JPH05251982A - Surface acoustic wave filter - Google Patents
Surface acoustic wave filterInfo
- Publication number
- JPH05251982A JPH05251982A JP4048450A JP4845092A JPH05251982A JP H05251982 A JPH05251982 A JP H05251982A JP 4048450 A JP4048450 A JP 4048450A JP 4845092 A JP4845092 A JP 4845092A JP H05251982 A JPH05251982 A JP H05251982A
- Authority
- JP
- Japan
- Prior art keywords
- electrode
- surface acoustic
- acoustic wave
- wave filter
- substrate
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は弾性表面波フィルタに関
し、さらに詳細には36°YカットX方向伝搬LiTa
O3 基板を使用した弾性表面波フィルタに関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a surface acoustic wave filter, and more particularly to 36 ° Y-cut X-direction propagation LiTa.
The present invention relates to a surface acoustic wave filter using an O 3 substrate.
【0002】[0002]
【従来の技術】移動体通信機の小型化にともない、小型
かつ軽量の弾性表面波フィルタが要求されている。特に
RF帯のフィルタとしては従来使用されていた誘電体フ
ィルタの小型化が難しく弾性表面波フィルタの開発が進
められている。このRF帯のフィルタには低損失、高選
択性、高帯域外減衰特性が要求されていて、一般には多
電極構成方法が使用される。多電極構成方法による多電
極方式弾性表面波フィルタにおいて、電極数を多くする
ことによって低損失化が可能である。また、基板として
は高選択性の要求から、一般に温度特性の比較的良好な
36°YカットX方向伝搬LiTaO3 基板が使用され
る。2. Description of the Related Art With the miniaturization of mobile communication devices, there is a demand for small and lightweight surface acoustic wave filters. In particular, as a filter in the RF band, it is difficult to miniaturize a dielectric filter that has been conventionally used, and development of a surface acoustic wave filter is being advanced. This RF band filter is required to have low loss, high selectivity and high out-of-band attenuation characteristics, and a multi-electrode construction method is generally used. In the multi-electrode surface acoustic wave filter using the multi-electrode configuration method, it is possible to reduce the loss by increasing the number of electrodes. Further, as a substrate, a 36 ° Y-cut X-direction propagation LiTaO 3 substrate having a relatively good temperature characteristic is generally used because of the requirement of high selectivity.
【0003】また、弾性表面波フィルタの電極指は図5
に示すように入力電極および出力電極それぞれにおける
電極指の線幅Lmと電極指間の空隙幅Lgとの比(Lm
/Lg)が通常1になるように設定される。このように
設定された弾性表面波フィルタの周波数特性は図6に示
す如くである。ここで図6は電極指対数18の入力電極
が7個、電極指対数26の出力電極が6個で構成された
弾性表面波フィルタの例である。The electrode fingers of the surface acoustic wave filter are shown in FIG.
As shown in, the ratio (Lm between the line width Lm of the electrode fingers and the gap width Lg between the electrode fingers in each of the input and output electrodes (Lm
/ Lg) is normally set to 1. The frequency characteristics of the surface acoustic wave filter thus set are as shown in FIG. Here, FIG. 6 shows an example of a surface acoustic wave filter having seven input electrodes with 18 electrode finger pairs and six output electrodes with 26 electrode finger pairs.
【0004】[0004]
【発明が解決しようとする課題】しかるに、36°Yカ
ットX方向伝搬LiTaO3 基板を使用した多電極方式
弾性表面波フィルタの場合、図6に示したように一般的
に周波数特性において、周波数が高い領域の損失が大き
いという問題点があった。However, in the case of a multi-electrode type surface acoustic wave filter using a 36 ° Y-cut X-direction propagating LiTaO 3 substrate, as shown in FIG. There is a problem that the loss in the high region is large.
【0005】36°YカットX方向伝搬LiTaO3 基
板を伝搬する波は基板表面の電気的状態によって大きく
変化し、いわゆるSSBW(Surface Skimming Bulk Wa
ve)とLSAW(Leaky Surface Acoustic Wave)が複雑
に結合したグレーティングモードとして伝搬する(「高
結合回転YカットLiNbO3 およびLiTaO3 を伝
搬するSSBWと Leaky SAW」電子通信学会論文誌
Vol.J67−C No.1P. 158 − 165(1984))。The wave propagating in the 36 ° Y-cut X-direction propagation LiTaO 3 substrate largely changes depending on the electrical state of the substrate surface, so-called SSBW (Surface Skimming Bulk Wafer).
ve) and LSAW (Leaky Surface Acoustic Wave) propagate as complexly coupled grating modes (“Highly coupled rotating Y-cut LiNbO 3 and LiTaO 3 propagate SSBW and Leaky SAW” IEICE Transactions.
