JPH03218111A - Piezoelectric vibrator for overtone oscillation - Google Patents

Piezoelectric vibrator for overtone oscillation

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Publication number
JPH03218111A
JPH03218111A JP1430490A JP1430490A JPH03218111A JP H03218111 A JPH03218111 A JP H03218111A JP 1430490 A JP1430490 A JP 1430490A JP 1430490 A JP1430490 A JP 1430490A JP H03218111 A JPH03218111 A JP H03218111A
Authority
JP
Japan
Prior art keywords
vibration
electrode
frequency
overtone
vibration energy
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.)
Granted
Application number
JP1430490A
Other languages
Japanese (ja)
Other versions
JP2746278B2 (en
Inventor
Katsuyuki Nakamura
勝幸 中村
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.)
Daishinku Corp
Original Assignee
Daishinku Corp
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Filing date
Publication date
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Priority to JP2014304A priority Critical patent/JP2746278B2/en
Publication of JPH03218111A publication Critical patent/JPH03218111A/en
Application granted granted Critical
Publication of JP2746278B2 publication Critical patent/JP2746278B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Abstract

PURPOSE:To stably extract a desired frequency component without using together a resonance circuit or the like by attenuating or making leak the overtone vibration of a fundamental wave and low-order harmonic waves whose frequency is lower than the major vibration and undesired sub vibration whose frequency is high to extract the major vibration effectively. CONSTITUTION:A main vibration energy confinement part 2 is provided on the middle of a piezoelectric substrate 1 with electrodes 2a, 2b, a vibration energy propagation part 3 having an interruption frequency Fc higher than the interruption frequency fc is provided around the part 2, and a vibration energy absorbing part 4 having a cutoff frequency lower than the frequency Fc is provided on the outside of the part 3. The frequency Fc is set lower than the sub vibration frequency of the desired overtone vibration and higher than the major vibration frequency fo of the overtone vibration, the vibration energy absorbing part 4 absorbs the energy of the vibration mode of lower-order than the desired overtone order to make the sub vibration higher than the main vibration leak to the outside. Thus, all the undesired vibration energy is made to leak to the absorbing part 4 and the third overtone without undesired vibration is confined as the major vibration.

Description

【発明の詳細な説明】 〈産業上の利用分野〉 本発明は、オーバートーン用共振回路を必要とせずに所
望のオーバートーン周波数での発振を可能にするオーバ
ートーン発振用圧電振動子に関する。
DETAILED DESCRIPTION OF THE INVENTION <Industrial Application Field> The present invention relates to a piezoelectric vibrator for overtone oscillation that enables oscillation at a desired overtone frequency without requiring an overtone resonant circuit.

〈従来の技術〉 従来、ATカノト水晶板を用いた圧電振動子等において
オーバートーン振動を用いようとする場合、−・般的に
はこの圧電振動子を用いた発振回路に所望のオーバート
ーン周波数と合致するLC同調回路を挿入して、真性抵
抗をこのオーハートン周波数付近においてのみ大きくな
るようにしてオーバートーン周ei.数を取り出してい
た。
<Conventional technology> Conventionally, when trying to use overtone vibration in a piezoelectric vibrator using an AT-shaped crystal plate, it is generally necessary to set a desired overtone frequency to an oscillation circuit using this piezoelectric vibrator. By inserting an LC tuning circuit that matches the overtone frequency ei. He was taking out a number.

ところが、このように同調回路を挿入することは回路構
成の複雑化をまねき、また取り出したオハートーン振動
に対する副振動が十分に抑制されず、当該発振回路の周
波数が不安定になり、信頼性に欠ける欠点を有していた
However, inserting a tuned circuit in this way complicates the circuit configuration, and sub-oscillations relative to the extracted Ohartone vibration are not sufficiently suppressed, making the frequency of the oscillation circuit unstable and lacking reliability. It had drawbacks.

