JPH0456508A - Piezoelectric vibrator and its frequency adjustment method - Google Patents
Piezoelectric vibrator and its frequency adjustment methodInfo
- Publication number
- JPH0456508A JPH0456508A JP2167706A JP16770690A JPH0456508A JP H0456508 A JPH0456508 A JP H0456508A JP 2167706 A JP2167706 A JP 2167706A JP 16770690 A JP16770690 A JP 16770690A JP H0456508 A JPH0456508 A JP H0456508A
- Authority
- JP
- Japan
- Prior art keywords
- frequency
- airtight container
- frequency adjustment
- diaphragm
- 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
Links
Landscapes
- Piezo-Electric Or Mechanical Vibrators, Or Delay Or Filter Circuits (AREA)
Abstract
Description
【発明の詳細な説明】
産業上の利用分野
本発明は、種々の電子機器の基準信号の発生源等に用い
られる圧電振動子およびその周波数調整方法に関するも
のである。DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a piezoelectric vibrator used as a reference signal generation source for various electronic devices, and a method for adjusting its frequency.
従来の技術
水晶等を用いた圧電振動子には、その使用目的などによ
り種々の振動モードが存在するが、現在では一般的に厚
みすべりモードが利用されている。BACKGROUND OF THE INVENTION Piezoelectric vibrators using crystals or the like have various vibration modes depending on the purpose of use, but the thickness shear mode is generally used at present.
この厚みすべりモードでは、圧電振動子の共振周波数は
振動板の厚みに反比例して変化する。また、電極の質量
付加効果によシ共振周波数が低下することが知られてお
り、この質量付加効果を利用して共振周波数を調整して
いる。In this thickness shear mode, the resonant frequency of the piezoelectric vibrator changes in inverse proportion to the thickness of the diaphragm. Furthermore, it is known that the resonance frequency decreases due to the mass addition effect of the electrode, and this mass addition effect is used to adjust the resonance frequency.
以下、従来の圧電振動子およびその周波数調整方法につ
いて説明する。A conventional piezoelectric vibrator and its frequency adjustment method will be described below.
第7図は従来の圧電振動子の中で一般的に使用されてい
る水晶振動子の内部構造図を示しており、第8図は水晶
振動子の周波数調整方法を示した概略図である。FIG. 7 shows an internal structure diagram of a crystal resonator commonly used in conventional piezoelectric resonators, and FIG. 8 is a schematic diagram showing a method for adjusting the frequency of the crystal resonator.
第7図において、両面を精密に研磨(ときにはポリッシ
ュ)して周波数を調整した水晶板13の両面上に銀、ア
ルミニウム等の金属を数千への厚さに蒸着して電極16
を形成し、それをサポータ−18で保持器のベース14
に取り付けている。このサポータ−18は、図では板状
のものであるが、種V条件によって線状のものもある。In FIG. 7, electrodes 16 are formed by depositing metals such as silver or aluminum to a thickness of several thousand on both sides of a crystal plate 13 whose frequency has been adjusted by precisely polishing both sides (sometimes polishing).
and attach it to the base 14 of the retainer with the supporter 18.
It is attached to. Although this supporter 18 is plate-shaped in the figure, it may also be linear depending on the type V conditions.
また、このサポータ−18は、水晶板13の支持と共に
電気的な導線の働きを兼ねるもので、板状、線状いずれ
の場合も、水晶板13との接点は水晶板13の脱落を防
ぐため、導電性接着剤19で固定しである。In addition, this supporter 18 not only supports the crystal plate 13 but also functions as an electrical conductor.Whether in the form of a plate or a wire, the contact point with the crystal plate 13 is to prevent the crystal plate 13 from falling off. , and fixed with a conductive adhesive 19.
ベース14は、入・出力端子16が貫通され、さらに外
周に金属カバー20が接合されて密封されている。さら
に、水晶板13の電極16上には、周波数の最終調整を
行うだめの周波数調整体17が水晶板13の電極16よ
シ少し小さめの形状で一様に付加されている。The input/output terminals 16 pass through the base 14, and a metal cover 20 is bonded to the outer periphery of the base 14 for sealing. Furthermore, a frequency adjusting body 17 for final frequency adjustment is uniformly attached on the electrode 16 of the crystal plate 13 in a slightly smaller shape than the electrode 16 of the crystal plate 13.
