JPH0275211A - Piezoelectric resonator - Google Patents

Piezoelectric resonator

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Publication number
JPH0275211A
JPH0275211A JP22728688A JP22728688A JPH0275211A JP H0275211 A JPH0275211 A JP H0275211A JP 22728688 A JP22728688 A JP 22728688A JP 22728688 A JP22728688 A JP 22728688A JP H0275211 A JPH0275211 A JP H0275211A
Authority
JP
Japan
Prior art keywords
load member
frequency adjustment
electrodes
vibrating
vibrating electrode
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP22728688A
Other languages
Japanese (ja)
Inventor
Takashi Yamamoto
隆 山本
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.)
Murata Manufacturing Co Ltd
Original Assignee
Murata Manufacturing 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 Murata Manufacturing Co Ltd filed Critical Murata Manufacturing Co Ltd
Priority to JP22728688A priority Critical patent/JPH0275211A/en
Publication of JPH0275211A publication Critical patent/JPH0275211A/en
Pending legal-status Critical Current

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  • Piezo-Electric Or Mechanical Vibrators, Or Delay Or Filter Circuits (AREA)

Abstract

PURPOSE:To obtain a demodulation characteristic as designed by forming a frequency adjustment load member so as to surround the vibration electrode and not to reach the side ridge of the vibration electrode. CONSTITUTION:A frequency adjustment load member 16 made of a synthetic resin or a rubber is coated to a ring area D shown in hatched lines. That is, the frequency adjustment load member 16 is formed so as to surround the vibration electrode 12 and so as not to reach the outer circumferential ridge of the vibration electrode 12 with a distance from the outer circumferential ridge of the vibration electrode 12. Since no load member 16 exists just above the vibration electrode 12, a bulk wave excited between the vibration electrodes 12 and 13 is not propagated in the load member 16 and a reflected bulk wave from the load member 16 is exerted to the base 11 between the vibration electrodes 12 and 13. Thus, the demodulation characteristic as designed is obtained.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、例えばディスクリミネータとして使用される
エネルギ閉込め型の圧電共振装置に関し、特に周波数調
整用負荷部材が圧電基板上に塗布された構造を備えるも
のに関する。
[Detailed Description of the Invention] [Field of Industrial Application] The present invention relates to an energy confinement type piezoelectric resonant device used as, for example, a discriminator, and in particular, a piezoelectric resonator device in which a frequency adjustment load member is coated on a piezoelectric substrate. It relates to something with a structure.

[従来の技術] 第3図及び第4図は、従来の圧電共振装置を説明するた
めの平面図及び部分拡大断面図である。
[Prior Art] FIGS. 3 and 4 are a plan view and a partially enlarged sectional view for explaining a conventional piezoelectric resonator device.

分極処理された圧電基板1の一方主面中央領域に振動電
極2が、他方主面上には、振動電極2と圧電基板1を介
して表裏対向するように振動電極3が形成されている。
A vibrating electrode 2 is formed in the central region of one principal surface of the polarized piezoelectric substrate 1, and a vibrating electrode 3 is formed on the other principal surface so as to face each other with the vibrating electrode 2 and the piezoelectric substrate 1 interposed therebetween.

なお、振動電極2と振動電極3は同径に形成されるが、
第3図では、裏面側の振動電極3を図示するために便宜
上振動電極2より大径に表しであることを指摘しておく
Although the vibrating electrode 2 and the vibrating electrode 3 are formed to have the same diameter,
It should be pointed out that in FIG. 3, the vibrating electrode 3 on the back side is shown with a larger diameter than the vibrating electrode 2 for convenience of illustration.

振動電極2.3には、それぞれ、外部との電気的な接続
を果たすために、引出し電極4,5が接続されている。
Extracting electrodes 4 and 5 are connected to the vibrating electrodes 2.3, respectively, in order to achieve electrical connection with the outside.

この引出し電極4.5から電圧を印加することにより振
動電極2,3で挟まれた圧電基板部分が振動し、該振動
のエネルギが振動電極2.3で挟まれた基板部分に閉込
められるように構成されている。
By applying a voltage from this extraction electrode 4.5, the piezoelectric substrate portion sandwiched between the vibrating electrodes 2 and 3 vibrates, and the energy of the vibration is confined in the substrate portion sandwiched between the vibrating electrodes 2.3. It is composed of

この種の圧電共振装置の共振周波数を調整するためには
、第3図にハツチングを付して示した領域Aに、第4図
に示すように周波数調整用樹脂材6を塗布した構造が採
用されている。すなわち、振動領域上に樹脂材6を塗布
することにより、振動をダンピングし、それによって共
振周波数を調整するものである。
In order to adjust the resonant frequency of this type of piezoelectric resonator, a structure is adopted in which a frequency adjustment resin material 6 is applied to the hatched region A in FIG. 3 as shown in FIG. 4. has been done. That is, by coating the resin material 6 on the vibration region, vibrations are damped and the resonance frequency is thereby adjusted.

