JPH04216208A - Piezoelectric resonator - Google Patents

Piezoelectric resonator

Info

Publication number
JPH04216208A
JPH04216208A JP40231390A JP40231390A JPH04216208A JP H04216208 A JPH04216208 A JP H04216208A JP 40231390 A JP40231390 A JP 40231390A JP 40231390 A JP40231390 A JP 40231390A JP H04216208 A JPH04216208 A JP H04216208A
Authority
JP
Japan
Prior art keywords
piezoelectric
electrode
mode
piezoelectric resonator
resonator
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
JP40231390A
Other languages
Japanese (ja)
Inventor
Koji Matsuno
公二 松野
Hiroshi Kuroda
廣 黒田
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP40231390A priority Critical patent/JPH04216208A/en
Publication of JPH04216208A publication Critical patent/JPH04216208A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To reduce the unnecessary resonance response of a nonconfined mode and to present the compact and low-priced piezoelectric resonator concerning the piezoelectric resonator using a longitudinal thickness higher harmonic energy confining resonator used for a filter or an oscillator. CONSTITUTION:Oscillating electrodes 2 facing the front and back sides are formed on both the main plane central parts of a piezoelectric substrate 1 while being overlapped, and a pair of independent partial electrodes 5 are formed on the counter sides close to these oscillating electrodes 2. Therefore, since oscillation energy is attenuated at the above-mentioned partial electrode parts 5 because of mechanical load as the electrode and the effect of piezoelectric short-circuiting, the piezoelectric resonator can be obtained to reduce the unnecessary resonance response close to thickness longitudinal fundamental resonance.

Description

【発明の詳細な説明】[Detailed description of the invention]

【0001】0001

【産業上の利用分野】本発明はフィルタや発振子などに
使用される厚み縦高調波エネルギー閉じこめ型共振子を
用いた圧電共振子に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a piezoelectric resonator using a thick longitudinal harmonic energy confinement type resonator used in filters, oscillators, etc.

【0002】0002

【従来の技術】代表的な従来例について図3(a),(
b)を用いて以下に説明する。同図(d)は厚み縦高調
波エネルギー閉じこめ形振動モードを用いた圧電共振子
を示す平面図であり、圧電基板6の主平面中央部に表裏
一対で対向する振動電極7と、この振動電極7から導き
出した引き出し電極8を端部に設けた取出し電極9に接
続した状態を示すものであり、このように電極形成を行
った圧電基板6を図3(b)に示すように外装樹脂10
で表面部全体をモールドすると共に前記振動電極7上お
よびその近傍に自由振動空間11を形成して構成されて
いた。
[Prior Art] Typical conventional examples are shown in Figs. 3(a) and (
This will be explained below using b). FIG. 6(d) is a plan view showing a piezoelectric resonator using a thickness-longitudinal harmonic energy confinement type vibration mode. This figure shows a state in which the extraction electrode 8 led out from the electrode 7 is connected to the extraction electrode 9 provided at the end.
The entire surface portion was molded with a mold, and a free vibration space 11 was formed on and in the vicinity of the vibration electrode 7.

【0003】このように構成された圧電共振子の厚み縦
高調波エネルギー閉じ込めモードは、前記振動電極7上
およびその近傍に形成された自由振動空間11により振
動電極7の振動を阻害されず電極的共振応答が効率良く
行われると同時に、振動電極7から圧電基板6の輪郭部
に向かって伝搬していく非閉じ込めモードは外装樹脂1
0の粘性によって熱エネルギーとなって減衰するため輪
郭部からの反射波が有効に減少し、基本波および所定の
厚み縦高調波モード以外の共振周波数近傍の電気的不要
共振応答を減衰させるように構成されたものであった。
The thickness vertical harmonic energy confinement mode of the piezoelectric resonator configured as described above is achieved by the free vibration space 11 formed on and near the vibrating electrode 7, which allows the vibration of the vibrating electrode 7 to be unhindered and to be controlled by the electrode. At the same time as the resonance response is performed efficiently, the unconfined mode propagating from the vibrating electrode 7 toward the contour of the piezoelectric substrate 6 is caused by the outer resin 1.
Since the viscosity of zero is turned into thermal energy and attenuated, the reflected wave from the contour is effectively reduced, and unnecessary electrical resonance responses near the resonance frequency other than the fundamental wave and the predetermined thickness vertical harmonic mode are attenuated. It was composed.