一方、圧電振動子単体でオーバートーン振動を実現しよ
うとする考案が特開昭61−236208号公報に開示
されている。これは、例えば第13図に示すように、圧
電基板1の中央部両面に円形の電極2,2′を設けて、
その周辺の振動エネルギ伝搬部3.3′の遮断周波数f
2に対し、中央電極2.2′の主振動周波数fIを低く
設定しその間にf2−f,なる遮断周波数差を設けて中
央電極を主振動エネルギ閉じ込め部とし、その周辺の振
動エネルギ伝If!j3.3’のさらに外周に遮断周波
数f3なる振動エネルギ吸収部4.4’(ただしf:+
<fz)を設けた構造である。
On the other hand, Japanese Patent Laid-Open No. 61-236208 discloses an idea for realizing overtone vibration with a single piezoelectric vibrator. For example, as shown in FIG. 13, circular electrodes 2 and 2' are provided on both sides of the central part of the piezoelectric substrate 1.
The cutoff frequency f of the vibration energy propagation section 3.3' around it
2, the main vibration frequency fI of the center electrode 2.2' is set low, and a cutoff frequency difference of f2-f is provided between them, so that the center electrode becomes the main vibration energy confinement part, and the vibration energy around it is transmitted If! Further on the outer periphery of j3.3', there is a vibration energy absorbing part 4.4' with a cutoff frequency f3 (however, f: +
<fz).

〈発明が解決しようとする課題〉 この従来例によれば、振動工矛ルギ伝搬部3,3の穂断
固波数12が高くなり、その為に基本波振動モートを含
む所望のオーハー1・−ン次数より低次の振動モートの
エネルキを漏洩させることは容易である。しかレながら
、所望のオーバートーン振動の主振動周波数付近に生じ
る不要な副振動周波数を減衰させることはできす、上記
同調回路を用いた場合と同様に所望の周波数か不安定乙
こなる問題かあった。
<Problems to be Solved by the Invention> According to this conventional example, the wave number 12 of the vibration wave propagation parts 3, 3 becomes high, and therefore the desired wave number 12 including the fundamental wave vibration mote is increased. It is easy to leak the energy of vibration motes of lower orders. However, it is possible to attenuate unnecessary sub-vibration frequencies that occur near the main vibration frequency of the desired overtone vibration, but as with the case of using the above-mentioned tuning circuit, there may be problems with the instability of the desired frequency. there were.

そこで本発明の目的1よ、振動エネルギ伝&部の遮断周
波数f2を所望のオーバートーン次数における主振動周
波数に対する不要振動周波数よりも低く設定することを
容易にすることにより、不要t振動エネルギをすへて吸
収部へ漏洩させることかでき、その結果、例えば不要振
動の生じない3次オーバートーンを主振動として閉じ込
めることを容易乙こする改良されたオーバートーン発振
用圧電振動子を提供することである。
Therefore, the first objective of the present invention is to easily set the cutoff frequency f2 of the vibration energy transmission section lower than the unnecessary vibration frequency with respect to the main vibration frequency in a desired overtone order, thereby eliminating all unnecessary vibration energy. By providing an improved piezoelectric vibrator for overtone oscillation, which can easily confine third-order overtones as main vibrations without causing unnecessary vibrations, for example. be.

(課題を解決するための手段〉 第1図:よ、本発明の構成を模型的に示す断面図である
。これにより本発明オーバートーン発振用圧電振動子の
構成を説明する。圧電基仮1の中央部に電極2a,2b
を設けることにより主振動エネルギ閉じ込め部2を設け
、その周囲に上記主振動エネルギ閉じ込め部の酋断周波
数fcよりも高い遮断周波数Fcをもつ振動エネルギ伝
搬部3を設け、更にその外側に上記遮断周波数Fcより
も低い遮断周波数をもつ振動エネルギ吸収部4を設け、
上記遮断周波数Fcが、所望のオーハートン振動の副振
動周波数よりも低く、かつ、このオハートーン振動の主
振動周波数foより高く設定されており、上記振動工矛
ルギ吸収部4が所望のオーバートーン次数より低次の振
動モート (基本波振動モードを含む)のエネルギを吸
収するとともに、上記主振動よりも高い副振動を外部へ
漏洩させるよう構成されている。
(Means for Solving the Problems) Fig. 1: This is a sectional view schematically showing the configuration of the present invention.The configuration of the piezoelectric vibrator for overtone oscillation of the present invention will be explained with this.Piezoelectric base 1 Electrodes 2a, 2b are placed in the center of
A main vibration energy confinement section 2 is provided by providing a main vibration energy confinement section 2, a vibration energy propagation section 3 having a cutoff frequency Fc higher than the cutoff frequency fc of the main vibration energy confinement section is provided around the main vibration energy confinement section 2; A vibration energy absorption section 4 having a cut-off frequency lower than Fc is provided,
The cutoff frequency Fc is set lower than the sub-vibration frequency of the desired O-Herton vibration and higher than the main vibration frequency fo of the O-Her-Tone vibration, and the vibration mechanical contradiction absorbing section 4 is set to be lower than the desired overtone order. It is configured to absorb the energy of low-order vibration motes (including fundamental wave vibration modes) and to leak secondary vibrations higher than the main vibrations to the outside.

