JPH0241950Y2 - - Google Patents

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Publication number
JPH0241950Y2
JPH0241950Y2 JP16852884U JP16852884U JPH0241950Y2 JP H0241950 Y2 JPH0241950 Y2 JP H0241950Y2 JP 16852884 U JP16852884 U JP 16852884U JP 16852884 U JP16852884 U JP 16852884U JP H0241950 Y2 JPH0241950 Y2 JP H0241950Y2
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JP
Japan
Prior art keywords
filter
surface acoustic
acoustic wave
attenuation
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.)
Expired
Application number
JP16852884U
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Japanese (ja)
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JPS6183330U (en
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Priority to JP16852884U priority Critical patent/JPH0241950Y2/ja
Publication of JPS6183330U publication Critical patent/JPS6183330U/ja
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Description

【考案の詳細な説明】 (産業上の利用分野) この発明は表面弾性波フイルタに関する。[Detailed explanation of the idea] (Industrial application field) The present invention relates to a surface acoustic wave filter.

(従来の技術) 従来から種々の構成の表面弾性波フイルタが提
案され又実用化されている。第3図は電気入力及
び電気出力に夫々一個の表面弾性波変換器(以
下、単に変換器と称する)で構成される従来の表
面弾性波フイルタ(以下、単に、2電極構成フイ
ルタと称する)の一例を示す線図である。同図に
おいて、1は圧電基板、2は入力用変換器、3は
出力用変換器、4は入力端子、5は出力端子、6
及び7は入力信号が入力用変換器から弾性波とし
て出力した表面弾性波である。
(Prior Art) Surface acoustic wave filters with various configurations have been proposed and put into practical use. Figure 3 shows a conventional surface acoustic wave filter (hereinafter simply referred to as a 2-electrode filter) that is composed of one surface acoustic wave transducer (hereinafter simply referred to as a transducer) for each electrical input and output. It is a diagram showing an example. In the figure, 1 is a piezoelectric substrate, 2 is an input converter, 3 is an output converter, 4 is an input terminal, 5 is an output terminal, and 6
and 7 are surface acoustic waves whose input signals are output as elastic waves from the input transducer.

一般に、変換器は双方向性を有するため、入力
端子4に供給された電気信号は、入力用変換器2
によつて、相対向する二方向にそれぞれ進む二つ
の表面弾性波6及び7に変換される。出力変換器
3が受信する表面弾性波は一方側に進む弾性波7
だけであり、さらに、そのうち電気信号に変換さ
れるのは、その1/2であるため、入力信号の1/4だ
けが出力信号に変換されて出力端子5から出力さ
れる。これがため、2電極構成フイルタでは、理
想的な状態であつても6dBの挿入損失があること
が知られている。
Generally, the converter has bidirectionality, so that the electrical signal supplied to the input terminal 4 is transmitted to the input converter 2.
The waves are converted into two surface acoustic waves 6 and 7 which travel in two opposing directions. The surface acoustic wave received by the output transducer 3 is an elastic wave 7 that propagates to one side.
Furthermore, only 1/2 of the input signal is converted into an electrical signal, so only 1/4 of the input signal is converted into an output signal and output from the output terminal 5. For this reason, it is known that a two-electrode filter has an insertion loss of 6 dB even under ideal conditions.

従来から、この表面弾性波フイルタの挿入損失
の低下を図るため、多電極構成フイルタと称する
表面弾性波フイルタが提案され用いられてきた
(昭和58年度電子通信学会総合全国大会予稿集、
No.100,)。このフイルタは例えば第4図に示すよ
うに、圧電基板1上に入力用及び入力用変換器2
及び3を交互に等間隔に複数個配列して構成した
構造となつている。この構造は、出力信号として
変換されない表面弾性波の量を減らすことによつ
て挿入損失の減少を図ることを狙つたものであ
り、変換器の総数を増加させれば挿入損失はさら
に減少する。
Conventionally, in order to reduce the insertion loss of surface acoustic wave filters, surface acoustic wave filters called multi-electrode filters have been proposed and used (Proceedings of the 1981 National Conference of the Institute of Electronics and Communication Engineers,
No.100,). For example, as shown in FIG.
and 3 are arranged alternately at equal intervals. This structure aims to reduce insertion loss by reducing the amount of surface acoustic waves that are not converted into output signals, and increasing the total number of transducers further reduces insertion loss.

