JPH09181554A - Surface acoustic wave device - Google Patents
Surface acoustic wave deviceInfo
- Publication number
- JPH09181554A JPH09181554A JP33944995A JP33944995A JPH09181554A JP H09181554 A JPH09181554 A JP H09181554A JP 33944995 A JP33944995 A JP 33944995A JP 33944995 A JP33944995 A JP 33944995A JP H09181554 A JPH09181554 A JP H09181554A
- Authority
- JP
- Japan
- Prior art keywords
- surface acoustic
- acoustic wave
- electrodes
- wave device
- electrode
- 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 70
- 239000000758 substrate Substances 0.000 claims abstract description 11
- 230000001902 propagating effect Effects 0.000 claims description 2
- 230000004048 modification Effects 0.000 description 14
- 238000012986 modification Methods 0.000 description 14
- WSMQKESQZFQMFW-UHFFFAOYSA-N 5-methyl-pyrazole-3-carboxylic acid Chemical compound CC1=CC(C(O)=O)=NN1 WSMQKESQZFQMFW-UHFFFAOYSA-N 0.000 description 1
- 229910013641 LiNbO 3 Inorganic materials 0.000 description 1
- 238000013459 approach Methods 0.000 description 1
- 238000006243 chemical reaction Methods 0.000 description 1
- 239000004020 conductor Substances 0.000 description 1
- GQYHUHYESMUTHG-UHFFFAOYSA-N lithium niobate Chemical compound [Li+].[O-][Nb](=O)=O GQYHUHYESMUTHG-UHFFFAOYSA-N 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 230000000644 propagated effect Effects 0.000 description 1
- 239000010453 quartz Substances 0.000 description 1
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N silicon dioxide Inorganic materials O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 1
Landscapes
- Surface Acoustic Wave Elements And Circuit Networks Thereof (AREA)
Abstract
Description
【0001】[0001]
【発明が属する技術分野】本発明は、フィルタとして利
用されるのに適した弾性表面波装置に係り、特に圧電基
板上に設けた櫛歯状の入力電極及び出力電極を傾斜電極
で構成した弾性表面波装置に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a surface acoustic wave device suitable for use as a filter, and in particular, an elastic device in which comb-teeth-shaped input electrodes and output electrodes provided on a piezoelectric substrate are composed of inclined electrodes. The present invention relates to a surface wave device.
【0002】[0002]
【従来の技術】従来、この種の装置は、図9(A)
(B)に示すように、厚さの薄い直方体状に成形した圧
電基板10上に弾性表面波が伝搬する方向に並設させた
櫛歯状の入力電極11及び出力電極12を有し、前記両
電極11,12の各複数の電極指をそれぞれ所定の曲率
係数P(パワーファクタPともいう)で傾斜させるよう
にしている。そして、各電極11,12における弾性表
面波の伝搬方向両端間の各中央位置を電極指の延設方向
に沿ってつなげた各線(中心線L1,L2)が互いに平行
になるように両電極11,12を配置するとともに、両
電極11,12を前記中心線L1,L2に対してそれぞれ
対称になるように構成している。2. Description of the Related Art Conventionally, this type of device is shown in FIG.
As shown in (B), a piezoelectric substrate 10 formed in a thin rectangular parallelepiped shape has comb-teeth-shaped input electrodes 11 and output electrodes 12 arranged in parallel in a direction in which a surface acoustic wave propagates. The plurality of electrode fingers of both electrodes 11 and 12 are respectively inclined with a predetermined curvature coefficient P (also referred to as power factor P). Then, both electrodes 11 and 12 are arranged such that lines (center lines L1 and L2) connecting center positions between both ends of the surface acoustic wave propagation direction of the electrodes 11 and 12 along the extending direction of the electrode fingers are parallel to each other. , 12 are arranged, and both electrodes 11, 12 are configured to be symmetrical with respect to the center lines L1, L2.
【0003】[0003]
【発明が解決しようとする課題】しかし、上記従来の弾
性表面波装置では、弾性表面波の回折現象、ビームの偏
り(ビームステアリリング)などの影響で、図9(C)
に示すように、群遅延特性における群遅延時間が周波数
が高くなるにしたがって長くなり、所望の群遅延特性を
有する弾性表面波装置を製造することが難しいという問
題があった。通常、この群遅延特性は周波数の変化に対
して群遅延時間がフラットであることが望ましい。However, in the above-described conventional surface acoustic wave device, the surface acoustic wave diffraction phenomenon, the beam deviation (beam steering), etc. cause the influence of FIG.
