JPS5943620A - Piezoelectric ceramic element - Google Patents
Piezoelectric ceramic elementInfo
- Publication number
- JPS5943620A JPS5943620A JP57154204A JP15420482A JPS5943620A JP S5943620 A JPS5943620 A JP S5943620A JP 57154204 A JP57154204 A JP 57154204A JP 15420482 A JP15420482 A JP 15420482A JP S5943620 A JPS5943620 A JP S5943620A
- Authority
- JP
- Japan
- Prior art keywords
- piezoelectric ceramic
- ceramic element
- pair
- thickness
- vibration
- 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
Links
- 239000000919 ceramic Substances 0.000 title claims abstract description 57
- 239000007769 metal material Substances 0.000 claims abstract description 11
- NKZSPGSOXYXWQA-UHFFFAOYSA-N dioxido(oxo)titanium;lead(2+) Chemical compound [Pb+2].[O-][Ti]([O-])=O NKZSPGSOXYXWQA-UHFFFAOYSA-N 0.000 claims abstract description 10
- 230000010287 polarization Effects 0.000 description 5
- 229910010293 ceramic material Inorganic materials 0.000 description 3
- 230000008878 coupling Effects 0.000 description 2
- 238000010168 coupling process Methods 0.000 description 2
- 238000005859 coupling reaction Methods 0.000 description 2
- 230000010355 oscillation Effects 0.000 description 2
- 238000007738 vacuum evaporation Methods 0.000 description 2
- FERIUCNNQQJTOY-UHFFFAOYSA-M Butyrate Chemical compound CCCC([O-])=O FERIUCNNQQJTOY-UHFFFAOYSA-M 0.000 description 1
- BQCADISMDOOEFD-UHFFFAOYSA-N Silver Chemical compound [Ag] BQCADISMDOOEFD-UHFFFAOYSA-N 0.000 description 1
- RTAQQCXQSZGOHL-UHFFFAOYSA-N Titanium Chemical compound [Ti] RTAQQCXQSZGOHL-UHFFFAOYSA-N 0.000 description 1
- 239000011230 binding agent Substances 0.000 description 1
- 230000001419 dependent effect Effects 0.000 description 1
- 238000000151 deposition Methods 0.000 description 1
- 230000008021 deposition Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 230000005684 electric field Effects 0.000 description 1
- PCHJSUWPFVWCPO-UHFFFAOYSA-N gold Chemical compound [Au] PCHJSUWPFVWCPO-UHFFFAOYSA-N 0.000 description 1
- 239000010931 gold Substances 0.000 description 1
- 229910052737 gold Inorganic materials 0.000 description 1
- 229910052735 hafnium Inorganic materials 0.000 description 1
- 238000011534 incubation Methods 0.000 description 1
- 229910052748 manganese Inorganic materials 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 229910052751 metal Inorganic materials 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 238000011084 recovery Methods 0.000 description 1
- 229910052709 silver Inorganic materials 0.000 description 1
- 239000004332 silver Substances 0.000 description 1
- 229910000679 solder Inorganic materials 0.000 description 1
- 238000004544 sputter deposition Methods 0.000 description 1
- 229910052719 titanium Inorganic materials 0.000 description 1
- 239000010936 titanium Substances 0.000 description 1
- 229910052721 tungsten Inorganic materials 0.000 description 1
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03H—IMPEDANCE NETWORKS, e.g. RESONANT CIRCUITS; RESONATORS
- H03H9/00—Networks comprising electromechanical or electro-acoustic elements; Electromechanical resonators
- H03H9/15—Constructional features of resonators consisting of piezoelectric or electrostrictive material
- H03H9/17—Constructional features of resonators consisting of piezoelectric or electrostrictive material having a single resonator
- H03H9/177—Constructional 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)
Abstract
Description
【発明の詳細な説明】
この発明は、圧電セラミクス素子に関し、特に厚みすべ
り1ネルギ閉じ込め振動モードを利用するチタン酸鉛系
圧電セラミクス素子に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a piezoelectric ceramic element, and more particularly to a lead titanate-based piezoelectric ceramic element that utilizes a thickness-shear one-energy confined vibration mode.
