JP2003034574A - Piezoelectric ceramic composition and piezoelectric resonator - Google Patents
Piezoelectric ceramic composition and piezoelectric resonatorInfo
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- JP2003034574A JP2003034574A JP2001222972A JP2001222972A JP2003034574A JP 2003034574 A JP2003034574 A JP 2003034574A JP 2001222972 A JP2001222972 A JP 2001222972A JP 2001222972 A JP2001222972 A JP 2001222972A JP 2003034574 A JP2003034574 A JP 2003034574A
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Abstract
(57)【要約】
【課題】共振周波数と反共振周波数の間の周波数で位相
歪みが発生せず、P/Vを大きくできるとともに、−2
0℃〜+80℃の温度範囲で発振周波数の温度安定性に
優れ、且つ焼成ばらつきによる特性変動を抑制できる圧
電磁器組成物および圧電共振子を提供する。
【解決手段】金属元素として少なくともBa、Biおよ
びTiを含有し、モル比による組成式をBi4Ti3O12
・x{(Ba1-aAa)TiO3}と表したとき、前記
x、aが、0.5≦x≦0.9、0≦a≦0.4、A
は、Bi、La、Nd、GdおよびPrのうち少なくと
も1種を満足する主成分と、該主成分100重量部に対
してMnをMnO2換算で0.05〜1.5重量部含有
するものである。
(57) [Summary] A phase distortion does not occur at a frequency between a resonance frequency and an anti-resonance frequency, and P / V can be increased.
Provided are a piezoelectric ceramic composition and a piezoelectric resonator that are excellent in temperature stability of an oscillation frequency in a temperature range of 0 ° C. to + 80 ° C. and that can suppress characteristic fluctuation due to firing variation. The composition contains at least Ba, Bi and Ti as metal elements, and has a composition formula based on a molar ratio of Bi 4 Ti 3 O 12.
When x {(Ba 1 -a A a ) TiO 3 }, x and a are 0.5 ≦ x ≦ 0.9, 0 ≦ a ≦ 0.4, A
Is a main component that satisfies at least one of Bi, La, Nd, Gd and Pr, and contains 0.05 to 1.5 parts by weight of Mn in terms of MnO 2 with respect to 100 parts by weight of the main component. It is.
Description
【0001】[0001]
【発明の属する技術分野】本発明は、圧電磁器組成物お
よび圧電共振子に関し、例えば、共振子、超音波振動
子、超音波モータ、あるいは加速度センサ、ノッキング
センサ、およびAEセンサ等の圧電センサなどに適し、
特に、厚み滑り振動の基本波振動を利用したエネルギ一
閉じ込め型発振子の高周波発振子用として好適に用いら
れる圧電磁器組成物および圧電共振子に関するものであ
る。TECHNICAL FIELD The present invention relates to a piezoelectric ceramic composition and a piezoelectric resonator, for example, a resonator, an ultrasonic oscillator, an ultrasonic motor, or a piezoelectric sensor such as an acceleration sensor, a knocking sensor, and an AE sensor. Suitable for
In particular, the present invention relates to a piezoelectric ceramic composition and a piezoelectric resonator that are preferably used for a high-frequency oscillator of an energy-entrapment type oscillator that utilizes fundamental vibration of thickness shear vibration.
【0002】[0002]
【従来技術】従来から、圧電磁器を利用した製品として
は、例えば、フィルタ、圧電共振子(以下、発振子を含
む概念である)、超音波振動子、超音波モータ、圧電セ
ンサ等がある。2. Description of the Related Art Conventionally, products using a piezoelectric ceramic include, for example, a filter, a piezoelectric resonator (hereinafter, a concept including an oscillator), an ultrasonic vibrator, an ultrasonic motor, a piezoelectric sensor, and the like.
【0003】ここで、発振子は、マイコンの基準信号発
振用として、例えば、コルピッツ発振回路等の発振回路
に組み込まれて利用される。図1はコルピッツ発振回路
を基本とした回路構成においてインダクタの部分を圧電
発振子に置き換えたピアス発振回路を示すものである。
このピアス発振回路は、コンデンサ11、12と、抵抗
13と、インバータ14および発振子15により構成さ
れている。そして、ピアス発振回路において、発振信号
を発生するには、以下の発振条件を満足する必要があ
る。Here, the oscillator is used by being incorporated in an oscillation circuit such as a Colpitts oscillation circuit for oscillating a reference signal of a microcomputer. FIG. 1 shows a Pierce oscillator circuit in which the inductor is replaced with a piezoelectric oscillator in a circuit configuration based on the Colpitts oscillator circuit.
This Pierce oscillator circuit is composed of capacitors 11 and 12, a resistor 13, an inverter 14 and an oscillator 15. Then, in the pierce oscillator circuit, in order to generate an oscillation signal, it is necessary to satisfy the following oscillation conditions.
【0004】即ち、インバータ14と抵抗13からなる
増幅回路における増幅率をα、位相量をθ1として、ま
た、発振子15とコンデンサ11、12からなる帰還回
路における帰還率をβ、位相量をθ2としたとき、ルー
プゲインがα×β≧1であり、かつ、位相量がθ1+θ2
=360゜×n(但しn=1,2,…)であることが必
要となる。That is, the amplification factor in the amplifier circuit composed of the inverter 14 and the resistor 13 is α, the phase amount is θ 1 , and the feedback factor in the feedback circuit composed of the oscillator 15 and the capacitors 11 and 12 is β, the phase amount is When θ 2 is set, the loop gain is α × β ≧ 1 and the phase amount is θ 1 + θ 2
= 360 ° × n (where n = 1, 2, ...).
【0005】一般的に抵抗13およびインバータ14か
らなる増幅回路は、マイコンに内蔵されている。誤発振
や不発振を起さない、安定した発振を得るためにはルー
プゲインを大きくしなければならない。ループゲインを
大きくするには、帰還率βのゲインを決定する、発振子
15のP/V、すなわち共振インピーダンスR0および
反共振インピーダンスRaの差を大きくすることが必要
となる。なお、P/Vは20×Log(Ra/R0)の値
として定義される。Generally, an amplifier circuit including a resistor 13 and an inverter 14 is built in a microcomputer. The loop gain must be increased in order to obtain stable oscillation without causing erroneous oscillation or non-oscillation. In order to increase the loop gain, it is necessary to increase the P / V of the oscillator 15, that is, the difference between the resonance impedance R 0 and the anti-resonance impedance R a , which determines the gain of the feedback ratio β. P / V is defined as a value of 20 × Log (R a / R 0 ).
【0006】また、位相量の条件を満足させるために
は、共振周波数と反共振周波数の間およびその近傍の周
波数で、位相が約−90゜から約+90゜まで位相反転
し、且つ共振周波数と反共振周波数の間にスプリアス振
動による位相歪みが発生しないことも重要となる。In order to satisfy the condition of the phase amount, the phase is inverted from about -90 ° to about + 90 ° between the resonance frequency and the anti-resonance frequency and in the vicinity of the resonance frequency and the resonance frequency. It is also important that phase distortion due to spurious vibration does not occur between anti-resonant frequencies.
