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JPS6313573B2 - - Google Patents
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JPS6313573B2 - - Google Patents

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Publication number
JPS6313573B2
JPS6313573B2 JP1684780A JP1684780A JPS6313573B2 JP S6313573 B2 JPS6313573 B2 JP S6313573B2 JP 1684780 A JP1684780 A JP 1684780A JP 1684780 A JP1684780 A JP 1684780A JP S6313573 B2 JPS6313573 B2 JP S6313573B2
Authority
JP
Japan
Prior art keywords
piezoelectric ceramic
aging
resonant frequency
vibrator
piezoelectric
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.)
Expired
Application number
JP1684780A
Other languages
Japanese (ja)
Other versions
JPS56114421A (en
Inventor
Takeshi Inoe
Sadayuki Takahashi
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.)
NEC Corp
Original Assignee
Nippon Electric 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 Nippon Electric Co Ltd filed Critical Nippon Electric Co Ltd
Priority to JP1684780A priority Critical patent/JPS56114421A/en
Priority to US06/233,141 priority patent/US4384229A/en
Publication of JPS56114421A publication Critical patent/JPS56114421A/en
Publication of JPS6313573B2 publication Critical patent/JPS6313573B2/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 elements; 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
    • H03H9/177Constructional features of resonators consisting of piezoelectric or electrostrictive material having a single resonator of the energy-trap type

Landscapes

  • Physics & Mathematics (AREA)
  • Acoustics & Sound (AREA)
  • Piezo-Electric Or Mechanical Vibrators, Or Delay Or Filter Circuits (AREA)

Description

【発明の詳細な説明】 本発明は厚み振動をする圧電磁器振動子に関す
る。一般に、厚み振動をする圧電磁器振動子(以
下単に圧電磁器振動子と記す)は数百KHz〜数十
MHz帯で使用され、高結合係数を有し、比較的帯
域帯の広いフイルタ等に実用化されている。しか
し、水晶のような圧電単結晶やエリンバ等のメタ
ルメカニカル振動子に比較して圧電磁器振動子は
共振周波数のエージングに対する安定度が劣ると
いつた欠点があり、そのため通信用フイルタ等の
ような高安定なエージング特性が要求されるよう
な場合、圧電磁器振動子でフイルタを構成しよう
とすると材料的に困難であつた。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a piezoelectric ceramic vibrator that performs thickness vibration. In general, piezoelectric ceramic resonators that vibrate through thickness (hereinafter simply referred to as piezoelectric ceramic resonators) are used in the band of several hundred KHz to several tens of MHz, and have a high coupling coefficient and are used in filters, etc. with a relatively wide band. has been made into However, compared to piezoelectric single crystals such as quartz and metal mechanical resonators such as Elinva, piezoelectric ceramic resonators have a disadvantage in that they are less stable with respect to aging of the resonance frequency, so they are used in communication filters, etc. In cases where highly stable aging characteristics are required, it is difficult to construct a filter using a piezoelectric ceramic vibrator due to material considerations.

圧電磁器振動子は、あらかじめ直流高電圧をか
けて分極され、分極直後から共振周波数rp、反
共振周波数ap及び並列容量Coといつた振動子諸
定数のエージングが始まる。一般に、圧電磁器振
動子の分極直後の共振周波数をrpo、エージン
グ中の共振周波数をrpとしたとき、規準化され
た共振周波数変化量Δrp(=rp−rpo)は、日
数を横軸にとると第1図に示すようになる。すな
わち、圧電磁器振動子の共振周波数はエージング
とともに上昇し、分極直後ほど共振周波数の変化
が大きく、時間経過とともに共振周波数の変化が
小さくなつていることがわかる。
The piezoelectric ceramic resonator is polarized in advance by applying a high DC voltage, and aging of the resonator constants such as the resonant frequency rp, the anti-resonant frequency ap, and the parallel capacitance Co starts immediately after polarization. In general, when the resonant frequency of a piezoelectric vibrator immediately after polarization is rpo, and the resonant frequency during aging is rp, the normalized resonant frequency change amount Δrp (= rp−rpo) is calculated by taking the number of days as the horizontal axis. The result is as shown in FIG. That is, it can be seen that the resonant frequency of the piezoelectric ceramic vibrator increases with aging, that the change in the resonant frequency is larger immediately after polarization, and that the change in the resonant frequency becomes smaller as time passes.