従来、フィルタ、発振子などを構成する圧電セラミクス
素子として、PZT系すなわちPb (Zr 、 J
i> os系セラミクス材料が用いられてきた。PZl
−系セラミクス素子では、厚み縦振動モードおよび厚み
すべり振動L−ドが利用されている。第1図は、厚み縦
振動モードのうち厚み組]−ネルギ閉じ込め振動モード
を利用りる[)ZT系圧電セラミクス素子を概略的に示
づ側面図である。Conventionally, PZT-based piezoelectric ceramic elements constituting filters, oscillators, etc., namely Pb (Zr, J
i> os ceramic materials have been used. PZl
- type ceramic elements utilize a thickness longitudinal vibration mode and a thickness shear vibration L-mode. FIG. 1 is a side view schematically showing a ZT-based piezoelectric ceramic element that utilizes the thickness group]-energy confined vibration mode among the thickness longitudinal vibration modes.
第1図から明らかなように、厚み縦エネルギ閉じ込め振
動モードを利用する圧電セラミクス素子1では、1対の
対向電極2.3は、その対向方向が分極軸方向Pと同一
となるように形成されている。As is clear from FIG. 1, in the piezoelectric ceramic element 1 that utilizes the thickness longitudinal energy confinement vibration mode, the pair of opposing electrodes 2.3 are formed so that their opposing direction is the same as the polarization axis direction P. ing.
他方、第2図は、厚みすべり振動モードのうち厚みすべ
りエネルギ閉じ込め振動モードを利用づる従来から用い
られできたP Z T系L1電セラミクス素子5を示す
側面図である。厚みすべりエネルギ閉じ込め振動モード
を利用する圧電セラミクス素子5では、1対の対向電極
2,3の対向方向が、分極軸方向Pと垂直となるように
1対の対向電極2.3が形成されている。ところで、圧
電セラミクス素子をフィルタなどに用いる際には、その
インピーダンスマツチングのためにその誘電率εが小さ
いこと、ならびに安定性を確保するためにQIが大きい
ことなどが要請されるが、従来のP7丁系圧電セラミク
ス素子では、これらの要請を満たずことはできなかった
。On the other hand, FIG. 2 is a side view showing a conventionally used PZT-based L1 electroceramic element 5 that utilizes the thickness shear energy trapped vibration mode among the thickness shear vibration modes. In the piezoelectric ceramic element 5 that utilizes the thickness shear energy trapping vibration mode, the pair of opposing electrodes 2 and 3 are formed such that the opposing direction of the pair of opposing electrodes 2 and 3 is perpendicular to the polarization axis direction P. There is. By the way, when piezoelectric ceramic elements are used in filters, etc., they are required to have a small dielectric constant ε for impedance matching, and a large QI to ensure stability. P7-type piezoelectric ceramic elements have not been able to meet these requirements.
