor Substances 0.000 description 2
- 230000003247 decreasing effect Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 238000010295 mobile communication Methods 0.000 description 2
- 238000012986 modification Methods 0.000 description 2
- 230000004048 modification Effects 0.000 description 2
- 238000012545 processing Methods 0.000 description 2
- 230000009467 reduction Effects 0.000 description 2
- WSMQKESQZFQMFW-UHFFFAOYSA-N 5-methyl-pyrazole-3-carboxylic acid Chemical compound CC1=CC(C(O)=O)=NN1 WSMQKESQZFQMFW-UHFFFAOYSA-N 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 230000008859 change Effects 0.000 description 1
- 239000002131 composite material Substances 0.000 description 1
- 230000002542 deteriorative effect Effects 0.000 description 1
- 238000011161 development Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 230000005284 excitation Effects 0.000 description 1
- 239000010408 film Substances 0.000 description 1
- GQYHUHYESMUTHG-UHFFFAOYSA-N lithium niobate Chemical compound [Li+].[O-][Nb](=O)=O GQYHUHYESMUTHG-UHFFFAOYSA-N 0.000 description 1
- 229910052751 metal Inorganic materials 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 150000002739 metals Chemical class 0.000 description 1
- 239000000203 mixture Substances 0.000 description 1
- UKDIAJWKFXFVFG-UHFFFAOYSA-N potassium;oxido(dioxo)niobium Chemical compound [K+].[O-][Nb](=O)=O UKDIAJWKFXFVFG-UHFFFAOYSA-N 0.000 description 1
- 230000008569 process Effects 0.000 description 1
- 239000010453 quartz Substances 0.000 description 1
- 238000012827 research and development Methods 0.000 description 1
- 238000003786 synthesis reaction Methods 0.000 description 1
Landscapes
- Surface Acoustic Wave Elements And Circuit Networks Thereof (AREA)
Abstract
Description
【0001】[0001]
【発明の属する技術分野】本発明は、例えば、自動車電
話機、携帯電話機、通信機器等の種々の回路に用いら
れ、特に信号通過帯域幅を調整できる構成にした共振器
型弾性表面波(Surface Acoustic Wave 、以下「SA
W」という)フィルタに関するものである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a surface acoustic wave (Surface Acoustic) which is used in various circuits of, for example, an automobile telephone, a portable telephone, a communication device and the like, and in particular, has a configuration in which a signal passing bandwidth can be adjusted. Wave, "SA
W ”).
【0002】[0002]
【従来の技術】一般に、SAW装置は、SAWを励振す
るためのすだれ状トランスデューサ(Interdigital Tran
sducer、以下「IDT」という)を有し、このIDTを
加工することにより、該SAW装置にいろいろな特性や
機能をもたせることができる。従来、SAW装置といえ
ば主にSAWフィルタを指すことが多く、そしてSAW
フィルタの中では多電極型SAWフィルタが主役であっ
た。ところが、近年、多電極型SAWフィルタの他に、
共振器型SAWフィルタの研究開発も盛んになり、SA
Wフィルタといえば、必ずしも多電極型SAWフィルタ
を意味しなくなってきた。2. Description of the Related Art Generally, a SAW device is an interdigital transducer for exciting a SAW.
The SAW device can have various characteristics and functions by processing the IDT. Conventionally, SAW devices are often mainly referred to as SAW filters, and
Among the filters, a multi-electrode SAW filter played a leading role. However, recently, in addition to the multi-electrode SAW filter,
Research and development of resonator-type SAW filters has also become active, and SA
Speaking of the W filter, it has not always meant a multi-electrode SAW filter.
【0003】共振器型SAWフィルタは、古典的な電気
フィルタの設計方法に基づいて構成されるSAW共振子
を用いたフィルタである。SAW共振子の本体は、すだ
れ状電極指が対向したIDTで、場合によって該IDT
の左右に反射器が設けられることもある。反射器もID
Tと同様にすだれ状電極指で構成され、この全電極指が
電気的に短絡される場合もあれば、開放される場合もあ
る。反射器は、主にIDTの左右に漏洩するSAWを音
響的に反射するものであり、その全電極指を電気的に短
絡しても、或いは開放しても、SAW共振子の特性に対
する影響は殆ど無い。SAW共振子のインピーダンス特
性は、LC共振子のインピーダンス特性に極めて類似し
ているので、電気フィルタの設計方法が適用できる。[0003] A resonator type SAW filter is a filter using a SAW resonator configured based on a classical electric filter design method. The main body of the SAW resonator is an IDT with interdigital electrodes facing each other.
Reflectors may be provided on the left and right of the camera. Reflector ID
Like T, it is composed of interdigital electrodes, all of which may be electrically short-circuited or open. The reflector mainly reflects the SAW leaking to the left and right of the IDT acoustically. Even if all the electrode fingers are electrically short-circuited or opened, the influence on the characteristics of the SAW resonator is not affected. Almost no. Since the impedance characteristics of the SAW resonator are very similar to the impedance characteristics of the LC resonator, the design method of the electric filter can be applied.
【0004】図2は、従来のSAW共振子を示す平面図
である。このSAW共振子10は、例えば、タンタル酸リ
チウム(LiTaO3 )、ニオブ酸リチウム(LiNb
O3 )或いは水晶(SiO2 )等の圧電基板11を有し、
この圧電基板11上に入力端子12、出力端子13、及び複数
本の電極指14a を有するIDT14が形成されている。I
DT14の両側には、反射器15L,15R が形成されている。
尚、反射器15L,15R は、不要な場合には形成されない。FIG. 2 is a plan view showing a conventional SAW resonator. The SAW resonator 10 includes, for example, lithium tantalate (LiTaO 3 ), lithium niobate (LiNb
O 3 ) or quartz (SiO 2 ).
An IDT 14 having an input terminal 12, an output terminal 13, and a plurality of electrode fingers 14a is formed on the piezoelectric substrate 11. I
Reflectors 15L and 15R are formed on both sides of DT14.
Incidentally, the reflectors 15L and 15R are not formed if they are unnecessary.
【0005】図3(a)〜(c)は、図2中の反射器15
L,15R を示す平面図であり、同図(a)は略図、同図
(b)は短絡型、及び同図(c)は開放型をそれぞれ示
している。各反射器15L,15R の電極指15a の数は、50
〜100本程度が適切である。一般に、各反射器15L,15
R の電極指15a は、図3(b)のように電気的に短絡さ
れるか、或いは図3(c)のように開放された形状にな
っている。反射器15L,15R を配置する位置は、所望のイ
ンピーダンスを得るために種々の位置が設定されるが、
IDT14の一番外側の電極指14a の中心と、反射器15L,
15R の該IDT14側の電極指15a の中心との距離が、励
振するSAWの1/4波長前後の距離になるように設定
されることが多い。このSAW共振子10の製造過程にお
いて、IDT14と反射器15L,15R とは同時に形成される
ので、その材質及び膜厚が同一になっている。IDT14
の材質は純Alまたは該純Alを主成分とした合金が一
般的であるが、場合によっては、純Au、純Ti又はこ
れらの金属を主材料とする合金が用いられることもあ
る。IDT14の膜厚は、数百Aから数千Aに設定され
る。このように構成されたSAW共振子10は、LC共振
器と類似したリアクタンス特性を示すので、その等価回
路がLC共振器で近似的に表されることが多い。FIGS. 3 (a) to 3 (c) show the reflector 15 shown in FIG.
FIGS. 5A and 5B are plan views showing L, 15R, wherein FIG. 5A shows a schematic diagram, FIG. 5B shows a short-circuit type, and FIG. The number of electrode fingers 15a of each reflector 15L, 15R is 50
About 100 is suitable. Generally, each reflector 15L, 15
The R electrode finger 15a is electrically short-circuited as shown in FIG. 3B, or has an open shape as shown in FIG. 3C. The positions where the reflectors 15L and 15R are arranged are set at various positions in order to obtain a desired impedance.
The center of the outermost electrode finger 14a of the IDT 14 and the reflector 15L,
The distance from the center of the electrode finger 15a on the IDT 14 side of the 15R is often set to be a distance of about 前後 wavelength of the SAW to be excited. In the manufacturing process of the SAW resonator 10, the IDT 14 and the reflectors 15L and 15R are formed at the same time, and therefore have the same material and thickness. IDT14
Is generally a pure Al or an alloy mainly containing the pure Al, but depending on the case, pure Au, pure Ti, or an alloy mainly containing these metals may be used. The thickness of the IDT 14 is set to several hundreds A to several thousands A. Since the SAW resonator 10 configured as described above has a reactance characteristic similar to that of an LC resonator, an equivalent circuit is often represented approximately by the LC resonator.
【0006】図4(a),(b)は、図2のSAW共振
子10の等価回路とリアクタンス特性を示す図である。図
4(a)の等価回路では、入力端子12と出力端子13との
間にインダクタンスLのインダクタ16、静電容量c1 の
キャパシタ17及び抵抗値rの抵抗18が直列接続され、こ
れらと並列に静電容量C0 のキャパシタ19が接続されて
いる。図4(b)のリアクタンス特性において、リアク
タンス特性X0 が0Ωになる周波数が共振周波数Fr1及
び反共振周波数Fa1であり、近似的に次式(1),
(2)でそれぞれ表される。 Fr1=1/2π√(Lc1) ・・・(1) Fa1=(1/2π)√{(c1 +C0 )/( c1 C0 L)} ・・・(2) このようなリアクタンス特性を有する素子を用いて電気
フィルタを設計する方法は、古くから知られている。FIGS. 4A and 4B are diagrams showing an equivalent circuit and reactance characteristics of the SAW resonator 10 shown in FIG. In the equivalent circuit of FIG. 4 (a), the inductor 16 of inductance L, a capacitor 17 and a resistor of resistance value r 18 of the electrostatic capacitance c 1 are connected in series between the input terminal 12 and output terminal 13, these parallel capacitor 19 of capacitance C 0 is connected to. In the reactance characteristic of FIG. 4B, the frequencies at which the reactance characteristic X0 becomes 0Ω are the resonance frequency Fr1 and the antiresonance frequency Fa1, and approximately the following equations (1) and (2).