(考案が解決しようとする問題点) ところで、この多電極構成フイルタのフイルタ
特性と、2電極構成フイルタのフイルタ特性とを
第5図に示す。第5図において、横軸に周波数を
及び縦軸に損失(dB)をそれぞれプロツトして
示し、0は中心周波数を示す。この第5図のフイ
ルタ特性からも明らかなように、2電極構成フイ
ルタ特性(実線で示す)に比べて、多電極構成
フイルタのフイルタ特性(破線で示す)は、通
過域における損失は少なくなるが、その反面、減
衰域において、先鋭状に著しく損失が減少してし
まい、減衰域で充分な減衰量が得られないという
欠点があつた。例えば、5電極構成フイルタ、7
電極構成フイルタ及び9電極構成フイルタの減衰
域での減衰量は2電極構成フイルタに比べて、そ
れぞれ約10dB,15dB及び20dB程度劣化してい
る。
(Problems to be Solved by the Invention) FIG. 5 shows the filter characteristics of this multi-electrode filter and the two-electrode filter. In FIG. 5, frequency is plotted on the horizontal axis and loss (dB) is plotted on the vertical axis, where 0 indicates the center frequency. As is clear from the filter characteristics in Figure 5, compared to the two-electrode filter characteristics (shown by the solid line), the filter characteristics of the multi-electrode filter (shown by the broken line) have less loss in the passband, but However, on the other hand, there was a drawback that the loss decreased sharply and significantly in the attenuation region, making it impossible to obtain a sufficient amount of attenuation in the attenuation region. For example, a 5-electrode configuration filter, 7
The attenuation amounts in the attenuation range of the electrode configuration filter and the 9-electrode configuration filter are degraded by approximately 10 dB, 15 dB, and 20 dB, respectively, compared to the 2-electrode configuration filter.

このように、フイルタ特性が減衰域で充分な減
衰量が得られない原因は次のように考えられる。
すなわち、一般に、表面弾性波フイルタにおいて
は、大きな減衰量を得るためフイルタ特性の減衰
の極がほぼ等間隔Δ1となるように変換器を設計
し、しかも、その設計は2電極構成フイルタをも
とに行われている。
As described above, the reason why a sufficient amount of attenuation cannot be obtained in the attenuation region of the filter characteristic is considered to be as follows.
That is, in general, in surface acoustic wave filters, in order to obtain a large amount of attenuation, the transducer is designed so that the attenuation poles of the filter characteristic are approximately equally spaced Δ 1 , and the design also includes a two-electrode filter. It is being carried out.

一方、多電極構成フイルタでは、lを変換器の
中心間の表面弾性波伝搬距離とし、λを表面弾性
波の波長とし、0をフイルタの中心周波数とする
と、フイルタの減衰域に相当する周波数帯域で先
鋭状の損失の減少が起る周期Δ2は理論的に
0λ/(2l)となることがわかつている。
On the other hand, in a multi-electrode filter, if l is the surface acoustic wave propagation distance between the centers of the transducer, λ is the wavelength of the surface acoustic wave, and 0 is the center frequency of the filter, then the frequency band corresponding to the attenuation range of the filter is The period Δ 2 at which the sharp loss decrease occurs is theoretically
It is known that 0 λ/(2l).

ところが、変換器の設計に当り、変換器を多数
個配列させて構成される多電極構成フイルタのフ
イルタ特性について考慮をしていないため、変換
器の減衰の極の周期Δ1と、多電極構成フイルタ
の先鋭状の損失の減少周期Δ2との間にずれが生
じているため、上述したような減衰域での損失の
劣化が生じてしまうのである。
However, when designing the converter, the filter characteristics of a multi-electrode filter constructed by arranging a large number of transducers were not considered, so the attenuation pole period Δ1 of the converter and the multi-electrode structure Since there is a difference between the filter's sharp loss reduction period Δ 2 and the loss reduction period Δ 2 of the filter, the loss deteriorates in the attenuation region as described above.

従つて、減衰の極の周期Δ1と、先鋭状の損失
の減少周期Δ2とを一致させるようにすれば、通
過域での低挿入損失を維持しつつ減衰域での減衰
量の劣化を最小限に抑えることが期待出来る。
Therefore, by matching the attenuation pole period Δ 1 and the sharp loss reduction period Δ 2 , it is possible to maintain low insertion loss in the passband and reduce the deterioration of the attenuation amount in the attenuation region. It is hoped that this can be kept to a minimum.

この考案の目的は、通過域でのフイルタ特性を
損なうことなく、減衰域での先鋭状の損失低下を
抑えることにより、充分な減衰量を持つた良好な
フイルタ特性を有する多電極構成の表面弾性波フ
イルタを提供することにある。
The purpose of this invention is to suppress the sharp drop in loss in the attenuation region without impairing the filter characteristics in the passband, thereby improving the surface elasticity of a multi-electrode structure with sufficient attenuation and good filter characteristics. Our goal is to provide wave filters.

