JPH04306011A - Piezoelectric resonator - Google Patents
Piezoelectric resonatorInfo
- Publication number
- JPH04306011A JPH04306011A JP9818191A JP9818191A JPH04306011A JP H04306011 A JPH04306011 A JP H04306011A JP 9818191 A JP9818191 A JP 9818191A JP 9818191 A JP9818191 A JP 9818191A JP H04306011 A JPH04306011 A JP H04306011A
- Authority
- JP
- Japan
- Prior art keywords
- piezoelectric
- piezoelectric substrate
- piezoelectric resonator
- electrode
- insulating resin
- 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
- 239000000758 substrate Substances 0.000 claims abstract description 32
- 239000011347 resin Substances 0.000 claims abstract description 21
- 229920005989 resin Polymers 0.000 claims abstract description 21
- 239000000919 ceramic Substances 0.000 claims abstract description 7
- 239000007772 electrode material Substances 0.000 claims description 12
- 238000004519 manufacturing process Methods 0.000 abstract description 2
- 238000009413 insulation Methods 0.000 abstract 2
- 238000000034 method Methods 0.000 description 3
- 229910003781 PbTiO3 Inorganic materials 0.000 description 2
- 229910010293 ceramic material Inorganic materials 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 230000032683 aging Effects 0.000 description 1
- 239000011248 coating agent Substances 0.000 description 1
- 238000000576 coating method Methods 0.000 description 1
- 238000004891 communication Methods 0.000 description 1
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 230000002093 peripheral effect Effects 0.000 description 1
- 229910052709 silver Inorganic materials 0.000 description 1
- 239000004332 silver Substances 0.000 description 1
- 238000004544 sputter deposition Methods 0.000 description 1
- 238000007740 vapor deposition Methods 0.000 description 1
Landscapes
- Piezo-Electric Or Mechanical Vibrators, Or Delay Or Filter Circuits (AREA)
Abstract
Description
【0001】0001
【産業上の利用分野】この発明は、例えば圧電フィルタ
等として利用されるものであって、厚み縦振動を利用す
るエネルギー閉じ込め型の圧電共振子に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an energy trapping type piezoelectric resonator which is used as a piezoelectric filter, for example, and which utilizes longitudinal vibration in the thickness.
【0002】0002
【従来の技術】この種の圧電共振子の従来例を図5およ
び図6に示す。2. Description of the Related Art Conventional examples of this type of piezoelectric resonator are shown in FIGS. 5 and 6.
【0003】図5の圧電共振子は、周波数上昇型のもの
であり、圧電セラミックスから成る圧電基板2に凹部を
形成し、そことその反対側に振動電極4を設けた構造を
している。図6の圧電共振子は、周波数降下型のもので
あり、圧電基板2を挟んで相対向するように振動電極4
を設けている。両図中のf1 、f2 および不等記号
は、その部分の振動の周波数および大小関係を示してい
る。The piezoelectric resonator shown in FIG. 5 is of a frequency increasing type, and has a structure in which a recess is formed in a piezoelectric substrate 2 made of piezoelectric ceramics, and a vibrating electrode 4 is provided on the opposite side of the recess. The piezoelectric resonator shown in FIG. 6 is of a frequency drop type, and vibrating electrodes 4 are placed opposite each other with a piezoelectric substrate 2 in between.
has been established. In both figures, f1, f2, and inequality symbols indicate the frequency and magnitude relationship of the vibrations of the portions.
【0004】厚み縦振動を利用するものであって、温度
特性や経時変化特性の良好なPbTiO3系のようなポ
アソン比(σ)が1/3以下の圧電セラミックスから成
る圧電基板2では、図5のような周波数上昇型でしか基
本波のエネルギー閉じ込めができないことが知られてい
る(例えば田中、清水:電子通信学会論文誌J62−A
477(1979))。In the case of a piezoelectric substrate 2 that utilizes thickness longitudinal vibration and is made of a piezoelectric ceramic having a Poisson's ratio (σ) of 1/3 or less, such as PbTiO3-based material having good temperature characteristics and aging characteristics, the piezoelectric substrate 2 shown in FIG. It is known that the energy of the fundamental wave can only be confined in the frequency increasing type (for example, Tanaka, Shimizu: Journal of the Institute of Electronics and Communication Engineers J62-A).