Each is represented by (2). Fr1 = 1 / 2π√ (Lc 1 ) (1) Fa1 = (1 / 2π) √ {(c 1 + C 0 ) / (c 1 C 0 L)} (2) Such reactance A method of designing an electric filter using an element having characteristics has been known for a long time.
【0007】図2のSAW共振子10を用いてフィルタを
構成する場合、1段梯子型回路が基本回路になる。図5
(a),(b)は、従来の1段梯子型回路の2種類の例
を示す構成図である。図5(a)の1段梯子型回路20A
と図5(b)の1段梯子型回路20B とは、共に並列アー
ム(arm)共振子10P と直列アーム共振子10S とを有
し、且つ対称である。即ち、梯子型回路20A の左側の端
子21-0,22-0 から該梯子型回路20A を見たインピーダン
スは、梯子型回路20B の右側の端子21-1,22-1 から該梯
子型回路20B を見たインピーダンスに等しく、梯子型回
路20A の右側の端子21-1,22-1から該梯子型回路20A を
見たインピーダンスは、梯子型回路20B の左側の端子21
-0,22-0 から該梯子型回路20B を見たインピーダンスに
等しい。梯子型回路20A,20B を用いてフィルタを構成す
る場合、梯子型回路20A,20B 間のインピーダンスを考慮
しながら、梯子型回路20A 又は20B を選択する。梯子型
回路20A,20B において、並列アーム共振子10P の反共振
周波数と直列アーム共振子10S の共振周波数とが非常に
接近するか又は一致すれば、系全体の入力端子と出力端
子における整合状態が極めて良好な帯域フィルタの特性
が得られる。When a filter is formed using the SAW resonator 10 shown in FIG. 2, a one-stage ladder circuit is a basic circuit. FIG.
(A), (b) is a block diagram showing two types of examples of a conventional one-stage ladder type circuit. One stage ladder type circuit 20A of FIG.
5B and the one-stage ladder type circuit 20B of FIG. 5B both have a parallel arm (arm) resonator 10P and a series arm resonator 10S and are symmetrical. That is, the impedance of the ladder circuit 20A viewed from the left terminals 21-0 and 22-0 of the ladder circuit 20A is equal to the impedance of the ladder circuit 20B from the right terminals 21-1 and 22-1 of the ladder circuit 20B. The impedance when viewing the ladder-type circuit 20A from the right side terminals 21-1 and 22-1 of the ladder-type circuit 20A is equal to the impedance of the ladder-type circuit 20B.
It is equal to the impedance when the ladder type circuit 20B is viewed from -0, 22-0. When a filter is formed using the ladder circuits 20A and 20B, the ladder circuit 20A or 20B is selected in consideration of the impedance between the ladder circuits 20A and 20B. In the ladder type circuits 20A and 20B, if the anti-resonance frequency of the parallel arm resonator 10P and the resonance frequency of the series arm resonator 10S are very close to or coincide with each other, the matching state of the input terminal and the output terminal of the entire system will be improved. Very good bandpass filter characteristics are obtained.
【0008】図6は、図5の1段梯子型回路20A,20B の
リアクタンス特性及び伝送特性を示す図である。図6に
おいて、並列アーム共振子10P のリアクタンス特性及び
直列アーム共振子10S のリアクタンス特性は、特性曲線
Xp,Xsで示され、それぞれ共振周波数Frp,Frsと
反共振周波数Fap,Fasとを有する。その結果、1段梯
子型回路20A 又は20B の挿入損失特性は特性曲線I0 、
及び反射損失特性は特性曲線R0に示すようになる。FIG. 6 is a diagram showing reactance characteristics and transmission characteristics of the one-stage ladder type circuits 20A and 20B of FIG. In FIG. 6, the reactance characteristic of the parallel arm resonator 10P and the reactance characteristic of the series arm resonator 10S are shown by characteristic curves Xp and Xs, and have resonance frequencies Frp and Frs and antiresonance frequencies Fap and Fas, respectively. As a result, the insertion loss characteristic of the single-stage ladder type circuit 20A or 20B is represented by a characteristic curve I0,
The return loss characteristics are as shown in a characteristic curve R0.
【0009】この挿入損失特性I0 は帯域フィルタの挿
入損失特性で、梯子型回路20A ,20B の段数を増加する
ことによって通過帯域以外の減衰量が著しく増加する
が、通過帯域の挿入損失も増加する。そのため、フィル
タの構成に必要な段数は該フィルタの特性の条件、例え
ば通過帯域の挿入損失や帯域外減衰量のレベル等によっ
て設定する。又、この段数は或る程度フィルタの通過帯
域幅BWに寄与するが、決定的な要因ではない。通過帯域
幅BWを決めるのは、該フィルタを構成する直列アーム共
振子10S 及び並列アーム共振子10P の帯域幅、即ちそれ
ぞれのSAW共振子の共振周波数Frp,Frsと反共振周
波数Fap,Fasの周波数間隔と直列アーム共振子10S の
共振周波数Frsと並列アーム共振子10P の反共振周波数
Fapの周波数間隔である。図6では、共振器型SAWフ
ィルタを構成する各SAW共振子のリアクタンス特性が
示されているが、フィルタの通過帯域幅BWは、並列アー
ム共振子10P の共振周波数Frpと直列アーム共振子10S
の反共振周波数Fasの間に収まっている。即ち、フィル
タの通過帯域幅BWは並列アーム共振子10P の共振周波数
Frpと直列アーム共振子10S の反共振周波数Fasの周波
数間隔より広くなることはありえない。又、図6では、
反共振周波数Fapと共振周波数Frsとが一致するように
示されているが、これらの周波数Fap,Frsが一致せず
に、例えば反共振周波数Fapが共振周波数Frsより低け
れば、通過帯域幅BWが広くなり、反共振周波数Fapが共
振周波数Frsより高ければ、通過帯域幅BWが狭くなる。
いずれの場合においてもこの2つの周波数が一致しなけ
れば、そのずれの量が大きければ大きいほど梯子型回路
20A,20B 内の整合状態が悪化し、結果的にフィルタ特性
が劣化することになる。The insertion loss characteristic I0 is the insertion loss characteristic of the band-pass filter. The attenuation of the components other than the pass band is significantly increased by increasing the number of stages of the ladder circuits 20A and 20B, but the insertion loss of the pass band also increases. . Therefore, the number of stages required for the configuration of the filter is set according to the condition of the characteristics of the filter, for example, the level of the insertion loss in the pass band and the level of the out-of-band attenuation. The number of stages contributes to a certain extent to the pass band width BW of the filter, but is not a decisive factor. The pass bandwidth BW is determined by the bandwidth of the series arm resonator 10S and the parallel arm resonator 10P constituting the filter, that is, the resonance frequencies Frp and Frs of the respective SAW resonators and the frequencies of the anti-resonance frequencies Fap and Fas. The interval is the frequency interval between the resonance frequency Frs of the series arm resonator 10S and the anti-resonance frequency Fap of the parallel arm resonator 10P. FIG. 6 shows the reactance characteristics of each SAW resonator constituting the resonator type SAW filter. The pass bandwidth BW of the filter is different from the resonance frequency Frp of the parallel arm resonator 10P and the series arm resonator 10S.
Within the anti-resonance frequency Fas. That is, the pass bandwidth BW of the filter cannot be wider than the frequency interval between the resonance frequency Frp of the parallel arm resonator 10P and the anti-resonance frequency Fas of the series arm resonator 10S. In FIG. 6,
Although the anti-resonance frequency Fap and the resonance frequency Frs are shown to match, if the frequencies Fap and Frs do not match, for example, if the anti-resonance frequency Fap is lower than the resonance frequency Frs, the pass bandwidth BW becomes If the anti-resonance frequency Fap is higher than the resonance frequency Frs, the pass bandwidth BW becomes narrow.
In any case, if the two frequencies do not match, the larger the amount of deviation, the larger the ladder-type circuit
The matching state in 20A and 20B deteriorates, and as a result, the filter characteristics deteriorate.
【0010】しかし、従来、各種の通信機器に対して法
律によって割当てられた使用周波数帯域は、必ずしも梯
子型回路20A,20B 内の整合状態がよいときの通過帯域幅
BWと一致しない。従って、法律によって決められた使用
可能な周波数帯域に合うように通過帯域幅BWを調整しな
ければならない。そのため、共振器型SAWフィルタで
は、梯子型回路20A,20B 内の整合状態を犠牲にしてでも
並列アーム共振子10Pの反共振周波数Fapと直列アーム
共振子10S の共振周波数Frsとを互いにずらし、通過帯
域幅BWが割当てられた使用周波数帯域に合うように調整
せざるをえない。このようにすると、共振器型SAWフ
ィルタの挿入損失特性や反射損失特性が劣化し、フィル
タの低損失化が妨げられる。[0010] However, conventionally, the frequency band used by law for various communication devices is not necessarily the pass band width when the matching state in the ladder type circuits 20A and 20B is good.
