JPS59148421A - Piezoelectric resonator - Google Patents

Piezoelectric resonator

Info

Publication number
JPS59148421A
JPS59148421A JP2260383A JP2260383A JPS59148421A JP S59148421 A JPS59148421 A JP S59148421A JP 2260383 A JP2260383 A JP 2260383A JP 2260383 A JP2260383 A JP 2260383A JP S59148421 A JPS59148421 A JP S59148421A
Authority
JP
Japan
Prior art keywords
piezoelectric substrate
oscillation
length
resonance frequency
cross
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
JP2260383A
Other languages
Japanese (ja)
Inventor
Takamichi Kitajima
北嶋 宝道
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 JP2260383A priority Critical patent/JPS59148421A/en
Publication of JPS59148421A publication Critical patent/JPS59148421A/en
Pending 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
    • H03H9/02Details
    • H03H9/02007Details of bulk acoustic wave devices
    • H03H9/02157Dimensional parameters, e.g. ratio between two dimension parameters, length, width or thickness
    • 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
    • H03H9/17Constructional features of resonators consisting of piezoelectric or electrostrictive material having a single resonator

Abstract

PURPOSE:To eliminate the spurious oscillation at the operating frequency band by adjusting the lengthwise size of a piezoelectric substrate so as to take out the harmonics of oscillation where the resonance frequency is decided by the length of the lengthwise side of the piezoelectric substrate generated in the piezoelectric substrate from the operating frequency band. CONSTITUTION:The length l of the piezoelectric substrate 1 is adjusted so that the harmonics of the oscillation where the resonance frequency is decided by the length of the lengthwise side of the piezoelectric substrate 1 generated in the piezoelectric substrate 1 together with the cross section contour shear oscillation are taken out of the frequency band between the resonance frequency and the anti-resonance frequency of the cross section contour shear oscillation of the piezoelectric substrate 1. That is, in taking the thickness (t) of the piezoelectric substrate 1 as t=614mum, the width (w) as w=736mum as constant values, and in cutting the length l in the range from 5,200mum to 3,800mum by 100mum each by a dicing cut machine, the resonance characteristic is measured by fitting a lead to electrodes 2, 3 of the piezoelectric substrate 1. In taking the l as l=4,000mum, the spurious radiation (s) by the oscillation of lengthwise side is taken out of the frequency band between the resonance frequency fr of the cross section contour oscillation of the piezoelectric substrate 1 and the anti-resonance frequency fa.

Description

【発明の詳細な説明】 共術分肚 本発明は直方体形Z状を有する圧電基板が断面輪郭スベ
リ振動モードで振動する圧電共振子に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a piezoelectric resonator in which a piezoelectric substrate having a rectangular parallelepiped Z shape vibrates in a cross-sectional profile sliding vibration mode.

従来技術。Conventional technology.

従来より、この種の圧電共振子としては、第1図および
第2図に示すように、長さ4、巾W1厚さくの直方体形
状を有する圧電基板1の相対向する両生面に夫々電極2
,3を形成し、上記圧電基板1を[1]Wの方向に下で
示すように分極させたものが知られている。
Conventionally, as shown in FIGS. 1 and 2, this type of piezoelectric resonator has a piezoelectric substrate 1 having a rectangular parallelepiped shape with a length of 4 and a width of W1 in thickness.
, 3, and the piezoelectric substrate 1 is polarized in the [1]W direction as shown below.

ところで、上記の如き圧電共振子においては、圧電基板
1の厚さtおよび[1]Wは、使用周波数が定まれば一
義的に定まるのに対し、長さeはe≧2Wてあればよい
ことから、使用周波数か2メガヘルツ前後ではl=50
00μmと一定の寸法としていた。
By the way, in the piezoelectric resonator as described above, the thickness t and [1]W of the piezoelectric substrate 1 are uniquely determined once the operating frequency is determined, whereas the length e only needs to be e≧2W. Therefore, l = 50 at the operating frequency of around 2 MHz.
The size was set to be constant at 00 μm.

上記のように、圧電基板1の長手方向の長さ4を一定と
すると、使用周波数によっては、圧電基板1の断面輪郭
スベリ振動とともに、圧電基板1の上記長さβを基とし
た辺振動の高調波によるスプリアスが上記圧電基板1の
断面輪郭スベリ振動の共振周波数frと反共振周波数「
aとの間に現れる。たとえば、t=614μm、w==
614Q’l。
As mentioned above, if the length 4 in the longitudinal direction of the piezoelectric substrate 1 is constant, depending on the frequency of use, not only the cross-sectional contour sliding vibration of the piezoelectric substrate 1 but also the side vibration based on the above-mentioned length β of the piezoelectric substrate 1 may occur. The spurious due to harmonics is the resonant frequency fr and the anti-resonant frequency of the cross-sectional contour sliding vibration of the piezoelectric substrate 1.
Appears between a. For example, t=614μm, w==
614Q'l.