第8図において、気密封止前の水晶振動子の周波数調整
方法を示している。すなわち、真空チャンバー22内に
、第7図から金属カバー20を被せる前のものをセント
する。そして前記真空チャンバー22内を高真空雰囲気
にした後、蒸発源24を電気的に加熱させ、加熱により
溶けた周波数調整用の銀、又はアルミニウム等の金属2
3を蒸発させ、マスク21を介して水晶板13の電極1
6上に千の電極16よシ少し小さめの形状で一様に°蒸
着する。同時にこの銀の蒸着中の水晶振動子の発振周波
数をカウンター28で読みながら、発振周波数がある設
定値まで下がった時点でコンパレータ2了によりシャッ
ター26を閉じ、蒸着を止めることで発振周波数を調整
していた。FIG. 8 shows a method of adjusting the frequency of the crystal resonator before hermetically sealing it. That is, in the vacuum chamber 22, the one shown in FIG. 7 before being covered with the metal cover 20 is placed. After creating a high vacuum atmosphere in the vacuum chamber 22, the evaporation source 24 is electrically heated, and the metal 2, such as silver or aluminum, for frequency adjustment is melted by heating.
3 is evaporated, and the electrode 1 of the crystal plate 13 is exposed through the mask 21.
6, uniformly evaporate a thousand electrodes 16 in a slightly smaller shape. At the same time, while reading the oscillation frequency of the crystal oscillator during silver deposition using the counter 28, when the oscillation frequency drops to a certain set value, the shutter 26 is closed by the comparator 2, stopping the evaporation and adjusting the oscillation frequency. was.
発明が解決しようとする課題
しかしながら、上記従来の一般的な真空蒸着法による周
波数調整方法では、1O−storr以上の高真空が要
求され、真空チャンバー22等を含む真空設備に高額の
費用が発生するほか、周波数の調整をするにも真空引き
などの余分な時間がかかシ生産性を悪くしていた。また
、周波数調整は気密封止前に行わねばならず、抵抗溶接
、コールドウェルド等の気密封止により水晶振動子の共
振周波数が変化する為、結果的に完成品での共振周波を
高精度に調整することは非常に難しいものとなっていた
。さらに、高い周波数帯になるにつれ、水晶振動子も小
型化され、水晶板13の電極16も小さくなるため、従
来の様な真空蒸着法では、周波数調整体17が水晶板1
3の電極16外へ一部がはみ出すものも発生するなど周
波数の調整もきわめて困難となるばかりでなく、等価抵
抗を増大させる等の信頼性にも影響を及ぼしていた。Problems to be Solved by the Invention However, in the conventional frequency adjustment method using the general vacuum evaporation method, a high vacuum of 1 O-storr or more is required, and a high cost is incurred for vacuum equipment including the vacuum chamber 22 etc. In addition, adjusting the frequency required extra time for vacuuming, etc., which worsened productivity. In addition, frequency adjustment must be performed before hermetic sealing, and as the resonant frequency of the crystal oscillator changes due to hermetic sealing such as resistance welding or cold welding, the resonant frequency of the finished product can be adjusted with high precision. It was extremely difficult to adjust. Furthermore, as the frequency band becomes higher, the crystal resonator becomes smaller and the electrode 16 of the crystal plate 13 also becomes smaller.
Not only is it extremely difficult to adjust the frequency, as a portion of the electrode 16 sometimes protrudes outside the electrode 16 of No. 3, but the reliability is also affected, such as by increasing the equivalent resistance.
そこで本発明は共振周波数調整が高精度に、しかも生産
性良く行えるものを提供することを目的とするものであ
る。SUMMARY OF THE INVENTION Therefore, an object of the present invention is to provide a device that allows resonance frequency adjustment to be performed with high precision and with good productivity.