Does not match BW. Therefore, the pass bandwidth BW must be adjusted to match the usable frequency band determined by law. Therefore, in the resonator type SAW filter, the anti-resonance frequency Fap of the parallel arm resonator 10P and the resonance frequency Frs of the series arm resonator 10S are shifted from each other even if the matching state in the ladder circuits 20A and 20B is sacrificed. The bandwidth BW must be adjusted to match the allocated frequency band. In this case, the insertion loss characteristic and the reflection loss characteristic of the resonator type SAW filter are deteriorated, and the reduction of the filter loss is prevented.
【0011】一方、実際に使用されている共振器型SA
Wフィルタの段数は、一般に3段以上であるが、フィル
タの構成の基本は上述したような一段の場合と変わらな
い。又、フィルタを構成するSAW共振子の梯子型回路
20A,20B の段数は、通過帯域幅BWに多少の影響を及ぼす
が、決定的な要因ではない。しかし、説明の簡単化を図
るために、便宜上、多段梯子型回路で構成した共振器型
SAWフィルタの構成を説明する。共振器型SAWフィ
ルタを構成する梯子型回路20A,20B の段数が増加する
と、共振子10P,10S の数も段数に比例して増加する。On the other hand, the resonator type SA actually used
The number of stages of the W filter is generally three or more, but the basic configuration of the filter is not different from the case of the single stage as described above. Also, a ladder type circuit of a SAW resonator constituting a filter
The number of stages of 20A and 20B has some influence on the pass bandwidth BW, but is not a decisive factor. However, for the sake of simplicity, the configuration of a resonator type SAW filter composed of a multi-stage ladder type circuit will be described for convenience. As the number of stages of the ladder type circuits 20A and 20B constituting the resonator type SAW filter increases, the number of resonators 10P and 10S also increases in proportion to the number of stages.
【0012】図7は、図5の梯子型回路20A,20B を用い
て構成された従来の4段共振器型SAWフィルタを示す
構成図である。この共振器型SAWフィルタでは、図5
(a),(b)の1段梯子型回路20A,20B を用い、段間
のインピーダンスが整合されるようにインピーダンスの
等しい端子同士が接続され、合計8個の共振子からなる
フィルタが構成されている。即ち、1段目の梯子型回路
20-1の並列アーム共振子10P-1 、2段目の梯子型回路20
-2の並列アーム共振子10P-2 、3段目の梯子型回路20-3
の並列アーム共振子10P-3 及び4段目の梯子型回路20-4
の並列アーム共振子10P-4 によって並列アームが構成さ
れ、直列アームには、梯子型回路20-1の直列アーム共振
子10S-1 、梯子型回路20-2の直列アーム共振子10S-2 、
梯子型回路20-3の直列アーム共振子10S-3及び梯子型回
路20-4の直列アーム共振子10S-4 が組込まれている。FIG. 7 is a block diagram showing a conventional four-stage resonator type SAW filter formed using the ladder type circuits 20A and 20B of FIG. In this resonator type SAW filter, FIG.
Using the one-stage ladder type circuits 20A and 20B of (a) and (b), terminals having the same impedance are connected so that the impedance between the stages is matched, and a filter composed of a total of eight resonators is formed. ing. That is, the first stage ladder type circuit
20-1 parallel arm resonator 10P-1, second stage ladder type circuit 20
-2 parallel arm resonator 10P-2, third stage ladder type circuit 20-3
Parallel arm resonator 10P-3 and fourth stage ladder type circuit 20-4
The parallel arm is constituted by the parallel arm resonator 10P-4 of the ladder type circuit 20-1, the series arm resonator 10S-1 of the ladder type circuit 20-1, the series arm resonator 10S-2 of the ladder type circuit 20-2,
The series arm resonator 10S-3 of the ladder type circuit 20-3 and the series arm resonator 10S-4 of the ladder type circuit 20-4 are incorporated.
【0013】直列に接続された2個の共振子又は並列に
接続された2個の共振子は、1個の共振子に合成するこ
とができる。この合成共振子は、各2個の共振子系とほ
ぼ同等のインピーダンス特性を持つことが特徴である。
例えば、梯子型回路20-2の直列アーム共振子10S-2 と梯
子型回路20-3の直列アーム共振子10S-3 とを合成し、梯
子型回路20-1の並列アーム共振子10P-1 と梯子型回路20
-2の並列アーム共振子10P-2 とを合成し、更に、梯子型
回路20-3の並列アーム共振子10P-3 と梯子型回路20-4の
並列アーム共振子10P-4 とを合成することにより、図7
の4段共振器型SAWフィルタは、図8(a),(b)
のようになる。図8(a),(b)は、図7の合成後の
4段共振器型SAWフィルタを示す構成図であり、同図
(a)は等化回路図、及び同図(b)は平面図である。[0013] Two resonators connected in series or two resonators connected in parallel can be combined into one resonator. This composite resonator is characterized in that it has impedance characteristics substantially equal to those of the two resonator systems.
For example, the series arm resonator 10S-1 of the ladder type circuit 20-1 is synthesized by combining the series arm resonator 10S-2 of the ladder type circuit 20-2 and the series arm resonator 10S-3 of the ladder type circuit 20-3. And ladder circuit 20
And the parallel arm resonator 10P-3 of the ladder type circuit 20-4 and the parallel arm resonator 10P-4 of the ladder type circuit 20-4. As a result, FIG.
(A) and (b) of FIG.
become that way. FIGS. 8A and 8B are configuration diagrams showing the combined four-stage resonator type SAW filter of FIG. 7, in which FIG. 8A is an equalization circuit diagram, and FIG. FIG.
【0014】図8(a)の等化回路において、並列アー
ム共振子10P-1 及び10P-2 の共振子合成により、新たな
並列アーム共振子10P-12が構成され、直列アーム共振子
10S-2 及び10S-3 の共振子合成により、新たな直列アー
ム共振子10S-23が構成され、並列アーム共振子10P-3 及
び10P-4 の共振子合成により、新たな並列アーム共振子
10P-34が構成される。よって、図7では8個の共振子10
P-1,10P-2,10P-3,10P-4,10S-1,10S-2,10S-3,10S-4 が必
要であったのに対し、図8では5個の共振子10P-12,10P
-34,10S-1,10S-23,10S-4で図7と同じ伝送特性及びイン
ピーダンス特性を持つ共振器型SAWフィルタが構成さ
れる。In the equalizer circuit shown in FIG. 8A, a new parallel arm resonator 10P-12 is formed by combining the resonators of the parallel arm resonators 10P-1 and 10P-2, and a series arm resonator is formed.
A new series arm resonator 10S-23 is formed by combining the resonators of 10S-2 and 10S-3, and a new parallel arm resonator is formed by combining the resonators of the parallel arm resonators 10P-3 and 10P-4.
10P-34 is configured. Therefore, in FIG. 7, eight resonators 10
While P-1, 10P-2, 10P-3, 10P-4, 10S-1, 10S-2, 10S-3, 10S-4 were required, in FIG. 8, five resonators 10P- 12,10P
-34, 10S-1, 10S-23 and 10S-4 constitute a resonator type SAW filter having the same transmission characteristics and impedance characteristics as those in FIG.
【0015】図8(b)の平面図において、この共振器
型SAWフィルタは、圧電基板11上に形成された入力端
子21-0及び出力端子21-4と、共振子10S-1,10S-23,10S-
4,10P-12,10P-34と、該各直列アーム共振子10S-1,10S-2
3,10S-4、並列アーム共振子10P-12,10P-34 間を接続す
る伝送路パタン23と、並列アーム共振子10P-12,10P-34
のアースパタン24とで、構成されている。共振器型SA
Wフィルタは一般に帯域フィルタなので、通過帯域の挿
入損失及び帯域外減衰量と同様に、通過帯域幅BWも特性
の重要な要素のひとつである。しかし、通過帯域幅BWは
基本的にフィルタの構成に用いられる圧電基板11の電気
機械結合係数k2 で決まり、しかも圧電基板11の材質も
数種類しかないので、通過帯域幅BWを所望の値にするこ
とは困難である。ここで、電気機械結合係数k2 とは、
圧電材料や磁歪材料について電気系と機械系との結合の
程度を表す定数であり、外から試料に与えた電気的エネ
ルギーEiのうち機械的エネルギーとして貯えられるも
のをEmとしたとき、 k2 =Em/Ei で与えられる。In the plan view of FIG. 8B, this resonator type SAW filter includes an input terminal 21-0 and an output terminal 21-4 formed on a piezoelectric substrate 11, and resonators 10S-1 and 10S-. 23,10S-
4,10P-12,10P-34 and each series arm resonator 10S-1,10S-2
3, 10S-4, transmission line pattern 23 connecting between parallel arm resonators 10P-12, 10P-34, and parallel arm resonators 10P-12, 10P-34
And an earth pattern 24. Resonator type SA
Since the W filter is generally a bandpass filter, the passband width BW is one of the important elements of the characteristic as well as the insertion loss and the out-of-band attenuation of the passband. However, the passband width BW is determined by the electromechanical coupling coefficient k 2 of the piezoelectric substrate 11 to be used in basically the filter configuration, and since there are only several kinds also the material of the piezoelectric substrate 11, the pass band width BW to the desired value It is difficult to do. Here, the electromechanical coupling coefficient k 2 is
It is a constant indicating the degree of coupling between an electric system and a mechanical system for a piezoelectric material or a magnetostrictive material. When Em is the electric energy Ei externally applied to a sample and stored as mechanical energy, k 2 = It is given by Em / Ei.
