JPH03184412A - Piezoelectric resonator - Google Patents

Piezoelectric resonator

Info

Publication number
JPH03184412A
JPH03184412A JP32342689A JP32342689A JPH03184412A JP H03184412 A JPH03184412 A JP H03184412A JP 32342689 A JP32342689 A JP 32342689A JP 32342689 A JP32342689 A JP 32342689A JP H03184412 A JPH03184412 A JP H03184412A
Authority
JP
Japan
Prior art keywords
cavity
shape
electrode
vibrating electrode
ceramic 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.)
Pending
Application number
JP32342689A
Other languages
Japanese (ja)
Inventor
Shinichi Sawahara
沢原 真一
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.)
Murata Manufacturing Co Ltd
Original Assignee
Murata Manufacturing 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 Murata Manufacturing Co Ltd filed Critical Murata Manufacturing Co Ltd
Priority to JP32342689A priority Critical patent/JPH03184412A/en
Publication of JPH03184412A publication Critical patent/JPH03184412A/en
Pending legal-status Critical Current

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  • Piezo-Electric Or Mechanical Vibrators, Or Delay Or Filter Circuits (AREA)

Abstract

PURPOSE:To suppress spurious resonance without blocking a main response by forming the contour shape of a cavity in non-circular shape so as to set the shortest distance from each corner part of a resonance electrode to the edge of the cavity at a range of two-three times the plate thickness of a piezoelectric ceramic substrate. CONSTITUTION:The shape of the cavity 10 is formed in such a way that the upper and lower parts of the resonance electrode are formed in circular arc shape and both side parts in non-circular shape forming linear shape. By forming the cavity 10 in such shape, it is possible to set the shortest distances d1 and d2 from each corner part of the oscillation electrode to the edge of the cavity 10 at the range of unmagnified to three times the plate thickness (t) of the piezoelectric ceramic substrate 1. In other words, by satisfying conditions t<=d1 and d2<=3t, it is possible to confine sufficient energy and to suppress the spurious resonance without blocking the main response required originally.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は圧電共振子、特に圧電モノリシックフィルタと
して好適な二重モード共振子に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a piezoelectric resonator, particularly a dual mode resonator suitable as a piezoelectric monolithic filter.

〔従来の技術〕[Conventional technology]

一般に、二重モード共振子は、第5図、第6図に示すよ
うに圧電セラミックス基板20の一主面に対をなす入,
出力用の方形振動電極21.22を形成し、他主面の上
記振動電極21.22と対向する部位にアース用の方形
振動電極23を形成したものであり、上記振動電極21
〜23の周囲に空洞24を残して圧電セラミックス基板
20の外周を外装樹脂25で封止しである。なお、振動
電極を方形としたのは、円形の振動電極に比べて、縦・
横の寸法比を変えることにより特性の自由度を大きく取
れるからである。
In general, a dual mode resonator has a pair of inputs and
A rectangular vibrating electrode 21.22 for output is formed, and a rectangular vibrating electrode 23 for grounding is formed on the other main surface at a portion facing the vibrating electrode 21.22.
The outer periphery of the piezoelectric ceramic substrate 20 is sealed with an exterior resin 25, leaving a cavity 24 around the piezoelectric ceramic substrate 23. Note that the rectangular vibrating electrode is more vertical and vertical than the circular vibrating electrode.
This is because by changing the lateral dimension ratio, a greater degree of freedom in characteristics can be achieved.

上記空洞24の形成方法は、振動電極21〜23の上に
予めワックスやパラフィンなどの空洞形成材を塗布し、
外装樹脂の封止時または封止後に加熱し、上記空洞形成
材を融解させて外装樹脂に吸収させることにより、空洞
を形成する方法が用いられる(特公昭45−22384
号公報)。
The method for forming the cavity 24 is to apply a cavity forming material such as wax or paraffin on the vibrating electrodes 21 to 23 in advance,
A method is used in which a cavity is formed by heating the exterior resin during or after sealing to melt the cavity-forming material and absorb it into the exterior resin (Japanese Patent Publication No. 45-22384).
Publication No.).