As shown in, the group delay time in the group delay characteristic becomes longer as the frequency becomes higher, and there is a problem that it is difficult to manufacture a surface acoustic wave device having a desired group delay characteristic. Usually, it is desirable that the group delay characteristic has a flat group delay time with respect to a change in frequency.
【0004】本発明は上記問題を解決するためになされ
たもので、その目的は所望の群遅延特性を得ることがで
きる弾性表面波装置を提供することにある。The present invention has been made to solve the above problems, and an object thereof is to provide a surface acoustic wave device capable of obtaining a desired group delay characteristic.
【0005】[0005]
【課題を解決するための手段】上記目的を達成するため
に、本発明の構成上の特徴は、入力及び出力電極を傾斜
電極で構成し、各電極における弾性表面波の伝搬方向両
端間の各中央位置を電極指の延設方向に沿ってつなげた
各線が互いに平行にならないように両電極を配置したこ
とにある。In order to achieve the above-mentioned object, a structural feature of the present invention is that the input and output electrodes are composed of inclined electrodes, and each electrode has a surface acoustic wave propagating direction between both ends. Both electrodes are arranged so that the lines connecting the central positions along the extending direction of the electrode fingers are not parallel to each other.
【0006】この場合、例えば、前記各電極における弾
性表面波の伝搬方向両端間の各中央位置を電極指の延設
方向に沿ってつなげた各線が直線になり、かつ同各線間
の一端側の距離が各他端側の距離より短くなるように両
電極を構成したり、同各線が曲線になるように両電極を
構成したりするとよい。In this case, for example, each line connecting the central positions between both ends in the propagation direction of the surface acoustic wave in each electrode along the extending direction of the electrode fingers is a straight line, and one end side between the respective lines is connected. It is preferable to configure both electrodes so that the distance is shorter than the distance on the other end side, or to configure both electrodes so that each line is a curve.
【0007】[0007]
【発明の作用及び効果】上記のように構成した弾性表面
波装置においては、各電極における弾性表面波の伝搬方
向両端間の各中央位置を電極指の延設方向に沿ってつな
げた各線が互いに平行でないので、入力電極にて電気信
号から変換された弾性表面波が出力電極に到達するまで
の時間は前記中央位置をつなげた各線に沿った位置に応
じて異なる。一方、傾斜電極においては、一般的に入力
電極にて弾性表面波に変換されかつ出力電極にて電気信
号に再変換される信号の周波数は前記中央位置をつなげ
た各線に沿った位置に応じて決定されるので、前記到達
時間の相違は伝搬される信号の周波数に応じて変更され
ることになる。したがって、入力電極における前記中央
位置をつなげた線と出力電極における前記中央位置をつ
なげた線とがなす角度(0度を除く)を適宜設定するこ
とにより、群遅延時間が信号の周波数の変化に対してフ
ラットになる群遅延特性を有する弾性表面波装置を実現
したり、群遅延時間が信号の周波数の変化に対して任意
に変化する弾性表面波装置を実現できる。その結果、本
発明によれば、所望の群遅延特性を有する弾性表面波装
置を簡単に製造できるようになる。In the surface acoustic wave device configured as described above, the respective lines connecting the respective central positions between both ends of the surface acoustic wave in the respective electrodes in the propagation direction of the electrodes are connected to each other along the extending direction of the electrode fingers. Since they are not parallel, the time until the surface acoustic wave converted from the electric signal at the input electrode reaches the output electrode differs depending on the position along each line connecting the central positions. On the other hand, in the inclined electrode, the frequency of the signal generally converted into the surface acoustic wave at the input electrode and reconverted into the electric signal at the output electrode depends on the position along each line connecting the central positions. Since it is determined, the difference in arrival times will change depending on the frequency of the propagated signal. Therefore, by appropriately setting the angle (excluding 0 degrees) formed by the line connecting the central positions of the input electrodes and the line connecting the central positions of the output electrodes, the group delay time can be changed to the frequency of the signal. On the other hand, it is possible to realize a surface acoustic wave device having a group delay characteristic that becomes flat, or a surface acoustic wave device in which the group delay time arbitrarily changes in response to a change in signal frequency. As a result, according to the present invention, a surface acoustic wave device having a desired group delay characteristic can be easily manufactured.
【0008】[0008]
【発明の実施の形態】以下、本発明の一実施形態を図面
を用いて説明すると、図1(A)は同実施形態に係る弾
性表面波装置を平面図により概略的に示している。BEST MODE FOR CARRYING OUT THE INVENTION An embodiment of the present invention will be described below with reference to the drawings. FIG. 1 (A) schematically shows a surface acoustic wave device according to the embodiment in a plan view.