【0007】従来、圧電性が高く例えば大きなP/Vが
得られるPZTやPT系材料が使用されていた。しかし
ながら、PZTやPT系材料には鉛が自重の約60%の
割合で含有されているため酸性雨により鉛の溶出が起こ
り環境汚染を招く危険性が指摘されている。そこで、鉛
を含有しない圧電材料への高い期待が寄せられている。
鉛を含有しないビスマス層状化合物を主体とする材料系
においては、PZTやPT系材料と比較して機械的品質
係数(Qm)が比較的高いという特徴があり、発振子用
の圧電材料としての応用が可能である。Conventionally, PZT or PT type materials which have high piezoelectricity and can obtain a large P / V, for example, have been used. However, it has been pointed out that PZT and PT-based materials contain lead in an amount of about 60% of their own weight, so that acid elution may lead to lead elution and environmental pollution. Therefore, high expectations are placed on piezoelectric materials that do not contain lead.
A material system mainly composed of a lead-free bismuth layered compound is characterized by a relatively high mechanical quality factor (Qm) compared to PZT and PT based materials, and is applied as a piezoelectric material for an oscillator. Is possible.
【0008】[0008]
【発明が解決しようとする課題】しかしながら、従来の
ビスマス層状化合物、例えばSrBi4Ti4O15を主体
とする圧電磁器組成物を、圧電発振子の圧電磁器として
用いた場合、共振周波数の温度変化率が±6000pp
mよりも大きく、高機能な制御を必要とする電子機器か
ら要求される温度特性に対する周波数の許容公差±30
00ppm以内の精度には対応できないという問題があ
った。However, when a conventional piezoelectric ceramic composition mainly composed of a bismuth layered compound, for example, SrBi 4 Ti 4 O 15 is used as a piezoelectric ceramic of a piezoelectric oscillator, the resonance frequency changes with temperature. The rate is ± 6000pp
Frequency tolerance of ± 30 with respect to temperature characteristics required from electronic equipment that requires high-performance control and is larger than m
There is a problem that the accuracy within 00 ppm cannot be supported.
【0009】例えば、従来、SrBi4Ti4O15を基本
組成として希土類添加や置換が知られているが、この組
成物では、P/Vは比較的大きくなるものの共振周波数
の温度変化率が約±6000ppmと大きいといった問
題があった。For example, it has been known that SrBi 4 Ti 4 O 15 is used as a basic composition for adding or substituting a rare earth element. With this composition, although the P / V is relatively large, the temperature change rate of the resonance frequency is about the same. There was a problem that it was as large as ± 6000 ppm.
【0010】また、従来のビスマス層状化合物を圧電発
振子の圧電磁器として用いた場合、圧電発振子の小型化
を図っていくと、充分なP/Vが得られないばかりか、
加工性が悪くチッピング(共振子用磁器エッジの欠け)
により共振周波数と反共振周波数の間にスプリアス振動
に伴う位相歪みが発生し、位相の条件を満足しなくな
り、不発振が生じたり、安定した発振が得られないとい
う問題があった。When a conventional bismuth layered compound is used as a piezoelectric ceramic of a piezoelectric oscillator, a sufficient P / V cannot be obtained if the piezoelectric oscillator is miniaturized.
Poor workability and chipping (porcelain edge for resonator)
As a result, there is a problem that phase distortion due to spurious vibration occurs between the resonance frequency and the anti-resonance frequency, the phase condition is not satisfied, non-oscillation occurs, and stable oscillation cannot be obtained.
【0011】さらに、従来のビスマス層状化合物では、
磁器密度の焼成温度依存性が急峻であるとともに磁器の
焼成温度範囲が狭く、焼成ばらつきにともなう特性変動
が大きくなるという問題があった。Further, in the conventional bismuth layered compound,
There is a problem that the firing temperature dependence of the porcelain density is steep, the firing temperature range of the porcelain is narrow, and the characteristic variation due to firing variations becomes large.
【0012】従って、本発明は、共振周波数と反共振周
波数の間の周波数で位相歪みが発生せず、厚み滑り振動
や厚み縦振動の基本波振動のP/Vを大きくできるとと
もに、−20℃〜+80℃の温度範囲で発振周波数の温
度安定性に優れ、且つ焼成温度の範囲を広くして焼成ば
らつきによる特性変動を抑制できる圧電磁器組成物およ
び圧電共振子を提供することを目的とする。Therefore, according to the present invention, phase distortion does not occur at a frequency between the resonance frequency and the anti-resonance frequency, the P / V of the fundamental wave vibration of the thickness sliding vibration and the thickness longitudinal vibration can be increased, and at the same time, -20 ° C. An object of the present invention is to provide a piezoelectric ceramic composition and a piezoelectric resonator which are excellent in temperature stability of an oscillation frequency in a temperature range of up to + 80 ° C. and which can widen a firing temperature range to suppress characteristic variation due to firing variation.
【0013】[0013]
【課題を解決するための手段】本発明の圧電磁器組成物
は、金属元素として少なくともBa、BiおよびTiを
含有するビスマス層状化合物であって、モル比による組
成式をBi4Ti3O12・x{(Ba1-aAa)TiO3}
と表したとき、前記x、aが0.5≦x≦0.9、0≦
a≦0.4、Aは、Bi、La、Nd、GdおよびPr
のうち少なくとも1種を満足する主成分と、該主成分1
00重量部に対してMnをMnO2換算で0.05〜
1.5重量部含有するものである。The piezoelectric ceramic composition of the present invention is a bismuth layered compound containing at least Ba, Bi and Ti as metal elements, and has a composition formula of Bi 4 Ti 3 O 12 ·. x {(Ba 1-a A a ) TiO 3 }
And x is 0.5 ≦ x ≦ 0.9, 0 ≦
a ≦ 0.4, A is Bi, La, Nd, Gd and Pr
A main component satisfying at least one of the
Mn is 0.05 to 0.05 parts by weight in terms of MnO 2.
It contains 1.5 parts by weight.
【0014】このような圧電磁器組成物によれば、特に
厚み滑り基本波振動やあるいは厚み縦の基本波および3
次オーバートーン振動でのP/V値を大きくすることが
できるとともに、−20℃〜+80℃の温度範囲で発振
周波数の温度安定性に優れた特性が得られ、さらに加工
時にチッピングの発生を著しく少なくなることから共振
周波数と反共振周波数の間にスプリアス振動に伴う位相
歪みを抑制することができ、さらに焼成温度の範囲を広
くして焼成ばらつきによる特性変動を抑制することがで
きる。According to such a piezoelectric ceramic composition, especially the thickness shear fundamental wave vibration or the thickness longitudinal fundamental wave and 3
The P / V value in the next overtone vibration can be increased, and the temperature stability of the oscillating frequency is excellent in the temperature range of -20 ° C to + 80 ° C. Further, chipping is remarkably generated during processing. Since the amount is reduced, the phase distortion caused by spurious vibration can be suppressed between the resonance frequency and the anti-resonance frequency, and the range of the firing temperature can be widened to suppress the characteristic variation due to the firing variation.
