JPH04284013A - Surface acoustic wave filter - Google Patents

Surface acoustic wave filter

Info

Publication number
JPH04284013A
JPH04284013A JP4789791A JP4789791A JPH04284013A JP H04284013 A JPH04284013 A JP H04284013A JP 4789791 A JP4789791 A JP 4789791A JP 4789791 A JP4789791 A JP 4789791A JP H04284013 A JPH04284013 A JP H04284013A
Authority
JP
Japan
Prior art keywords
electrode
length
reflector
electrodes
apodized
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP4789791A
Other languages
Japanese (ja)
Inventor
Kazunori Nishimura
和紀 西村
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP4789791A priority Critical patent/JPH04284013A/en
Publication of JPH04284013A publication Critical patent/JPH04284013A/en
Pending legal-status Critical Current

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

Abstract

PURPOSE:To solve the problem of lowering a filter characteristic due to the distortion of exciting strength distribution and to offer the surface acoustic wave filter having the satisfactory filter characteristic, at the surface acoustic wave filter used for a filter for digital car telephone or a filter for timing extraction. CONSTITUTION:The two couples of a pair of interlaced electrodes are provided on a piezoelectric substrate 4, a pair of the interlaced electrodes are taken as uniform normal type electrodes (b), the other pair of interlaced electrodes are taken as apodization type electrode (a) changing the interlaced length in respect to the direction of arranging interlaced electrodes 1a, plural reflectors 2b and 2a are provided between the normal type electrode (b) and the apodization type electrode (a) and for the reflector 2a on the side of the electrode (a), the length is changed corresponding to the change of the interlaced length of the interlaced electrode 1a. Therefore, the satisfactory filter characteristics lowering a loss, enlarging the attenuation amount of a side lobe, enlarging the range of a group delay characteristic and making it flat can be obtained.

Description

【発明の詳細な説明】[Detailed description of the invention]

【0001】0001

【産業上の利用分野】本発明はデジタル自動車電話用フ
ィルタ,タイミング抽出フィルタ等に利用される弾性表
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 used in digital car telephone filters, timing extraction filters, and the like.

【0002】0002

【従来の技術】近年、情報通信分野のデジタル化が進め
られ、システムの構成上、低損失で比較的狭帯域のフィ
ルタが求められるようになってきた。しかしながら、ト
ランスバーサル型の弾性表面波フィルタは比帯域が小さ
い程チップサイズが大きくなってしまう。そのため低損
失のフィルタを実現するために3電極構成にすることは
部品の大きさ,コストの面で非常に不利であり、一方向
性変換器を用いて2電極で構成することが望ましい。
2. Description of the Related Art In recent years, digitalization in the information and communication field has progressed, and a filter with a relatively narrow band and low loss is required for system configuration. However, in a transversal surface acoustic wave filter, the smaller the specific band, the larger the chip size becomes. Therefore, using a three-electrode configuration to realize a low-loss filter is extremely disadvantageous in terms of component size and cost, and it is desirable to use a two-electrode configuration using a unidirectional transducer.

【0003】そこで、交差電極の交差電極指間に反射器
を備えた単相一方向性電極を用いるのは有効な手段と考
えられる。従来、この種の弾性表面波フィルタは、図4
に示すような構成が一般的であった。図において、a2
は入力側の正規型電極、bは出力側の正規型電極で、入
力側の正規型電極a2および出力側の正規型電極bはそ
れぞれ多数の交差電極指1a2,1b、反射器2a2,
2bおよび引出し電極3a2,3bより構成され、これ
らは圧電基板4上に形成されている。5は吸収材であり
、圧電基板4の両端部に設けられている。
[0003] Therefore, it is considered an effective means to use a single-phase unidirectional electrode provided with a reflector between the intersecting electrode fingers of the intersecting electrodes. Conventionally, this type of surface acoustic wave filter is shown in Fig. 4.
The configuration shown in is common. In the figure, a2
is a regular type electrode on the input side, b is a regular type electrode on the output side, and the regular type electrode a2 on the input side and the regular type electrode b on the output side each have a large number of crossed electrode fingers 1a2, 1b, reflectors 2a2,
2b and extraction electrodes 3a2 and 3b, which are formed on the piezoelectric substrate 4. Reference numeral 5 denotes an absorbing material, which is provided at both ends of the piezoelectric substrate 4.