課題を解決するだめの手段
そして上記目的を達成すべく本発明は、少なくともその
一部分が透光性となった気密容器と、この気密容器内に
設けた振動板と、この振動板の表面と裏面とにそれぞれ
設けた電極と、前記気密容器の外部からその内部に導入
されて前記表面と裏面の電極に接続された電気的導通手
段と、前記気密容器の透光部に対応するこの気密容器内
部分に設けた周波数調整物とを備え、前記周波数調整物
に対応する前記電極部分上には、前記周波数調整物から
飛散された周波数調整体を設け、この周波数調整体は、
連続的または不連続的な直線部が複数本平行状態で配置
された形状としたものである。Means for Solving the Problems and In order to achieve the above object, the present invention provides an airtight container, at least a portion of which is translucent, a diaphragm provided in the airtight container, and a front and back surface of the diaphragm. an electrically conductive means introduced into the inside of the airtight container from the outside and connected to the electrodes on the front and back surfaces; a frequency adjustment object provided on a portion, a frequency adjustment object scattered from the frequency adjustment object is provided on the electrode portion corresponding to the frequency adjustment object, and this frequency adjustment object:
It has a shape in which a plurality of continuous or discontinuous straight portions are arranged in parallel.
その製造方法としては、前記気密容器の外部から前記透
光部を介してこの気密容器内面側に設けた周波数調整物
にレーザ光を照射し、この照射により前記周波数調整物
を飛散させ、この飛散した周波数調整物を前記振動板の
電極上に、上記配置形状で付着させることにより、この
振動板の周波数の調整を行うものである。The manufacturing method includes irradiating a laser beam from the outside of the airtight container through the light-transmitting part to the frequency adjustment object provided on the inner surface of the airtight container, scattering the frequency adjustment object by this irradiation, and scattering the frequency adjustment object. The frequency of the diaphragm is adjusted by attaching the frequency adjustment material on the electrodes of the diaphragm in the arrangement shape described above.
作用
本発明は、上記構成により、振動片を気密容器に気密封
止した完成品のものを用いるのが大気中で周波数調整が
可能となり、真空容器等の真空設備が不要となり簡単な
設備構成で短時間で連続的に周波数調整ができるように
なるため、生産能率もかなり向上できる。まだ、−個ず
つ気密封止後に周波数を調整するだめ後工程での周波数
ばらつきを考える必要がなく、完成品での周波数偏差を
小さくできる。Effects of the present invention With the above configuration, it is possible to adjust the frequency in the atmosphere by using a finished product in which the vibrating piece is hermetically sealed in an airtight container, and vacuum equipment such as a vacuum container is not required, resulting in a simple equipment configuration. Since the frequency can be adjusted continuously in a short period of time, production efficiency can be significantly improved. However, there is no need to consider frequency variations in post-processing since the frequency is adjusted after hermetically sealing each unit, and the frequency deviation in the finished product can be reduced.
実施例
第1図は本発明の一実施例を示す一部切欠斜視図である
。表裏面に電極子を配した長方形の水晶振動子6は、導
電性接着剤6により電気的導通手段の一例として用いた
リード端子3の保持部4に支持されると共に電気的に導
通されている。透明なガラスカバー1の内面側には周波
数調整物の一例として金属コート膜9が真空蒸着法によ
り施されている。なお、このガラスカバー1の内面側は
サンドブラストや研磨等で粗面化加工され、この粗面化
部分上に前記金属コート膜9が設けられている。さらに
、本実施例では金属コート膜9の材質は、水晶振動子6
に形成された電極7と同じ銀を用いている。そして、前
記水晶振動子6はケース2および前記ガラスカバー1に
よシ封着剤8を用いて気密封止されている。つまり、ガ
ラスカバー1とケース2で気密容器が形成されているの
である。Embodiment FIG. 1 is a partially cutaway perspective view showing an embodiment of the present invention. A rectangular crystal resonator 6 with electrodes arranged on its front and back surfaces is supported and electrically connected to the holding part 4 of the lead terminal 3, which is used as an example of an electrically conductive means, by means of a conductive adhesive 6. . A metal coating film 9 as an example of a frequency adjustment material is applied to the inner surface of the transparent glass cover 1 by vacuum deposition. The inner surface of the glass cover 1 is roughened by sandblasting, polishing, etc., and the metal coating film 9 is provided on this roughened portion. Furthermore, in this embodiment, the material of the metal coating film 9 is the material of the crystal resonator 6.