【0004】0004

【発明が解決しようとする課題】しかしながら上記従来
の電圧共振子では、厚み縦高調波のうち特定のエネルギ
ー閉じ込めモードのみを利用するものであり、特にこの
特定のエネルギー閉じ込めモードを利用した圧電共振子
を発振素子として用いた場合に、低次の非閉じ込めモー
ド(伝搬モード)を十分に減衰させることができず、低
次モード近傍に発生する不要共振応答が低周波で発生す
ることになる。
[Problem to be Solved by the Invention] However, the conventional voltage resonator described above utilizes only a specific energy trapping mode of the thickness longitudinal harmonic, and in particular, a piezoelectric resonator that utilizes this specific energy trapping mode is When used as an oscillation element, low-order unconfined modes (propagation modes) cannot be sufficiently attenuated, and unnecessary resonance responses occur near the low-order modes at low frequencies.

【0005】本発明はこの非閉じ込めモード(伝搬モー
ド)を、上記従来例で説明した外装樹脂10でモールド
するような付加的工法を採用することなく簡単な構成で
分散させることにより、低次モード近傍に発生する不要
共振応答を低減することが可能な小型の圧電共振子を提
供することを目的としたものである。
The present invention disperses this unconfined mode (propagation mode) with a simple structure without adopting an additional method such as molding with the exterior resin 10 explained in the conventional example, thereby reducing the low-order mode. The object of the present invention is to provide a small piezoelectric resonator that can reduce unnecessary resonance responses that occur nearby.

【0006】[0006]

【課題を解決するための手段】上記課題を解決するため
に本発明による圧電共振子は、圧電基板の両主平面中央
部に重なり合って表裏対向する振動電極と、この振動電
極から導き出され端部の一辺に設けた取出し電極に交差
接続する引き出し電極をそれぞれに設け、前記振動電極
に近接した対向する辺に独立した一対の部分電極を形成
した構成にしたものである。
[Means for Solving the Problems] In order to solve the above problems, a piezoelectric resonator according to the present invention includes a vibrating electrode that overlaps the central portion of both principal planes of a piezoelectric substrate and faces each other, and an end portion that is led out from the vibrating electrode. Each of the vibration electrodes is provided with an extraction electrode cross-connected to the extraction electrode provided on one side of the vibrating electrode, and a pair of independent partial electrodes are formed on opposing sides close to the vibrating electrode.

【0007】[0007]

【作用】この構成により、振動電極部から主平面を伝搬
し圧電基板の輪郭部分に達する非閉じ込めモードは、前
記振動電極に近接した対向する辺に設けた一対の部分電
極部において電極としての機械的負荷と圧電短絡の効果
により振動エネルギーが減衰されるため厚み縦基本共振
近傍の不要共振応答の低減が可能になり、特にこの共振
子を初振用素子として用いた場合に、低次モードでの発
振を制御することができる。
[Operation] With this configuration, the unconfined mode that propagates from the vibrating electrode part through the main plane and reaches the contour part of the piezoelectric substrate can be transmitted to the mechanical Because the vibration energy is attenuated by the mechanical load and the piezoelectric short circuit effect, it is possible to reduce unnecessary resonance responses near the thickness longitudinal fundamental resonance, and especially when this resonator is used as an initial resonance element, it is possible to reduce the unnecessary resonance response in the low-order mode. oscillation can be controlled.

【0008】[0008]

【実施例】以下、本発明による一実施例を図1および図
2を用いて説明する。図1は本発明による圧電共振子を
示す斜視図であり、圧電基板1は厚み方向に分極され厚
さtで決まる厚み縦基本モードが非閉じ込め(伝搬)モ
ード、厚み縦3倍モードがエネルギー閉じ込めモードと
なるような定数(ポアソン比)を持つように構成したも
のであり、本実施例では分極処理された圧電基板1を用
いたが、本発明の適用範囲はこれに限定されるものでは
なく自発分極を持つ圧電単結晶,配向膜等を用いること
も可能である。
Embodiment An embodiment of the present invention will be described below with reference to FIGS. 1 and 2. FIG. 1 is a perspective view showing a piezoelectric resonator according to the present invention, in which a piezoelectric substrate 1 is polarized in the thickness direction, the fundamental thickness longitudinal mode determined by the thickness t is an unconfined (propagating) mode, and the triple thickness longitudinal mode is an energy confined mode. The piezoelectric substrate 1 is configured to have a constant (Poisson's ratio) that becomes a mode, and although a polarized piezoelectric substrate 1 is used in this embodiment, the scope of application of the present invention is not limited to this. It is also possible to use a piezoelectric single crystal with spontaneous polarization, an oriented film, etc.

【0009】前記圧電基板1の主平面の略中央部に蒸着
,メッキ等の手段で重なり合って表裏対向するように振
動電極2を形成し、この振動電極2から導き出した引き
出し電極3を端部の一辺に設けた取出し電極4に交差接
続した形状の電極部を表裏面にそれぞれ形成し、前記振
動電極2は重なり合って振動閉じ込め電極部を構成し、
取出し電極4は重ならないように配置されたものである
A vibrating electrode 2 is formed approximately at the center of the main plane of the piezoelectric substrate 1 by means of vapor deposition, plating, etc. so that the front and back sides are overlapping each other, and an extraction electrode 3 led out from the vibrating electrode 2 is connected to the end portion of the piezoelectric substrate 1. electrode portions each having a cross-connected shape to the extraction electrode 4 provided on one side are formed on the front and back surfaces, and the vibrating electrodes 2 overlap to form a vibration confinement electrode portion;
The extraction electrodes 4 are arranged so as not to overlap.