【0004】次にその動作について説明する。入力側の
正規型電極a2の引出し電極3a2と出力側の正規型電
極bの引出し電極3bはそれぞれ入力用または出力用の
外部電極(図示せず)にワイヤボンディング等によって
接続されて、信号の入出力が行われる。引出し電極3a
2より入力された信号は圧電基板4上に形成された入力
側の正規型電極a2の交差電極指1a2で電気信号から
機械信号に変換される。励振された表面波は反射器2a
2により方向性を与えられ、図4中の矢印で示すように
伝搬し、対向する出力側の正規型電極bの交差電極指1
bにより再び機械信号から電気信号に変換され、引出し
電極3bから外部電極へ出力される。なお吸収材5はこ
のような動作において発生する表面波の悪影響を防ぐた
めに圧電基板4上の両端に塗布されているものである。
Next, its operation will be explained. The extraction electrode 3a2 of the regular type electrode a2 on the input side and the extraction electrode 3b of the regular type electrode b on the output side are connected to external electrodes for input or output (not shown) by wire bonding or the like, respectively, to input signals. Output is done. Extracting electrode 3a
The signal inputted from the piezoelectric substrate 4 is converted from an electrical signal to a mechanical signal by the intersecting electrode fingers 1a2 of the regular type electrode a2 on the input side formed on the piezoelectric substrate 4. The excited surface waves are reflected by the reflector 2a.
2 gives directionality and propagates as shown by the arrow in FIG.
b, the mechanical signal is again converted into an electrical signal, and is output from the extraction electrode 3b to the external electrode. Note that the absorbing material 5 is coated on both ends of the piezoelectric substrate 4 in order to prevent the adverse effects of surface waves generated during such operations.

【0005】[0005]

【発明が解決しようとする課題】しかしながら図4に示
すような入力側の正規型電極a2および出力側の正規型
電極bの交差電極指1a2,1bの交差長が一定の長さ
である交差電極を用いた場合、得られるフィルタ特性は
、サイドローブの減衰がせいぜい26〜33dBであり
、33dB以上の減衰量を必要とする用途には使用する
ことができない。そのため図5に示すように一方の交差
電極をアポダイズ型電極a3とし、減衰量を確保するこ
とが考えられるが、アポダイズ型電極a3側の反射器2
a3をアポダイズせずに、従来と同じ一定の長さで構成
した場合、その反射器2a3により励振強度分布が乱れ
、図6に示すように周波数特性に肩ができてしまい、群
遅延特性も乱れてしまうという課題がある。
[Problem to be Solved by the Invention] However, the intersecting electrodes in which the intersecting length of the intersecting electrode fingers 1a2 and 1b of the regular type electrode a2 on the input side and the regular type electrode b on the output side as shown in FIG. 4 are a constant length. When using this filter, the obtained filter characteristic has a sidelobe attenuation of 26 to 33 dB at most, and cannot be used for applications requiring attenuation of 33 dB or more. Therefore, as shown in FIG. 5, it is possible to use one of the intersecting electrodes as an apodized electrode a3 to ensure attenuation, but the reflector 2 on the apodized electrode a3 side
If a3 is configured with the same constant length as the conventional one without apodizing, the excitation intensity distribution will be disturbed by the reflector 2a3, a shoulder will be formed in the frequency characteristics as shown in Fig. 6, and the group delay characteristics will also be disturbed. There is a problem with this.

【0006】本発明はこのような課題を解決するもので
あり、優れたフィルタ特性を有する弾性表面波フィルタ
を提供することを目的とする。
[0006] The present invention is intended to solve these problems, and an object of the present invention is to provide a surface acoustic wave filter having excellent filter characteristics.

【0007】[0007]

【課題を解決するための手段】上記目的を達成するため
に本発明は、アポダイズ型電極側に設けられている反射
器の反射器長をアポダイズ型電極の交差電極指の交差長
に応じた長さとしたものである。
[Means for Solving the Problems] In order to achieve the above object, the present invention provides a method in which the reflector length of the reflector provided on the apodized electrode side is adjusted to a length corresponding to the intersecting length of the intersecting electrode fingers of the apodized electrode. It is a very important thing.

【0008】[0008]

【作用】したがって本発明によれば、反射器の長さをア
ポダイズ型電極の交差電極指の交差長に合わせて変化さ
せているために、励振強度の分布が乱れることなく、本
来のアポダイズ型電極の特性を発揮することが可能とな
り、低損失でサイドローブの減衰が大きく、しかも群遅
延特性が広範囲で平坦なフィルタ特性を得ることができ
る。
[Operation] Therefore, according to the present invention, since the length of the reflector is changed according to the intersecting length of the intersecting electrode fingers of the apodized electrode, the excitation intensity distribution is not disturbed, and the original apodized electrode This makes it possible to obtain filter characteristics with low loss, large sidelobe attenuation, and flat group delay characteristics over a wide range.

【0009】[0009]

【実施例】以下、本発明の一実施例について、図1〜図
3とともに図4〜図6と同一部分については同一番号を
付して詳しい説明を省略し、相違する点について説明す
る。
DESCRIPTION OF THE PREFERRED EMBODIMENTS Hereinafter, an embodiment of the present invention will be described with reference to FIGS. 1 to 3 as well as to FIGS. 4 to 6, in which the same parts are given the same reference numerals, detailed explanations thereof will be omitted, and differences will be explained.