他方、近年、低誘電率(ε−300)および高Qmのセ
ラミクス材料として、ブータン酸鉛系セラミクス(1−
T系セラミクス)が開発され、注目を集め−(いる。チ
タン酸鉛系セラミクスでは、誘電率εが小さり、)幾械
的Qが高いため、上述のような従来のP/−[系セラミ
クスの欠点を解消し得る。On the other hand, in recent years, lead butanate ceramics (1-
Lead titanate ceramics (T-based ceramics) have been developed and have attracted attention because of their small dielectric constant ε and high mechanical Q. can eliminate the drawbacks of
しかしながら、現在のところ、チタン酸鉛系セラミクス
を用いた圧電セラミクス素子では、厚みすべり振動の3
倍波(T’ E 、 rd)を利用したものは公知であ
るが、より大きな振動を得ることがでさるjワみ縦振動
基本波(TEISt>および厚みづべり振動基本波(T
SISt)は、ともに振動エネルギの閉込めが困難であ
り、これらの振動モードを利用づることは未だ実施され
ていない。もつとも、理論的には、チタン酸鉛系圧電セ
ラミクスを用いて、第2図のような厚みづべり振動を利
用する圧電セラミクス素子を構成して、エネルギを閉込
めることは可能ひあるが、実際には、このようにして構
成した圧電セラミクス素子は、第3図で示寸ように、波
形の分割が発生し、側底利用づる(ことはできなかった
。However, at present, piezoelectric ceramic elements using lead titanate-based ceramics have three types of thickness-shear vibration.
Those using harmonics (T'E, rd) are well known, but it is possible to obtain larger vibrations using the warp longitudinal vibration fundamental wave (TEISt> and the thickness shear vibration fundamental wave (T
SISt), it is difficult to confine vibration energy, and the use of these vibration modes has not yet been implemented. Theoretically, it is possible to use lead titanate-based piezoelectric ceramics to construct a piezoelectric ceramic element that utilizes thickness vibration as shown in Figure 2, and to trap energy, but in reality it is not possible. In the piezoelectric ceramic element constructed in this way, waveform division occurred as shown in FIG. 3, and it was not possible to use the piezoelectric ceramic element at the bottom of the piezoelectric element.
それゆえに、この発明の目的は、チタンrn@1系セラ
ミクスを用いて、従来のP/[系セラミクスからなる圧
電セラミクス材料の欠点を解消し、りなわち誘電率が低
く、機械的Qが高く、かつj9みJべり振動基本波を利
用する、圧電セラミクス素子を提供することである。Therefore, an object of the present invention is to eliminate the drawbacks of the conventional piezoelectric ceramic materials made of P/[ type ceramics by using titanium rn@1 type ceramics, which have a low dielectric constant and a high mechanical Q. It is an object of the present invention to provide a piezoelectric ceramic element that utilizes the fundamental wave of oscillation of j9 and j9 oscillations.
この発明は、要約すれば、チタン酸鉛系セラミクスから
なる圧電セラミクスと、この圧電セラミクスを挾んで対
向する1対の対向電極とを尚え、厚みづべりエネルギ閉
じ込め振動モードを利用する圧電セラミクス素子におい
て、1対の対向電極の少なくとも一方に、質量負荷用金
属材料が(−1着されている圧電セラミクス素子である
。Jなわち、この発明の特徴は、圧電セラミクス素子を
挾んで対向する1対の対向電極の少なくとも一方に、質
は負荷用金属材料が+j着されていることにある。In summary, the present invention is a piezoelectric ceramic element that utilizes a thickness-dependent energy trapping vibration mode, which comprises a piezoelectric ceramic made of lead titanate ceramic, and a pair of opposing electrodes that face each other with the piezoelectric ceramic sandwiched between them. This is a piezoelectric ceramic element in which a mass-loading metal material (-1) is attached to at least one of a pair of opposing electrodes. The quality lies in that a load metal material is deposited on at least one of the pair of opposing electrodes.
質(6)負荷用金属材料としては、l”b、Hf、丁a
。Quality (6) Loading metal materials include l”b, Hf, and a
.
W、pt、13iなどの様々な金W!4祠利を用いるこ
とが可能である。好ましくは、Pbが用いられる。Various gold W such as W, pt, 13i! It is possible to use 4 shrines. Preferably, Pb is used.
Pb表面に生じる酸化膜により、対向電極が保護され、
信頼性が向上覆るからであり、かつ電極に端子をはノυ
だイ→け覆る1県のはんだi=Jけ性が増し、作業性が
向上Jるからである。「質吊負荷用金属月11」のイ」
着につい(は、真空蒸着、スパッタリング、イΔンブレ
ーテイングなどの様々な公知のh法が用いられ19る。The counter electrode is protected by the oxide film formed on the Pb surface,
Reliability is improved because the terminals are covered and the terminals are not connected to the electrodes.