Vol. J67-C No. 1P. 158-165 (1984)).
【0006】しかし、このグレーティングモードは速い
横波と結合すると、バルク波としてエネルギを基板内部
に放射する。このエネルギ放射には周波数特性があり、
フィルタ特性とした場合の通過帯域特性に影響を及ぼす
と考えられる。However, this grating mode, when coupled with a fast transverse wave, radiates energy into the substrate as a bulk wave. This energy radiation has frequency characteristics,
It is considered that the pass band characteristic is affected when the filter characteristic is used.
【0007】本発明は36°YカットX方向伝搬LiT
aO3 基板を使用し、通過帯域特性を改善した弾性表面
波フィルタを提供することを目的とする。The present invention is a 36 ° Y-cut X-direction propagating LiT
An object is to provide a surface acoustic wave filter using an aO 3 substrate and having improved pass band characteristics.
【0008】[0008]
【課題を解決するための手段】本発明の弾性表面波フィ
ルタは、36°YカットX方向伝搬LiTaO3 を基板
とし、該基板上に入力電極と出力電極の合計が3個以上
で構成された多電極方式弾性表面波フィルタにおいて、
入力電極および出力電極それぞれにおける電極指の線幅
Lmと電極指間の空隙幅Lgとの比(Lm/Lg)を
1.2<(Lm/Lg)<3の範囲としたことを特徴と
する。The surface acoustic wave filter of the present invention comprises a substrate made of 36 ° Y-cut X-direction propagating LiTaO 3 and has a total of three or more input electrodes and output electrodes on the substrate. In the multi-electrode surface acoustic wave filter,
The ratio (Lm / Lg) of the line width Lm of the electrode fingers and the gap width Lg between the electrode fingers in each of the input electrode and the output electrode is set in the range of 1.2 <(Lm / Lg) <3. .
【0009】[0009]
【作用】本発明の弾性表面波フィルタによれば、入力電
極および出力電極それぞれにおける電極指の線幅Lmと
電極指間の空隙幅Lgとの比(Lm/Lg)を1.2<
(Lm/Lg)<3の範囲としたためバルク波の放射が
抑えられて、通過帯域特性は向上し、かつ入力インピー
ダンスの変化が大きくなく、製造が容易となる。According to the surface acoustic wave filter of the present invention, the ratio (Lm / Lg) between the line width Lm of the electrode fingers and the gap width Lg between the electrode fingers at the input electrode and the output electrode is 1.2 <.
Since the range of (Lm / Lg) <3 is set, the emission of the bulk wave is suppressed, the pass band characteristic is improved, and the change of the input impedance is not large, which facilitates the manufacturing.
【0010】[0010]
【実施例】以下本発明を実施例によって説明する。EXAMPLES The present invention will be described below with reference to examples.
【0011】図1は本発明の一実施例の構成を示す電極
指部分の拡大図である。FIG. 1 is an enlarged view of an electrode finger portion showing the structure of an embodiment of the present invention.
【0012】本実施例の弾性表面波フィルタは図4に示
すように多電極方式弾性表面波フィルタ10で構成して
あり、36°YカットX方向伝搬LiTaO3 基板1
と、36°YカットX方向伝搬LiTaO3 基板1上に
形成した入力電極11a、11b、11c、11d、1
1eおよび出力電極12a、12b、12c、12dと
から構成してあり、その電極指E1 、E2 、E3 、…と
電極指間の空隙G1 、G 2 、G3 、…とは図1に拡大し
て示すように、電極指Ei(i=1、2、3…)の線幅
Lmと、電極指Ei+1 と電極指Ei との間の空隙幅Lg
との比(Lm/Lg)が2.3になるように形成してあ
る。なお、図1には入力電極側を示しているが、出力電
極側も同一である。The surface acoustic wave filter of this embodiment is shown in FIG.
As shown in FIG.
Yes, 36 ° Y-cut X-direction propagation LiTaO3Board 1
And 36 ° Y cut X direction propagation LiTaO3On board 1
The formed input electrodes 11a, 11b, 11c, 11d, 1
1e and output electrodes 12a, 12b, 12c, 12d
And its electrode finger E1, E2, E3,…When
Gap between electrode fingers G1, G 2, G3, ... is enlarged in Figure 1.
, The line width of the electrode finger Ei (i = 1, 2, 3, ...)
Lm and the gap width Lg between the electrode finger Ei + 1 and the electrode finger Ei
It is formed so that the ratio (Lm / Lg) is 2.3.
It Although the input electrode side is shown in FIG.