分極直後に近いほど共振周波数の変化は大きい
わけであるから、従来、エージング対策として一
般の圧電磁器振動子では、分極後に150℃〜200℃
の高温下で熱処理することにより、あらかじめ強
制エージングさせておき、エージング特性の改善
を図つていることは周知の通りである。しかし、
このように強制エージングを行つたとしても、強
制エージング終了時点からまた新たなエージング
が始まり、従来の圧電磁器振動子では、どんなに
高安定な材料でもせいぜい0.03%/decade程度ま
で改善させるのが限度であつた。
The change in resonance frequency is greater the closer it is to immediately after polarization, so conventionally, as a countermeasure against aging, general piezoelectric ceramic resonators have been heated at temperatures of 150℃ to 200℃ after polarization.
It is well known that the aging characteristics are improved by performing forced aging in advance by heat treatment at high temperatures. but,
Even if forced aging is performed in this way, a new aging process will begin once the forced aging ends, and with conventional piezoelectric ceramic resonators, no matter how highly stable the material is, the improvement can only be achieved by 0.03%/decade at most. It was hot.

本発明の目的は、従来の圧電磁器振動子の共振
周波数のエージングの安定度に対する欠点を解消
し、更に優れた共振周波数のエージング特性を有
する圧電磁器振動子ユニツトを得ることにある。
SUMMARY OF THE INVENTION An object of the present invention is to eliminate the disadvantages of conventional piezoelectric ceramic vibrators regarding the stability of aging of the resonant frequency, and to obtain a piezoelectric vibrator unit having even better aging characteristics of the resonant frequency.

以下、本発明の詳細について説明する。本発明
の圧電磁器振動子ユニツトは、第3図に示した例
のように、分極処理が施された圧電磁器31に電
極(第3図中斜線を施した部分)を設置した圧電
磁器振動子と、この圧電磁器振動子に直列に接続
された磁器容量32とから構成されている。ここ
で用いられている磁器容量32Caは、圧電磁器
振動子に寄生して存在する並列容量Coとの比
Ca/Coが時間の経過とともにしだいに大きくな
るようなエージング特性を有する磁器容量であ
る。
The details of the present invention will be explained below. As shown in the example shown in FIG. 3, the piezoelectric ceramic vibrator unit of the present invention is a piezoelectric ceramic vibrator in which electrodes (shaded areas in FIG. 3) are installed on a polarized piezoelectric ceramic 31. and a ceramic capacitor 32 connected in series to this piezoelectric ceramic vibrator. The ceramic capacitance 32Ca used here is the ratio of the parallel capacitance Co that exists parasitically to the piezoelectric ceramic vibrator.
It is a porcelain capacitor with aging characteristics in which Ca/Co gradually increases over time.

周知の如く、圧電磁器振動子は共振周波数rp
を与える動インダクタンスと動容量の直列接続で
表わされる部分及び並列容量Coからなる部分を
並列に接続した形の等価回路で表わされる。ここ
で上記、動インダクタンス及び動容量は圧電磁器
振動子のインピーダンスが極小になる共振周波数
r及びインピーダンスが極大になる反共振周波数
aを与えることによつて一意的に決定されるも
のである。
As is well known, piezoelectric ceramic vibrators have a resonant frequency rp
It is represented by an equivalent circuit in which a part represented by a series connection of dynamic inductance and dynamic capacitance that gives , and a part consisting of a parallel capacitance Co are connected in parallel. Here, as mentioned above, the dynamic inductance and dynamic capacitance are the resonance frequencies at which the impedance of the piezoelectric ceramic vibrator becomes minimum.
Anti-resonant frequency where r and impedance are maximum
It is uniquely determined by giving a.