【0016】例えば、LiTaO3 の圧電基板11を用い
て図8のような共振器型SAWフィルタを作製した場
合、十分な帯域外減衰量を得るためには、梯子型回路20
A,20Bの段数が4段以上も必要なので、並列アーム共振
子10P の反共振周波数Fapと直列アーム共振子10S の共
振周波数Frsを図6のように一致させると、フィルタの
通過帯域幅BWが約20MHz になる。しかし、通過帯域幅BW
の仕様は25MHz なので、この条件を満たすためにフィル
タを構成する並列アーム共振子10P の反共振周波数Fap
を低域に2.5MHz以上、直列アーム共振子10S の共振周波
数Frsを高域に2.5MHzずらさなければならない。この結
果、通過帯域の挿入損失は約1.0dB 劣化してしまう。For example, when a resonator type SAW filter as shown in FIG. 8 is manufactured by using the piezoelectric substrate 11 of LiTaO 3 , in order to obtain a sufficient amount of out-of-band attenuation, a ladder-type circuit 20 is required.
Since the number of stages A and 20B is required to be four or more, if the anti-resonance frequency Fap of the parallel arm resonator 10P and the resonance frequency Frs of the series arm resonator 10S are made to match as shown in FIG. It is about 20MHz. But the pass bandwidth BW
Is 25 MHz, so to satisfy this condition, the anti-resonance frequency Fap of the parallel arm resonator 10P constituting the filter is
Must be shifted to 2.5 MHz or more in the low band, and the resonance frequency Frs of the series arm resonator 10S must be shifted to 2.5 MHz in the high band. As a result, the insertion loss in the pass band is degraded by about 1.0 dB.
【0017】又、電気機械結合係数k2 がLiTaO3
(k2 は、例えば0.66%)よりも約9倍のLiNbO3
(k2 は、例えば5.5%)の圧電基板を用いて図8の
ような共振器型SAWフィルタを作製した場合、逆に通
過帯域幅BWが仕様よりも広すぎ、該フィルタの梯子型回
路20A,20B を構成する並列アーム共振子10P の反共振周
波数Fapを高域に10.0MHz 以上、及び直列アーム共振子
10S の共振周波数Frsを低域に10.0MHz ずらさなければ
ならない。この結果、並列アーム共振子10P と直列アー
ム共振子10S との間に相当なインピーダンス不整合が生
じ、通過帯域の挿入損失は数デシベル劣化してしまう。
このように、従来の共振器型SAWフィルタでは、使用
条件によって必要不可欠な特性を優先的に実現される代
わりに、別の特性を犠牲にしている。Also, the electromechanical coupling coefficient k 2 is LiTaO 3
(K 2, for example 0.66%) LiNbO 3 to about 9 times greater than
When a resonator type SAW filter as shown in FIG. 8 is manufactured using a piezoelectric substrate (k 2 is, for example, 5.5%), the pass band width BW is too large compared with the specification, and the ladder type The anti-resonance frequency Fap of the parallel arm resonator 10P constituting the circuits 20A and 20B is set to a high range of 10.0 MHz or more, and the series arm resonator
The resonance frequency Frs of 10S must be shifted to the low band by 10.0 MHz. As a result, a considerable impedance mismatch occurs between the parallel arm resonator 10P and the series arm resonator 10S, and the insertion loss in the pass band deteriorates by several decibels.
As described above, in the conventional resonator-type SAW filter, indispensable characteristics are preferentially realized depending on use conditions, but other characteristics are sacrificed.
【0018】[0018]
【発明が解決しようとする課題】従来の図8のようなS
AWフィルタの高性能化にはいろいろな課題があるが、
主に低損失化(即ち、通過帯域挿入損失の低減)、通過
帯域外の高減衰量化、高耐電力化等が重要視されてい
る。しかし、近年、移動体通信技術の発展によって各種
の移動体通信機器が増加し、既に不足しがちの周波数帯
域の管理も厳しくなっているので、各種の移動体通信機
器の中に使用されているフィルタが低損失、高帯域外減
衰量、及び高耐電力であるという性能の他に、厳しく決
められた周波数帯域内にこれらの性能を維持しなければ
ならないという要求も追加される。この点において、S
AWフィルタは他のフィルタよりも不利な立場に立たさ
れてしまう。The conventional S as shown in FIG.
There are various issues in improving the performance of AW filters,
Emphasis is mainly placed on low loss (that is, reduction of passband insertion loss), high attenuation outside the passband, high power handling, and the like. However, in recent years, various types of mobile communication devices have been increased due to the development of mobile communication technology, and the management of frequency bands, which are often in short supply, has become stricter. In addition to the performance of filters with low loss, high out-of-band attenuation, and high power handling, there is an added requirement that these performances be maintained within tightly defined frequency bands. In this regard, S
AW filters are disadvantaged over other filters.
【0019】即ち、SAWフィルタの通過帯域幅BWは該
フィルタの圧電基板11の電気機械結合係数k2 にほぼ比
例するので、設計の自由度が制限されるわけである。前
述のように、SAWフィルタの基板として利用できる圧
電基板11の材質は数種類しかなく、例えばLiTa
O3 、LiNbO3 、SiO2 、ニオブ酸カリウム(K
NbO3 )、ランガサイト(La3 Ga5 SiO14)等
であるが、それぞれの電気機械結合係数k2 も決まって
いるので、これらを用いて図8のようなSAWフィルタ
を作製すると、その通過帯域幅BWはほぼ決まってしま
う。この場合、基板加工の過程で圧電基板11を切断する
ときに切断面と結晶軸の角度を調整すると、わずかなが
ら電気機械結合係数k2 を変えることができるので、S
AWフィルタの通過帯域幅BWもこれで微調整が可能であ
る。ところが、切断面と結晶軸の角度はSAWフィルタ
の挿入損失に支配的な役割をもっているので、簡単に変
えることはできず、通過帯域幅BWを変えるために切断面
と結晶軸の角度を調整すると、フィルタ通過帯域挿入損
失の劣化を招くという課題があった。That is, since the pass band width BW of the SAW filter is substantially proportional to the electromechanical coupling coefficient k 2 of the piezoelectric substrate 11 of the filter, the degree of freedom in design is limited. As described above, there are only a few types of materials for the piezoelectric substrate 11 that can be used as the substrate of the SAW filter.
O 3 , LiNbO 3 , SiO 2 , potassium niobate (K
NbO 3 ), langasite (La 3 Ga 5 SiO 14 ), and the like. Since the respective electromechanical coupling coefficients k 2 are also determined, a SAW filter as shown in FIG. The bandwidth BW is almost fixed. In this case, if the angle between the cut surface and the crystal axis is adjusted when cutting the piezoelectric substrate 11 in the process of processing the substrate, the electromechanical coupling coefficient k 2 can be slightly changed.
The pass band width BW of the AW filter can be finely adjusted by this. However, since the angle between the cut plane and the crystal axis has a dominant role in the insertion loss of the SAW filter, it cannot be easily changed, and if the angle between the cut plane and the crystal axis is adjusted to change the pass bandwidth BW, However, there is a problem that the insertion loss of the filter pass band is deteriorated.
【0020】本発明は、このような矛盾を除去し、Li
NbO3 等のような電気機械結合係数k2 の大きい圧電
基板を用いて共振器型SAWフィルタを作製する場合に
おいて、フィルタ通過帯域挿入損失の劣化を招くような
圧電基板の切断面と結晶軸の角度を変えることなく、フ
ィルタの通過帯域幅BWを所望の値に縮小できる構成の共
振器型SAWフィルタを提供することを目的とする。The present invention eliminates such inconsistency and provides Li
In the case of manufacturing a resonator type SAW filter with large piezoelectric substrate of the electromechanical coupling coefficient k 2, such as NbO 3, etc., the cut surface of the piezoelectric substrate, such as deteriorating the filter passband insertion loss of the crystal axis It is an object of the present invention to provide a resonator type SAW filter having a configuration capable of reducing a pass band width BW of a filter to a desired value without changing an angle.
【0021】[0021]
【課題を解決するための手段】SAW共振子の通過帯域
幅BWは、該SAW共振子の圧電基板の電気機械結合係数
k2 でほぼ決まるので、簡単にSAW共振子の構造だけ
で変えることはできない。SAW共振子の圧電基板とし
て、安価で温度特性の良好なLiTaO3 やSiO2 が
従来から使われているが、これらは電気機械結合係数k
2 が小さいので、通過帯域幅BWの広いSAW共振子やS
AWフィルタには適切ではない。特に、SAW共振子を
用いて共振器型SAWフィルタを構成する場合、梯子型
回路の段間の整合状態を最良の状態にすると、該フィル
タの通過帯域幅BWは仕様の幅よりかなり狭くなってしま
う。一方、電気機械結合係数k2 がLiTaO3 やSi
O2 よりも大きい材質(例えば、LiNbO3 )を圧電
基板として使うと、SAW共振子の通過帯域幅BWが広く
なりすぎるので、帯域フィルタには適切ではない。そこ
で、本発明のうちの請求項1に係る発明では、共振器型
SAWフィルタにおいて、所定の電気機械結合係数k2
を有する圧電基板と、前記圧電基板上に形成され、入力
信号を入力する入力端子と、前記圧電基板上に形成さ
れ、出力信号を出力する出力端子と、前記圧電基板上に
形成され且つ前記入力端子と出力端子との間に直列接続
され、所定のインピーダンス特性を有するSAW共振子
で構成された1つ又は複数の直列アーム共振子と、前記
1つ又は複数の直列アーム共振子にそれぞれ1つずつ直
列接続された1つ又は複数の第1のキャパシタと、前記
圧電基板上に形成され且つ前記各直列アーム共振子に対
して梯子型に接続され、所定のインピーダンス特性を有
するSAW共振子で構成された1つ又は複数の並列アー
ム共振子と、前記1つ又は複数の並列アーム共振子にそ
れぞれ1つずつ直列接続された1つ又は複数の第2のキ
ャパシタとを、備えている。Means for Solving the Problems] bandwidth BW pass of the SAW resonator, since substantially determined by electromechanical coupling coefficient k 2 of the piezoelectric substrate of the SAW resonator, simply by changing only the structure of the SAW resonator Can not. LiTaO 3 and SiO 2, which are inexpensive and have good temperature characteristics, have been conventionally used as the piezoelectric substrate of the SAW resonator.