〔発明が解決しようとする技術的課題〕しかしながら、
上記のような周波数調整用樹脂材6を塗布した場合、第
5図に破線で囲んだ部分x、Yに示すように、アドミタ
ンス特性及び位相特性に不連続性が生じるという問題が
あった。この特性の不連続性は、以下のような原因で生
しているものと考えられる。
[Technical problem to be solved by the invention] However,
When the frequency adjustment resin material 6 as described above is applied, there is a problem that discontinuity occurs in the admittance characteristics and phase characteristics, as shown in the portions x and Y surrounded by broken lines in FIG. This discontinuity in characteristics is thought to be caused by the following reasons.

すなわち、振動電極2,3から電圧を印加して励振させ
た場合、第4図に矢印Bで示すように励振されたバルク
波が厚め方向に伝搬し、電極2あるいは3において反射
されて定在波が形成される。
That is, when a voltage is applied from the vibrating electrodes 2 and 3 to excite them, the excited bulk waves propagate in the thick direction as shown by arrow B in FIG. 4, are reflected at the electrodes 2 or 3, and become stationary. Waves are formed.

しかしながら、このバルク波の進行方向には、圧電基板
】と比べて密度が極端に異なる樹脂材6が存在する。従
って、このバルク波は、樹脂材6中にも伝搬し、矢印C
で示すように樹脂材6の外表面において反射し、該反射
波が圧電基板1内に再度伝搬する。よって、振動領域で
は、定在波に、樹脂材6側から反射してきた反射波が加
わることになる。この結果、上記のような共振装置のア
[・ミタンス特性及び位相特性のある特定の周波数位置
において不連続性が生じるものと考えられる。
However, in the direction of propagation of this bulk wave, there is a resin material 6 whose density is extremely different from that of the piezoelectric substrate. Therefore, this bulk wave also propagates into the resin material 6, and arrow C
As shown, the wave is reflected on the outer surface of the resin material 6, and the reflected wave propagates into the piezoelectric substrate 1 again. Therefore, in the vibration region, the reflected waves reflected from the resin material 6 side are added to the standing waves. As a result, it is thought that discontinuity occurs at a certain frequency position in the amitance and phase characteristics of the resonant device as described above.

従って、従来の圧電共振装置では、ある特定の周波数位
置においてアドミタンス特性や位相特性に不連続性が生
しるため、例えばディスクリミネータとして使用した場
合、復調特性に不連続性が生しるという問題が生じてい
た。
Therefore, in conventional piezoelectric resonators, discontinuities occur in the admittance characteristics and phase characteristics at a certain frequency position, so when used as a discriminator, for example, discontinuities occur in the demodulation characteristics. A problem had arisen.

よって、本発明の目的は、周波数調整用負荷部材を塗布
したことによるアドミタンス特性や位相特性の不連続性
を解消し得る構造を備えたエネルギ閉込め型の圧電共振
装置を提供することにある。
Therefore, an object of the present invention is to provide an energy confinement type piezoelectric resonator having a structure that can eliminate discontinuities in admittance characteristics and phase characteristics caused by applying a frequency adjustment load member.

〔技術的課題を解決するための手段] 本発明は、厚み縦振動モードを利用したエネルギ閉込め
型の圧電共振装置であって、圧電基板と、該圧電基板の
両主面上に圧電基板を介して表裏対向するように形成さ
れた振動電極と、少なくとも1の振動電極の周囲を取囲
むようにかつ該振動電極の端縁に至らないように塗布さ
れた周波数調整j− 用負荷部材とを備えることを特徴とするものである。
[Means for Solving Technical Problems] The present invention is an energy confinement type piezoelectric resonator device that utilizes a thickness longitudinal vibration mode, and includes a piezoelectric substrate and piezoelectric substrates on both main surfaces of the piezoelectric substrate. vibrating electrodes formed so as to face each other through the vibrating electrode, and a frequency adjustment load member coated so as to surround at least one vibrating electrode but not reaching the edge of the vibrating electrode. It is characterized by having

〔作用〕[Effect]