【0009】この弾性表面波装置は、ニオブ酸リチウム
(LiNbO3)、タンタル酸リチウム(LiTaO3)、水晶など
の圧電材料で厚さの薄い直方体状に形成した圧電基板2
0を備えている。圧電基板20上には、入力電極30及
び出力電極40が並設されていて、入力電極30により
電気信号が弾性表面波に変換され、同変換された弾性表
面波が圧電基板20上を図示矢印方向に伝搬して出力電
極40に到達し、かつ同到達した弾性表面波が出力電極
40にてふたたび電気信号に変換されるようになってい
る。This surface acoustic wave device comprises a piezoelectric substrate 2 formed of a piezoelectric material such as lithium niobate (LiNbO 3 ), lithium tantalate (LiTaO 3 ), and quartz in a thin rectangular parallelepiped shape.
0 is provided. An input electrode 30 and an output electrode 40 are arranged side by side on the piezoelectric substrate 20, an electric signal is converted into a surface acoustic wave by the input electrode 30, and the converted surface acoustic wave is shown on the piezoelectric substrate 20 by an arrow. The surface acoustic wave propagates in the direction and reaches the output electrode 40, and the surface acoustic wave reaching the output electrode 40 is converted into an electric signal again at the output electrode 40.
【0010】入力電極30は、圧電基板20上の図示左
側部分にて、弾性表面波の伝搬方向に平行かつ相対向し
て延設された一対の帯状の導電体で構成した連結部3
1,32を備えている。連結部31は連結部32よりも
短く構成されている。連結部31,32には、連結部3
1から連結部32に向かうにしたがって電極指間距離が
長くなるように所定の曲率係数をもって曲線的に傾斜さ
せた複数の電極指33,34の各一端がそれぞれ接続さ
れ、各電極指33,34は交差長を異ならせて互いに交
差している。連結部31,32及び電極指33,34の
弾性表面波の伝搬方向両端間の中央位置を電極指33,
34の延設方向に沿ってつなげた線(以下、単に入力電
極30の中心線L1という)は、連結部31,32の延
設方向と直角な直線L10(以下、単に基準線L10とい
う)に対して、連結部31の中央位置が出力電極40に
近づきかつ連結部32の中央位置が出力電極40から遠
ざかる方向に傾いている。そして、入力電極30は、中
心線L1に対しても基準線L10に対しても非対称に形成
されている。なお、この場合、中心線L1は直線であ
る。The input electrode 30 is formed on the left side of the piezoelectric substrate 20 in the drawing by a connecting portion 3 formed of a pair of strip-shaped conductors extending parallel to and facing each other in the propagation direction of the surface acoustic wave.
1 and 32 are provided. The connecting portion 31 is configured to be shorter than the connecting portion 32. The connecting portion 3 is connected to the connecting portions 31 and 32.
One end of each of a plurality of electrode fingers 33, 34 that are curvedly curved with a predetermined curvature coefficient so that the distance between the electrode fingers becomes longer from 1 toward the connecting portion 32, is connected to each electrode finger 33, 34. Intersect with each other with different lengths of intersection. The center position between the ends of the connecting portions 31, 32 and the electrode fingers 33, 34 in the surface acoustic wave propagation direction is set to the electrode finger 33,
A line connected along the extending direction of 34 (hereinafter, simply referred to as a center line L1 of the input electrode 30) is a straight line L10 (hereinafter simply referred to as a reference line L10) perpendicular to the extending direction of the connecting portions 31 and 32. On the other hand, the central position of the connecting portion 31 approaches the output electrode 40 and the central position of the connecting portion 32 is inclined in a direction away from the output electrode 40. The input electrode 30 is formed asymmetrically with respect to the center line L1 and the reference line L10. In this case, the center line L1 is a straight line.
【0011】出力電極40も、圧電基板20の図示右側
上面にて、入力電極30と同様な連結部41,42及び
電極指43,44により構成されている。連結部41,
42及び電極指43,44の弾性表面波の伝搬方向両端
間の中央位置を電極指43,44の延設方向に沿ってつ
なげた線(以下、単に出力電極40の中心線L2とい
う)は、連結部41,42の延設方向と直角な直線L20
(以下、単に基準線L20という)に対して、連結部41
の中央位置が入力電極30に近づきかつ連結部42の中
央位置が出力電極30から遠ざかる方向に傾いている。
そして、出力電極40は、中心線L2に対しても基準線
L20に対しても非対称に形成されている。なお、この場
合も、中心線L2は直線である。The output electrode 40 is also composed of connecting portions 41, 42 and electrode fingers 43, 44 similar to the input electrode 30 on the upper surface of the piezoelectric substrate 20 on the right side in the drawing. Connection part 41,
A line connecting the central positions of the electrode 42 and the electrode fingers 43 and 44 in the propagation direction of the surface acoustic wave along the extending direction of the electrode fingers 43 and 44 (hereinafter, simply referred to as the center line L2 of the output electrode 40) is Straight line L20 perpendicular to the extending direction of the connecting portions 41 and 42
With respect to (hereinafter, simply referred to as reference line L20), the connecting portion 41
Is closer to the input electrode 30 and the central position of the connecting portion 42 is inclined in a direction away from the output electrode 30.