g=5o ooμmで使用周波数が2.225メガヘル
ツの場合、第3図に示すように、共振周波数「r=2.
160メガヘルツと反共振周波数fa:=2.280メ
ガヘルツとの1hjにスプリアスSが現れ、このような
圧電共振子を発振子やフィルタとして使用すると、発振
周波数がジャンプしたり群遅延時間特性が乱れたりする
問題があった。
When g=5oooμm and the working frequency is 2.225 MHz, as shown in FIG. 3, the resonant frequency "r=2.
Spurious S appears at 1hj between 160 MHz and anti-resonance frequency fa:=2.280 MHz, and when such a piezoelectric resonator is used as an oscillator or filter, the oscillation frequency may jump or the group delay time characteristics may be disturbed. There was a problem.

発明の目的 本発明は従来の圧電共振子における上記問題を解消すべ
くなされたものであって、その目間は、直方体形状の圧
電基板の断面輪郭スベリ振動を利用する圧電共振子にお
いて、圧電基板の長手方向の寸法を調整することにより
、圧電基板に発生する圧電基板の長手方向の辺の長さで
共振周波数が定まる振動の高調波を使用周波数帯域から
外し、圧電共振子の使用周波数帯における不用振動を除
去することである。
OBJECTS OF THE INVENTION The present invention has been made to solve the above-mentioned problems in conventional piezoelectric resonators. By adjusting the longitudinal dimension of the piezoelectric resonator, harmonics of vibrations generated in the piezoelectric substrate, whose resonant frequency is determined by the length of the longitudinal side of the piezoelectric substrate, can be removed from the operating frequency band. The purpose is to eliminate unnecessary vibrations.

発明の要旨 本発明を要約すれば、直方体形状を有する圧電基板か断
面輪郭スベリ振動で振動する圧電共振子であって、上記
圧電基板に断面輪郭スベリ振動とともに発生する上記圧
電基板の長手方向の辺の長さで共振周波数が定まる振動
の高調波が上記圧電基板の断面輪郭スベリ振動の共振周
波数と反共振周波数との間の周波数帯域から外れるよう
に圧電基板の長手方向の寸法を調整するようにしたこと
を特徴とする圧電共振子である。
SUMMARY OF THE INVENTION To summarize the present invention, there is provided a piezoelectric resonator that vibrates with a cross-sectional contour sliding vibration of a piezoelectric substrate having a rectangular parallelepiped shape, the piezoelectric resonator vibrating along a longitudinal side of the piezoelectric substrate that occurs along with cross-sectional contour sliding vibration in the piezoelectric substrate. The longitudinal dimensions of the piezoelectric substrate are adjusted so that the harmonics of the vibration, whose resonance frequency is determined by the length of the piezoelectric substrate, are out of the frequency band between the resonant frequency and anti-resonance frequency of the cross-sectional contour of the piezoelectric substrate and the anti-resonance frequency of the sliding vibration. This piezoelectric resonator is characterized by the following characteristics.

実施例 以下、添付図面を参照して本発明の詳細な説明する。Example Hereinafter, the present invention will be described in detail with reference to the accompanying drawings.

本発明においては、第1図および第2図に示すように、
長さ4、巾W、厚さtの直方体形状を有する圧電基板1
の相対向する両主面に夫々電極2゜3を形成し、上記圧
電基板1を巾Wの方向にPで分極させて、圧電基板1の
断面輪郭スベリ振動を利用する圧電共振子において、上
記長さeを次のように調整する。
In the present invention, as shown in FIGS. 1 and 2,
Piezoelectric substrate 1 having a rectangular parallelepiped shape with length 4, width W, and thickness t
In the piezoelectric resonator that utilizes the sliding vibration of the cross-sectional contour of the piezoelectric substrate 1, the piezoelectric substrate 1 is polarized at P in the direction of the width W by forming electrodes 2.3 on both opposing principal surfaces of the piezoelectric substrate 1, respectively. Adjust the length e as follows.

すなわち、上記圧電基板1に断面輪郭スベリ振動ととも
に発生する上記圧電基板1の長手方向の辺の長さで共振
周波数が定まる振動の高調波が上記圧電基板1の断面輪
郭スベリ振動の共振周波数と反共振周波数との間の周波
数帯域から外れるように、圧電基板1の上記長さlを調
整する。
That is, the harmonics of the vibration, whose resonant frequency is determined by the length of the longitudinal side of the piezoelectric substrate 1, which occurs in the piezoelectric substrate 1 along with the cross-sectional contour sliding vibration, are opposite to the resonant frequency of the cross-sectional contour sliding vibration of the piezoelectric substrate 1. The length l of the piezoelectric substrate 1 is adjusted so that it is out of the frequency band between the resonance frequency and the resonance frequency.