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

ところが、従来の場合には空洞24の形状が円形である
ため、スプリアス振動が大きくなるという問題があった
。その原因は、第7図に示すように振動電極21.22
の外側の角部から空洞24の周縁までの最短路jlld
、に比べて、内側の角部から空洞24の周縁までの最短
路#d4が遥かに大きくなり、振動電極の内側部分から
放射方向へ伝播する振動のダンピングが不十分となり、
スプリアスレスポンスが大きくなるからである。一方、
第7図−点鎖線で示すように空洞24の周縁が振動電極
21.22の外側の角部の近傍に位置するように空洞2
4を小さくすれば、内側の角部から空洞24の周縁まで
の最短距離d4も小さくなるが、これでは厚み縦振動の
メインレスポンスが阻害され、伝送損失が大きくなる欠
点がある。
However, in the conventional case, since the shape of the cavity 24 is circular, there has been a problem that spurious vibrations become large. The cause of this is as shown in FIG.
The shortest path from the outer corner of the jlld to the periphery of the cavity 24
, the shortest path #d4 from the inner corner to the periphery of the cavity 24 is much larger, and the damping of the vibration propagating in the radial direction from the inner part of the vibrating electrode is insufficient.
This is because the spurious response becomes large. on the other hand,
FIG. 7 - The cavity 24 is arranged so that the periphery of the cavity 24 is located in the vicinity of the outer corner of the vibrating electrode 21.22, as shown by the dashed line.
If 4 is made small, the shortest distance d4 from the inner corner to the periphery of the cavity 24 is also made small, but this has the disadvantage that the main response of thickness longitudinal vibration is inhibited and transmission loss becomes large.

そこで、本発明の目的は、振動電極の間隔が大きくなっ
ても、メインレスポンスを阻害せずにスプリアス振動を
抑制できる圧電共振子を提供することにある。
SUMMARY OF THE INVENTION Therefore, an object of the present invention is to provide a piezoelectric resonator that can suppress spurious vibrations without inhibiting the main response even when the interval between vibrating electrodes becomes large.

(!II!i!を解決するための手段〕上記目的を達成
するため、本発明は、圧電セラミックス基板の一主面に
対をなす入,出力用の方形振動電極を隣接して形成し、
他主面の上記振動電極と対向する部位に上記振動電極を
包含するアース用の方形振動電極を形成してなり、上記
振動電極の周囲に空洞を残して圧電セラミックス基板の
外周を外装樹脂で封止してなるエネルギー閉じ込め型厚
み縦振動モードを利用した圧電共振子において、上記空
洞は、その輪郭が非円形でかつ振動電極の各角部からの
最短距離が圧電セラミックス基板の板厚の等倍〜3倍の
範囲に形成されていることを特徴とするものである。
(Means for solving !II!i!) In order to achieve the above object, the present invention forms a pair of rectangular vibration electrodes for input and output adjacent to one main surface of a piezoelectric ceramic substrate,
A rectangular vibrating electrode for grounding that includes the vibrating electrode is formed on the other principal surface at a portion facing the vibrating electrode, and the outer periphery of the piezoelectric ceramic substrate is sealed with an exterior resin, leaving a cavity around the vibrating electrode. In a piezoelectric resonator using an energy-trapped thickness longitudinal vibration mode, the cavity has a non-circular outline, and the shortest distance from each corner of the vibrating electrode is equal to the thickness of the piezoelectric ceramic substrate. It is characterized by being formed in a range of ~3 times as large.

〔作用〕[Effect]

本発明者が種々検討したところ、振動電極の角部から空
洞の周縁までの最短距離が圧電セラミックス基板の板厚
より小さい範囲にあると、本来必要な厚み縦振動のメイ
ンレスポンスが抑圧されて伝送損失が大きくなり、逆に
、振動電極の角部から空洞の周縁までの最短距離が圧電
セラミックス基板の板厚の3倍より大きい範囲にあると
、エネルギー閉じ込めが不十分となり、スプリアス振動
を抑制できないことが判った。したがって、振動電極の
各角部からの最短距離を圧電セラミックス基板の板厚の
等倍〜3倍の範囲に設定することが必要であるが、従来
のような円形の空洞ではこの条件を満足することは不可
能である。
The inventor conducted various studies and found that if the shortest distance from the corner of the vibrating electrode to the periphery of the cavity is smaller than the thickness of the piezoelectric ceramic substrate, the main response of the originally necessary thickness longitudinal vibration is suppressed and transmitted. On the other hand, if the shortest distance from the corner of the vibrating electrode to the periphery of the cavity is greater than three times the thickness of the piezoelectric ceramic substrate, energy confinement will be insufficient and spurious vibrations will not be suppressed. It turned out that. Therefore, it is necessary to set the shortest distance from each corner of the vibrating electrode to a range that is equal to or three times the thickness of the piezoelectric ceramic substrate, but a conventional circular cavity satisfies this condition. That is impossible.