【0010】図1は本発明の一実施例の構成を示す平面
図であり、図において、aは入力側のアポダイズ型電極
、1aはそのアポダイズ型交差電極aの交差電極指、2
aは反射器、3aは引出し電極である。
FIG. 1 is a plan view showing the configuration of an embodiment of the present invention. In the figure, a is an apodized electrode on the input side, 1a is an intersecting electrode finger of the apodized intersecting electrode a, and 2 is an apodized electrode on the input side.
a is a reflector, and 3a is an extraction electrode.

【0011】次にその動作について説明する。圧電基板
4上に形成された入力側アポダイズ型電極aの引出し電
極3aより入力された信号は交差電極指1aにより電気
信号から機械信号に変換される。励振された表面波はア
ポダイズされた交差電極指1aの交差長に合わせて変化
した長さを有する反射器2aにより方向性を与えられ、
図1中の矢印で示すように伝搬し、出力側の正規型電極
bの交差電極指1bによって再び機械信号から電気信号
に変換され、引出し電極3bから外部電極(図示せず)
へ出力される。
Next, its operation will be explained. A signal inputted from the extraction electrode 3a of the input side apodized electrode a formed on the piezoelectric substrate 4 is converted from an electrical signal to a mechanical signal by the crossed electrode fingers 1a. The excited surface waves are given directionality by a reflector 2a having a length that varies according to the intersecting length of the apodized intersecting electrode fingers 1a,
The signal propagates as indicated by the arrow in FIG. 1, is converted from a mechanical signal to an electrical signal again by the crossed electrode fingers 1b of the regular type electrode b on the output side, and is transferred from the extraction electrode 3b to an external electrode (not shown).
Output to.

【0012】このように上記実施例によれば、入力側ア
ポダイズ型電極aの反射器2aの長さをアポダイズされ
た交差電極指1aの交差長に合わせて変化させているた
めに、励振された表面波の励振強度の分布が乱れること
なく、図3に示すように低損失でサイドローブの減衰が
大きく、かつ群遅延特性が広範囲でフラットになるとい
う効果を得ることができる。
As described above, according to the above embodiment, since the length of the reflector 2a of the input side apodized electrode a is changed in accordance with the length of the apodized intersecting electrode fingers 1a, the excited As shown in FIG. 3, it is possible to obtain the effects of low loss, large sidelobe attenuation, and flat group delay characteristics over a wide range, without disturbing the distribution of the excitation intensity of the surface wave.

【0013】図2は本発明の他の実施例の弾性表面波フ
ィルタの構造を示すものであり、図においてa1は入力
側アポダイズ型電極、1a1はそのアポダイズ型電極a
1の交差電極指、2a1はアポダイズ型電極a1の中心
より出力側の正規型電極b側の半分を交差電極指1a1
の最大交差長と同じ長さ、または最大交差長よりやや長
い一定の長さとした出力側反射器、2a11は同アポダ
イズ型電極a1の他の半分を交差電極指1a1の交差長
の変化に合わせた長さとした反出力側反射器であり、第
1の実施例と同様な効果が得られるものである。
FIG. 2 shows the structure of a surface acoustic wave filter according to another embodiment of the present invention. In the figure, a1 is an apodized electrode on the input side, and 1a1 is the apodized electrode a.
The crossed electrode fingers 1a1 and 2a1 are the half of the regular electrode b side on the output side from the center of the apodized electrode a1.
The output side reflector 2a11 has a constant length that is the same as the maximum crossing length of or slightly longer than the maximum crossing length, and the other half of the apodized electrode a1 is adjusted to the change in the crossing length of the crossed electrode fingers 1a1. This is a long reflector on the opposite output side, and the same effect as in the first embodiment can be obtained.

【0014】なお、上記実施例において、アポダイズ型
電極aまたはa1を入力側、正規型電極bを出力側とし
て説明したが、アポダイズ型電極aまたはa1を出力側
、正規型電極bを入力側の交差電極として用いることも
可能である。
In the above embodiment, the apodized electrode a or a1 was described as being on the input side and the regular electrode b as the output side, but the apodized electrode a or a1 was on the output side and the regular electrode b as the input side. It is also possible to use it as a crossed electrode.