The same silver as the electrode 7 formed in is used. The crystal resonator 6 is hermetically sealed to the case 2 and the glass cover 1 using a sealant 8. In other words, the glass cover 1 and the case 2 form an airtight container.
第2図は、本発明の周波数調整方法の一実施例を示して
おり、真空封止後にレーザ光により周波数調整する概念
図である。周波数調整は、ガラスカバー1をケース2に
封着剤8で接着させた気密封止後に実施される。図示し
ていないが、リード端子3は、発振器に接続されており
発振周波数はカウンターで確認できる。ここで外部から
ガラスカバー1を通して連続発振光をQスイッチでパル
ス化した!五Gレーザ光12を金属コート膜9付近に焦
光レンズ11で焦点をあわせる。そして、2つのガルバ
ノメータを用いてレーザ光12をスキャニングさせるガ
ルバノメータ方式によりレーザ光12を前記金属コート
膜9上を左右方向に移動させながら照射する。ここでレ
ーザ光12を移動させるのに前記ガルバノメータ形を用
いだが、2枚のミラーヌはプリズムをXYテーブルに固
定したXYテーブル方式さらに光ファイバーの出射光学
部をロボットで自在に移動させるファイバー方式も可能
である。XAGレーザ光12はガラヌカパー1を透過し
、前記金属コート膜9だけを選択して瞬間的に飛散させ
ることができる。飛散した金属は第3図に示す様に水晶
振動子6に配した電極7上に直線部が複数本平行状態で
配置された連続的な蛇行状に周波数調整体10として付
着され、質量付加効果により水晶振動子6の発振周波数
は下がる。さらにYAGレーザ光12を掃引して所定の
設定周波数に達するまで繰り返される。FIG. 2 shows an embodiment of the frequency adjustment method of the present invention, and is a conceptual diagram of frequency adjustment using a laser beam after vacuum sealing. Frequency adjustment is performed after the glass cover 1 is hermetically sealed to the case 2 by adhering it to the case 2 with an adhesive 8. Although not shown, the lead terminal 3 is connected to an oscillator, and the oscillation frequency can be checked with a counter. Here, continuous wave light was pulsed from the outside through the glass cover 1 using a Q switch! The 5G laser beam 12 is focused near the metal coating film 9 by a focusing lens 11. Then, the laser beam 12 is irradiated onto the metal coat film 9 while moving in the left-right direction using a galvanometer method in which the laser beam 12 is scanned using two galvanometers. Here, the galvanometer type described above is used to move the laser beam 12, but the two Miranes can also be used with an XY table method in which the prism is fixed to an XY table, or a fiber method in which the output optical part of the optical fiber is moved freely by a robot. be. The XAG laser beam 12 can be transmitted through the Galanuka permeate 1, and only the metal coated film 9 can be selected and instantaneously scattered. As shown in FIG. 3, the scattered metal is deposited on the electrode 7 disposed on the crystal oscillator 6 as a frequency adjustment body 10 in a continuous meandering shape with a plurality of straight sections arranged in parallel, resulting in a mass addition effect. As a result, the oscillation frequency of the crystal resonator 6 decreases. Furthermore, the YAG laser beam 12 is swept and repeated until a predetermined set frequency is reached.
本実施例ではレーザ光12にYAGレーザ光を使用した
が、ガラスカバー1を透過できるものであれば何でも使
用できる。また電極7及び金属コート膜9には銀を用い
真空蒸着法で施したが電極7の上で安定であればよく、
また印刷などの方法によシ施すことも可能である。In this embodiment, a YAG laser beam is used as the laser beam 12, but any laser beam that can be transmitted through the glass cover 1 can be used. Further, although silver was used for the electrode 7 and the metal coating film 9 and was applied by vacuum evaporation, it is sufficient that it is stable on the electrode 7.