そこで、本発明では空洞の輪郭形状、換言すれば空洞形
成材の塗布形状を上記の条件を満足する非円形形状とし
たものである。
Therefore, in the present invention, the contour shape of the cavity, in other words, the shape of the cavity forming material applied, is made into a non-circular shape that satisfies the above conditions.

〔実施例〕〔Example〕

第1図、第2図は本発明をエネルギー閉じ込め型圧電モ
ノリシックフィルタに適用した一例を示し、同一基板上
に2個の二重モード共振子を形成した構造となっている
FIGS. 1 and 2 show an example in which the present invention is applied to an energy trap type piezoelectric monolithic filter, which has a structure in which two dual mode resonators are formed on the same substrate.

図において、圧電セラミックス基板1はその厚み方向に
分極処理が施されており、その−主面には2対の入出力
用の方形振動電極2a、 4aおよび3a。
In the figure, a piezoelectric ceramic substrate 1 is polarized in its thickness direction, and has two pairs of input/output rectangular vibrating electrodes 2a, 4a, and 3a on its main surface.

4bが形成されている。下側の振動電極2a、 3aは
それぞれ引出電極2b、 3bを介して端子電極2c、
 3cと接続されている。また、上側の振軌電極4a、
 4bは接続電極4cを介して互いに導通しており、接
続電極4cの中間部にはコンデンサ電極4dが形成され
ている。一方、圧電セラミックス基板1の他主面には、
上記振動電極2a、 4aおよび3a、 4bと対向す
る位置にアース用の方形振動電極5a、 5bが設けら
れ、この振動電極5a、 5bは接続電極5c、 5d
を経て上記コンデンサ電極4dと対向するコンデンサ電
極5eと接続され、さらに端子電極5fと接続されてい
る。
4b is formed. The lower vibrating electrodes 2a and 3a are connected to the terminal electrodes 2c and 2c via lead electrodes 2b and 3b, respectively.
It is connected to 3c. In addition, the upper vibration orbit electrode 4a,
4b are electrically connected to each other via a connecting electrode 4c, and a capacitor electrode 4d is formed in the middle of the connecting electrode 4c. On the other hand, on the other main surface of the piezoelectric ceramic substrate 1,
Square vibrating electrodes 5a, 5b for grounding are provided at positions facing the vibrating electrodes 2a, 4a and 3a, 4b, and these vibrating electrodes 5a, 5b are connected to connecting electrodes 5c, 5d.
It is connected to a capacitor electrode 5e facing the capacitor electrode 4d, and further connected to a terminal electrode 5f.

上記のように圧電セラミックス基板1を間にして対向す
る振動電極2a、 4aと5aとで一方の二重モードフ
ィルタを構成し、振動電極3a、 4bと5bとで他方
の二重モードフィルタを構成する。そして、圧電セラミ
ックス基板lを間にして対向するコンデンサ電極4d、
 5eでコンデンサを構成する。
As described above, the vibrating electrodes 2a, 4a and 5a facing each other with the piezoelectric ceramic substrate 1 in between constitute one double mode filter, and the vibrating electrodes 3a, 4b and 5b constitute the other double mode filter. do. and capacitor electrodes 4d facing each other with the piezoelectric ceramic substrate l in between;
5e constitutes a capacitor.

上記端子電極2c、 3cには入,出力端子6.7が半
田付は等にて接続され、端子電極5fにはアース端子8
が半田付は等にて接続されている。その結果、第3図に
示す等価回路が形成される。
Input and output terminals 6.7 are connected to the terminal electrodes 2c and 3c by soldering, etc., and a ground terminal 8 is connected to the terminal electrode 5f.
However, they are connected by soldering, etc. As a result, the equivalent circuit shown in FIG. 3 is formed.

上記圧電セラミックス基板lの振動電極2a、 4a。Vibrating electrodes 2a, 4a of the piezoelectric ceramic substrate l.