477 (1979)).
【0005】ところが、周波数上昇型の場合は、図5に
示すように圧電基板2に凹部を形成してそこに振動電極
4を設けなければならず加工がしずらいため、図6のよ
うに圧電基板2が平板で加工しやすい周波数降下型構造
でエネルギー閉じ込めができる圧電共振子であって3倍
あるいは5倍の高次波を利用するものが多く使われてい
る。However, in the case of the frequency increasing type, as shown in FIG. 5, it is necessary to form a recess in the piezoelectric substrate 2 and install the vibrating electrode 4 there, which is difficult to process. The piezoelectric resonator is a piezoelectric resonator in which the substrate 2 is a flat plate, has a frequency-dropping structure that is easy to process, and can trap energy, and uses three or five times higher order waves.
【0006】[0006]
【発明が解決しようとする課題】ところが、図6のよう
な周波数降下型の圧電共振子は、高次波を利用するため
、■電気機械結合係数(k)が小さく、帯域幅の狭いも
のしかできない、■基本波利用よりも圧電共振子2の厚
みが厚くなり、二つの振動電極4間の静電容量が小さい
ため、浮游容量の影響を受けやすく、マッチングインピ
ーダンスも高くなり使用しにくい、■圧電基板2の厚み
が厚いため圧電セラミックス材料が多く必要になりその
ぶんコスト的に高くなる、等の欠点がある。[Problems to be Solved by the Invention] However, since the frequency-drop type piezoelectric resonator as shown in Fig. 6 uses high-order waves, it has only a small electromechanical coupling coefficient (k) and a narrow bandwidth. It is not possible, ■The thickness of the piezoelectric resonator 2 is thicker than when using the fundamental wave, and the capacitance between the two vibrating electrodes 4 is small, so it is easily affected by floating capacitance, and the matching impedance is also high, making it difficult to use.■ Since the piezoelectric substrate 2 is thick, a large amount of piezoelectric ceramic material is required, which increases the cost.
【0007】そこでこの発明は、量産加工しやすい構造
で基本波を利用することができる圧電共振子を提供する
ことを主たる目的とする。Therefore, the main object of the present invention is to provide a piezoelectric resonator that can utilize a fundamental wave and has a structure that is easy to mass-produce.
【0008】[0008]
【課題を解決するための手段】上記目的を達成するため
、この発明の圧電共振子は、圧電セラミックスから成る
圧電基板の表裏両面に、それよりも低誘電率の絶縁樹脂
を、振動電極を形成すべき部分を除いて、しかも当該部
分が圧電基板を挟んで互いに対向するように付与し、更
に少なくともこの振動電極を形成すべき部分からその周
りの絶縁樹脂上にかけて電極材を付与して成ることを特
徴とする。[Means for Solving the Problems] In order to achieve the above object, the piezoelectric resonator of the present invention includes an insulating resin having a lower dielectric constant than the piezoelectric substrate and a vibrating electrode formed on both sides of the piezoelectric substrate made of piezoelectric ceramics. The electrode material is applied at least from the part where the vibrating electrode is to be formed to the surrounding insulating resin, and the electrode material is applied so that the parts are opposite to each other with the piezoelectric substrate in between. It is characterized by
【0009】[0009]
【作用】上記構造によれば、絶縁樹脂のない振動電極を
形成すべき部分に付与された電極材が振動電極となる。
そして上下の電極材間に電圧を印加すると、絶縁樹脂が
付与された部分ではそれと圧電基板の誘電率比で印加電
圧が圧電基板に分配され、絶縁樹脂が付与されていない
振動電極部では印加電圧がそのまま圧電基板に印加され
るので、両者で圧電基板における圧電特性に差が生じる
。[Function] According to the above structure, the electrode material applied to the portion where the vibrating electrode is to be formed without the insulating resin becomes the vibrating electrode. Then, when a voltage is applied between the upper and lower electrode materials, the applied voltage is distributed to the piezoelectric substrate in the part where the insulating resin is applied according to the dielectric constant ratio of that and the piezoelectric substrate, and the applied voltage is applied to the vibrating electrode part where the insulating resin is not applied. is applied to the piezoelectric substrate as it is, so a difference occurs in the piezoelectric characteristics of the piezoelectric substrate between the two.