振動をダンピングして周波数調整を行う周波数調整用負
荷部材は、振動電極の周囲を取囲むように、かつ振動電
極の端縁に至らないように塗布されている。従って、振
動電極の直上に負荷部材が存在しないので、振動電極間
において励振されたバルク波が負荷部材中に伝搬しない
。よって、振動電極間の基板部分には、負荷部材側から
のバルク波の反射波が加わらないため、設計通りの共振
特性を実現することができる。
A frequency adjustment load member that performs frequency adjustment by damping vibrations is applied so as to surround the vibrating electrode and not to reach the edges of the vibrating electrode. Therefore, since there is no load member directly above the vibrating electrodes, the bulk wave excited between the vibrating electrodes does not propagate into the load member. Therefore, reflected waves of bulk waves from the load member side are not applied to the substrate portion between the vibrating electrodes, so that designed resonance characteristics can be achieved.

〔実施例の説明〕[Explanation of Examples]

第1図及び第2回は、本発明の一実施例を説明するだめ
の平面図及び部分切欠断面図である。
FIGS. 1 and 2 are a plan view and a partially cutaway sectional view illustrating an embodiment of the present invention.

第1図を参照して、圧電基板11の一方主面中央領域に
振動電極12が、他方主面の中央領域に振動電極12と
圧電基板11を介して表裏対向するように振動電極13
が形成されている。振動電極12,1.3は第2図に示
すように同径に形成されているが、第3図の場合と同様
に、第1図においても他方主面側の振動電極13を図示
するために、便宜上振動電極13を大径に図示しである
ことを指摘しておく。
Referring to FIG. 1, a vibrating electrode 12 is disposed in the central region of one main surface of the piezoelectric substrate 11, and a vibrating electrode 13 is disposed in the central region of the other principal surface such that the vibrating electrode 12 and the piezoelectric substrate 11 face each other.
is formed. The vibrating electrodes 12, 1.3 are formed to have the same diameter as shown in FIG. 2, but as in the case of FIG. 3, the vibrating electrode 13 on the other main surface side is shown in FIG. It should be noted that, for convenience, the vibrating electrode 13 is shown with a large diameter.

各振動電極12.13には、それぞれ、外部との電気的
な接続を果たすために引出し電極14゜15が接続され
ており、引出し電極14.15は圧電基板11の外周端
縁に至るように引出されている。
Extracting electrodes 14 and 15 are connected to each of the vibrating electrodes 12 and 13 in order to achieve electrical connection with the outside. It is being pulled out.

本実施例の特徴は、第1図にハツチングを付して示した
リング状領域りに、第2図に示すように、合成樹脂やゴ
ム等からなる周波数調整用負荷部材16が塗布されてい
ることにある。すなわち、周波数調整用負荷部材16は
、振動電極12を取囲むように、かつ振動電極12の外
周端縁に至らないように、振動電極12の外周端縁とあ
る距離を隔てて形成されている。
The feature of this embodiment is that, as shown in FIG. 2, a frequency adjustment load member 16 made of synthetic resin, rubber, etc. is applied to the ring-shaped area indicated by hatching in FIG. There is a particular thing. That is, the frequency adjustment load member 16 is formed at a certain distance from the outer peripheral edge of the vibrating electrode 12 so as to surround the vibrating electrode 12 and not to reach the outer peripheral edge of the vibrating electrode 12. .

本実施例では、振動電極12,1.3は円形に、負荷部
材16は円環状に形成されているため、第2図中に示し
た寸法a、b、c間には、b≧a及びc−b>0の関係
がある。もっとも、振動電極12.13及び負荷部材1
6の平面形状については図示のものに限らない。すなわ
ち、振動電極12.13を矩形状のものとしてもよく、
また負荷部材16についても角環状等の任意の形状にす
ることができる。さらに、負荷部材16は、振動電極を
取囲むような形状でありさえすればよく、必ずしも閉環
とする必要もなく、部分的に開いた形状であってもよい
In this embodiment, since the vibrating electrodes 12, 1.3 are circular and the load member 16 is circular, the dimensions a, b, and c shown in FIG. There is a relationship c-b>0. However, the vibrating electrodes 12, 13 and the load member 1
The planar shape of 6 is not limited to that shown in the drawings. That is, the vibrating electrodes 12, 13 may be rectangular,
Further, the load member 16 can also be formed into any shape such as a rectangular ring shape. Furthermore, the load member 16 only needs to have a shape that surrounds the vibrating electrode, and does not necessarily have to be a closed ring, but may have a partially open shape.