圧電磁器振動子の共振周波数をrp、反共振周
波数をap並列容量をCoとし、この圧電磁器振動
子に直列に接続される磁器容量をCaとすると圧
電磁器振動子と外付磁器容量からなる本発明の圧
電磁器振動子ユニツトの共振周波数rは次式で表
わされる。
Let the resonant frequency of the piezoelectric ceramic vibrator be rp, the anti-resonant frequency be ap, the parallel capacitance be Co, and the ceramic capacitor connected in series with this piezoelectric vibrator be Ca. The resonant frequency r of the piezoelectric ceramic vibrator unit of the invention is expressed by the following equation.

r2=1/1+(Ca/Co){(Ca/Co)r2p+a2p} 上式から、Ca/Coが無限大のときはr=rpと
なるが、Ca/Coが小さくなるに従い、圧電磁器
振動子ユニツトの共振周波数rが次第に高くなり
圧電磁器振動子の反共振周波数に近ずいていくこ
とがわかる。
r 2 = 1/1 + (Ca/Co) {(Ca/Co) r 2 p + a 2 p} From the above formula, when Ca/Co is infinite, r = rp, but as Ca/Co becomes smaller, It can be seen that the resonant frequency r of the piezoelectric ceramic vibrator unit gradually increases and approaches the anti-resonant frequency of the piezoelectric vibrator.

圧電磁器振動子の共振周波数rpのエージング
特性については、すでに第1図でエージングとと
もに次第に高くなつていくことを示したが、反共
振周波数apは材料によつてまれにエージングと
ともに次第に低くなるものもあるが、次第に高く
なる材料が一般的である。
Regarding the aging characteristics of the resonant frequency rp of a piezoelectric ceramic resonator, we have already shown in Figure 1 that it gradually increases with aging, but the anti-resonant frequency ap may in rare cases gradually decrease with aging depending on the material. However, increasingly expensive materials are common.

上式から解るように、rpが時間と共に増大す
ると、Ca/Coが時間の経過に対し常に不変であ
るとするとrも時間の経過にしたがいrpと同じ
ように変化する。しかし、本発明のようにCa/
Coが時間の経過と共に増大すると、r2は時間と
共にしだいにr2pに近づいて行く。rは常にrp
より大きいわけであるからr2の経時変化の変化
量はr2pの経時変化の変化量より小さくなる。す
なわち本発明の圧電磁器振動子ユニツトのエージ
ング特性は従来の圧電磁器振動子のそれより優れ
たものとなる。
As can be seen from the above equation, if rp increases over time, r will also change over time in the same way as rp, assuming that Ca/Co remains unchanged over time. However, as in the present invention, Ca/
As Co increases over time, r 2 gradually approaches r 2 p over time. r is always rp
Therefore, the amount of change in r 2 over time is smaller than the amount of change in r 2 p over time. That is, the aging characteristics of the piezoelectric ceramic vibrator unit of the present invention are superior to those of conventional piezoelectric ceramic vibrators.

例えば、圧電磁器振動子の並列容量Coのエー
ジング特性が負であり、かつ反共振周波数apが
エージングとともに低下するものであれば、圧電
磁器振動子ユニツトの共振周波数rのエージング
特性は、単に並列容量Coと同じエージング特性
を有する容量Caを直列に接続しただけで改善さ
れ、さらに並列容量Coに比べてエージング特性
が十分小さな容量Caを直後に接続した場合には、
共振周波数rのエージング特性は一層改善される
わけである。
For example, if the aging characteristic of the parallel capacitance Co of a piezoelectric ceramic resonator is negative and the antiresonance frequency ap decreases with aging, then the aging characteristic of the resonant frequency r of the piezoelectric ceramic resonator unit is simply the parallel capacitance The improvement is achieved simply by connecting a capacitor Ca that has the same aging characteristics as Co in series, and furthermore, if a capacitor Ca whose aging characteristics are sufficiently smaller than that of the parallel capacitor Co is connected immediately after,
This means that the aging characteristics of the resonance frequency r are further improved.

しかし、apは材料的に時間経過とともに上昇
する振動子がむしろ一般的である。
However, it is rather common for ap to be a oscillator that increases over time due to the material.