(問題点を解決するための手段) この目的の達成を図るため、この考案によれ
ば、フイルタ特性の減衰の極の周波数間隔Δ1
有する表面弾性波変換器を複数個並べて成る多電
極構成の表面弾性波フイルタにおいて、各表面弾
性波変換器2,3を、これら表面弾性波変換器
2,3の中心間の間隔lを l=0λ/(2Δ1) 但し、 λ :表面弾性波の波長 0:フイルタの中心周波数 として、配列して成ることを特徴とする。
(Means for Solving the Problems) In order to achieve this purpose, according to this invention, a multi-electrode structure is constructed in which a plurality of surface acoustic wave transducers having a frequency interval of attenuation poles of filter characteristics with a frequency interval Δ 1 are arranged. In the surface acoustic wave filter, each surface acoustic wave transducer 2, 3 is connected to the surface acoustic wave transducer 2, 3, and the distance l between the centers of these surface acoustic wave transducers 2, 3 is l= 0 λ/(2Δ 1 ), where λ: surface acoustic wave Wavelength 0 : As the center frequency of the filter, it is characterized by being arranged in an array.

(作用) このように構成すれば、変換器の減衰の極の周
期Δ1と、多電極構成フイルタの先鋭状の損失の
減少周期Δ2とを一致させることが出来るので、
周波数領域上で、減衰域において先鋭上に損失が
減少する位置を充分減衰の取れていない位置に合
せることが可能となり、良好なフイルタ特性を得
ることが出来る。
(Function) With this configuration, the period Δ 1 of the attenuation pole of the converter can be made to match the period Δ 2 of the sharp loss reduction of the multi-electrode filter.
In the frequency domain, it is possible to align the position where the loss sharply decreases in the attenuation region with the position where sufficient attenuation is not achieved, and it is possible to obtain good filter characteristics.

(実施例) 以下、第1図及び第2図A,B,Cを参照し
て、この考案の表面弾性波フイルタの一実施例を
説明する。尚、第1図において第3図及び第4図
に示した構成成分と同一の構成成分については同
一の符号を付して示し、その詳細な説明を省略す
る。
(Embodiment) An embodiment of the surface acoustic wave filter of this invention will be described below with reference to FIG. 1 and FIGS. 2A, B, and C. Components in FIG. 1 that are the same as those shown in FIGS. 3 and 4 are designated by the same reference numerals, and detailed explanation thereof will be omitted.

第1図に示す実施例は5電極構成フイルタであ
り、この場合の出力用変換器3と入力用変換器2
とを交互に一定の中心間間隔lで配列させた構造
となつている。この場合、先鋭状に損失が減少す
る周期Δ2は、上述したように、Δ20λ/
(2l)として理論的に与えられているので、変換
器の減衰の極の周期Δ1と、多電極構成フイルタ
の先鋭状の損失の減少周期Δ2とを一致させると
いう条件から、この間隔lは l=0λ/(2Δ1) で与えられることとなる。
The embodiment shown in FIG. 1 is a five-electrode filter, in which an output converter 3 and an input converter 2
It has a structure in which these are alternately arranged at a constant center-to-center spacing l. In this case, the period Δ 2 in which the loss decreases sharply is Δ 2 = 0 λ/
Since it is theoretically given as ( 2l ), this interval l is given by l = 0 λ/(2Δ 1 ).

従つて、この考案の表面弾性波フイルタでは間
隔lを0λ/(2Δ1)と設定して各変換器2及び
3を交互に等ピツチで配列させている。
Therefore, in the surface acoustic wave filter of this invention, the interval l is set to 0 λ/(2Δ 1 ), and the transducers 2 and 3 are arranged alternately at equal pitches.

第2図aはこの多電極構成フイルタのフイルタ
特性を示す線図で、この図からも明らかなよう
に、先鋭状の損失の減少が周期Δ2毎に現われて
いる。一方、第2図Bは2電極構成フイルタとし
て設計されたフイルタ特性を示し、減衰の極が周
期Δ1で生じている。従つて、この考案の多電極
構成のフイルタではΔ1=Δ2であるので、その
フイルタ特性は第2図A及びBの各特性の和とし
て得られ、従つて、第2図Cに示したような、通
過域での特性が損なわれることなく、減衰域での
損失量の低下が最小限に抑えられた極めた良好な
フイルタ特性となる。
FIG. 2a is a diagram showing the filter characteristics of this multi-electrode filter, and as is clear from this diagram, a sharp decrease in loss appears every period Δ 2 . On the other hand, FIG. 2B shows the filter characteristics designed as a two-electrode filter, in which the attenuation pole occurs at a period Δ 1 . Therefore, since Δ 1 = Δ 2 in the multi-electrode filter of this invention, the filter characteristics are obtained as the sum of the characteristics shown in FIG. 2A and B, and therefore, as shown in FIG. 2C. This results in extremely good filter characteristics in which the characteristics in the passband are not impaired and the decrease in loss in the attenuation region is minimized.