It is also possible to apply by a method such as printing.
なお、本実施例において、ガラスカバー1の内面を粗面
化したのは次のような理由からである。In this example, the inner surface of the glass cover 1 was roughened for the following reasons.
つまり、レーザ光12を照射された金属コート膜9部分
は直ちに飛散するのでここに照射された残りのレーザ光
12のエネルギーは今後は電極7を侵すことになる。よ
ってこのような残りのエネルギーによる弊害を防止すべ
く上述の粗面化を行ったものであり、粗面化しておけば
残りのエネルギーは粗面化部で分散された後に電極7の
方へ向かうことになり、局部的に電極7を侵すことのな
いものとなる。In other words, since the portion of the metal coat film 9 irradiated with the laser beam 12 immediately scatters, the energy of the remaining laser beam 12 irradiated thereon will attack the electrode 7 in the future. Therefore, the above-mentioned surface roughening was performed in order to prevent the adverse effects caused by such residual energy.If the surface is roughened, the remaining energy will be dispersed in the roughened portion and then directed toward the electrode 7. Therefore, the electrode 7 will not be locally attacked.
上記の周波数調整方法によれば、気密容器と水晶振動子
6よシなる圧電振動子自体を大気雰囲気中に置くことが
できるため従来の真空容器のような高真空設備が不要に
なシ簡単な構成の設備で周波数調整が可能となる。また
周波数調整の速度も従来のものと比較して速くすること
ができ、連続的、効率的に周波数調整ができるようにな
る。つぎに従来の工程では周波数調整後に水晶振動子6
をケース内に収納し、抵抗溶接またはコールドウェルド
等の気密封止を行うが、気密封止後に周波数が変化して
しまうという課題があったが、本実施例による水晶振動
子6の周波数調整は気密封止後に行うので完成品の周波
数偏差を小さくできた。According to the frequency adjustment method described above, since the airtight container and the piezoelectric vibrator itself such as the crystal resonator 6 can be placed in the atmosphere, high vacuum equipment such as a conventional vacuum container is not required. Frequency adjustment becomes possible with the configuration equipment. Furthermore, the frequency adjustment speed can be increased compared to the conventional method, and frequency adjustment can be performed continuously and efficiently. Next, in the conventional process, after frequency adjustment, the crystal oscillator 6
is housed in a case and hermetically sealed by resistance welding or cold welding, but there was a problem that the frequency changed after hermetically sealing, but the frequency adjustment of the crystal oscillator 6 according to this embodiment Since this was done after hermetic sealing, the frequency deviation of the finished product could be reduced.
さらにレーザ光12を用いた従来例のように電極7を直
接剤シとることがないため水晶振動子6の等価抵抗は殆
ど劣化することがなかった。なお第2図において焦光レ
ンズ11を透過後のレーザ光12の焦点はガラスカバー
1に入射する手前に設けてもレーザ光で金属コート膜9
は飛散させることができる。またこのようにした場合レ
ーザ光12のエネルギーが強すぎてガラスカバー1が破
損スることもなくなる。Further, since the electrode 7 is not directly removed unlike the conventional example using the laser beam 12, the equivalent resistance of the crystal resonator 6 hardly deteriorates. In addition, in FIG. 2, even if the focal point of the laser beam 12 after passing through the focusing lens 11 is placed before it enters the glass cover 1, the laser beam will still cause the metal coating film 9.
can be dispersed. In addition, in this case, the glass cover 1 will not be damaged due to the energy of the laser beam 12 being too strong.
第4図〜第6図は電極9上に設けられた周波数調整体1
oの他の実施例を示すもので、第4図。4 to 6 show the frequency adjustment body 1 provided on the electrode 9.
Fig. 4 shows another embodiment of o.
第5図のものは、連続的、または不連続的な直線を複数
本平行状態で配置したものである。また第6図に示すも
のは第3図に代え、不連続的な蛇行状の周波数調整体1
0を設けたものである。In FIG. 5, a plurality of continuous or discontinuous straight lines are arranged in parallel. In addition, the one shown in FIG. 6 is a discontinuous meandering frequency adjustment body 1 instead of the one shown in FIG. 3.