本実施例では、負荷部材16が振動電極12に至らない
ように形成されているので、振動電極12.13間で励
振されたバルク波が負荷部材16中にはほとんど伝搬し
ない。よって、負荷部材16側からの反射波が振動領域
に加わることがないため、アドミタンス特性や位相特性
に不連続性が生じない。
In this embodiment, since the load member 16 is formed so as not to reach the vibrating electrode 12, the bulk wave excited between the vibrating electrodes 12 and 13 hardly propagates into the load member 16. Therefore, since the reflected wave from the load member 16 side is not applied to the vibration region, no discontinuity occurs in the admittance characteristic or phase characteristic.

なお、上記実施例における周波数調整量については、第
6図に示すように、負荷部材16の塗布厚みを変化させ
ることにより、従来例と同様に共振周波数を低下させる
方向に調整することが可能である。 なお、第6図にお
ける周波数低下量比は、次式で表される数値である。
The amount of frequency adjustment in the above embodiment can be adjusted in the direction of lowering the resonant frequency by changing the coating thickness of the load member 16, as shown in FIG. 6, as in the conventional example. be. Note that the frequency reduction amount ratio in FIG. 6 is a numerical value expressed by the following formula.

周波数低下量比−(周波数低下量/調整前の共振周波数
)X100  (%) 第6図の曲線P、Q及びRは負荷部材の形状を変化させ
た場合の実施例の特性を示す。これらの曲線P−Hの特
性で示されているように、本実施例においても周波数調
整用負荷部材16の厚みを変えることにより共振周波数
を調整し得ることが解る。
Frequency reduction amount ratio - (frequency reduction amount/resonant frequency before adjustment) x 100 (%) Curves P, Q and R in FIG. 6 show the characteristics of the embodiment when the shape of the load member is changed. As shown by the characteristics of these curves PH, it can be seen that the resonance frequency can be adjusted by changing the thickness of the frequency adjustment load member 16 in this embodiment as well.

のみならず、曲線P、Q、Rで示された特性では、P−
>Q→Rとなるに従って、負荷部材16の内径b(第2
図参照)が小さくなるように、あるいは外径Cが大きく
なるように変化させた場合の各特性を示すものであるが
、これらの特性例からも明らかなように、本実施例では
負荷部材16の塗布形状を変えることにより、従来例に
比べてより細かな周波数調整を行い得ることがわかる。
In addition, in the characteristics shown by curves P, Q, and R, P-
>Q→R, the inner diameter b (second
The graph shows the characteristics when the load member 16 is changed to become smaller or the outer diameter C becomes larger (see figure).As is clear from these characteristic examples, in this example, the load member 16 It can be seen that by changing the application shape, it is possible to perform more fine frequency adjustment than in the conventional example.

上述した実施例では、一方主面に形成された振動電極1
2側にのみ周波数調整用負荷部材16を塗布したが、他
方主面側に形成された振動電極13側にも同様に負荷部
材を塗布してもよい。
In the embodiment described above, the vibrating electrode 1 formed on one main surface
Although the frequency adjustment load member 16 is applied only to the second side, the load member may be similarly applied to the vibrating electrode 13 formed on the other main surface side.

さらに、図示の実施例では両生面に1の振動電極が形成
されたものを示したが、一方主面側に分割された複数の
電極が形成されており、該電極が他方主面に形成された
共通電極と表裏対向するように形成されたエネルギ閉込
め型の3端子型の共振装置にも、本発明を適用すること
ができる。
Further, in the illustrated embodiment, one vibrating electrode is formed on the amphibatic surface, but a plurality of divided electrodes are formed on one main surface, and the electrodes are formed on the other main surface. The present invention can also be applied to an energy confinement type three-terminal type resonator device formed so as to face a common electrode on the front and back sides.

また、圧電基板11としては、圧電セラミックよりなる
ものの他、他の圧電材料より構成されたものを用いるこ
とが可能である。
Moreover, as the piezoelectric substrate 11, it is possible to use one made of other piezoelectric materials in addition to one made of piezoelectric ceramic.

〔発明の効果] 本発明では、周波数調整用負荷部材が振動電極の周囲を
取囲むように、かつ振動電極の端縁に至らないように形
成されているので、共振装置のアドミタンス特性や位相
特性に不連続性を与えることなく、共振周波数を調整す
ることが可能となる。
[Effects of the Invention] In the present invention, since the frequency adjustment load member is formed so as to surround the vibrating electrode and not reach the edge of the vibrating electrode, the admittance characteristics and phase characteristics of the resonant device are It becomes possible to adjust the resonant frequency without causing discontinuity.