【0015】本発明では、AがBiの場合、即ち、主成
分が、Bi4Ti3O12・x{(Ba 1-aBia)Ti
O3}と表わされるものが望ましい。この場合には、特
に、厚み滑り基本波振動の基本波および3次オーバート
ーン振動でのP/V値を大きくできるとともに、−20
℃〜+80℃の温度範囲における発振周波数の温度安定
性を向上し、且つ焼成温度の範囲を広くして焼成ばらつ
きによる特性変動を抑制できる。In the present invention, when A is Bi, that is,
Minutes are BiFourTi3O12・ X {(Ba 1-aBia) Ti
O3} Is preferable. In this case,
In addition, the fundamental wave of thickness slip fundamental wave vibration and the third order overtone
It is possible to increase the P / V value in the chain vibration and
Temperature stability of oscillation frequency in the temperature range of ℃ to + 80 ℃
And improve the firing temperature and widen the firing temperature range.
It is possible to suppress the characteristic fluctuation due to the vibration.
【0016】本発明の圧電共振子は、圧電磁器の両主面
に電極を形成してなるとともに、前記圧電磁器が上記圧
電磁器組成物からなるものである。In the piezoelectric resonator of the present invention, electrodes are formed on both main surfaces of the piezoelectric ceramic, and the piezoelectric ceramic comprises the above piezoelectric ceramic composition.
【0017】このような圧電共振子によれば、例えば、
厚み滑り基本波振動を適用した発振子ではP/Vが大き
くなることから発振余裕度が高まり、且つ共振周波数と
反共振周波数の間の周波数で位相歪みが発生しないこと
から安定した発振が得られるとともに、発振周波数の温
度安定性に優れた高精度な発振が得られ、さらに、焼成
温度の範囲が広くなることから焼成ばらつきによる特性
変動を著しく抑制した2〜20MHzの広い周波数に適
応できる発振子を得ることができる。According to such a piezoelectric resonator, for example,
In the oscillator to which the thickness shear fundamental vibration is applied, the P / V becomes large, so that the oscillation allowance is increased, and the phase distortion does not occur at the frequency between the resonance frequency and the anti-resonance frequency, so that stable oscillation can be obtained. At the same time, a highly accurate oscillation with excellent temperature stability of the oscillation frequency can be obtained, and further, since the range of the firing temperature is widened, it is possible to adapt to a wide frequency range of 2 to 20 MHz in which characteristic fluctuation due to firing variation is significantly suppressed. Can be obtained.
【0018】[0018]
【発明の実施の形態】本発明の圧電磁器組成物は、金属
元素として少なくともBa、BiおよびTiを含有し、
モル比による組成式をBi4Ti3O12・x{(Ba1-a
Aa)TiO3}と表したとき、前記x、aが0.5≦x
≦0.9、0≦a≦0.4、Aは、Bi、La、Nd、
GdおよびPrのうち少なくとも1種を満足する主成分
と、該主成分100重量部に対してMnをMnO2換算
で0.05〜1.5重量部含有するものである。BEST MODE FOR CARRYING OUT THE INVENTION The piezoelectric ceramic composition of the present invention contains at least Ba, Bi and Ti as metallic elements,
The composition formula based on the molar ratio is Bi 4 Ti 3 O 12 · x {(Ba 1-a
A a ) TiO 3 }, the above x and a are 0.5 ≦ x
≦ 0.9, 0 ≦ a ≦ 0.4, A is Bi, La, Nd,
A main component satisfying at least one of Gd and Pr, and 0.05 to 1.5 parts by weight of Mn in terms of MnO 2 with respect to 100 parts by weight of the main component.
【0019】ここで、係数であるxを上記の範囲に設定
した理由ついて説明する。上記組成式において、xを
0.5≦x≦0.9の範囲に設定した理由は、xが0.
5より少ないとP/Vが55dBより小さくなるからで
ある。一方xが0.9より多いとP/Vが55dBより
小さくなるとともに、位相歪みの発生頻度が大きくなり
安定した発振子を得ることができないからである。Now, the reason why the coefficient x is set in the above range will be described. In the above composition formula, the reason for setting x in the range of 0.5 ≦ x ≦ 0.9 is that x is 0.
This is because if it is less than 5, P / V becomes smaller than 55 dB. On the other hand, if x is more than 0.9, P / V will be less than 55 dB and the frequency of phase distortion will increase, so that a stable oscillator cannot be obtained.
【0020】また、0.5≦x≦0.9の範囲において
は、焼成密度の焼成温度依存性が小さくなることから焼
成温度の範囲を広く設定でき、焼成ばらつきによるP/
Vの特性変動や位相歪みの発生を著しく抑制できること
から、歩留まりが高く安定した発振子を得ることができ
る。xは、P/Vをより大きくするとともに、位相歪み
の発生を著しく抑制するという理由から、0.6≦x≦
0.8であることが望ましい。Further, in the range of 0.5 ≦ x ≦ 0.9, the firing temperature dependency of the firing density is reduced, so that the firing temperature range can be set broadly and P /
Since it is possible to remarkably suppress the characteristic variation of V and the occurrence of phase distortion, it is possible to obtain a stable oscillator having a high yield. x is 0.6 ≦ x ≦ for the reason that P / V is made larger and phase distortion is significantly suppressed.
It is preferably 0.8.
【0021】また、本発明では0≦a≦0.4を満足す
るものであり、特に0<a≦0.4を満足することが望
ましい。Baの一部を、Bi、La、Nd、Gdおよび
Prのうち少なくとも1種で置換することにより、焼成
温度の範囲が広くなることから、焼成ばらつきによるP
/Vなどの特性変動を著しく低下させることができるか
らである。特に、焼成温度範囲を広くし焼成ばらつきに
よるP/Vの特性変動を著しく小さくするという理由か
ら、0.1≦a≦0.2とすることが望ましい。Further, in the present invention, 0 ≦ a ≦ 0.4 is satisfied, and it is particularly desirable that 0 <a ≦ 0.4 is satisfied. By substituting a part of Ba with at least one of Bi, La, Nd, Gd, and Pr, the range of the firing temperature is widened, so that P due to variations in firing is increased.
This is because characteristic fluctuations such as / V can be significantly reduced. In particular, it is desirable to set 0.1 ≦ a ≦ 0.2 for the reason that the firing temperature range is widened and the variation in P / V characteristics due to firing variations is significantly reduced.