3a、 4bおよび5a、 5b上にはそれぞれワック
スやパラフィン等からなる空洞形成材(図示せず)が塗
布され、その後、外装樹脂9で封止することにより、空
洞形成材が外装樹脂9中に吸収されて、空洞IOが形成
される。このように振動電極部分のみ空洞lOが形成さ
れ、コンデンサ電極4d、 5a部分は外装樹脂9で固
定されるため、圧電セラ〔ツクス基板Iの振動電極で挟
まれた部分でのみ厚み縦振動が励起される。詳しくは、
対称モードと非対称モードの二重モードの振動が励起さ
れる。
A cavity-forming material (not shown) made of wax, paraffin, etc. is applied onto 3a, 4b and 5a, 5b, respectively, and then sealed with exterior resin 9, so that the cavity-forming material is injected into exterior resin 9. Upon absorption, a cavity IO is formed. In this way, the cavity 10 is formed only in the vibrating electrode part, and the capacitor electrodes 4d and 5a are fixed with the exterior resin 9, so that the thickness longitudinal vibration is excited only in the part sandwiched between the vibrating electrodes of the piezoelectric ceramic substrate I. be done. For more information,
Dual modes of vibration, symmetric and asymmetric modes, are excited.

上記空洞IOの形状は、振動電極の上下部が円弧状で、
両側部が直線状をなした非円形に形成されている。なお
、上記のような形状の空洞10を形成するには、先端部
が上記空洞IOとほぼ同一形状のコテを用いて空洞形成
材を塗布すればよい。空洞lOをこのような形状とする
ことにより、振動電極の各角部から空洞lOの周縁まで
の最短距離ddt  (第4図参照)を、圧電セラミッ
クス基板1の板厚tの等倍〜3倍の範囲に設定すること
ができる。即ち、 t≦d、、dl  ≦31 このような条件を満足することにより、本来必要なメイ
ンレスポンスを阻害することなく、十分なエネルギー閉
じ込めを行うことができ、スプリアス振動を抑制できる
0例えば、本発明者が中心周波数10.7MH,のフィ
ルタについてスプリアスレスポンス(通過帯域外減衰量
)を測定したところ、従来の円形空洞の場合には40d
Bであったのに対し、本発明の非円形空洞10では45
dBに改善できた。なお、振動電極の各角部から空洞I
Oの周縁までの最短路gla+ 、atをほぼ同等な距
離とすれば、さらに特性が向上することは勿論である。
The shape of the cavity IO is such that the upper and lower parts of the vibrating electrode are arcuate,
It is formed into a non-circular shape with straight sides. Note that in order to form the cavity 10 having the above shape, the cavity forming material may be applied using a trowel whose tip end has substantially the same shape as the cavity IO. By making the cavity lO into such a shape, the shortest distance ddt (see Fig. 4) from each corner of the vibrating electrode to the periphery of the cavity lO can be made equal to or three times the thickness t of the piezoelectric ceramic substrate 1. It can be set to a range of . That is, t≦d,, dl≦31 By satisfying these conditions, sufficient energy can be trapped without inhibiting the originally necessary main response, and spurious vibrations can be suppressed. The inventor measured the spurious response (attenuation outside the passband) of a filter with a center frequency of 10.7 MH, and found that it was 40 d in the case of a conventional circular cavity.
B, whereas in the non-circular cavity 10 of the present invention, it was 45
I was able to improve it by dB. In addition, from each corner of the vibrating electrode, the cavity I
Of course, if the shortest paths gla+ and at to the periphery of O are made approximately equal distances, the characteristics will be further improved.

また、対称モードと非対称モードの結合を疎とするため
に振動電極2a、 4aおよび3a、 4bの間隔δを
大きくした場合には、空洞lOを上下方向に引き延ばし
た形状にすれば、上記の条件を容易に満足することがで
きる。
Furthermore, if the spacing δ between the vibrating electrodes 2a, 4a and 3a, 4b is increased in order to make the coupling between the symmetrical mode and the asymmetrical mode sparse, the above conditions can be met by making the cavity lO elongated in the vertical direction. can be easily satisfied.

なお、空洞の形状は上記のように振動電極の上下部が円
弧状で、両側部が直線状をなした形状に限らず、楕円形
状や方形状など種々変更可能である。
Note that the shape of the cavity is not limited to the above-mentioned shape in which the upper and lower portions of the vibrating electrode are arcuate and both sides are linear, but can be changed to various shapes such as an elliptical shape or a rectangular shape.