【0010】しかも、絶縁樹脂付与部では、それの質量
負荷効果から音速が遅く(即ち振動の周波数が低く)、
これに対して絶縁樹脂が付与されていない振動電極部で
は音速が速く(即ち振動の周波数が高く)なり、結果と
して周波数上昇型のエネルギー閉じ込めができ、基本波
の閉じ込めができる。Moreover, in the insulating resin application section, the sound velocity is slow (that is, the vibration frequency is low) due to its mass load effect.
On the other hand, in the vibrating electrode portion to which no insulating resin is applied, the speed of sound becomes faster (that is, the frequency of vibration becomes higher), and as a result, energy confinement of the frequency increasing type is achieved, and the fundamental wave can be confined.
【0011】[0011]
【実施例】図1は、この発明の一実施例に係る圧電共振
子を示す断面図であり、図2は図1の圧電共振子を電極
材を除いて示す平面図である。DESCRIPTION OF THE PREFERRED EMBODIMENTS FIG. 1 is a sectional view showing a piezoelectric resonator according to an embodiment of the present invention, and FIG. 2 is a plan view showing the piezoelectric resonator of FIG. 1 with electrode materials removed.
【0012】この圧電共振子は、例えばPbTiO3系
の圧電セラミックスから成る圧電基板2の表裏両面に、
それよりも低誘電率の(例えば圧電基板2の1/2以下
の)絶縁樹脂6を以下に述べる部分を除いて塗布等によ
って付与し、更にその上からこの実施例ではほぼ全面に
、銀等から成る電極材8を蒸着、スパッタ等によって付
着させて成る。[0012] This piezoelectric resonator has a piezoelectric substrate 2 made of, for example, PbTiO3-based piezoelectric ceramics.
An insulating resin 6 having a lower dielectric constant (for example, 1/2 or less than that of the piezoelectric substrate 2) is applied by coating, etc., except for the parts described below, and then, in this embodiment, almost the entire surface is coated with silver, etc. The electrode material 8 is deposited by vapor deposition, sputtering, or the like.
【0013】絶縁樹脂6は、圧電基板2の表裏両面に、
この実施例では図2に示すように、中央部の振動電極を
形成すべき部分6a、端部の外部接続電極を形成すべき
部分6bおよび両者をつなぐ部分6cを除いて付与され
ている。しかも上下の振動電極を形成すべき部分6aは
、図1に示すように、圧電基板2を挟んで互いに対向す
るようにされている。The insulating resin 6 is placed on both the front and back surfaces of the piezoelectric substrate 2.
In this embodiment, as shown in FIG. 2, a portion 6a at the center where the vibrating electrode is to be formed, a portion 6b at the end where the external connection electrode is to be formed, and a portion 6c connecting the two are provided. Furthermore, the portions 6a where the upper and lower vibrating electrodes are to be formed are arranged to face each other with the piezoelectric substrate 2 in between, as shown in FIG.
【0014】上記構造によれば、電極材8の内で、絶縁
樹脂6の付与されていない部分6aおよび6bに付着さ
れた部分が、それぞれ、振動電極および外部接続電極に
なる。According to the above structure, the portions of the electrode material 8 attached to the portions 6a and 6b to which the insulating resin 6 is not applied become the vibrating electrode and the external connection electrode, respectively.