The output electrode 40 is formed asymmetrically with respect to the center line L2 and the reference line L20. In this case as well, the center line L2 is a straight line.
【0012】上記のように構成した弾性表面波装置にお
いては、入力電極30にて電気信号から変換された弾性
表面波は圧電基板20上を伝搬して出力電極40に到達
し、同出力電極40にて電気信号に再変換される。この
信号の変換においては、電極指間距離が連結部31,4
1から連結部32,42に向かうにしたがって長くなっ
ているので、入力電極30にて弾性表面波に変換されか
つ出力電極40にて電気信号に再変換される信号の周波
数は、連結部31,41から連結部32,42に向かう
にしたがって低くなる。一方、両電極30,40の各中
心線L1,L2は互いに平行でなく、同中心線L1,L2間
の距離は連結部31,41側にて連結部32,42側よ
りも短いので、入力電極30にて変換された弾性表面波
が出力電極40に到達するまでの時間は、連結部31,
41から連結部32,42に向かうにしたがって長くな
る。その結果、この弾性表面波装置の群遅延特性におけ
る群遅延時間は、信号周波数が低くなるにしたがって長
くなる側に補正されることになる。In the surface acoustic wave device configured as described above, the surface acoustic wave converted from the electric signal in the input electrode 30 propagates on the piezoelectric substrate 20 and reaches the output electrode 40, and the output electrode 40. Is converted back into an electrical signal at. In the conversion of this signal, the distance between the electrode fingers depends on the connecting portions 31, 4
Since it becomes longer from 1 toward the connecting portions 32, 42, the frequency of the signal converted into the surface acoustic wave at the input electrode 30 and re-converted into the electric signal at the output electrode 40 is equal to the connecting portion 31, It becomes lower from 41 toward the connecting portions 32 and 42. On the other hand, the center lines L1 and L2 of the electrodes 30 and 40 are not parallel to each other, and the distance between the center lines L1 and L2 is shorter on the side of the connecting portions 31 and 41 than on the side of the connecting portions 32 and 42. The time required for the surface acoustic waves converted by the electrode 30 to reach the output electrode 40 is
It becomes longer from 41 toward the connecting portions 32 and 42. As a result, the group delay time in the group delay characteristic of this surface acoustic wave device is corrected to become longer as the signal frequency becomes lower.
【0013】したがって、中心線L1,L2間の距離が連
結部31,41側にて短くなるように同中心線L1,L2
を基準線L10,L20に対して適宜角度だけ傾けることに
より、すなわち中心線L1と中心線L2とがなす角度(0
度以外)を適宜設定することにより、図9(C)に示し
た群遅延特性における低い周波数に対応した群遅延時間
を長くするとともに高い周波数に対応した群遅延時間を
短くするように補正でき、群遅延時間が周波数の変化に
対してフラットになる図1(B)に示すような群遅延特
性を実現できる。Therefore, the center lines L1 and L2 are so arranged that the distance between the center lines L1 and L2 becomes shorter on the connecting portions 31 and 41 side.
Is inclined with respect to the reference lines L10 and L20 by an appropriate angle, that is, the angle (0 between the center line L1 and the center line L2).
By appropriately setting (except the degree), the group delay time corresponding to the low frequency in the group delay characteristic shown in FIG. 9 (C) can be corrected to be long and the group delay time corresponding to the high frequency can be shortened. It is possible to realize a group delay characteristic as shown in FIG. 1B in which the group delay time becomes flat with respect to a change in frequency.
【0014】また、上記実施形態においては、両電極3
0,40の両中心線L1,L2間の距離が連結部31,4
1側にて短くなるように両中心線L1,L2を基準線L1
0,L20に対して互いに異なる方向にそれぞれ傾けるよ
うにしたが、図2(A)に示すように、出力電極40の
中心線L2を基準線L20に対して傾けないで、入力電極
30の中心線L1のみを基準線L10に対して連結部31
側にて出力電極40の中心線L2に近づく側に傾けて、
両中心線L1,L2間の距離が連結部31,41側にて短
くなるようにしてもよい。逆に、入力電極30の中心線
L1を基準線L10に対して傾けないで、出力電極40の
中心線L2のみを基準線L20に対して連結部41側にて
入力電極30の中心線L1に近づく側に傾けて、両中心
線L1,L2間の距離が連結部31,41側にて短くなる
ようにしてもよい。In the above embodiment, both electrodes 3
The distance between the center lines L1 and L2 of 0 and 40 is the connecting portion 31 and 4
Set both center lines L1 and L2 to the reference line L1 so that
Although it is arranged to incline in directions different from each other with respect to 0 and L20, as shown in FIG. 2A, the center line L2 of the output electrode 40 is not inclined with respect to the reference line L20, and the center of the input electrode 30 is Only the line L1 is connected to the reference line L10 by the connecting portion 31.