2 is small, so that a SAW resonator having a wide pass bandwidth BW or S
Not suitable for AW filters. In particular, when a resonator type SAW filter is configured using a SAW resonator, if the matching state between the stages of the ladder type circuit is set to the best state, the pass band width BW of the filter becomes considerably narrower than the specified width. I will. On the other hand, when the electromechanical coupling coefficient k 2 is LiTaO 3 or Si
If a material (for example, LiNbO 3 ) larger than O 2 is used as the piezoelectric substrate, the pass band width BW of the SAW resonator becomes too wide, and is not suitable for a bandpass filter. Therefore, in the invention according to claim 1 of the present invention, in the resonator type SAW filter, a predetermined electromechanical coupling coefficient k 2
A piezoelectric substrate having: an input terminal formed on the piezoelectric substrate for inputting an input signal; an output terminal formed on the piezoelectric substrate for outputting an output signal; and an input terminal formed on the piezoelectric substrate and receiving the input signal. One or more series arm resonators connected in series between a terminal and an output terminal and configured by a SAW resonator having predetermined impedance characteristics, and one each for the one or more series arm resonators One or a plurality of first capacitors connected in series with each other, and a SAW resonator formed on the piezoelectric substrate and connected in a ladder shape to each of the series arm resonators and having a predetermined impedance characteristic. One or a plurality of parallel arm resonators, and one or a plurality of second capacitors serially connected to the one or a plurality of parallel arm resonators, respectively. There.
【0022】このような構成を採用したことにより、入
力信号が入力端子から入力されると、各直列アーム共振
子は、それぞれの反共振周波数以下の周波数を信号を通
過させ、反共振周波数以上の周波数を反射する。又、各
並列アーム共振子は、それぞれの共振周波数以上の周波
数の信号を通過させ、共振周波数以下の周波数を反射す
る。そのため、共振器型SAWフィルタは、並列アーム
共振子の共振周波数から直列アーム共振子の反共振周波
数までの周波数の信号を通過させ、帯域フィルタの働き
をする。例えば、圧電基板として電気機械結合係数k2
の大きいLiNbO3 を用いた場合、各SAW共振子の
帯域幅が必要以上に広くなっているので、各直列アーム
共振子及び並列アーム共振子に各第1及び第2のキャパ
シタをそれぞれ直列接続することにより、共振周波数を
高くし且つ反共振周波数を低くしている。そのため、信
号通過周波数帯域幅が縮小され、所望の値に調整され
る。請求項2に係る発明では、請求項1の第1及び第2
のキャパシタを、圧電基板の外部に接続される容量素
子、該圧電基板上に形成したすだれ状電極型の容量素
子、又は該圧電基板上に形成した多層電極型の容量素子
で構成している。これにより、フィルタを構成する各S
AW共振子にキャパシタが直列接続され、得られた新し
いSAW共振子の共振周波数と反共振周波数の周波数間
隔又は帯域幅を狭くすることにより、これらのキャパシ
タの容量の値でフィルタの通過帯域幅BWが所望の帯域幅
に調整される。By adopting such a configuration, when an input signal is input from the input terminal, each series arm resonator passes a signal having a frequency equal to or lower than the anti-resonance frequency and transmits a signal having a frequency equal to or higher than the anti-resonance frequency. Reflects frequency. Further, each parallel arm resonator passes a signal having a frequency equal to or higher than its resonance frequency and reflects a frequency equal to or lower than the resonance frequency. Therefore, the resonator-type SAW filter passes a signal having a frequency ranging from the resonance frequency of the parallel arm resonator to the anti-resonance frequency of the series arm resonator, and functions as a bandpass filter. For example, as a piezoelectric substrate, an electromechanical coupling coefficient k 2
In the case of using LiNbO 3 , the bandwidth of each SAW resonator is unnecessarily wide, so that each first and second capacitor is connected in series to each series arm resonator and parallel arm resonator. Thereby, the resonance frequency is increased and the anti-resonance frequency is decreased. Therefore, the signal passing frequency bandwidth is reduced and adjusted to a desired value. According to the second aspect of the invention, the first and second aspects of the first aspect are provided.
Are composed of a capacitive element connected to the outside of the piezoelectric substrate, an interdigital electrode type capacitive element formed on the piezoelectric substrate, or a multilayer electrode type capacitive element formed on the piezoelectric substrate. Thereby, each S constituting the filter is
Capacitors are connected in series to the AW resonators, and by narrowing the frequency interval or bandwidth between the resonance frequency and the antiresonance frequency of the obtained new SAW resonator, the pass band width BW of the filter is determined by the value of the capacitance of these capacitors. Is adjusted to the desired bandwidth.
【0023】[0023]
【発明の実施の形態】第1の実施形態 図9(a),(b)は、本発明の第1の実施形態を示す
SAW共振子の構成図であり、同図(a)は平面図、及
び同図(b)は等化回路である。図9(a)の平面図に
おいて、このSAW共振子30は、例えば、LiNbO3
の圧電基板31を有し、この圧電基板31上に入力端子32、
出力端子33、SAW共振子40及びすだれ状電極型のキャ
パシタ50が形成されている。SAW共振子40及びすだれ
状電極型のキャパシタ50は、入力端子32と出力端子33と
の間に直列接続されている。SAW共振子40は、複数本
の電極指41a を有するIDT41と、IDT41の両側に形
成された反射器42L,42R を有している。キャパシタ50
は、すだれ状電極50a を有している。このキャパシタ50
は、構造的には反射器を備えていないSAW共振子と同
一であるが、SAW励振を行うのではなく、静電容量を
得ることが目的なので、SAW共振子40より電極指間が
数十倍も広く、電極対数と交差長は、必要とする静電容
量の値に基づいて設定されている。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS First Embodiment FIGS. 9A and 9B are configuration diagrams of a SAW resonator according to a first embodiment of the present invention, and FIG. 9A is a plan view. , And FIG. 3B shows an equalizing circuit. In the plan view of FIG. 9A, the SAW resonator 30 is, for example, LiNbO 3
Of the piezoelectric substrate 31, the input terminal 32 on the piezoelectric substrate 31,
An output terminal 33, a SAW resonator 40 and an interdigital electrode type capacitor 50 are formed. The SAW resonator 40 and the interdigital electrode type capacitor 50 are connected in series between the input terminal 32 and the output terminal 33. The SAW resonator 40 has an IDT 41 having a plurality of electrode fingers 41a, and reflectors 42L and 42R formed on both sides of the IDT 41. Capacitor 50
Has an interdigital electrode 50a. This capacitor 50
Is structurally the same as a SAW resonator without a reflector, but the purpose is not to perform SAW excitation, but to obtain capacitance. The number of pairs of electrodes and the intersection length are set based on the required capacitance value.
【0024】図9(b)の等価回路において、入力端子
32と出力端子33との間に、SAW共振子40及びキャパシ
タ50が直列接続されている。SAW共振子40では、キャ
パシタ50と出力端子33との間にインダクタンスLのイン
ダクタ40a 、静電容量c1 のキャパシタ40b 及び抵抗値
rの抵抗40c が直列接続され、これらと並列に静電容量
c0 のキャパシタ40d が接続されている。In the equivalent circuit of FIG.
A SAW resonator 40 and a capacitor 50 are connected in series between 32 and the output terminal 33. In the SAW resonator 40, an inductor 40a having an inductance L, a capacitor 40b having a capacitance c 1 , and a resistor 40c having a resistance value r are connected in series between the capacitor 50 and the output terminal 33. 0 capacitor 40d is connected.
【0025】次に、図9(a)の動作を説明する。入力
端子32から高周波の入力信号が入力されると、該入力
信号がキャパシタ50を通過してSAW共振子40に到達す
るが、キャパシタ50の容量をC50、及び入力信号の角周
波数をωとすると、キャパシタ50のインピーダンスは
(−1/C50ω)になるので、SAW共振子40のインピ
ーダンスからインピーダンス1/C50ωが引かれる。一
方、SAW共振子40を構成するすべてのIDTの電極指
間に電圧差が生じてSAWが励振され、該SAW共振子
40が水晶共振子又は従来のLC共振子のようなインピー
ダンス特性を示す。Next, the operation of FIG. 9A will be described. When a high-frequency input signal is input from the input terminal 32, the input signal passes through the capacitor 50 and reaches the SAW resonator 40. The capacitance of the capacitor 50 is C 50 and the angular frequency of the input signal is ω. Then, since the impedance of the capacitor 50 becomes (−1 / C 50 ω), the impedance 1 / C 50 ω is subtracted from the impedance of the SAW resonator 40. On the other hand, a voltage difference is generated between the electrode fingers of all the IDTs constituting the SAW resonator 40, and the SAW is excited.
Numeral 40 indicates impedance characteristics like a quartz resonator or a conventional LC resonator.