【0015】このような圧電共振子においては、上下の
電極材8間に電圧を印加すると、絶縁樹脂6が付与され
た部分ではそれと圧電基板2の誘電率比で印加電圧が圧
電基板2に分配され、絶縁樹脂6が付与されていない振
動電極部では印加電圧がそのまま圧電基板2に印加され
るので、両者で圧電基板2における圧電特性に差が生じ
る。In such a piezoelectric resonator, when a voltage is applied between the upper and lower electrode materials 8, the applied voltage is distributed to the piezoelectric substrate 2 at the portion where the insulating resin 6 is applied, depending on the dielectric constant ratio of that and the piezoelectric substrate 2. In the vibrating electrode portion to which the insulating resin 6 is not applied, the applied voltage is directly applied to the piezoelectric substrate 2, so a difference occurs in the piezoelectric characteristics of the piezoelectric substrate 2 between the two.
【0016】しかも、絶縁樹脂6の塗布部では、それの
質量負荷効果から音速が遅く(即ち振動の周波数が低く
)、これに対して絶縁樹脂6が塗布されていない振動電
極部では音速が速く(即ち振動の周波数が高く)なり、
即ち前者の周波数をf2 、後者の周波数をf1 とす
るとf1 >f2 になり、結果として周波数上昇型の
エネルギー閉じ込めができ、基本波の閉じ込めができる
。Furthermore, in the part where the insulating resin 6 is coated, the sound velocity is slow (that is, the vibration frequency is low) due to its mass load effect, whereas in the vibrating electrode part where the insulating resin 6 is not coated, the sound velocity is fast. (i.e. the frequency of vibration becomes higher),
That is, when the former frequency is f2 and the latter frequency is f1, f1 > f2, and as a result, frequency-increasing energy confinement is achieved, and the fundamental wave is confined.
【0017】これをインピーダンス波形で説明すると、
従来の図6の構造の圧電共振子では、図4に示すように
基本波の共振応答は小さく、基本波のエネルギー閉じ込
めが不充分であったのが、上記実施例の圧電共振子では
、図3に示すように基本波の共振応答は大きくシャープ
な波形が得られており、十分なエネルギー閉じ込めが実
現されていることが分かる。[0017] To explain this using an impedance waveform,
In the conventional piezoelectric resonator having the structure shown in FIG. 6, the resonance response of the fundamental wave was small and the energy confinement of the fundamental wave was insufficient, as shown in FIG. As shown in Figure 3, the resonance response of the fundamental wave has a large and sharp waveform, indicating that sufficient energy confinement has been achieved.
【0018】なお、圧電基板2の周縁部は、振動に直接
影響しないので、その辺りにまで絶縁樹脂6や電極材8
を付与するかとか、外部接続電極部分をどのようにする
か等については基本的でなく任意である。Note that the peripheral edge of the piezoelectric substrate 2 does not directly affect vibration, so the insulating resin 6 and electrode material 8 are also applied to that area.
It is not fundamental and is arbitrary as to how to provide externally connected electrode portions, etc.
【0019】また、上記圧電基板2には、Pb(Zr,
Ti)O3系でポアソン比が1/3以下の圧電セラミッ
クスを用いても良い。Further, the piezoelectric substrate 2 is made of Pb (Zr,
Ti)O3-based piezoelectric ceramics having a Poisson's ratio of 1/3 or less may be used.
【0020】[0020]
【発明の効果】以上のようにこの発明の圧電共振子によ
れば、周波数上昇型で基本波のエネルギー閉じ込めがで
きるので、基本波を利用することができる。しかも、従
来の周波数上昇型の圧電共振子のように圧電基板に凹部
を形成する場合に比べて、絶縁樹脂を付与する方が加工
が簡単なので、量産加工もしやすい。As described above, according to the piezoelectric resonator of the present invention, the energy of the fundamental wave can be confined by increasing the frequency, so that the fundamental wave can be used. Moreover, since it is easier to process by applying an insulating resin than forming a recess in a piezoelectric substrate as in a conventional frequency increasing type piezoelectric resonator, it is easier to mass-produce the resonator.