Tilt toward the side closer to the center line L2 of the output electrode 40,
The distance between the center lines L1 and L2 may be shortened on the connecting portions 31 and 41 side. On the contrary, the center line L1 of the input electrode 30 is not inclined with respect to the reference line L10, and only the center line L2 of the output electrode 40 is connected to the center line L1 of the input electrode 30 at the connecting portion 41 side with respect to the reference line L20. The distance between the center lines L1 and L2 may be shortened on the side of the connecting portions 31 and 41 by inclining toward the approaching side.
【0015】さらに、図2(B)に示すように、両電極
30,40の両中心線L1,L2を両基準線L10,L20に
対して同一方向に傾けるとともに、一方の中心線L1又
はL2の傾きを大きくして、両中心線L1,L2間の距離
が連結部31,41側にて短くなるようにしてもよい。
なお、これらの図2(A)(B)の場合にも、各連結部
31,32,41,42は弾性表面波の伝搬方向に平行
に延設されている。Further, as shown in FIG. 2B, both center lines L1 and L2 of both electrodes 30 and 40 are tilted in the same direction with respect to both reference lines L10 and L20, and one center line L1 or L2. May be increased so that the distance between the center lines L1 and L2 becomes shorter on the connecting portions 31 and 41 side.
2A and 2B, the connecting portions 31, 32, 41, 42 extend in parallel with the surface acoustic wave propagation direction.
【0016】このように上記実施形態を変形しても、中
心線L1と中心線L2とがなす角度(0度以外)を適宜設
定することにより、図9(C)に示した群遅延特性にお
ける低い周波数に対応した群遅延時間を長くするととも
に高い周波数に対応した群遅延時間を短くするように補
正でき、群遅延時間が周波数の変化に対してフラットに
なる図1(B)に示すような群遅延特性を実現できる。Even if the above embodiment is modified as described above, the angle (other than 0 degree) formed by the center line L1 and the center line L2 is appropriately set to obtain the group delay characteristic shown in FIG. 9C. As shown in FIG. 1B, the group delay time corresponding to the low frequency can be corrected to be long and the group delay time corresponding to the high frequency can be corrected to be short, and the group delay time becomes flat with respect to the frequency change. Group delay characteristics can be realized.
【0017】次に、上記実施形態の他の変形例について
説明すると、図3(A)は同変形例に係る弾性表面波装
置を平面図により概略的に示している。この場合も、両
電極30,40の両中心線L1,L2間の距離が連結部3
1,41側にて短くなるように両中心線L1,L2を基準
線L10,L20に対して互いに異なる方向に傾けてある
が、両中心線L1,L2がなす角度を上記図1(A)の場
合よりも大きくする。したがって、この場合には、低い
周波数に対する群遅延時間がより長くなり、かつ高い周
波数に対する群遅延時間がより短くなるので、この弾性
表面波装置の群遅延特性は図3(B)に示すようにな
る。また、この場合も、上記実施形態の図2(A)
(B)に示すような変形例と同様に、両電極30,40
の中心線L1,L2のうちの一方のみを傾けたり、両方を
同一方向に傾けるようにしてもよい。Next, another modified example of the above embodiment will be described. FIG. 3A schematically shows a surface acoustic wave device according to the modified example in a plan view. Also in this case, the distance between the center lines L1 and L2 of both electrodes 30 and 40 is determined by the connecting portion 3
The center lines L1 and L2 are inclined in directions different from each other with respect to the reference lines L10 and L20 so that the center lines L1 and L2 are shortened on the 1st and 41th sides. Larger than the case. Therefore, in this case, the group delay time for a low frequency becomes longer and the group delay time for a higher frequency becomes shorter, so that the group delay characteristic of this surface acoustic wave device is as shown in FIG. Become. Also in this case, FIG. 2A of the above embodiment is also used.
In the same manner as in the modified example shown in (B), both electrodes 30, 40
One of the center lines L1 and L2 may be tilted, or both may be tilted in the same direction.