【0022】特にP/Vを55dBより大きくしながら
位相歪みの発生を著しく低減させ、焼成温度の範囲を広
くでき、焼成ばらつきによる特性変動を低下させるとい
う点から、Baの一部をBiで置換することが望まし
く、特にP/Vをより大きくするという理由から、0.
1≦a≦0.15とすることが望ましい。即ち、主成分
が、モル比による組成式をBi4Ti3O12・x{(Ba
1-aBia)TiO3}と表したとき、0.6≦x≦0.
8、0<a≦0.4、特に0.1≦a≦0.15を満足
することが望ましい。In particular, a part of Ba is replaced with Bi from the viewpoint that the generation of phase distortion can be remarkably reduced while the P / V is made larger than 55 dB, the firing temperature range can be widened, and the characteristic fluctuation due to firing variations can be reduced. It is desirable that the P.V.
It is desirable that 1 ≦ a ≦ 0.15. That is, the main component has a composition formula of Bi 4 Ti 3 O 12 · x {(Ba
1-a Bi a) when expressed as TiO 3}, 0.6 ≦ x ≦ 0.
It is desirable to satisfy 8 and 0 <a ≦ 0.4, particularly 0.1 ≦ a ≦ 0.15.
【0023】また、主成分に対してMnO2を含有せし
めることにより、P/Vの向上に大きく向上できるが、
MnO2含有量が主成分l00重量部に対してl.5重
量部より多いと体積固有抵抗値が下がり、分極時に電流
が流れ充分な分極ができず厚み滑り振動のP/Vが低く
なるからである。一方、0.05重量部よりも少なくな
るとチッピングが生じやすく位相歪みが出やすくなるか
らである。Mnは、焼結性を高め、P/Vを大きくする
という点から、主成分100重量部に対して、MnO2
換算で0.3〜0.7重量部含有することが望ましい。Further, by adding MnO 2 to the main component, the P / V can be greatly improved.
The content of MnO 2 is less than 100 parts by weight of the main component. This is because if the amount is more than 5 parts by weight, the volume resistivity value decreases, a current flows during polarization and sufficient polarization cannot be performed, and the P / V of thickness shear vibration decreases. On the other hand, if the amount is less than 0.05 parts by weight, chipping easily occurs and phase distortion easily occurs. Mn enhances sinterability and increases P / V, so that MnO 2 is added to 100 parts by weight of the main component.
It is desirable to contain 0.3 to 0.7 parts by weight in terms of conversion.
【0024】本発明の圧電磁器組成物においては、組成
式としてBi4Ti3O12・x{(Ba1-aAa)Ti
O3}で表されるが、主結晶相としてはビスマス層状化
合物からなるものである。即ち、本発明の圧電磁器組成
物は、(Ba1-aAa)xBi4Ti 3+xO12+3xと表すこと
ができ、(Bi2O2)2+(αm-1βmO3m+1)2-で書き表
されるビスマス層状化合物の一般式において、αサイト
とβサイト及び酸素サイトに欠陥をともないながらがら
m=4の結晶構造を有し、Mnが一部固溶したビスマス
層状化合物になっていると考えられる。Mnは主結晶相
中に固溶し、一部Mn化合物の結晶として粒界に析出す
る場合がある。また、その他の結晶相として、パイロク
ロア相、ペロブスカイト相、構造の異なるBi層状化合
物が存在することもあるが、微量であれば特性上問題な
い。In the piezoelectric ceramic composition of the present invention, the composition
Bi as an expressionFourTi3O12・ X {(Ba1-aAa) Ti
O3}, Bismuth layered as the main crystal phase
It consists of compound. That is, the piezoelectric ceramic composition of the present invention
The thing is (Ba1-aAa)xBiFourTi 3 + xO12 + 3xTo express
And (Bi2O2)2+(Αm-1βmO3m + 1)2-Written in
In the general formula of the bismuth layered compound
And β-site and oxygen site with defects
Bismuth, which has a crystal structure of m = 4 and partially contains Mn as a solid solution
It is considered to be a layered compound. Mn is the main crystal phase
It forms a solid solution in the crystal and partly precipitates at the grain boundaries as Mn compound crystals.
There is a case. In addition, as another crystal phase,
Lower phase, perovskite phase, Bi layered compound with different structure
There may be things, but if there is a small amount, it is not a problem in terms of characteristics.
Yes.
【0025】本発明の圧電磁器組成物は、粉砕時のZr
O2ボールからZr等が混入する場合もあるが、微量で
あれば特性上問題ない。The piezoelectric ceramic composition of the present invention contains Zr when crushed.
Zr or the like may be mixed from the O 2 ball, but if the amount is very small, there is no problem in terms of characteristics.
【0026】本発明の組成を有する圧電磁器は、例え
ば、原料として、BaCO3、Bi2O 3、MnO2、Ti
O2、La2O3、Pr2O3、Nd2O3、Gd2O3からな
る各種酸化物或いはその塩を用いることができる。原料
はこれに限定されず、焼成により酸化物を生成する炭酸
塩、硝酸塩等の金属塩を用いても良い。A piezoelectric ceramic having the composition of the present invention is, for example,
For example, as a raw material, BaCO3, Bi2O 3, MnO2, Ti
O2, La2O3, Pr2O3, Nd2O3, Gd2O3Empty
Various oxides or salts thereof can be used. material
Is not limited to this, carbonic acid that forms an oxide by firing
A metal salt such as salt or nitrate may be used.
【0027】これらの原料を上記した組成となるように
秤量し、混合後の平均粒度分布(D 50)が0.3〜1μ
mの範囲になるように粉砕し、この混合物を850〜1
000℃で仮焼し、仮焼後の平均粒度分布(D50)が
0.3〜1μmの範囲になるように粉砕し、再度所定の
有機バインダを加え湿式混合し造粒する。These raw materials are made to have the above composition.
Average particle size distribution (D 50) Is 0.3-1μ
Grind to a range of m, and mix this mixture from 850 to 1
Calcination at 000 ° C, average particle size distribution (D50)But
Pulverize to a range of 0.3-1 μm, and again
Add an organic binder and wet mix to granulate.
【0028】このようにして得られた粉体を、公知のプ
レス成形等により所定形状に成形し、大気中等の酸化性
雰囲気において1000〜1250℃の温度範囲で2〜
5時間焼成し、本発明の組成を有する圧電磁器が得られ
る。The powder thus obtained is molded into a predetermined shape by a known press molding or the like, and the powder is heated in an oxidizing atmosphere such as air at a temperature range of 1000 to 1250 ° C.
After firing for 5 hours, a piezoelectric ceramic having the composition of the present invention is obtained.