【0026】図10は、図9のSAW共振子30のリアク
タンスの特性図である。但し、この図10では、比較の
ため、図4(b)中の特性曲線X0 も表示されている。
この図10において、特性曲線Xvは、図9のSAW共
振子30のリアクタンス特性を示している。共振周波数F
r1及び反共振周波数Fa1は従来の図2のSAW共振子10
の値であり、共振周波数Fr2及び反共振周波数Fa2は図
9のSAW共振子30の値である。キャパシタ50のインピ
ーダンスは負であるので、これをSAW共振子40に直列
に接続すると、系(即ち、SAW共振子30)全体のリア
クタンスは負の方向に下がることになる。その結果、図
10に示すように、(Fr2−Fa2)は(Fr1−Fa1)よ
りも小さくなっている。即ち、SAW共振子40にキャパ
シタ50を直列接続することにより、このSAW共振子40
の帯域幅が従来の図2のSAW共振子30よりも縮小され
ている。つまり、圧電基板31の電気機械結合係数k2 で
決まるSAW共振子40の帯域幅(Fr1−Fa1)が、キャ
パシタ50を直列接続することによって帯域幅(Fr2−F
a2)に縮小されている。FIG. 10 is a characteristic diagram of the reactance of the SAW resonator 30 shown in FIG. However, FIG. 10 also shows the characteristic curve X0 in FIG. 4B for comparison.
In FIG. 10, the characteristic curve Xv indicates the reactance characteristic of the SAW resonator 30 in FIG. Resonant frequency F
r1 and anti-resonance frequency Fa1 are the same as those of the conventional SAW resonator 10 shown in FIG.
The resonance frequency Fr2 and the anti-resonance frequency Fa2 are the values of the SAW resonator 30 in FIG. Since the impedance of the capacitor 50 is negative, if it is connected in series with the SAW resonator 40, the reactance of the entire system (that is, the SAW resonator 30) will decrease in the negative direction. As a result, as shown in FIG. 10, (Fr2−Fa2) is smaller than (Fr1−Fa1). That is, by connecting the capacitor 50 to the SAW resonator 40 in series,
Is smaller than that of the conventional SAW resonator 30 shown in FIG. In other words, the bandwidth of the SAW resonator 40 that is determined by the electromechanical coupling coefficient k 2 of the piezoelectric substrate 31 (Fr1-Fa1) is the bandwidth by serially connecting a capacitor 50 (Fr2-F
a2) has been reduced.
【0027】図1(a),(b)は、図9のSAW共振
子を用いた本実施形態の4段共振器型SAWフィルタの
構成図であり、同図(a)は平面図、及び同図(b)は
等化回路図である。図1(a)の平面図において、この
共振器型SAWフィルタは圧電基板31を有し、この圧電
基板31上に入力端子41-0、出力端子41-4、直列アーム共
振子40S-1,40S-23,40S-4 、並列アーム共振子40P-1
2,40P-34、及びすだれ状電極型のキャパシタ50S-1 ,5
0S-23,50S-4 ,50P-12,50P-34が形成されている。更
に、圧電基板31上には、直列アーム共振子40S-1 とキャ
パシタ50S-23,50P-12との間を接続する伝送路パタン6
1、直列アーム共振子40S-23とキャパシタ50S-4 ,50P-3
4との間を接続する伝送路パタン62、並列アーム共振子4
0P-12とキャパシタ50P-12との間を接続する伝送路パタ
ン63、並列アーム共振子40P-34とキャパシタ50P-34との
間を接続する伝送路パタン64、及び並列アーム共振子40
P-12,40P-34のアースパタン65が形成されている。FIGS. 1A and 1B are configuration diagrams of a four-stage resonator type SAW filter of the present embodiment using the SAW resonator shown in FIG. 9, and FIG. 1A is a plan view and FIG. FIG. 1B is an equalization circuit diagram. In the plan view of FIG. 1A, this resonator type SAW filter has a piezoelectric substrate 31, on which an input terminal 41-0, an output terminal 41-4, a series arm resonator 40S-1, 40S-23, 40S-4, parallel arm resonator 40P-1
2, 40P-34 and interdigital electrode type capacitors 50S-1,5
0S-23, 50S-4, 50P-12 and 50P-34 are formed. Further, on the piezoelectric substrate 31, a transmission line pattern 6 connecting the series arm resonator 40S-1 and the capacitors 50S-23 and 50P-12 is formed.
1, Series arm resonator 40S-23 and capacitors 50S-4, 50P-3
Transmission line pattern 62 connecting between 4 and parallel arm resonator 4
A transmission line pattern 63 connecting between 0P-12 and the capacitor 50P-12, a transmission line pattern 64 connecting between the parallel arm resonator 40P-34 and the capacitor 50P-34, and a parallel arm resonator 40
Earth patterns 65 of P-12 and 40P-34 are formed.
【0028】図1(b)の等価回路において、直列アー
ム共振子40S-1 ,40S-23,40S-4 、並列アーム40P-12,
40P-34にキャパシタ50S-1 ,50S-23,50S-4 ,50P-12,
50P-34が直列にそれぞれ接続され、直列アーム素子30S-
1 ,30S-23,30S-4 及び並列アーム素子30P-12,30P-34
が構成されている。入力端子41-0とノードN1との間に
直列アーム素子30S-1 が接続され、該ノードN1とアース
パタン65との間に並列アーム素子30P-12が接続されてい
る。ノードN1とノードN2との間に直列アーム素子30S-23
が接続され、該ノードN2とアースパタン65との間に並列
アーム素子30P-34が接続されている。ノードN2と出力端
子41-4との間に直列アーム素子30S-4 が接続されてい
る。In the equivalent circuit of FIG. 1B, the series arm resonators 40S-1, 40S-23, 40S-4, the parallel arms 40P-12,
Capacitors 50S-1, 50S-23, 50S-4, 50P-12, 40P-34
50P-34 are connected in series respectively, and the series arm element 30S-
1, 30S-23, 30S-4 and parallel arm element 30P-12, 30P-34
Is configured. The series arm element 30S-1 is connected between the input terminal 41-0 and the node N1, and the parallel arm element 30P-12 is connected between the node N1 and the ground pattern 65. Series arm element 30S-23 between node N1 and node N2
Are connected, and the parallel arm element 30P-34 is connected between the node N2 and the ground pattern 65. Series arm element 30S-4 is connected between node N2 and output terminal 41-4.
【0029】次に、図1の動作を説明する。各直列アー
ム素子30S-1,30S-23,30S-4は、それぞれの共振周波数以
上と反共振周波数以下の周波数を信号をよく通し、該反
共振周波数以上の周波数をあまり通さない。又、並列ア
ーム素子30P-12,30P-34 は、それぞれの共振周波数以上
と反共振周波数以下の周波数をよく通し、該共振周波数
以下の周波数をあまり通さない。その結果、この共振器
型SAWフィルタは、並列アーム素子30P-12,30P-34の
共振周波数から直列アーム素子30S-1,30S-23,30S-4の反
共振周波数までの周波数の信号を通過させ、帯域フィル
タとして働く。但し、本実施形態では、圧電基板31とし
て電気機械結合係数k2 の大きいLiNbO3 を用いた
ので、直列アーム共振子40S-1,40S-23,40S-4及び並列ア
ーム共振子40P-12,40P-34 の帯域幅が必要以上に広くな
っている。そのため、これらの各共振子にキャパシタ50
S-1,50S-23,50S-4,50P-12,50P-34をそれぞれ直列接続
し、帯域幅を縮小することによって所望の値に調整す
る。Next, the operation of FIG. 1 will be described. Each of the series arm elements 30S-1, 30S-23, and 30S-4 passes a signal well at a frequency equal to or higher than the resonance frequency and equal to or lower than the anti-resonance frequency, and does not pass a frequency higher than the anti-resonance frequency. Also, the parallel arm elements 30P-12 and 30P-34 pass frequencies higher than their respective resonance frequencies and lower than the antiresonance frequency well, and do not pass much frequencies below the resonance frequency. As a result, this resonator type SAW filter passes signals of frequencies from the resonance frequency of the parallel arm elements 30P-12, 30P-34 to the anti-resonance frequency of the series arm elements 30S-1, 30S-23, 30S-4. And acts as a bandpass filter. However, in the present embodiment, since using the larger LiNbO 3 of the electromechanical coupling coefficient k 2 as the piezoelectric substrate 31, series arm resonators 40S-1,40S-23,40S-4 and the parallel arm resonator 40P-12, 40P-34 bandwidth is wider than necessary. Therefore, a capacitor 50 is connected to each of these resonators.
S-1, 50S-23, 50S-4, 50P-12, 50P-34 are connected in series, respectively, and the bandwidth is adjusted to a desired value by reducing the bandwidth.
【0030】図11は、図1の共振器型SAWフィルタ
の挿入損失特性を示す特性図である。但し、この図11
では、比較のため、図1中の各共振子にキャパシタ50S-
1,50S-23,50S-4,50P-12,50P-34を接続しない場合の特性
曲線I1 も表示されている。この図11において、特性
曲線Ivは、図1の共振器型SAWフィルタの挿入損失
特性を示し、このフィルタを構成する直列アーム共振子
40S-1,40S-23,40S-4及び並列アーム共振子40P-12,40P-3
4 にキャパシタ50S-1,50S-23,50S-4,50P-12,50P-34をそ
れぞれ直列接続することにより、通過帯域幅BWが縮小さ
れていることが示されている。図9のSAW共振子30を
用いて構成した図1の共振器型SAWフィルタの通過帯
域幅BWは、このSAW共振子30の帯域幅の約1/2にな
る。このように、例えばLiNbO3 のような電気機械
結合係数k2 の大きい圧電基板31を用いて共振器型SA
Wフィルタを構成しても、直列アーム共振子40S-1,40S-
23,40S-4及び並列アーム共振子40P-12,40P-34 にキャパ
シタ50S-1,50S-23,50S-4,50P-12,50P-34をそれぞれ直列
接続することにより、広すぎる通過帯域幅BWが所望の値
に調整される。FIG. 11 is a characteristic diagram showing the insertion loss characteristics of the resonator type SAW filter of FIG. However, FIG.