【0018】また、他の変形例は、図4(A)に示すよ
うに、両電極30,40の両中心線L1,L2間の距離が
連結部32,42側にて短くなるように両中心線L1,
L2を基準線L10,L20に対して互いに異なる方向に傾
けてある。これによれば、前記場合と逆に低い周波数に
対する群遅延時間が短くなり、かつ高い周波数に対する
群遅延時間が長くなるので、この弾性表面波装置の群遅
延特性は図4(B)に示すようになる。また、この場合
も、上記実施形態の図2(A)(B)に示すような変形
例と同様に、両電極30,40の中心線L1,L2のうち
の一方のみを傾けたり、両方を同一方向に傾けるように
してもよい。In another modification, as shown in FIG. 4 (A), the distance between the center lines L1 and L2 of both electrodes 30 and 40 is shortened on the connecting portions 32 and 42 side. Center line L1,
L2 is tilted in directions different from each other with respect to the reference lines L10 and L20. According to this, contrary to the above case, the group delay time for low frequencies becomes short and the group delay time for high frequencies becomes long, so the group delay characteristic of this surface acoustic wave device is as shown in FIG. 4 (B). become. Also in this case, similarly to the modification of the above-described embodiment as shown in FIGS. 2A and 2B, only one of the center lines L1 and L2 of both electrodes 30 and 40 may be inclined, or both of them may be inclined. You may make it incline in the same direction.
【0019】また、前述した各例では中心線L1,L2は
直線であったが、これらの中心線L1,L2を曲線にした
変形例について次に説明する。この種の変形例は、図5
(A)に示すように、両電極30,40の両中心線L
1,L2が曲線になるように両電極30,40を構成す
る。そして、両中心線L1,L2間の距離が連結部31,
41側及び連結部32,42側にて短くなるとともに、
連結部31,41と連結部32,42との各中央位置に
て長くなるように、両中心線L1,L2を基準線L10,L
20に対して互いに異なる方向に曲げてある。これによれ
ば、低域及び高域の周波数に対する群遅延時間が短くな
り、かつ中域の周波数に対する群遅延時間が長くなるの
で、この弾性表面波装置の群遅延特性は図5(B)に示
すようになる。Although the center lines L1 and L2 are straight lines in each of the above-mentioned examples, a modification in which the center lines L1 and L2 are curved will be described below. This kind of modification is shown in FIG.
As shown in (A), both center lines L of both electrodes 30 and 40
Both electrodes 30, 40 are constructed so that 1 and L2 are curved. The distance between the center lines L1 and L2 is the connecting portion 31,
41 side and connecting parts 32, 42 side is shortened,
The center lines L1 and L2 are set so as to be long at the central positions of the connecting portions 31 and 41 and the connecting portions 32 and 42, respectively.
Bent in different directions with respect to 20. According to this, the group delay time for the low frequency band and the high frequency band becomes short, and the group delay time for the middle frequency band becomes long. Therefore, the group delay characteristic of this surface acoustic wave device is shown in FIG. As shown.
【0020】さらに、他の変形例も、図6(A)に示す
ように、両電極30,40の両中心線L1,L2が曲線に
なるように両電極30,40を構成する。そして、両中
心線L1,L2間の距離が連結部31,41側及び連結部
32,42側にて長くなるとともに、連結部31,41
と連結部32,42との各中央位置にて短くなるよう
に、両中心線L1,L2を基準線L10,L20に対して互い
に異なる方向に曲げてある。これによれば、低域及び高
域の周波数に対する群遅延時間が長くなり、かつ中域の
周波数に対する群遅延時間が短くなるので、この弾性表
面波装置の群遅延特性は図6(B)に示すようになる。Further, in another modification, as shown in FIG. 6 (A), both electrodes 30, 40 are constructed such that both center lines L1, L2 of both electrodes 30, 40 are curved. The distance between the center lines L1 and L2 becomes longer on the side of the connecting portions 31 and 41 and on the side of the connecting portions 32 and 42, and the connecting portions 31 and 41 are
The center lines L1 and L2 are bent in directions different from each other with respect to the reference lines L10 and L20 so that the center lines L1 and L2 are shortened at the central positions of the connecting portions 32 and 42. According to this, the group delay time for the low frequency band and the high frequency band becomes long, and the group delay time for the middle frequency band becomes short. Therefore, the group delay characteristic of this surface acoustic wave device is shown in FIG. 6 (B). As shown.