【0015】[0015]

【発明の効果】上記実施例より明らかなように本発明は
、圧電基板上に形成されている反射器を内蔵する2個の
交差電極の一方の電極をアポダイズ型電極とし、反射器
の全てまたは一部の長さをそのアポダイズ型電極の交差
電極指の交差長の変化に合わせた長さとすることによっ
て、低損失でサイドローブの減衰量が大きく、かつ群遅
延特性が広範囲でフラットな優れたフィルタ特性を得る
ことができるものである。
Effects of the Invention As is clear from the above embodiments, the present invention provides an apodized electrode as one electrode of two intersecting electrodes each having a built-in reflector formed on a piezoelectric substrate. By adjusting the length of a part to match the change in the intersecting length of the intersecting electrode fingers of the apodized electrode, an excellent structure with low loss, large sidelobe attenuation, and flat group delay characteristics over a wide range can be achieved. It is possible to obtain filter characteristics.

【図面の簡単な説明】[Brief explanation of the drawing]

【図1】本発明の一実施例における弾性表面波フィルタ
の平面図
FIG. 1 is a plan view of a surface acoustic wave filter according to an embodiment of the present invention.

【図2】本発明の他の実施例における弾性表面波フィル
タの平面図
FIG. 2 is a plan view of a surface acoustic wave filter according to another embodiment of the present invention.

【図3】本発明の実施例における弾性表面波フィルタの
フィルタ特性図
[Fig. 3] Filter characteristic diagram of the surface acoustic wave filter in the embodiment of the present invention

【図4】従来の弾性表面波フィルタの平面図[Figure 4] Plan view of a conventional surface acoustic wave filter

【図5】他
の従来の弾性表面波フィルタの平面図
[Fig. 5] Plan view of another conventional surface acoustic wave filter

【図6】従来の弾
性表面波フィルタのフィルタ特性図
[Figure 6] Filter characteristic diagram of conventional surface acoustic wave filter

【符号の説明】[Explanation of symbols]

a  アポダイズ型電極(交差電極) 1a  交差電極指 2a  反射器 3a  引出し電極 b  正規型電極(交差電極) 4  圧電基板 a Apodized electrode (crossed electrode) 1a Cross electrode fingers 2a Reflector 3a Extraction electrode b Regular type electrode (crossed electrode) 4 Piezoelectric substrate

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】圧電基板上に1対の交差電極を2組備え、
その1組の交差電極を交差長が一様な正規型電極、他の
1組の交差電極を交差電極指の配列方向に対し交差長に
変化をつけたアポダイズ型電極とし、前記正規型電極お
よびアポダイズ型電極それぞれに交差電極の間に複数の
反射器を設け、前記アポダイズ型電極側の前記反射器を
前記交差電極指の交差長の変化に合わせ、その反射器長
を変えた弾性表面波フィルタ。
Claim 1: Two sets of crossed electrodes are provided on a piezoelectric substrate,
One set of intersecting electrodes is a regular type electrode with a uniform crossing length, and the other set of intersecting electrodes is an apodized type electrode whose crossing length is varied with respect to the arrangement direction of the intersecting electrode fingers. A surface acoustic wave filter in which a plurality of reflectors are provided between the crossed electrodes of each apodized electrode, and the reflector length of the reflector on the apodized electrode side is changed in accordance with the change in the crossing length of the crossed electrode fingers. .
【請求項2】アポダイズ型電極内に設けられている複数
の反射器をそのアポダイズ型電極の中心を境とし、正規
型電極のある側(表面波の伝搬方向側)の半分を前記ア
ポダイズ型電極の交差電極指の最大交差長と同じかまた
は交差長よりやや長い一様な反射器長を有する出力側反
射器とし、表面波の伝搬方向の反対側の他の半分を前記
交差長の変化に合わせた長さの反射器長を有する反出力
側反射器とした請求項1記載の弾性表面波フィルタ。
2. A plurality of reflectors provided in an apodized electrode are arranged so that the center of the apodized electrode is the boundary, and half of the side where the regular electrode is located (surface wave propagation direction side) is connected to the apodized electrode. The output side reflector has a uniform reflector length that is equal to or slightly longer than the maximum crossing length of the crossed electrode fingers, and the other half on the opposite side of the surface wave propagation direction is used as the output side reflector to change the crossing length. 2. The surface acoustic wave filter according to claim 1, wherein the reflector on the opposite output side has reflector lengths that are equal in length to each other.
JP4789791A 1991-03-13 1991-03-13 Surface acoustic wave filter Pending JPH04284013A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4789791A JPH04284013A (en) 1991-03-13 1991-03-13 Surface acoustic wave filter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4789791A JPH04284013A (en) 1991-03-13 1991-03-13 Surface acoustic wave filter

Publications (1)

Publication Number Publication Date
JPH04284013A true JPH04284013A (en) 1992-10-08

Family

ID=12788195

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4789791A Pending JPH04284013A (en) 1991-03-13 1991-03-13 Surface acoustic wave filter

Country Status (1)

Country Link
JP (1) JPH04284013A (en)

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