For comparison, each resonator in FIG.
The characteristic curve I1 when the 1,50S-23, 50S-4, 50P-12, and 50P-34 are not connected is also displayed. 11, a characteristic curve Iv indicates the insertion loss characteristic of the resonator type SAW filter of FIG. 1, and a series arm resonator constituting this filter.
40S-1,40S-23,40S-4 and parallel arm resonator 40P-12,40P-3
FIG. 4 shows that the pass bandwidth BW is reduced by connecting the capacitors 50S-1, 50S-23, 50S-4, 50P-12, and 50P-34 in series. The pass band width BW of the resonator type SAW filter shown in FIG. 1 configured by using the SAW resonator 30 shown in FIG. 9 is about の of the bandwidth of the SAW resonator 30. Thus, for example, an electromechanical coupling coefficient k 2 of the large cavity with a piezoelectric substrate 31 SA such as LiNbO 3
Even if a W filter is configured, the series arm resonators 40S-1, 40S-
By connecting capacitors 50S-1, 50S-23, 50S-4, 50P-12, and 50P-34 in series to 23, 40S-4 and parallel arm resonators 40P-12, 40P-34, respectively, the passband is too wide. The width BW is adjusted to a desired value.
【0031】以上のように、この第1の実施形態では、
例えば、LiNbO3 のような電気機械結合係数k2 の
大きい圧電基板31を用いて共振器型SAWフィルタを構
成した場合、直列アーム共振子40S-1,40S-23,40S-4及び
並列アーム共振子40P-12,40P-34 にキャパシタ50S-1,50
S-23,50S-4,50P-12,50P-34をそれぞれ直列接続すること
により、広すぎる通過帯域幅BWを所望の値に調整でき
る。As described above, in the first embodiment,
For example, when a resonator-type SAW filter using a piezoelectric substrate 31 having a large electromechanical coupling coefficient k 2, such as LiNbO 3, the series arm resonator 40S-1,40S-23,40S-4 and the parallel arm resonator 40P-12,40P-34 and capacitor 50S-1,50
By connecting S-23, 50S-4, 50P-12, and 50P-34 in series, the excessively wide pass bandwidth BW can be adjusted to a desired value.
【0032】第2の実施形態 図12は、本発明の第2の実施形態を示すSAW共振子
の断面図であり、第1の実施形態を示す図9(a)中の
要素と共通の要素には共通の符号が付されている。この
SAW共振子では、図9(a)中のキャパシタ50に代え
て、異なる構成のキャパシタ60が設けられている。この
キャパシタ60は、多層電極型キャパシタの構造を有し、
圧電基板31上に、導体薄膜61、誘電体薄膜(例えば、S
iO2 )62、導体薄膜63、誘電体薄膜64及び導体薄膜65
が順に積層されて構成されている。導体薄膜65は、入力
端子32に接続されている。キャパシタ60の静電容量は、
導体薄膜61,63,65の交差面積、及び誘電体薄膜62,64 の
膜厚と誘電率によって決定される。このSAW共振子を
用いて図1と同様の共振器型SAWフィルタ0構成した
場合には、第1の実施形態とほぼ同様の動作が行われ
る。多層電極型のキャパシタ60は、第1の実施形態のす
だれ状電極型のキャパシタ50と比べて製造プロセスに手
間がかかるが、静電容量の設定の自由度が大きいので、
設計の都合によって採用されることがある。以上のよう
に、この第2の実施形態では、直列アーム共振子40S-1,
40S-23,40S-4及び並列アーム共振子40P-12,40P-34 に直
列接続するキャパシタとして多層電極型のキャパシタ60
を採用したので、第1の実施形態にの利点に加え、静電
容量の設定の自由度を大きくできる。 Second Embodiment FIG. 12 is a cross-sectional view of a SAW resonator showing a second embodiment of the present invention, and is common to the elements in FIG. 9A showing the first embodiment. Are denoted by the same reference numerals. In this SAW resonator, a capacitor 60 having a different configuration is provided in place of the capacitor 50 in FIG. This capacitor 60 has a multilayer electrode type capacitor structure,
A conductor thin film 61 and a dielectric thin film (for example, S
iO 2 ) 62, conductive thin film 63, dielectric thin film 64 and conductive thin film 65
Are sequentially laminated. The conductive thin film 65 is connected to the input terminal 32. The capacitance of the capacitor 60 is
It is determined by the intersection area of the conductor thin films 61, 63, 65 and the film thickness and the dielectric constant of the dielectric thin films 62, 64. When a resonator type SAW filter 0 similar to that of FIG. 1 is configured using this SAW resonator, substantially the same operation as in the first embodiment is performed. The multilayer electrode type capacitor 60 requires more time for the manufacturing process than the IDT-type capacitor 50 of the first embodiment, but has a large degree of freedom in setting the capacitance.
May be adopted for design reasons. As described above, in the second embodiment, the series arm resonators 40S-1,
A multilayer electrode type capacitor 60 is used as a capacitor connected in series to the 40S-23, 40S-4 and the parallel arm resonators 40P-12, 40P-34.
Is adopted, the degree of freedom in setting the capacitance can be increased in addition to the advantages of the first embodiment.
【0033】尚、本発明は上記実施形態に限定されず、
種々の変形が可能である。その変形例としては、例えば
次のようなものがある。 (a) 実施形態では、4段の共振器型SAWフィルタ
について説明したが、この段数は必要な減衰量の仕様に
応じて増減してもよい。 (b) 共振器型SAWフィルタの構成は、図7に示す
回路構成にすると部品点数が多くなるが、図1と同様の
作用、効果が得られる。 (c) 図9中の反射器42L,42R は、損失が多くてもよ
い場合には削除してもよい。 (d) 図9中のキャパシタ50は、出力端子33とSAW
共振子40との間に形成してもよい。 (e) 図9中のキャパシタ50及び図1中のキャパシタ
50S-1,50S-23,50S-4,50P-12,50P-34は全てすだれ状電極
型になっているが、圧電基板31の寸法、SAW共振子40
の位置、寸法等により、多層電極型、又はすだれ状電極
型と多層電極型との混合にしてもよく、又、圧電基板31
の外部に接続してもよい。これにより、共振器型SAW
フィルタの設計の自由度を大きくできる。The present invention is not limited to the above embodiment,
Various modifications are possible. For example, there are the following modifications. (A) In the embodiment, a four-stage resonator type SAW filter has been described, but the number of stages may be increased or decreased according to the required specification of the amount of attenuation. (B) In the configuration of the resonator type SAW filter, if the circuit configuration shown in FIG. 7 is used, the number of components is increased, but the same operation and effect as in FIG. 1 can be obtained. (C) The reflectors 42L and 42R in FIG. 9 may be deleted if the loss may be large. (D) The capacitor 50 in FIG.
It may be formed between the resonator 40. (E) Capacitor 50 in FIG. 9 and capacitor in FIG.
50S-1, 50S-23, 50S-4, 50P-12, 50P-34 are all of the IDT type, but the dimensions of the piezoelectric substrate 31, the SAW resonator 40
Depending on the position, size, etc. of the piezoelectric substrate 31, a multilayer electrode type or a mixture of an interdigital electrode type and a multilayer electrode type may be used.
May be connected to the outside. Thereby, the resonator type SAW
The degree of freedom in filter design can be increased.
【0034】[0034]
【発明の効果】以上詳細に説明したように、請求項1に
係る発明によれば、共振器型SAWフィルタを構成する
各直列アーム共振子及び各並列アーム共振子に各キャパ
シタをそれぞれ直列接続することにより、広すぎる通過
帯域幅BWを所望の値に調整できる。請求項2に係る発明
によれば、各直列アーム共振子及び並列アーム共振子に
直列接続するキャパシタとして圧電基板の外部に接続さ
れる容量素子、該圧電基板上に形成したすだれ状電極型
の容量素子、又は多層電極型の容量素子を採用したの
で、請求項1に係る発明の効果に加え、静電容量の設定
の自由度を大きくできる。As described above in detail, according to the first aspect of the present invention, each capacitor is connected in series to each of the series arm resonators and each of the parallel arm resonators constituting the resonator type SAW filter. Thereby, the passband BW that is too wide can be adjusted to a desired value. According to the second aspect of the present invention, a capacitance element connected to the outside of the piezoelectric substrate as a capacitor connected in series to each of the series arm resonators and the parallel arm resonators, and an interdigital electrode type capacitance formed on the piezoelectric substrate Since the element or the multilayer electrode type capacitance element is employed, the degree of freedom in setting the capacitance can be increased in addition to the effect of the invention according to claim 1.
【図1】本発明の第1の実施形態の4段共振器型SAW
フィルタの構成図である。FIG. 1 shows a four-stage resonator type SAW according to a first embodiment of the present invention.
It is a block diagram of a filter.
【図2】従来のSAW共振子の平面図である。FIG. 2 is a plan view of a conventional SAW resonator.
【図3】図2中の反射器15L,15R の平面図である。FIG. 3 is a plan view of reflectors 15L and 15R in FIG.
【図4】図2のSAW共振子10の等価回路とリアクタン
ス特性を示す図である。FIG. 4 is a diagram showing an equivalent circuit and reactance characteristics of the SAW resonator 10 of FIG.