本発明は種々の態様により実施することができるか、本
発明の特徴をなす前項は、圧電基板の片面のみに電極が
設けられ他の片面に電極不在部が形式された領域により
振動エネルギ電搬部が構成されていることである。第2
項記載の発明は電極不在部が圧電基板の片面のみCこ形
式されている態様のものであり、第3項記載の発明は電
極不在部が圧電基板の両面に形式されている態様のもの
である。
The present invention can be carried out in various ways, but the feature of the present invention is that vibration energy is transferred by a region in which an electrode is provided on only one side of a piezoelectric substrate and an electrode-free area is formed on the other side. This means that the department is composed of: Second
The invention described in item 3 is an embodiment in which the electrode-absent portion is formed in a C shape only on one side of the piezoelectric substrate, and the invention described in item 3 is an embodiment in which the electrode-absent portion is formed in a C shape on both sides of the piezoelectric substrate. be.

〈作用〉 本発明において、例えば第3次オーハー1・−ン振動(
振動周波数fo)を主振動として利用したい場合、基本
波振動(周波数f o/ 3 )および第3次オーハ−
トーン振動の不要な副振動(周波数f,,f2等)のエ
ネルギが実用上差支つかえない程度に低く抑えられる。
<Operation> In the present invention, for example, the third Oher-1 vibration (
If you want to use the vibration frequency fo) as the main vibration, the fundamental wave vibration (frequency fo/3) and the third order
The energy of unnecessary sub-vibrations (frequency f, f2, etc.) of tone vibration can be suppressed to a practically acceptable level.

これを経験則により説明する。This will be explained using empirical rules.

第2図に示すように、圧電基板1の中央部に設けられた
主振動エネルギ閉じ込め部を構成する中央部電極2aと
、圧電基板1の周辺部に設けられた振動エネルギ吸収部
を構成する周辺部電極4aとの間に形成される振動エネ
ルギ伝段部、すなわち電極不在部3の幅寸法Gを変化さ
せた場合の、圧電振動子のCI値(クリ.スタル・イン
ピーダンス、振動抵抗)の変化を第3図に示す。
As shown in FIG. 2, a central electrode 2a is provided at the center of the piezoelectric substrate 1 and constitutes a main vibration energy trapping section, and a peripheral electrode 2a is provided at the periphery of the piezoelectric substrate 1 and constitutes a vibration energy absorbing section. Changes in the CI value (crystal impedance, vibration resistance) of the piezoelectric vibrator when the width dimension G of the vibration energy transmission part formed between the external electrode 4a, that is, the electrode absent part 3, is changed. is shown in Figure 3.

これによれば、例えば電極不在部の幅寸法GがG.と比
較的大きいときは、基本波F。、3次オハート−ンF3
.5次オーバートーンF,ともにcr値が低く、当然に
基本波F。の周波数成分が最も強く、つづいて3次オー
ハ−トーン振動F3の周波数成分、5次オーバートーン
振動F,の周波数成分の順で弱くなるから、所望次数の
オーバートーン例えば3次オーバートーン成分のみを、
共振回路を併用することなく取り出すことは難しい。し
かし例えば電極不在部の幅寸法が62と比較的小さくな
ると、基本波F。の周波数成分が大きく減退するのに対
し、オーバートーン振動F3,F,の周波数成分は減退
せず、しかも、5次オハートーン振動F5の周波数成分
は3次オーバートーン振動F3の周波数成分に比べて弱
いから、共振回路を併用することなく3次オーバートー
ン振動F3の周波数成分を取り出すことができ、また例
えば、電極不在部の幅寸法が63と更に小さくなると、
基本波F。の周波数成分、並びに3次オーハ−トーン振
動F3の周波数成分がともに大きく減衰するのに対し,
、5次オ−ハ−ト−ン振動F,の周波数成分はイ成衰せ
ず、従って、共振回路を併用することなく5次オーバー
トーン振動F5の周波数成分を取り出すことができる。
According to this, for example, the width dimension G of the electrode absent portion is G. When it is relatively large, the fundamental wave F. , 3rd O'Hartton F3
.. The 5th overtone F has a low CR value, and is naturally the fundamental wave F. The frequency component is the strongest, followed by the frequency component of the third-order Ochertone vibration F3, and the frequency component of the fifth-order overtone vibration F. Therefore, the overtone of a desired order, for example, only the third-order overtone component, becomes weaker. ,
It is difficult to extract it without using a resonant circuit. However, if the width of the non-electrode portion is relatively small, for example 62, the fundamental wave F. The frequency component of the overtone vibration F3, F, is significantly reduced, whereas the frequency component of the overtone vibration F3, F, is not reduced, and the frequency component of the fifth-order Ohartone vibration F5 is weaker than the frequency component of the third-order overtone vibration F3. Therefore, the frequency component of the third overtone vibration F3 can be extracted without using a resonant circuit, and for example, if the width of the electrode-absent part is further reduced to 63,
Fundamental wave F. While the frequency components of , as well as the frequency components of the third-order Ocher tone vibration F3 are both greatly attenuated,
, the fifth-order overtone vibration F, do not undergo any decay, and therefore, the frequency component of the fifth-order overtone vibration F5 can be extracted without using a resonant circuit.