0 is set.
発明の効果
上記の説明で明らかなように本発明の圧電振動子とその
周波数調整方法によれば、大気中で連続的、効率的に圧
電振動子の周波数調整ができるという効果がある。まだ
気密容器内に振動片を気密封止した後周波数調整ができ
るため完成品の周波数偏差を小さくできるという効果が
得られる。Effects of the Invention As is clear from the above description, the piezoelectric vibrator and its frequency adjustment method of the present invention have the advantage that the frequency of the piezoelectric vibrator can be continuously and efficiently adjusted in the atmosphere. However, since the frequency can be adjusted after the vibrating piece is hermetically sealed in the airtight container, it is possible to reduce the frequency deviation of the finished product.
第1図は本発明の圧電振動子の一実施例を示す一部切欠
斜視図、第2図は本発明の圧電振動子の周波数調整方法
の一実施例を示す断面図、第3図6図は周波数調整体の
他の実施例の斜視図、第7図は、1従来の圧電振動子の
構造を示す半断面正面図、第8図は従来の真空蒸着法に
よる周波数調整方法を示す構成図である。
1・・・・・・ガラヌカバー、2・・・・・・ケース、
3・・・・・・リード端子、4・・・・・・保持部、6
・・・・・・導電性接着剤、6・・・・・・水晶振動子
、7・・・・・・電極、8・・・・・・封着剤、9・・
・・・・金属コート膜、1o・・・・・・周波数調整体
、11・・・・・・焦点レンズ、12・・・・・・レー
ザ光。FIG. 1 is a partially cutaway perspective view showing an embodiment of the piezoelectric vibrator of the present invention, FIG. 2 is a cross-sectional view showing an embodiment of the frequency adjustment method for a piezoelectric vibrator of the present invention, FIG. 3, and FIG. 1 is a perspective view of another embodiment of the frequency adjustment body, FIG. 7 is a half-sectional front view showing the structure of a conventional piezoelectric vibrator, and FIG. 8 is a configuration diagram showing a conventional frequency adjustment method using a vacuum evaporation method. It is. 1... Galanu cover, 2... Case,
3... Lead terminal, 4... Holding part, 6
... Conductive adhesive, 6 ... Crystal resonator, 7 ... Electrode, 8 ... Sealing agent, 9 ...
...Metal coat film, 1o...Frequency adjustment body, 11...Focal lens, 12...Laser light.
Claims (6)
と、この気密容器内に設けた振動板と、この振動板の表
面と裏面とにそれぞれ設けた電極と、前記気密容器の外
部から、その内部に導入されて前記表面と裏面の電極に
接続された電気的導通手段と、前記気密容器の透光部に
対応するこの気密容器内部分に設けた周波数調整物とを
備え、前記周波数調整物に対応する前記電極部分上には
、前記周波数調整物から飛散された周波数調整体を設け
、この周波数調整体は、連続的、または不連続的な直線
部が複数本平行状態で配置された形状とした周波数調整
体を設けた圧電振動子。(1) An airtight container, at least a portion of which is translucent, a diaphragm provided within the airtight container, electrodes provided on the front and back surfaces of the diaphragm, and an airtight container from the outside of the airtight container. an electrically conductive means introduced into the interior thereof and connected to the electrodes on the front and back surfaces; and a frequency adjustment member provided in a portion inside the airtight container corresponding to a light-transmitting portion of the airtight container; A frequency adjustment body scattered from the frequency adjustment object is provided on the electrode portion corresponding to the object, and this frequency adjustment body has a plurality of continuous or discontinuous straight portions arranged in parallel. A piezoelectric vibrator with a shaped frequency adjustment body.
物は、気密容器の透光部内面側に設けた金属コート膜に
より形成した圧電振動子。(2) In claim (1), the frequency adjustment object is a piezoelectric vibrator formed of a metal coated film provided on the inner surface of the light-transmitting part of the airtight container.
