JPS60242713A - Electrode structure of piezoelectric transducer - Google Patents

Electrode structure of piezoelectric transducer

Info

Publication number
JPS60242713A
JPS60242713A JP9957584A JP9957584A JPS60242713A JP S60242713 A JPS60242713 A JP S60242713A JP 9957584 A JP9957584 A JP 9957584A JP 9957584 A JP9957584 A JP 9957584A JP S60242713 A JPS60242713 A JP S60242713A
Authority
JP
Japan
Prior art keywords
vibrating
electrode
branches
electrode structure
longitudinal
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
JP9957584A
Other languages
Japanese (ja)
Other versions
JPH0538483B2 (en
Inventor
Hiromi Ueda
上田 浩美
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.)
Citizen Holdings Co Ltd
Citizen Watch Co Ltd
Original Assignee
Citizen Holdings Co Ltd
Citizen Watch 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 Citizen Holdings Co Ltd, Citizen Watch Co Ltd filed Critical Citizen Holdings Co Ltd
Priority to JP9957584A priority Critical patent/JPS60242713A/en
Publication of JPS60242713A publication Critical patent/JPS60242713A/en
Publication of JPH0538483B2 publication Critical patent/JPH0538483B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H03ELECTRONIC CIRCUITRY
    • H03HIMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
    • H03H9/00Networks comprising electromechanical or electro-acoustic devices; Electromechanical resonators
    • H03H9/15Constructional features of resonators consisting of piezoelectric or electrostrictive material
    • H03H9/21Crystal tuning forks
    • H03H9/215Crystal tuning forks consisting of quartz

Abstract

PURPOSE:To prevent a crystal impedance (CI) from being increased even if a frequency is designed high by inverting alternately the polarity of plural electrodes fixed along the lengthwise direction of the vibrating branch in the electrode structure of the piezoelectric transducer having three vibrating branches activated in the longitudinal vibrating mode. CONSTITUTION:An E-type transducer 10 is formed incorporatedly with a crystal of uniform plate thickness and a metallic vapor-deposition film as electrodes is provided at the side face of the vibrating branches 11, 12, 13. Then the electrode films 14a, 15a and 14b, 15b are connected to the electrode terminals 14, 15 so that the polarity is opposite to each other. Then the electrode films 15b, 14b are formed in this order from the base on the other side face 11b by vapor-deposition. Thus, since the high order lengthwise longitudinal vibrating mode is excited easily, the E-type vibrator having a high frequency and low CI value is manufactured in the full range of an intermediate frequency band (300kHz-3MHz) without shortening the lengthwise of the vibrating branches.

Description

【発明の詳細な説明】 〔産業上の″fFIJ用分野〕 本発明は、長さたて振動モードで動作する。3本の振動
枝を有する圧電振動子(以下簡単のためE型振動子゛と
略称する)の高次振動を励振する電極構造に関する。
Detailed Description of the Invention [Industrial field of fFIJ] The present invention operates in a longitudinal vibration mode.A piezoelectric vibrator (hereinafter referred to as an E-type vibrator for simplicity) having three vibrating branches. It relates to an electrode structure that excites higher-order vibrations (abbreviated as ).

〔従来技術と問題点〕[Prior art and problems]

近年エレクトロニクスの発展に伴って一使用される水晶
振動子の周波数帯は拡大の一途をた片っている。高周波
帯では厚みすべりモードを利用し。
In recent years, with the development of electronics, the frequency band of the crystal oscillators used has continued to expand. In the high frequency band, the thickness shear mode is used.