次に第4図!こ、コンピュータ・シュミレーションによ
る振動エネルギ伝{殺部3の遮断周波数Fcに重要な関
係があるプレートパンク量Rを変化させたときの主振動
(例えば3次オーバートーン振動の有用な周波数振動f
o)に対するその副振動(例えば3次オーバートーン振
動の不要な周波数振動f+,fz)の滅衰比の特性図を
示す。ここでプレートハノクiRとは、第2図に示すよ
うに圧電基板の厚さをt,振動エネルギ伝雁部3を構成
する基板片面の電極の厚さをSとするとき、S R一 し Cこより与えられる。これはまた、圧電基板の固有振動
数『。′と電極を付け1こ部分の固有振動数f。
Next is Figure 4! Vibration energy transfer by computer simulation {Main vibration (for example, useful frequency vibration f of third overtone vibration) when changing the plate puncture amount R, which has an important relationship with the cutoff frequency Fc of the killing section 3
Fig. 3 shows a characteristic diagram of the extinction ratio of sub-vibrations (for example, unnecessary frequency vibrations f+, fz of third-order overtone vibration) with respect to o). Here, plate hanoku iR means, as shown in Fig. 2, when the thickness of the piezoelectric substrate is t, and the thickness of the electrode on one side of the substrate constituting the vibration energy transmission goose section 3 is S, S R is C. It is given from this. This is also the natural frequency of the piezoelectric substrate. ′ and the natural frequency f of the first part with the electrode attached.

の差(f.’−fo)の固有振動数f。′に対する割合 f0 に相当する。また、第5図に圧電振動子のアドミクンス
の周波数特性図の一例を示す。
The natural frequency f of the difference (f.'-fo). It corresponds to the ratio f0 to '. Further, FIG. 5 shows an example of an admit frequency characteristic diagram of a piezoelectric vibrator.

なお、第4図に示す実験図は、実験を簡単化するため、
圧電基板の片面全面に付ける電極の厚さSを一様に変化
させて行っており、そのため、プレートハソク量の変化
に応して主振動エネルギ閉じ込め部2の遮断周波数fc
、および、振動エネルギ吸収部4の遮断周波数にも影響
を及ぼしている。
Note that the experimental diagram shown in Figure 4 is
This is done by uniformly changing the thickness S of the electrode attached to the entire surface of one side of the piezoelectric substrate, and therefore, the cutoff frequency fc of the main vibration energy confinement section 2 changes according to the change in the plate thickness.
, and also affects the cutoff frequency of the vibration energy absorbing section 4.

実験データによれば、プレートハソク量Rが0.005
よりも小さくなるほどに、主振動成分のアトミタンスに
対する副振動成分のアドミタンスの減衰比、すなわちス
プリアスレヘル(dB)が急増していることが認められ
る。従って、振動エネルギ伝雁部を構成する圧電基板片
面の電極層の厚さを適当に選定することにより、不要な
副振動成分を抑え込むことができる。
According to the experimental data, the plate hassock amount R is 0.005
It is recognized that as the value becomes smaller, the attenuation ratio of the admittance of the sub-vibration component to the atmittance of the main vibration component, that is, the spurious level (dB) increases rapidly. Therefore, by appropriately selecting the thickness of the electrode layer on one side of the piezoelectric substrate constituting the vibration energy transmission goose portion, unnecessary sub-vibration components can be suppressed.

〈実施例〉 第6図(al、(blに本発明の一実施例の平面図およ
び底面図を示す。
<Embodiment> Figures 6(al) and 6(bl) show a plan view and a bottom view of an embodiment of the present invention.