従って、例えばディスクリミネークとして用いた場合、
設計通りの復調特性を実現することが可能となる。
Therefore, for example, when used as a discriminator,
It becomes possible to realize demodulation characteristics as designed.

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

第1図は本発明の一実施例の平面図、第2図は第1図実
施例の部分切欠拡大断面図、第3図は従来例の平面図、
第4図は従来例の部分切欠拡大断面図、第5図は従来例
の問題点を説明するための図でありアドミタンス特性及
び位相特性を示す図、第6図は従来例及び実施例の共振
周波数低下量比−周波数調整用負荷部材の厚みの関係を
示す図である。 図において、11は圧電基板、12.13は振動電極、
16は周波数調整用負荷部材を示す。 ヒー−+ a 第3図
FIG. 1 is a plan view of an embodiment of the present invention, FIG. 2 is a partially cutaway enlarged sectional view of the embodiment of FIG. 1, and FIG. 3 is a plan view of a conventional example.
Fig. 4 is a partially cutaway enlarged sectional view of the conventional example, Fig. 5 is a diagram for explaining the problems of the conventional example and shows the admittance characteristics and phase characteristics, and Fig. 6 is the resonance of the conventional example and the embodiment. It is a figure which shows the relationship of frequency reduction amount ratio - thickness of the load member for frequency adjustment. In the figure, 11 is a piezoelectric substrate, 12.13 is a vibrating electrode,
Reference numeral 16 indicates a frequency adjustment load member. He + a Figure 3

Claims (1)

【特許請求の範囲】  厚み縦振動を利用したエネルギ閉込め型の圧電共振装
置であって、 圧電基板と、 前記圧電基板の両主面上に圧電基板を介して表裏対向す
るように形成された複数の振動電極と、少なくとも1の
前記振動電極の周囲を取囲むように、かつ前記振動電極
の端縁に至らないように塗布された周波数調整用負荷部
材とを備えることを特徴とする圧電共振装置。
[Claims] An energy confinement type piezoelectric resonator using thickness longitudinal vibration, comprising: a piezoelectric substrate; and formed on both main surfaces of the piezoelectric substrate so as to face each other with the piezoelectric substrate interposed therebetween. Piezoelectric resonance characterized by comprising a plurality of vibrating electrodes and a frequency adjustment load member applied so as to surround at least one of the vibrating electrodes and not to reach the edges of the vibrating electrodes. Device.
JP22728688A 1988-09-09 1988-09-09 Piezoelectric resonator Pending JPH0275211A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP22728688A JPH0275211A (en) 1988-09-09 1988-09-09 Piezoelectric resonator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP22728688A JPH0275211A (en) 1988-09-09 1988-09-09 Piezoelectric resonator

Publications (1)

Publication Number Publication Date
JPH0275211A true JPH0275211A (en) 1990-03-14

Family

ID=16858433

Family Applications (1)

Application Number Title Priority Date Filing Date
JP22728688A Pending JPH0275211A (en) 1988-09-09 1988-09-09 Piezoelectric resonator

Country Status (1)

Country Link
JP (1) JPH0275211A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7012353B2 (en) * 2002-07-22 2006-03-14 Toyo Communication Equipment Co., Ltd. Piezoelectric resonator and the method for making the same
JP2007309901A (en) * 2006-05-22 2007-11-29 Mitsubishi Electric Corp Water level detection device and facility equipment
JP2008047982A (en) * 2006-08-10 2008-02-28 Daishinku Corp Piezoelectric vibration device

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* Cited by examiner, † Cited by third party
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JPS5138595A (en) * 1974-07-24 1976-03-31 Gen Electric Suchiimuaironno kanetsubankozotai
JPS6144927B2 (en) * 1979-12-06 1986-10-06 Nippon Steel Corp

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JPS6144927B2 (en) * 1979-12-06 1986-10-06 Nippon Steel Corp

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US7012353B2 (en) * 2002-07-22 2006-03-14 Toyo Communication Equipment Co., Ltd. Piezoelectric resonator and the method for making the same
JP2007309901A (en) * 2006-05-22 2007-11-29 Mitsubishi Electric Corp Water level detection device and facility equipment
JP4498312B2 (en) * 2006-05-22 2010-07-07 三菱電機株式会社 Water level detector and equipment
JP2008047982A (en) * 2006-08-10 2008-02-28 Daishinku Corp Piezoelectric vibration device
JP4687985B2 (en) * 2006-08-10 2011-05-25 株式会社大真空 Method for adjusting frequency of piezoelectric vibration device

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