【0021】これらの図4〜6の各(A)に示した弾性
表面波装置は、上記実施形態に示したように、群遅延時
間が周波数の変化に対してフラットになるものではない
が、特異な周波数特性を必要とするフィルタなどに利用
される。そして、このように中心線L1,L2を直線にす
るとともにそれらの傾きを変えたり、曲線にするととも
にその曲率を変えたりすることにより、任意の群遅延特
性特性を有する弾性表面波装置を製造できる。The surface acoustic wave device shown in each of FIGS. 4 to 6A does not have a flat group delay time with respect to a change in frequency, as shown in the above embodiment, It is used for filters that require unique frequency characteristics. By thus making the center lines L1 and L2 straight and changing their inclinations, or making them curved and changing their curvatures, a surface acoustic wave device having an arbitrary group delay characteristic can be manufactured. .
【0022】また、上記実施形態及び各種変形例におい
ては、電極指33,34,43,44を曲線にするとと
もに重み付けして両電極30,40を傾斜電極で構成し
た弾性表面波装置について説明したが、本発明は、図7
(A)に示すように電極指33,34,43,44を直
線にするとともに重み付けするように構成したり、図7
(B)(C)に示すように電極指33,34,43,4
4を曲線にするとともに重み付けしないように構成した
り、図7(D)に示すように電極指33,34,43,
44を直線にするとともに重み付けしないように構成し
た両電極30,40を有する弾性表面波装置にも適用で
きる。さらに、図8に示すように電極指33,34,4
3,44をダブルに構成した両電極30,40を有する
弾性表面波装置にも適用できる。Further, in the above-described embodiment and various modifications, the surface acoustic wave device in which the electrode fingers 33, 34, 43 and 44 are curved and weighted so that both electrodes 30 and 40 are inclined electrodes has been described. However, the present invention is shown in FIG.
As shown in FIG. 7A, the electrode fingers 33, 34, 43, 44 may be configured to be linear and weighted, or as shown in FIG.
(B) As shown in (C), electrode fingers 33, 34, 43, 4
4 is curved and is not weighted, or as shown in FIG. 7D, the electrode fingers 33, 34, 43,
The present invention can also be applied to a surface acoustic wave device having both electrodes 30 and 40 in which 44 is linear and is not weighted. Further, as shown in FIG. 8, electrode fingers 33, 34, 4
It can also be applied to a surface acoustic wave device having both electrodes 30, 40 in which 3, 44 are doubled.
【図1】 (A)は本発明の一実施形態を示す弾性表面
波装置の平面概略図であり、(B)は同弾性表面波装置
の群遅延特性を示すグラフである。FIG. 1A is a schematic plan view of a surface acoustic wave device showing an embodiment of the present invention, and FIG. 1B is a graph showing a group delay characteristic of the surface acoustic wave device.
【図2】 (A)は上記実施形態の変形例を示す弾性表
面波装置の平面概略図であり、(B)は同実施形態の他
の変形例を示す弾性表面波装置の平面概略図である。FIG. 2A is a schematic plan view of a surface acoustic wave device showing a modified example of the above embodiment, and FIG. 2B is a schematic plan view of a surface acoustic wave device showing another modified example of the same embodiment. is there.
【図3】 (A)は本発明の上記実施形態の他の変形例
を示す弾性表面波装置の平面概略図であり、(B)は同
他の変形例に係る弾性表面波装置の群遅延特性を示すグ
ラフである。FIG. 3A is a schematic plan view of a surface acoustic wave device showing another modification of the embodiment of the present invention, and FIG. 3B is a group delay of the surface acoustic wave device according to the other modification. It is a graph which shows a characteristic.
【図4】 (A)は本発明の上記実施形態の他の変形例
を示す弾性表面波装置の平面概略図であり、(B)は同
他の変形例に係る弾性表面波装置の群遅延特性を示すグ
ラフである。FIG. 4A is a schematic plan view of a surface acoustic wave device showing another modification of the embodiment of the present invention, and FIG. 4B is a group delay of the surface acoustic wave device according to the other modification. It is a graph which shows a characteristic.
【図5】 (A)は本発明の上記実施形態の他の変形例
を示す弾性表面波装置の平面概略図であり、(B)は同
他の変形例に係る弾性表面波装置の群遅延特性を示すグ
ラフである。FIG. 5A is a schematic plan view of a surface acoustic wave device showing another modification of the above-described embodiment of the present invention, and FIG. 5B is a group delay of the surface acoustic wave device according to the other modification. It is a graph which shows a characteristic.
【図6】 (A)は本発明の上記実施形態の他の変形例
を示す弾性表面波装置の平面概略図であり、(B)は同
他の変形例に係る弾性表面波装置の群遅延特性を示すグ
ラフである。FIG. 6A is a schematic plan view of a surface acoustic wave device showing another modification of the above-described embodiment of the present invention, and FIG. 6B is a group delay of the surface acoustic wave device according to the other modification. It is a graph which shows a characteristic.