This is because the solder i = J in one prefecture that covers the surface increases, and the workability improves. "Quality Lifting Load Metal Month 11"
For deposition, various known methods such as vacuum evaporation, sputtering, and incubation can be used.
また、質用工1荷用金属材料は、[少なくとも一方」に
形成されればよい。すなわち、対向電極の双方に形成さ
れでもJ、く、あるいtよ一方のみに形成されてもよい
。Further, the metal material for pawn work may be formed on [at least one side]. That is, it may be formed on both sides of the opposing electrodes, or only on one side.
この発明の圧電セラミクス素子は、上述のようなI質量
負荷用金属材料」が1対の対向電極の少なくとも一方に
付着されているため、質燈角荷効果により、完全な■ネ
ルギ閉込め振動をiりることが可能となる。す゛なわち
、従来エネルギの閉込め不可能であった、厚みづべり振
動基本波に基づく振動エネルギを、効果的に閉込めるこ
とが可能となる。また、この発明の圧電セラミクス素子
が、チタン酸鉛系セラミクスを材料とするため、拡がり
振動の電気機械結合係数にとが厚み方向の電気機械結合
係数+<tよりも無視できるほど小さいため、目的の振
動以外の不要な振動が発生しにくく、厚みすべり1ネル
ギ閉じ込め振動モードを利用するため超低スプリアスレ
ベルの圧電セラミクス材料を得ることができる。さらに
、チタン酸鉛系セラミクスでは、上述のように、誘電率
εが小さく、かつ機械的Qが大きいため、素子のハイイ
ンピーダンス化を容易に達成づることができ、かつ安定
度に優れた圧電セラミクス素子を得ることができる。Since the piezoelectric ceramic element of the present invention has the above-mentioned "metal material for mass loading" attached to at least one of the pair of opposing electrodes, the piezoelectric ceramic element of the present invention can completely suppress energy confinement vibration due to the angular charge effect. It becomes possible to move. In other words, it becomes possible to effectively confine the vibration energy based on the fundamental wave of thickness shear vibration, which was conventionally impossible to confine. Furthermore, since the piezoelectric ceramic element of the present invention is made of lead titanate-based ceramics, the electromechanical coupling coefficient of the spreading vibration is negligibly smaller than the electromechanical coupling coefficient +<t in the thickness direction. It is possible to obtain a piezoelectric ceramic material with an ultra-low spurious level because it is difficult to generate unnecessary vibrations other than the vibrations of , and the thickness-shear one-energy confined vibration mode is used. Furthermore, as mentioned above, lead titanate ceramics have a small dielectric constant ε and a large mechanical Q, so it is easy to achieve high impedance of the element, and piezoelectric ceramics have excellent stability. element can be obtained.
以下、実施例につき説明する。Examples will be described below.
実施例
(P ho3o L a c、ツユ ) T
: 03 →−0,5重量%Mn 02 +0.3m
m%CUOの組成の試料を調合し、混合ミル内で湿式混
合し、次に脱水・乾燥し、ざらに仮焼した後にバインダ
を混合して弱水乾燥・造粒した後に、35mmx35I
x 12mmの大きさに形成した。次に、1250℃で
2時間保持し焼成した後に、分極用の電極を800”C
で焼イ」G′Jで、その後80℃で3KV/mlの直流
電界を1時間印加し分極処理を行ない、スライシングマ
シンによりスライスした。スライスしたセラミクスを次
にラップし、かつ銀を蒸着し−C対向電極を形成した。Example (Pho3oLac, Tsuyu) T
: 03 →-0.5wt%Mn 02 +0.3m
A sample with a composition of m% CUO was prepared, wet-mixed in a mixing mill, dehydrated and dried, roughly calcined, mixed with a binder, dried in weak water and granulated.