円形の圧電基{反11の表面には、その中央に電+】1
2か設けられその周囲に幅Gの電極不在部13が設けら
れ更にその外周・2こ電極14が設けられている。また
、圧電基板11の裏面には、全面に電極15が設けられ
ている。このような構造において、電極12とそれに対
応する電極15の一部分が主振動エネルギ閉じ込め部を
構成し、電極不在部13とそれに対応する電極15の一
部分が振動エネルギ伝搬部を構成し、電極14とそれに
対応する電極15の一部分が振動エネルギ吸収部を構成
している。中央電極12から圧電基板11の一端縁Aま
でリード電極16が形成され、外周電極1および裏面電
極15ば圧電基板11の反対側の端8MBまで延びてい
る。そして、円形圧電基仮11は両端縁A,Bて支持さ
れる。周波数調整工程において、裏面電極15の中央部
16に金属を芸着させて電極15の厚みを微調整するこ
とができる。
Circular piezoelectric base {The surface of the diagonal 11 has an electric +】1
Two electrode-free areas 13 having a width G are provided around the electrodes, and two electrodes 14 are provided around the outer periphery thereof. Moreover, an electrode 15 is provided on the entire back surface of the piezoelectric substrate 11. In such a structure, the electrode 12 and the corresponding part of the electrode 15 constitute the main vibration energy confinement part, the electrode absent part 13 and the corresponding part of the electrode 15 constitute the vibration energy propagation part, and the electrode 14 and the corresponding part of the electrode 15 constitute the vibration energy propagation part. A portion of the electrode 15 corresponding thereto constitutes a vibration energy absorption section. A lead electrode 16 is formed from the center electrode 12 to one end edge A of the piezoelectric substrate 11, and extends to the opposite end 8MB of the piezoelectric substrate 11 through the outer peripheral electrode 1 and the back electrode 15. The circular piezoelectric base 11 is supported by both end edges A and B. In the frequency adjustment step, the thickness of the electrode 15 can be finely adjusted by applying metal to the center portion 16 of the back electrode 15.

裏面の電極15の厚みは全面にわたって均一でな4 くてもよく、各構成部分に応して変化させることができ
る。同様にして、表面の電極12.14の厚みを個別に
設定することができる。各部の遮断周波数は圧電基板1
1の材質、厚み、両面に設けられた電極の材質、厚みに
依存しており、片側の電極の厚みを変えることにより遮
断周波数を制御することができる。
The thickness of the electrode 15 on the back surface does not have to be uniform over the entire surface, and can be changed depending on each component. Similarly, the thickness of the surface electrodes 12, 14 can be set individually. The cutoff frequency of each part is piezoelectric substrate 1
The cutoff frequency depends on the material and thickness of the electrode 1 and the material and thickness of the electrodes provided on both sides, and the cutoff frequency can be controlled by changing the thickness of the electrode on one side.

第7図に、前記実施例において、中央電極12の直径を
21とし、電極不在部13の幅寸法Gを変化させたとき
の基本波振動と3次オーバートーン振動に対する比抵抗
(G−00を1とする)の測定データを示す。寸法Gが
0.7以下になると基本波振動に対する比抵抗が3次オ
ーバートーンのそれを上まわり、寸法Gが0.4以下に
なると基本波振動に対する比抵抗が非常に太き《なるの
に比べ、3次オーバートーンに対する比抵抗は小さな値
に保たれている。
FIG. 7 shows the specific resistance (G-00) for the fundamental wave vibration and the third overtone vibration when the diameter of the central electrode 12 is 21 and the width G of the electrode absent area 13 is changed in the above embodiment. 1) is shown. When the dimension G becomes 0.7 or less, the resistivity to the fundamental wave vibration exceeds that of the third overtone, and when the dimension G becomes 0.4 or less, the resistivity to the fundamental wave vibration becomes very thick. In comparison, the resistivity for the third overtone is kept at a small value.

第8図に、前記と同じ実施例において、裏面電極15の
プレートハソク量Rを0.01とし、寸法Gを変化させ
たときの3次オーバートーンの主振動に対する不要な副
振動(スプリアス)の減衰量の測定値を示す。
FIG. 8 shows attenuation of unnecessary secondary vibrations (spurious) with respect to the main vibration of the tertiary overtone when the plate width R of the back electrode 15 is set to 0.01 and the dimension G is changed in the same embodiment as above. Indicates a measurement of a quantity.

第9図に、同し実施例において裏面電極15の厚みSを
変化させたときの3次オーノ入−トーンの主振動に対す
る不要な副振動(スプリアス)の減衰量の測定値を示す
FIG. 9 shows measured values of the amount of attenuation of unnecessary sub-vibration (spurious) with respect to the main vibration of the tertiary ohno tone when the thickness S of the back electrode 15 is changed in the same example.