【図7】 (A)〜(D)は本発明の他の適用例に係る
弾性表面波装置の平面概略図である。7A to 7D are schematic plan views of a surface acoustic wave device according to another application example of the present invention.
【図8】 本発明の他の適用例に係る弾性表面波装置の
平面概略図である。FIG. 8 is a schematic plan view of a surface acoustic wave device according to another application example of the present invention.
【図9】 (A)(B)は共に従来の弾性表面波装置の
平面概略図であり、(C)は同弾性表面波装置の群遅延
特性を示すグラフである。9A and 9B are schematic plan views of a conventional surface acoustic wave device, and FIG. 9C is a graph showing group delay characteristics of the surface acoustic wave device.
20…圧電基板、30…入力電極、31,32…連結
部、33,34…電極指、40…出力電極、41,42
…連結部、43,44…電極指、L1,L2…中心線、L1
0,L20…基準線。20 ... Piezoelectric substrate, 30 ... Input electrodes, 31, 32 ... Connection parts, 33, 34 ... Electrode fingers, 40 ... Output electrodes, 41, 42
... Connection parts, 43, 44 ... Electrode fingers, L1, L2 ... Center line, L1
0, L20 ... Reference line.
Claims (3)
櫛歯状の入力電極及び出力電極を並設するとともに、前
記両電極を傾斜電極で構成した弾性表面波装置におい
て、前記各電極における弾性表面波の伝搬方向両端間の
各中央位置を電極指の延設方向に沿ってつなげた各線が
互いに平行にならないように前記両電極を配置したこと
を特徴とする弾性表面波装置。1. A surface acoustic wave device in which comb-teeth-shaped input electrodes and output electrodes are arranged in parallel on a piezoelectric substrate in a propagation direction of surface acoustic waves, and both electrodes are inclined electrodes. In the surface acoustic wave device, the electrodes are arranged so that the lines connecting the central positions between both ends of the surface acoustic wave in the propagation direction along the extending direction of the electrode fingers are not parallel to each other.
向両端間の各中央位置を電極指の延設方向に沿ってつな
げた各線が直線になり、かつ同各線間の一端側の距離が
各多端側の距離より短くなるように前記両電極を構成し
たことを特徴とする前記請求項1に記載の弾性表面波装
置。2. The lines connecting the respective central positions between both ends of the surface acoustic wave propagation direction of the respective electrodes along the extending direction of the electrode fingers are straight lines, and the distance between the respective lines on one end side is The surface acoustic wave device according to claim 1, wherein the both electrodes are configured to be shorter than the distance on the multi-end side.
向両端間の各中央位置を電極指の延設方向に沿ってつな
げた各線が曲線になるように前記両電極を構成したこと
を特徴とする前記請求項1に記載の弾性表面波装置。3. The electrodes are configured such that each line connecting the central positions between both ends of the surface acoustic wave propagating direction in each electrode along the extending direction of the electrode fingers is a curve. The surface acoustic wave device according to claim 1.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP33944995A JPH09181554A (en) | 1995-12-26 | 1995-12-26 | Surface acoustic wave device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP33944995A JPH09181554A (en) | 1995-12-26 | 1995-12-26 | Surface acoustic wave device |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH09181554A true JPH09181554A (en) | 1997-07-11 |
Family
ID=18327575
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP33944995A Pending JPH09181554A (en) | 1995-12-26 | 1995-12-26 | Surface acoustic wave device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH09181554A (en) |
Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US7400218B2 (en) | 2003-11-12 | 2008-07-15 | Murata Manufacturing Co., Ltd. | Surface acoustic wave filter |
| JP2013223178A (en) * | 2012-04-18 | 2013-10-28 | Nippon Dempa Kogyo Co Ltd | Acoustic wave filter |
| WO2024029360A1 (en) * | 2022-08-04 | 2024-02-08 | 株式会社村田製作所 | Elastic wave device and filter device |
| WO2024116813A1 (en) * | 2022-11-28 | 2024-06-06 | 株式会社村田製作所 | Elastic wave device and filter device |
-
1995
- 1995-12-26 JP JP33944995A patent/JPH09181554A/en active Pending
Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US7400218B2 (en) | 2003-11-12 | 2008-07-15 | Murata Manufacturing Co., Ltd. | Surface acoustic wave filter |
| JP2013223178A (en) * | 2012-04-18 | 2013-10-28 | Nippon Dempa Kogyo Co Ltd | Acoustic wave filter |
| WO2024029360A1 (en) * | 2022-08-04 | 2024-02-08 | 株式会社村田製作所 | Elastic wave device and filter device |
| WO2024116813A1 (en) * | 2022-11-28 | 2024-06-06 | 株式会社村田製作所 | Elastic wave device and filter device |
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