JP2900663B2 - Weighted electrodes for surface acoustic wave filters - Google Patents
Weighted electrodes for surface acoustic wave filtersInfo
- Publication number
- JP2900663B2 JP2900663B2 JP27844691A JP27844691A JP2900663B2 JP 2900663 B2 JP2900663 B2 JP 2900663B2 JP 27844691 A JP27844691 A JP 27844691A JP 27844691 A JP27844691 A JP 27844691A JP 2900663 B2 JP2900663 B2 JP 2900663B2
- Authority
- JP
- Japan
- Prior art keywords
- electrode
- electrodes
- acoustic wave
- surface acoustic
- floating
- 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 - Fee Related
Links
Landscapes
- Surface Acoustic Wave Elements And Circuit Networks Thereof (AREA)
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、弾性表面波フィルタに
係り、特に、弾性表面波フィルタの重み付け電極に関す
る。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a surface acoustic wave filter, and more particularly, to a weighting electrode of a surface acoustic wave filter.
【0002】[0002]
【従来の技術】従来の弾性表面波フィルタに用いる重み
付け電極は、図3に示すような交叉幅21を場所により
重み付け関数に比例して変化させるアポダイズド電極、
或いは図5に示すように、交叉幅31が一定で該交叉幅
を有する電極指の密度を重み付け関数に比例して変化さ
せる間引き電極などが主に用いられている。2. Description of the Related Art A weighted electrode used in a conventional surface acoustic wave filter is an apodized electrode that changes an intersection width 21 in proportion to a weighting function depending on a location as shown in FIG.
Alternatively, as shown in FIG. 5, a thinning electrode or the like is mainly used in which the cross width 31 is constant and the density of electrode fingers having the cross width is changed in proportion to a weighting function.
【0003】[0003]
【発明が解決しようとする課題】これら従来の重み付け
電極にはそれぞれ欠点があり、場合により使い分けてい
るのが実状であった。即ち、図3に示すアポダイズド電
極は、重み付け関数を忠実に交叉幅により表現できる
が、重み付け係数の小さい部分、即ち交叉幅の狭い部分
は波の回折効果により誤差が生じ、フィルタ特性が劣化
しやすく、また電極から励振されるエネルギー分布25
が図4に示す如く重み付け関数の分布により一定でない
ため、重み付け損失の原因となる、という欠点があっ
た。However, these conventional weighting electrodes have respective disadvantages, and the actual situation is that they are properly used in some cases. That is, although the apodized electrode shown in FIG. 3 can faithfully express the weighting function by the crossover width, an error is generated in a portion where the weighting coefficient is small, that is, a portion where the crossover width is narrow, due to a wave diffraction effect, and the filter characteristics are easily deteriorated. And the energy distribution 25 excited from the electrodes
However, as shown in FIG. 4, there is a drawback in that it is not constant due to the distribution of the weighting function, causing weight loss.
【0004】また、図5に示す間引き電極は、励振され
るエネルギー分布34は均一(図6参照)であるが、交
叉幅の有無による密度の高低で重み付け関数を表現する
ため、アポダイズド電極に比べ量子化誤差が大きく、所
望の特性が得にくいという問題点があった。The thinned electrode shown in FIG. 5 has a uniform energy distribution 34 excited (see FIG. 6). However, since the weighting function is expressed by the density depending on the presence or absence of the crossing width, the thinning electrode is compared with the apodized electrode. There is a problem that a quantization error is large and it is difficult to obtain desired characteristics.
【0005】[0005]
【発明の目的】本発明は、かかる従来例の有する不都合
を改善し、とくに、弾性表面波フィルタに特有の量子化
誤差を少なくすることが可能な弾性表面波フィルタ用重
み付け電極を提供することを、その目的とする。SUMMARY OF THE INVENTION It is an object of the present invention to provide a weighting electrode for a surface acoustic wave filter capable of improving the disadvantages of the prior art and reducing the quantization error peculiar to the surface acoustic wave filter. And its purpose.
【0006】[0006]
【課題を解決するための手段】上記目的を達成するた
め、請求項1記載の本発明では、圧電基板上に形成され
対向して配設された二つのバス電極から所定間隔を隔て
て並列に且つ同一線上に相手側に向けて突出形成された
複数の交叉指電極を有すると共に、この各交叉指電極の
先端が同一線上で所定の間隔を隔てて止められた状態に
設定されて成る重み弾性表面波フィルタ用重み付け電極
において、並列に形成された隣接する各交叉指電極の相
互間に、一端部が互いに接続された一対の浮き電極を設
け、この浮き電極および前記各交叉指電極の相互間の間
隔を同一に設定する。そして、前述した各交叉指電極と
浮き電極との間の交差幅を、当該各交叉指電極の場所に
よらず一定とする、という構成を採っている。According to the first aspect of the present invention, there is provided a piezoelectric substrate formed on a piezoelectric substrate.