次に、本発明の一実施例として、第3図に示す
ようなエネルギー閉じ込め型厚み辷り振動子31
に直列に磁器容量32を接続した構成の圧電磁器
振動子ユニツトについて説明する。エネルギー閉
じ込め型厚み辷り圧電磁器振動子31は、圧電磁
器材料として東北金属製NEPEC―31を用い、
長さ12mm、厚さ0.552mm、幅0.32mmの外形寸法を
有し、表裏面に圧電磁器の各端部から中央部分に
かけて斜線で示したような幅方向全体に広がる
Cr―Au電極を設けてあり、電極の相対応する重
なり部分は2.5mmである。この振動子31の並列
容量Coは13.41PFでありエージング特性は第2図
の実線で示した特性(初期値で規格化してある)
を有する。また、外付の磁器容量32は未分極の
NEPEC―31を用い、40.3PFでそのエージング
特性は第2図点線で示した物性(初期値で規格化
してある)を有する。あらかじめ150℃で熱処理
を施した圧電磁器振動子のエージング特性を、熱
処理直後の共振周波数rpoで規準化したものを
第4図に点線で示す。また、点線で示した圧電磁
器振動子と同一条件で熱処理を行つた圧電磁器振
動子を用いた本発明の圧電磁器振動子ユニツトの
共振周波数のエージング特性をrpoで規格化し
て第4図に実線で示す。
Next, as an embodiment of the present invention, an energy trapping type thickness sliding oscillator 31 as shown in FIG.
A piezoelectric ceramic vibrator unit having a configuration in which a ceramic capacitor 32 is connected in series with the piezoelectric ceramic vibrator unit will be explained. The energy trapping type thickness sliding piezoelectric ceramic vibrator 31 uses NEPEC-31 manufactured by Tohoku Metals as the piezoelectric ceramic material.
It has external dimensions of 12 mm in length, 0.552 mm in thickness, and 0.32 mm in width, and extends across the entire width from each end of the piezoelectric ceramic on the front and back sides to the center as shown by diagonal lines.
Cr--Au electrodes are provided, and the corresponding overlap between the electrodes is 2.5 mm. The parallel capacitance Co of this resonator 31 is 13.41PF, and its aging characteristics are shown by the solid line in Figure 2 (normalized by the initial value).
has. In addition, the external ceramic capacitor 32 is unpolarized.
Using NEPEC-31, its aging characteristics at 40.3PF have the physical properties (normalized by the initial value) shown by the dotted line in Figure 2. The aging characteristics of a piezoelectric ceramic resonator that has been heat-treated at 150°C in advance, normalized to the resonance frequency rpo immediately after the heat treatment, is shown by the dotted line in Figure 4. In addition, the aging characteristics of the resonant frequency of the piezoelectric ceramic resonator unit of the present invention, which uses a piezoelectric ceramic resonator heat-treated under the same conditions as the piezoelectric resonator shown by the dotted line, are normalized by rpo and are shown as a solid line in Fig. 4. Indicated by

以上から、非常に高安定であるとされている
NEPEC―31を用いた圧電磁器振動子でさえ、
共振周波数のエージング特性が0.03%/decade程
度であるのに対し、本発明による圧電磁器振動子
ユニツトでは0.015%/decade程度にまで改善さ
れていることがわかる。
From the above, it is said to be extremely stable.
Even a piezoelectric ceramic vibrator using NEPEC-31,
It can be seen that while the aging characteristic of the resonant frequency is about 0.03%/decade, it is improved to about 0.015%/decade in the piezoelectric ceramic vibrator unit according to the present invention.

また、本発明の圧電磁器振動子ユニツトの応用
として第5図に示すように、NEPEC―31未分
極容量51と厚み辷り振動子52からなる圧電磁
器振動子ユニツト50が2個と、段間容量53と
してNEPEC―31未分極容量から構成された
2.0MHz帯比帯域幅0.5%の狭帯域フイルタを試作
した。その結果、フイルタの中心周波数のエージ
ング特性が従来の圧電磁器振動子単体を用いたと
きの値0.03%/decadeから0.013%/decadeにい
ちぢるしく改善された。この0.013%/decadeと
いう値は従来の圧電磁器振動子では、とうてい不
可能とされていた値である。
Further, as an application of the piezoelectric ceramic resonator unit of the present invention, as shown in FIG. 53 consisting of NEPEC-31 unpolarized capacitors
We prototyped a narrowband filter with a 2.0MHz band specific bandwidth of 0.5%. As a result, the aging characteristics of the center frequency of the filter were significantly improved from 0.03%/decade when using a conventional piezoelectric ceramic vibrator alone to 0.013%/decade. This value of 0.013%/decade was a value that was considered impossible with conventional piezoelectric ceramic vibrators.

以上説明したように、本発明によれば、エージ
ング特性の極めて優れた圧電振動子ユニツトを提
供することができ工業的価値は多大である。
As explained above, according to the present invention, it is possible to provide a piezoelectric vibrator unit with extremely excellent aging characteristics, which has great industrial value.