The pole side is also the same.
【0013】上記のように構成した本実施例の多電極方
式弾性表面波フィルタ10においてはバルク波の放射が
抑えられて、電極指対数18の入力電極が7個、電極指
対数26の出力電極が6個で構成した多電極方式弾性表
面波フィルタ10の周波数特性を測定したとき図2に示
す如くであった。図2からも明らかなように周波数特性
において、周波数が高い領域において損失の増加はなく
なっている。これは図6との比較からも明らかである。In the multi-electrode surface acoustic wave filter 10 of the present embodiment constructed as described above, the emission of bulk waves is suppressed, and the number of electrode finger pairs is 18 and the number of electrode finger pairs is 7 and 26 are output electrodes. When the frequency characteristics of the multi-electrode type surface acoustic wave filter 10 composed of 6 pieces were measured, it was as shown in FIG. As is clear from FIG. 2, in the frequency characteristic, the increase in loss disappears in the high frequency region. This is also clear from the comparison with FIG.
【0014】ここで、電極指の線幅Lmと電極指間の空
隙幅Lgとの比(Lm/Lg)を変化させたときの多電
極方式弾性表面波フィルタ10の帯域内最大挿入損失は
図3に示すように凹特性を示し、電極指の線幅Lmと電
極指間の空隙幅Lgとの比(Lm/Lg)が2.3のと
きに最小であった。Here, the maximum insertion loss in the band of the multi-electrode surface acoustic wave filter 10 when the ratio (Lm / Lg) between the line width Lm of the electrode fingers and the gap width Lg between the electrode fingers is changed is shown in FIG. As shown in FIG. 3, the concave characteristics were exhibited, and it was the smallest when the ratio (Lm / Lg) of the line width Lm of the electrode fingers and the gap width Lg between the electrode fingers was 2.3.
【0015】一方、電極指の線幅Lmと電極指間の空隙
幅Lgとの比(Lm/Lg)が大きい程、バルク波の放
射が抑えられ、バルク波放射による減衰は小さくなっ
て、通過帯域特性の平坦性は保たれる。しかし、電極指
の線幅Lmと電極指間の空隙幅Lgとの比(Lm/L
g)が大きい程、電極の静電容量の変化率も大きくなっ
て、多電極方式弾性表面波フィルタ10の入力インピー
ダンスが大きく変化するため、製造上の歩留りは低下し
ていく。On the other hand, the larger the ratio (Lm / Lg) of the line width Lm of the electrode fingers to the gap width Lg between the electrode fingers is, the more the bulk wave radiation is suppressed, and the attenuation due to the bulk wave radiation is reduced, and the bulk wave radiation is reduced. The flatness of the band characteristic is maintained. However, the ratio of the line width Lm of the electrode fingers to the gap width Lg between the electrode fingers (Lm / L
The larger g), the larger the rate of change of the electrostatic capacity of the electrodes, and the larger the input impedance of the multi-electrode surface acoustic wave filter 10, and the lower the manufacturing yield.
【0016】そこで、電極指の線幅Lmと電極指間の空
隙幅Lgとの比(Lm/Lg)を、1.2<(Lm/L
g)<3の範囲としたとき周波数特性はほぼ図2と同様
であって、通過帯域特性の平坦性も保たれ、最大挿入損
失も3dB程度に抑えられ、かつ製造上の歩留りも良好
であった。Therefore, the ratio (Lm / Lg) of the line width Lm of the electrode fingers to the gap width Lg between the electrode fingers is 1.2 <(Lm / L
g) When the range is set to <3, the frequency characteristic is almost the same as that of FIG. 2, the flatness of the pass band characteristic is maintained, the maximum insertion loss is suppressed to about 3 dB, and the manufacturing yield is good. It was
【0017】なお、電極指をアポダイズ法によって重み
づけした場合も、チルト型に重みづけした場合でも同様
である。The same applies to the case where the electrode fingers are weighted by the apodization method or the tilt type.
【0018】[0018]
【発明の効果】以上説明した如く本発明によれば、36
°YカットX方向伝搬LiTaO3 を基板とし、該基板
上に入力電極と出力電極の合計が3個以上で構成された
多電極方式弾性表面波フィルタにおいて、入力電極およ
び出力電極それぞれにおける電極指の線幅Lmと電極指
間の空隙幅Lgとの比(Lm/Lg)を1.2<(Lm
/Lg)<3の範囲としたため、バルク波の放射が抑え
られ、通過帯域特性が向上する効果がある。さらに入力
インピーダンスの変化も少なくてすみ、歩留りも向上す
る効果もある。As described above, according to the present invention, 36
In a multi-electrode type surface acoustic wave filter including a Y-cut X-direction propagation LiTaO 3 as a substrate and a total of three or more input electrodes and output electrodes formed on the substrate, electrode finger of each of the input electrode and the output electrode is The ratio (Lm / Lg) of the line width Lm to the gap width Lg between the electrode fingers is 1.2 <(Lm
/ Lg) <3, so that the emission of bulk waves is suppressed and the pass band characteristic is improved. Furthermore, the change in the input impedance is small, and the yield is improved.