At a predetermined distance from two bus electrodes arranged opposite to each other
Are formed in parallel and on the same line to project toward the other side
A plurality of cross finger electrodes, and
In a state where the tip is stopped at a predetermined interval on the same line
In the set weighted surface acoustic wave filter weighting electrode, the phase of each adjacent cross finger electrode formed in parallel is set.
A pair of floating electrodes , one end of which is connected to each other , are provided between the floating electrodes and the interdigital electrodes.
Set the same interval . And each of the above-mentioned cross finger electrodes and
The intersection width between the floating electrode and the floating electrode is
It is configured to keep it constant .
【0007】[0007]
【発明の実施例】以下、本発明の一実施例を図1ないし
図2に基づいて説明する。この図1ないし図2に示す実
施例は、圧電基板上に形成され交叉指電極で構成された
互いに隣合う複数の電極11,14を有すると共に、こ
の各複数の電極11,14の相互間に、互いに接続され
た一対の浮き電極17,18が設けられている。この場
合、隣接する各電極11,14の相互間の間隔は、例え
ばλ/2に設定されている。又、隣接する各電極11,
17,18,14の各相互間の間隔は、例えばλ/6に
設定されている。ここで、λは弾性表面波の波長を示
す。 DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS One embodiment of the present invention will be described below with reference to FIGS. The embodiment shown in FIGS. 1 and 2 has a plurality of adjacent electrodes 11 and 14 formed on a piezoelectric substrate and formed by intersecting finger electrodes, and has a space between the plurality of electrodes 11 and 14. And a pair of floating electrodes 17 and 18 connected to each other. This place
In this case, the distance between the adjacent electrodes 11 and 14 is, for example,
For example, it is set to λ / 2. In addition, adjacent electrodes 11,
The spacing between each of 17, 18, and 14 is, for example, λ / 6.
Is set. Here, λ indicates the wavelength of the surface acoustic wave.
You.
【0008】弾性表面波は、一般に交叉部を有する二本
の電極指間に電圧が印加されることによって励振され、
その大きさは交叉部の静電容量に比例し、印加電圧にも
比例する。従って、励振される弾性表面波の大きさは交
叉部に蓄積される電荷量に比例することになる。この場
合、浮き電極17,18を設けると、交叉部設定の自由
度が大きいことから、汎用性が高められる。 前述した電
極指11及び13はバス電極15と、電極指12及び1
4はバス電極16とそれぞれ接続されており、又、浮き
電極17及び18は互いに接続されている。電極指11
と浮き電極17との交叉幅W1 と、電極指12と浮き電
極17との交叉幅W2 との和(W1 +W2 )、及び電極
指13と浮き電極18との交叉幅W3 と、電極指14と
浮き電極18との交叉幅W4 との和(W3 +W4 )は、
同じであり、かつ、場所によらず一定となる様にしてあ
る。A surface acoustic wave generally has two crosses.
Excited by applying a voltage between the electrode fingers of
Its magnitude is proportional to the capacitance of the crossover, and the applied voltage
Proportional. Therefore, the magnitude of the surface acoustic wave excited is
It will be proportional to the amount of charge stored in the fork. This place
In this case, if the floating electrodes 17 and 18 are provided, the freedom of setting the intersection
Since the degree is large, versatility is enhanced. The aforementioned electrode fingers 11 and 13 are connected to the bus electrode 15 and the electrode fingers 12 and 1 respectively.
4 is connected to the bus electrode 16 respectively, and the floating electrodes 17 and 18 are connected to each other. Electrode finger 11
And cross width W 1 between the floating electrode 17, the sum of the overlap width W 2 between the electrode fingers 12 and the floating electrode 17 (W 1 + W 2), and an electrode finger 13 and the overlap width W 3 of the floating electrode 18 The sum (W 3 + W 4 ) of the intersection width W 4 between the electrode finger 14 and the floating electrode 18 is
They are the same and are constant regardless of location.
【0009】この様に構成とすることにより、交叉幅W
1 とW2 及び交叉幅W3 とW4 から励振される弾性表面
波の強さは(W1 −W3 )=(W4 −W2 )に比例す
る。With such a configuration, the cross width W
Strength of 1 and W 2 and overlap width W 3 and W 4 surface acoustic wave excited from is proportional to (W 1 -W 3) = ( W 4 -W 2).
【0010】 このため、上記実施例によると、バス電極
15,16側の隣接する各浮き電極17,18との間の
各交叉幅の和が場所によらず一定(W1 +W2 )=(W
3 +W4 )でありながら、弾性表面波の励振強度は、そ
れぞれバス電極15,16側の各交叉幅の差がそれぞれ
等しく設定し(W1 −W3 )=(W4 −W2 )に比例す
るようにしたので、従来のアポダイズド電極の欠点であ
る回折効果による劣化が少なくなり、かつ、従来の間引
き電極のような量子化誤差による設計上の制限がなくな
るという利点がある。 For this reason, according to the above embodiment, the sum of the crossing widths between the adjacent floating electrodes 17 and 18 on the bus electrode 15 and 16 side is constant regardless of the location (W 1 + W 2 ) = ( W
3 + W 4 ), the excitation intensity of the surface acoustic wave is set such that the difference between the cross widths of the bus electrodes 15 and 16 is set equal to (W 1 −W 3 ) = (W 4 −W 2 ). Since the ratio is set to be proportional, there is an advantage that deterioration due to a diffraction effect, which is a drawback of the conventional apodized electrode, is reduced, and design limitation due to a quantization error unlike a conventional thinned electrode is eliminated.