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

第1図は、従来の圧電磁器振動子の共振周波数
の規準化されたエージング特性例を示す。第2図
は、規準化された容量のエージング特性例を示
し、実線は厚み辷り圧電磁器振動子の並列容量の
エージング特性、また点線は圧電磁器振動子に直
列に接続する磁器容量に用いる未分極容量のエー
ジング特性である。第3図は、本発明の一実施例
として、エネルギー閉じ込め型厚み辷り圧電磁器
振動子に直列に未分極の磁器容量を接続した圧電
磁器振動子ユニツトを示し、矢印は分極方向を示
す。第4図で、点線は従来の圧電磁器振動子の共
振周波数のエージング特性を示し、実線は本発明
の実施例の圧電磁器振動子ユニツトの共振周波数
のエージング特性を示す。第5図は、本発明の圧
電磁器振動子ユニツトを応用したフイルタの一例
を示す。 図において、31は厚み辷り圧電磁器振動子、
32は磁器容量、50は圧電磁器振動子ユニツ
ト、51は未分極磁器容量、52は圧電磁器振動
子、53は段間容量である。
FIG. 1 shows an example of normalized aging characteristics of the resonant frequency of a conventional piezoelectric ceramic vibrator. Figure 2 shows an example of aging characteristics of a normalized capacitor, where the solid line is the aging characteristic of a parallel capacitor of a thick piezoelectric ceramic resonator, and the dotted line is an unpolarized capacitor used for a ceramic capacitor connected in series with a piezoelectric ceramic resonator. This is the aging characteristic of capacity. FIG. 3 shows, as an embodiment of the present invention, a piezoelectric ceramic resonator unit in which an unpolarized ceramic capacitor is connected in series with an energy-trapped thickness-stretching piezoelectric vibrator, and the arrow indicates the polarization direction. In FIG. 4, the dotted line shows the aging characteristic of the resonant frequency of the conventional piezoelectric ceramic vibrator, and the solid line shows the aging characteristic of the resonant frequency of the piezoelectric vibrator unit according to the embodiment of the present invention. FIG. 5 shows an example of a filter to which the piezoelectric ceramic vibrator unit of the present invention is applied. In the figure, 31 is a thickness-stretching piezoelectric ceramic vibrator;
32 is a ceramic capacitor, 50 is a piezoelectric ceramic vibrator unit, 51 is an unpolarized ceramic capacitor, 52 is a piezoelectric ceramic vibrator, and 53 is an interstage capacitor.

Claims (1)

【特許請求の範囲】[Claims] 1 厚み振動を利用した圧電磁器振動子と、当該
圧電磁器振動子に直列に接続された磁器容量Ca
とから構成され、当該磁器容量Caは当該磁器容
量Caと前記圧電磁器振動子に寄生して存在する
並列容量Coとの比Ca/Coが時間の経過と共にし
だいに大きくなるようなエージング特性を有する
磁器容量であることを特徴とする圧電磁器振動子
ユニツト。
1 A piezoelectric ceramic vibrator that uses thickness vibration and a ceramic capacitor Ca connected in series to the piezoelectric ceramic vibrator
The magnetic capacitance Ca has an aging characteristic such that the ratio Ca/Co of the magnetic capacitance Ca and the parallel capacitance Co parasitic to the piezoelectric ceramic vibrator gradually increases with the passage of time. A piezoelectric ceramic vibrator unit characterized by a magnetic capacitance.
JP1684780A 1980-02-14 1980-02-14 Piezoelectric magnetic oscillator unit Granted JPS56114421A (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP1684780A JPS56114421A (en) 1980-02-14 1980-02-14 Piezoelectric magnetic oscillator unit
US06/233,141 US4384229A (en) 1980-02-14 1981-02-10 Temperature compensated piezoelectric ceramic resonator unit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1684780A JPS56114421A (en) 1980-02-14 1980-02-14 Piezoelectric magnetic oscillator unit

Publications (2)

Publication Number Publication Date
JPS56114421A JPS56114421A (en) 1981-09-09
JPS6313573B2 true JPS6313573B2 (en) 1988-03-26

Family

ID=11927596

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1684780A Granted JPS56114421A (en) 1980-02-14 1980-02-14 Piezoelectric magnetic oscillator unit

Country Status (1)

Country Link
JP (1) JPS56114421A (en)

Also Published As

Publication number Publication date
JPS56114421A (en) 1981-09-09

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