具体的には、上記圧電基板1の厚み【をL=614μm
、巾WをW=736μmの一定値とし、長さeをN=5
200.c+mから3800μmの範囲で100μ■1
毎にグイシングカゾト機(図示せず。うにてカントし、
圧電基板1の電極2,3にリード線(図示せず。)を夫
々取り付けた状態で共振特性を測定する。たとえば、1
=5200μm。
Specifically, the thickness of the piezoelectric substrate 1 [L=614 μm
, the width W is a constant value of W=736 μm, and the length e is N=5.
200. 100μ■1 in the range from c+m to 3800μm
Each time, the Guising Kazoto machine (not shown) cant the sea urchin,
Resonance characteristics are measured with lead wires (not shown) attached to the electrodes 2 and 3 of the piezoelectric substrate 1, respectively. For example, 1
=5200μm.

4500μm、4200μmおよび4000μmでは夫
々第4図、第5図、第6図および第7図に夫々示すよう
な結果を得る。
At 4500 μm, 4200 μm, and 4000 μm, the results shown in FIGS. 4, 5, 6, and 7, respectively, are obtained.

上記第4図、第5図、第6図および第7図から明らかな
ように、6=5200μmの場合は2.2メガヘルツ付
近に、1=4500μmの場合は225メガヘルツ付近
に、l=4200μmの場合は2.27メガヘルツ付近
に、また、eに4000μmの場合は2゜33メガヘル
ツ付近に、夫々圧電基板1の長手方向の辺振動によるス
プリアスSが生じる。
As is clear from the above figures 4, 5, 6, and 7, when 6 = 5200 μm, the frequency is around 2.2 MHz, when 1 = 4500 μm, the frequency is around 225 MHz, and when l = 4200 μm, the frequency is around 2.2 MHz. When e is 4000 .mu.m, spurious S is produced near 2.27 MHz, and when e is 4000 .mu.m, near 2.33 MHz due to side vibration in the longitudinal direction of the piezoelectric substrate 1.

一方、上記圧電基板1の断面輪郭振動の共振周波数【r
は[r−4−2,17メガヘルツであり、反共振周波数
faはfa*2.30メガヘルツである。
On the other hand, the resonance frequency [r
is [r-4-2.17 MHz, and the anti-resonant frequency fa is fa*2.30 MHz.

従って、L=614μm 、w=736μmの場合は、
l=4000μmとすれば、圧電基板1の長手方向の辺
振動によるスプリアスSは、上記圧電基板1の断面輪郭
振動の共振周波数frと反共振周波数faとの間の周波
数帯域から外れ、上記1モ電共振子を発振子やフィルタ
として使用した場合、安定な発振特性および良好な群遅
延特性を得る。
Therefore, when L=614μm and w=736μm,
If l = 4000 μm, the spurious S caused by the side vibration in the longitudinal direction of the piezoelectric substrate 1 deviates from the frequency band between the resonant frequency fr of the cross-sectional contour vibration of the piezoelectric substrate 1 and the anti-resonant frequency fa, and When an electric resonator is used as an oscillator or filter, stable oscillation characteristics and good group delay characteristics are obtained.

t=614μm、w=736μm以外の場合も、上記と
全く同様にしてlの長さを実験的に定めることができる
Even in cases other than t=614 μm and w=736 μm, the length of l can be determined experimentally in exactly the same manner as above.

発明の効果 以上、詳述したことからも明らかなように、本発明は、
直方体状の圧電基板の断面輪郭振動モードを利用する圧
電共振子において圧電基板の長手方向の寸法を調整して
使用周波数帯域から圧電基板の長手方向の辺の長さで共
振周波数が定まる振動高調波が外れるようにしたから、
圧電共振子の使用周波数帯における不用振動がなくなり
、良好な共振特性を有する圧電共振子を得ることができ
る。
Effects of the Invention As is clear from the detailed explanation, the present invention has the following effects:
In a piezoelectric resonator that uses the cross-sectional contour vibration mode of a rectangular parallelepiped piezoelectric substrate, the longitudinal dimension of the piezoelectric substrate is adjusted to generate vibration harmonics whose resonant frequency is determined by the length of the longitudinal side of the piezoelectric substrate from the operating frequency band. Because I made it come off,
Unwanted vibrations in the frequency band in which the piezoelectric resonator is used are eliminated, and a piezoelectric resonator having good resonance characteristics can be obtained.