さらに第10図に、同じ実施例における3次オーバート
ーンの周波数特性を示す。(a+図は裏面電極15のプ
レートハノク量R=0.003のもの、fbl図はR=
0.01のものである。
Furthermore, FIG. 10 shows the frequency characteristics of the third overtone in the same example. (The a+ figure is for the plate thickness R=0.003 of the back electrode 15, and the fbl figure is for R=
0.01.

第11図に本発明の他の実施例を示す。第6図の実施例
との相違点は、中央電極12と一体形成されるリード電
極16が中心角180゜の半円形に拡大され、それに応
じて外周電極14が中心角180゜の半円形に減縮され
たことてある。裏面には全面に裏面電極15か設けられ
ている。この実施例において、リード電極16と外周電
極14の設けられた外周部全体が振動エネルギ吸収部を
構成している。
FIG. 11 shows another embodiment of the present invention. The difference from the embodiment shown in FIG. 6 is that the lead electrode 16 formed integrally with the center electrode 12 is enlarged into a semicircle with a center angle of 180°, and the outer electrode 14 is accordingly formed into a semicircle with a center angle of 180°. There are some things that have been reduced. A back electrode 15 is provided on the entire back surface. In this embodiment, the entire outer circumference where the lead electrode 16 and the outer circumferential electrode 14 are provided constitutes a vibration energy absorbing section.

第12図に本発明のさ;)Sこ池の実施例を示す。FIG. 12 shows an embodiment of the present invention.

+al図が平面図、(blが底面図、(ci図かA−B
断面図である。図示の通りこの実施例の構造は、圧電基
板11の中点に対して点対称形である。これを説明する
と、圧電基板11の片面11aに、主振動エネルキ閉じ
込め部を構成する第1の中央部電極21と、その第1中
央部電極と一体形成され、かつ、その中央部電極21の
周囲の一部に形成された第1の周辺部電極22と、第1
の中央部電極21と第1の電極不在部23を介して形成
された第2の周辺部電極24とが設けられており、その
圧電基板11の他の片面1lbに、主振動エネルギ閉じ
込め部を構成する第2の中央部電極25と、その第2の
中央部電極25と一体形成され、かつ、上記第2の周辺
部電極24と対応する場所に形成された第3の周辺部電
極26と、第2の中央部電極25と第2の電極不在部2
7を介して形成された第4の周辺部電極28とが設けら
れており、第1および第4の周辺部電極22、28が相
対向する領域、並びに、第2および第3の周辺部電極2
426が相対向する領域が振動エネルギ吸収部を構成し
、第1および第2の電極不在部23.27の設けられた
領域か振動エネルギ伝搬部を構成している。
+al figure is top view, (bl is bottom view, (ci figure or A-B
FIG. As shown in the figure, the structure of this embodiment is point symmetrical with respect to the midpoint of the piezoelectric substrate 11. To explain this, on one side 11a of the piezoelectric substrate 11, a first center electrode 21 constituting the main vibration energy confinement section is formed integrally with the first center electrode, and the periphery of the center electrode 21 is a first peripheral electrode 22 formed in a part of the first peripheral electrode 22;
A central part electrode 21 and a second peripheral part electrode 24 formed through the first electrode absent part 23 are provided, and a main vibration energy confinement part is provided on the other side 1 lb of the piezoelectric substrate 11. a third peripheral electrode 26 formed integrally with the second central electrode 25 and corresponding to the second peripheral electrode 24; , second central electrode 25 and second electrode absent area 2
A fourth peripheral electrode 28 formed through the 7 is provided, and a region where the first and fourth peripheral electrodes 22 and 28 face each other, and a region where the second and third peripheral electrodes 2
The region where the electrodes 426 face each other constitutes a vibration energy absorbing portion, and the region where the first and second electrode absent portions 23 and 27 are provided constitutes a vibration energy propagation portion.

〈発明の効果〉 本発明によれば、主振動よりも周波数が低い基本波およ
び低次のオーバートーン振動のみでなく、主振動よりも
周波数が高い不要な副振動をも減衰または漏洩させて、
主振動のみを有効に取り出すことができるので、共振回
路等を併用することなく所望の周波数成分のみを安定に
取り出すことができる。
<Effects of the Invention> According to the present invention, not only fundamental waves and low-order overtone vibrations having a lower frequency than the main vibration, but also unnecessary sub-vibrations having a higher frequency than the main vibration are attenuated or leaked.
Since only the main vibration can be effectively extracted, only the desired frequency component can be stably extracted without using a resonant circuit or the like.