たATカット振動子が主流であり一低周波帯では屈曲モ
ードを利用した音叉型振動子が主流となっている、一方
中周波帯では、長さたてモードを利用した振動子が注目
されはじめており、E型振動子もそのなかの一つである
。しかし従来のE型振動子は−1次振動モードの励振に
適し、た電極構造をとって℃・るため1周波数の高いE
型振動子を設計しようとすると一娠動枝の長さ寸法は、
非常に短かくしなければならず、その結果クリスタルイ
ンピーダンス(CI値)が大きくなってしまうという欠
点があった、 〔発明の目的〕 本発明の目的は2周波数を高く設計してもCI値が大き
くならないようなE型振動子の電極構造を提供すること
にある。
AT-cut vibrators are mainstream, and in the low frequency band, tuning fork type vibrators that use a bending mode are the mainstream.On the other hand, in the medium frequency band, vibrators that use a longitudinal mode are beginning to attract attention. The E-type resonator is one of them. However, the conventional E-type vibrator is suitable for excitation in the -1st vibration mode, and has a high-frequency E
When trying to design a type oscillator, the length dimension of the single moving branch is
[Object of the Invention] The purpose of the present invention is to make the crystal impedance (CI value) large as a result of having to make it extremely short. It is an object of the present invention to provide an electrode structure for an E-type vibrator that does not occur.

〔発明の構成〕[Structure of the invention]

この目的を達成するために一本発明では−長さたて振動
モードで動作する− 3本の振動枝を有する圧電振動子
の電極構造において一振動枝に固着されている電極の極
性が一振動枝の長手方向にそって交互に反転しているこ
とを特徴とし7ている。
In order to achieve this object, in the present invention, in the electrode structure of a piezoelectric vibrator having three vibrating branches, which operates in a longitudinal vibration mode, the polarity of the electrode fixed to one vibrating branch is set to one vibration. It is characterized by alternating inversions along the longitudinal direction of the branches.

〔発明の実施例〕[Embodiments of the invention]

以下図面に基づき本発明の詳細な説明する。 The present invention will be described in detail below based on the drawings.

第1図は本発明の一実施例を示す斜視図である。FIG. 1 is a perspective view showing an embodiment of the present invention.

E型振動子10はm=様な板厚の水晶から一体に形成さ
れており、振動技111113の側面には、電極として
金属の蒸着膜がもうけられている、例えば、振動技11
の一方の側面11a上には電極膜IAa−15aが各々
独立に基部側からこの順に蒸着により形成されている。
The E-type vibrator 10 is integrally formed from crystal with a plate thickness of m=, and a metal vapor-deposited film is formed as an electrode on the side surface of the vibration technique 111113.
Electrode films IAa-15a are independently formed on one side surface 11a of the electrode film IAa-15a in this order from the base side by vapor deposition.

そして電極膜1da−15aは極性が互℃・に逆極性と
なるように電極端子14−15に接続されている。そし
て振動技11の他方の側面1ib上には電極膜15b−
1abがやはり基部側からこの順に蒸着にて形成されて
いる。そして電極膜1db−15bの極性も互いに逆極
性となるよう電極端子1115に接続されており、それ
と共に電極膜IAaと15b−15aとtabは夫々枝
を挾んで逆極性にて対向配置されている。振動技12−
13の電極配置も同様である。E型振動子10の電極端
子1115に2次の長さたて振動モードの共振周波数に
等しい周波数の交流電圧を印加すると振動技11111
3の巾方向には一矢印で示す向きの駆動電界(以下簡単
に平行電界と称する)が発生する。その結果−振動技1
1.12−13は、水晶の逆圧電効果によって、長手方
向にのび縮みのひずみ成分を伴った2次の長さたて振動
を行う。この場合振動技11と16は同相で−振動枝1
2は逆相で振動する。
The electrode films 1da-15a are connected to electrode terminals 14-15 so that their polarities are opposite to each other. Then, on the other side surface 1ib of the vibration technique 11, an electrode film 15b-
1ab are also formed by vapor deposition in this order from the base side. The electrode films 1db-15b are connected to the electrode terminal 1115 so that the polarities are opposite to each other, and the electrode films IAa, 15b-15a and tab are arranged opposite to each other with opposite polarities between the branches. . Vibration technique 12-
The arrangement of electrodes No. 13 is also similar. When an AC voltage with a frequency equal to the resonance frequency of the secondary longitudinal vibration mode is applied to the electrode terminal 1115 of the E-type vibrator 10, the vibration technique 11111
In the width direction of 3, a driving electric field (hereinafter simply referred to as a parallel electric field) is generated in the direction indicated by an arrow. The result - vibration technique 1
1.12-13 performs second-order longitudinal vibration accompanied by a strain component of expansion and contraction in the longitudinal direction due to the inverse piezoelectric effect of the crystal. In this case, vibration techniques 11 and 16 are in phase - vibration branch 1
2 vibrates in opposite phase.