【0029】本発明の組成を有する圧電磁器は、図1に
示すようなピアス発振回路の発振子の圧電磁器、特に厚
み滑り振動の基本波振動を利用する高周波発振子用とし
て最適であるが、それ以外の圧電共振子、超音波振動
子、超音波モータおよび加速度センサ、ノッキングセン
サ、AEセンサ等の圧電センサなどにも用いることがで
きる。The piezoelectric ceramic having the composition of the present invention is most suitable for the piezoelectric ceramic of the oscillator of the Pierce oscillator circuit as shown in FIG. 1, especially for the high frequency oscillator utilizing the fundamental vibration of the thickness shear vibration. Other piezoelectric resonators, ultrasonic transducers, ultrasonic motors and acceleration sensors, knock sensors, piezoelectric sensors such as AE sensors, and the like can also be used.
【0030】図2に本発明の圧電共振子(圧電発振子)
を示す。この圧電共振子は、上記した組成の圧電磁器1
の両面に電極2、3を形成して構成されている。このよ
うな圧電共振子では、厚み滑り振動における基本波のP
/Vを高くでき、発振余裕度が高まり、共振周波数と反
共振周波数の間の周波数で移相歪みが発生しないことか
ら安定した発振が得られ、さらに発振周波数の温度安定
性に優れた高精度な発振が得られ、特に2〜20MHz
の周波数に適応できる圧電発振子を得ることができる。FIG. 2 shows a piezoelectric resonator (piezoelectric oscillator) of the present invention.
Indicates. This piezoelectric resonator is a piezoelectric ceramic 1 having the above composition.
The electrodes 2 and 3 are formed on both surfaces of. In such a piezoelectric resonator, P of the fundamental wave in thickness shear vibration is
/ V can be increased, the oscillation margin can be increased, and stable oscillation can be obtained because phase shift distortion does not occur at a frequency between the resonance frequency and the anti-resonance frequency. Further, the oscillation frequency has high temperature stability and high precision. Oscillation is obtained, especially 2 to 20 MHz
It is possible to obtain a piezoelectric oscillator that can be adapted to the frequency of.
【0031】[0031]
【実施例】まず、出発原料として純度99.9%のBa
CO3粉末、Bi2O3粉末、MnO2粉末、TiO2粉
末、La2O3粉末、Pr2O3粉末、Nd2O3粉末、Gd
2O3粉末を、モル比による組成式を主成分Bi4Ti3O
12・x{(Ba1-aAa)TiO3}と表したとき、A、
x、aが表1に示すような元素、値の主成分と、この主
成分100重量部に対してMnO2粉末を表1に示すよ
うな重量部となるように秤量混合した。EXAMPLE First, as a starting material, Ba having a purity of 99.9% was used.
CO 3 powder, Bi 2 O 3 powder, MnO 2 powder, TiO 2 powder, La 2 O 3 powder, Pr 2 O 3 powder, Nd 2 O 3 powder, Gd
The composition formula of 2 O 3 powder based on the molar ratio is Bi 4 Ti 3 O as the main component.
When expressed as 12 · x {(Ba 1-a A a ) TiO 3 }, A,
The main components of x and a having the elements and values shown in Table 1 and MnO 2 powder were weighed and mixed so that 100 parts by weight of the main components would be the weight parts shown in Table 1.
【0032】秤量した原料粉末を、純度99.9%のジ
ルコニアボール、イオン交換水と共に500mlポリポ
ットに投入し、16時間回転ミルにて混合した。The weighed raw material powder was put into a 500 ml polypot together with zirconia balls having a purity of 99.9% and ion-exchanged water, and mixed in a rotary mill for 16 hours.
【0033】混合後のスラリ−を大気中にて乾燥し、#
40メッシュを通し、その後、大気中950℃、3時間
保持して仮焼し、この合成粉末を純度99.9%のZr
O2ボールとイオン交換水と共に500mlポリポット
に投入し、20時間粉砕して評価粉末を得た。The mixed slurry is dried in the atmosphere,
After passing through a 40-mesh, it was kept in the air at 950 ° C. for 3 hours to be calcined, and this synthetic powder was purified with Zr having a purity of 99.9%.
The powder was put into a 500 ml polypot together with O 2 balls and ion-exchanged water and ground for 20 hours to obtain an evaluation powder.
【0034】この粉末に適量の有機バインダーを添加し
て造粒し、金型プレスにて150MPaで長さ25m
m、幅38mm、厚みlmmの板状に成形し、大気中に
おいて1050℃〜1250℃で3時間本焼成し圧電磁
器を得た。An appropriate amount of an organic binder was added to this powder to granulate it, and the length was 25 m at 150 MPa with a die press.
m, a width of 38 mm, and a thickness of 1 mm were formed into a plate shape, and main firing was performed in the atmosphere at 1050 ° C to 1250 ° C for 3 hours to obtain a piezoelectric ceramic.
【0035】その後、長さ6mm、幅30mmに加工
後、長さ方向に分極するための端面電極を形成し分極処
理を施した。その後、分極用電極を除去し、厚み約0.
17mmとなるようにラップ機により加工した。その
後、長さ6mmと幅30mmからなる面の両面にCr−
Agを蒸着し、電極と磁器との密着強度を高めるために
250℃で12時間のアニール処理を施した。Then, after processing into a length of 6 mm and a width of 30 mm, an end face electrode for polarization in the length direction was formed and subjected to polarization treatment. After that, the polarization electrode is removed, and the thickness is about 0.
It processed with the lapping machine so that it might become 17 mm. After that, Cr-on both sides of the surface consisting of 6 mm in length and 30 mm in width
Ag was vapor-deposited, and an annealing treatment was performed at 250 ° C. for 12 hours in order to enhance the adhesion strength between the electrode and the porcelain.
【0036】その後、図2に示す電極構造となるよう
に、無電極に相当する部位の電極をエッチングで除去
し、長さ2.2mm(L)、幅0.9mm(W)、厚み
0.17mm(H)形状にダイシングソーを用いて加工
し、8MHzの発振に相当する小型な厚み滑り振動の基
本波振動用発振子を得た。図2において、Pは分極方向
を示す。After that, the electrode in a portion corresponding to no electrode is removed by etching so as to obtain the electrode structure shown in FIG. 2, and the length is 2.2 mm (L), the width is 0.9 mm (W), and the thickness is 0. A 17 mm (H) shape was processed by using a dicing saw to obtain a small oscillator for fundamental wave vibration of thickness shear vibration corresponding to 8 MHz oscillation. In FIG. 2, P indicates the polarization direction.
【0037】発振子の特性は、インピーダンスアナライ
ザによリインピーダンス波形を測定し、厚み滑り振動の
基本波振動でのP/VをP/V=20×Log(Ra/
R0)の式により算出した(但し、Ra:反共振インピー
ダンス、R0:共振インピーダンス)。The characteristics of the oscillator are measured by measuring the re-impedance waveform with an impedance analyzer, and P / V at the fundamental vibration of thickness shear vibration is P / V = 20 × Log (R a /
R 0 ) was calculated by the equation (where R a is the anti-resonance impedance and R 0 is the resonance impedance).