It was formed to a size of 12 mm x 12 mm. Next, after holding and baking at 1250℃ for 2 hours, the polarization electrode was heated to 80”C.
Thereafter, a DC electric field of 3 KV/ml was applied at 80° C. for 1 hour to perform polarization treatment, and sliced using a slicing machine. The sliced ceramics were then lapped and silver deposited to form a -C counter electrode.
ざらに、この1対の対向電極の上面に、それぞれ、Ni
口荷合属材料としての鉛を真空蒸着により付着した。こ
のようにして準備した圧電セラミクス素子10を、第4
図に側面図で示す。Roughly, Ni
Lead as an additional material was deposited by vacuum evaporation. The piezoelectric ceramic element 10 prepared in this way was
It is shown in side view in the figure.
第4図から明らかなように、(P b、、2a L
aθμ )T’i Os +0.5重量%M002 +
0.3重量%CuOの組成からなる圧電セラミクス11
を挾んで1対の対向層tM12.13が形成されている
。As is clear from Fig. 4, (P b, 2a L
aθμ ) T'i Os +0.5% by weight M002 +
Piezoelectric ceramics 11 having a composition of 0.3% by weight CuO
A pair of opposing layers tM12 and tM13 are formed between them.
圧電セラミクス11の分極軸方向く矢印Pで記す。The direction of the polarization axis of the piezoelectric ceramic 11 is indicated by an arrow P.
)は、対向電極12.13の対向方向と短歯にされ−C
いる。づなわら、この実施例の圧電セラミクス素子10
は、厚みづべり1ネルギ閉じ込め振動モードを利用する
ものである。また、各対向電極12.13の上面には、
質量負荷金属材料としての鉛層14,15が形成されて
いる。) is in the opposite direction of the counter electrode 12.13 and short toothed -C
There is. In other words, the piezoelectric ceramic element 10 of this example
utilizes a thickness-thickness one-energy confined vibration mode. Moreover, on the upper surface of each counter electrode 12.13,
Lead layers 14 and 15 are formed as mass-loading metal materials.
以上のようにして製造したこの実施例の圧電セラミクス
素子10についで、減衰a゛−周波数特性を測定した。The attenuation a-frequency characteristics of the piezoelectric ceramic element 10 of this example manufactured as described above were measured.
この結果を第5図に示す1.第す図から明らかなように
、この実施例によ11ば、厚みリベリJネルギ閉じ込め
振動の基本波には、波形の分割がほとんど生じていない
。このことは、買か負荷用金属材料を只備しないチタン
酸鉛系圧電1!ラミクスについて測定した第3図と比較
づれば、明白に理解されるて゛あろう。The results are shown in Figure 5.1. As is clear from FIG. 11, in this embodiment, almost no waveform division occurs in the fundamental wave of the thickness-recovery J-energy confined vibration. This means that the lead titanate-based piezoelectric device, which does not have any metal material for the load, can be purchased! This will be clearly understood if you compare it with Figure 3, which was measured for Lamics.