第2図は本発明の他の実施例を示す斜視図である。本実
施例においては振動技212123の上下面に金属の蒸
着膜がもうけられていて一駆動電界の方向は振動技の厚
み方向(以下簡単に垂直電界と称す)になっている。電
極配置と振動子の動作については前記第1図の実施例と
同様である。
FIG. 2 is a perspective view showing another embodiment of the invention. In this embodiment, a metal vapor deposited film is formed on the upper and lower surfaces of the vibration technique 212123, and the direction of the driving electric field is the thickness direction of the vibration technique (hereinafter simply referred to as a vertical electric field). The electrode arrangement and the operation of the vibrator are the same as in the embodiment shown in FIG. 1 above.

第3図は本発明の他の実施例を示す斜視図である。、E
型振動子60は3次の長さたて振動モードで動作する、
電極配置については−例えば振動技31の同一側面−3
18は極性が交互に反転した3つの電極35.66−3
7が配置されており、振動技61の反対側の同一側面3
1bにも同様の電極が配置されている、他の振動技31
33の電極配置も同様である。この場合のE型振動子の
駆動は平行電界で行われる。第3図の実施例に対応する
実施例とl、て−雷、極配置は振動技の上下面にもうけ
、駆動は垂直電界で行う方法があるが一図示は省略する
FIG. 3 is a perspective view showing another embodiment of the present invention. , E
The mold vibrator 60 operates in a third-order longitudinal vibration mode.
Regarding electrode placement - for example, the same side of vibration technique 31 - 3
18 is three electrodes 35.66-3 whose polarity is alternately reversed.
7 is placed, and the same side 3 opposite the vibration technique 61
Other vibration technique 31 where similar electrodes are placed in 1b
The arrangement of electrodes 33 is also similar. In this case, the E-type vibrator is driven by a parallel electric field. In an embodiment corresponding to the embodiment shown in FIG. 3, there is a method in which the pole arrangement is provided on the upper and lower surfaces of the vibrating device and the driving is performed using a vertical electric field, but this method is omitted from illustration.

以上の説明から明らかなように一般に0次(n=1、l
:l 4・・・・・・)の長さたて振動モードを励振す
る場合は一極性が交互に反転するn個の電極を配置すれ
ばよく一電極を振動技の側面にもうけるか、上下面にも
うけるかは一駆動電界を平行電界とするか一垂直電界と
するかによって決めればよいことがわかる。以上の実施
例では、振動子の材質は水晶でできている場合について
説明してきたが1本発明は材質が水晶に限定されるもの
ではなく、他の圧電材−例えば−タンタル酸リチウム−
ニオブ酸リチウム、セラミックス等に適用できることは
明らかである、又E型振動子の形状も一3大の場11)
I朽の妨由寸炊が笛りい場合に限らず一枝巾寸法が互い
に異なっている場合にも適用できるものである。
As is clear from the above explanation, it is generally 0th order (n=1, l
:l 4...) When exciting the vertical vibration mode, it is sufficient to arrange n electrodes whose polarity is alternately reversed. Either place one electrode on the side of the vibration technique, or It can be seen that whether to apply the driving electric field to the lower surface can be determined depending on whether the driving electric field is a parallel electric field or a perpendicular electric field. In the above embodiments, a case has been described in which the material of the vibrator is quartz; however, the present invention is not limited to quartz, and may be made of other piezoelectric materials such as lithium tantalate.
It is clear that it can be applied to lithium niobate, ceramics, etc., and the shape of the E-type resonator is also applicable to 13 major fields11)
This can be applied not only to cases where the length of the pipe is different, but also to cases where the width of one branch is different from each other.