【0021】また、基本波を利用できるため圧電基板が
薄くて済み、当該圧電共振子の小型化および圧電セラミ
ックス材料の削減によるコストダウンを図ることができ
る。またそれによって、低周波の圧電共振子の製作も容
易になる。Furthermore, since the fundamental wave can be used, the piezoelectric substrate can be made thinner, and costs can be reduced by downsizing the piezoelectric resonator and reducing the amount of piezoelectric ceramic material. It also facilitates the production of low frequency piezoelectric resonators.
【図1】 この発明の一実施例に係る圧電共振子を示
す断面図である。FIG. 1 is a sectional view showing a piezoelectric resonator according to an embodiment of the present invention.
【図2】 図1の圧電共振子を電極材を除いて示す平
面図である。FIG. 2 is a plan view showing the piezoelectric resonator of FIG. 1 with electrode materials removed.
【図3】 図1の圧電共振子のインピーダンス波形の
一例を示す図である。3 is a diagram showing an example of an impedance waveform of the piezoelectric resonator of FIG. 1. FIG.
【図4】 図6の圧電共振子のインピーダンス波形の
一例を示す図である。4 is a diagram showing an example of an impedance waveform of the piezoelectric resonator of FIG. 6. FIG.
【図5】 従来の周波数上昇型の圧電共振子の一例を
示す断面図である。FIG. 5 is a cross-sectional view showing an example of a conventional frequency increasing type piezoelectric resonator.
【図6】 従来の周波数降下型の圧電共振子の一例を
示す断面図である。FIG. 6 is a cross-sectional view showing an example of a conventional frequency drop type piezoelectric resonator.
2 圧電基板 6 絶縁樹脂 6a 振動電極を形成すべき部分 8 電極材 2 Piezoelectric substrate 6 Insulating resin 6a Part where the vibrating electrode should be formed 8 Electrode material
Claims (1)
表裏両面に、それよりも低誘電率の絶縁樹脂を、振動電
極を形成すべき部分を除いて、しかも当該部分が圧電基
板を挟んで互いに対向するように付与し、更に少なくと
もこの振動電極を形成すべき部分からその周りの絶縁樹
脂上にかけて電極材を付与して成ることを特徴とする圧
電共振子。[Claim 1] An insulating resin having a lower dielectric constant is applied to both the front and back surfaces of a piezoelectric substrate made of piezoelectric ceramics, except for the part where the vibrating electrode is to be formed, and furthermore, the said parts are opposite to each other with the piezoelectric substrate in between. A piezoelectric resonator characterized in that an electrode material is further applied from at least a portion where the vibrating electrode is to be formed to an insulating resin around the portion.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP9818191A JPH04306011A (en) | 1991-04-02 | 1991-04-02 | Piezoelectric resonator |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP9818191A JPH04306011A (en) | 1991-04-02 | 1991-04-02 | Piezoelectric resonator |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH04306011A true JPH04306011A (en) | 1992-10-28 |
Family
ID=14212856
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP9818191A Pending JPH04306011A (en) | 1991-04-02 | 1991-04-02 | Piezoelectric resonator |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH04306011A (en) |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5516382A (en) * | 1978-07-21 | 1980-02-05 | Omron Tateisi Electronics Co | Method of manufacturing terminal base |
JPS6164179A (en) * | 1984-09-05 | 1986-04-02 | Murata Mfg Co Ltd | Piezoelectric device |
JPH02235422A (en) * | 1989-03-08 | 1990-09-18 | Matsushita Electric Ind Co Ltd | Thickness longitudinal resonator |
-
1991
- 1991-04-02 JP JP9818191A patent/JPH04306011A/en active Pending
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5516382A (en) * | 1978-07-21 | 1980-02-05 | Omron Tateisi Electronics Co | Method of manufacturing terminal base |
JPS6164179A (en) * | 1984-09-05 | 1986-04-02 | Murata Mfg Co Ltd | Piezoelectric device |
JPH02235422A (en) * | 1989-03-08 | 1990-09-18 | Matsushita Electric Ind Co Ltd | Thickness longitudinal resonator |
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