¥51図は、PZT系セラミクスを用いた従来の圧電セ
ラミクス素子の一例の側面図である。第2図は、従来の
圧電セラミクス素子の他の例を示づ側面図である。第3
図(J、チタン酸鉛系セラミクスを用いた従来の圧電セ
ラミクス素子の厚みすべりエネルギ閉じ込め振動基本波
の波形を示すグラフである。第4図は、この発明の一実
施例を示づ側面図である。第5図は、第4図に示した実
施例の厚みすべりエネルギ閉じ込め振動の基本波の波形
を示すグラフである。
図において、10は圧電セラミクス素子、11は圧電セ
ラミクス、12,134よ1対の対向電擾罎、14.1
5は質量負荷用金属材flを示づ。
持n出願人 株式会社村田製伯三i91代 理 人
弁理士 深 児 久 部 1.′:1′i
]″り+4、−
(ほか2名)″−I譬L
Q−
糸 11ツ)7,2
3
第2(2) 7.Z¥51 is a side view of an example of a conventional piezoelectric ceramic element using PZT ceramics. FIG. 2 is a side view showing another example of a conventional piezoelectric ceramic element. Third
Figure (J) is a graph showing the waveform of the thickness-shear energy trapped vibration fundamental wave of a conventional piezoelectric ceramic element using lead titanate-based ceramics. Figure 4 is a side view showing an embodiment of the present invention. Fig. 5 is a graph showing the waveform of the fundamental wave of the thickness-shear energy confined vibration of the embodiment shown in Fig. 4. In the figure, 10 is a piezoelectric ceramic element, 11 is a piezoelectric ceramic element, 12, 134, etc. A pair of opposing electrical cables, 14.1
5 indicates a mass-loading metal material fl. Current applicant Murata Seihakuzo Co., Ltd. Representative Patent attorney Hisabe Fukaji 1. ′:1′i
]"ri+4,- (2 others)"-I example L Q- thread 11) 7, 2 3 2nd (2) 7. Z
Claims (1)
の圧電セラミクスを挾んで対向づる1対の対向電極とを
備え、厚みすべりエネルギ閉じ込め振動モードを利用す
る圧電セラミクス素子において、 前記1対の対向電極の少なくとも一方には、質量負荷用
金属材料が付着されている圧電セラミクス素子。[Scope of Claims] A piezoelectric ceramic element comprising a piezoelectric ceramic made of lead titanate-based ceramics and a pair of opposing electrodes sandwiching the piezoelectric ceramic, and utilizing a thickness shear energy trapping vibration mode, comprising: A piezoelectric ceramic element in which a mass-loading metal material is attached to at least one of a pair of opposing electrodes.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP57154204A JPS5943620A (en) | 1982-09-03 | 1982-09-03 | Piezoelectric ceramic element |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP57154204A JPS5943620A (en) | 1982-09-03 | 1982-09-03 | Piezoelectric ceramic element |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS5943620A true JPS5943620A (en) | 1984-03-10 |
Family
ID=15579115
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP57154204A Pending JPS5943620A (en) | 1982-09-03 | 1982-09-03 | Piezoelectric ceramic element |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5943620A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH03139909A (en) * | 1989-10-25 | 1991-06-14 | Murata Mfg Co Ltd | Piezoelectric resonator |
JPH0524405A (en) * | 1991-07-19 | 1993-02-02 | Reizu Eng:Kk | Wheel and wheel assembly for automobile |
WO1999037023A1 (en) * | 1998-01-16 | 1999-07-22 | Mitsubishi Denki Kabushiki Kaisha | Thin film pietoelectric element |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5327742B2 (en) * | 1972-11-24 | 1978-08-10 | ||
JPS54153592A (en) * | 1978-05-25 | 1979-12-03 | Nippon Denpa Kogyo Kk | Thickness slide vibrator |
-
1982
- 1982-09-03 JP JP57154204A patent/JPS5943620A/en active Pending
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5327742B2 (en) * | 1972-11-24 | 1978-08-10 | ||
JPS54153592A (en) * | 1978-05-25 | 1979-12-03 | Nippon Denpa Kogyo Kk | Thickness slide vibrator |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH03139909A (en) * | 1989-10-25 | 1991-06-14 | Murata Mfg Co Ltd | Piezoelectric resonator |
JPH0524405A (en) * | 1991-07-19 | 1993-02-02 | Reizu Eng:Kk | Wheel and wheel assembly for automobile |
WO1999037023A1 (en) * | 1998-01-16 | 1999-07-22 | Mitsubishi Denki Kabushiki Kaisha | Thin film pietoelectric element |
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