〔発明の効果〕〔Effect of the invention〕

本発明によれば一高次の長さたて撮動モードが容易に励
振できるため一振動枝の長さ寸法は短かくすることなく
、高い周波数で−低いCI値をもったE型振動子が中周
波帯(300KHz〜3’MHz)の全レンジで製造で
きるようになり、中周波帯振動子の周波数拡大に対する
本発明の効果は大きい。
According to the present invention, since the first higher-order length vertical imaging mode can be easily excited, the length dimension of one vibration branch does not need to be shortened, and an E-type vibrator with a -low CI value is produced at high frequencies. can now be manufactured in the entire range of medium frequency bands (300 KHz to 3'MHz), and the present invention has a great effect on frequency expansion of medium frequency band vibrators.

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

第1図は本発明の実施例の電極構造を示す斜視図で一2
次の長さたてモードを励振する電界は平行電界の場合で
ある。 第2図は本発明の他の実施例の電極構造を示す斜視図で
、2次の長さたてモードを励振する電界は垂直電界の場
合である。 第3図は本発明の他の実施例を示す斜視図で一3次の長
さたてモードを励振する電界は平行電界の場合である。 ′ 10−30・・・・・・E型振動子。 11 11 11 21 21 2.11 31313
3・・・・・・振動技− 1da−15a−35−66−37・・・・・・金属の
蒸着膜電極。 特許出願人 シチズン時計株式会社
FIG. 1 is a perspective view showing the electrode structure of an embodiment of the present invention.
The next electric field that excites the longitudinal mode is a parallel electric field. FIG. 2 is a perspective view showing the electrode structure of another embodiment of the present invention, in which the electric field that excites the second-order longitudinal mode is a vertical electric field. FIG. 3 is a perspective view showing another embodiment of the present invention, in which the electric field that excites the 13th-order longitudinal mode is a parallel electric field. ' 10-30...E-type vibrator. 11 11 11 21 21 2.11 31313
3... Vibration technique - 1da-15a-35-66-37... Metal vapor deposited film electrode. Patent applicant Citizen Watch Co., Ltd.

Claims (1)

【特許請求の範囲】[Claims] 長さたて振動モードで動作する3本の振動枝を有する圧
電振動子の電極構造において一振動枝の長手方向に沿っ
て固着されている複数の電極の極性が、交互に反転して
いることを特徴とする圧電振動子の電極構造。
In the electrode structure of a piezoelectric vibrator having three vibrating branches that operate in a longitudinal vibration mode, the polarity of the plurality of electrodes fixed along the longitudinal direction of one vibrating branch is alternately reversed. An electrode structure of a piezoelectric vibrator featuring:
JP9957584A 1984-05-17 1984-05-17 Electrode structure of piezoelectric transducer Granted JPS60242713A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9957584A JPS60242713A (en) 1984-05-17 1984-05-17 Electrode structure of piezoelectric transducer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9957584A JPS60242713A (en) 1984-05-17 1984-05-17 Electrode structure of piezoelectric transducer

Publications (2)

Publication Number Publication Date
JPS60242713A true JPS60242713A (en) 1985-12-02
JPH0538483B2 JPH0538483B2 (en) 1993-06-10

Family

ID=14250903

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9957584A Granted JPS60242713A (en) 1984-05-17 1984-05-17 Electrode structure of piezoelectric transducer

Country Status (1)

Country Link
JP (1) JPS60242713A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002118441A (en) * 2000-10-10 2002-04-19 Citizen Watch Co Ltd Torsional vibrator

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5760720A (en) * 1980-09-26 1982-04-12 Seiko Instr & Electronics Ltd Tuning fork type quartz vibrator
JPS58111515A (en) * 1981-12-25 1983-07-02 Citizen Watch Co Ltd Crystal oscillator
JPS58205318A (en) * 1982-05-25 1983-11-30 Citizen Watch Co Ltd Electrode construction of piezoelectric crystal oscillator

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5760720A (en) * 1980-09-26 1982-04-12 Seiko Instr & Electronics Ltd Tuning fork type quartz vibrator
JPS58111515A (en) * 1981-12-25 1983-07-02 Citizen Watch Co Ltd Crystal oscillator
JPS58205318A (en) * 1982-05-25 1983-11-30 Citizen Watch Co Ltd Electrode construction of piezoelectric crystal oscillator

Also Published As

Publication number Publication date
JPH0538483B2 (en) 1993-06-10

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