また、裏面全面、あるいは半面の比較的広い面積に電極
が設けられているので、周波数微調整工程における金属
蒸着作業に従来のように高度な位置精度か要求されず、
調整作業が容易になった。
In addition, since the electrodes are provided over a relatively large area on the entire back surface or half of the back surface, the metal deposition work in the frequency fine adjustment process does not require high positional accuracy as in the past.
Adjustment work has become easier.

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

第1図は本発明の構成を模型的に示す断面図、第2図は
本発明の作用を説明するための各部寸法を記入した断面
図、 第3図および第4図は本発明の作用を説明する特性図、 第5図はオーバートーン振動のアドミタンスの周波数特
性の一例を示す図、 第6図は、本発明の一実施例を示す図であって、(al
図は平面図、(b)図は底面図である。 第7図、第8図、第9図および第10図は第6図に示す
実施例の特性図、 第11図は本発明の他の実施例を示す図であって、fa
l図は平面図、fbl図はA−B断面図である。 第12図は本発明のさらに他の実施例を示す図であって
、(al図は平面図、fbl図は底面図、(C)図はA
−B断面図である。 第13図は従来例を示す断面図である。 1.11・・・圧電基板 2・・・主振動エネルギ閉じ込め部 3・・・振動エネルギ伝搬部 4・・・振動エネルギ吸収部 12・・・中央電極 13・・・電極不在部 14・・・周辺電極 1 5 ・裏面電極
Fig. 1 is a sectional view schematically showing the structure of the present invention, Fig. 2 is a sectional view with dimensions of each part to explain the function of the present invention, and Figs. 3 and 4 are sectional views showing the function of the present invention. FIG. 5 is a diagram showing an example of frequency characteristics of admittance of overtone vibration, and FIG. 6 is a diagram showing an example of the present invention.
The figure is a plan view, and the figure (b) is a bottom view. 7, 8, 9 and 10 are characteristic diagrams of the embodiment shown in FIG. 6, and FIG. 11 is a diagram showing another embodiment of the present invention.
Figure l is a plan view, and figure fbl is a sectional view taken along line A-B. FIG. 12 is a diagram showing still another embodiment of the present invention (al figure is a plan view, fbl figure is a bottom view, (C) figure is A
-B sectional view. FIG. 13 is a sectional view showing a conventional example. 1.11... Piezoelectric substrate 2... Main vibration energy confinement section 3... Vibration energy propagation section 4... Vibration energy absorption section 12... Center electrode 13... Electrode absent section 14... Peripheral electrode 1 5 ・Back electrode

Claims (3)