【0038】さらにインピーダンス波形より、共振周波
数と反共振周波数の間で位相が約−90゜から約+90
゜に位相反転した後の約+90゜の位相からなる周波数
帯域において、10゜を超える位相歪みが発生するか否
かを調査した。位相歪みの評価は、位相歪み=|(+)
側の最大位相値−最大値から局所的に変化した位相値|
により求め、共振子100個中5個以上において10゜
を超える位相歪みが発生した場合においては×、それ以
下の場合は○とした。Further, according to the impedance waveform, the phase is about −90 ° to about +90 between the resonance frequency and the anti-resonance frequency.
It was investigated whether or not a phase distortion of more than 10 ° would occur in a frequency band composed of about + 90 ° phase after being inverted to 0 °. Phase distortion is evaluated by phase distortion = | (+)
Side maximum phase value-phase value locally changed from the maximum value |
When the phase distortion of more than 10 out of 100 resonators was more than 10 °, it was evaluated as x, and when it was less than that, it was evaluated as o.
【0039】さらに、同一組成において、焼成温度を1
5℃低下させて密度とP/Vの焼成温度依存性を求め、
焼成温度が15℃変化した場合においてもP/Vの変化
が5%以下である場合を○、5〜10%である場合を
△、P/Vの差が10%より大きい場合を×として、表
1に焼成分布特性として表記した。Further, with the same composition, the firing temperature is 1
Decrease the temperature by 5 ° C to obtain the firing temperature dependence of density and P / V,
When the change in P / V is 5% or less even when the firing temperature changes by 15 ° C., it is Δ when it is 5 to 10%, and when it is more than 10%, the difference is P. It is shown in Table 1 as firing distribution characteristics.
【0040】尚、試料No.21は、SrCO3粉末、
Bi2O3粉末、TiO2粉末をSrBi4Ti4O15とな
るように秤量混合し、1180℃で焼成したものであ
る。また、試料No.29は、SrCO3粉末、Bi2O
3粉末、La2O3粉末、TiO2粉末を(Sr0.9L
a0.1)Bi4Ti4O15となるように秤量混合し、11
70℃で焼成し、試料No.30は、SrCO3粉末、
Bi2O3粉末、La2O3粉末、TiO2粉末を、SrB
i4Ti4O15 100重量部に対してLa2O3が0.5
重量部となるように添加し、1170℃で焼成したもの
である。Sample No. 21 is SrCO 3 powder,
Bi 2 O 3 powder and TiO 2 powder were weighed and mixed so as to be SrBi 4 Ti 4 O 15 and baked at 1180 ° C. In addition, the sample No. 29 is SrCO 3 powder, Bi 2 O
3 powder, La 2 O 3 powder, TiO 2 powder (Sr 0.9 L
a 0.1 ) Bi 4 Ti 4 O 15 Weigh and mix to obtain 11
The sample No. was fired at 70 ° C. 30 is SrCO 3 powder,
Bi 2 O 3 powder, La 2 O 3 powder, TiO 2 powder, SrB
i 4 Ti 4 O 15 is 100 parts by weight, and La 2 O 3 is 0.5.
It is added so as to be added in parts by weight and baked at 1170 ° C.
【0041】さらに、発振周波数の温度変化率は、25
℃の発振周波数を基準にして、−20℃もしくは+80
℃での発振周波数の変化を以下の式により算出した。Further, the temperature change rate of the oscillation frequency is 25
-20 ℃ or +80 based on the oscillation frequency of ℃
The change in oscillation frequency at ° C was calculated by the following formula.
【0042】Fosc変化率(ppm)={(Fosc
(drift)一Fosc(25))/Fosc(2
5)}×100、但し、Fosc(dfift)は、−
20℃もしくは+80℃での発振周波数であり、Fos
c(25)は25℃での発振周波数である。これらの結
果を表1に示す。Fosc change rate (ppm) = {(Fosc
(Drift) 1 Fosc (25)) / Fosc (2
5)} × 100, where Fosc (dfitt) is −
Oscillation frequency at 20 ℃ or + 80 ℃, Fos
c (25) is the oscillation frequency at 25 ° C. The results are shown in Table 1.
【0043】[0043]
【表1】 [Table 1]
【0044】表1から明らかなように、本発明の範囲内
の試料は、厚み滑り振動における基本波振動のP/V値
を55dB以上と大きくでき、且つ10゜を超える位相
歪みが発生しないことから安定した発振を得ることがで
きるとともに、焼成温度範囲が広く、焼成温度変化によ
る特性ばらつきが小さく、さらに、発振周波数の温度変
化率が±3000ppm以内となり小さいことが判る。
また、xの値を小さくしていくと温度変化率を小さくで
きることが判る。As is clear from Table 1, the samples within the range of the present invention can have a large P / V value of the fundamental vibration in the thickness shear vibration of 55 dB or more and do not generate a phase distortion exceeding 10 °. It is found that stable oscillation can be obtained, the firing temperature range is wide, the characteristic variation due to the firing temperature change is small, and the temperature change rate of the oscillation frequency is within ± 3000 ppm, which is small.
Further, it can be seen that the rate of temperature change can be reduced by decreasing the value of x.
【0045】一方、比較例である、試料No.20のM
nを含有しない場合には、焼結体の密度が低く、P/V
値が43dBと小さく、且つ10゜を上回る位相歪みが
発生し、安定した発振が得られられないことが判る。On the other hand, Sample No. which is a comparative example. 20 M
When n is not contained, the density of the sintered body is low and P / V
It can be seen that the value is as small as 43 dB and the phase distortion exceeds 10 °, so that stable oscillation cannot be obtained.
【0046】また、係数xの値が1の試料No.1の場
合、P/Vは小さく、さらに試作した発振子100個中
10個において10゜を上回る数多くの位相歪みが発生
したことから安定した発振が得られられないことがわか
る。さらに、xの値が0.9より大きい試料No.19
の場合においても、位相歪みが発生しやすいことから、
歩留まりが悪く安定した特性を示す発振子が得られられ
にくいことがわかる。また、試料No.29、30は、
発振周波数の温度変化率が±6000ppmを越えるこ
とが判る。Sample No. 1 having a coefficient x value of 1 In the case of 1, the P / V was small, and moreover, it was found that stable oscillation could not be obtained because a large number of phase distortions exceeding 10 ° occurred in 10 out of 100 prototyped oscillators. Furthermore, the sample No. in which the value of x is larger than 0.9. 19
Even in the case of, since phase distortion easily occurs,
It can be seen that it is difficult to obtain an oscillator with poor yield and stable characteristics. In addition, the sample No. 29 and 30 are
It can be seen that the temperature change rate of the oscillation frequency exceeds ± 6000 ppm.
【0047】また、Aの種類をBiにした試料No.7
の場合、P/Vを70dBまで高めながら、−20〜8
0℃の発振周波数の温度変化率を±2250ppm以内
と優れた温度安定性を有していることがわかる。Further, the sample No. in which the type of A is Bi 7
In the case of, while increasing P / V to 70 dB, -20 to 8
It can be seen that the temperature change rate of the oscillation frequency of 0 ° C. is within ± 2250 ppm, which is excellent in temperature stability.