【0010】また、前記振動電極2の形状は円形とし、
この振動電極2の直径Dはオーバートーン共振を避ける
ため圧電基板の厚さt、周波数低下量Δできまるベック
マン定数より上限の決まる値とし、厚み縦3次高調波モ
ードの振動が振動電極2およびその近傍に閉じ込められ
る単一共振を実現するように構成したものである。
Further, the shape of the vibrating electrode 2 is circular,
In order to avoid overtone resonance, the diameter D of the vibrating electrode 2 is set to a value whose upper limit is determined by the Beckmann constant determined by the thickness t of the piezoelectric substrate and the amount of frequency reduction Δ, so that the vibration of the third harmonic mode in the thickness longitudinal direction is It is configured to realize a single resonance confined in the vicinity.

【0011】また、前記圧電基板1の両主平面上に前記
振動電極2に近接した対向する辺に独立した一対の部分
電極5を表裏対向するように長方形の形状で形成した。 この部分電極5は前記振動電極2近傍の厚み縦3倍高調
波モードが閉じ込められている部分に重ならないことと
前記引き出し電極3および取出し電極4に接触しない限
り形状および大きさは任意のもので良い。
A pair of independent partial electrodes 5 were formed on both main planes of the piezoelectric substrate 1 on opposite sides close to the vibrating electrode 2 in a rectangular shape so as to face each other from front to back. This partial electrode 5 may have any shape and size as long as it does not overlap with the area in the vicinity of the vibrating electrode 2 where the triple-thickness vertical harmonic mode is confined and does not come into contact with the extraction electrode 3 and the extraction electrode 4. good.

【0012】前記部分電極5の働きは、振動電極2に厚
みtで決まる厚み縦基本振動モードを励振する近傍の周
波数の高周波電界が印加された際に、振動電極2部に閉
じこまらない伝搬波となって圧電基板1の周囲に円筒波
状に伝搬していくが、前記部分電極5の電極としての機
械的負荷と圧電短絡との効果により部分電極5部に振動
エネルギーが吸収され不要共振応答が低減されるもので
ある。
The function of the partial electrode 5 is that when a high frequency electric field having a frequency close to that which excites the thickness longitudinal fundamental vibration mode determined by the thickness t is applied to the vibrating electrode 2, a propagating wave that is not confined in the vibrating electrode 2 is generated. The vibration energy propagates around the piezoelectric substrate 1 in a cylindrical wave shape, but due to the mechanical load of the partial electrode 5 as an electrode and the piezoelectric short circuit, the vibration energy is absorbed by the partial electrode 5, causing an unnecessary resonance response. It is something that will be reduced.

【0013】図2(a),(b)は厚み縦基本振動モー
ド近傍と厚み縦3倍高調波モードの共振インピーダンス
Zの関係を示した周波数特性図であり、破線は本実施例
による圧電共振子を示し実線は部分電極5を作成しない
従来方式の圧電共振子を示すものである。この周波数特
性図から明らかなように、同図(b)に示す厚み縦3倍
モードはエネルギー閉じ込めが十分に行われているので
両者の間に差異は認められないが、同図(d)に示す非
閉じ込めモードの厚み縦基本モードの共振周波数近傍で
は本発明による圧電共振子は不要共振応答に大きな改善
効果が認められる。
FIGS. 2(a) and 2(b) are frequency characteristic diagrams showing the relationship between the resonance impedance Z in the vicinity of the thickness longitudinal fundamental vibration mode and the thickness longitudinal triple harmonic mode, and the broken line indicates the piezoelectric resonance according to this embodiment. The solid line indicates a conventional piezoelectric resonator in which the partial electrode 5 is not formed. As is clear from this frequency characteristic diagram, energy confinement is sufficient in the triple-thickness longitudinal mode shown in Figure (b), so there is no difference between the two, but in Figure (d), there is no difference between the two. In the vicinity of the resonant frequency of the thickness longitudinal fundamental mode of the unconfined mode shown in FIG.