また、本発明は同一基板上に二重モード共振子を2個設
けた圧電モノリシックフィルタに限らず、第5図のよう
に1個の二重モード共振子を形成したもの、あるいは3
個以上の二重モード共振子を形成したものでもよい。
Furthermore, the present invention is not limited to a piezoelectric monolithic filter in which two dual mode resonators are provided on the same substrate, but also a piezoelectric monolithic filter in which one double mode resonator is formed as shown in FIG.
It is also possible to form two or more dual mode resonators.

〔発明の効果〕 以上の説明で明らかなように、本発明によれば、空洞の
輪郭形状を、振動電極の各角部から空洞の周縁までの最
短距離が圧電セラミックス基板の板厚の等倍〜3倍の範
囲となるように非円形に形成したので、メインレスポン
スを阻害せずにスプリアス振動を抑制でき、特性の優れ
た二重モード共振子を得ることができる。
[Effects of the Invention] As is clear from the above description, according to the present invention, the contour shape of the cavity is such that the shortest distance from each corner of the vibrating electrode to the periphery of the cavity is equal to the thickness of the piezoelectric ceramic substrate. Since it is formed into a non-circular shape so as to have a range of ~3 times, spurious vibrations can be suppressed without interfering with the main response, and a dual mode resonator with excellent characteristics can be obtained.

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

第1図は本発明にかかる圧電共振子の一例の正面図、第
2図は第1図の■−■線断面図、第3図は圧電共振子の
等価回路図、第4図は振動電極部分の拡大図、第5図は
従来の圧電共振子の正面図、第6図は第5図のVl−V
l線断面図、第7図は振動電極部分の拡大図である。 !・・・圧電セラミックス基板、2a、3a、4a、4
b、5a、5・・・振動電極、 9・・・外装樹脂、 10・・・空洞。
Fig. 1 is a front view of an example of a piezoelectric resonator according to the present invention, Fig. 2 is a sectional view taken along the line ■-■ in Fig. 1, Fig. 3 is an equivalent circuit diagram of the piezoelectric resonator, and Fig. 4 is a vibrating electrode. An enlarged view of the part, Figure 5 is a front view of a conventional piezoelectric resonator, and Figure 6 is the Vl-V of Figure 5.
7 is an enlarged view of the vibrating electrode portion. ! ...Piezoelectric ceramic substrate, 2a, 3a, 4a, 4
b, 5a, 5... Vibrating electrode, 9... Exterior resin, 10... Cavity.

Claims (1)

【特許請求の範囲】[Claims] (1)圧電基板の一主面に対をなす入,出力用の方形振
動電極を隣接して形成し、他主面の上記振動電極と対向
する部位にアース用の方形振動電極を形成してなり、上
記振動電極の周囲に空洞を残して圧電基板の外周を外装
樹脂で封止してなるエネルギー閉じ込め型厚み縦振動モ
ードを利用した圧電共振子において、 上記空洞は、その輪郭が非円形でかつ振動電極の各角部
からの最短距離が圧電基板の板厚の等倍〜3倍の範囲に
形成されていることを特徴とする圧電共振子。
(1) A pair of rectangular vibrating electrodes for input and output are formed adjacent to each other on one main surface of the piezoelectric substrate, and a rectangular vibrating electrode for grounding is formed on the other main surface of the piezoelectric substrate at a portion facing the above-mentioned vibrating electrode. In a piezoelectric resonator using an energy-trap thickness longitudinal vibration mode in which the outer periphery of the piezoelectric substrate is sealed with an exterior resin while leaving a cavity around the vibrating electrode, the cavity has a non-circular outline. A piezoelectric resonator characterized in that the shortest distance from each corner of the vibrating electrode is formed within a range of equal to three times the thickness of the piezoelectric substrate.
JP32342689A 1989-12-13 1989-12-13 Piezoelectric resonator Pending JPH03184412A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP32342689A JPH03184412A (en) 1989-12-13 1989-12-13 Piezoelectric resonator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP32342689A JPH03184412A (en) 1989-12-13 1989-12-13 Piezoelectric resonator

Publications (1)

Publication Number Publication Date
JPH03184412A true JPH03184412A (en) 1991-08-12

Family

ID=18154553

Family Applications (1)

Application Number Title Priority Date Filing Date
JP32342689A Pending JPH03184412A (en) 1989-12-13 1989-12-13 Piezoelectric resonator

Country Status (1)

Country Link
JP (1) JPH03184412A (en)

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