【0048】さらに、Baの一部をLa、Nd、Pr、
Gdで置換した試料No.13、14、15、16、1
7、18の場合、xの値が0.75でP/Vが60dB
以上と大きな値を有しながら、−20〜80℃の発振周
波数の温度変化率が±2900ppm以内と優れた温度
特性を有し発振子として好ましい特性となる。Further, a part of Ba is La, Nd, Pr,
Sample No. replaced with Gd. 13, 14, 15, 16, 1
In case of 7 and 18, x value is 0.75 and P / V is 60 dB
While having a large value as described above, the temperature change rate of the oscillation frequency of −20 to 80 ° C. is within ± 2900 ppm, which is an excellent temperature characteristic, which is a preferable characteristic as an oscillator.
【0049】図3に、本発明の試料No.7のインピー
ダンスと位相特性を、図4に試料No.7の発振周波数
の温度変化率を示した。図5に位相歪みが発生した比較
例の試料No.1のインピーダンスと位相特性を示し
た。FIG. 3 shows the sample No. of the present invention. The impedance and phase characteristics of Sample No. 7 are shown in FIG. The rate of temperature change of the oscillation frequency of No. 7 is shown. The sample No. of the comparative example in which the phase distortion occurred in FIG. The impedance and phase characteristics of No. 1 are shown.
【0050】図4から本発明の試料No.7では大きな
位相歪みが発生せず、また、図4から−20〜80℃の
発振周波数の温度変化率が±3000ppm以内と優れ
た温度特性を有することが判る。一方、図5から、試料
No.1では、共振周波数と反共振周波数の間で位相が
約−90゜から約+90゜に位相反転した後の約+90
゜の位相からなる周波数帯域において、符号Aで示す、
位相が10゜を超える大きな位相歪みが発生しているこ
とが判る。As shown in FIG. 7, no large phase distortion is generated, and it can be seen from FIG. 4 that the temperature change rate of the oscillation frequency of −20 to 80 ° C. is within ± 3000 ppm, which is an excellent temperature characteristic. On the other hand, from FIG. In the case of 1, the phase between the resonance frequency and the anti-resonance frequency is about +90 after the phase is inverted from about -90 ° to about + 90 °.
In the frequency band consisting of the phase of °, shown by the symbol A,
It can be seen that a large phase distortion of which the phase exceeds 10 ° has occurred.
【0051】さらに、図6に試料No.7と、従来より
知られた組成からなる試料No.21の密度の焼成温度
依存性を示した。図7に、試料No.7と試料No.2
1のP/Vの焼成温度依存性を示した。これらのグラフ
から、本発明の試料では、広い焼成温度範囲で磁器密度
が高くかつ一定であることから、焼成温度が多少ばらつ
いたとしても磁器密度が殆ど変化せず、P/Vも殆ど変
化しないことが判る。Further, in FIG. No. 7 and sample No. 7 having a conventionally known composition. 21 showed the firing temperature dependence of the density. 7 shows the sample No. 7 and sample No. Two
The firing temperature dependence of P / V of No. 1 was shown. From these graphs, in the sample of the present invention, since the porcelain density is high and constant in a wide firing temperature range, the porcelain density hardly changes and the P / V hardly changes even if the firing temperature varies a little. I understand.
【0052】このように、本発明の組成を有する圧電磁
器においては、特に、厚み滑り振動の基本波振動のP/
Vを大きくできるとともに、共振周波数と反共振周波数
の間において、10゜を超える位相歪みが発生せず、さ
らに、−20℃〜80℃での発振周波数の温度変化率を
小さくすることができ、さらに焼成温度依存性を小さく
できることから発振子の安定性を向上できる。As described above, in the piezoelectric ceramic having the composition of the present invention, in particular, P / of the fundamental wave vibration of the thickness shear vibration
V can be increased, phase distortion exceeding 10 ° does not occur between the resonance frequency and the anti-resonance frequency, and the temperature change rate of the oscillation frequency at −20 ° C. to 80 ° C. can be reduced. Furthermore, since the firing temperature dependency can be reduced, the stability of the oscillator can be improved.
【0053】また、図8に試料No.7のX線回折図を
示す。図8からビスマス層状化合物を主結晶相としてい
ることが分かる。試料No.7は基本組成式としてはB
i4Ti3O12・0.75{(Ba0.85Bi0.15)TiO
3}のビスマス層状化合物とペロブスカイト化合物の組
み合わせとして書き表している。一方ビスマス層状化合
物は一般式として(Bi2O2)2+(αm-1βmO3m+1)2-
で書き表されるが、Bi4Ti3O12は一般式のαの元素
はBi3+で、βの元素はTi4+からなるm=3のビスマ
ス層状化合物であり電気的な中性条件は保たれている。Further, in FIG. 7 shows an X-ray diffractogram of 7. It can be seen from FIG. 8 that the bismuth layer compound is the main crystal phase. Sample No. 7 is B as a basic composition formula
i 4 Ti 3 O 12 · 0.75 {(Ba 0.85 Bi 0.15 ) TiO
3 } is shown as a combination of the bismuth layered compound and the perovskite compound. On the other hand, the bismuth layered compound has a general formula of (Bi 2 O 2 ) 2+ (α m-1 β m O 3m + 1 ) 2-
Bi 4 Ti 3 O 12 is a bismuth layered compound of m = 3 consisting of Bi 3+ as the α element and Ti 4+ as the β element in the general formula, and is electrically neutral. Is kept.
【0054】図8の試料No.7のX線回折図から、m
=4のビスマス層状化合物が主結晶相として認められる
事から、ペロブスカイト化合物はm=3からなるビスマ
ス層状化合物に取りこまれて、m=4の結晶を有するよ
うになったものと考えることができる。即ち、試料N
o.7のαはBi、Baからなる元素からなり、またβ
はTiからなる元素で構成され、αサイトとβサイト及
び酸素サイトに欠陥をともないながらがらm=4の結晶
構造を有し、具体的には(Ba0.85Bi0.15)0. 75Bi
4Ti3.75O14.25にMnが一部固溶したビスマス層状化
合物になっているものと考えている。The sample No. of FIG. From the X-ray diffraction pattern of No. 7, m
= 4 bismuth layered compound is recognized as the main crystal phase, it can be considered that the perovskite compound was incorporated into the bismuth layered compound of m = 3 to have crystals of m = 4. . That is, sample N
o. Α in 7 consists of the elements consisting of Bi and Ba, and β
Consists of elements consisting of Ti, it has a crystal structure of reluctant m = 4 while accompanied by defects in α site and β site and the oxygen site, specifically (Ba 0.85 Bi 0.15) 0. 75 Bi
It is considered that the bismuth layered compound is a solid solution of Mn in 4 Ti 3.75 O 14.25 .