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

第1図は断面輪郭振動を行う圧電共振子の斜視図、第2
図は第1図の圧電共振子の分極説明図、第3図は従来の
圧電共振子の挿入損失特性図、第4図、第5図、第6図
および第7図は夫々圧電基板の長平方間の長さを種々変
化させた場合の挿入損失特性図である。 1・・・圧電基板、2,3・・・電極、【・・・厚さ、
W・・・巾、l・・・長さ、S・・・スプリアス。 特許出願人 株式会社村田製作所 代理人デ理士青山葆ほか2名 7s1 図 第2図
Figure 1 is a perspective view of a piezoelectric resonator that performs cross-sectional contour vibration;
The figure is an explanatory diagram of the polarization of the piezoelectric resonator in Figure 1, Figure 3 is an insertion loss characteristic diagram of a conventional piezoelectric resonator, and Figures 4, 5, 6, and 7 are the lengths of the piezoelectric substrates, respectively. It is an insertion loss characteristic diagram when the length between squares is changed variously. 1... Piezoelectric substrate, 2, 3... Electrode, [... Thickness,
W...width, l...length, S...spurious. Patent Applicant: Murata Manufacturing Co., Ltd. Agent, Physician Aoyama Hajime, and 2 others 7s1 Figure 2

Claims (1)

【特許請求の範囲】[Claims] (1)直方体形状を有する圧電基板が断面輪郭スベリ振
動で振動する圧電共振子であって、上記圧電基板に断面
輪郭スベリ振動とともに発生する上記圧電基板の長手方
向の辺の長さで共振周波数が定まる振動の高調波が上記
圧電基板の断面輪郭スベリ振動の共振周波数と反共振周
波数との間の周波数帯域から外れるように圧電基板の長
平方向の寸法を調整するようにしたことを特徴とする圧
電共振子。
(1) A piezoelectric resonator in which a piezoelectric substrate having a rectangular parallelepiped shape vibrates with cross-sectional contour sliding vibration, and the resonant frequency is determined by the length of the longitudinal side of the piezoelectric substrate that occurs in the piezoelectric substrate along with cross-sectional contour sliding vibration. A piezoelectric device characterized in that the dimension in the longitudinal direction of the piezoelectric substrate is adjusted so that the harmonics of the determined vibration are out of a frequency band between the resonance frequency and the anti-resonance frequency of the cross-sectional contour sliding vibration of the piezoelectric substrate. resonator.
JP2260383A 1983-02-14 1983-02-14 Piezoelectric resonator Pending JPS59148421A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2260383A JPS59148421A (en) 1983-02-14 1983-02-14 Piezoelectric resonator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2260383A JPS59148421A (en) 1983-02-14 1983-02-14 Piezoelectric resonator

Publications (1)

Publication Number Publication Date
JPS59148421A true JPS59148421A (en) 1984-08-25

Family

ID=12087412

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2260383A Pending JPS59148421A (en) 1983-02-14 1983-02-14 Piezoelectric resonator

Country Status (1)

Country Link
JP (1) JPS59148421A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61154211A (en) * 1984-12-26 1986-07-12 Daiwa Shinku Kogyosho:Kk Ceramic resonator
US5942836A (en) * 1997-01-10 1999-08-24 Murata Manufacturing Co., Ltd. Energy-trapping thickness-shear resonator and electronic components using the same
WO2006133807A1 (en) * 2005-06-15 2006-12-21 Epcos Ag Electroacoustic resonator, filter, duplexer and method for determining parameters of a resonator

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS51102485A (en) * 1975-03-05 1976-09-09 Murata Manufacturing Co ATSUDENJIKI KYOSHINSHI
JPS51135486A (en) * 1975-05-20 1976-11-24 Matsushita Electric Ind Co Ltd Piezo-electric ceramics oscillator
JPS5791016A (en) * 1980-11-26 1982-06-07 Murata Mfg Co Ltd Piezoelectric oscillator

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS51102485A (en) * 1975-03-05 1976-09-09 Murata Manufacturing Co ATSUDENJIKI KYOSHINSHI
JPS51135486A (en) * 1975-05-20 1976-11-24 Matsushita Electric Ind Co Ltd Piezo-electric ceramics oscillator
JPS5791016A (en) * 1980-11-26 1982-06-07 Murata Mfg Co Ltd Piezoelectric oscillator

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61154211A (en) * 1984-12-26 1986-07-12 Daiwa Shinku Kogyosho:Kk Ceramic resonator
US5942836A (en) * 1997-01-10 1999-08-24 Murata Manufacturing Co., Ltd. Energy-trapping thickness-shear resonator and electronic components using the same
DE19758033C2 (en) * 1997-01-10 1999-10-14 Murata Manufacturing Co Piezoelectric thickness shear resonator
WO2006133807A1 (en) * 2005-06-15 2006-12-21 Epcos Ag Electroacoustic resonator, filter, duplexer and method for determining parameters of a resonator
US8076999B2 (en) 2005-06-15 2011-12-13 Epcos Ag Electroacoustic resonator, filter, duplexer and method for determining parameters of a resonator

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