【図5】従来の1段梯子型回路の構成図である。FIG. 5 is a configuration diagram of a conventional one-stage ladder type circuit.
【図6】図5の伝送特性図である。6 is a transmission characteristic diagram of FIG.
【図7】図5の梯子型回路を用いて構成された従来の4
段共振器型SAWフィルタの構成図である。FIG. 7 shows a conventional ladder circuit constructed using the ladder type circuit of FIG.
It is a block diagram of a step resonator type SAW filter.
【図8】合成後の共振器型SAWフィルタの構成図であ
る。FIG. 8 is a configuration diagram of a resonator-type SAW filter after synthesis.
【図9】本発明の第1の実施形態のSAW共振子の構成
図である。FIG. 9 is a configuration diagram of a SAW resonator according to the first embodiment of the present invention.
【図10】図9のリアクタンスの特性図である。FIG. 10 is a characteristic diagram of the reactance of FIG. 9;
【図11】図1の挿入損失特性の特性図である。11 is a characteristic diagram of the insertion loss characteristic of FIG.
【図12】本発明の第2の実施形態のSAW共振子の断
面図である。FIG. 12 is a sectional view of a SAW resonator according to a second embodiment of the present invention.
30,40 SAW共
振子 30S-1,30S-23,30S-4 直列アー
ム素子 30P-12,30P-34 並列アー
ム素子 40S-1,40S-23,40S-4 直列アー
ム共振子 40P-12,40P-34 並列アー
ム共振子 31 圧電基板 32,41-0 入力端子 33,41-4 出力端子 41 IDT 42L,42R 反射器 50,50S-1,50S-23,50S-4,50P-12,50P-34,60 キャパシ
タ30,40 SAW resonator 30S-1,30S-23,30S-4 Series arm element 30P-12,30P-34 Parallel arm element 40S-1,40S-23,40S-4 Series arm resonator 40P-12,40P -34 Parallel arm resonator 31 Piezoelectric substrate 32,41-0 Input terminal 33,41-4 Output terminal 41 IDT 42L, 42R Reflector 50,50S-1,50S-23,50S-4,50P-12,50P- 34,60 capacitors
Claims (2)
板と、 前記圧電基板上に形成され、入力信号を入力する入力端
子と、 前記圧電基板上に形成され、出力信号を出力する出力端
子と、 前記圧電基板上に形成されて前記入力端子と前記出力端
子との間に直列接続され、所定のインピーダンス特性を
有する弾性表面波共振子で構成された1つ又は複数の直
列アーム共振子と、 前記1つ又は複数の直列アーム共振子にそれぞれ1つず
つ直列接続された1つ又は複数の第1のキャパシタと、 前記圧電基板上に形成されて前記各直列アーム共振子に
対して梯子型に接続され、所定のインピーダンス特性を
有する弾性表面波共振子で構成された1つ又は複数の並
列アーム共振子と、 前記1つ又は複数の並列アーム共振子にそれぞれ1つず
つ直列接続された1つ又は複数の第2のキャパシタと
を、備えたことを特徴とする共振器型弾性表面波フィル
タ。A piezoelectric substrate having a predetermined electromechanical coupling coefficient; an input terminal formed on the piezoelectric substrate for inputting an input signal; and an output terminal formed on the piezoelectric substrate for outputting an output signal. One or more series arm resonators formed on the piezoelectric substrate, connected in series between the input terminal and the output terminal, and configured by surface acoustic wave resonators having predetermined impedance characteristics, One or more first capacitors respectively connected in series to the one or more series arm resonators, and one or more first capacitors formed on the piezoelectric substrate and in a ladder form with respect to each of the series arm resonators One or more parallel arm resonators connected to each other and configured by a surface acoustic wave resonator having a predetermined impedance characteristic, and one series connection to each of the one or more parallel arm resonators A resonator-type surface acoustic wave filter comprising one or more second capacitors.
上に形成されるすだれ状電極型の容量素子、又は該圧電
基板上に形成される多層電極型の容量素子で構成したこ
とを特徴とする請求項1記載の共振器型弾性表面波フィ
ルタ。2. The capacitor according to claim 1, wherein the first and second capacitors are capacitive elements connected to the outside of the piezoelectric substrate, IDT-type capacitive elements formed on the piezoelectric substrate, or formed on the piezoelectric substrate. 2. A resonator type surface acoustic wave filter according to claim 1, wherein said surface acoustic wave filter comprises a multilayer electrode type capacitive element.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10129841A JPH11330904A (en) | 1998-05-13 | 1998-05-13 | Resonator type surface acoustic wave filter |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP10129841A JPH11330904A (en) | 1998-05-13 | 1998-05-13 | Resonator type surface acoustic wave filter |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH11330904A true JPH11330904A (en) | 1999-11-30 |
Family
ID=15019568
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP10129841A Pending JPH11330904A (en) | 1998-05-13 | 1998-05-13 | Resonator type surface acoustic wave filter |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH11330904A (en) |
Cited By (12)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2004072411A (en) * | 2002-08-06 | 2004-03-04 | Matsushita Electric Ind Co Ltd | SAW filter and electronic device using the same |
| JP2005311568A (en) * | 2004-04-20 | 2005-11-04 | Sony Corp | Filter device and transceiver |
| US7116187B2 (en) * | 2001-09-25 | 2006-10-03 | Tdk Corporation | Saw element and saw device |
| KR100708062B1 (en) | 2003-07-28 | 2007-04-16 | 가부시키가이샤 무라타 세이사쿠쇼 | Surface acoustic wave device and communication apparatus |
| EP1758247A3 (en) * | 2005-08-25 | 2007-11-14 | Fujitsu Media Devices Limited | Duplexer having matching circuit |
| JP2008005277A (en) * | 2006-06-23 | 2008-01-10 | Kyocera Kinseki Corp | Low pass filter |
| US7688161B2 (en) * | 2006-10-25 | 2010-03-30 | Fujitsu Media Devices Limited | Acoustic wave device and filter using the same |
| US20130021116A1 (en) * | 2010-05-13 | 2013-01-24 | Murata Manufacturing Co., Ltd. | Elastic wave device |
| JP2016096529A (en) * | 2014-11-13 | 2016-05-26 | ワイソル株式会社 | Surface acoustic wave (SAW) filter capacitor, surface acoustic wave (SAW) filter, and manufacturing method thereof |
| CN108028641A (en) * | 2015-09-09 | 2018-05-11 | 株式会社村田制作所 | Frequency varying filter, high-frequency front-end circuit |
| WO2018147135A1 (en) * | 2017-02-07 | 2018-08-16 | 株式会社村田製作所 | High frequency filter, high frequency front-end circuit, and communication device |
| US10979027B2 (en) * | 2016-09-29 | 2021-04-13 | Murata Manufacturing Co., Ltd. | Acoustic wave device, radio frequency front-end circuit, and communication device |
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Cited By (17)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US7116187B2 (en) * | 2001-09-25 | 2006-10-03 | Tdk Corporation | Saw element and saw device |
| EP1296454A3 (en) * | 2001-09-25 | 2007-02-07 | TDK Corporation | SAW element and SAW device |
| JP2004072411A (en) * | 2002-08-06 | 2004-03-04 | Matsushita Electric Ind Co Ltd | SAW filter and electronic device using the same |
| KR100708062B1 (en) | 2003-07-28 | 2007-04-16 | 가부시키가이샤 무라타 세이사쿠쇼 | Surface acoustic wave device and communication apparatus |
| JP2005311568A (en) * | 2004-04-20 | 2005-11-04 | Sony Corp | Filter device and transceiver |
| EP1758247A3 (en) * | 2005-08-25 | 2007-11-14 | Fujitsu Media Devices Limited | Duplexer having matching circuit |
| JP2008005277A (en) * | 2006-06-23 | 2008-01-10 | Kyocera Kinseki Corp | Low pass filter |
| US7688161B2 (en) * | 2006-10-25 | 2010-03-30 | Fujitsu Media Devices Limited | Acoustic wave device and filter using the same |
| US20130021116A1 (en) * | 2010-05-13 | 2013-01-24 | Murata Manufacturing Co., Ltd. | Elastic wave device |
| US8710940B2 (en) * | 2010-05-13 | 2014-04-29 | Murata Manufacturing Co., Ltd. | Elastic wave device having a capacitive electrode on the piezoelectric substrate |
| JP2016096529A (en) * | 2014-11-13 | 2016-05-26 | ワイソル株式会社 | Surface acoustic wave (SAW) filter capacitor, surface acoustic wave (SAW) filter, and manufacturing method thereof |
| US9654084B2 (en) | 2014-11-13 | 2017-05-16 | Wisol Co., Ltd. | Capacitor for saw filter, saw filter and method of manufacturing thereof |
| CN108028641A (en) * | 2015-09-09 | 2018-05-11 | 株式会社村田制作所 | Frequency varying filter, high-frequency front-end circuit |
| CN108028641B (en) * | 2015-09-09 | 2021-04-20 | 株式会社村田制作所 | Frequency variable filter, high frequency front-end circuit |
| US10979027B2 (en) * | 2016-09-29 | 2021-04-13 | Murata Manufacturing Co., Ltd. | Acoustic wave device, radio frequency front-end circuit, and communication device |
| WO2018147135A1 (en) * | 2017-02-07 | 2018-08-16 | 株式会社村田製作所 | High frequency filter, high frequency front-end circuit, and communication device |
| US10763825B2 (en) | 2017-02-07 | 2020-09-01 | Murata Manufacturing Co., Ltd. | Radio-frequency filter, radio-frequency front-end circuit, and communication device |
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