【特許請求の範囲】[Claims] (1)所望の次数にてオーバートーン振動する圧電振動
子であって、圧電基板中央部に上記所望次数のオーバー
トーン振動の主振動を閉じ込める主振動エネルギ閉じ込
め部を設け、その周囲に上記主振動エネルギ閉じ込め部
の遮断周波数fcよりも高い遮断周波数Fcをもつ振動
エネルギ伝搬部を設け、更にその外側に上記遮断周波数
Fcよりも低い遮断周波数をもつ振動エネルギ吸収部を
設け、上記遮断周波数Fcが、所望のオーバートーン振
動の副振動周波数よりも低く、かつ、このオーバートー
ン振動の主振動周波数foより高く設定されており、上
記振動エネルギ吸収部が基本波振動モードを含む所望の
オーバートーン次数より低次の振動モードのエネルギを
吸収するとともに、上記主振動より高い副振動を外部へ
漏洩させるよう構成されたことを特徴とするオーバート
ーン発振用圧電振動子。
(1) A piezoelectric vibrator that vibrates overtone at a desired order, in which a main vibration energy confinement section is provided in the center of the piezoelectric substrate to confine the main vibration of the overtone vibration of the desired order, and around the main vibration A vibration energy propagation part having a cut-off frequency Fc higher than the cut-off frequency fc of the energy confinement part is provided, and a vibration energy absorption part having a cut-off frequency lower than the cut-off frequency Fc is provided outside the vibration energy propagation part, and the cut-off frequency Fc is It is set lower than the secondary vibration frequency of the desired overtone vibration and higher than the main vibration frequency fo of this overtone vibration, and the vibration energy absorbing section is set to a frequency lower than the desired overtone order including the fundamental wave vibration mode. A piezoelectric vibrator for overtone oscillation, characterized in that the piezoelectric vibrator is configured to absorb the energy of the next vibration mode and to leak the secondary vibration higher than the main vibration to the outside.
(2)圧電基板の片面に、上記主振動エネルギ閉じ込め
部を構成する中央部電極と、上記振動エネルギ伝搬部を
構成する電極不在部と、上記振動エネルギ吸収部を構成
する周辺部電極か形成され、上記圧電基板の他の片面全
面に電極が形成されている、オーバートーン発振用圧電
振動子。
(2) On one side of the piezoelectric substrate, a central electrode that constitutes the main vibration energy trapping section, an electrode absent section that constitutes the vibration energy propagation section, and a peripheral electrode that constitutes the vibration energy absorption section are formed. , a piezoelectric vibrator for overtone oscillation, wherein an electrode is formed on the entire other surface of the piezoelectric substrate.
(3)圧電基板の片面に、上記主振動エネルギ閉じ込め
部を構成する第1の中央部電極と、その第1の中央部電
極と一体形成され、かつ、その中央部電極の周囲の一部
に形成された第1の周辺部電極と、上記第1の中央部電
極と第1の電極不在部を介して形成された第2の周辺部
電極とが設けられており、 その圧電基板の他の片面に、上記主振動エネルギ閉じ込
め部を構成する第2の中央部電極と、その第2の中央部
電極と一体形成され、かつ、上記第2の周辺部電極と対
応する場所に形成された第3の周辺部電極と、上記第2
の中央部電極と第2の電極不在部を介して形成された第
4の周辺部電極とが設けられており、 上記第1および第4の周辺部電極の対向する領域、並び
に、上記第2および第3の周辺部電極の対向する領域が
上記振動エネルギ吸収部を構成し、上記第1および第2
の電極不在部に対応する領域が上記振動エネルギ伝搬部
を構成している、オーバートーン発振用電極振動子。
(3) A first center electrode constituting the main vibration energy confinement section is formed integrally with the first center electrode on one side of the piezoelectric substrate, and a part of the periphery of the center electrode is formed integrally with the first center electrode. A first peripheral electrode is formed, and a second peripheral electrode is formed via the first center electrode and the first electrode absent area, and On one side, a second central electrode constituting the main vibration energy confinement section, and a second central electrode formed integrally with the second central electrode and corresponding to the second peripheral electrode. 3 peripheral electrode, and the second peripheral electrode.
a central electrode and a fourth peripheral electrode formed through the second electrode-absent part, and the opposing regions of the first and fourth peripheral electrodes and the second peripheral electrode are provided. and the opposing regions of the third peripheral electrode constitute the vibration energy absorbing section, and the first and second peripheral electrodes constitute the vibration energy absorbing section.
An electrode vibrator for overtone oscillation, wherein a region corresponding to the electrode absent part constitutes the vibration energy propagation part.
JP2014304A 1990-01-23 1990-01-23 Piezoelectric vibrator for overtone oscillation Expired - Lifetime JP2746278B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2014304A JP2746278B2 (en) 1990-01-23 1990-01-23 Piezoelectric vibrator for overtone oscillation

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2014304A JP2746278B2 (en) 1990-01-23 1990-01-23 Piezoelectric vibrator for overtone oscillation

Publications (2)

Publication Number Publication Date
JPH03218111A true JPH03218111A (en) 1991-09-25
JP2746278B2 JP2746278B2 (en) 1998-05-06

Family

ID=11857363

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2014304A Expired - Lifetime JP2746278B2 (en) 1990-01-23 1990-01-23 Piezoelectric vibrator for overtone oscillation

Country Status (1)

Country Link
JP (1) JP2746278B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US9503045B2 (en) 2015-01-19 2016-11-22 Seiko Epson Corporation Resonator element, resonator, oscillator, electronic apparatus, and moving object

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6179316A (en) * 1984-09-27 1986-04-22 Nippon Dempa Kogyo Co Ltd Piezo-electric vibrator
JPS61236208A (en) * 1985-04-11 1986-10-21 Toyo Commun Equip Co Ltd Piezoelectric resonator for over-tone oscillation

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6179316A (en) * 1984-09-27 1986-04-22 Nippon Dempa Kogyo Co Ltd Piezo-electric vibrator
JPS61236208A (en) * 1985-04-11 1986-10-21 Toyo Commun Equip Co Ltd Piezoelectric resonator for over-tone oscillation

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US9503045B2 (en) 2015-01-19 2016-11-22 Seiko Epson Corporation Resonator element, resonator, oscillator, electronic apparatus, and moving object

Also Published As

Publication number Publication date
JP2746278B2 (en) 1998-05-06

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