数調整物は同一金属材料で形成した圧電振動子。(3) A piezoelectric vibrator according to claim (2), in which the electrode and the frequency adjuster are made of the same metal material.
と、この気密容器内に設けた振動板と、この振動板の表
面と裏面とにそれぞれ設けた電極と、前記気密容器の外
部から、その内部に導入されて前記表面と裏面の電振に
接続された電気的導通手段と、前記気密容器の透光部に
対応するこの気密容器内部分に設けた周波数調整物とを
備え、前記気密容器の透光部において、前記気密容器の
外部から、前記透光部を介してこの気密容器内に設けた
周波数調整物にレーザー光を照射し、この照射により前
記周波数調整物を飛散をさせ、この飛散した周波数調整
物を前記振動板の電極上に、連続的、または不連続的な
直線部が複数本平行状態で配置された形状に付着させる
ことにより、この振動板の周波数を調整する圧電振動子
の周波数調整方法。(4) An airtight container, at least a portion of which is translucent, a diaphragm provided within the airtight container, electrodes provided on the front and back surfaces of the diaphragm, and from the outside of the airtight container, an electrically conductive means introduced into the interior thereof and connected to the electromagnetic waves on the front and back surfaces; and a frequency adjustment member provided in the interior portion of the airtight container corresponding to the light-transmitting portion of the airtight container; In a light-transmitting part of the container, a laser beam is irradiated from the outside of the airtight container through the light-transmitting part to a frequency adjustment object provided in the airtight container, and the frequency adjustment object is scattered by this irradiation, By attaching this scattered frequency adjustment material to the electrode of the diaphragm in a shape in which a plurality of continuous or discontinuous linear parts are arranged in parallel, a piezoelectric material that adjusts the frequency of the diaphragm is applied. How to adjust the frequency of a vibrator.
物は、気密容器の透光部内面側に設けた金属コート膜で
構成した圧電振動子の周波数調整方法。(5) A method for adjusting the frequency of a piezoelectric vibrator according to claim (4), wherein the frequency adjusting object is a metal coated film provided on the inner surface of a light-transmitting part of an airtight container.
膜は、気密容器の内面側の粗面化部分上に設けた圧電振
動子の周波数調整方法。(6) A method for adjusting the frequency of a piezoelectric vibrator according to claim (5), wherein the metal coating film is provided on a roughened inner surface of an airtight container.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2167706A JPH0456508A (en) | 1990-06-26 | 1990-06-26 | Piezoelectric vibrator and its frequency adjustment method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2167706A JPH0456508A (en) | 1990-06-26 | 1990-06-26 | Piezoelectric vibrator and its frequency adjustment method |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0456508A true JPH0456508A (en) | 1992-02-24 |
Family
ID=15854706
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2167706A Pending JPH0456508A (en) | 1990-06-26 | 1990-06-26 | Piezoelectric vibrator and its frequency adjustment method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0456508A (en) |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6787970B2 (en) * | 2003-01-29 | 2004-09-07 | Intel Corporation | Tuning of packaged film bulk acoustic resonator filters |
| JP2010074840A (en) * | 2009-11-06 | 2010-04-02 | Seiko Epson Corp | Piezoelectric vibrating piece, and method of manufacturing the same |
| JP2023125801A (en) * | 2022-02-28 | 2023-09-07 | 株式会社大真空 | Frequency adjustment method of piezoelectric vibration device and piezoelectric vibration device |
-
1990
- 1990-06-26 JP JP2167706A patent/JPH0456508A/en active Pending
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6787970B2 (en) * | 2003-01-29 | 2004-09-07 | Intel Corporation | Tuning of packaged film bulk acoustic resonator filters |
| JP2010074840A (en) * | 2009-11-06 | 2010-04-02 | Seiko Epson Corp | Piezoelectric vibrating piece, and method of manufacturing the same |
| JP2023125801A (en) * | 2022-02-28 | 2023-09-07 | 株式会社大真空 | Frequency adjustment method of piezoelectric vibration device and piezoelectric vibration device |
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