【0011】[0011]
【発明の効果】以上説明したように本発明によると、交
叉幅が場所によらず一定で且つ弾性表面波の励振強度が
隣接する浮き電極との間の交叉幅の差に比例するように
したので、従来のアポダイズド電極の欠点である回折効
果による劣化が少なくなり、かつ、従来の間引き電極の
ような量子化誤差による設計上の制限がないという従来
にない優れた弾性表面波フィルタ用重み付け電極を提供
することができる。According to the present invention as described in the foregoing, in proportion to the difference between the cross width between the floating electrode excitation intensity constant at and SAW cross width regardless of the location is <br/> adjacent as to
As a result , there is less deterioration due to the diffraction effect, which is a drawback of the conventional apodized electrode, and there is no design limitation due to quantization errors unlike the conventional thinned electrode. Electrodes can be provided.
【図1】本発明の一実施例を示す重み付け電極の平面図
である。FIG. 1 is a plan view of a weighting electrode showing one embodiment of the present invention.
【図2】図1のエネルギー分布を示す説明図である。FIG. 2 is an explanatory diagram showing the energy distribution of FIG.
【図3】従来例のアポダイズド電極を示す平面図であ
る。FIG. 3 is a plan view showing a conventional apodized electrode.
【図4】図3のエネルギー分布を示す説明図である。FIG. 4 is an explanatory diagram showing the energy distribution of FIG.
【図5】他の従来例における間引き電極を示す平面図で
ある。FIG. 5 is a plan view showing a thinning electrode in another conventional example.
【図6】図5のエネルギー分布を示す説明図である。FIG. 6 is an explanatory diagram showing the energy distribution of FIG.
11,12,13,14 電極指 15,16 バス電極 17,18 浮き電極 19 弾性表面波エネルギー分布 11, 12, 13, 14 Electrode finger 15, 16 Bus electrode 17, 18 Floating electrode 19 Surface acoustic wave energy distribution
───────────────────────────────────────────────────── フロントページの続き (58)調査した分野(Int.Cl.6,DB名) H03H 9/145 H03H 9/64 ──────────────────────────────────────────────────続 き Continued on the front page (58) Field surveyed (Int.Cl. 6 , DB name) H03H 9/145 H03H 9/64
Claims (1)
た二つのバス電極から所定間隔を隔てて並列に且つ同一
線上に相手側に向けて突出形成された複数の交叉指電極
を有すると共に、この各交叉指電極の先端が同一線上で
所定の間隔を隔てて止められた状態に設定されて成る重
み弾性表面波フィルタ用重み付け電極において、前記並列に形成された隣接する各交叉指電極の相互間
に、一端部が 互いに接続された一対の浮き電極を設け、
この浮き電極および前記各交叉指電極の相互間の間隔を
同一に設定し、 前記各交叉指電極と浮き電極との間の交差幅を、前記各
交叉指電極の場所によらず一定とし たことを特徴とする
弾性表面波フィルタ用重み付け電極。1. A piezoelectric device formed on a piezoelectric substrate and disposed opposite to the piezoelectric substrate.
In parallel and at the same distance from the two bus electrodes
Plural cross finger electrodes protruding toward the other side on the line
And the tip of each interdigital electrode is aligned on the same line.
In a weighting electrode for a weighted surface acoustic wave filter, which is set to be stopped at a predetermined interval, a distance between adjacent ones of the intersecting finger electrodes formed in parallel with each other.
A pair of floating electrodes having one end connected to each other ,
The distance between the floating electrode and each of the cross finger electrodes is set to
The width of the intersection between each of the interdigital electrodes and the floating electrode is set to be the same,
A weighting electrode for a surface acoustic wave filter, wherein the weighting electrode is constant irrespective of the location of a cross finger electrode.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP27844691A JP2900663B2 (en) | 1991-09-30 | 1991-09-30 | Weighted electrodes for surface acoustic wave filters |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP27844691A JP2900663B2 (en) | 1991-09-30 | 1991-09-30 | Weighted electrodes for surface acoustic wave filters |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH0595251A JPH0595251A (en) | 1993-04-16 |
JP2900663B2 true JP2900663B2 (en) | 1999-06-02 |
Family
ID=17597455
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP27844691A Expired - Fee Related JP2900663B2 (en) | 1991-09-30 | 1991-09-30 | Weighted electrodes for surface acoustic wave filters |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP2900663B2 (en) |
-
1991
- 1991-09-30 JP JP27844691A patent/JP2900663B2/en not_active Expired - Fee Related
Also Published As
Publication number | Publication date |
---|---|
JPH0595251A (en) | 1993-04-16 |
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