【図1】本発明の一実施例の構成を示す電極指部分の拡
大図である。FIG. 1 is an enlarged view of an electrode finger portion showing a configuration of an embodiment of the present invention.
【図2】本発明の一実施例にける周波数特性図である。FIG. 2 is a frequency characteristic diagram according to an embodiment of the present invention.
【図3】本発明の一実施例における電極指の線幅Lmと
電極指間の空隙幅Lgとの比(Lm/Lg)対帯域内最
大挿入損失を示す特性図図である。FIG. 3 is a characteristic diagram showing the ratio (Lm / Lg) of the line width Lm of the electrode finger to the gap width Lg between the electrode fingers and the maximum insertion loss in the band in one embodiment of the present invention.
【図4】多電極方式弾性表面波フィルタの構成を示す模
式図である。FIG. 4 is a schematic diagram showing a configuration of a multi-electrode surface acoustic wave filter.
【図5】従来例における電極指部分の拡大図である。FIG. 5 is an enlarged view of an electrode finger portion in a conventional example.
【図6】従来例における周波数特性図である。FIG. 6 is a frequency characteristic diagram in a conventional example.
1…36°YカットX方向伝搬LiTaO3 基板 10…多電極方式弾性表面波フィルタ 11a〜11e…入力電極 12a〜12d…出力電極1 ... 36 ° Y-cut X-direction propagation LiTaO 3 substrate 10 ... Multi-electrode type surface acoustic wave filter 11a-11e ... Input electrode 12a-12d ... Output electrode
Claims (1)
基板とし、該基板上に入力電極と出力電極の合計が3個
以上で構成された多電極方式弾性表面波フィルタにおい
て、入力電極および出力電極それぞれにおける電極指の
線幅Lmと電極指間の空隙幅Lgとの比(Lm/Lg)
を1.2<(Lm/Lg)<3の範囲としたことを特徴
とする弾性表面波フィルタ。1. A multi-electrode type surface acoustic wave filter comprising a 36 ° Y-cut X-direction propagation LiTaO 3 as a substrate, and a total of three or more input electrodes and output electrodes on the substrate. Ratio (Lm / Lg) of the line width Lm of the electrode fingers and the gap width Lg between the electrode fingers in each electrode
In the range of 1.2 <(Lm / Lg) <3.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP4048450A JPH0828642B2 (en) | 1992-03-05 | 1992-03-05 | Surface acoustic wave filter |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP4048450A JPH0828642B2 (en) | 1992-03-05 | 1992-03-05 | Surface acoustic wave filter |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH05251982A true JPH05251982A (en) | 1993-09-28 |
JPH0828642B2 JPH0828642B2 (en) | 1996-03-21 |
Family
ID=12803688
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP4048450A Expired - Fee Related JPH0828642B2 (en) | 1992-03-05 | 1992-03-05 | Surface acoustic wave filter |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0828642B2 (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5420472A (en) * | 1992-06-11 | 1995-05-30 | Motorola, Inc. | Method and apparatus for thermal coefficient of expansion matched substrate attachment |
WO2001037426A1 (en) * | 1999-11-16 | 2001-05-25 | Mitsubishi Denki Kabushiki Kaisha | Elastic wave device |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS564913A (en) * | 1979-06-27 | 1981-01-19 | Nec Corp | Elastic surface wave transducer |
-
1992
- 1992-03-05 JP JP4048450A patent/JPH0828642B2/en not_active Expired - Fee Related
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS564913A (en) * | 1979-06-27 | 1981-01-19 | Nec Corp | Elastic surface wave transducer |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5420472A (en) * | 1992-06-11 | 1995-05-30 | Motorola, Inc. | Method and apparatus for thermal coefficient of expansion matched substrate attachment |
WO2001037426A1 (en) * | 1999-11-16 | 2001-05-25 | Mitsubishi Denki Kabushiki Kaisha | Elastic wave device |
US6674215B1 (en) | 1999-11-16 | 2004-01-06 | Mitsubishi Denki Kabushiki Kaisha | Elastic wave device |
Also Published As
Publication number | Publication date |
---|---|
JPH0828642B2 (en) | 1996-03-21 |
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