さらに、挿入損失を減少させるため、変換器の
数を増加させた場合には、減衰域での損失の劣化
は一層大きくなるが、この考案の電極構造でその
多電極構成フイルタを構成すれば、減衰量の劣化
の抑制効果が著しくなり、しかも、2電極構成の
場合の減衰域での減衰量よりも改善される。
Furthermore, if the number of transducers is increased to reduce insertion loss, the loss degradation in the attenuation region will become even greater, but if the multi-electrode filter is configured with the electrode structure of this invention, The effect of suppressing the deterioration of the attenuation amount is remarkable, and moreover, it is improved more than the attenuation amount in the attenuation range in the case of the two-electrode configuration.

(考案の効果) 上述した説明からも明らかなように、この考案
の多電極構成フイルタによれば、各変換器の中心
間間隔を、フイルタの減衰の極の周期と、先鋭状
の損失の減少周期とが一致するように設定してあ
るので、通過域での特性を損なうことがなく、し
かも、減衰域での減衰量の低下を最小限に抑える
ことが出きる。従つて、この考案の多電極構成フ
イルタは低損失で、充分な減衰量の取れた良好な
フイルタ特性を有する表面弾性波フイルタとな
る。
(Effect of the invention) As is clear from the above explanation, according to the multi-electrode filter of this invention, the center-to-center spacing of each transducer can be adjusted to match the period of the attenuation pole of the filter and the reduction of sharp loss. Since the periods are set to match, the characteristics in the pass band are not impaired, and furthermore, the decrease in the amount of attenuation in the attenuation band can be minimized. Therefore, the multi-electrode filter of this invention is a surface acoustic wave filter having low loss, sufficient attenuation, and good filter characteristics.

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

第1図はこの考案の表面弾性波フイルタの一実
施例を示す線図、第2図A及びBこの考案の説明
に供する多電極構成フイルタ及び2電極構成フイ
ルタのフイルタ特性を示す線図、第2図Cはこの
考案の表面弾性波フイルタのフイルタ特性を示す
線図、第3図〜第5図は従来の表面弾性波フイル
タの説明に供する線図である。 1……圧電基板、2……入力用変換器、3……
出力用変換器、4……入力端子、5……出力端
子。
FIG. 1 is a diagram showing an embodiment of the surface acoustic wave filter of this invention, FIGS. FIG. 2C is a diagram showing the filter characteristics of the surface acoustic wave filter of this invention, and FIGS. 3 to 5 are diagrams for explaining conventional surface acoustic wave filters. 1...Piezoelectric substrate, 2...Input converter, 3...
Output converter, 4...input terminal, 5...output terminal.

Claims (1)

【実用新案登録請求の範囲】 フイルタ特性の減衰の極の周波数間隔Δ1を有
する表面弾性波変換器を複数個並べて成る多電極
構成の表面弾性波フイルタにおいて、各表面弾性
波変換器を、これら表面弾性波変換器の中心間の
間隔lを l=0λ/(2Δ1) 但し、 λ :表面弾性波の波長 0:フイルタの中心周波数 として、配列して成ることを特徴とする表面弾性
波フイルタ。
[Claims for Utility Model Registration] In a surface acoustic wave filter having a multi-electrode configuration in which a plurality of surface acoustic wave transducers each having a frequency interval Δ 1 between poles of attenuation of filter characteristics are arranged, each surface acoustic wave transducer is The spacing l between the centers of the surface acoustic wave transducers is l = 0 λ/(2Δ 1 ) where λ is the wavelength of the surface acoustic wave 0 is the center frequency of the filter. filter.
JP16852884U 1984-11-08 1984-11-08 Expired JPH0241950Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP16852884U JPH0241950Y2 (en) 1984-11-08 1984-11-08

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP16852884U JPH0241950Y2 (en) 1984-11-08 1984-11-08

Publications (2)

Publication Number Publication Date
JPS6183330U JPS6183330U (en) 1986-06-02
JPH0241950Y2 true JPH0241950Y2 (en) 1990-11-08

Family

ID=30726296

Family Applications (1)

Application Number Title Priority Date Filing Date
JP16852884U Expired JPH0241950Y2 (en) 1984-11-08 1984-11-08

Country Status (1)

Country Link
JP (1) JPH0241950Y2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2933171B2 (en) * 1989-09-04 1999-08-09 日本無線株式会社 Surface acoustic wave filter

Also Published As

Publication number Publication date
JPS6183330U (en) 1986-06-02

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