【0055】[0055]
【発明の効果】以上詳述したように、本発明の圧電磁器
組成物では、厚み滑り振動における基本波振動のP/V
値を大きくしながら、共振周波数と反共振周波数の間で
10゜を超える位相歪みの発生を著しく少なくすること
ができ、さらに共振周波数の温度変化率が小さく、さら
に焼成温度範囲が広くなることから焼成ばらつきによる
P/Vの特性変動を抑制でき、高い歩留まりが実現でき
る。As described above in detail, in the piezoelectric ceramic composition of the present invention, the P / V of the fundamental vibration in the thickness shear vibration is
While increasing the value, it is possible to remarkably reduce the occurrence of phase distortion exceeding 10 ° between the resonance frequency and the anti-resonance frequency, further reduce the temperature change rate of the resonance frequency, and further widen the firing temperature range. P / V characteristic variations due to firing variations can be suppressed, and high yield can be realized.
【図1】コルピッツ型発振回路を原型としたピアス発振
回路を示した概略図である。FIG. 1 is a schematic diagram showing a Pierce oscillator circuit that is a prototype of a Colpitts oscillator circuit.
【図2】8MHz用発振子の概略図である。FIG. 2 is a schematic view of an 8 MHz oscillator.
【図3】本発明の試料No.7のインピーダンスと位相
特性を示すグラフである。FIG. 3 shows the sample No. of the present invention. 7 is a graph showing impedance and phase characteristics of No. 7;
【図4】本発明の試料No.7の発振周波数の温度変化
率を示すグラフである。FIG. 4 shows a sample No. of the present invention. 7 is a graph showing the temperature change rate of the oscillation frequency of No. 7;
【図5】比較例の試料No.1のインピーダンスと位相
歪みを表すグラフである。5 is a sample No. of a comparative example. It is a graph showing the impedance of 1 and phase distortion.
【図6】試料No.7と試料No.21の密度の焼成温
度依存性を示すグラフである。6 is a sample No. 7 and sample No. It is a graph which shows the firing temperature dependence of the density of 21.
【図7】試料No.7と試料No.21のP/Vの焼成
温度依存性を示すグラフである。7] Sample No. 7 and sample No. It is a graph which shows the firing temperature dependence of P / V of 21.
【図8】試料No.7の粉末X線回折図を示す。8] Sample No. 7 shows a powder X-ray diffraction pattern of No. 7.
l・・・圧電磁器 2、3・・・電極 l ... Piezoelectric ceramic 2, 3 ... Electrodes
Claims (3)
びTiを含有し、モル比による組成式を Bi4Ti3O12・x{(Ba1-aAa)TiO3} と表したとき、前記x、aが 0.5≦x≦0.9 0≦a≦0.4 Aは、Bi、La、Nd、GdおよびPrのうち少なく
とも1種 を満足する主成分と、該主成分100重量部に対してM
nをMnO2換算で0.05〜1.5重量部含有するこ
とを特徴とする圧電磁器組成物。1. When at least Ba, Bi and Ti are contained as a metal element and the composition formula by molar ratio is expressed as Bi 4 Ti 3 O 12 .x {(Ba 1-a A a ) TiO 3 }, x and a are 0.5 ≦ x ≦ 0.9 0 ≦ a ≦ 0.4 A is a main component satisfying at least one of Bi, La, Nd, Gd and Pr, and 100 parts by weight of the main component. Against M
A piezoelectric ceramic composition containing 0.05 to 1.5 parts by weight of n in terms of MnO 2 .
ともに、前記圧電磁器が、請求項1記載の圧電磁器組成
物からなることを特徴とする圧電共振子。2. A piezoelectric resonator, wherein electrodes are formed on both main surfaces of the piezoelectric ceramic, and the piezoelectric ceramic comprises the piezoelectric ceramic composition according to claim 1.
とする請求項2記載の圧電共振子。3. The piezoelectric resonator according to claim 2, which operates in a thickness shear vibration mode.
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| JP2001222972A JP4471542B2 (en) | 2001-07-24 | 2001-07-24 | Piezoelectric ceramic composition and piezoelectric resonator |
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Cited By (7)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2004087611A1 (en) * | 2003-03-28 | 2004-10-14 | Tdk Corporation | Piezoelectric ceramic |
| WO2008078703A1 (en) | 2006-12-25 | 2008-07-03 | Kyocera Corporation | Piezoelectric ceramic and piezoelectric element |
| WO2008081842A1 (en) * | 2006-12-26 | 2008-07-10 | Kyocera Corporation | Piezoelectric ceramic material and piezoelectric element |
| JP2008285340A (en) * | 2007-05-15 | 2008-11-27 | Kyocera Corp | Piezoelectric ceramic and piezoelectric element |
| JP2009084067A (en) * | 2007-09-27 | 2009-04-23 | Kyocera Corp | Piezoelectric ceramic and piezoelectric element |
| JP2010047465A (en) * | 2008-07-25 | 2010-03-04 | Kyocera Corp | Piezoelectric ceramic and piezoelectric element using the same |
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Cited By (11)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2004087611A1 (en) * | 2003-03-28 | 2004-10-14 | Tdk Corporation | Piezoelectric ceramic |
| US7390426B2 (en) | 2003-03-28 | 2008-06-24 | Tdk Corporation | Piezoelectric ceramic |
| WO2008078703A1 (en) | 2006-12-25 | 2008-07-03 | Kyocera Corporation | Piezoelectric ceramic and piezoelectric element |
| JP2008179525A (en) * | 2006-12-25 | 2008-08-07 | Kyocera Corp | Piezoelectric ceramic and piezoelectric element |
| EP2119685A4 (en) * | 2006-12-25 | 2011-07-13 | Kyocera Corp | PIEZOELECTRIC CERAMIC AND PIEZOELECTRIC ELEMENT |
| US8258679B2 (en) | 2006-12-25 | 2012-09-04 | Kyocera Corporation | Piezoelectric ceramic comprising a bismuth layered compound and piezoelectric element |
| WO2008081842A1 (en) * | 2006-12-26 | 2008-07-10 | Kyocera Corporation | Piezoelectric ceramic material and piezoelectric element |
| JP2008285340A (en) * | 2007-05-15 | 2008-11-27 | Kyocera Corp | Piezoelectric ceramic and piezoelectric element |
| JP2009084067A (en) * | 2007-09-27 | 2009-04-23 | Kyocera Corp | Piezoelectric ceramic and piezoelectric element |
| JP2010047465A (en) * | 2008-07-25 | 2010-03-04 | Kyocera Corp | Piezoelectric ceramic and piezoelectric element using the same |
| JP2016025193A (en) * | 2014-07-18 | 2016-02-08 | 国立研究開発法人産業技術総合研究所 | Broadband high-sensitivity ae sensor |
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