【0014】[0014]

【発明の効果】以上のように、本発明による圧電共振子
は厚み縦高調波エネルギー閉じ込め型振動子の非閉じ込
めモードの不要共振応答が、圧電基板上に独立した一対
の部分電極を設けることにより容易に低減することが可
能になり、特に別工程を追加して外装樹脂でコーティン
グを行うなどの作業ならびにそのためのスペースを圧電
基板上に確保することを必要としないで小形高性能の圧
電共振子を得ることができるなど工業的価値の大なるも
のである。
[Effects of the Invention] As described above, in the piezoelectric resonator according to the present invention, the unnecessary resonance response of the unconfined mode of the thickness vertical harmonic energy confined type vibrator can be suppressed by providing a pair of independent partial electrodes on the piezoelectric substrate. In particular, it is possible to create a small, high-performance piezoelectric resonator without the need to add a separate process to coat it with an exterior resin, or to secure space for this on the piezoelectric substrate. It is of great industrial value as it can be used to obtain

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

【図1】本発明の一実施例による圧電共振子を示す斜視
FIG. 1 is a perspective view showing a piezoelectric resonator according to an embodiment of the present invention.

【図2】(a)同実施例の厚み縦基本共振周波数近傍の
周波数特性図 (b)同実施例の厚み縦3倍共振周波数近傍の周波数特
性図
[Figure 2] (a) Frequency characteristic diagram near the thickness longitudinal fundamental resonance frequency of the same example (b) Frequency characteristic diagram near the thickness longitudinal threefold resonance frequency of the same example

【図3】(a)従来の圧電共振子を示す平面図(b)従
来の圧電共振子を示す断面図
[Figure 3] (a) Plan view showing a conventional piezoelectric resonator (b) Cross-sectional view showing a conventional piezoelectric resonator

【符号の説明】[Explanation of symbols]

1  圧電基板 2  振動電極 3  引き出し電極 4  取出し電極 5  部分電極 1 Piezoelectric substrate 2 Vibrating electrode 3 Extraction electrode 4 Takeout electrode 5 Partial electrode

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】中央部に振動電極とこの振動電極から導き
出され端部の一辺に設けた取出し電極に交差接続する引
き出し電極を板状の圧電基板の両主平面に表裏一対で前
記振動電極が重なり合うように形成し、前記振動電極に
近接した圧電基板の対向する辺に独立した一対の部分電
極を形成してなる圧電共振子。
Claim 1: A vibrating electrode is arranged in a pair on both main planes of a plate-shaped piezoelectric substrate. A piezoelectric resonator comprising a pair of independent partial electrodes formed on opposing sides of a piezoelectric substrate close to the vibrating electrode, which are formed so as to overlap each other.
JP40231390A 1990-12-14 1990-12-14 Piezoelectric resonator Pending JPH04216208A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP40231390A JPH04216208A (en) 1990-12-14 1990-12-14 Piezoelectric resonator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP40231390A JPH04216208A (en) 1990-12-14 1990-12-14 Piezoelectric resonator

Publications (1)

Publication Number Publication Date
JPH04216208A true JPH04216208A (en) 1992-08-06

Family

ID=18512134

Family Applications (1)

Application Number Title Priority Date Filing Date
JP40231390A Pending JPH04216208A (en) 1990-12-14 1990-12-14 Piezoelectric resonator

Country Status (1)

Country Link
JP (1) JPH04216208A (en)

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE19854912C2 (en) * 1997-12-16 2001-07-12 Murata Manufacturing Co Piezoelectric resonator
JP2001339272A (en) * 2000-05-30 2001-12-07 Kyocera Corp Piezoelectric resonator
US6525449B1 (en) 1997-12-04 2003-02-25 Murata Manufacturing Co., Ltd. Piezoelectric resonator utilizing a harmonic in a thickness-extensional vibration mode
US7567014B2 (en) 2004-10-14 2009-07-28 Murata Manufacturing Co., Ltd. Energy trap piezoelectric resonator
DE19951523B4 (en) * 1998-10-26 2010-09-30 Murata Mfg. Co., Ltd., Nagaokakyo-shi Energy-blocking piezoelectric resonator and energy-blocking piezoelectric resonance component

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6525449B1 (en) 1997-12-04 2003-02-25 Murata Manufacturing Co., Ltd. Piezoelectric resonator utilizing a harmonic in a thickness-extensional vibration mode
DE19854699B4 (en) * 1997-12-04 2005-07-14 Murata Mfg. Co., Ltd., Nagaokakyo Piezoelectric resonator
DE19854912C2 (en) * 1997-12-16 2001-07-12 Murata Manufacturing Co Piezoelectric resonator
US6274964B1 (en) 1997-12-16 2001-08-14 Murata Manufacturing Co., Ltd. Piezoelectric resonator
DE19951523B4 (en) * 1998-10-26 2010-09-30 Murata Mfg. Co., Ltd., Nagaokakyo-shi Energy-blocking piezoelectric resonator and energy-blocking piezoelectric resonance component
JP2001339272A (en) * 2000-05-30 2001-12-07 Kyocera Corp Piezoelectric resonator
US7567014B2 (en) 2004-10-14 2009-07-28 Murata Manufacturing Co., Ltd. Energy trap piezoelectric resonator

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